2011 PE Review: Michael C. Hirschi, PhD, PE, D.WRE Professor and Assistant Dean University of...

97
2011 PE Review: Michael C. Hirschi, PhD, PE, D.WRE Professor and Assistant Dean University of Illinois [email protected]

Transcript of 2011 PE Review: Michael C. Hirschi, PhD, PE, D.WRE Professor and Assistant Dean University of...

Page 1: 2011 PE Review: Michael C. Hirschi, PhD, PE, D.WRE Professor and Assistant Dean University of Illinois mch@illinois.edu.

2011 PE Review:

Michael C. Hirschi, PhD, PE, D.WREProfessor and Assistant Dean

University of [email protected]

Page 2: 2011 PE Review: Michael C. Hirschi, PhD, PE, D.WRE Professor and Assistant Dean University of Illinois mch@illinois.edu.

Acknowledgements:

Rod Huffman, PE Review coordinatorDaniel Yoder (2006 presenter)

Rabi Mohtar & Majdi Abu Najm (2010 presenters)

Page 3: 2011 PE Review: Michael C. Hirschi, PhD, PE, D.WRE Professor and Assistant Dean University of Illinois mch@illinois.edu.

Topics

• Principles of Soil Physics (some duplication with Management session)

• Soil Strength & Mechanics

• Sediment Transport

• Erosion Control

• Slope Stabilization

Page 4: 2011 PE Review: Michael C. Hirschi, PhD, PE, D.WRE Professor and Assistant Dean University of Illinois mch@illinois.edu.

Sources

• Environmental Soil Physics; Hillel; 1998 Hi• Essentials of Soil Mechanics & Foundations, 2nd ed.;

McCarthy; 1982; M• Soil and Water Conservation Engineering

– 4th ed. Schwab, Fangmeier, Elliott, Frevert: S4– 5th ed. Fangmeier, Elliott, Workman, Huffman, Schwab: S5

• Design Hydrology & Sedimentology for Small Catchments; Haan, Barfield, Hayes: H

• USLE/RUSLE Handout: HO

Page 5: 2011 PE Review: Michael C. Hirschi, PhD, PE, D.WRE Professor and Assistant Dean University of Illinois mch@illinois.edu.

Soil Physics & Mechanics

• Soil classes and particle size distributions

• Soil water– Content– Potential– Flow

• Soil strength & mechanics

Page 6: 2011 PE Review: Michael C. Hirschi, PhD, PE, D.WRE Professor and Assistant Dean University of Illinois mch@illinois.edu.

Soil classes & particle sizes

Hi.61

Page 7: 2011 PE Review: Michael C. Hirschi, PhD, PE, D.WRE Professor and Assistant Dean University of Illinois mch@illinois.edu.

Soil classes & particle sizes - 2

• ISSS easiest– Sand 0.02-2.0mm (20-2000μ)– Silt 0.002-0.02mm (2-20μ)– Clay <0.002mm (<2μ)

• Soil texture classes based on USDA– Sand 0.05-2.0mm– Silt 0.002-0.05mm– Clay <0.002mm

Page 8: 2011 PE Review: Michael C. Hirschi, PhD, PE, D.WRE Professor and Assistant Dean University of Illinois mch@illinois.edu.

Soil classes & particle sizes – 3

• Texture– EX: 50% sand,

20% silt

30% clay?

Hi.64

Page 9: 2011 PE Review: Michael C. Hirschi, PhD, PE, D.WRE Professor and Assistant Dean University of Illinois mch@illinois.edu.

Soil classes & particle sizes – 4

• Particle size distribution– EX: draw in a sandy clay loam?

Hi.65

Page 10: 2011 PE Review: Michael C. Hirschi, PhD, PE, D.WRE Professor and Assistant Dean University of Illinois mch@illinois.edu.

Soil water content

• Mt = Ms + Mw + Ma

• Vt = Vs + Vw + Va

– t = total, s = solids, w = water, a = air

• ρb = bulk density = Ms/Vt≈ 1.1-1.4 g/cc

• ρp = particle density = Ms/Vs ≈ 2.65 g/cc

• Porosity = (Vw + Va) / Vt ≈ 25-60%

• ρw = water density = Mw/Vw = 1.0 g/cc

0

Page 11: 2011 PE Review: Michael C. Hirschi, PhD, PE, D.WRE Professor and Assistant Dean University of Illinois mch@illinois.edu.

