Bolivia seismic properties k. rainer massarsch
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Transcript of Bolivia seismic properties k. rainer massarsch
Seismic Testing – Determination of Deformation Parameters
K. R. Massarsch Geo Risk & Vibration AB, Stockholm, Sweden
Overview • Introduction • Applications of seismic testing
o Seismic field testing o Compaction control o Deep soil mixing monitoring
• Small-strain shear modulus • Static shear modulus from seismic tests
o Strain-softening Effects
o Modulus Reduction • Conclusions
Application of Seismic Field Testing
• Acoustic emission monitoring (in rock and soil
• Monitoring of construction activities which generate ground vibrations (pile driving, blasting, ground improvement, traffic etc.)
• Control of foundation works by seismic methods (piling, ground improvement etc.)
• Determination of dynamic and cyclic soil and rock properties
• Determination of static soil and rock properties (modulus)
Reasons for Increased Use • Robustness of electronic systems for use at
construction sites (out of the office..) • Sensitive and less expensive vibration sensors
(airbags, computers) • Powerful data acquisition systems (storage
capacity, data handling) • Data transmission from construction site
(Mobile phone, Internet) • Powerful software for data analyses (music
industry) • Computer programs for advanced analyses
Seismic Field Testing Methods
• Seismic refraction • Surface waves (e.g. SASW, MASW) • Cross-hole • Down-hole o Seismic cone penetration testing
(SCPT) o Seismic dilatometer (SDMT)
• Seismic tomography
Vibration Emission from Vertically Oscillating Mass
Rayleigh Wave
Compression Wave
Shear Wave
FEM Simulation by Dr. W. Haupt, Karlsruhe
Surface Wave Test
x
y
Identification of Particle Motion during Surface Wave
Test x
y
Vertical
Horizontal
Vertical
Horizontal
Analyses and animation by Torben Kirk Wolf
Seismic Refraction Test
SASW Falling Weight Test
10 !
Falling Weight (1 ton, 1 m)
Geophone
Spectral Analysis of Surface Wave
Seismic Cross-‐‑hole Test
11
Vibration Source Vertical or Horizontal Geophone
Seismic Down-‐‑hole Test
Evaluation Methods
› First arrival › Peak to peak › Cross-over › Cross correlation
Testing of Mixed-‐‑in Place Columns
Injection of dry cement in soft clay
Mixing tool
Determination of Soil and Column Stiffness
Load distribution between soil and columns depends on relative stiffness
Dry Mixed-‐‑in-‐‑Place Column
Transducer
Source
Amplifier
Oscilloscope Trigger
Det går Det går
Connecting Accelerometer
Insertion of Accelerometer into Measuring Tube
Soft Column
Accelerometer
Accelerometer
Seismic Down-‐‑hole Test in Soil Column
Seismic Monitoring of Vibro-‐‑compaction
Resonance Compaction, Map Ta Phut, Thailand
Compaction Control by Seismic Test
21
22
Seismic Tomography
Seismic Tomography
23
Shear Wave Speed before and after Compaction
Compaction
Before Compaction
Time, hours
Shear W
ave Sp
eed, m
/s
Determination of Small-‐‑Strain Soil Modulus from
Seismic Test
2max SG Cρ=
2max PM Cρ=
Small-Strain Shear Modulus from Shear Wave Speed
Confined Modulus from Compression Wave Speed
Modulus ratio for different values of Poisson’s ratio E = 2(1+ν )G M =
(1+ν )(1− 2ν )(1+ν )
E
Poisson’s ratio, ν is an important parameter – but which value should be chosen?
Relationship between S-‐‑wave and P-‐‑wave Speed
27
ν =cP2 − 2cS
2
2 cP2 − cS
2( )
Dry Soils Water-‐‑saturated Soils
ν is Strain-‐‑dependent!
28 From: Wojciech Sas, Katarzyna Gabryś, Alojzy Szymański (2013)
Seismic Testing
Poisson’s Ratio, ν is Strain-‐‑dependent
• At shear strain <10-3 %, Poisson’s ratio is approximately 0.15 – 0.20.
• Do not rely on P- and S-wave speed for determination of ν.
• Poisson’s ratio increases with increasing strain. • When shear strain > 10-1 %, Poisson’s ratio is
approximately 0.3 – 0.5. • Poisson’s ratio depends on drainage condition
(ν ≈ 0.5 at undrained loading).
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Shear Modulus Variation with Depth and Void Ratio
Shear Strain
Shear S
tress
Effect of Strain on Soil Modulus
Shear Stress
Deformation
Shear Modulus
Deformation
Shear Modulus Decrease with Shear Strain
Clay
Sand Rm
= G
* / G
max
Shear Strain
Relativ
e Stiffness. G
/Gmax Modulus Reduction
Factor: RM = G/Gmax
Effect of Shear Strain on Shear Modulus
Effect of Shear Strain on Soil Modulus
35
0.50 %
Cohesive Soils
Non-‐‑cohesive Soils
R M = G/G
max
0.1 % 0.25 %
Modulus Reduction Factor Mod
ulus Red
uctio
n Factor, R
M
Modulus Reduction Factor, RM at 0.5 % shear strain
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RM = 0.0043 PI + 0.103
Effect of Degree of Saturation
RM = 0.0003 Sr + 0.1069
Effect of Void Ratio RM = 0.11 e+ 0.063
DENSE VERY DENSE COMPACT LOOSE
Effect of Strain Rate • Strain rate at seismic field test ≈ 0.0005 to
0.005 %/s. • Strain rate at static triaxial (CU) test ≈
0.0003 %/s • Resonant column tests (50 Hz) and
torsional shear tests (one week) give same shear modulus, Gmax
• Strain rate at seismic tests comparable to static laboratory tests
• Shear modulus not (strongly) affected by strain rate 40
Determination of Static Modulus from Seismic Test 1. Determine Gmax from cS. 2. Use effective (dry) density of material to
calculate Gmax?! 3. Calculate small strain moduli, (Emax, Mmax)
using small-strain Poisson’s ratio, ν. 4. Estimate static shear modulus, GS by
applying modulus reduction factor, RM. 5. Calculate Emax, Mmax using large-strain
Poisson’s ratio, ν. 41
Static Modulus from Seismic Test
42
GS = RM Gmax
0.5 %
Conclusions • Seismic field and laboratory testing has
gained increasing use in geotechnical and earthquake engineering
• Seismic field testing can reliably determine wave speed in soil and rock
• Wave speed can be correlated to deformation modulus (rock or soil)
• Small-strain shear modulus can be correlated to static shear modulus applying modulus degradation
• Increasing potential for seismic methods in geotechnical and civil engineering, especially for field monitoring.
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