pdfs.semanticscholar.org€¦ · Evaluation of the Cone Penetrometer for liquefaction Hazard...

359
Evaluation of the Cone Penetrometer for liquefaction Hazard Assessment Geoffrey R. Martin and Bruce J. Douglas Fugro, Inc. 3777 Long Beach Boulevard Long Beach, California 90807 USGS CONTRACT NO. 14-08-0001-17790 Supported by the EARTHQUAKE HAZARDS REDUCTION PROGRAM OPEN-FILE NO.81-284 U.S. Geological Survey OPEN FILE REPORT This report was prepared under contract to the U.S. Geological Survey and has not been reviewed for conformity with USGS editorial standards and stratigraphic nomenclature. Opinions and conclusions expressed herein do not necessarily represent those of the USGS. Any use of trade names is for descriptive purposes only and does not imply endorsement by the USGS.

Transcript of pdfs.semanticscholar.org€¦ · Evaluation of the Cone Penetrometer for liquefaction Hazard...

Page 1: pdfs.semanticscholar.org€¦ · Evaluation of the Cone Penetrometer for liquefaction Hazard Assessment Geoffrey R. Martin and Bruce J. Douglas Fugro, Inc. 3777 Long Beach Boulevard

Evaluation of the Cone Penetrometer for liquefaction Hazard Assessment

Geoffrey R. Martinand

Bruce J. Douglas

Fugro, Inc.3777 Long Beach Boulevard

Long Beach, California 90807

USGS CONTRACT NO. 14-08-0001-17790 Supported by the EARTHQUAKE HAZARDS REDUCTION PROGRAM

OPEN-FILE NO.81-284

U.S. Geological Survey OPEN FILE REPORT

This report was prepared under contract to the U.S. Geological Survey and has not been reviewed for conformity with USGS editorial standards and stratigraphic nomenclature. Opinions and conclusions expressed herein do not necessarily represent those of the USGS. Any use of trade names is for descriptive purposes only and does not imply endorsement by the USGS.

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Fugro, Inc./Consulting Engineers and Geologists

3777 Long Beach Boulevard PO. Box 7765 Long Beach, California 90807

Phone: (213) 595-6611, 979-1721 Telex: 656338

October 3, 1980

Mr. Gordon GreeneU.S. Department of the InteriorGeological Survey345 Middlefield RoadMenlo Park, California 94025

Dear Mr. Greene:

This letter serves to transmit our final Technical Report for U.S.G.S. Contract No. 14-08-0001-17790. We are submit­ ting fifteen copies of our report as per contract requirements. The report is titled, "Evaluation of the Cone Penetrometer for Liquefaction Hazard Evaluation". In addition, we are submit­ ting five copies of our final Management Report to the Contract­ ing Officer.

We have enjoyed working on this most interesting and valuable project and appreciate the flexibility shown by the U.S.G.S regarding project schedules. We hope this report serves to increase the present capabilities for definition of earthquake induced hazards.

Should you have any questions regarding our report, please contact me.

Sincerely,

ORIGINAL SIGNED BY

Bruce J. Douglas Project Engineer,

BDrmv

Enclosures

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EVALUATION OF THE CONE PENETROMETER FOR LIQUEFACTION HAZARD ASSESSMENT

Prepared for:

U.S. Department of the InteriorGeological SurveyMenlo Park, California 94025

Prepared by:

Fugro, Inc.Consulting Engineers and Geologists3777 Long Beach BoulevardLong Beach, California 90807

Principal Investigators:

Geoffrey R. MartinAssociate and Director of Engineering

Bruce J. DouglasProject Engineer, and Manager In-Situ Testing

October, 1980

CONTRACT NO. 14-08-0001-17790

IGRD

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TABLE OF CONTENTS

Page

1. INTRODUCTION ................... 1-1

1.1 CURRENT METHODS OF LIQUEFACTIONPOTENTIAL ASSESSMENT ............ 1-1

1.1 MICROZONATION OF EARTHQUAKE HAZARDS ..... 1-3

1.3 FACTORS AFFECTING LIQUEFACTION POTENTIAL,SPT, CPT .................. 1-5

1.4 SCOPE OF RESEARCH .............. 1-8

2. FIELD AND LABORATORY INVESTIGATIONS ....... 2-1

2.1 INTRODUCTION ................ 2-1

2.2 PROCEDURES ................. 2-1

2.3 SITE DESCRIPTIONS .............. 2-4

2.3.1 San Diego, California ........ 2-4

2.3.2 Salinas, California ......... 2-6

2.3.3 Moss Landing, California ....... 2-8

2.3.4 Sunset Beach, California ....... 2-9

2.3.5 San Jose, California ......... 2-10

2.3.6 Edmond, Oklahoma ........... 2-11

2.4 CONCLUSIONS ................. 2-13

3. DATA ANALYSES .................. 3-1

3.1 INTRODUCTION ................ 3-1

3.2 PREVIOUS INVESTIGATIONS ........... 3-2

3.2.1 SPT Research ............. 3-2

3.2.2 CPT Research ............. 3-5

3.2.2.1 CPT Versus Soil Type ..... 3-5

3.2.2.2 CPT Versus OverburdenPressure ........... 3-9

CRO

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TABLE OF CONTENTS (Cont.)

Page

3.2.2.3 CPT Versus SPT ........... 3-10

3.3 CURRENT INVESTIGATIONS ........... 3-14

3.3.1 CPT Classification of Soil Type . . . 3-14

3.3.2 Correlation of CPT Measurementsfor Overburden Pressure ....... 3-21

3.3.3 Correlation of qc to N ....... 3-25

3.3.3.1 qc/N Range Comparisons . . . 3-26

3.3.3.2 qc/N Versus Depth ..... 3-28

3.3.3.3 qc/N Versus N ....... 3-31

3.3.3.4 qc/N Versus qc ....... 3-32

3.3.3.5 qc/N Versus Friction Ratio. . 3-34

3.3.3.6 qc/N Versus MedianGrain Size ......... 3-35

3.3.3.7 qc/N Versus N ........ 3-36

3.3.3.8 Comparison of N andSide Friction ........ 3-42

3.3.3.9 Summary of qc/N Relations . . 3-42

4. SUMMARY AND CONCLUSIONS .... .......... 4-1

4.1 SUMMARY .................... 4-1

4.2 CONCLUSIONS .................. 4-3

4.3 RESEARCH SUGGESTIONS ............. 4-7

5. REFERENCES ..................... 5-1

APPENDICES Appendix No.

A ................ (Under Separate Cover)

B ................ (Under Separate Cover)

ii

IGRO

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LIST OF FIGURES

Chapter 2

Figure No.

2.1 Electric Friction Cone Penetrometer

2.2 Mechanical Trip Hammer (Pilcon Engineering)

2.3 San Diego Site Location

2.4 San Diego Site Layout

2.5 San Diego Site, CPT Profile

2.6 San Diego Site, Composite Site Profile

2.7 Moss Landing/Salinas, Site Locations

2.8 Salinas Site Layout

2.9 Salinas Site, CPT Profile

2.10 Salinas Site, Composite Site Profile

2.11 Moss Landing Site Layout

2.12 Moss Landing Site, CPT Profile

2.13 Moss Landing Site, Composite Site Profile

2.14 Sunset Beach Site Location

2.15 Sunset Beach Site Layout

2.16 Sunset Beach Site, CPT Profile

2.17 San Jose Site Locations: Coyote Creek North and Coyote Creek South

2.18 Coyote Creek North and South Site Layout

2.19 San Jose Site: Coyote North, CPT Profile

2.20 San Jose Site: Coyote North, Composite Site Profile

2.21 San Jose Site: Coyote South, CPT Profile

2.22 San Jose Site: Coyote South, Composite Site Profile

2.23 Edmond, Oklahoma Site Location

iii

IGRO

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LIST OF FIGURES (Cont.)

Chapter 2 (Cont.)

Figure No.

2.24 Oklahoma Site, CPT layout

2.25 San Diego Site, Composite N profile and

2.26 Salinas Site, Composite N profile and NS/NT

2.27 Moss Landing Site, Composite N Profile and

2.28 San Jose Site£: _Coyote North and South, Composite N Profiles and

2.29 Effect of Borehole on Subsequent Adjacent CPT Soundings - Salinas Site

Chapter 3

3.1 Cjvj Factors Versus Effective Overburden Pressue

3.2 Effects of Rod Length on SPT Blowcounts

3.3 CPT Soil Classification, Begemann Method

3.4 CPT Soil Classification, After Schmertmann (1978)

3.5 Effective Overburden Pressure Versus Cp=qc @ lTsf/qc

3.6 Comparison of Cp, C^ and Rod Length

3.7 Previous Correlations: qc = F(SPT), For Pure Sands (After de Mello, 1971)

3.8 Previous Correlations: qc = F(SPT), For Sands (After Sangerlat, 1972)

3.9 Composite: All Sites, qc vs Friction Ratio, Soil Classification Chart

3.10 Continuous Trace Method, Edmond Site, CPT Probe 119

3.11 Soil Type Classifications Using the CPT Continuous Trace Method

3.12 Soil Type Classifications Using the CPT Continuous Trace Method

iv

ICRQ

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LIST OF FIGURES (Cont.)

Chapter 3 (Cont.)

Figure No.

3.13 Limited Trace Method; Coyote North Site

3.14 Selected Points - Edmond Site, Liquidity Index vs qc and Friction Ratio

3.15 Trends in CPT Soil Classification

3.16 qc vs o-v ' for CPT Measurements in Sands (After Treadwell, 1975)

3.17 Composite: All Sites, <TV ' vs Cpj, Standard Hammer

3.18 Composite: All Sites, <TV ' vs Cpi, Trip Hammer

3.19 Composite: All Sites, trv ' vs Cp^, by Layer Average, Standard Hammer

3.20 Composite: All Sites, (TV ' vs Cpj by Layer Average, Trip Hammer

3.21 Select Points: All Sites, trv i vs Cpj, Standard Hammer

3.22 Select Points: All Sites, trv ' vs Cp i, Trip Hammer

3.23 San Diego Site: qc/N Range Comparison, Standard Hammer

3.24 Salinas Site: qc/N Range Comparisons, Standard Hammer

3.25 Moss Landing Site: qc/N Range Comparison, Standard Hammer

3.26 San Jose Site: Coyote North and South, qc/N Range Comparisons, Standard Hammer

3.27 San Diego Site: NAS North Island, qc/N Range Comparisons, Trip Hammer

3.28 Salinas Site: qc/N Range Comparisons, Trip Hammer

3.29 Moss Landing Site: qc/N Range Comparisons, Trip Hammer

3.30 San Jose Site: Coyote North and South, qc/N Range Comparisons, Trip Hammer

3.31 Composite Blowcount -vs Depth, San Diego: North Island

3.32 Composite Blowcount vs Depth, Salinas Site

_,- vTUGRd

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LIST OF FIGURES (Cont.)

Chapter 3 (Cont.)

Figure No.

3.33 Composite Blowcount vs Depth, Moss Landing Site

3.34 Composite Blowcount vs Depth, San Jose Site: Coyote North

3.35 Composite Blowcount vs Depth, San Jose Site: Coyote South

3.36 Composite: All Sites, qc/N vs Depth by Layer Averages

3.37 qc/N vs Effective Overburden Pressure (After Schmertmann, 1978)

3.38 Composite: All Sites, qc/N vs Depth, Standard Hammer

3.39 Composite: All Sites, qc/N vs Depth, Trip Hammer

3.40 Composite: All Sites, qc /N~ vs N, by Layer Averages

3.41 Composite: All Sites, qc/N vs N, Standard Hammer

3.42 Composite: All Sites, qc/N vs N, Trip Hammer

3.43 Composite: All Sites, qc/N vs N, for Selected Points, Standard Hammer

3.44 Composite: All Sites, qc/N vs N for Selected Points, Trip Hammer

3.45 Composite: All Sites, qc/N" vs q c , by Layer Averaging

3.46 Composite: All Sites, qc/N vs qc , Standard Hammer

3.47 Composite: All Sites, qc/N vs qc , Trip Hammer

3.48 Composite: All Sites, qc/N vs qc , for Select Points, Standard Hammer

3.49 Composite: All Sites, qc/N vs qc , for Select Points, Trip Hammer

3.50 Comparison of End Bearing of Mechanical vs Electric Cone (After Schmertmann, 1978)

3.51 Composite: All Sites, qc/N vs Friction Ratio, by Layer Averages

vi

ICRD

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LIST OF FIGURES (Cont.)

Chapter 3 (Cont.)

Figure No.

3.52 Composite: All Sites, qc/N vs Friction Ratio, Standard Hammer

3.53 Composite: All Sites, qc /N vs Friction Ratio, Trip Hammer

3.54 Composite: All Sites, q c /N vs Friction Ratio, for Select Points, Standard Hammer

3.55 Composite: All Sites, qc/N vs Friction Ratio, for Select Points, Trip Hammer

3.56 Composite: All Sites, qc/N vs 059, Standard Hammer

3.57 Composite: All Sites, qc/N vs 050, Trip Hammer

3.58 Composite: All Sites, qc vs N by Layer Averages

3.59 Composite: All Sites, qc vs N, Standard Hammer

3.60 Composite: All Sites, qc vs N, Trip Hammer

3.61 Composite: All Sites, qc vs N, for Select Points, Standard Hammer

3.62 Composite: All Sites, qc vs N, for Selected Points, Trip Hammer

3.63 Comparison of qc vs N, Standard Hammer and Schmertmann Relation

3.64 Comparison of qc vs N, Trip Hammer and Schmertmann Relation

3.65 Comparison of qc vs N, Trip Hammer and COE Trip Hammer

3.66 Penetration Resistance in Layered Media (after Treadwell (1975)

3.67 Composite: Average Corrected Blowcount vs Plasticity Indices, Edmond Site

3.68 Edmond Site, Range of Average CPT End Bearing for Friction Ratio Bands

VI 1

FUGRO

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LIST OF FIGURES (Cont.)

Chapter 3 (Cont.)

Figure No.

3.69 Comparison of Edmond Site, SPT with PK3 and CPT with Friction Ratio = 0.8 to 2.25%

3.70 Edmond Site, SPT N to LI, All Borings with Adjacent CPT Soundings

3.71 Composite: All Soundings: Edmond Site, Corrected qc vs Depth for Sand Zone

3.72 Composite: All Soundings and Borings, Edmond Site, qc/N vs Depth for CPT Sand Zones and Blowcounts with Pj<3

3.73 Composite: All Sites, CPT Side Friction vs N, Standard Hammer

3.74 Composite: All Sites, CPT Side Friction vs N, Trip Hammer

3.75 Composite: All Sites, Frequency Histograms by Layer Average

3.76 Composite: All Sites, Frequency Histogram, qc/N vs Friction Ratio, Standard Hammer

3.77 Composite: All Sites, Frequency Histogram, qc/N vs Friction Ratio, Trip Hammer

3.78 Composite: All Sites, Frequency Histogram, qc/N

Chapter 4

4.1 Composite: All Sites, N vs qc vs Friction Ratio, Standard Hammer

4.2 Composite: All Sites, N vs qc vs Friction Ratio, Trip Hammer

4.3 Predicted vs Measured N Value Profile: Edmond Site Boring 120

Vlll

flJGRa

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LIST OF APPENDICES

APPENDIX A

Appendix No.

A.I - A.10 Cone Penetrometer Tests, San Diego

A.11 - A.18 Log of Borings, San Diego

A.19 - A.33 Cone Penetrometer Tests, Salinas Site

A.34 - A.41 Log of Borings, Salinas Site

A.42 - A.50 Cone Penetrometer Tests, Moss Landing Site

A.51 - A.58 Log of Borings, Moss Landing Site

A.59 - A.61 Cone Penetrometer Tests, Sunset Beach

A.62 - A.73 Cone Penetrometer Tests, San Jose:Coyote North

A. 74 - A.83 Cone Penetrometer Tests, San Jose:Coyote South

A.84 - A.89 Log of Borings, San Jose: Coyote North

A.90 - A.93 Log of Borings, San Jose: Coyote South

APPENDIX B

B.I San Diego Site: %/N vs Depth by Layer Averages

B.2 Salinas Site, qc/N vs Depth by Layer Averages

B.3 Moss Landing Site, q^c /N vs Depth by Layer Averages

B.4 San Jose Site: Coyote North and South, vs Depth by Layer Averages

B.5 San Diego Site qc /N vs Depth, Standard Hammer

B.6 Salinas Site, qc/N vs Depth, Standard Hammer

ICRD

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LIST OF APPENDICES

APPENDIX B (Cont.)

Appendix No.

B.7 Moss Landing Site, qc/N vs Depth, Standard Hammer

B.8 San Jose Site: Coyote North and South, qc/N vs Depth, Standard Hammer

B.9 San Diego Site qc/N vs Depth, Standard Hammer

B.10 Salinas Site, qc/N vs Depth, Trip Hammer

B.ll Moss Landing Site, qc/N vs Depth, Trip Hammer

B.12 San Jose Site: Coyote North and South, qc/N vs Depth, Trip Hammer

B.13 San Diego Site, qc/N vs N by Layer Averages

B.14 Salinas Site, qc/N vs N by Layer Averages

B.15 Moss Landing Site, q"c/N vs N by Layer Averages

B.16 San_Jose_Sites: Coyote North and South, qc/N vs N by Layer Averages

B.17 San Diego Site, qc/N vs N, Standard Hammer

B.18 Salinas Site, qc/N vs N, Standard Hammer

B.19 Moss Landing Site, qc/N vs N, Standard Hammer

B.20 San Jose Site: Coyote North and South, qc/N vs N, Standard Hammer

B.21 San Diego Site, qc/N vs N, Trip Hammer

B.22 Salinas Site, qc/N vs N, Trip Hammer

B.23 Moss Landing, qc/N vs N, Trip Hammer

B.24 San Jose Site: Coyote North and South, qc/N vs N, Trip Hammer

B.25 San Diego: qc/N vs qc by Layer Average

B.26 Salinas Site, qc/N vs qc by Layer Average

IGRU

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LIST OF APPENDICES

APPENDIX B (Cont.)

Appendix No.

B.27 Moss Landing, qc/N vs qc , by Layer Average

B.28 San Jose Site: Coyote North and South,

qc/N vs q c , by Layer Average

B.29 San Diego Site, qc/N vs qc , Standard Hammer

B.30 Salinas Site, qc/N vs qc , Standard Hammer

B.31 Moss Landing Site, qc/N vs qc , Standard Hammer

B.32 San Jose Site: Coyote North and South, qc/N vs qc , Standard Hammer

B.33 San Diego Site, qc/N vs qc , Trip Hammer

B.34 Salinas Site, qc/N vs qc , Trip Hammer

B.35 Moss Landing Site, qc/N vs qc , Trip Hammer

B.36 San_Jose S^te^ Coyote North and South, qc/N vs qc , Trip Hammer

B.37 San Diego Site,~qc7N vs Friction Ratio, by Layer Averages

B.38 Salinas Site, qc/N vs Friction Ratio, by Layer Averages

B.39 Moss Landing, qc/N vs Friction Ratio, by Layer Averages

B.40 San Jose: Coyote North and South, qc/N 'vs Friction Ratio by Layer Averages

B.41 San Diego Site qc/N vs Friction Ratio, Standard Hammer

B.42 Salinas Site, qc/N vs Friction Ratio, Standard Hammer

B.43 Moss Landing Site, qc/N vs Friction Ratio, Standard Hammer

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LIST OF APPENDICES

APPENDIX B (Cont.)

Appendix No.

B.44 San Jose Site: Coyote North and South, qc/N vs Friction Ratio, Standard Hammer

B.45 San Diego Site, qc/N vs Friction ratio, Trip Hammer

B.46 Salinas Site, qc N vs Friction Ratio, Trip Hammer

B.47 Moss Landing Site, qc/N vs Friction Ratio, Trip Hammer

B.48 San Jose Site: Coyote North and South, qc/N vs Friction Ratio, Trip Hammer

B.49 San Diego Site: NAS North Island, q"c vs N", by Layer Averages

B.50 Salinas Site, q"c vs N by Layer Averages

B.51 Moss Landing Site, q"c vs N" by Layer Averages

B.52 S^an Jo£e Site: Coyote North and South, qc vs N by Layer Averages

B.53 San Diego, qc vs N, Standard Hammer

B.54 Salinas Site, qc vs N, Standard Hammer

B.55 Moss Landing Site, qc vs N, Standard Hammer

B.56 San Jose: Coyote North and South, qc vs N, Standard Hammer

B.57 San Diego Site, qc vs N, Trip Hammer

B.58 Salinas Site, qc vs N, Trip Hammer

B.59 Moss Landing Site, qc vs N, Trip Hammer

B.60 San Jose Site: Coyote North and South, qc vs N, Trip Hammer

IGRO

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1. INTRODUCTION

This report describes the activities and results of the

investigations of the correspondence between Cone Penetrometer

Tests (CPT) and Standard Penetration Tests (SPT) performed

under USGS Contract No. 14-08-0001-17780. The program involved

performance of CPTs and SPTs at several sites in California and

at one site in Oklahoma. The comparison of the correspondence

between those test results has as a primary goal the development

of a data base facilitating the use of the CPT for use in

liquefaction potential assessments. The scope of investigations

was defined in proposal P78-310 in response to USGS RFP 460W.

1.1 CURRENT METHODS OF LIQUEFACTION POTENTIAL ASSESSMENT

Current methods of liquefaction potential assessment are in

general limited to either extensive field sampling, laboratory

testing, and dynamic analyses, or rely upon the simplified,

empirical SPT-based method developed by Seed (1979). The

former method has the disadvantages of high cost and time

commitment, the need for field borings and sophisticated

laboratory equipment, and advanced computational capabilities.

In addition, taking high-quality samples of liquefiable soils

(loose, saturated, sands and silts) is a difficult procedure,

and almost invariably results in changed sample structure and .

density.

In addition, the idealization of the soil profile based upon

lab test results usually requires selection of some average

or bounding properties for use in subsequent analyses. It

ICRO

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1-2

is never known which properties are most important for trans­

mission of shear waves and, therefore, parametric studies

usually need be performed.

The second routine method, the Standard Penetration Test (SPT),

avoids the extreme costs of the more analytical approach, yet

still suffers from the need for expensive field operations

and some laboratory work. Although the test is dynamic, and

should therefore provide some direct indication of dynamic soil

properties, the results can be taken as only general indica­

tions of site conditions.

It is well known in the geotechnical industry how error-plagued

is the SPT, with some 30 different error sources having been

defined (Fletcher, F. A., 1965; Kovacs, et al, 1975). A survey

of equipment and procedures in use throughout the U.S. reveals

that not only equipment but also procedure suffers from lack of

standardization. Efforts by many, notably Schmertmann (1976)

and Kovacs (1978), to standardize the test have met with only

limited success. One of the major impediments to standardization

results from the importance of maintaining the SPT data base

that has been developed in the last forty years. This data

base is found in publications as well as in design guidelines

for use at national or local levels. Further, most practitioners

have developed a "feeling" for SPT results, and are able to

make valid engineering judgments from such results. Many of

these practitioners feel that by standardization (such as using

controlled-energy, or velocity, mechanical hammers) the data

IGRO

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base developed over the years will be invalidated. This is a

realistic concern, and several researchers have responded by

instituting a nationwide program of hammer-energy measurements.

Once such measurements have been made, it should be possible

to correlate the average energies represented by any particular

data base with the energy of the standardized hammer (Kovacs,

1978).

1.2 MICROZONATION OF EARTHQUAKE HAZARDS

In recent years there has been an effort, in response to

recognized need, to develop procedures for regional-level

microzonation of earthquake hazards, in particular with respect

to liquefaction potential. With regard to liquefaction hazard

assessment, the usual method involves qualitative definition

of two necessary conditions: a sufficient driving source and

susceptible soils (Youd, et al, 1978; Youd and Perkins, 1977;

Kennedy, et al, 1977). Ignoring the delineation of zones

having potential to receive sufficient strong motion shaking,

the delineation of susceptible soil zones has been based upon

existence of high ground water levels (liquefaction is primarily

of concern in the upper 40 feet of a soil profile) in cohesion-

less, young (Holocene age) soils. The delineation of water

letels is usually through records of ground water investiga­

tions, and provides adequate information for regional assess­

ments. Site specific investigations still need more accurate

definition of water level, but this factor is relatively easily

determined.

IGRO

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The delineation of susceptible soils (young, cohesionless) has

been through recourse to published data. These data are

usually either geologic or soils maps, or boring information

from previous investigations. The shortcoming of using geo­

logic maps is their overly generalized nature. Certainly such

generalization is necessary for microzonation efforts covering

hundreds of square miles of land surface; however, the method

provides only an indication of actual extent of susceptible

materials. On a regional basis, it is possible to define zones

of clearly nonsusceptible materials, such as clays or gravels,

as differentiated from susceptible materials such as beach or

river sand. The primary difficulty arises in those intermed­

iate and mixed soils: silts, silty sands, clayey sands, sands,

sandy silts, and even silty and sandy clays. The liquefaction

potential of a soil depends, for a given driving energy, upon

the grain size and distribution, and the amount and activity

of any clay size components. In addition, the in-situ stress

conditions and soil density have a significant influence on

liquefaction potential. Although some qualitative estimates

of stress state and density can be made on the basis of geologic

history, it becomes difficult to attach any quantitative

information to such estimates.

The difficulty in quantifying microzonation delineations

reinstates the need for some field measurement. The cost and

time associated with a boring-type measurement likely becomes

prohibitive. This is where the Cone Penetrometer Test (CPT)

is seen to be of value. The test is very rapid, with up to

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800 feet of measurements being made in a single day, as compared

to a maximum of about 100 feet of comparable SPT measurements

in a like time. Further, the CPT is standardized, is not

operator or technique dependent, and provides a repeatable

set of continuous measurements of soil resistance.