Soil water content – 2

• ww = Mw / (Ms + Mw)

– Water content wet basis

• w = mass wetness = Mw / Ms

– Water content dry basis

• θ = Vw/Vt = Vw / (Vs + Vw + Va)

– Volumetric water content

Page 12: 2011 PE Review: Michael C. Hirschi, PhD, PE, D.WRE Professor and Assistant Dean University of Illinois mch@illinois.edu.

Calc.: soil water content

• Given:– Soil with 30% water content dry basis

• Find:– Best guess at equivalent inches of water in the top

foot of soil?

Page 13: 2011 PE Review: Michael C. Hirschi, PhD, PE, D.WRE Professor and Assistant Dean University of Illinois mch@illinois.edu.

Calc.: soil water content – 2

• Mw / Ms = 0.30– Mw = Vw * ρw

– ρb = Ms / Vt; Ms = Vt * ρb

Page 14: 2011 PE Review: Michael C. Hirschi, PhD, PE, D.WRE Professor and Assistant Dean University of Illinois mch@illinois.edu.

Calc.: soil water content – 3

• Mw / Ms = 0.30– Mw = Vw * ρw

– ρb = Ms / Vt; Ms = Vt * ρb

– Mw / Ms = (Vw * ρw)/(Vt * ρb) = (Vw / Vt)(ρw / ρb)

– θ = Vw/Vt

– θ *(ρw / ρb) = 0.3; θ = (ρb / ρw) * 0.3

– θ = 0.3 *(1.3/1.0) = 0.39– 0.39 * 1 ft * 12”/ft = 4.7”

Page 15: 2011 PE Review: Michael C. Hirschi, PhD, PE, D.WRE Professor and Assistant Dean University of Illinois mch@illinois.edu.

Soil water potential

Hi.157

Page 16: 2011 PE Review: Michael C. Hirschi, PhD, PE, D.WRE Professor and Assistant Dean University of Illinois mch@illinois.edu.

Soil water potential – 2

Cuenca.58

Page 17: 2011 PE Review: Michael C. Hirschi, PhD, PE, D.WRE Professor and Assistant Dean University of Illinois mch@illinois.edu.

Soil water potential – 3

S5.337

Page 18: 2011 PE Review: Michael C. Hirschi, PhD, PE, D.WRE Professor and Assistant Dean University of Illinois mch@illinois.edu.

Soil water potential – 4

Hi.162

Page 19: 2011 PE Review: Michael C. Hirschi, PhD, PE, D.WRE Professor and Assistant Dean University of Illinois mch@illinois.edu.

Calc.: soil water potential

• Given:– Mercury tensiometer

• SG = 13.6

– Situation as shown

• Find:– Total potential at C– Above or below water table?

Cuenca.64

Page 20: 2011 PE Review: Michael C. Hirschi, PhD, PE, D.WRE Professor and Assistant Dean University of Illinois mch@illinois.edu.

Calc.: soil water potential - 2

• 1) pick datum• 2) add pressures

– Suction– Water depth– Gravity

• T = z + p + pos

– = -86cm– Above water table

Page 21: 2011 PE Review: Michael C. Hirschi, PhD, PE, D.WRE Professor and Assistant Dean University of Illinois mch@illinois.edu.

Soil water flow

• q = A*K*H/L– K = (q*L)/(A*H)

• K values S4.359; S5.261; H.430

A

q

LH

Page 22: 2011 PE Review: Michael C. Hirschi, PhD, PE, D.WRE Professor and Assistant Dean University of Illinois mch@illinois.edu.

Calc.: soil water flow

• Given:– Need 50000 gpd through a 1-ft thick sand filter

with K = 8 ft/d, and a total driving head of 3 ft

• Find :– Required diameter for circular tank?

Page 23: 2011 PE Review: Michael C. Hirschi, PhD, PE, D.WRE Professor and Assistant Dean University of Illinois mch@illinois.edu.

Calc.: soil water flow – 2

• q = A*K*H/L; A = (q*L)/(K*H)2

3

278481.7

1

3

1

81

150000ft

gal

ft

ftft

dayft

day

galA

ftA

d 184

Page 24: 2011 PE Review: Michael C. Hirschi, PhD, PE, D.WRE Professor and Assistant Dean University of Illinois mch@illinois.edu.