The primary concern in using CPT for microzonation efforts is

establishing some correlation between CPT results and liquefac­

tion potential. Such correlation exits for SPT results (Seed,

1979). The SPT-liquefaction potential correlation is based

upon SPT measurements made at sites which subsequently lique­

fied during earthquake shaking. The correlation was extended

through use of "shaking-table" tests. Knowledge of the magni­

tude and acceleration characterizing the actual or artificial

earthquake allowed development of a set of values, for any

specific earthquake, bounding the soil cyclic strength dividing

liquefiable from non-liquefiable soils. The soil cyclic

strength was then represented by a normalized SPT blowcount.

Because no extensive data base of this type exists for CPT

measurements, a possible approach is to first compare the CPT to

liquefaction potential through the intermediate use of the SPT

data base. Thus the current program is designed to further

study correspondence between the CPT and SPT as a step toward

the eventual goal of a CPT-liquefaction potential correlation.

1.3 FACTORS AFFECTING LIQUEFACTION POTENTIAL, SPT, CPT

Several questions arise when considering such a correlation

program. First, for any empirical "index" to be valid for

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prediction of some other property, such as liquefaction poten­

tial, the index and the property should be similarly dependent

upon the same variables. Typical variables include soil type,

stress state and stress history, soil density, and soil structure.

Given the range in parameter variation in-situ, it is not sensible

to try to account for the effect of variations producing only a

small change in the correlation. Rather, major changes should

be investigated. The variables accepted as having major affect

upon liquefaction potential are: soil type, degree of satura­

tion, effective overburden pressure, density or relative density,

lateral stress, and soil structure or fabric. It is assumed

that location of permanent ground water can be established, thus

eliminating degree of saturation from concern. This leaves, as

of primary importance, the influences of soil type, structure,

and density and effective stress history.

These variables are not easily rated in terms of their effect

upon either liquefaction potential or SPT measurements. First,

it is in general true that increasing clay content results

in decreased liquefaction potential and decreased blowcounts.

Increased sand content results in increased blowcount and

increased liquefaction potential as compared to clayey soils.

However, for a given soil, an increase in blowcount results

in decrease of liquefaction potential. Further, the effect

of intermediate fines content upon liquefaction potential is

not known. It is generally assumed that some value of Plas­

ticity Index (PI) can divide susceptible from nonsusceptible

soils (Donovan and Singh, 1976). This value has been assumed

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at from 5 to 12 percent. It is unlikely, however, that the SPT

varies inversely proportional to liquefaction potential as

fines content increases up to this point of low PI. Further,

there is no certainty that the criteria is applicable on other

than a case-by-case level.

The same type of arguments can be advanced relating liquefaction

potential to median grain size (059). Although the trend in

the relation between D^Q and liquefaction potential holds for

comparison of extremes, it is not valid for comparisons within

the range most commonly of concern: sands and silts.

t>

A second primary factor, effective overburden and lateral pres­

sures, is likewise difficult to assess. The cyclic strength

of a soil (or liquefaction potential) certainly varies with the

effective stress in the soil in that increased driving energy

is required to generate sufficient shear strains to result in

increased porewater pressure at increased confining pressures.

Thus for a sand at a constant relative density, the blowcount

measured would non-linearly vary proportional to the effective

pressure at the location of the blowcount. In order to elimi­

nate the influence of this variable, both cyclic strength and

blowcounts are normalized by either the effective vertical

stress or some measure of that stress. For blowcounts, the

measure is the factor CN , which is intended to normalize a

blowcount to that which would be obtained at an effective

overburden pressure of one ton per square foot. This factor

is appropriate for normally consolidated soils only.

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being of different ages. In particular, the correlations are

examined as dependent upon soil type, resistance, and overburden

pressure, as these are the primary, presently quantifiable,

factors affecting liquefaction potential.

Considerable attention is placed upon the method of data

comparison. The primary reason for this attention is the

essential difference between the data of the CPT and SPT.

The CPT provides continuous, repeatable measurements, while

the SPT provides point data dependent upon equipment and

method. The variability of SPT measurements is clearly

evidenced in examination of the data presented in this report.

Such variability further emphasizes the need for SPT hammer

energy measurements, as discussed previously. This need,

as well as other research needs related to field methods of

liquefaction potential assessment, are further discussed in

Chapter 4, Summary and Conclusions.

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2. FIELD AND LABORATORY INVESTIGATIONS

2.1 INTRODUCTION

Field investigations supported under this research program

included Standard Penetration Tests and electric Cone Penetrometer

Tests performed at several sites in California. In addition,

data from other projects are also included, in particular, from

a project in Oklahoma. Samples taken from California sites

during the SPT program were returned to the Long Beach soils

laboratory for classification testing. All classification data

and SPT measurements from the Oklahoma site were developed and

provided by the Tulsa District U.S. Army Corps of Engineers,

who also allowed use of the CPT data from the site. A summary

of field investigations is given in Table 2.1.

2.2 PROCEDURES

The testing procedures used in this program were in general

accordance with those procedures recommended by the ASTM.

Applicable standards used in the program are: D1586 for SPT

procedures, D3441-75T for CPT procedures, and D422 for labora­

tory grain size analyses. Corps of Engineers field and

laboratory tests were performed in accordance with U.S. Army

Corps of Engineers Testing Standards.

The CPT soundings were performed using a truck-mounted electric

cone penetrometer. The electric CPT system consists of a

40,000 pound truck equipped with a hydraulic loading system

capable of applying 40,000 pounds of force onto the end of

1.4 inch diameter, hollow "sounding" rods. The electric

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friction cone tip is mounted on the end of the rod string with

an electrical cable threaded from the cone, through the.trailing

rods, and into the electronics located in the truck.

The electric friction cone tip essentially consists of a strain-

gage-instrumented body enclosed within a cylindrical friction

sleeve of 150 square centimeters surface area, and capped with

a 60-degree apex angle conical tip of 10 square centimeters

projected surface area. An inclinometer is located within the

cylindrical body. A description of this friction cone and the

general CPT methodology is given by de Ruiter (1971); a schematic

diagram of the electric friction cone is shown in Figure 2.1.

The sounding rods with attached friction cone are pushed into

the soil at a constant rate of two cm/sec in one-meter runs.

At the end of each one-meter run, an additional one-meter

length of rod is added, and the sounding continued. This

process is repeated until reaching refusal or a specified

depth. Additional information about the general procedures

used for CPT site investigations are described elsewhere

(Sangerlat, 1972).

A continuous analog record of the forces on the end (cone end

bearing, q c ) and friction sleeve (side friction) of the cone

is taken on a strip-chart recorder located in the penetrometer

truck. The chart recorder is driven by an optical encoder

controlled by the advance of the sounding rods; the length of»

the cone record is directly and exactly proportional to the

length of extended sounding rods. Inclinometer readings (taken

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during rod breaks) showed inclinations of no more than 3 degrees

during any of the sounding.

The Standard Penetration Tests at California sites were performed

using Failing 750 drill rigs and drill pipe having an I.D. of

1.5 inches and an O.D. of 2.375 inches with a weight of 55

pounds per 10.5 foot long rod section. Drill bits were 5-7/8"

fishtails baffled to prevent any jetting-induced soil disturbance

Particular care was taken to thoroughly flush the hole prior to

slow removal of the drill bit. Drilling mud was maintained at

ground surface in all borings.

SPT hammers were of two types: a rope-around-the-cathead

"donut" hammer provided by the drillers (total weight of 225

pounds), and a "free-fall", mechanical trip hammer (total

weight of 210 pounds) manufactured by Pilcon Engineering

(Figure 2.2). The trip hammer uses a rocker arm cam release

system which provides a constant hammer drop height of 30+ 1

inches. No measurements of the energies delivered by these

hammers were obtained.

Sampling spoons were newly constructed following ASTM guide­

lines with the exception that space for liners was provided,

but liners were not used. Schmertmann (1976, 1979) notes that

liner samplers used without liners is the common practice, and

represents a de facto change to ASTM D2586.

The Corps of Engineers SPT procedures follow ASTM guidelines

with the exception of hammer type. The hammer used in this

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program is of the type described by Marcuson and Bieganousky

(1977) and is a free-fall hammer with hydraulic drive. More

information about the effects of such free fall hammers is

given in later sections. The rate of application of hammer

blows with this device was about five per minute, while the

rates with both the standard and the Pilcon mechanical hammer

were about 40 blows per minute.

2.3 SITE DESCRIPTIONS

The sites investigated during this program were generally

selected on the basis of having saturated, cohesionless soils.

Sites were located in San Diego, Seal Beach, Salinas, Moss

Landing, and San Jose, California, and Edmond, Oklahoma* The

following sections provide brief description of site geology

and soil profiles based upon the boring, sounding, and labor­

atory investigations.

2.3.1 San Diego, California

The site is located at the Naval Air Station near San Diego,

on artificial fill emplaced between North Island and Coronado

Island to connect the islands across the old Spanish Bight.

North Island and Coronado Island are probably remnants of the

Quaternary Nestor or lower marine terrace (Ellis and Lee,

1919). Surficial terrace deposits are chiefly silts and sands

In the Spanish Bight area, hydraulic fill, principally sand

silty sand, and silt dredged from San Diego Bay, occurs at

the surface (Forrest and Ferritto, 1976). Fill in this zone

was placed in 1945.

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Bedrock beneath terrace deposits and artificial fill consists

of Cretaceous and Tertiary marine, lagoonal, and fluviatile

clastic rocks, chiefly sandstone, conglomerate, and shale

(Kennedy, 1973). These rocks dip gently northeast on the

northeast flank of a northwest trending anticline with axis

off the coast of San Diego. Planation of these dipping beds

has resulted in removal of upper (Eocene-Pliocene) units

beneath North Island with occurrence of progressively younger

rocks to the east (Kennedy, 1973) . Only the Cretaceous Rosario

Group occurs beneath North Island. In the vicinity of the

Spanish Bight and Coronado Island, rocks of the Eocene La Jolla

Group overlie Cretaceous rocks in the subsurface (Kennedy,

1973) . Further east, marine Pliocene deposits of the San Diego

Formation overlie these Eocene rocks, and may extend into the

test site area (Forrest and Ferritto, 1976).

Basement in the area consists of Cretaceous and older metamor-

phic and intrusive rocks (Kennedy, 1973; Forrest and Ferritto,

1976). The Rose Canyon fault is postulated to occur just west

of the test site forming the eastern edge of North Island

(Forrest and Ferritto, 1976), although others place the south­

ern extension of this fault along the east side of San Diego

Bay (Ziony, 1973). Movement on this fault has probably occurred

during late Pleistocene and may be as recently as early Holocene

(Ziony, 1973).

Nine Cone Penetrometer Tests and eight Standard Penetration

Tests were performed at the San Diego site. The location of

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the site and of each sounding and boring is given in Figures 2.3

and 2.4. The sounding logs are shown summarized in Appendix A

in Figure A.I, and individually in Figures A.2 through A.10,

and the boring logs in Figures A.11 through A.18. Site profiles

were drawn based on the CPT results, and the SPT logs and

laboratory classification results. These two profiles are

shown in Figures 2.5 and 2.6. It should be noted that all of

the CPT profile-series logs have been smoothed, that is,

averaged over a vertical distance of one foot. The effect of

such smoothing can be seen by comparison of the profile-series

logs of Figure 2.5 with the individual logs of Figures A.2

through A.10.

Examination of the profiles shown in Figures 2.5 and 2.6 reveals

that essentially identical profiles result using either CPT or

SPT methods. The SPT results revealed changes in color indica­

tive of a layer transition, while the CPT, being essentially a

strength measurement, shows virtually no layering. However,

the CPT continuous record does reveal the presence of lenses or

pockets of dissimilar materials not found with the SPT method.

2.3.2 Salinas, California

The Salinas site is on the southwest bank of the Salinas River

near the mouth of El Toro Creek. Sediments in the area consist

chiefly of interbedded fluvial silty sand and sand deposited

by the Salinas River, with interbeds of sand and gravel from

the El Toro Creek alluvial fan. These fluvial deposits are

Holocene age and extend to depths of 10-20 m (Tinsley, 1980,

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personal communication). They are underlain by delta and

estuarine sediments deposited during higher stands of sea level

when the sea transgressed up the Salinas Valley into the area.

Estuarine deposits are chiefly black muds (organic silty clays)

of Holocene age. These fine-grained deposits interfinger with

delta/fluvial sandy deposits, and generally do not persist to

depths exceeding 30 m (Tinsley, 1980, personal communication).

At these depths, deposits are again predominantly fluvial in

origin and are Pleistocene in age. Beneath these Pleistocene-

age Salinas River fluvial deposits is the Plio-Pleistocene

nonmarine Paso Robles Formation, generally at depths greater

than 300 feet (Tinsley, 1980, personal communication).

Dibblee (1976) has mapped and named the Rinconada-Reliz fault

along the northeastern flank of the Sierra de Salinas, forming

the southwestern edge of the Salinas Valley. The fault would

project very close to the site, between it and the mountain

front 1/4 mile to the west. Movement along the fault was

right-lateral during late Pleistocene times, but has since

shifted to predominantly reverse-slip during Holocene time

(Tinsley, 1980, personal communication).

Fifteen CPTs and eight SPTs were performed at the Salinas

site. The locations of the site and each sounding and boring

are given in Figures 2.7 and 2.8. The sounding and boring

logs are shown in Appendix A Figures A.19 through A.33 and

A.34 through A.41, respectively. It should be noted that

some of the soundings were performed using an oversized cone

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(15 square centimeter projected end area). These soundings are

also shown in Appendix A (identified as F15CKE) along with the

rest of the Salinas soundings. The final site profiles, again

as based on CPT and SPT and laboratory test data are shown in

Figures 2.9 and 2.10.

Comparison of the logs shown in Figures 2.9 and 2.10 reveals

the expected differences. The SPT method provides information

regarding soil grain size, while the CPT method implicitly

provides strength data and more detailed stratigraphic data

than possible using the SPT method.

2.3.3 Moss Landing, California

The site at Moss Landing is underlain by beach sands to prob­

able depths of ten meters or more. Eolian sands, derived

from reworking of beach sands, form a thin cover at the surface

and may occur interbedded with beach deposits at depth. Other

deposits in areas adjacent to the site are part of a late

Holocene transgressive sequence consisting of relatively thick

sands offshore and estuarine and fluvial deposits onshore

(Tinsley, 1980, personal communication). The site is near

the mouths of the Salinas and Pajoro Rivers which empty into

Monterey Bay. Sloughs (Elkhorn, Moro Cojo) and tidal channels

occur just east of Moss Landing, forming an area of modern

fine-grained estuarine deposits which thin to the east. These

types of deposits occur at depth near Moss Landing, interbedded

and underlain by sandy fluvial deposits (Tinsley, 1980, personal

communication), and contain gravel lenses, particularly at the

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base of the Holocene section which extends to about 100 to 180

feet below the surface (Tinsley, 1980, personal communication)

In the immediate site vicinity, deposits are principally

littoral, i.e., deposited in the shoreline environment within

the zone of tidal fluctuation. Sands predominate with some

interbedded silts and clays.

Nine CPTs and eight SPTs were performed at the Moss Landing

site. The site and boring and sounding locations are shown in

Figures 2.10 and 2.11. The sounding logs are given in Figures

A.42 through A.50 of Appendix A, and boring logs in Figures

A.51 through A.58. The final site profile for Moss Landing

based upon the CPT and the SPT and laboratory classification

data is shown in Figures 2.12 and 2.13, respectively.

2.3.4 Sunset Beach, California

The Sunset Beach site lies east of Anaheim Bay along the

principal tidal inlet into Sunset Bay. Sunset Bay is a tidal

marshland which has been closed off by a barrier beach. The

site is on the landward side of the barrier beach adjacent

to the marshlands. Surface materials consist of beach sands

(U.S. Department of Agriculture, 1978), probably reworked to

some extent by man during modification of the beach. Beach

sands at the site probably overlie and interfinger with tidal

marsh deposits (organic sands, silts, and clays) derived from

both marine and continental sources. Immediately inland from

the beach, Holocene deposits generally do not extend to depths

greater than 20 feet (Poland, et al, 1956). Along the beach,

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deposits may be somewhat thicker, consisting of unconsolidated

sand, silt and clay with no known gravels in the area (Poland

et al, 1956; Poland, 1959). Holocene deposits are underlain by

the Pleistocene Lakewood and San Pedro Formations, which extend

to depths greater than 500 feet consisting of loosely to

moderately consolidated sandstone, claystone, siltstone, and

marl (California Department of Water Resources, 1968; Poland

et al, 1956).

Three CPTs were performed at the Sunset Beach site (Figure

2.14) at the locations shown in Figure 2.15. No SPTs were

performed as the site was selected primarily because the

uniformity of the site soils facilitates estimation of the

effect of depth (or pressure) on cone penetrometer readings.

The results of the soundings are shown in Appendix A in Figures

A.59 through A.61 and the interpreted profile is shown in

Figure 2.16.

2.3.5 San Jose, California

Two different sites in the Coyote Creek vicinity near San Jose

were investigated. These sites occur in the gently sloping

alluvial plain of the Santa Clara Valley six to seven miles

south of the southern tip of San Francisco Bay. The surficial

material at the sites is predominantly medium-grained alluvium

(fine sand, silt, and clayey silt) of Holocene age (Helley

and Brabb, 1971; Helley, et al, 1979). This alluvium was

derived from sources to the east and south along the Coyote

Creek drainage. Natural levees deposited during flood stage

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occur along the banks of Coyote Creek in which test sites are

located. The site areas are near the southern limit of modern

bay mud and may be underlain at shallow depths by thin bay muds

deposited when the bay extended further southward as recently

as 125 years ago (Helley and others, 1979). At greater depths,

Pleistocene alluvium and Pleistocene bay mud interfinger, but

alluvial deposits probably predominate beneath the site area.

No known faults traverse or underlie the area, although the

historically active Hayward fault occurs about 5 kilometers

to the east. Holocene and Pleistocene beds underlying the

area are generally undeformed, dipping slightly northward

toward the bay in original depositional position.

The locations of the two Coyote Creek sites are shown in Fig­

ure 2.17. The north site had eleven CPT soundings (two with

the oversized cone) and six borings, while the south site

had ten soundings (two with oversized cone) and four borings.

The locations of the borings and soundings are shown in Figure

2.18. The sounding logs are presented in Appendix A,in Figures

A.62 through A.73 and A.74 through A.83 for the north and south

sites, and the boring logs in Figures A.84 through A.89 and

A.90 through A.93 for north and south sites, respectively.

The site profiles based on these data are given in Figures 2.19

and 2.20 for the north site, and in Figures 2.21 and 2.22 for

the south site.

2.3.6 Edmond, Oklahoma

The Oklahoma site lies in the valley of the Deep Fork River

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northeast of Oklahoma City (Figure 2.23). The area is on

the east flank of the Anadarko Basin, characterized by gently

west-dipping Permian-age sedimentary rocks. The rocks in

the site vicinity are principally sandstone of the Garber

Sandstone and Wellington Formations of Lower Permian age

(Wood and Burton, 1968). These two formations are litho-

logically similar, consisting of lenticular beds of cross-

bedded sandstone interbedded with shale, generally sandy to

silty. Sands are fine- to very fine-grained, and are poorly

cemented (Wood and Burton, 1968). The site lies essentially

along the gradational contact between the two formations

(Bingham and Moore, 1975).

The site is underlain by modern alluvium of the Deep Fork

River Valley. Alluvium consists of sand, silt and clay with

lenticular beds of gravel (Bingham and Moore, 1975). The

thickness of alluvium in the valley overlying the Permian

bedrock varies from several feet to more than 50 feet (Wood

and Burton, 1968; Bingham and Moore, 1975). At the dam

centerline, the alluvium is about 83 feet thick, but upstream

300 feet it is only 14.5 feet thick (U.S. Army Corps of

Engineers, 1978). Valley bottom alluvium is Holocene age

and is unconsolidated.

Twenty-three CPTs and twenty-four SPTs were performed at the

Arcadia site at locations shown in Figure 2.24. Because of

the extremely complex nature of the site profile, significant

changes in soil type or resistance were found over distances

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of only a few feet in either horizontal or vertical directions.

For this reason, some of the data analyses (discussed in sub­

sequent sections) were performed upon average CPT and SPT results

Likewise, only a generalized profile could be developed. This

profile covers several hundred feet both along the dam centerline

and in the upstream-downstream axis and is not shown in this

report. For more information about the characteristics of this

site, the Corps of Engineers Design Memorandum may be consulted.

The complete set of boring and sounding logs from the Arcadia

site are available in that memorandum. Select information

about site characteristics is discussed in a subsequent section

of this report.

2.4 CONCLUSIONS

Primary conclusions that can be drawn based upon the field

investigations focus upon testing procedures, data consistency,

data interpretation, and the degree to which the test methods

provide data representative of site conditions. In regard to

testing procedures, it was noted during the field program that

constant attention was required to keep repeatability of SPT

method, although, only one driller was used. The tendency was

for the rope-around-the-cathead method hammer-drop height to

decrease with increasing number of blowcounts. Further, as the

focus of measurements was on sandy soils, after the first boring

was complete and the location of significant clay layers known,

the driller tended to assume layer continuity without actually

checking the clay layer extent encountered in subsequent borings.

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The effect of this assumption can be seen in comparison of the

CPT and SPT profiles where thin interlayers of sands and silts

are apparent in the CPT records but missing from the SPT records

Further comparison of the CPT-SPT profiles reveals that greater

evidence of spatial variability of soil types and layering is

visible with the CPT method. This includes the definition of

interlayers as well as thickness and extent of more massive

layers. However, the CPT method primarily reveals changes in

material type via the intermediary of changes in strength using

the tip measurement and the sleeve measurement, and no visual

fee of material change is obtained. At the sites investi-

this lack of sample presented no difficulties, but

.als were in general fairly common, well behaved sands,

', and mixes. One notable shortcoming is that the CPT

profiles presented in previous sections reveal no information

allowing definition of water table depth.

The potential for use of the piezometric cone penetrometer to

define water levels was to be investigated in this program.

However, due to equipment fabrication problems and because the

location of sensing elements within the tip and the interpreta­

tion of measured data are areas of current controversy, no such

investigations were performed. Subsequent investigations in

which the piezometric cone has been used indicate that if the

porous element is saturated with a high viscosity fluid, then

penetration through a dry layer overlying a saturated layer

will not result in loss of saturation to a degree eliminating

pore pressure response upon entering the saturated layer.

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Another interesting phenomenon observed during the field

program was the apparent "smoothing" of layer resistances

during SPT penetration using the higher energy free-fall

hammer. Figures 2.25 through 2.28 show average blowcount

versus depth profiles for each hammer type at each site. The

average blowcount values were calculated over three-foot

intervals where layer continuity was present. Also shown in

those figures are the ratios of average blowcounts using the

two hammers.

Further examination of the blowcount ratios by material type

reveals a trend toward increase in blowcount ratio with increas­

ing blowcount. A possible explanation for this trend revolves

around the question of the extension wave reflected from the

"free" end of the rod string. As the soil hardens, the free

end becomes progressively more fixed, allowing more of the

available energy to be transmitted by the rod string. The trip

hammer is of a type having a large diameter anvil which acts

as a wave trap, in particular for the free end condition.

Thus with increasing fixity, the trapped energy is more fully

transmitted, with resultant reduction in trip hammer blowcount

as compared with standard hammer blowcounts. This trend is

more fully discussed by Schmertmann (1979b).

As a final examination of field data, a series of CPT soundings

is presented in Figure 2.29. These soundings were performed

adjacent to and after a boring had been placed to determine

how close a sounding could be without showing any effects of

IGRO

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2-16

the nearby boring. In Figure 2.29 it can be seen that the

sounding placed one and one-half foot from the boring shows

one anomalously low end-bearing zone. Whether or not this

reduction resulted from the nearby boring cannot be certain

with only one test series; however, based upon this result,

the few soundings performed after a boring was completed were

placed at a distance of from six to twelve feet from the

nearest boring, a distance which is close enough to allow a

high degree of horizontal uniformity without being close

enough to sense any effect of the boring.

ICRD

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SITE

SAN DIEGO: MAS NORTH ISLAND

SALINAS SOUTH

MOSS LANDINGS

SUNSET BEACH

SAN JOSE: COYOTE NORTH

SAN JOSE: COYOTE SOUTH

ARCADIA:* EDMOND, OKLAHOMA

SPT

DATE

10/10-12/79

11/6-9,12-13/79

11/13-15/79

-

11/16-17,

20-21/79

11/19-20/79

1/20-5/8/80

TYPE

STANDARD TRIP

STANDARD TRIP

STANDARD TRIP

-

STANDARD

TRIP

STANDARD TRIP

STANDARD TRIP

NUMBER

4

5

4

4

4

4

-

3

3

2

2

24

CRT

NUMBER

9

15

9

3

11

10

23

DATE

4/18-19/79

11/12.14-15/79

11/12-13/79

3/17/80

7/11/80

11/5-16,19/79

11/17-19/79

3/28-4/3/80

*ALL SPT's PERFORMED BY U.S. ARMY CORPS OF ENGINEERS, TULSA, OKLAHOMA, DISTRICT ana

PROJECT NO:

USGS

SUMMARY OF FIELD WORK

79-153

11-80 TABLE 2.1

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ELECTRIC CABLE

CABLE CHANNEL-

STRAIN GAGES FOR FRICTION SLEEVE

INCLINOMETER

STRAIN GAGES FOR CONE-

"0" RINGS

CONNECTION ROD

> FRICTION SLEEVE

CONE

rJTJGROPROJECT NO.: 79-153

USGS CPT-SPT

ELECTRIC FRICTION CONE PENETROMETER

9-80 FIGURE 2.1

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AA

AA

1. THE WHOLE ASSEMBLY IS SHACKLED TO THE WINCH ROPE, HOISTED ON TO THE ROD OR PIPE CONNECTION AND SCREWED HOME

2. THE LOCKING PIN IS THEN REMOVED AND THE OUTER TUBE ASSEMBLY - CARRYING WITH IT THE MONKEY - IS RAISED BY THE WINCH

3.ON REACHING A HEIGHT OF 30", THE TRIP CAM OPERATES THE PAWLS, RE­ LEASING THE MONKEY TO DROP FREELY ON THE ANVIL

4. THE OUTER TUBE IS LOWERED TO RE­ ENGAGE THE HAMMER

PROJECT NO.: 79-153

USGS CPT-SPT

MECHANICAL TRIP HAMMER (PILCON ENGINEERING)

9-80 FIGURE 2.2

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\~\BRILLO NAT MON

Did lighthouse

\ Light^

SEE FIGURE : NORTH ISLAND

os X . fWate^. -

BORDER FIELD '

FROM USGS 2° TOPOGRAPHIC MAP OF SAN DIEGO, CA. 1959, REVISED 1978

PROJECT NO.: 79-153

USGS CPT-SPT

SAN DIEGO SITE LOCATION

9-80 FIGURE 2.3

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K.Ul

MAIN STRt 6-LANEJ

en"

8

en"1 en" en"1

CO

en"

3

L

EXPLANATION

X FUG RO ELECTRIC CONE BORINGS

SECTION A

NAS, NORTH ISLAND

PARKING LOT

SCALE: 1"- 100'

ABC,- IBT^ GROUP

1 xxx ^1ASJ 1 AISLE 14

^^. 2AS ^ GROUP

' 2BT J 2XX -^

3AS"! AISLE 13w ^»? 3AS 1 GROUP

^ -3BT ? 3

. 4AT 1 GROUP0 <^L 4BS * AISLE 12 xxx J

! SIGN POSTS AISLE 11~i~

^--"-\ \PO8LH, WOKKS ___Ijnsiui-rES3¥-

y^rssEsr. TTsois-/64«H*OTRACfW*>

TOUCH M/aO STgie 628rszTrtrf

433TNAV,Y:EXCHANGE\ vL

\l^^1

IINO-NASNI- 10713/1 (REV 7-75 )DRAWN BY LEO H. GAUDREAU PW ENGINEERING (PLANNING)

REFERENCE NAVAL AIR STATION. NORTH ISLAND, CA 1975

PROJECT NO.:

USGS CPT-SPT

NORTH ISLAND SITE LAYOUT

9-80

79-153

FIGURE 2.4

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La Selva Beach'

' I ^ V -1 &"v M I ' " ^*sl^ 4 ,_._,._.._ -_ -, -*p V V . H >^^ -m-. .4-| <». ^r-w*»^ ft,

^^J^p^'^'^io; I" 1 v.^

shu MOSS LANDING

.gQSALINAail 5

Workfield

Point Pinos

IVIONTEREYPHKSIDIO OK

i ^ V-V^Sfe

'ST^C r>

FROM USGS 2° TOPOGRAPHIC MAP OF SANTA CRUZ, CA. 1965

9-80

PROJECT NO.:

USGS CPT-SPT

MOSS LANDING/SALINAS SITE LOCATIONS

79-153

FIGURE 2.7

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TO SAUNAS 3 MILES

FUGRO CONE SOUNDINGS

O BORINGST-TRIP HAMMER

S-STANDARD

5X ENLARGEMENT ADAPTED FROM USGS 15" TOPOGRAPHIC MAP

OFSALINAS. CA 1947

PROJECT NO.: 79-153

USGS CPT-SPT

SAUNAS SITE LAYOUT

9-80 FIGURE 2.8

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MOSS LANDING

MOSS LANDING

MARINE LABORATORY

PARKING LOT

MOSS LANDING

MARINE LAB

x FUGRO CONE SOUNDINGS

BORINGS CASTROVlLLE

MOSS LANDrMG

CEMETARY \

JSALINAS

12 MILESSALINAS RIVER STATE BEACH

EXIT

PROJECT NO.:

USGS CPT-SPT

MOSS LANDING SITE LAYOUT4X ENLARGEMENT ADAPTED FROM USGS 7%" TOPOGRAPHIC MAP

OF MOSS LANDING, CA 1954, PHOTOREVISED 1968

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oI o

I

COo

Io

I o

I

in o

i

FRICTION RBTI3

C8NE FRICTI8NRE3I3TRNCE RRTIdCTSH C%)

C8NE FRICTI8NRE3I3TRNCE RRTI8(TSF) (Z)

C8NE FRICT18NRESISTflNCE RRTI8(TSF) (Z)

C8NE RES18TRNCE (TSF)

.ac

2a

IXTURESSILT

SAND (SM-SP)

PROJECT NO.:

USGS CPT-SPT

MOSS LANDING SITE CRT PROFILE

9-80

79-153

FIGURE 2.12

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HUNTINGTON BEACI

FROM USGS 2° TOPOGRAPHIC MAP OF

LONG BEACH, CA 1957. REVISED 1970

PROJECT NO.: 79-153

USGS CPT-SPT

SUNSET BEACH SITE LOCATION

9-80 FIGURE 2.14

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FRICTI8N C8NE RHTI8 KESlSTflNCE (X) I CTSF)

0 100 ZOO

L MC818TIWCCI CTSf)

0 100 ZOO

RRTI0 ME818TRNCCCZ) I (T8F)

8 3 0 100 200

CLAY (CL) AND SANDY CLAY

-flJBWOPROJECT NO.: 79-153

USGS CPT-SPT

SUNSET BEACH SITE CRT PROFILE

9-80 FIGURE 2.16

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US Veteran^,, - AdmtrtetratiorK,'&

SEE FIGURECOYOTE CREEK NORTH

SEE FIGURECOYOTE CREEK SOUTH

*$>J X'^, M<^ ^

FROM USGS 2° TOPOGRAPHIC MAP OF SAN JOSE, CA. 1962, REVISED 1969

PROJECT NO.:

USGS CPT-SPT

SAN JOSE SITE LOCATIONS:COYOTE CREEK NORTH AND

COYOTE CREEK SOUTH9-80

79-153

FIGURE 2.17

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Co

mp

iled

by

Dra

wn b

y.

. Check

ed b

yA

ppro

ved b

y

^ *

> o

5

mm

^

3D

mo

5>

H

2 O

o «

_>

o'

coC

m

V)

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3

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5 >

vj

CO<0

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z > "

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~ 7fe"%~-^" 7^

~&.^_ j'^ j ;- <;Bj 1 ^otfjflgisjatiart^r

, 3 v_ "-I __ _ _._ ,T_ __^

' .If^^^L.']h , -I n'°oi ^.X li«N

-J - \ ' , i\--. i; ' " i ~ Wateit lowec': " I "f fraokfomi^^?N I " x f '" ' " I '"J ' *^^^ I

v f^nwV" 0!.

-^ T'J T-.rtI lLo..* 1 - ^P

'^^-^^^i-. ^-ito/^ * i L.' ~^ ,\ u

FROM USGS 2° TOPOGRAPHIC MAP OF

OKLAHOMA CITY. OK. 1957, LIMITED REVISION 1968

j-flJGflOPROJECT NO.: 79-153

USGS CPT-SPT

EDMOND, OKLAHOMA SITE LOCATION

9-80 FIGURE 2.23

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3-1

3. DATA ANALYSES

3.1 INTRODUCTION

Because the primary purpose of this research was to investigate

the correspondence between CPT and SPT, facilitating use of

CPT for liquefaction potential assessments, the investigations

were directed mainly at definition of the form of CPT-SPT cor­

respondence for soils in which the blowcount method of assessment

is applicable (sands with less than about 30 percent fines).

However, the correlations were examined for all natural soils

encountered. These soils ranged from medium sized clean sands,

to clayey fine sands possessing structural sensitivity. Only

occasionally were pure clays encountered. The reason for

examining these other soils is not only to allow prediction of

particular SPT values but, more importantly, to allow increased

certainty in the assessment of types of soils encountered

in-situ. That is, without being able to differentiate soil

types, it would never be clear when the CPT-SPT conversions

would be valid and, therefore, when the CPT use for simplified

liquefaction potential assessments would be valid.

The second requisite for use of the simplified method of

liquefaction potential evaluation is a means to normalize CPT

data in a manner eliminating the effect of overburden pressure.

Such normalization would be directly comparable to the blow-

count correction factor, C^, which is used to adjust a

blowcount to that expected for the soil if confined under an

effective overburden pressure of one ton per square foot. The

blowcount correction factor, CN , or its equivalent for CPT

~FUGRH

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3-2

measurements, Cp, is a function of effective overburden

pressure and, therefore, soil unit density and location of

phreatic surface must be determined or reliably estimated.

Finally, the relation between CPT end bearing, qc , and

SPT blowcount, N, must be determinable from CPT measurements

alone. Although a more satisfying approach to the estimation

of liquefaction potential from CPT measurements would be

through some strength or compressibility related factor, it

is currently necessary to use the already-existing blowcount

relation. Although such correlation may not be satisfactory

for site-specific liquefaction potential assessments for

critical structures, certainly the method is applicable to

regional zonation or site specific screening to the extent of

defining the existence or lack of a problem requiring more

detailed site investigation.

Because the SPT is so widespread in U.S. application, and

because the SPT is recognized as an uncertain measurement,

several researchers have investigated the test, from equipment

and procedures to theory and usage. Likewise, the relation

between SPT and CPT has been investigated, and the CPT alone

has been the subject of controlled studies. It is informative

to review some of those studies.

3.2 PREVIOUS INVESTIGATIONS

3.2.1 SPT Research

When investigating use of an in-situ tool the greatest need is

to establish a reference against which the measurements made

fijGRO

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3-3

with the tool may be evaluated. For investigation in sands

the most common reference is the SPT. Thus, not only the CPT

and CPT-SPT correlations need be studied, but also the SPT

alone.

The question of repeatability of the SPT as a result of natural

in-situ spatial variability of soil properties or vagaries of

equipment and procedure has been discussed at length by several

authors (de Mello, 1971; Tavenas, 1971; Fletcher, 1965; Schmert-

mann, 1976; Kovacs, 1978). The message contained in these works

is that although the SPT is beset with equipment and procedural

difficulties, the test does provide useful information. Some

20 potential error sources are mentioned, and some results are

cited showing up to a j^lOO percent error in SPT measurements

under controlled conditions. Such errors tend to be largest at

shallow depths. When such lack of repeatability is compounded

by the use of different hammer energies (Kovacs, 1978; Schmert-

mann, 1976), and different CN adjustments for depth (effective

overburden), it is clear that use of any particular set of N

values with the Seed blowcount method requires considerable

caution. For example, Kovacs notes that the combinations of

rope age, sheave speed, and driller effort also significantly

affect the hammer-delivered energy, while Schmertmann (1976)

shows that average energies delivered to the sampler by the

common rope-around-the-cathead method are about 55 percent of

the theoretical amount and that the actual energy entering the

rods depends not only upon the hammer system but also the rod

type and length.

IGRD

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3-4

Following this question of the effect of rod length, and hence,

depth, upon entering and delivered energy is of interest in

that the CPT measurements should depend upon effective overburden

pressure but not upon rod length. Several researchers have

examined the N- effective pressure relation (CN ) proposed

by Gibbs and Holtz (1957) and have presented modifications.

Notable among these are Bazarra (1967), Seed (1976), Peck, et

al (1973), and Marcuson and Bieganousky (1977). These authors

have identified soil type, relative density, and overburden and

lateral pressure as the primary variables influencing blowcount,

although other variables such as soil structure have been

considered. In Figure 3.1, a plot is shown comparing the CN:

relations suggested by these authors. The wide range in values

at any pressure precludes certainty in selection of an appropriate

N value correction factor. Further, it is of interest that the

curves presented by Marcusson and Bieganousky developed using a

free fall hammer with laboratory sands show reasonable agreement

with those developed empirically. The Marcuson-Bieganousky

studies did not include rod length as a control variable, yet

Schmertmann (1976) showed rod length to have a significant

effect upon hammer-rod system efficiency and, presumably, upon

blowcount. In Figures 3.2(A) through 3.2(D) a progression is

shown based upon the Schmertmann (1976) data whereby rod length

is related through energy measurements to N values. The final

figure, 3.2(D) shows a CN curve for rod length alone (CRL)

in which it is noted that because of the lesser delivered

energies at shallow depths, the blowcounts must be adjusted

IGRO

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3-5

downward rather than upward as is the usual case for CN

adjustments. It should also be noted that some research

appears to disagree with the Schmertmann data (Steiger, 1980),

and that perhaps the apparent rod length effects are primarily

inertial and may be cancelled by other losses such as stress

wave attenuation or joint energy losses. In summary, it is

found that the overburden correction factor depends upon more

factors than effective overburden pressure, and that published

values of CN factors constitute a range precluding precision.

3.2.2 CPT Research

The two primary factors relating to CPT measurements that are

of concern to this study are the influence of soil type and

overburden pressure upon the CPT measurements.

3.2.2.1 CPT versus Soil Type

The CPT provides two distinct indicators of soil type: the end

bearing record (qc ) and the ratio of side friction to end

bearing expressed as a percentage (friction ratio). Prior to

development of friction cones, the end bearing record alone was

used to identify soil types: high readings indicated sands and

low readings, clays. In addition, the variation of the curve

provided information about soil type and layering. However,

the ability to predict soil types was greatly increased with

the development of the Begemann (1964) friction cone penetrometer

Data compiled by Begemann formed the basis of the soil differ­

entiation charts shown in Figure 3.3. In Figure 3.4 is a com­

posite of the classification and blowcount versus CPT relations

ICRO

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3-6

developed by Schmertmann following Begemann and modified by

data measured in Florida.

Schmertmann (1978) notes that his chart is appropriate primarily

for the mechanical friction cone and that local correlations

are preferable. Further, he notes that structural sensitivity

can produce values not corresponding with the presented delinea­

tions, and that friction ratios are undependable at low values

of end bearing.

Alperstein and Leifer (1976) present data in general agreement

with the Begemann-Schmertmann relations, again developed with

the mechanical friction cone. Campanella, et al, (1979) also

show general agreement with those classification guidelines.

It should be noted that disagreement should be encountered

when comparing data measured with the electric friction cone

penetrometer to the mechanical cone penetrometer classifica­

tion chart. Several factors contribute to such disagreement.

First, the mechanical cone is not continuously penetrated;

rather, the tip is advanced and then the sleeve is advanced.

Second, the mechanical friction sleeve has a beveled leading

edge which adds some contribution from end bearing to the

measured sleeve values. Although it is widely recognized that

the Schmertmann-Begemann chart is not entirely appropriate for

use with the electric cone, no applicable charts or recognized

relations exist, and so, the -mechanical-cone-based chart is

usually used.

ICRO

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3-7

Because the CPT is essentially dependent upon strength and

compressibility of a given soil, information about soil type

is only indirectly known. Soil type is inferred based upon

the two different measurements provided by the electric CPT,

and upon the relation between these measurements. The usual

comparatives are end bearing and friction ratio, equal to ratio

of sleeve resistance to end resistance. To understand the

classification of soils using these factors, the measurements

themselves must be fully understood.

The cone resistance increases in value for sands and gravel

with increasing values of friction angle, in-situ relative

density, or overburden and lateral stress. The relative

density depends primarily upon stress history and method of

deposition while friction angle depends upon mineral type,

particle size and distribution, and relative density. Further,

cone resistance in sands increases approximately as an exponen­

tial function of the friction angle. Although the sleeve

friction depends upon the same factors, its resistance increases

roughly as a linear function of the friction angle. Therefore,

the friction ratio for sands should decrease with increased

values of friction angle.

The cone resistance in clays is dependent on the clay type,

in-situ strength, overburden stress and stress history. The

sleeve resistance is dependent on the same items as the cone

with special importance on the in-situ lateral stress (Ko, which

depends on the stress history, soil type and soil activity,)

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3-8

and sensitivity. The resistance of the cone and sleeve are

both generally related to a linear function of soil strength

and should, therefore, show an essentially constant friction

ratio with increasing strength.

Further complicating the understanding of penetration resis­

tances is the existence of the so called limiting depth, and

the controversy regarding basic failure mechanisms as evidenced

by the use of both bearing capacity and cavity expansion

theories. In addition, cone and sleeve measurements in soil

types such as silts, clayey silts, sandy silts, sandy clays,

and silty clays are even harder to understand because of the

number of variables acting simultaneously. For example, the

intergranular soil matrix in sands has a large effect upon the

behavior of the cone and sleeve. Depending on the condition of

the soil matrix and gradation of the coarse fraction, several

conditions can occur, including dilation, structural breakdown,

pore water pressure generation, transmission of penetration

resistance from sand structure to soil matrix, and grain

crushing.

During penetration of the cone, soil in a zone extending

several cone diameters in front of the tip experience com-

pressive stresses resulting in some pore pressure generation

depending on soil permeability and the speed of cone advance­

ment. Soil closer to the front of the cone experiences high

shear strains as it is translated from in front of the cone

to the side of the shaft. Such large deformations result in

IGRO

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3-9

rearrangement of the near-field soil structure. If the soil

structure was initally loose and of high permeability, a denser

zone develops in front of the tip. This zone then carries

greater stresses until finally the zone fails and the cone

resistance drops to the lower values indicative of the underly­

ing non-densif ied soil, and the process begins anew.

Most of these questions of mixed soil-penetrometer interaction

have been avoided, with research being directed at understand­

ing of behavior of purer soils (Levadoux and Baligh, 1980;

Mitchell and Lunne, 1978; Yong and Chen, 1976; Janbu and

Senneset, 1974). Such research has resulted in clearer under­

standing of the penetration mechanics, particularly with respect

to end bearing behavior. What is notably lacking is research

into the significance and interpretation of side friction.

3.2.2.2 CPT versus Overburden Pressure

Little information is available quantifying the effect of

increased overburden upon CPT results. What little information

is available relates primarily to end bearing, and the constancy

of friction ratio with increasing overburden is assumed (Schmert-

mann, 1976) . Treadwell (1975) examined the effect of gravity

(or force) upon the CPT penetration including evaluation of the

work of Vesic, while Schmertmann (1976) empirically found a set

of summary curves of qc versus overburden pressure for normally

consolidated, recent, SP sands. By normalizing his curves

(qc at 1 tsf divided by qc at any pressure) a Cp curve is

obtained. This curve is shown in Figure 3.5, where it can be

compared to the more common CN curves shown in Figure 3.1.

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From examination of Figures 3.1 and 3.5, it can be noted that

the Cp relation is within the band of CN relations presented

previously. However, assuming that the CN curve does include

the effect of rod length as well as pressure, the final curve

of Figure 3.2 relating rod length to CN (CRL) can be used to

adjust the Seed et al. (1976) CN relation. The resultant

quotient of these two curves is shown in Figure 3.6 where it is

noted that, perhaps coincidentally, good agreement is obtained

with the Cp developed from the work of Schmertmann. Such

comparisons are of interest, but do not serve to adjust any

actual CN curves , as the effects of relative density and

soil type are certainly larger than that of rod length. At*

this time no quantitative data appears available describing

the effects of soil type, density and stress conditions upon

the Cp appropriate for use with CPT measurements.

3.2.2.3 CPT Versus SPT

Penetrometers of numerous varieties have been used and correla­

tion between the types studied (Sangerlat, 1972; Sangerlat,

1974). An early compilation of research results was provided

by de Mello (1971) and is presented in Figure 3.7. A summary

provided by Sangerlat (1972) is shown in Figure 3.8. Alperstein

and Leifer compiled and extended existing comparative data as

shown in Table 3.1. The comparisons found by Campanella, et

al. (1979) are shown added to those of Table 3.1. It should be

noted that many of these tabulations are based upon mechanical

CPT results and that indicated soil types are often defined by

visual classfication only.

ICRO

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TABLE 3.1

SUMMARY OF REPORTED qc/N VALUES (from Campanella, et al., 1979)

3-11

Campanella, Alperstein LaCroix Soil Type et al. and Leifer Schmertmann Simons and Horn

Micaceous silty coarse to fine sand, some clay

0-1.5 10 4-6

Micaceous fine sand, trace to some silt

1.5-3.5 5.5 3-4 4-6

Coarse to fine sand, trace to some gravel

3.5-7.0 5-6 4-6

The summation of these results shows that the ratio of qc to

N (for constant equipment and procedures) increases when moving

from plastic (ductile) to nonplastic materials and with grain

size in the latter case. Further, the above-mentioned authors

all note that the q c/N values are not universal and depend

upon site specific characteristics. How much of this range

results from variability in the SPT and how much from soil con­

ditions is not known. Further, the mechanical CPT data usually

provides only an average soil resistance over about six inches,

while the electric CPT provides point data representing some

weighted influence of a few inches of soil ahead and behind the

cone. None of the available research defines whether or not

the data was averaged.

IGRO

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The most complete summary of factors affecting the qc-N com­

parisons is given by Schmertmann (1976) in which theoretical

considerations of penetration energy are used to relate the

components of penetration resistances for the different tests.

Through consideration of the role of side and tip resistance

in penetration through any soil, an equation relating the

components of resistance was developed (Schmertmann, 1971):

N = (A+B*FR%)*qc

where N equals SPT blowcount, A and B are constants, FR is

friction ratio, and qc is end bearing in tsf. The equation

can be converted to:

qc/N = n = 1/(A+B*FR%),

in which the dependence of the ratio qc/N on friction ratio

is clearly seen. A further modification proposed by Schmert­

mann (1976) gives:

qc = N a/(A+B*FR%),

in which form nonlinearity is incorporated to better fit data

obtained in low resistance soils. Schmertmann gives values

for the various parameters as follows: a=4/3, A=0.641, B=0.224

for the case of fifty percent of the theoretical energy avail­

able in the SPT. A set of curves showing these relations is

given in Figure 3.63 of a later section. The curves are also

shown, in different form, as contours of constant N value in

Figure 3.4.

ICRO

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The brief preceding discussion is not intended to represent a

thorough review of the state-of-the-art of static and dynamic

penetration. The discussion is designed to illustrate what

specific CPT-SPT research has been performed. Further informa­

tion can be found in the 1976 Schmertmann reference. This

reference provides the most complete examination of the q c-N

relations available, and provides theoretical as well as

empirical examinations. Further, some information is available

regarding the relative influences of side friction and end

bearing of the CPT and SPT on the measured results. This is of

great importance in any but the most uniform, artificial soil

deposits. This importance can be seen when examining what is

actually occurring in each test. The SPT sampler is driven six

inches into the soil. The blows required for the next twelve

inches of penetration are the recorded blowcount. At the start

of the final twelve inches of penetration, the sampler is

already subjected to six inches of side friction. By the end

of the test, eighteen inches of side friction are resisting

sampler penetration. The electric CPT on the other hand, has

a constant area throughout the penetration. The situation is

further complicated when the zone of measurement passes through

a change in soil type or resistance. In such case a weighting

of the CPT resistances would probably result in better compari­

son with the automatic weighting that occurs naturally during

the SPT. It appears that only little research has been directed

at such non-uniform conditions, although such conditions are

invariably the rule rather than the exception in-situ.

IGRO

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3.3 CURRENT INVESTIGATIONS

The following sections provide examination of all of the data

measured during this investigation. The data is subdivided

into three sections: CPT Classification of Soil Type; Correc­

tion of CPT Measurements for Overburden Pressure; and Correla­

tion of qc to N.

3.3.1 CPT Classification of Soil Type

The sites selected for investigation were primarily sand sites.

Further, only a limited number of samples were obtained when

clayey layers were encountered. For these reasons, the classi­

fication data described in the following sections is heavily

weighted toward definition of saturated sand zones by use of

the CPT measurements. As mentioned previously, the CPT provides

two measurements, both of which are predominantly influenced by

soil strength and compressibility. Research has shown strength

of soils dependent upon density or relative density, stress

level, soil structure, grain size shape and distribution, and

physico-chemical characteristics. As combinations of these

numerous variables exist in-situ, and because such combinations

may vary rapidly,, strength-based classifications may not always

agree with other classifications such as those of the Unified

Soil Classification System (USCS). However, soil classifica­

tion is usually used as an index to define potential problems

and their magnitude. These goals of soil classification

are to large degree determinable by the CPT method.

TUGRO

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The program of CPT soil type (or, more appropriately, soil-

behavior type) classification was based, in large part, upon

idealization of the profiles encountered in-s-itu. After

preliminary idealization was complete, laboratory grain size

analyses were performed upon select representative samples.

During this phase two factors became apparent. First, the

boring logs represent an oversimplified view of in-situ condi­

tions and, second, the classification names are not necessarily

good indicators of soil behavior. For example, a sand with

95 percent of the material lying between the number 100 and

200 sieve sizes is classified as a SP, while a sand having

95 percent of the material just finer than the number 200 sieve

is classified ML.

Certainly the behavior of these two materials would not be

expected to greatly differ. Further, a mixture of 45 percent

sand, 45 percent silt (or sand finer than the number 200 sieve),

and 10 percent of an active clay is classified as CL, while a

soil having 60 percent material in the clay size range with

low Activity is also classified as CL. For this case, it is

expected that significant differences in behavior should occur.

Three different approaches were used to examine the effect of

changing material type upon the CPT measurements. First, all

SPT samples were classified, either in the laboratory or

visually with reference to adjacent samples that had been

classified in the laboratory. The laboratory classifications

have been compiled in the boring logs shown in Appendix A.

ICRO

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Next, the CPT end bearing and friction ratio from an adjacent

sounding were averaged over the length of the SPT sample. The

points were then plotted, as shown in Figure 3.9. In that

figure some attempt was made to divide the most troublesome

classification, SM, into two groups: SM, having fines content

between 12 and 30 percent, and SM-ML having fines content

between 30 and 60 percent. Examination of the data in Figure

3.9 shows some fairly well defined zones of differing soil

types. It should be recalled that anomalous points may easily

result from spatial variability in-situ, or from the presence

of an interface which would significantly affect the CPT

measurements but may not be reflected in the retrieved sample.