Soil strength and mechanics

• M.233-237,373-379• Soil stresses

– Normal = Fn/A = σ

– Shear = Ft/A = τ• Fn = normal force

• Ft = tangential or shear force

– As σ ↑ τ to cause failure = τf↑

– tan Φ = τf / σ; Φ = angle of internal friction

Page 25: 2011 PE Review: Michael C. Hirschi, PhD, PE, D.WRE Professor and Assistant Dean University of Illinois mch@illinois.edu.

Soil strength and mechanics – 2

M.234

Page 26: 2011 PE Review: Michael C. Hirschi, PhD, PE, D.WRE Professor and Assistant Dean University of Illinois mch@illinois.edu.

Calc.: soil strength

• Given:– Well-graded sand; density 124 lb/ft3

• Find:– Ultimate shear strength 6 ft below surface?

Page 27: 2011 PE Review: Michael C. Hirschi, PhD, PE, D.WRE Professor and Assistant Dean University of Illinois mch@illinois.edu.

Calc.: soil strength – 2

• From table, for well-graded sand, Φ = 32-35o = 33.5o

• Normal stress = (124 lb/ft3)(6 ft) = 744 lb/ft2

• tan Φ = τf / σ; τf = σ * tan Φ =

τf = 744 lb/ft2 * tan(33.5o) = 492 lb/ft2

Page 28: 2011 PE Review: Michael C. Hirschi, PhD, PE, D.WRE Professor and Assistant Dean University of Illinois mch@illinois.edu.

Footing bearing loads

• M.374-379• qult = a1*c*Nc + a2*B*γ1*Nγ + γ2*Df*Nq

– c = soil cohesion beneath footer– γ1,, γ2 = effective soil unit weight

above and below footer– B = footer size term– Nc, Nγ, Nq = capacity factors– Df = footing depth below surface

• qdesign = qult / FS

Length/width B a1 a2

1 (square) Width 1.2 0.42

2 Width 1.12 0.45

3 Width 1.07 0.46

4 Width 1.05 0.47

6 Width 1.03 0.48

Strip Width 1.00 0.50

Circular Radius 1.2 0.60

Page 29: 2011 PE Review: Michael C. Hirschi, PhD, PE, D.WRE Professor and Assistant Dean University of Illinois mch@illinois.edu.

Footing bearing loads – 2

M.375

Page 30: 2011 PE Review: Michael C. Hirschi, PhD, PE, D.WRE Professor and Assistant Dean University of Illinois mch@illinois.edu.

Calc.: footing load

• Given:– Strip footing 3 ft wide– Wet soil with density of 125 lb/ft3

– Angle of internal friction = 30o

– Cohesive strength of 400 lb/ft2

– Use factor of safety of 3• Find:

– qdesign in lb/ft2

Page 31: 2011 PE Review: Michael C. Hirschi, PhD, PE, D.WRE Professor and Assistant Dean University of Illinois mch@illinois.edu.

Calc.: footing load – 2

• a1 = 1.0, a2 = 0.5, B = width = 3’• γ1 = 125/2 = 62.5 lb/ft3; γ2 = 125 lb/ft3

• c = 400 lb/ft2

• Nc = 30, Nγ = 18, Nq = 20

• qdesign = 23,700/3 = 7900 lb/ft2

2332

/700,23)20)(4(125

)18(5.62

)3)(5.0()30(400

)0.1( ftlbftft

lb

ft

lbft

ft

lbqult

Page 32: 2011 PE Review: Michael C. Hirschi, PhD, PE, D.WRE Professor and Assistant Dean University of Illinois mch@illinois.edu.

Soil compaction and density

• Soil compaction– Greater strength– Dependent on water content

• Proctor test– Pack soil into mold with pounding– Modified Proctor > 56000 ft-lbs

Page 33: 2011 PE Review: Michael C. Hirschi, PhD, PE, D.WRE Professor and Assistant Dean University of Illinois mch@illinois.edu.

The Erosion Process

• Soil erosion is a multi-step process:– Soil particle/aggregate detachment– Soil particle/aggregate transport– Soil particle/aggregate deposition

• There must be detachment and transport for erosion to occur

• Deposition (sedimentation) will occur somewhere downstream

Page 34: 2011 PE Review: Michael C. Hirschi, PhD, PE, D.WRE Professor and Assistant Dean University of Illinois mch@illinois.edu.