Another method of comparison involved calculation of average

properties and CPT measurements by zone within more or less

well defined layers. This approach was selected to define

trends in data, not the boundaries between soil types. As the

averaging was also used for estimation of the qc/N relation,

those plots are shown in a later section. However, it may be

seen that the indicated soil classification trends fall within

the boundaries shown in Figure 3.9.

Because of the rapid variation in CPT measurements in-situ,

some investigations of measurement variance were performed

to facilitate selection of comparison points in well defined

zones. Variance can be shown by plotting a continuous CPT

sounding on the q c-FR plot. A typical plot of this type

is shown in Figure 3.10. The numbers on the sounding trace

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3-17

represent depth in feet. By examination of the boring logs

for depths at which the CPT trace stays in a small zone of the

qc-FR plot, soil classification information can be attached

to those qc-FR zones. Examples of classification by these

zones are shown in Figures 3.11 and 3.12. Again, these zones

compare well with the boundaries shown in Figure 3.9. To

define the complete boundaries of different soil types using

the continuous trace-zone method, several large layers of

different uniform soils at different densities and pressures

would have to be encountered. At present, no such collection

of data is available.

A modification of the continuous trace method is to have the

continuous record traced on the qc-FR plots only over depths

at which a sample was obtained. The behavior of the soil

during CPT penetration is then immediately apparent. An

example of this method is shown in Figure 3.13. In that figure

it can be seen that some depths tend to have CPT measurements

staying in a small zone of the q c-FR plot, while other SPT

depths show extreme changes in CPT. The logic is that compar­

ison of points in which the CPT is radically varying will be

futile. An average value calculated for a limited trace

ranging from sand to clay zones would show some intermediate

classification, such as sandy clay. If, for example, the

Schmertmann (1976) method of computing an equivalent CPT side

friction and end bearing from incremental measurements of the

SPT penetration was used with resultant similarity in behavior

to the CPT trace, then neglecting the differences between

ICRD

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static and dynamic behavior would allow comparison of the two

measurements.

The approach used in the limited trace method was to select for

comparison only SPT values where the adjacent CPT measurement

stayed within a small zone. The implicit assumption is that

the SPT measurement would show similar constancy if treated

using the incremental method. As with the layer-average method,

the data from the limited-trace method is also used in compari­

son of the qc/N ratio and, therefore, data plots are presented

in subsquent sections. Review of that data does show agreement

with the zones and boundaries shown in Figure 3.9.

As an extension of the classification data already presented,

some select data obtained from the Edmond, Oklahoma site is

presented. The reason for presentation of select data only

is the heterogeneity of the site. Initial attempts at pro­

filing of the site showed only the most generalized layers:

from zero to about twenty feet are sandy clays, from twenty

to about 60 feet are mixed soils (clay, silt, sand in varying

percentages), and from 60 to about 80 feet is relatively clean

sand with occasional lenses or stringers of sandy or clayey

silt.

However, at any particular depth, a soil encountered in one

boring or sounding may not be encountered in a second boring

or sounding at the same depth at a distance of only a few

horizontal feet. Even when the same soils are encountered,

the penetration resistances are often quite different.

ICRO

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The CPT sounding logs usually evidenced the most disagreement

with boring logs in the twenty to sixty foot depth zone. The

most common material in which traditional CPT classification

differed from the boring logs was a soil mixture consisting of

about sixty to seventy percent fines with ten to twenty percent

being clay-sized particles with a PI of about four to fifteen.

Further examination of the CPT logs in these soils showed uniformly

low friction ratios (one-half to one percent) with the smooth

end bearing usually associated with plastic soils. It was noted

that the soils typically had water contents close to the measured

liquid limits, thus having a Liquidity Index (water content -

Plastic Limit divided by Plasticity Index) close to unity.

A plot of the Liquidity Index of these CL-ML and CL soils is

shown against measured q c and FR in Figure 3.14. It can be

noted that the apparent trend is for increasing Liquidity Index

with decreasing cone side friction or, with decreasing end

bearing and friction ratio. This fact is particularly impor­

tant when recalling that friction ratios this low are generally

associated with clean sands. Also of interest is the location

of the boundary of the zone in which these soils having measur­

able Liquidity Index exist. A sand, not having a PI, has an

undefined Liquidity Index. The boundary of soils found to have

a Liquidity Index is very similar to the SM to SM-ML boundary

shown in Figure 3.9.

Examination of the data in Figures 3.9 through 3.14 shows that

general trends in soil type classification using the CPT method

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seem to follow lines of constant side friction as well as of

end bearing and friction ratio. That is, soils with a high

specific volume (volume per unit mass) (clays) occupy the zone

of high friction ratio, with increased overburden stresses

(or depth) resulting in higher side friction and slightly

increased friction ratio. Intermediate specific volume soils

occupy the range between the clay zone and the sand zone, again

with increasing side friction and friction ratio resulting from

increased overburden stress. In this zone anomalous behavior

can result because of the different compressibilities of the

coarse and fine fractions. For soils in which the sand content

is high enough (40 percent?) to form a continual interlocked

structure, the application of overburden stress results in

essentially sand-like compression of the structure, leaving

the interstitial clay fraction in an psuedo-underconsolidated

state. The application of large amplitude undrained shear

strains collapses the sand skeleton, with resultant increase

in pore pressure response and decrease in effective stresses,

particularly with respect to the friction sleeve. This behavior

causes the reduction in friction ratio observed for soundings

in a given material as Liquidity Index increases. This use of

Liquidity Index is as a measure of soil structural sensitivity.

Sensitivity in clays is known to reduce friction ratios (Schmer-

tmann, 1978). As lines of constant side friction are followed

into zones of higher end bearing, sands of decreasing relative

density are encountered, again with increasing overburden

causing increasing side friction. A summary of these expected

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trends is given in Figure 3.15. It should be emphasized that

these trends are hypothesized on the basis of limited amounts

of data, and do not rigorously account for the effect of inter­

action, of all the shown variables.

3.3.2 Correction of CPT Measurements for Overburden Pressure

Comparison of CPT data with other CPT or SPT data requires some

normalization to account for the effect of overburden stress on

the measurements. Current methods of adjusting SPT blowcounts

make use of the CN factor. This factor is the subject of

continuing research and, at present, is only poorly defined

(that is, a wide range of values have been proposed as appro­

priate at any particular pressure). Because it is intended to

relate CPT to SPT, a possible approach is to convert CPT to

the corrected SPT value: N^ = N C^j. The use of a particular

CN relation to adjust CPT data would be appropriate if the

relation of qc to N was constant with increasing overburden.

In the next section it is shown that the relation is not

constant and, therefore, a different correction must be used.

Examining the range of CN shown in Figure 3.1 reveals that

CN uncertainty precludes certainty in prediction of the CPT

correction factor, Cp . Although it is known that relative

density, soil type, stress history, and structural anisotropy

and sensitivity all affect such corrections, the appropriate

weighting to account for each variable is not known.

Three methods were selected for examination of the Cp rela­

tion with increasing overburden. The simplest was simply a

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modification of the existing CN curves by quantitative removal

of the influence of rod length. This has been discussed previously

The second approach was to select a site of constant material

type with constant depositional history, thus leaving effective

overburden pressure as the only variable. The third approach

was to correct all N values to the 1 tsf overburden using a

standard CN relation, and to then divide each corrected blow-

count by the uncorrected CPT end bearing, resulting in the

parameter needed to equate qc and N^. This parameter (Cp i) is

equal to an overburden correction to CPT readings (Cp ) divided

by a constant q c/N relation.

Three sites were selected as being most appropriate for examina­

tion of the Cp relations: the San Diego Site at North Island,

the Salinas site, and the Sunset Beach site. Although all of

these sites are of essentially constant material type, examina­

tion of the CPT records (Appendix A) shows lack of uniformity of

penetration resistance. However, by comparison of select points

an indication of the implicit in-situ Cp behavior is evidenced.

In Figure 3.16 plots are shown of the q c-effective overburden

pressure relation proposed by Schmertmann (1976) as well as

those developed by Treadwell (1975) and Vesic (1972). Super­

imposed on that plot are the average relations found at the

Sunset Beach, Salinas and San Diego sites. It is seen that

no relation of the type found by other researchers completely

fits the in-situ measurements. The data in Figure 3.16 suggests

that either Relative Density is constantly changing, or that

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the material type is constantly changing. In either case,

it appears that none of the investigated sites had complete

uniformity of soil type and/or density. The normalization of

the curves shown in Figure 3.16 by the value of end bearing

at an effective overburden pressure of 1 tsf produces a Cp

curve differing from that presented by Schmertmann, as would

be expected if Relative Density is constantly changing.

The next method of Cp investigation is based upon the concept

that the qc/N relation is a function of confining stress.

This variance in qc/N is discussed more fully in subsequent

sections. At this point the variance is assumed and a factor

to account for such variance is advanced. If C p were equal

to CN , then qc/N would be constant for constant soil conditions

The appropriate relation is:

N*CN = (qc *cp)/n

where C^ r n, and Cp are all functions of confining stress.

Carrying the relation one step further allows definition of

an equivalent Cpi by which an equivalent N^ may be estimated:

N*CN = NX = qc *Cp/n = qc C pl , or

where Cp ^ = C p/n

In Figures 3.17 and 3.18, plots are shown of N^/qc where q c

is the average end bearing measured over the one-foot depth

interval at which the blowcount was recorded in an adjacent

~RjGRH

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boring. Likewise, the friction ratios shown in those figures

are the average over the one-foot interval. The trend lines

shown in the figures represent the behavior of material with an

average friction ratio less than 2.0 percent (essentially sandy

soils). The scatter in Cp^ with pressure is a probable result

of the variation in relative density at constant pressure, as

was seen in Fig. 3.16.

It is of interest to note that although the trend of the

relation based upon the trip-hammer measurements is similar

to that of the standard hammer, the scatter seems greatly

diminished, a result possibly caused by the inherent "smoothing"

of variable resistance layers when using the higher energy trip

hammer. As the hammer total weights are similar, as were rate

of application of blows, inertial effects or pore pressure

effects were discarded as causative factors.

In hopes of reducing the data scatter, two variants of the

above method were included: the use of average end bearing

and N values selected from well defined layers only, and the

use of points selected on the basis of uniformity of CPT record

as described previously. The results of these investigations

are shown in Figures 3.19 through 3.22. The indicated trends

reveal the increased scatter using the standard hammer, but

also reveal the constancy of the trend regardless of method

used. The trip hammer curves also show the similarity of trend

regardless of method. In addition, the trip hammer curves are

relatively well defined. The comparison of the C^ relation

IGRQ

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to Cp needs estimation of the trend of qc/N with increasing

overburden. Thus, such comparisons are relegated to a subse­

quent section.

The practical significance of the data scatter is small when

compared against the scatter that normally results from the

spatial variability of soil type and relative density in-situ.

With such consideration, it is clear that selection of an

overburden correction factor, C p or CN , must invariably

produce only a rough estimate of the actual normalization

factor appropriate for any particular soil.

3.3.3 Correlation of qc to N

The precise correlation of CPT end bearing to SPT blowcount

requires that measurements be performed under similar condi­

tions of soil type, stress state, density and fabric, and

particle size, shape, and distribution. Most of these simi­

larities will only generally be found in an in-situ comparative

program. For example, Tavenas (1971) shows the range of N

values obtained at single, supposedly uniform site using a

single crew with equipment and procedure carefully controlled.

His explanation for the N value scatter is advanced denying

the repeatability of the test under even ideal conditions,

an explanation which ignores the natural spatial variability

of penetration resistance in even the most uniform of sites.

Review of the CPT logs of Appendix A further reveals this

natural variability, for the CPT is a carefully controlled test

in which equipment, crew, and procedure have been eliminated as

error sources.

"~ GRO

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In fact, the careful elimination of error sources has provided

even more proof of spatial variability in-situ. Any of the

sounding logs presented in Appendix A reveal the presence of

pockets or lenses of dissimilar materials within supposedly

homogeneous layers. This heterogeneity is particularly evident

when examining the sounding traces on the soil classification

chart as presented in Section 3.2.2.1. Further, such inter-

layering can produce arching stresses resulting in non-uniformity

of vertical stresses. As any penetration measurement is depen­

dent upon soil type, density, and overburden stress, as well

as stress history and age of the deposit, it is difficult to

isolate the effect of a change in any single variable in-situ.

Several methods of data presentation are used in the qc/N

comparisons in order to well define the trends with changes

in different variables. The range in qc/N possible within

any layer at a site was first examined. Next were comparisons

of all measured N values with corresponding CPT measurements

at the same depths in adjacent soundings . Average values of

N and qc by layer were compared and, finally, the comparisons

were made for select depths at which the end bearing and fric­

tion ratio trace showed constant soil conditions. Using each

method, several variables are isolated: qc/N versus friction

ratio; qc/N versus N; qc/N versus q c ; and q c /N versus depth.

3.3.3.1 qc/N Range Comparisons

With a goal of using the CPT for the equivalent blowcount

method of liquefaction potential assessment, it is informative

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to examine the range in qc/N that could possibly be encoun­

tered at any site. The blowcount method is not a continuous

test in that samples are usually taken at a maximum frequency

of 3.0 feet and the results represent a weighted average of

between 18 and 12 inches of soil resistance. Thus any particular

horizontal and vertical location within a site boundary selected

for testing can have a significantly different resistance than

any other area selected.

The procedure used to investigate this range was to divide the

profile into three foot thick layers and to tabulate the upper

and lower bound of all SPT and CPT measurements made in each

layer. By comparison of the maximum CPT with the minimum SPT a

maximum qc/N is obtained. Likewise, the minimum CPT and maxi­

mum SPT gives the minimum possible qc/N. Comparison of maximum

CPT with maximum SPT, and minimum SPT with minimum CPT bound the

probable range. "Probable" is based upon the assumption that

the most significant resistance variations within any horizontal

layer occur at the widest horizontal separation of measurements,

and that site investigations using either method will probably

have similar horizontal distribution of measurements.

The results of these range comparisons are shown in Figs. 3.23

through 3.26 and 3.27 through 3.30 for standard hammer and

trip hammer measurements, respectively. Also shown in those

figures are the soil layers that show continuity of depth

and general material type across the entire site. However, it

should be noted that the layers do include a range of materials

within a general soil classification such as sand or clay.

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It can be seen in Figs. 3.23 through 3.30 that the probable

range for sandy soils using the standard hammer is about 2 to 5

and about 3 to 10 for the trip hammer. This large range for

the trip hammer is surprising in that it would be expected that

because sampling energy is more controlled, the comparisons

would show reduced scatter. However, in this program the

standard hammer measurements were also carefully controlled

with respect to drop height, frequency, rod inclination and

rope obstruction. Composite plots of all blowcounts measured

with each hammer at each site are shown in Figs. 3.31 through

3.35 where the greater variability of the standard hammer

measurements is apparent. Further, examination of the average

blowcount versus depth profiles of Section 2.4 reveals that

the standard hammer profiles show better general agreement with

the CPT profiles than do the trip hammer profiles. The higher

energy of the trip hammer appears to extend the zone of influence

in front of the sampler as compared to the lower energy standard

hammer. This would result in an averaging of thin variations

in penetration resistance. Such an averaging would be much

less pronounced for the CPT measurements, producing the wider

qc/N range for the trip hammer comparisons.

3.3.3.2 qc/N Versus Depth

Examination of the ranges in qc/N versus depth (or effective

overburden pressure) presented in the preceding section indi­

cates the need for further refinement. As a first step in such

refinement, the comparisons were performed for average measure­

ments within each layer identified as continuous. Thus, if a

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3-29

layer was dipping in cross section, the averaging procedure

would exclude those zones bounded by the dipping-layer interface.

Figures B.I through B.4 of Appendix B show qc/N versus depth

for each site, and Figure 3.36 presents a composite of all such

data. Again the standard hammer qualitatively shows less scatter

than the trip, and it is apparent that the qc/N ratio tends

to decrease with depth for constant friction ratio materials.

Examination of the behavior of friction ratio with increasing

depth for constant grain size and distribution materials shows

slight increases with depth. However, such an effect is small

for constant materials, and does not appear to be the cause of

the reduction in q c/N with depth (or more appropriately, with

increasing effective overburden pressure). The scatter in

values is not particularly well tracked by the friction ratio;

however, recall that horizontal and vertical averaging was used

within each layer and that the resultant average friction

ratios probably are not weighted in a manner equivalent to the

averaging of the N values.

It is of interest to compare the q c /N versus depth relation

with that predicted by the Schmertmann relations. In Figure

3.37 the effect of increasing effective overburden pressure

on the qc /N ratio is shown for soils having friction ratios

indicative of sands for which Relative Density is an appro­

priate parameter. These data are drawn from a variety of

measurements and, therefore, the portrayed behavior should

be regarded qualitatively. It is seen that in all cases the

ICRO

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qc/N relation rapidly increases with increasing pressure,

a trend not supported by the data measured in this program.

Examination of the effect of increasing overburden on qc/N

may also be through comparison of qc/N versus depth plots for

all blowcount measurements. Such an approach will, of course,

produce significant scatter because of the inherent spatial

nonhomogeneity of natural soils. However, trends should be

apparent. In Figures B.5 through B.8 are shown the comparisons

for the standard hammer measurements, and in Figures B.9

through B.12 for the trip hammer measurements. Examination

of those figures reveals the same trends as noted previously:

the qc/N ratio decreases with increasing depth.

Finally, the effect of overburden on the qc/N ratio can be

through examination of the behavior evidenced by points selected

on the basis of the uniformity of the CPT record over the blow-

count depth interval. This approach depends completely on the

assumption of horizontal uniformity of soil type and resistance.

The criteria by which uniformity of CPT measurement is defined

has been described in Section 3.3.2.

The composite plots of qc/N versus depth for select points

from all sites are shown in Figs. 3.38 and 3.39 for standard

and trip hammer measurements, respectively. It can be seen

that as in the other plots, the q c/N ratio decreases with

depth and, therefore, with increasing effective overburden

pressure. The decrease seems to hold for all materials (as

represented by constant friction ratio) and, again, trends

CRD

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are better defined for the standard hammer than for the trip

hammer.

In summary, it has been shown by a variety of comparisons that

the q c/N ratio decreases with depth, and that the tendency

for increasing friction ratio with depth is not large enough

to account for such decreases. This observation is directly

contrary to the relations suggested by Schmertmann (1976).

However, as discussed in subsequent sections, there are equip­

ment differences that may account for such discrepancies

between the Schmertmann data and the data presented herein.

3.3.3.3 qc/N versus N

As described in preceding sections, the influence of the N

value upon the qc/N ratio was investigated through examina­

tions of layer average values, of all individual measurements,

and of select points. Figures B.13 through B.16 of Appendix B

show the layer average data from each site, and Figure 3.40

shows the composite of all such comparisons. Also shown in

Figure 3.40 is the apparent qualitative trend line through the

data, showing a decrease in q c/N with increasing N.

The presentation of all individual measurements of qc/N

versus N is in Figures B.17 through B.20 and B. 21 through

B.24 for standard and trip hammer, respectively, for each site

and the data is summarized in Figure 3.41 for standard hammer

measurements and Figure 3.42 for trip hammer measurements.

Again the trend line is shown and it is apparent that the

standard hammer comparisons show less scatter than do the trip

ICRQ

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hammer results for the same reasons as discussed previously,

and that the qc/N ratio decreases for sands with increas­

ing blowcount.

Finally, the results of the qc/N versus N comparisons for all

sites using select CPT measurements are presented in Figs. 3.43

and 3.44 for standard and trip hammer measurements respectively,

Again, the trend lines are indicated in the figures, and show

generally decreasing ratios with increasing N value.

In summary, the qualitative trends show consistent disagreement

with the Schmertmann (1976) relations in which qc/N increases

with increasing N value. The disagreement between the data

presented herein and the Schmertmann data is expected based

upon the disagreement in trend of qc/N with depth as noted in

the previous section. The correspondence of increasing N with

increasing depth forces such concurrence. However, by exam­

ining the relation as dependent upon different variables, more

certainty is obtained that the trends are not just coincidental

to any one set of comparisons. Again, a reason for such

disagreement is advanced in the following section.

3.3.3.4 qc/N versus qc

The results of the same set of comparative measurements as used

previously but applied to qc/N versus qc are shown for layer

averages in Figures B.25 through B.28 and summarized in Figure

3.45; for all individual measurements in Figures B.29 through

B.36 and summarized in Figures 3.46 and 3.47 for standard and

trip hammer measurements, respectively; and in Figures 3.48 and

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3.49 for select points with standard and trip hammer measure­

ments, respectively. The qualitative trend lines of individual

comparisons all show essentially the same behavior:

qc/N remains essentially constant with increasing qc using

the standard hammer, and increases slightly when using the

trip hammer. Comparison of these summary trends with the

Schmertmann (1976) relation again shows general disagreement,

as would be expected based upon the previous comparisons.

However, in this case Schmertmann shows a definite increase

in q c/N with q c , while the data presented herein shows

either a constant relation or one slightly increasing with

increasing qc . Again, it is expected that as depth increases,

the blowcounts and end bearing should also increase. However,

the values don't necessarily increase at the same rate. In

fact, examination of the CN and Cp curves of Figure 3.6

shows that qc will increase faster than N, particularly at

the low effective pressures studied in this program.

As a further explanation of differences between the data

presented herein and that presented by Schmertmann, Figure

3.50 shows a relation presented by Schmertmann (1978) between

end bearing of a mechanical cone penetrometer and an electric

cone penetrometer. It can be noted that at low values of end

bearing, and hence at shallow depths and low N values, the

mechanical cone shows higher resistance than the electric cone,

an that at higher end bearing values the electric cone measure­

ments are higher than the mechanical. Thus, because the

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Schmertmann data is primarily based on the mechanical cone,

it follows that his qc/N ratios would be higher than presented

herein at shallow depths, and lower at greater depths.

3.3.3.5 qc/N versus Friction Ratio

As discussed in Section 3.2.2.3, previous research has shown

qc/N to be a function of Friction Ratio. Essentially, as

side friction (and thus, friction ratio) increases at a con­

stant end bearing, the total penetration resistance, either

SPT or CPT, also increases. Therefore, the dependence of qc/N

on friction ratio is actually just the result of the equality

of total penetration resistance when measured with either

the SPT or CPT. That is, the SPT N value represents total

resistance, while both the CPT end bearing and sleeve friction

must be used to represent total resistance.

The results of the comparisons of qc/N with friction ratio

using the layer average method are shown in Figures B.37

through B.40 of Appendix B, and are summarized in Figure 3.51.

Likewise, the results of the individual point method are shown

in Figures B.41 through B.48 and are summarized in Figures

3.52 and 3.53 for the standard and trip hammer, respectively.

Finally, the results of the select point method are shown in

Figures 3.54 and 3.55 for standard and trip hammer measurements,

respectively. The summary qualitative trends show essentially

the same behavior as indicated by Schmertmann (1978) with

differences probably due primarily to the different cones used

in this study (electric) and by Schmertmann (mechanical). Of

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primary concern regarding this data is the scatter evidenced

using either the standard or trip hammer measurements. Again,

however, it must be emphasized that the natural heterogeneity

of the investigated sites precludes certainty that adjacent

CPT and SPT measurements are made in identical soils. Therefore,

the average qc/N versus friction ratio measurements probably

do represent a good indication of the behavior that would be

expected if the measurements were made in identical soils.

3.3.3.6 qc/N Versus Median Grain Size

As was discussed previously, the classification of soil types

using the USCS system is not particularly appropriate for CPT

investigations. The primary reason is that the USCS methodology

divides soils by grain size and distribution and by a more or

less arbitrary set of laboratory strength measurements. Often,

but not always, these indices do provide information about

expected in-situ performance of the soils. However, examination

of the behavior of soils around a penetrometer indicates that

other factors are of importance. In an attempt to provide some

means by which the standard classifications could be subdivided,

median grain size was examined for its effect upon the qc /N

ratio.

Plots of median grain size, 050 r against qc/N are shown

in Figures 3.56 and 3.57 for standard and trip hammer measure­

ments, respectively. Essentially, no relation is apparent for

non-clay soils other than that the trip hammer laboratory tests

tended to be performed on a more constant grain size material

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3-36

than used for the standard hammer laboratory tests. It is not

particularly surprising that 059 is poorly rated to qc/N, in

that it has been shown that qc/N varies primarily with stress

level, soil type, and equipment types. 050 relates only to

soil types, and then is only useful for extremes, providing no

information helping to define differences between similar soils

such as SM and ML. It is probable that some combination of

grain size information could help distinguish soil types. Such

a combination could be 059 and the coefficient of uniformity

(Cu ), or perhaps, a combination of sphericity, D^Q/ and Cu or

Coefficient of Curvature. Cursory examination of these factors

as a part of the investigations described herein identified no

predictive trends.

3.2.1.7 qc versus N

The most fundamental comparison of the correspondence between

CPT and SPT measurements is necessarily the comparison of qc

to N as a function of friction ratio or side friction. However,

as this relation is the primary goal of the research program,

it is best presented after the trends of the relation with

other factors have been estimated. The summary plots of the

preceding four sections have, in effect, defined the expected

behavior of the qc versus N relation as N, qc , friction

ratio, and depth (or overburden) are varied.

The qc versus N plots for layer averages are shown in Figures

B.49 through B.52 of Appendix B, and a composite summary is

shown in Figure 3.58. The qualitative best fit to the data is

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also shown in Figure 3.58. It should be noted that where

ambiguities exist, the trends from previous sections have been

used to guide the curve fitting.

Following the same methods as used previously, the individual

data comparisons of qc versus N are shown in Figures B.53

through B.60 and are summarized in Figures 3.59 and 3.60.

Again, data trends are indicated in the figures. Finally, the

select point comparisons are presented in Figures 3.61 and 3.62

for standard and trip hammer measurements, respectively.

It can be seen in Figures 3.59 and 3.60 that the expected

relation between qc , N and FR is well defined for the

standard hammer but shows some unexpected trends for the trip

hammer comparisons. In Figure 3.63 the average q c versus N

relations for the standard hammer are shown compared against

the Schmertmann (1976) relation. The trends are similar with

differences probably resulting from differences in cone and

hammer types, as discussed previously. In Figure 3.64 a plot

of the trip hammer qc versus N results is shown. Several

factors of interest emerge in examination of these figures.

First, the ratio of blowcounts for the trip and standard

hammers at a specific qc is not constant but increases with

friction ratio and increasing soil strength. Second, the trip

hammer curves show the same general trend toward decreasing

qc/N with increasing N as do the standard hammer curves.

However, in the low friction ratio zone (less than 2.0 percent)

the trip hammer curves show two curvature reversals, suggesting

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3-38

either a reduction of qc or an increse in N in the zone of qc

less than about 75 tsf. As no such anomaly is seen in the qc

versus N for the standard hammer, it follows that the N values

are the anomalous data.

Following this trend of trip hammer behavior, qc versus N com­

parisons were made for select points from the Edmond, Oklahoma

site. The results of these comparisons are shown in Fig. 3.65,

where it is seen that the Corps of Engineers hydraulically driven

trip hammer provides higher energy than the Pilcon trip hammer

and that again some trend for double curvature of the qc versus

N relation exists.

The use of a high energy hammer probably is the cause of many of

the difficulties in data comparison. As was discussed previously,

it is probable that the greater the hammer energy, the greater

volume of soil ahead of the sampler which will influence the

resistance to penetration. Thus the higher the hammer energy,

the more each measurement represents an average of soil character­

istics in the vertical plane. An indication of this effect can

be seen for the lower energy penetrometer data presented by

Treadwell (1975) in Fig. 3.66. Based upon the behavior shown

on Figure 3.66, it was considered that the CPT data could be

iteratively averaged over successively larger vertical extents

until continuity of qc versus N was obtained. However, it

is probable that the CPT vertical averaging would need include

some weighting function, requiring more information about the

interrelation of dynamics of the SPT failure mechanism and the

CPT failure mechanism than is presently known.

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As a further attempt to relate qc and N for the hetreogeneous

Edmond site, data was compared using Plasticity Index (PI) and

FR as control variables. The COE Design Memorandum (1980) for

the Edmond site shows blowcounts tabulated by range of Plasti­

city Index. The average corrected blowcount versus depth

relations for ranges in PI are shown in Figure 3.67. It can

be noted that no distinct trends are evident. However, the PI

of a soil is basically a measure of strength potential and may

not indicate anything about the actual strength of the sample

under field conditions.

Next, the CPT measurements were compiled by elevation and then

averaged by friction ratio bands. Thus, the averaging process

excluded all measurements having friction ratios outside of

the range of interest. Preliminary examination of the CPT data

revealed extremely low side friction measurements concurrent

with end bearing behavior indicative of plastic soils. A com­

puter run was performed segregating the CPT values into average

profiles for friction ratio bands of 0 to 0.5, 0.5 to 0.8, 0.8

to 2.25, 2.25 to 3.25, and greater than 3.25. Examination of

the range averages shown in Figure 3.68 reveals maximum and

minimum ranges of end bearing for each select friction ratio

band increasing with friction ratio, behavior contrary to usual.

It can be noted in Figure 3.68 that in the 0.0 to 0.5 friction

ratio band the average profile has a very low magnitude of end

bearing. Thus for soils supposedly non-plastic, extremely low

strengths are evidenced. However, for friction ratios in the

0.8 to 2.25 range (still typically sands based upon the literature)

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the end bearing values increase substantially. Thus, it appears

that this FR range best compares with the blowcounts taken in

the non-plastic soils. However, when examining the qc (adjusted

for overburden pressure) over N^ ratio for this friction ratio

band and blowcounts in materials of PI less than 3, only an ill

defined ratio is found, as shown in Figure 3.69.

Further examination of the blowcount data revealed a trend in

blowcount and side friction for a given material as a function

of increasing Liquidity Index (LI). The effect of LI on side

friction was shown in Figure 3.14. The trend of N^ versus LI

is shown for select points in Figure 3.70. Note, however, that

the LI of a sandy soil with only 10 to 20 percent clay sized

particles may not always be a good indicator of in-situ strength,

Further, as shown previously, it appears the LI increases for

constant end bearing and decreasing side friction. Thus, it

would be expected that low side friction soils would have high

structural sensitivity. Because the LI of a soil essentially

indicates degree of consolidation, and because these data points

were in general from a depth of 30 to 60 feet, it follows that

the clay size interstitial material is underconsolidated, being

prevented from fully consolidating by by the sand fraction

skeleton, which in turn is supported by the clay particles

against any vibration induced densification. However, when

sheared to large strains by the passage of a cone or split

spoon sampler, the interstitial underconsolidated, high water

content soils allow overriding shear of the granular phase

without the sliding and interlocking resistance encountered

~fuGRD

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in cleaner sands. This behavior, then, is similar to the

flowing of cleaner sands after the onset of liquefaction.

Examination of soil grain size distribution corresponding to

high LI revealed some pattern. Typically, all material was

finer than the number 40 sieve, was classed as CL-ML or CL with

PI about 4 to 15, had about 60 to 80 percent material finer

than the number 200 sieve, and had about 10 to 25 percent clay

sized particles. However, no boundary was found for grain size

distribution figures dividing "flowing" and nonflowing mixed

soils.

The existence of soils with PI as high as 20 in the zero to

2.0 percent friction ratio band invalidates the comparison of

N values for PI less than 3 soils with end bearings for the

0.8 to 2.25 percent friction ratio band. Rather, the classifi­

cation of soil types by combinations of end bearing and friction

ratio is necessary. This is in agreement with the classifica­

tion boundaries shown previously in Figure 3.9. These criteria

were then used to select sands and the CPT data again segregated

by bands of qc and FR. This average corrected end bearing

curve, Figure 3.71, was then compared against the less than PI

equal 3 blowcounts. The results of these comparisons are shown

in Figure 3.72. It can be seen in that figure that the scatter

in q c/N is reduced. However, it is still apparent that the

qc/N relation is erratic, particularly in the deep-sands zone.

Recall that the indicated reduction in qc/N for these high

resistance sands was noted in examination of the double curvature

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and resultant decrease in qc/N shown previously in Figure 3.65,

and may be the result of transition between compressive and

dilative-structure with resultant pore water pressure effects.

3.3.3.8 Comparison of N and CPT Side Friction

As a final comparison, all N values were plotted against the

average side friction measured in an adjacent CPT sounding at

the same depth. The results of this comparison are shown in

Figures 3.73 and 3.74 for standard and trip hammer measurements,

respectively. The trend in N with increasing side friction is

apparent in both measurements; however, no attempt was made to

refine the correlation through cross plots of side friction and

qc or FR versus N value.

3.3.3.9 Summary of qc/N Relations

In order to examine the total range of qc/N values described

in the preceding sections, frequency histograms were prepared,

as shown in Figures 3.75 through 3.78. In Figure 3.75 the

layer-average data is presented for trip and standard hammer

measurements. In Figure 3.76 and 3.77 the compilation of all

individual comparisons is by hammer type and friction ratio

band, while in Figure 3.77 all data is composited by hammer

type alone.

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o

MARCUSON - BIEGANOUSKY, 1977

C N

PROJECT NO.: 79-153

USGS CPT-SPT

C N FACTORS VERSUS

EFFECTIVE OVERBURDEN PRESSURE

9-80 FIGURE 3.1

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10 -

u] 20ill

I- 30az111_Ja o 40CC

50-

60I I I *

0.2 0.4 0.6 0.8

INCIDENT ENERGY Ei

THEORETICAL ENERGY = E*

(A)

1.0

10 -

20

30 -

O 40QC

50

60I I I

0.2 0.4 0.6

INCIDENT ENERGY

MAXIMUM INCIDENT ENERGY Ei'

(B)

1.0

Ei

7.0

6.0 -

5.0 -

4.0 -

3.0-

2.0 -

1.0

1.0I

0.8\

0.40.6

INCIDENT ENERGY

MAXIMUM ENERGY

(C)

0.2

EiEi*

FROM SCHMERTMAN (1976)

ID-

30-

40-

50-

60

0.6I

0.8I

1.0

N @ 16.7'

1.2 1.4 1.6

N @ ANY DEPTH

(D)

'NRL

"flJCROPROJECT NO : 79-153

USGS CPT-SPT

EFFECT OF ROD LENGTH ON SPT BLOWCOUNTS

9-80 FIGURE 3.2

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O

PERCENT PARTICLES < 16 u

100 -

uT HozCC

ssCO 10 -QZ HI

1 -

0 5 15 25 35 45 65 85 95

WITH GRAVEL

SAND

Q HI

HI

CC

O O

C 2 < (/

Jw '

>-

_J W

QZ

>-"

-1 O

-1

s o0 >--J <

o

><

C

»

(J J

1 2 3 4 56

FRICTION RAT 10, %

r y. ' ' 1 PROJbCT NO.: /9-1b3

CRT SOIL CLASSIFICATIONBEGEMAN METHOD

9'80 FIGURE 3.3

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200

INSENSITIVE. NON FISSURED

INORGANIC

ORGANICCLAYS AND

MIXED SOILS

FRICTION RATIO,

I-RJQROPROJECT NO.: 79-153

USGS CPT-SPT

CRT SOIL CLASSIFICATION AFTER SCHMERTMANN (1978)

9-80 FIGURE 3.4

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0.5 -

1.0 -

1.5 -

o

LUcc

Lit CC CL.Z Lit Q QC D CO DC Lit > O at

o 2.0at

ai

2.5 -

J3C

3.0

0.5I

1.0I

Cp (FROM SCHMERTMANN)

1.5 2.0 2.5I

3.0

FROM SCHMERTMANN (1976)

PROJECT NO.: 79-153

USGS CPT-SPT

9-80

EFFECTIVE OVERBURDEN PRESSURE

VERSUS

Cp=qc @1TSF/qcFIGURE 3.5

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0.2 0.6

I

C N , Cp, C RL, Cp'

1.0 1.4 1.8

I _______I____________I

2.2

I

2.6

10 -

20 -

uu uu

X

o.LUO

30 -

40 -

O

50 -

60 -

70

SCHMERTMANN Cp (1974)

EFFECT OF ROD LENGTH = CRL

ASSUME Cp'XCRL

CN/CRL

a

JASSUMES UNSATURATED SITE

rfuoRaPROJECT NO.: 79-153

USGS CPT-SPT

COMPARISON OF Cp, C N AND ROD LENGTH

9-80 FIGURE 3.6

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300

200

CME o

a. tr

100

20 40

SPT

60 80

PROJECT NO.: 79-153

USGS CPT-SPT

PREVIOUS CORRELATIONS: qc = f(SPT)FOR PURE SANDS

(AFTER deMELLO, 1971)9-80 FIGURE 3.7

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350

300

250

GO

zo

O

IV)UJ CC

Oo o

I

onn 2O°

150

100

50

10 20 30 40

N, SPT (BLOWS PER FOOT)

50 60 70

LOOSE

MEDIUM DENSE

DENSE

V

A

A

O PROJECT NO.: 79-153

USGS CPT-SPT

PREVIOUS CORRELATIONS: qc = f(SPT)

FOR SANDS (AFTER SANGERLAT, 1972)

9-80 FIGURE 3.8

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100-

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40

6 cr

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FRICTION RATIO,

O GPV SP-GP

O SP

A SP-SM

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SM-ML (30-60% FINES)

ML (>60% FINES)

CL

A SC

V ML-CL

NUMBERS ON SYMBOLS INDICATE NUMBER OF OBSERVATIONS

9-80

PROJECT NO.:

USGS CPT-SPT

COMPOSITE: ALL SITESqc VS FRICTION RATIO

SOIL CLASSIFICATION CHART

79-153

FIGURE 3.9

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1000800

600

400 -

LL. CO

LU CJ

crh- CO

CO LU

CD CJ

200 -

10080

60

40 -

20 -

108

6

4 H

2 -

2 3

FRICTI456

RRTI0 (7.)8

NUMBERS INDICATE DEPTH OF SOUNDING

|-flJCi»0PROJECT NO.: 79-153

USGS CPT-SPT

CONTINUOUS TRACE METHOD ARCADIA DAM CRT PROBE 119

9-80 FIGURE 3.10

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600

400 -

200 -

CO

UJ CJ 2ccI COI I

00 LU 0£

LU 2CD CJ

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60

40 -

108

6

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2 -1

SAND & GRAVEL (SP), 24-44', CN-7

SAND & GRAVEL (SP-GP), 35-45', CN-13

SILTY CLAY (CD, 45-60', CN-7

SANDY GRAVEL (GP). 20-25', CS-1

SAND (SP-SM), 23-30', CN-13

SILTYSAND (SM-SP), 20-28', CN-7

SANDY SILT(ML-SM), 0-10', CN-7

SILTYSAND (SM-ML), 0-10', CN-13

SILTYSAND <SM) 0-8', CS-1

SILTY CLAY (CD, 50-60', CS-1

SILTY CLAY (CD, 11-18', CN-13

CLAYEY SILT (ML), 9-17', CS-1

CLAYEY SILT (ML), 10-15', CN-7

23456

FRICTIQN RflTIQ (X)8

PROJECT NO.: 79-153

USGS CPT-SPT

SOIL TYPE CLASSIFICATIONS USING THE CPT CONTINUOUS TRACE METHOD

9-80 FIGURE 3.11

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400 -

U_ CO

UJ CJ Zcri CO i i

CD LU C£

UJ ZCD CJ

200 -

100 - 80 -

60 -

40 -

20 -

10 J

8

6

4 H

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<SAND (SP), 37-47', CS-5

SILTY SAND (SM), 10-40', SD

-SAND & GRAVEL (SP), 18-23', CS-5

SILTY SAND (SP-SM), 15-35'. SS-9

SAND (SP)29-33', ML-3

SANDY SILT(ML-SM) 1-5', CS-5

CLAY(CH). 46-47', SS-9

CLAY (CL-CH), 36-39', 45-46', SS-9

SANDY SILT (ML) 8-12', SS-9

SILTY CLAY (CL-ML), 33-37', CS-5

CLAYEY SILT(ML-CL), 6-13', CS-5

SILTY CLAY (CD 6-10', ML-3

2 3

FRICTI456

RRTI0 (X)8

|-ffJJGI»0PROJECT NO.: 79-153

USGS CPT-SPT

SOILTYPE CLASSIFICATION USING THE CONTINUOUS TRACE METHOD

9-80 FIGURE 3.12

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FRICTI RRTI0 (7.)

SYMBOLS INDICATE LABORATORY CLASSIFICATION BASED ON SIEVE SIZE ANALYSIS WITH THE LINE INDICATING THE qc TO FRICTION RATIO TRACE FOR V

SN - SP-SM MC- ML-CL

PROJECT NO.: 79-153

USGS CPT-SPT

LIMITED TRACE METHOD COYOTE NORTH SITE

9-80 FIGURE 3.13

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100 -

50 -

u_CO

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20 -

10

5 -I

UL CO

z"oo

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NUMBERS REPRESENT VALUES OF LIQUIDITY INDEX

PROJECT NO.: 79-153

USGS CPT-SPT

SELECT POINTS - EDMOND SITE LIQUIDITY INDEX VS qc AND FRICTION RATIO

9-80FIGURE 3.14

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200 -

FRICTION RATIO,

PROJECT NO.: 79-153

USGS CPT-SPT

TRENDS IN CRT SOIL CLASSIFICATION

9-80 FIGURE 3.15

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PROJECT NO.:

USGS CPT-SPT

COMPOSITE: ALL SITES Ov VSCp

STANDARD HAMMER

79-153

FIGURE 3.17

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a

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A 0.75-1.25

D 1.25-1.75

1.75-2.25

A 2.25 - 3.25

> 3.25

PROJECT NO.: 79-153

USGS CPT-SPT

SELECT POINTS: ALL SITESCTv'VS Cp,

STANDARD HAMMER9-80 FIGURE 3.21

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Page 123: pdfs.semanticscholar.org€¦ · Evaluation of the Cone Penetrometer for liquefaction Hazard Assessment Geoffrey R. Martin and Bruce J. Douglas Fugro, Inc. 3777 Long Beach Boulevard

SOIL PROFILE

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qc/N

PROBABLE RANGE

POSSIBLE RANGE

a

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PROJECT NO.: 79-153

USGS CPT-SPT

SALINASSITE

qc/N RANGE COMPARISONS

STANDARD HAMMER9-80 FIGURE 3.24

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20 -

LU UJ U_

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tUJ Q

40 -

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SP, SP-SM

50 ~

60

CL

SM

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10 15

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I

20

PROBABLE RANGE

POSSIBLE RANGE

a

I

PROJECT NO.: 79-153

USGS CPT-SPT

9-SO

MOSS LANDING SITE

qc/N RANGE COMPARISONSSTANDARD HAMMER

FIGURE 3.25

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SOIL PROFILE

10 -

20 -

1X1 1X1

£ 30 -I a.1X1a

40 -

50 -

60

ML,SM-ML

SM, SP-SM,SM-ML

SP,SP-SM,GP

CL

10

I15

I

20

PROBABLE RANGE

POSSIBLE RANGE

a

I

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USGS CPT-SPT

79-153

SAN JOSE SITE: COYOTE NORTH & SOUTHqc/N RANGE COMPARISONS

STANDARD HAMMER9-80 FIGURE 3.26

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I PROBABLE RANGE

I | POSSIBLE RANGE

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SM

SM

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I

20

Jjjjjfr

JECT NO.: 79-153

USGS CPT-SPT

SAN DIEGO SITE: NAS NORTH ISLANDqc/N RANGE COMPARISONS

TRIPHAMMER9-80 FIGURE 3.27

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10 -

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30 -

UJ UJu_z IQ.UJQ 40 -

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60 -

70 -

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1 1

1 1

1 1 10 5 10 15

qC/N

PROBABLE RANGE

I 1 POSSIBLE RANGE

1

SM, ML

SP-SM

SP, SP-SM

SM,SC,CL, ML

120

fjjjjjj^JECT NO.: 79-153

USGS CPT-SPT

SALINASSITEqc/N RANGE COMPARISONS

TRIPHAMMER9-80 FIGURE 3.28

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SOIL PROFILE

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20 -

UJ UJ

t LJJ Q

30 -

40 -

50 -

60

JOc

I10

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15

SP-SM, SM

CL

SP-SM

CL

20

PROBABLE RANGE

POSSIBLE RANGE

a

I

PROJECT NO.: 79-153

USGS CPT-SPT

9-80

MOSS LANDING SITEqc/N RANGE COMPARISONS

TRIPHAMMERFIGURE 3.29

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SOIL PROFILE

10 -

20 -

01

I

a.UJ

30 -

ML,SM-ML

SM, SP-SM, SM-ML

' SP, SP-SM, GP

40 -

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PROBABLE RANGE

POSSIBLE RANGE

PROJECT NO.:

USGS CPT-SPT

79-153

SAN JOSE SITE: COYOTE NORTH & SOUTH

Qc/N RANGE COMPARISONSTRIPHAMMER

9-80 FIGURE 3.30

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50 -

60 -

70 -

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NUMBERS ON POINTS REPRESENT FRICTION RATIO, %

0.51

g0.66

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0.55

* 0.45

B0.50

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^

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[-fvicsna ] PROJECTNO - : 79-153

LM B_^__|__^J

HflHHB USGS CPT-SPT

COMPOSITE: ALL SITESqc/N VS DEPTH BY LAYER AVERAGES

9-80 FIGURE 3.36

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200 -

100 -

F R = 0.5%

300

200 -

V)

uCT

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I I I I0.5 1.0 1.5 2.0 2.5

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100%

qc/N

a

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PROJECT NO.:

USGS CPT-SPT

79-153

9-80

qc/N VS EFFECTIVE OVERBURDEN PRESSURE

(AFTER SCHMERTMANN, 1978)FIGURE 3.37

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j_ 30 -LU LU U_

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70 - _________________________

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1.14

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0.99 0.35

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0.64

0.51

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NUMBERS ON POINTS REPRESENT FRICTION RATIO, %

1.25

hfijOROPROJECT NO.: 79-153

USGS CPT-SPT

COMPOSITE: ALL SITES qc/N VS DEPTH FOR SELECT POINTS

STANDARD HAMMER9-80 FIGURE 3.38

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80 -

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40 -

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SANDS; STANDARD HAMMER

0.50

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0.88

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AA VV

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NUMBERS ON POINTS REPRESENT FRICTION RATIO, %

PROJECT NO.: 79-153

USGS CPT-SPT

_COMPOSITE: ALL SITES qc/N VS N BY LAYER AVERAGES

9-80 FIGURE 3.40

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158

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100 -

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USGS CPT-SPT

COMPOSITE: ALL SITES

qc/N VS N STANDARD HAMMER

9-80 FIGURE 3.41

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USGS CPT-SPT

COMPOSITE: ALL SITES

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STANDARD HAMMER9-80 FIGURE 3.43

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f_C ~~1 PROJfcCI NO.: 79-153

UHMH USGS CPT-SPT

COMPOSITE: ALL SITES q c /N VS N FOR SELECT POINTS

TRIPHAMMER

9-80 FIGURE 3.44

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4-1

4. SUMMARY AND CONCLUSIONS

The goal of this section is to summarize the findings of this

research, to provide some conclusions regarding the reliability

of CPT.-SPT correlation for use in liquefaction potential

analyses, and to suggest some needs for additional research.

4.1 SUMMARY

The data presented-in the previous sections has been organized

to meet the three basic requirements for use of a CPT-SPT-lique-

faction potential assessment. These needs are the estimation

of liquefiable soils, the normalization of CPT measurements,

and the conversion of CPT measurements into SPT measurements.

As no direct rule is available regarding when the SPT can be

used to provide information for the empirical method, it is

assumed that the SPT is valid for sands and a small range of

silty sands, with fines content up to about 30 percent. An

estimated boundary between the zone of 30 percent fines content

and the 30 to 60 percent zone was shown in Figure 3.9. Also

shown in that figure are the boundaries for other soil categories

as interpreted from the data presented in the preceding sections.

Although it is seen that friction ratio alone does not completely

define soil-type boundaries, for the purposes of providing

conservative estimates of susceptible soils it is acceptable

to select a constant friction ratio as the boundary. Soft CL

and CL-ML soils may also fall in the band, but such soft or

sensitive soils may present their own hazard under earthquake

loading. A suggested friction ratio band for use with the

electric cone penetrometer is zero to 2.25 percent.

IGRO

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4-2

It was shown in Section 3.3.3.2 that a C p relation to account

for the effect of overburden pressure upon field investigations

shows a considerable degree of scatter. Development of a

parameter, Cp ^ f by which CPT measurements could be directly

converted to corrected equivalent blowcounts was also described.

cpl could be defined for a particular friction ratio band,

such as the sand range. The q c/N versus depth relation could

then be defined for the same band, and by multiplication of the

two relations, a new Cp relation would be found. This Cp

could then be used as an adjustment on the basis of constant

material type with associated assumption of a constant qc/N

for that material. The trend in Cp would then automatically

include the effect of the variable q c/N relation. Because

these field-based Cp ^ methods rely to large degree upon the

particular CN relation selected, and because the scatter in

CN relations is large and encompasses available Cp relations

determined under controlled circumstances, it is most appropriate

to use the available Cp relation shown in Figure 3.5.

Finally, the most appropriate means to convert qc and FR into

equivalent N values is discussed. It has been shown that

qc/N is primarily a function of soil type and in-situ stress

conditions. Thus, the conversion of qc to N for liquefaction

potential assessments must also depend upon these factors.

In Figures 4.1 and 4.2 are shown plots of N value ranges on

the qc -FR charts for standard and trip hammer measurements,

respectively. Lines showing conservative definition of the

constant N value trends are also shown on those figures. It

ICRO

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4-3

can be seen that those lines are essentially just the relations

shown in previous section. For example, the qc/N relation

decreases with increasing N, but begins to show rapid increases

with q^, at end bearing pressures above 100 tsf. The effect

of changing soil type on qc/N is also clearly visible.

4.2 CONCLUSIONS

Conclusions regarding the use of a CPT-SPT conversion with

subsequent use of the SPT-liquefaction potential relation focus

upon the method of CPT data analysis and the reliability of the

CPT-SPT correlation.

Figures 3.9 and 4.1 and 4.2 present composite plots of CPT

versus soil type and CPT versus N value data. Likewise, Figure

3.15 presents a summary of the classification trends as based

upon CPT data. It is noted that the Friction Ratio is a primary

variable used in all of the plots. Although many of the trends

in Figure 3.15 are speculative, it can be seen that estimation

of soil characteristics is dependent upon both of the primary

CPT measurements: end bearing and side friction. Thus, although

the normalized form of the data as represented by friction ratios

is convenient, the actual measured side frictions should be

routinely analyzed when using CPT data. The importance of side

friction is also seen in Figures 4.1 and 4.2. These figures

reveal the similarity of constant N value lines and lines of

constant side friction. Such agreement suggests that graphical

relations between the desired soil characteristic and end bearing

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4-4

and side friction may be preferable to the use of friction ratio

relations, and should be further investigated.

Although friction ratio indirectly accounts for side friction,

there are difficulties in its practical use. For example, the

end bearing penetration behavior in layered media was previously

shown to depend upon some weighted average of soil resistance

within several diameters in front and back of the tip. The

effect of layers on sleeve measurements is different, and it

appears that the influence of underlying layers is felt by the

sleeve much later than the influence is felt by the cone tip.