A little soils review…

• Soil primary particles:– Sand, 0.05mm to 2mm, 2.65 g/cc density– Silt, 0.002mm to 0.05mm, 2.65 g/cc– Clay, <0.002mm, 2.6 g/cc

• Soil aggregates, chemically/electrically bonded sets of primary particles:– Large, in the sand range, 1.6 g/cc– Small, in the large silt range, 1.8 g/cc

• These aggregate sizes are approximately those used in the CREAMS model (USDA-ARS)

Page 35: 2011 PE Review: Michael C. Hirschi, PhD, PE, D.WRE Professor and Assistant Dean University of Illinois mch@illinois.edu.

Detachment

• There are many sources of force and energy required to detach soil particles & aggregates:– Raindrop impact– Shallow surface flow shear– Concentrated flow shear– Many more, at larger scales

Page 36: 2011 PE Review: Michael C. Hirschi, PhD, PE, D.WRE Professor and Assistant Dean University of Illinois mch@illinois.edu.

Transportation

• Many of the same processes contribute force and energy for soil particle & aggregate transport:– Raindrop impact– Shallow surface flow– Concentrated surface flow– Channelized flow– Others

Page 37: 2011 PE Review: Michael C. Hirschi, PhD, PE, D.WRE Professor and Assistant Dean University of Illinois mch@illinois.edu.

Balancing act

• Foster & Meyer (1972) proposed a balance between detachment and transport for flowing water:

• 1 = (transport load/transport capacity) + (detachment load/detachment capacity)

Page 38: 2011 PE Review: Michael C. Hirschi, PhD, PE, D.WRE Professor and Assistant Dean University of Illinois mch@illinois.edu.

Essentially, if the flow is using all its transport capacity transporting sediment, there’s nothing left to detach more. Likewise, if the flow is detaching new sediment at detachment capacity, there’s no capacity to transport any sediment. Natural systems balance out…

Page 39: 2011 PE Review: Michael C. Hirschi, PhD, PE, D.WRE Professor and Assistant Dean University of Illinois mch@illinois.edu.

Example• In the 80’s and 90’s there was a successful push to

conservation tillage as a method to reduce sediment in lakes and streams

• In many situations, no improvement was seen, but streambank erosion became more of a problem than it was in the past

• I contend that now that the streams are receiving cleaner water (because of less upland erosion), but at similar rates, from farm fields, the stream uses less of its erosive energy to transport load it receives from runoff water, so it has capacity to undercut banks and scour the streambed

Page 40: 2011 PE Review: Michael C. Hirschi, PhD, PE, D.WRE Professor and Assistant Dean University of Illinois mch@illinois.edu.

Multi-stage erosion

Page 41: 2011 PE Review: Michael C. Hirschi, PhD, PE, D.WRE Professor and Assistant Dean University of Illinois mch@illinois.edu.

Soil erosion and sediment yield

• Hillslope erosion• Channel system erosion• Sediment delivery to streams• Sediment transport in streams• Slope stability

Page 42: 2011 PE Review: Michael C. Hirschi, PhD, PE, D.WRE Professor and Assistant Dean University of Illinois mch@illinois.edu.

Hillslope soil erosion

• S4.91-111; S5.134-156; H.238-285• Background

– Detachment• Raindrop impact• By turbulent overland flow

– Runoff

– Transport downslope• By runoff

Page 43: 2011 PE Review: Michael C. Hirschi, PhD, PE, D.WRE Professor and Assistant Dean University of Illinois mch@illinois.edu.

Hillslope soil erosion background

• At the top of the slope– Detachment by raindrop impact– Transport by shallow sheet flow– Sheet erosion

USDA-NRCS

Page 44: 2011 PE Review: Michael C. Hirschi, PhD, PE, D.WRE Professor and Assistant Dean University of Illinois mch@illinois.edu.

Hillslope soil erosion background - 2

• Lower on slope– Small flow concentrations– Start to cut small channels– Rills

• Roughly parallel• Head straight downslope• Random formation

– Flow from sheet areas between rills– Sheet and rill erosion

USDA-NRCS

Page 45: 2011 PE Review: Michael C. Hirschi, PhD, PE, D.WRE Professor and Assistant Dean University of Illinois mch@illinois.edu.

Hillslope soil erosion background - 3

• Bottom of hillslope– Ends at concentrated flow channel– Low area in macrotopography– “ephemeral gullies”

USDA-NRCS

Page 46: 2011 PE Review: Michael C. Hirschi, PhD, PE, D.WRE Professor and Assistant Dean University of Illinois mch@illinois.edu.