This often results in erratic calculated friction ratios in the

near vicinity of layer interfaces.

This rapid fluctuation in friction ratio is not as apparent

with the mechanical CPT as used by most previous researchers.

The reason is that the typical mechanical cone procedure

automatically averages measurements over the depth of the

sounding increments. Thus, the rapid changes in resistance

leading to erratic friction ratios are not as pronounced.

However, by the same reasoning, it is apparent that this use

of the mechanical penetrometers leads to an inability to

distinguish the occurrence of sudden resistance changes as

caused by a changed material type, and that resistances

measured in thin layers will represent average values or may

be entirely in error, as in the usual determination of side

friction in a zone of rapidly increasing or decreasing end

bearing.

ICRD

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4-5

Several methods of smoothing the friction ratio curve were

investigated. These included moving averages of either of or

both the end bearing and sleeve measurements, variable adjust­

ments .of the lead distance between sleeve zone of influence and

tip zone of influence, and filtering of high frequency components

of the friction ratio record. Although such devices are of use

-for investigation of the phase difference in response of the

tip and sleeve, it appears that direct use of the sleeve measure­

ment itself holds more promise than artificial adjustment of

the friction ratio. Although the sleeve readings are erratic

when passing through dense or interlayered soils, they are

smoother than the calculated friction ratios. Further, soil

types, stress conditions, and index characteristics and N

values seem to bear a closer relationship to sleeve readings

than to friction ratios.

Because little research has been focused on direct use of

sleeve measurements, current methods still must rely upon the

friction ratio method. That method as applied to N value

prediction has been well explained by Schmertmann. A major

concern, however, is still related to equipment. It has been

shown that different hammer energies not only produce different

N values, but also produce different shapes of the qc versus

N curve. Further, it appears that the ratio of N values relating

two different hammer energies is not necessarily constant, but

varies depending upon soil type and/or resistance. It is also

known that the use of electrical versus mechanical cones

results in different qc versus N relations.

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4-6

Therefore, in order to advance a set of qc versus N relations,

it is necessary to make an accurate assessment of the "average"

hammer energy represented in the blowcount method. It is also

necessary to specify the type of cone penetrometer for which

the relations are valid. It should be noted that this problem

of equipment standardization is everpresent but usually ignored

in routine use of the N value method.

A set of functional relations between qc , N, friction ratio

and overburden pressure is not presented in this report. Until

the standardization of SPT methods and equipment is complete,

or until the SPT hammer energy implicit in the blowcount method

is defined, the presentation of another set of equations for

use by practitioners unaware of the inherent assumptions that

must be accepted to use the equations seems inappropriate.

This is not to suggest that the CPT method is not valid for

prediction of N values or liquefaction potential, for it

certainly is. The profiling of a site using the CPT provides

more information, faster, more reliably and at a lower cost

than any other method now available. Likewise, the qualitative

determination of. strength variation throughout the site profile

is immediately obtained from the field records. Further, the

scatter in the CPT relation with another test measurement,

such as the SPT, stems primarily from the scatter in the other

test results or from the finite measurement intervals of the

other test as compared to the essentially continuous CPT

measurements. Even with the scatter in comparative relations,

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4-7

the CPT method is so rapid that a large statistical data base

can be developed, allowing precise definition of average site

characteristics.

An example of CPT estimation of SPT blowcounts can be drawn

from the Edmond site data. The q c versus N relations for

that site (Figure 3.65) were simplified (double curvature

removed), and fit with equations relating to q c and FR. The

relations were then applied to the CPT records from the site.

A plot of CPT predicted, corrected N value for a typical

sounding is shown in Figure 4.3 compared against the corrected

N value measured at the same location, wherein the accuracy

of the CPT prediction is self-evident. However, it must be

recalled that a hammer-specific blowcount is predicted in that

figure, and it is not known how well that hammer compares with

the hammers implicit in the empirical blowcount method. Thus,

considering the variability of SPT measurements, the use of

precise correlations of CPT and SPT measurements may be of

little use. That is, the precision of the CPT-SPT correlation

should be of the same order as the precision of the SPT and

SPT-liquefaction potential correlation.

4.3 RESEARCH SUGGESTIONS

Three areas of needed research are suggested by this report.

These areas deal with standardization of the SPT, analysis of

the CPT, and further investigation of relations between the CPT

and liquefaction potential.

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4-8

The standardization of the SPT has been underway for many years

and the only specific concern indicated in this report is the

selection of standardization energy. It appears that resolution

of soil type changes depends upon the energy delivered to the

sampler per blow of the hammer.

Needs in analysis of the CPT are many, and include research

into failure mechanism and the measurement process. Regarding

the measurement process, it appears that the value of direct

use of side friction measurements may be facilitated by reloca­

tion of the side friction sleeve to a location in which the

pore pressure field is less variable than at its present

location immediately behind the cone tip. In addition, some

reanalysis of CPT data in terms of side friction and end bear­

ing without dependence upon friction ratio may yield worthwhile

results.

The use of the CPT for liquefaction potential analyses requires

several related investigations. In the indirect approach, such

as presented in this report, measurements of SPT hammer energy

should be made. In fact, the hammers used in this study should

be so calibrated.. Direct approaches to the problem of CPT-lique-

faction potential evaluations should be pursued. These include

the use of piezometric (pore pressure measuring) cones, and the

performance of cone penetrometer tests at previously liquefied

sites.

IGRO

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5. REFERENCES

Alperstein, R., and Leifer, S. A., 1976, "Site Investigation with Static Cone Penetrometer," Journal of the Geotech- nical Engineering Division, ASCE, GT5, May.

American Society for Testing and Materials, 1975, "DeepQuasi-static, Cone and Friction-Cone Penetration Tests of Soil," ASTM Tentative Standards, Part 19, Designation: D3441-75T, December, and ASTM D 1586, D422 and D1586.

U.S. Army Corps of Engineers, Tulsa District, 1978, "General Design, Phase II, Project Design: Arcadia Lake Design Memorandum #3."

Bazaraa, A.R.S.S., 1967, "Use of the Standard PenetrationTest for Estimating Settlements of shallow foundations on sand," Ph.D. Thesis, Univ. of Illinois, Urbana.

Begemann, H. K., 1965, "The Friction Jacket Cone as an Aidin Determining the Soil Profile," Proc. 6th International Conference of Soil Mechanics and Foundation Engineering, Volume 1, pp. 17-20.

Bingham, R. H., and Moore, R. L., 1975, "Reconnaissance of the Water Resources of the Oklahoma City Quadrangle, Central Oklahoma," U.S. Geol. Survey and Oklahoma Geo­ logical Survey, Hydrologic Atlas 4 (HA-4).

California Department of Water Resources, 1968, Bolsa-Sunset Area, Orange County: CDWR Bull. 63-2.

Campanella, R. G., Berzins, W. E., and Shields, D. H., 1979, "A Preliminary Evaluation of Menard Pressuremeter, Cone Penetrometer, and Standard Penetration Tests in the Lower Mainland, British Columbia," Soil Mechanics Series No. 40, Department of Civil Engineering, The University of British Columbia, Vancouver, B.C., Canada, VGT 1W5, May.

de Mello, Victor, F. B., 1971, "The Standard Penetration Test," 4th Pan American Conference on Soil Mechanics and Foundation Engineering, San Juan, Puerto Rico r Vol. I, p. 43.

de Ruiter, J., 1971, "Electric Penetrometer for Site In­ vestigations," Journal of the Soil Mechanics and Foun­ dation Division, ASCE, SM-2, February.

Dibblee, J. W., Jr., 1976, "Rinconada and Related Faults in the Southern Coast Ranges, California, and Their Tectonic Significance," U.S. Geol. Survey Professional Paper 981 r 55 p.

IGRO

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5-2

Donovan, N. C., and Singh, S., 1976, "Liquefaction Criteriafor the Trans-Alaska Pipeline," ASCE National Convention, Sept. 27-Oct. 1, Philadelphia, PA., pp. 139-168.

Ellis, A. J., and Lee, C. H., 1919, "Geology and GroundWaters of the Western Part of San Diego County, CA," U.S. Geol. Survey Water-Supply Paper 446, 321 p.

Forrest, J., and Ferritto, J., 1976, "An Earthquake Analysis of the Liquefaction Potential at the Naval Air Station, North Island," Port Hueneme, California, Civil Engineer­ ing Lab, Technical Report R847.

Fletcher, G. F. A., 1965, "SPT: It's Uses and Abuses," ASCE Journal of the Soil Mechanics and Foundations Division, July.

Gibbs, H. J., and Holtz, W. H., 1957, "Research on Determining the Density of Sands by Spoon Penetration Testing," 4th ICSMFE, London, Vol. I.

Helley, E. J., and Brabb, E. E., 1971, "Geologic Map of Late Cenozoic Deposits, Santa Clara County, California," U.S. Geol. Survey Misc. Field Invest. Map MF-335.

Helley, E. J., LaJoie, K. R., Spangle, E. E., and Blair, M. L., 1979, "Flatland deposits of the San Francisco Bay Region, California - Their Geology and Engineering Properties, and Their Importance to Comprehensive Planning," U.S. Geol. Survey Prof. Paper 943, 88 p.

Janbu and Senneset, 1974, "Effective Stress Interpretationof In Situ Static Penetration Test," European Symposium on Penetration Testing, Stockholm, June, Vol. 2.2.

Kennedy, M. P., Welday, E. E., Borchardt, G., Chase, G. W., and Chapman, R. H., 1977, "Studies on Surface Faulting and Liquefaction as Potential Earthquake Hazards in Urban San Diego, California," Final Technical Report, California Division of Mines and Geology (CDMG) Sacra­ mento, California, October.

Kennedy, M. P., 1973, "Bedrock Lithologies, San Diego area, California," in Ross, A., and Dowlen, R. J. (eds.), Studies on the geology and geologic hazards of the greater San Diego Area, California: San Diego Associa­ tion of Geologists.

Kovacs, William D., 1975, "A Comparative Investigation of the Mobile Drilling Company's Safe-T-Driver with the Standard Cathead with Manila Rope for the Performance of the Standard Penetration Test."

ICRO

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5-3

Kovacs, William D. r 1978, "An Alternative to the Cathead and Rope for the Standard Penetration Test," ASTM, GTJODJ, Vol. l r No. 2. June.

Levadoux, J. N., and Baligh, M. M., 1980, "Pore PressureDuring Penetration in Clays," Publication No. R80-15, Massachusetts Institute of Technology, Department of Civil Engineering, Constructed Facilities Division, April.

Marcuson, William F. Ill, and Bieganousky, Wayne A., 1977, "SPT and Relative Density in Coarse Sands," ASCE, GTJ, Vol. 1302, No.GT 11 November.

Mitchell, J. K., and Lunne, T. A., 1978, "Cone Resistanceas a Measure of Sand Strength," Journal of the Geotech- nical Engineering Division, ASCE, GT-7, July.

Peck, R. B., Hanson, W., E., Thornburn, T. H., 1973, Founda­ tion Engineering, 2nd Ed., John Wiley & Sons, Inc., New York, New York, 514 p.

Poland, J F., 1959, "Hydrology of the Long Beach-Santa Ana Area, California," U.S. Geol. Survey Water-Supply Paper 1471, 257 p.

Poland, J. F., Piper, A. M., and others, 1956, "Ground-Water Geology of the Coastal Zone, Long Beach-Santa Ana Area, California," U.S. Geol. Survey Water-Supply Paper 1109, 162 p.

Sangerlat, G., 1972, The Penetrometer and Soil Exploration, Elsevier Publishing Company, New York.

Sangerlat, G., 1974, "European Symposium on PenetrationTesting," Stockholm, June, Vol. 2.2, State-of-the-Art Reports.

Schmertmann, J. H., "Discussion of the Standard Penetration Test," 4th Pan American Conference on Soil Mechanics and Foundation Engineering, San Juan, Puerto Rico, Vol. III.

Schmertmann, J. H., 1976, "Predicting the qc/N Ratio,"Final Report D-636, Engineering and Industrial Experi­ ment Station, Department of Civil Engineering, University of Florida, Gainesville, October.

______ , 1978, "Guidelines for Cone Penetration TestPerformance and Design," U.S. Department of Transpor­ tation, Federal Highway Administration Report No. FHWA-TS-78-209.

ICRD

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Schmertmann, J. H., 1979, "Statics of SPT," Journal of the Geotechnical Engineering Division, ASCE, GT5, May.

________, 1979b, "Energy Dynamics of SPT," Journal of the Geotechnical Engineering Division, ASCE, GT 8, August.

Seed, Bolton H., 1976, "Evaluation of Soil Liquefaction Effects on Level Ground During Earthquakes," ASCE National Convention, Sept. 27-Oct.l, Philadelphia, PA.

Seed, H. B., Mori, K., Chan, C. K., 1977, "Influence of Seismic History on Liquefaction of Sands," ASCE, GT Vol. 103, No. GT4, April.

Seed, H. B., 1979, "Soil Liquefaction and Cyclic MobilityEvaluation for Level Ground During Earthquakes," Journal of the Geotechical Engineering Division, ASCE, GT2, February.

Steiger, F., 1979, "A Technical Report on the SPT Workshop Held During ASTM's June 1979 Committee Week," Geotech­ nical Testing Journal, ASTM, Volume 2, Number 3, September.

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Treadwell, Donald D. 1975, "The Influence of Gravity, Pre-stress, Compressibility, and Layering on Soil Resistance to Static Penetration," Dissertation for Ph.D. in Engineering, Graduate Division of the University of Calif. Berkeley.

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Vesic, A. S., 1963 "Bearing Capacity of Deep Foundations in Sand," Highway Research Board, Highway Research Record No. 39.

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ICRO

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5-5

Youd, T. L., and Perkins, D. M. , 1977, "Mapping of Liquefac­ tion Potential Using Probability Concepts," Annual Con­ vention of the ASCE, Oct., San Francisco, California.

Ziony, J. I., 1973, "Recency of Faulting in the GreaterSan Diego Area, California," in Ross, A., and Dowlen, R. J. (eds.), "Studies on the Geology and Geologic Hazards of the Greater San Diego Area, California," San Diego Association of Geologists, p. 68-75.

ICRO

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APPENDIX A

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FRICTI

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FRICTI0N RESISTRNCE,

TSF

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FRICTI8N RESISTflNCE. TS

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RESISTflNCE, TS

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FRIC

TI8N

RE

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flNC

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1.5

0

C8NE RESISTflNCE. TS

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FRIC

TION

RESISTANCE,

TSF

1.5

0

C9NE RESISTANCE,

TSF

75

150

225

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TIQ

, X

300

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FRICTI8N RE

SIST

RNCE

, TSF

1.5

0

C8NE RE

SIST

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. TSF

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o3

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FRIC

TI0N

RESISTRNCE,

TSF

1.5

0

C0NE RESISTRNCE.

TSF

75

150

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FRICTI0N RRTI8

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FRIC

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RE

SIST

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. TS

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FRIC

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DEPTH IN

FEET0

10

20

30

50

60

80

SAMPLE TYPE

PENETRATION DENSITY/ , RESISTANCE MOISTURE CONSISTENCY

S

S

S

S

S

S

S

S

27

12

27

27

44

89

92

111

V

<^

ELEVATION: DATE DRI EQUIPMENT USED: 5 7/8" ROTARY WASH WATER LEVEL: 5'

fs\ STANDARD HAMMER SPLIT SPOON ^ SAMPLE

[7] TRIP HAMMER SPLIT SPOON SAMPLE £

PERCENT | !_

SON. TYPE 2O 40

SAND (SP-SM), brown, fin*, non-plastic, shell fragments

SILTY SAND (SM), grayish brown to brown, fin* no n -plastic

-----------

|!--

SILTY SAND (SM), yellowish brown, fine sands, occesionel f trace of low plasticity, fines, very micaceous, brown colored. |_less mica at 40' J

L........

FT _ "._._. .BORING TERMINATED AT 51* ._.... _j_ - . . .

LLED: 101279 t _. NPROJECTNO.; MgJgR^M

f^nnrvr *^^ USGSCPT-J

T PASSING 1 |

SO SO

1

79-163

>PT

o.oo2mm LOG OF BORING NO. 1A

SAN DIEGO SITE: NAS NORTH ISLAND

9-80 FIGUREA.11

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DEPTH IN

FEET0 |

10

20

30

40

50

70

80

SAMPLE TYPE

PENETRATION | RESISTANCE MOISTURE

T

T"

T

T

T

T

T

21

15

21

33

43

69

63

V

t^

DENSITY/ CONSISTENCY

ELEVATION: DATE DRI EQUIPMENT USED: 5 7/8" ROTARY WASH WATER LEVEL: 5 '

fs"| STANDARD HAMMER SPLIT SPOON ^ SAMPLE

[T] TRIP HAMMER SPLIT SPOON SAMPLE f

PERCEN | 1_

SOW. TYPE 20 40

SAND (SP-SM), brown, fin* sands, non-plastic, shall ' LL... .......fragments M^ k

ft

SILTY SAND (SM), grayish brown to brown, fin* sands, non-plastic, micaceous " "

SILTY SAND (SM), yellowish brown, fine sands, non-plastic with occasional trace of low plasticity, fines, heavy mica .___..___ ..content, less mica at 38'

=|---

BORING TERMINATED AT 51'

LLED; 101279 f ^ \ PROJECT NO. =

I7tm~irvr m^^^B USGSCPT-S

T PASSING 1 |

eo M

79-153

»PT

o.oozmm LOG OF BORING NO. 1B

SAN DIEGO SITE: NAS NORTH ISLAND

9-80 FIGURE A.12

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DEPTH SAMPLE TYPE

'* PENETRATION DENSITY/ H i , RESISTANCE f MOlSTUftE CONSlSTENCY(

-

20

in _

-

50

60

70

80

S

s

S

_s_

T

s

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s

s

s

£_

s

20

15*

17

2H

24

26

27

60

68

77

81

142

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«,

ELEVATION: DATE DRI

EQUIPMENT USED: 5 7/8" ROTARY WASH

WATER LEVEL: 5'

\S\ STANDARD HAMMER SPLIT SPOON SAMPLE

[T] TRIP HAMMER SPLIT SPOON SAMPLE f

SAND (SP-SM). brown, fin* si fragments

SILTY SAND (SM), grayish b plastic micaceous

SILTY SAND (SM), yellowish with occasional seams of low content, brown, colored less ri medium sand

PERCEN I H-

SOIL TYPE 20 40

nds, non-plastic, shell ' ..._..___...

urown to brown, fine sands, non- II

brown, fine sands, nonplasticplasticity, fines, heavy mica nica at 45 '-49' occasional

::::::::BORING TERMINATED AT 5V JT

LLED: 10-11-79

Ijonn QIFWC

0.002 mm

/ s PROJECT NO.:

MmgR^*^^^^^ USGS CPT-J

T PASSING I |

60 60

i

79-153

>PT

LOG OF BORING NO. 2A SAN DIEGO SITE: NAS NORTH ISLAND

g-80 FIGURE A.13

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DEPTH IN

FEET 0 L.

10

-

20

40

-

50;

60

70

80

SAMPLE TYPE

PENETRATION DENSITY/ RESISTANCE MOISTURE CONSISTENCY

T

T

_J_

T

T

T

T

T

T

T

J_

T

16

10

11

1

18

17

20

32

39

52

48

62

JT

\

SAND (SP'SM), brown, fina < micaceous

son. TYPE

land, non-plastic, shall fragments

PERCENT PASSING | | | ,

20 40 60 SO

TT

WnSILTY SAND (SM). grayish brown to brown, fina sands, [T f non-plastic, micacaous 1 1 1

SILTY SAND (SM), yellowis plastic, very micacaous, betw less mica content, lass silt cor

n brown, fine sands, non- een 45 -49' brown colored.itent

T '^

T" 1

,;:::

FBORING TERMINATED AT 51'

ELEVATION: DATE DRILLED: 101279

EQUIPMENT USED: 5 7/8" ROTARY WASH

WATER LEVEL: 5'

[s] STANDARD HAMMER SPLIT SPOON ^ 0200SIEVE SAMPLE

[T] TRIP HAMMER SPLIT SPOON SAMPLE f O.O02 mm

HRjBR^J

i k

2 r

NO.: 79-153

USGS CPT-SPT

LOG OF BORING NO. 2B SAN DIEGO SITE: NAS NORTH ISLAND

9-80 FIGURE A.14

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DEPTH IN

FEET 0 1

10

-

20

30

40

5O

en

70

SO

1 SAMPLE TYPE

PENETRATION i 1 RESISTANCE MOISTURE

S

S

S

S

jS_

_s_

S

J_

S

S

S

S

43

24

14

13

1

26

37

28

49

112

55

89

66

V

*,

DENSITY/ CONSISTENCY

ELEVATION: DATE DRI EQUIPMENT USED: 5 7/8" ROTARY WASH WATER LEVEU 5'

\S\ STANDARD HAMMER SPLIT SPOON ^ SAMPLE

|T] TRIP HAMMER SPLIT SPOON SAMPLE £

SOIL TYPE

SAND (SP-SM), brown, fin* to medium, micaceous withshall f ragments

SILTY SAND (SM), brown to grayish brown, fine sands, non-plastic, mica

PERCENT PASSING | | | ,

20 40 60 SO

non-plastic, locally having mica content

m 4

SILTY SAND (SM), brown, fine sands, occasional medium

BORING E BORING TERMINATED AT SO'

LLED: 10-11-79 r V- * PROJECTMrojBR^J

n

k

NO.:

USGS CPT-SPT

79-153

0.002 mm LOG OF BORING NO. 3A SAN DIEGO SITE: NAS NORTH ISLAND

9-80 FIGURE A.15

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DEPTH | SAMPLE TVP£

IN 1cecT PENETRATION DENSITY/ FEET 1 RESISTANCE MOISTURE CONSISTENCY

10

-

««*»

40

50

AA

70

80

T

T

T

T

T

T

T

T

T

T

T

T

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10

7

1

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22

29

41

55

48

47

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SILTY SAND (SM), brown to poorly graded, non-plastic, m

SILTY SAND (SM), yellow b locally heavy mica content

SILTY SAND (SM), brown, f micaceous

SOIL TYPE

> grayish brown, fina sands.cacaous

rown. fine sands, non-plastic,

PERCENT PASSING | | . 1

20 40

....

>,- TL

ine sands, non-plastic,

BORING TERMINATED AT 50*

ELEVATION: DATE DRILLED: 10-11-79

EQUIPMENT USED: 5 7/8" ROTARY WASH

WATER LEVEL: 5'

[i] STANDARD HAMMER SPLIT SPOON ^ #200 SIEVE SAMPLE

(Tj TRIP HAMMER SPLIT SPOON SAMPLE £ O.OO2 mm

i t

tO M

i

{

NO.: 79-163

USGS CPT-SPT

LOG OF BORING NO. 3B SAN DIEGO SITE: NAS NORTH ISLAND

9-80 FIGURE A.16

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DEPTH IN

FEET0 1

10

-20

30

40

50

60

80

T

T

T

T

T

T

T.

T

T_

T

: SAMPLE TYPE

ENETRATION RESISTANCE MOISTURE

13

10

1

15

23

29

32

31

38

76

T

DENSITY/ CONSISTENCY

ELEVATION: DATE DRI EQUIPMENT USED: 5 7/8" ROTARY WASH WATER LEVEL: 5'

fs"| STANDARD HAMMER SPLIT SPOON ^ SAMPLE

[f] TRIP HAMMER SPLIT SPOON SAMPLE f

SOIL TYPE

SAND (SP-SM), brown to dark brown, fine , sands, non-plastic, mica, some shell fragments

non-plastic, micaceous

mica content, non-plastic, occasional silt pockets I

f

[

micaceous

BORING TERMINATED AT 47'

LLED: 10-1079 ,-._.. .-. -^PROJECT

PERCENT PASSING

<r

l"i

v

20 40 60

A L.

k--

MO.:

USGS CPT-SPT

80

i

1

t

i 1

79-153

o.ooamm LOG OF BORING NO. 4A

SAN DIEGO SITE: NAS NORTH ISLAND

9-80 FIGURE A.17

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DEPTH SAMPLE TYPE

IM'"_ PENETRATION DENSITY/

PCtI ,, RESISTANCE MOISTURE CONSISTENCY0 M-« i " -

10

20

30

40

50

60

70

80

S

s

S

s

^_

s

s

s

s

s

23

17

1

.22

35

44

64

79

60

97

V

*%

SAND (SP-SM(, brown, fin* « hell fragments

SILTY SAND (SM), grayish b nonplastic, micaceous

BOH. TYPE

nds, nonplastic, micaceous.

SILTY SAND (SM), yellowish brown, fina sands, nonplastic.heavy mica content

SILTY SAND (SM), brown, f

PERCENT PASSING I | - 1

20 40

............flr 1 1P fl !fL..x_._. .. -i

BORING TERMINATED AT 46'

ELEVATION: DATE DRILLED: 101079 EQUIPMENT USED: 5 7/8" ROTARY WASH WATER LEVEL: 5'[i] STANDARD HAMMER SPLIT SPOON ^ 020OSIEVE

SAMPLE

[T] TRIP HAMMER SPLIT SPOON SAMPLE £ O.OO2 mm

nmgwj^............

60 «0

i

_ji

NO.: 79-153

USGS CPT-SPT

LOG OF BORING NO. 4B SAN DIEGO SITE: NAS NORTH ISLAND

9-80 FIGURE A.18

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FRICTI6N RE

SIST

flNC

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F

1.5

0

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9

Page 206: pdfs.semanticscholar.org€¦ · Evaluation of the Cone Penetrometer for liquefaction Hazard Assessment Geoffrey R. Martin and Bruce J. Douglas Fugro, Inc. 3777 Long Beach Boulevard

FRICTION RESISTRNCE.

TSF

1.5

0

CGNE

RE

SIST

RNCE

. TSF

75

150

225

300

§b.oo

FRICTION RflTIO

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FRICTI0N RESISTRNCE.

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DEPTH IN FEET75.00 60.00 45.00 30.0015.00

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CO

75.00DEPTH IN FEET

60.00 45.00 30.0015.00

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Page 210: pdfs.semanticscholar.org€¦ · Evaluation of the Cone Penetrometer for liquefaction Hazard Assessment Geoffrey R. Martin and Bruce J. Douglas Fugro, Inc. 3777 Long Beach Boulevard

FRIC

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Page 211: pdfs.semanticscholar.org€¦ · Evaluation of the Cone Penetrometer for liquefaction Hazard Assessment Geoffrey R. Martin and Bruce J. Douglas Fugro, Inc. 3777 Long Beach Boulevard

o3

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75.0060.00DEPTH IN FEET

45.00 30.00

mTJm

m m31H

75.00DEPTH IN FEET

60.00 45.00 30.0015.00

COz20 3)H

Page 213: pdfs.semanticscholar.org€¦ · Evaluation of the Cone Penetrometer for liquefaction Hazard Assessment Geoffrey R. Martin and Bruce J. Douglas Fugro, Inc. 3777 Long Beach Boulevard

o3

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FRIC

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FRIC

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FRICTI0N RESISTANCE, TS

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o3

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Page 218: pdfs.semanticscholar.org€¦ · Evaluation of the Cone Penetrometer for liquefaction Hazard Assessment Geoffrey R. Martin and Bruce J. Douglas Fugro, Inc. 3777 Long Beach Boulevard

FRIC

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FRIC

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SIST

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Page 220: pdfs.semanticscholar.org€¦ · Evaluation of the Cone Penetrometer for liquefaction Hazard Assessment Geoffrey R. Martin and Bruce J. Douglas Fugro, Inc. 3777 Long Beach Boulevard

DEPTH p SAMPLE TYPE

e»r PENETRATION DENSITY/ FEET 1 RESISTANCE MOISTURE CONSISTENCY

10

20

3O

40

en __

70

80

J_

S

s"s"

s

s

s s"

s

s

*vIT

s

s

s

13

7

13

8

16

IB

14

33

18

27

44

19

31

43

40

^r

«,

SON. TYPE

SANDY SILT (ML), brown, fine sands, non-plastic

PERCENT PASSING | , | . 1

20 40 SO

SILTY SAND (SM-ML), brown, fin*, non-plactfc ^

SANDY SILT (ML), brown, Ic trace of clay

tt .>w plasticity, wood chips,

SILTY SAND (SP-SM), brown, fin* to coarse

F--SAND (SP-SM), gray, medium to coarse sands

SAND (SP), gray, coarse sands, trace of fin* gravels

GRAVELLY SAND (SP). gray, coarse sands, flna gravels

CLAY (CH), gray, high plasticity

SANDY SILT (SM-ML), brown, low plasticity, occasional fin* sands

CLAY (CH). gray, high plasti

GRAVELLY SAND (SP), gra^

city

SILTY CLAY (CL-CH), high plasticity

BORING TERMINATED AT

ELEVATION: DATE DRILLED: 11-779 EQUIPMENT USED: 5 7/8" ROTARY WASH WATER LEVEL: 20'[i] STANDARD HAMMER SPLIT SPOON ^ #200 SIEVE

SAMPLE

[r] TRIP HAMMER SPLIT SPOON SAMPLE f 0.002mm

60'

i \ PROJECT

["fijCR^

i\

\

i\.

----- --I -

NO.:

USGS CPT-SPT

SO

\

1

79-163

LOG OF BORING NO. 1 SAUNAS SITE

9-80 FIGURE A.34

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DEPTH | SAMPLE TYPE

IN_ " PENETRATION DENSITY/ P6fcr t , RESISTANCE MOISTURE CONSISTENCY

10

-

20

30

50

60

80

T

T

T

T

T

T

T

T

T

T

T

T

T"

T

6

6

IK

6

9

12

10

12

11

12

15

7

14

16

V

«,

ELEVATION: DATE DRI

EQUIPMENT USED: 5 7/8" ROTARY WASH

WATER LEVEL: 20'

fs"| STANDARD HAMMER SPLIT SPOON ^ SAMPLE

|T] TRIP HAMMER SPLIT SPOON SAMPLE f

PERCEti 1 1-

SOM. TYPE 2O 4O

SILTY SANO (SM). brown, tine sends, non-pleetic

SILTY SAND (SM), brown, f

SILTY SAND (SM-ML), brow micaceous

...........

I"""-ne sands LL .........

n. fine sends, non-ptaetic, 11M.... -- iE .-t --~SILTY SAND (SM), brown, fine sands

SAND (SP & SP-SM), brown to gray, medium to coarse sands

GRAVELLY SAND (SP). gray, coarse sands, fine gravels ...........

CLAY (CH). gray, high plasticity ._-..-._...

CLAYEY SILT (ML-CL). bro medium sands

CLAY (CH), gray, high plasti

wn, low plasticity, trace of ._-...._...

CLAYEY SAND (SO, gray, coarse sands, low plasticity

SILTY CLAY (CL-CH), gray, chips and roots

high plasticity, some wood

BORING TERMINATED AT 62'

LLED: 11-6 & 7-79

#2OO SIEVE

0.002 mm

t N PROJECT NO.:

^^^^^* USGS CRT-

IT PASSING I |

0 SO

|

79-153

SPT

LOG OF BORING NO. 2 SAUNAS SITE

9.80 FIGUREA.35

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DEPTH r SAMPLE TYPE

'" PENETRATION DENSITY/ rtcl 1 RESISTANCE MOISTURE CONSISTENCY

10

20

30

40

70

80

S

s

S

S

S

_S_

S

S

~s~

s

s

9

8

15

18

19

24

25

25

20

19

18

V

«.

SANDY SILT -SILTY SAND ( plastic, micaceous

SOIL TYPE

SM-ML). brown, fine, non-

t

SILTY SAND (SM), brown, fine, non-plattk

SILTY SAND (SM-ML), brow some fine sands

rn. trace of low plastic fines, with

PERCENT PASSING 1 | '

20 40

rITSAND (SP-SM), brown, medium, trace of non-plastic silts

SAND (SP), gray, medium to coarse sands

GRAVELLY SAND (SP), gray, coarse sands, fine gravels

CLAY (CH), gray, high plasticity

CLAYEY SILT (ML-CL), brown, low plasticity, some fine M"d« ________________________________________

CLAY (CH), gray, high plasticity

SILTY SAND (SM-ML) & CL sands, low to medium plastic

CLAY (CL-CH), gray, mediur leaves and wood chips

BORING TERMINATED AT

ELEVATION: DATE DRILLED: 11-8-79 EQUIPMENT USED: 5 7/8" ROTARY WASH WATER LEVEL: 20

[si STANDARD HAMMER SPLIT SPOON ^ #200 SIEVESAMPLE

[7] TRIP HAMMER SPLIT SPOON SAMPLE f 0.002mm

AYEY SAND (SC). gray, coerse ty

n to high plasticity, some

60'

f ^^ \ PROJECT

T

- -

t i

I C

o to

NO.: 79-153

USGS CPT-SPT

LOG OF BORING NO. 3

SAUNAS SITE

9-80 FIGURE A.36

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DEPTH 1 «M«« TYPE

'* PENETRATION DENSITY/ *" T 1 RESISTANCE MOISTURE CONSISTENCY

10

20

50

70

80

T

T

T

T

T

T MBB

T

T

2_

T

T

T

4

4

7

6

7

7

11

13

12

8 .

19

28

V .

«.

SOIL TYPE

SANDY SIUT (SM-ML), brown, low plwtlelty, tr*o» of fin*sands

SILTY SAND (SM) & SAND 1 medium sands, micaceous

SAND (SP), gray, coarse sand poorly graded

PERCENT PASSING | t . . 1

20 40

I..........

| -4 £...f SILT (SM-ML), brown, fine to W~ ' r ~ ~ ~

LL.....J.....

ff

s, occasional medium sands.

CLAY (CH), gray, high plasticity

CLAYEY SILT (ML), brown, fine sands

CLAY (CH), gray, high plasti

low plasticity, traca of

city

1

n ^CLAYEY SANO (SO, gray, medium sands 1

CLAY (CH), gray, high plasti laavas

i

BORING TERMINATED AT 60'

ELEVATION: DATE DRILLED: 11-8-79

EQUIPMENT USED: 5 7/8" ROTARY WASH

WATER LEVEL: 20'

[¥] STANDARD HAMMER SPLIT SPOON ^ #200 SIEVE SAMPLE

[?] TRIP HAMMER SPLIT SPOON SAMPLE £ 0.002mm

60 90

I ki

1

] E

NO.: 79-163

USGS CPT-SPT

LOG OF BORING NO. 4

SAUNAS SITE

9-80 FIGURE A. 37

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DEPTH I" SAMPLE TYPE

«er PENETRATION DENSITY/ FEET f | RESISTANCE MOISTURE CONSISTENCY

10

-

20

-

40

ftfk ,_.,

70

80

S

s

8

IT

s

s

T

s

_s_

A

s

s

13

6

IS

9

21

26

29

45

27

22

9

27

V

*.

SILTY SAND-SANDY SILT tow plasticity

SANDY SILT (SM-ML). brow sands

SAND (SP-SM), brown, fin* t

SAND (SP), brown to gray, rr fina gravels

SON. TYPE

(SM-ML), brown, fin* sands.

i

»n. low plasticity, trace of fin* CT " "

Fo medium, non-plastic

tedium to coerse, occasional

GRAVELLY SAND (SP). gray, coarse, sands, fine gravels

CLAY (CH), grey, high plasticity

CLAYEY SILT (ML), brown,

CLAY (CH). grey, high plasti

CLAYEY SAND (SO, grey, c

CLAY (CH), gray, high plestii

BORING TERMINATED AT

ELEVATION: DATE DRILLED: 11-9-79 EQUIPMENT USED: 5 7/8" ROTARY WASH WATER LEVEL: 20'Hs] STANDARD HAMMER SPLIT SPOON ^ #200 SIEVE

SAMPLE

[r] TRIP HAMMER SPLIT SPOON SAMPLE £ 0.002mm

low plasticity, micaceous

city - - - -i

.oerse sands ~

:ity

60' - - - -

[ "RjGW^J

esl.B.B.Bi US

PERCENT PASSING H | | |

20 40 «0 M

i k

1

79-163

GS CPT-SPT

LOG OF BORING NO. 5 SAUNAS SITE

9-80 FIGURE A.38

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DEPTH f "AMPLE TYPE

recr PENETRATION DENSITY/ PEfcT 1 RESISTANCE MOISTURE CONSISTENCY

0 "-*- i '

1O

20

30

40

50

70

80

T

IHMI*

T

T

T

T

T

T

T

T

T

T

T

T

T

4

4

6

7

14

10

12

16

13

17

18

6

14

24

V

«.

8ILTY SANO (SM). brown, fi of none to tow plastic tilt (ML

SAND (SP & SP-SM), brown i sands, occasional fine gravels

CLAY (CL-CH), gray, mediun sands

SILT (ML), gray, low plastich

PERCEN1 | H-

80H. TYPE 20 4O

n* sands, non-plastic finct, tone.) at 2'-6' ............

.......

|...,,...

o gray, medium to coarse ._....__....

n to high plasticity, some fine

........in

y, uniform TT" - -

SAND (SP), gray, fine to medium

CLAY (CH), gray, high plastic

BORING TERMINATED AT

ELEVATION: DATE DRILLED: 11-9 a 12-79

EQUIPMENT USED: 5 7/8" ROTARY WASH

WATER LEVEL: 20'

[i] STANDARD HAMMER SPLIT SPOON ^ #200 SIEVE SAMPLE

[T] TRIP HAMMER SPLIT SPOON SAMPLE £ 0.002mm

:ity .___..___...

60' .__...___...

i v PROJECT NO.:

MRiGRI^

^^^^^^ USGS CPT-S

r PASSING | |

to so

.

1

I

i

79-153

PT

LOG OF BORING NO. 6 SAUNAS SITE

g.00 FIGURE A.39

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DEPTH I 8AMM TYPE

e«r PENETRATION DENSITY/ F"T 1 RESISTANCE MOISTURE CONSISTENCYo -*-* «

10

-

*%t\ _______

M

30

40

70

80

S^

S

S

s

s

s

s

s

s

s

s

s

~s~

7

4

7

11

16

9

18

19

33

24

32

28

23

T

^

SI LTV SANO (SM), brown, fl micaceous, occasional, silt poi

SILTY SAND (SM). gray. fin« sands, non-plastic

SAND (SP & SP-SM). gray, fit some coarse sands and fine gr

CLAY (CD gray, medium to

CLAYEY SAND (SC), gray, f plastic fines

CLAY (CH), gray, high plasti at 64' -65'

SOU. TYPE

*et*

PERCENT PASSING | | | ,

20 40 SO SO

' P!

iIE Lr

i to medium,occasional coarse f i

.>e to medium, non-plastic, k velsat31.0'-36.5' FT

high plasticity

ine to medium sands, low

city, lens of low plastic silt (ML)

BORING TERMINATED AT 65'

ELEVATION: DATE DRILLED: 11-12-79 EQUIPMENT USED: 5 7/8" ROTARY WASH WATER LEVEL: 20[s] STANDARD HAMMER SPLIT SPOON ^ *2OO SIEVE

SAMPLE

(T] TRIP HAMMER SPLIT SPOON SAMPLE £ O.OO2 mm

i s PROJECT

H^Bg^

i

i

I--"---'

'

i

1i

NO.: 79-163

USGS CPT-SPT

LOG OF BORING NO. 7 SALINASSITE

9-80 FIGURE A. 40

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DEPTH SAMPLE TYPE

e«T PENETRATION DENSITY/ *""' , RESISTANCE MOISTURE CONSISTENCY

10

20

40

50

60

70

80

T

T

T

T_

T

T

T

T

T

T

T

T

T"

3

5

3

6

11

10

12

6

13

17

12

5

14

V

+,

ON. TYK

SILTY SANO (SM), brown, fina, uniform, non-plastic, mica

SILTY SAND (SM), brown, f plastic

SAND (SP), light brown to gr plastic

GRAVELLY SAND (SP) & S coarse sands, fine gravels

;. '

na to madlum sands, non-

ay, fina to medium, non-

|AND (SP-SM). gray, fina to k

tCLAY (CH), gray, high plasticity

CLAYEY SAND (SC). grey, f ne to coarse, low plastic fines

CLAY (CH), gray, high plasticity

BORING TERMINATED AT 60'

ELEVATION: DATE DRILLED: 11-1 3-79 EQUIPMENT USED: 5 7/a» ROTARY WASH WATER LEVEL: 20'[T] STANDARD HAMMER SPLIT SPOON 02OOSIEVE

SAMPLE

[f] TRIP HAMMER SPLIT SPOON SAMPLE f O.O02 mm

i \ PROJECT f

HQJGR^J

PERCENT PASSING I | "

20 40

i k

i1 -----------

:;::::::::::i...h....

0 00

JO.: 79-163

USGS CPT-SPT

LOG OF BORING NO. 8 SAUNAS SITE

9-80 FIGURE A.41

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75.00DEPTH IN FEET

o o noi __o Z * m g -D o m

8m

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? H * m

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Page 229: pdfs.semanticscholar.org€¦ · Evaluation of the Cone Penetrometer for liquefaction Hazard Assessment Geoffrey R. Martin and Bruce J. Douglas Fugro, Inc. 3777 Long Beach Boulevard

75.00DEPTH IN FEET

30.0015.000.00

oim-o rnZ

m m

m

75.00DEPTH IN FEET

60.00 45.00 30.0015.00

Page 230: pdfs.semanticscholar.org€¦ · Evaluation of the Cone Penetrometer for liquefaction Hazard Assessment Geoffrey R. Martin and Bruce J. Douglas Fugro, Inc. 3777 Long Beach Boulevard

75.00DEPTH IN FEET

O

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m30

m23

75.00DEPTH IN FEET

60.00 45.00 30.00

Page 231: pdfs.semanticscholar.org€¦ · Evaluation of the Cone Penetrometer for liquefaction Hazard Assessment Geoffrey R. Martin and Bruce J. Douglas Fugro, Inc. 3777 Long Beach Boulevard

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Page 232: pdfs.semanticscholar.org€¦ · Evaluation of the Cone Penetrometer for liquefaction Hazard Assessment Geoffrey R. Martin and Bruce J. Douglas Fugro, Inc. 3777 Long Beach Boulevard

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Page 234: pdfs.semanticscholar.org€¦ · Evaluation of the Cone Penetrometer for liquefaction Hazard Assessment Geoffrey R. Martin and Bruce J. Douglas Fugro, Inc. 3777 Long Beach Boulevard

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Page 235: pdfs.semanticscholar.org€¦ · Evaluation of the Cone Penetrometer for liquefaction Hazard Assessment Geoffrey R. Martin and Bruce J. Douglas Fugro, Inc. 3777 Long Beach Boulevard

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Page 236: pdfs.semanticscholar.org€¦ · Evaluation of the Cone Penetrometer for liquefaction Hazard Assessment Geoffrey R. Martin and Bruce J. Douglas Fugro, Inc. 3777 Long Beach Boulevard

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Page 237: pdfs.semanticscholar.org€¦ · Evaluation of the Cone Penetrometer for liquefaction Hazard Assessment Geoffrey R. Martin and Bruce J. Douglas Fugro, Inc. 3777 Long Beach Boulevard

DEPTH IN

FEET 0

10

-

30

40

.50

-

-

SAMPLE TYPE

PENETRATION DENSITY/ | RESISTANCE MOISTURE CONSISTENCY

s

s

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EQUIPMENT USED: 5 7/8" ROTARY WASH

WATER LEVEL: 5'

[sT| STANDARD HAMMER SPLIT SPOON -^ SAMPLE

[r] TRIP HAMMER SPLIT SPOON SAMPLE m

OIL TYPE

SAND (SP), brown, tend to medium sands, uniform

SILTY CLAY (CL). dark 0r«V, medium plasticity l

SAND (SP & SP-SM). light brown, fina to medium sand, occasional coarsa sand, nonplastlc. occasionaly with silt

SILTY CLAY (CL). dark gray, medium plasticity

predominantly coarse sands, occasional shall fragments

SANDY SILT SILTY SAND (SP-SM), dark gray, fine sends.

of silt

PERCENT PASSING | | . . 1

20 40

...........

* -

:,:::::,:::p::::3::

CLAY & SAND (CL & SP), interbedded zone, predominantly clay materials, dark gray silty clay low PI, dark gray sand.fine to coarse

SILTY SAND (SM-ML). dark gray silty sand, occasional mica^occasional shell fragments ____________________________SILTY CLAY (CL), dark gray, medium plasticity, shell frag. j

--JsL. .-__, k-

SILTY SAND (SP), dark gray, fine to coarse send, uniform, fjf

clay pockets with low plasticity

SILTY CLAY (CL), dark pray, medium plasticity.occasional sand pockets, occasional shell fragments

BORING TERMINATED AT 60'

_LLED: 11-13-79 ..-.--_ ,....,,- PROJECT

Mfijeijo

O

to so

1

1

^

NO.: 79-153

USGS CPT-SPT

0.002 mm LOG OF BORING NO. 1 MOSS LANDING SITE

9-80 FIGURE A.51

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DEPTH IN

FEET0 i

10

<M

20

30

40

50

70

80

i SAMPLE TYPE

PENETRATION ( | RESISTANCE MOISTURE

"T"

T

T

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"r~

T

T"

T

6

27

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4

31

55

12

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fs"| STANDARD HAMMER SPLIT SPOON ^ SAMPLE

[T] TRIP HAMMER SPLIT SPOON SAMPLE f

SOIL TYPE

SAND (SP), light brown, sand, fin* to medium

PERCENT PASSING | ,____, , 1

20 40

r1

SAND (SP-SM), light brown sand, medium coarse, some layers of fines, totdark gray, fine sand, some clay lanses,occasional shall fragments

CLAY & SAND (CL-SP), interbedded zona, dark gray, finemedium sand, occasional shell fragments, clay layers at 35.5' and 37.5'

SAND (SP), dark gray fine to coarse sand, shell fragments, gravel layer at 47.5'

SILTY CLAY (CD, dark gray, medium plasticity

SILTY SAND (SP & SM), dark gray, fine to medium, trace fines, low plasticity, occasional shell fragments, occasionalthin clay layers

BORING TERMINATED AT 56'

LLED: 11-14-79 f , N PROJECTrlftiBg^J

1 1

60 60

NO.: 79-153

USGS CPT-SPT

0.002 mm LOG OF BORING NO. 2

MOSS LANDING SITE

9-80 FIGURE A.52

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DEPTH | 'SAMPLE TYPE

>«T PENETRATION DENSITY/ F"T 1 RESISTANCE MOISTURE CONSISTENCY

*

10

30

7O

8O

S

_s_

s

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SON. TYPE

S AN D (SP) , brown, fine to medium tend, clean

CLAY (CD, dark gray clay, medium plasticity

SAND (SP), light brown, fine to coarse sand, to dark gray fine sand, uniform mica

SILTY CLAY (CD, dark gray, medium plasticity | |SILTY SAND & SAND (SP-S uniform dark gray sand at 26

M), dark gray silty sand, fine A , fine to coarse L|_ _

CLAYEY SANDY SILT (SM-ML), dark gray, low plasticity jSANDY SILT (SM-ML). dark

CLAY & SAND (CL & SP). Interbedded zone, occasional sandpockets

SILTY CLAY (CL)

SAND (SP-SM), fine to coarse, shell fragments

SILTY CLAY (CL) with mica, medium elasticity

SAND & SILTY SAND (SM), shall fragments, vertically int» fine, trace of low plasticity f i

BORING TERMINATED AT

ELEVATION: DATE DRILLED: 11-13-79 EQUIPMENT USED: 5 7/8" ROTARY WASH WATER LEVEL: 5'[s] STANDARD HAMMER SPLIT SPOON ^ #200 SIEVE

SAMPLE [7] TRIP HAMMER SPLIT SPOON SAMPLE £ O.O02 mm

Idark gray sand, fine, medium I

nes ^

T

^ |

/ \ PROJECT NO.

rfucit^ a^a^a^a^B y

PERCENT PASSING | | | |

20 40 SO-SO

:::::::::,

4 i

A

: 79-153

SGS CPT-SPT

LOG OF BORING NO. 3 MOSS LANDING SITE

9-80 FIGURE A.53

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DEPTH IN

FEET0

J

10

«

M

M

60

70

80

SAMPLE TYPE

PENETRATION DENSITY/ t j RESISTANCE MOISTURE CONSISTENCY

T

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58

18

15

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V

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SAMPLE

[7] TRIP HAMMER SPLIT SPOON SAMPLE £

on. TYPESAND (SP), brown, fin* sand, uniform mica

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gravals at 17', to dark gray sand, fina, uniform ( \

CLAY (CL)

SAND (SP), dark gray, fina to madium sands, occasionalcoarse sand, some shall fragments

wCLAY (CL & SP), intarbaddad zona, dark gray clay, madium plasticity, sand, fine to coarse

SILTY CLAY (CL), dark graySAND & SILTY SAND (SM), dark gray, fina to medium sand,

silt clay pocket, gravel layer at 48.5'

BORING TERMINATED AT 56'

_ .___LLED: 11-14-79 f"""Vr \pnojccr r<

MRjcm^

PERCENT PASSING | J___H . 1

20 40 «0

f 1

tO.:

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0

79-153

0.002 mm LOG OF BORING NO. 4

MOSS LANDING SITE

9-80 FIGURE A.54

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DEPTH IN

FEET0

10

30

40

60

80

| SAMPLE TYPE

PENETRATION DENSITY/ { , RESISTANCE. MOISTURE CONSISTENCY

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_T_

T

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T

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68

21

17

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V

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SAMPLE

|Tj TRIP HAMMER SPLIT SPOON SAMPLE £

Oft. TYPE

SAND <SP). Hgrn brown aand. fin* to madtum eand, tmiform

i '

CLAY (CL). dark gray, medium plasticity

SAND (SP). light brown, firm to coarsa sand, soma firm gravels, layer of dark gray sand, uniform fine at 21'

CLAY (CL)

SAND (SP). light gray, fine to coarsa sand fl

_|1

CLAY & SAND (CL & SP), interbedded zone, dark gray silty ciay, medium plasticity; dark gray sand, fina to coarse

SAND (SP), light gray, fina to coarse sand, some fine gravel and shell fragments

CLAY (CL). gray sandy silty clay, low plasticity

BORING TERMINATED AT 55'

_ ii-< i-LLED:1 1-1 5-79 J.M."- >PnOJCCTI>

Mugn^

PERCENT PASSING | II

20 40 SO

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so

70-163

0.002 mm LOG OF BORING NO. 5 MOSS LANDING SITE

9-80 FIGURE A.55

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DEPTH IN

FEET

10

-

20

40

50

ftA

70

80

SAMPLE TYPE

PENETRATION DENSITY/ i J i RESISTANCE MOISTURE CONSISTENCY

T

T

T

T

T

T

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T

T

11

S

28

9

41

34

14

22

7

V

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ELEVATION: DATE DRI EQUIPMENT USED: 5 7/8" ROTARY WASH WATER LEVEL: 5'

[si STANDARD HAMMER SPLIT SPOON ^ SAMPLE

[7] TRIP HAMMER SPLIT SPOON SAMPLE f

OH. TYPE

SAND (SP), brown, fin* to medium «md

content

SAND (SP-SM), light brown, fine to coarse tend, some finegravels, layer of dark gray, fine sands at 20*

,CLAY (CD 1

CLAY & SAND (CL & SP), predominantly sand with thin X clay layers |

SAND (SP-SM), gray sand, fine to medium

CLAY & SAND (CL & SP). inter bedded zone, dark gray silty clay, medium plasticity; dark gray sand, medium to

SAND (SM), light gray sands, fine to coarse, occasionalsilty clay pockets, some shell fragments, gravels, dark gray fine sand with shell fragments

SILTY CLAY (CL-CH), dark gray, medium plasticity

BORING TERMINATED AT 57'

LLED: 11-14 79 r >pnoJccTKMraBRi^

PERCENT PASSING | | l 1

20 40 «

M k

f"

iO.:

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1 SO

79-153

o-oo2 """ LOG OF BORING NO. 6 MOSS LANDING SITE

9-80 FIGUREA.56

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DEPTH IN

FEET0

10

20

30

nn

70

80

t

S

S

s

s

s

s

s

s

s

SAMPLE TYPE

PENETRATION RESISTANCE MOISTURE

22

25

23

57

31

90

36

28

69

V_

«.