Hillslope erosion factors• Rainfall erosivity

– Intensity– Total storm energy

• Soil erodibility• Topography

– Slope length– Steepness

• Management– Reduce local erosion– Change runoff path– Slow and spread runoff => deposition

Page 47: 2011 PE Review: Michael C. Hirschi, PhD, PE, D.WRE Professor and Assistant Dean University of Illinois mch@illinois.edu.

USLE/RUSLE

• A = R * K * LS * C * P• A = average annual soil erosion (T/A/Y)• R = rainfall erosivity (awful units)• K = soil erodibility (awful units)

– R * K gives units of T/A/Y

• LS = topographic factor (dimensionless)• C = cover-management (dimensionless)• P = conservation practice (dimensionless)

Page 48: 2011 PE Review: Michael C. Hirschi, PhD, PE, D.WRE Professor and Assistant Dean University of Illinois mch@illinois.edu.

USLE/RUSLE – background

• Empirical approach– >10000 plot-years of data– International use

• Unit Plot basis; LS = C = P = 1– Near worst-case management

• R from good fit rainfall-erosion• K from K = A / R• C and P from studies

– Subfactors in later versions

Page 49: 2011 PE Review: Michael C. Hirschi, PhD, PE, D.WRE Professor and Assistant Dean University of Illinois mch@illinois.edu.

USLE/RUSLE – approach

• Lookup– Maps, tables, figures– Databases

• Process-based calculations– Show changes over time– Where don’t have good data

Page 50: 2011 PE Review: Michael C. Hirschi, PhD, PE, D.WRE Professor and Assistant Dean University of Illinois mch@illinois.edu.

R factor – rainfall erosivity

• maps– H.251; H.Appendix 8A; S4.99(SI); S5.143(SI); HO.1-5– R(customary SI) = 17.02 * R(customary US)

S4

Page 51: 2011 PE Review: Michael C. Hirschi, PhD, PE, D.WRE Professor and Assistant Dean University of Illinois mch@illinois.edu.

K factor – soil erodibility

• Soil surveys, NASIS, H.261-262; HO.6• Erodibility nomograph

– H.255; S4.101; S5.144; HO.7– No short-term OM

Page 52: 2011 PE Review: Michael C. Hirschi, PhD, PE, D.WRE Professor and Assistant Dean University of Illinois mch@illinois.edu.

LS – topography factor

• New tables & figures– H.264; HO.8

• Know susceptibility to rilling– High for highly disturbed soils– Low for consolidated soils

Page 53: 2011 PE Review: Michael C. Hirschi, PhD, PE, D.WRE Professor and Assistant Dean University of Illinois mch@illinois.edu.

C – cover-management factor

• Part of normal management scheme• Lookup: S4.102; S5.146; H.266; H.Appendix 8;

HO.9• Change over time

Page 54: 2011 PE Review: Michael C. Hirschi, PhD, PE, D.WRE Professor and Assistant Dean University of Illinois mch@illinois.edu.

C – cover-management factor - 2

• Subfactor approach (RUSLE)– C = PLU * CC * SC * SR * SM; all 0-1

• PLU = prior land use– roots, buried biomass, soil consolidation

• CC = canopy cover; % cover & fall height• SC = exp(-b * % cover)

– B = 0.05 if rills dominant; 0.035 typical; 0.025 interrill

• SR = roughness; set by tillage, reduces over time• SM = soil moisture; used only in NWRR

Page 55: 2011 PE Review: Michael C. Hirschi, PhD, PE, D.WRE Professor and Assistant Dean University of Illinois mch@illinois.edu.

P – conservation practice factor

• Common practices– Contouring, stripcropping, terraces

• Change flow patterns or cause deposition• Lookup tables

– S4.103; S5.146; H.281; HO.10

Page 56: 2011 PE Review: Michael C. Hirschi, PhD, PE, D.WRE Professor and Assistant Dean University of Illinois mch@illinois.edu.

Calc.: USLE/RUSLE

• Given:– Materials in handout– 3-Acre construction site near Chicago– Straw mulch applied at 4 T/A– Average 20% slope, 100’ length– Loamy sand subsoil– Fill (loose soil)

• Find:– Erosion rate in T/A/Y

Page 57: 2011 PE Review: Michael C. Hirschi, PhD, PE, D.WRE Professor and Assistant Dean University of Illinois mch@illinois.edu.