DENSITY/ CONSISTENCY

ELEVATION: DATE DR» EQUIPMENT USED: 5 7/8" ROTARY WASH WATER LEVEL: 5'[s] STANDARD HAMMER SPLIT SPOON ^ u~^ SAMPLE

[]F] TRIP HAMMER SPLIT SPOON SAMPLE f

PERCEN | 1_

I

Oft. TYPE 10 40

SAND (SP), light brown, sand, fina to medium, uniform

CLAY (CL), dark gray, clay, medium plasticity

.

II

CLAY & SAND (CL-SP). interbedded zona; dark gray ............ silty clay, medium plasticity, dark gray sand medium tocoarse, some shall fragments ............

SAND (SP & SP-SM), dark gray, fine to coarse sand, finegravels, some shell fragments, occasional clay pockets

BORING TERMINATED AT 55' ._._..__....

LLED: 11-15.79 f «-. NPROJCCTNO.. MRjggJjM

ff^ ...... ^^ USGSCPT-S

T PASSING

o to

.............79-153

JPT

0002 mm LOG OF BORING NO. 7 MOSS LANDING SITE

9-80 FIGURE A.S7

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DEPTH IN

FEET0 f-

10

20

-

40

50

60

70

80

| SAMPLE TYPE

PENETRATION DENSITY/ RESISTANCE MOISTURE CONSISTENCY

S

S

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S

S

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S

S

12

21

30

13

60'

82

29

24

77

V

SAND (SP). light brown sand

SOIL TYPE

fine to medium

CLAY (CD, dark gray clay, medium plasticity

SAND (SP), light brown, fine to coarse sand, soma f gravels; change to dark gray, fine to coarse sand, pre­ dominantly coarse sand; change to light gray, fine to sand, occasional shell fragments

CLAY & SANO (CL-SP), interbedded zone; dark gra clay, medium plasticity, dark gray sand, medium to some shell fragments

SAND (SP & SM), light gray, fine to coarse sand, sor fragments to dark gray sand, fine, occasional silty cli pocket, to light gray sand, fine with shell fragments

BORING TERMINATED AT 55'

ELEVATION: DATE DRILLED: 11 -15-79 EQUIPMENT USED: 5 7/8" ROTARY WASH WATER LEVEL: 5.fsl STANDARD HAMMER SPLIT SPOON ^ *200 S«EVB " SAMPLE

[f] TRIP HAMMER SPLIT SPOON SAMPLE f O.OO2 mm

HRjcwo

PERCENT PASSING

20 4O 60 80

ne

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y silty coarse.

ne shellIV

2 L

|-i »--

PROJECT NO.:

USGSCPT-SPT

79-163

LOG OF BORING NO. 8 MOSS LANDING SITE

9-80 FIGURE A.58

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75.00DEPTH IN FEET

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Page 247: pdfs.semanticscholar.org€¦ · Evaluation of the Cone Penetrometer for liquefaction Hazard Assessment Geoffrey R. Martin and Bruce J. Douglas Fugro, Inc. 3777 Long Beach Boulevard

FRICTI0N RE

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Page 248: pdfs.semanticscholar.org€¦ · Evaluation of the Cone Penetrometer for liquefaction Hazard Assessment Geoffrey R. Martin and Bruce J. Douglas Fugro, Inc. 3777 Long Beach Boulevard

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75.00DEPTH IN FEET

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75.0060.00DEPTH IN FEET

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Page 250: pdfs.semanticscholar.org€¦ · Evaluation of the Cone Penetrometer for liquefaction Hazard Assessment Geoffrey R. Martin and Bruce J. Douglas Fugro, Inc. 3777 Long Beach Boulevard

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Page 252: pdfs.semanticscholar.org€¦ · Evaluation of the Cone Penetrometer for liquefaction Hazard Assessment Geoffrey R. Martin and Bruce J. Douglas Fugro, Inc. 3777 Long Beach Boulevard

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Page 253: pdfs.semanticscholar.org€¦ · Evaluation of the Cone Penetrometer for liquefaction Hazard Assessment Geoffrey R. Martin and Bruce J. Douglas Fugro, Inc. 3777 Long Beach Boulevard

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Page 254: pdfs.semanticscholar.org€¦ · Evaluation of the Cone Penetrometer for liquefaction Hazard Assessment Geoffrey R. Martin and Bruce J. Douglas Fugro, Inc. 3777 Long Beach Boulevard

FRICTieN RESISTRNCE.

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Page 255: pdfs.semanticscholar.org€¦ · Evaluation of the Cone Penetrometer for liquefaction Hazard Assessment Geoffrey R. Martin and Bruce J. Douglas Fugro, Inc. 3777 Long Beach Boulevard

FRICTI8N RESISTRNCE.

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Page 256: pdfs.semanticscholar.org€¦ · Evaluation of the Cone Penetrometer for liquefaction Hazard Assessment Geoffrey R. Martin and Bruce J. Douglas Fugro, Inc. 3777 Long Beach Boulevard

75.00DEPTH IN FEET

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Page 257: pdfs.semanticscholar.org€¦ · Evaluation of the Cone Penetrometer for liquefaction Hazard Assessment Geoffrey R. Martin and Bruce J. Douglas Fugro, Inc. 3777 Long Beach Boulevard

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Page 258: pdfs.semanticscholar.org€¦ · Evaluation of the Cone Penetrometer for liquefaction Hazard Assessment Geoffrey R. Martin and Bruce J. Douglas Fugro, Inc. 3777 Long Beach Boulevard

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Page 259: pdfs.semanticscholar.org€¦ · Evaluation of the Cone Penetrometer for liquefaction Hazard Assessment Geoffrey R. Martin and Bruce J. Douglas Fugro, Inc. 3777 Long Beach Boulevard

FRICTI0N RESISTRNCE, TS

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Page 260: pdfs.semanticscholar.org€¦ · Evaluation of the Cone Penetrometer for liquefaction Hazard Assessment Geoffrey R. Martin and Bruce J. Douglas Fugro, Inc. 3777 Long Beach Boulevard

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Page 261: pdfs.semanticscholar.org€¦ · Evaluation of the Cone Penetrometer for liquefaction Hazard Assessment Geoffrey R. Martin and Bruce J. Douglas Fugro, Inc. 3777 Long Beach Boulevard

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Page 262: pdfs.semanticscholar.org€¦ · Evaluation of the Cone Penetrometer for liquefaction Hazard Assessment Geoffrey R. Martin and Bruce J. Douglas Fugro, Inc. 3777 Long Beach Boulevard

75.00DEPTH IN FEET

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Page 263: pdfs.semanticscholar.org€¦ · Evaluation of the Cone Penetrometer for liquefaction Hazard Assessment Geoffrey R. Martin and Bruce J. Douglas Fugro, Inc. 3777 Long Beach Boulevard

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Page 264: pdfs.semanticscholar.org€¦ · Evaluation of the Cone Penetrometer for liquefaction Hazard Assessment Geoffrey R. Martin and Bruce J. Douglas Fugro, Inc. 3777 Long Beach Boulevard

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Page 265: pdfs.semanticscholar.org€¦ · Evaluation of the Cone Penetrometer for liquefaction Hazard Assessment Geoffrey R. Martin and Bruce J. Douglas Fugro, Inc. 3777 Long Beach Boulevard

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Page 266: pdfs.semanticscholar.org€¦ · Evaluation of the Cone Penetrometer for liquefaction Hazard Assessment Geoffrey R. Martin and Bruce J. Douglas Fugro, Inc. 3777 Long Beach Boulevard

o3

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Page 267: pdfs.semanticscholar.org€¦ · Evaluation of the Cone Penetrometer for liquefaction Hazard Assessment Geoffrey R. Martin and Bruce J. Douglas Fugro, Inc. 3777 Long Beach Boulevard

FRICTI8N RE

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Page 268: pdfs.semanticscholar.org€¦ · Evaluation of the Cone Penetrometer for liquefaction Hazard Assessment Geoffrey R. Martin and Bruce J. Douglas Fugro, Inc. 3777 Long Beach Boulevard

FRICTIBN RE

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Page 269: pdfs.semanticscholar.org€¦ · Evaluation of the Cone Penetrometer for liquefaction Hazard Assessment Geoffrey R. Martin and Bruce J. Douglas Fugro, Inc. 3777 Long Beach Boulevard

FRIC

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Page 270: pdfs.semanticscholar.org€¦ · Evaluation of the Cone Penetrometer for liquefaction Hazard Assessment Geoffrey R. Martin and Bruce J. Douglas Fugro, Inc. 3777 Long Beach Boulevard

DEPTH IN

FEETo

10

-

20

30

70

80

| SAMPLE TYPE

PENETRATION DENSITY/ | RESISTANCE ( MOISTURE CONSISTENCY

s

T

s

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ELEVATION: DATE ORI EQUIPMENT USED: 5 7/8" ROTARY WASH WATER LEVEU 20-

FS] STANDARD HAMMER SPLIT SPOON ^" SAMPLf

[f] TRIP HAMMER SPLIT SPOON SAMPLE |

SOIL TYPE

SANDY SILT (ML) & SILTY SAND (SM). brown, uniform.

dark brown

SILTY SAND (SP-SM). dark brown, fine to coarse, nonplastic. ( some fine gravels

SILTY CLAY (CL). light brown, medium plasticity, some

SILTY SAND (SM), brown, fine sands, uniform, mica

sands, wet

SILTY SAND (SP-SM), dirk brown with dark gray from 35' to 41'. fine to coarse sands, fine gravels with a layer of sandy

SANDY GRAVEL (GP). brown, fine to medium gravels.medium to coarse sands

SILTY CLAY (CL), brown, medium plesticity, occasional

SILTY SAND - SANDY SILT (SM-ML), brown, fine sands, uniform, nonplastic

BORING TERMINATED AT 61*

LLED: 11-16-79 f v PROJECThmGR^J

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1

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SAN JOSE SITE: COYOTE NORTH

9-80 FIGURE A.84

Page 271: pdfs.semanticscholar.org€¦ · Evaluation of the Cone Penetrometer for liquefaction Hazard Assessment Geoffrey R. Martin and Bruce J. Douglas Fugro, Inc. 3777 Long Beach Boulevard

DEPTH IN

FEET

0 f-

10

20

30

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| SAMPLE TYPE

PENETRATION DENSITY/ , RESISTANCE MOISTURE CONSISTENCY

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ELEVATION: DATE DRI EQUIPMENT USED: 5 7/8" ROTARY WASH WATER LEVEL: 20-f?j STANDARD HAMMER SPLIT SPOON ^ w SAMPLE

frj TRIP HAMMER SPLIT SPOON SAMPLE (

SOIL TYPE

SILTY SAND (SM), brown, uniform, fine sands, non-plastic

SILTY CLAY (CL), dark brown, medium plasticity

t kSILTY SAND (SM), brown, uniform fine sands

SAND (SP-SM), brown to dark brown, fine to medium sands.

SANDY G RAVEL (GP), dark brown to dark grey, fine to

SILTY CLAY (CL), brown, medium plasticity, occasional fine sands

4

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9-80 FIGURE A.8S

Page 272: pdfs.semanticscholar.org€¦ · Evaluation of the Cone Penetrometer for liquefaction Hazard Assessment Geoffrey R. Martin and Bruce J. Douglas Fugro, Inc. 3777 Long Beach Boulevard

DEPTH SAMPLE TYPE

-'_ PENETRATION DENSITY/ee " . RESISTANCE MOISTURE CONSISTENCY0 L-i-1 ' ' '

10

20

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nr>

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SANDY SILT (ML) & SILTY non-plastic

SILTY CLAY (CL). brown, m sands

SOIL TYPE

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edium plasticity, some fine

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GRAVELLY SAND (SP), dart sands, fine gravels

SANDY GRAVEL (GP), dark fine to coarse sands

BORING TERMINATED AT

ELEVATION: DATE DRILLED: 11-17-79 EQUIPMENT USED: 5 7/8" ROTARY WASHWATER LEVEL: 20* t

fsl STANDARD HAMMER SPLIT SPOON ^ *200 SIEVE *-* SAMPLE

[f| TRIP HAMMER SPLIT SPOON SAMPLE £ 0.002mm

PERCENT PASSING | | 1

20 40

......... ---I- ------

c brown, medium to coarse I

45'

\

.

/ \ PROJECT

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60 80

1

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LOG OF BORING NO. 3 SAN JOSE SITE: COYOTE NORTH

940 FIGURE A.86

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DEPTH I SAMPLE TYPE

IN I _ " PENETRATION DENSITY/ 1-661 1 RESISTANCE MOISTURE CONSISTENCYo L.LJ i i i

10

20

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50

80

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36

19

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V

SOIL TYPE

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SILTY CLAY (CL), brown, m

SILTY SAND (SM), brown tc graded, some medium sands a

1

> dark brown, fine sands, poorlyt 26' . . _,

GRAVELLY SAND (SP), dark brown, fine to coarse sands, fine gravels

SANDY GRAVEL (GP), dark gravels, fine to coarse sands

gray to dark brown, fine

BORING TERMINATED AT 45

ELEVATION: DATE DRILLED: 11-15-79 EQUIPMENT USED: 9 7/9" ROTARY WASH WATER LEVEL: W [si STAND ARO HAMMER SPLIT SPOON A #20O SIEVE1 1 SAMPLE

[f] TRIP HAMMER SPLIT SPOON SAMPLE £ 0.002mm

1

_

^^ ^^ ^ ^^ ^^^^v u

PERCENT PASSING 1 1 1 I

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79-163

LOG OF BORING NO. 4 SAN JOSE SITE: COYOTE NORTH

9-80 FIGURE A.87

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DEPTH p SAMPLE TYPE

ccer PENETRATION DENSITY/ F" T | RESISTANCE MOISTURE CONSISTENCY

10

20

-

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fin

70

80

T

T

T

T

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11

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SANDY SILT (ML) & SILTY uniform, non-plastic

CLAYEY SANDY SILT (ML) plasticity, fine sands

SILTY SAND (SM). brown w fine sands, trace of low plastic

GRAVELLY SAND (SP), dar coarse sands, fine gravels to 1

GRAVELLY SAND-SANDY

SOIL TYPE

SAND (SM), brown, fin».

. brown with gray mottled, low

: fines

'size

GRAVEL (SP-GP). dark graymedium to coarse sands, fine gravels.

SILTY CLAY (CL). brown, nr trace of fine sands

BORING TERMINATED AT

ELEVATION: DATE DRILLED: 11-20-79 EQUIPMENT USED*. 5 7/8" ROTARY WASH WATER LEVEL: 20 [51 STAND AMD HAMMER SPLIT SPOON ^ *2OO SIEVEv-1 SAMPLE

[7] TRIP HAMMER SPLIT SPOON SAMPLE f O.OO2 mm

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1

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/ <t PROJECT »>

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PERCENT PASSING

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3K

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==

tO.:

USGSCPT-SPT

--- --ii-

79-1 S3

LOG OF BORING NO. 6 SAN JOSE SITE: COYOTE NORTH

9-80 FIGURE A.88

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DEPTH ( SAMPLE TYPE

IN !CCCT PENETRATION DENSITY/*" ttr 1 RESISTANCE MOISTURE CONSISTENCYo L-L-^ '

-

10

20

30

40

50

60

70

80

S

S

S

S

S

S

"s~

S

IT

S

S

S

7

6

0

1H

16

8

18

11

82

38

46

53

V

SANDY SILT (ML), brown, f medium sands

PERCE | t

SOIL TYPE 20 4(

ine sands, non-plastic occasional

:,::::::::CLAYEY SANDY SILT (ML), brown to gray, low plasticity ......--.. fine sands, occasional medium sands

SILTY SAND (SM), gray, fini plastic fines above 20'

GRAVELLY SAND (SP), da to coarse sands, fina gravels tc

GRAVELLY SAND-SANDY coarse sands, fine gravels

BORING TERMINATED AT

»

ELEVATION: DATE DRILLED; 11-2179 EQUIPMENT USED: 5 7/8" ROTARY WASH WATER LEVEL: *& [i] STANDARD HAMMER SPLIT SPOON A f 200 SIEVE

SAMPLE

|T] TRIP HAMMER SPLIT SPOON SAMPLE f 0.003 mm

rk brown to dark gray, medium»1"size ..........

A

GRAVEL (SP-GP), dark gray.

44.6' ..........

-

hmoR^ ^^^^^* USGSCPT

NT PASSING 1 ,

) 60 80

ft

I

79-153

SPT

LOG OF BORING NO. 8 SAN JOSE SITE: COYOTE NORTH

9-80 FIGURE A.89

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DEPTH SAMPLE TYPE

ecer PENETRATION DENSITY/ pttl , RESISTANCE MOISTURE CONSISTENCYo. -2-1 ' ' '

10

20

30 -

4Q

_

50

*

80

S

S

S

S

S

S

S

"s~

S

S

S

S

S

S

S

S

S

S

7

8

4

0

0

13

33

50

12

11

58

96

55

54

69

16

25

33

23

V

SILTY SAND (SM), dark bro* PI fines at 8'

CLAYEY SILT (ML), dark br fine sands

SOIL TYPE

nin, fine, uniform, trace af low

own, low plasticity, trace of

SILTY SAND (SM) and CLAYEY SILT (ML), dark brown fine, nonplastic

SANDY GRAVEL (GP), dark medium to coarse sands

brown, fine to medium gravels

CLAYEY SILT (ML-CL). brown, low plasticity

GRAVELLY SAND (SP), dar to medium gravels

k brown, coarse sands, fine

<

SAND (SP-SM). dark gray, fine, occasional fine gravels ^

SANDY GRAVEL (GP). dark coarse sands

SILTY CLAY (CL), brown, m fine sands.

-

BORING TERMINATED AT 6O*

ELEVATION: DATE DRILLED: 11-19-79 EQUIPMENT USED: S 7/8" ROT ARY WASH WATER LEVEL: ***f?| STANDARD HAMMfR SPLIT SPOON A f2OOSIEVE -1 SAMPLI :ii _

[?] TRIP HAMMfR SPLIT SPOON SAMPLE 0 0.002mm

PERCENT PASSING | | . I

20 40 ::f

iyTfl

iiii

i

1

1

O- -------

._......

60 80

i

...... _

1

\.

NO.: 79-163

USGSCPT-SPT

LOG OF BORING NO. 1 SAN JOSE SITE: COYOTE SOUTH

9-80 FIGURE A.9O

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DEPTH IN

FEET_

10

20

-

4O

.

60

m

80

r SAMPLE TYPE

PENETRATION DENSITY/ RESISTANCE MOISTURE CONSISTENCY

T

T

T

T~

T

T

T

T

T

0

9

21

23

7

25

33

43

18

V

ELEVATION: DATE DRI EQUIPMENT USED: 5 7/8" ROTARY WASH WATER LEVEL: ir

LH **>ANO ARO HAMME R SPLIT SPOON *

1 QTI«P HAMMER SPLIT SPOON SAMPLE (

SOIL TYPE

SILTY SAND (SM), dark brown, non-plastic, fine sands

SILT (ML), brown with fine sands, low PI, color change to

SILTY SAND (SM). dark brown, fine, nonplastic

SANDY GRAVEL (GP), dark brown to dark gray, fine tomedium gravel, medium to coarse sands

CLAYEY SILT (ML-CL), brown, low plasticity

GRAVELLY SAND (SP), dark grayish brown, medium tocoarse sands, fin* gravels

SAND (SP), dark gray, uniform fine to medium sands

SANDY G RAVEL (GP & GP-SP). dark grayish brown todark gray, fine to medium gravels, medium to coarse sand

BORING TERMINATED AT 46'V

-

,

LLED: 11-19-79 f p. % PROJECT N

PERCENT PASSING I I I |

20 40 60 80

;

O.:

USGSCPT-SPT

A

79-153

I o.oo2mm LOG OF BORING NO. 2 SAN JOSE SITE: COYOTE SOUTH

9-80 FIGURE A.91

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DEPTH IN

FEET

0

10

20

30

40

RA

aft

70

80

1 SAMPLE TYPE

PENETRATION DENSITY/ RESISTANCE MOISTURE CONSISTENCY

T

"s~

s

T

s

s

T

s

6

6

43

54

14

100

62

77

V

ELEVATION: DATE DRIEQUIPMENT USED: ft 7/8" ROTARY WASH

WATER LEVEL: 18*

[¥1 STANDARD HAMMER SPLIT SPOON ^ U- ' SAMPLE

[T] TRIP HAMMER SPLIT SPOON SAMPLE (

SOIL TYPE

SANDY SILT (ML), brown, uniform, fine sands, non-plasticsilt

CLAYEY SILT (ML & ML-CL), dark brown, low plasticity, trace of fine sands

SILTY CLAY (CL), dark gray, medium plasticitySAND (SP), dark grayish brown, fine to coarse sands, , I some fine gravels 'SANDY GRAVEL - GRAVELLY SAND (SP-GP), dark gray, medium to coarse sands, fine to medium gravels

SILTY CLAY (CL), dark grayish brown, trace of fine sands.

SANDY GRAVEL (SP). dark brown, fine to medium gravels medium to coarse sands

SAND (SP- SM), dark grayish brown, fine uniform 4 1

SANDY GRAVEL (GP), dark greyish brown, fine to medium .gravels, medium to coarse sands

BORING TERMINATED AT 45'

<

.

LLED: 11-19-79 r"r """ 1 PROJECT *

PERCENT PASSING | . . . 1

20

:......

....,,1

40 60

10.:

USGSCPT-SPT

80

i k

.....|_

A\.

i

79153

> 0.002 mm LOG OF BORING NO. 7 SAN JOSE SITE: COYOTE SOUTH

9-80 FIGURE A.92

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DEPTH IN

FEET 0

JO

20

30

40

50

6O

70

80

| SAMPLE TYPE

PENETRATION DENSITY/ j RESISTANCE MOISTURE CONSISTENCY

T_

T

T

T_

T

T

T

T

4

4

26

15

12

37

27

40

T

ELEVATION: DATE DRIEQUIPMENT USED: 6 7/»" ROT A^V WASH

WATER LEVEL: ta­

rsi STANDARD HAMMER SPLIT SPOON & ^ * SAMPLE[T] TRIP HAMMER SPLIT SPOON SAMPLE f

SOIL TYPE

SANDY SILT (ML), brown, fine sands, non-plastic

o0-

CLAYEY SILT (ML), dark brown, low plasticity, trace of

SILTY CLAY (CD, dark gray, medium plasticity

SANDY SILTY SAND (SP-SM), dark brown, fine to medium

n ^

SILTY CLAY (CD, brown, low plasticity, occasional finesands

SILTY SAND (SM), dark gray, fine sands, trace of low PI fines

GRAVELLY SAND (SP), dark brown, fine to medium Ol" gravels, medium to coarse sands

SAND (SP-SM). dark grayish brown, fine to medium

SANDY G RAVEL (GP). dark brown, fin* to medium gravels, . . . Jmedium to coarse sends

BORING TERMINATED AT 45' '--"

<

LLED: 11-20-79 r~r: \PROJECTNO.: l-ftiORO 1

HUH

PERCENT PASSING H , . . I

20 40 60 80

GSCPT-SFT

1

79-1 S3

> o.ooa mm LOG OF BORING NO. 8 SAN JOSE SITE: COYOTE SOUTH

9-80 FIGURE A.93

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APPENDIX B

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NUMBE RS ON POINTS REPRESENT F RICTION RATIO, %

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r~ \PHOJECTNO.: 79-163

LJUHJIHB JLJSGS CPT-SPT

SAftDIEGOSITE: N AS NORTH ISLAND VN VS DEPTH BY LAYER AVERAGES

9-8O FIGURE B.I

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1

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NUMBERS ON POINTS REPRESENT FRICTION RATIO. %

/ - NPROJbCT NO.: 79-lb3

rj^^^^^M

V^HIH USGS CPT-SPT

SALINASSITEQc/N VS DEPTH BY LAYER AVERAGES

9-80 FIGURE B.2

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NUMBERS ON POINTS REPRESENT FRICTION RATIO. %

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f""^ "' " "" "\ PROJECT NO.: /9-1b3r"l^[OW^MUHlliHI USGS CPT-SPT

MOSS LANDING SITE qc/R VS DEPTH BY LAYER AVERAGES

9-80 FIGURE B.3

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NUMBERS ON POINTS REPRESENT FRICTION RATIO. %

f "'^.'" ""~^ PROJECT NO.: /9-1b3

MB^HB USGS CPT-SPT

SAN JOSE SITE:COYOTE NORTH AND SOUTH

qc/R VS DEPTH BY LAYER AVERAGES

9-80 FIGURE B.4

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STANDARD HAMMER9-80 FIGURE B.7

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SAN JOSE SITE:COYOTE NORTH & SOUTH

Qc/N VS DEPTHSTANDARD HAMMER

9-80 FIGURE B.8

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9-80 FIGURE B.9

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TRIPHAMMERFIGURE B.11

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980 FIGURE B.12

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9-80 FIGURE B.13

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_SALINASSITE qc/N VS N BY LAYER AVERAGES

9-80 FIGURE B.14

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