Calc: USLE/RUSLE – 2

• R = 150 (HO.1)• K = 0.24 (HO.7)• LS = 4 (HO.8-high rilling)• C = 0.02 (HO.9)• P = 1.0• A = R * K * LS * C * P = 2.9 T/A/Y

Page 58: 2011 PE Review: Michael C. Hirschi, PhD, PE, D.WRE Professor and Assistant Dean University of Illinois mch@illinois.edu.

Calc: USLE/RUSLE – 2.1

• Given:– Materials in handout– 16-A site near Dallas, TX– Silty clay loam subsoil– Average 50% slope, 75’ length– Cut soil

• Find:– By what percentage will the erosion be reduced if we

increase our straw mulch cover from 40% cover to 80% cover?

Page 59: 2011 PE Review: Michael C. Hirschi, PhD, PE, D.WRE Professor and Assistant Dean University of Illinois mch@illinois.edu.

Calc: USLE/RUSLE – 2.2

• Only thing different is C– Only subfactor different is SC

• SC = exp(-b * %cover)– For consolidated soil, b = 0.025

• SC1 = exp(-0.025 * 40%) = 0.368

• SC2 = exp(-0.025 * 80%) = 0.135

• Reduction = (0.368 – 0.135)/0.368 = 63%

Page 60: 2011 PE Review: Michael C. Hirschi, PhD, PE, D.WRE Professor and Assistant Dean University of Illinois mch@illinois.edu.

Sediment delivery

• USLE/RUSLE for hillslopes– Erosion– Delivery

• Erosion critical for soil resource conservation

• Delivery critical for water quality– Movement through channel system

Page 61: 2011 PE Review: Michael C. Hirschi, PhD, PE, D.WRE Professor and Assistant Dean University of Illinois mch@illinois.edu.

Sediment delivery – 2

Page 62: 2011 PE Review: Michael C. Hirschi, PhD, PE, D.WRE Professor and Assistant Dean University of Illinois mch@illinois.edu.

Sediment delivery – 3

• SDR (Sediment Delivery Ratio)– Hillslope erosion– Empirical fit for watershed delivery

• Channel erosion/deposition modeling– Erosion– Transport– Deposition

Page 63: 2011 PE Review: Michael C. Hirschi, PhD, PE, D.WRE Professor and Assistant Dean University of Illinois mch@illinois.edu.

Sediment Delivery Ratio

• H.293-299• SDR = SY / HE

– SDR = sediment delivery ratio– SY = sediment yield at watershed exit– HE = hillslope erosion over watershed

Page 64: 2011 PE Review: Michael C. Hirschi, PhD, PE, D.WRE Professor and Assistant Dean University of Illinois mch@illinois.edu.

Sediment Delivery Ratio – 2

• Area-delivery relationship

H.294

Page 65: 2011 PE Review: Michael C. Hirschi, PhD, PE, D.WRE Professor and Assistant Dean University of Illinois mch@illinois.edu.

Sediment Delivery Ratio – 3

• Relief-length ratio– Relief = elev change along main branch– Length = length along main branch

H.294

Page 66: 2011 PE Review: Michael C. Hirschi, PhD, PE, D.WRE Professor and Assistant Dean University of Illinois mch@illinois.edu.

Sediment Delivery Ratio – 4

• Forest Service Delivery Index Method

H.295

Page 67: 2011 PE Review: Michael C. Hirschi, PhD, PE, D.WRE Professor and Assistant Dean University of Illinois mch@illinois.edu.

Sediment Delivery Ratio – 5

• MUSLE (H.298)– Y = 95(Q * qp)0.56 (Ka)(LSa)(Ca)(Pa)

• Y = storm yield in tons• Q = storm runoff volume in acre-in• q = peak runoff rate in cfs• K, LS, C, P = area=weighted watershed values

– SDR = 95(Q * qp)0.56/(R * area)• R = storm erosivity in US units

– Routing for channel delivery

Page 68: 2011 PE Review: Michael C. Hirschi, PhD, PE, D.WRE Professor and Assistant Dean University of Illinois mch@illinois.edu.

Calc: SDR

• Given:– Flow path length in watershed = 4000ft– Elevation difference = 115ft

• Find:– SDR

Page 69: 2011 PE Review: Michael C. Hirschi, PhD, PE, D.WRE Professor and Assistant Dean University of Illinois mch@illinois.edu.

Calc.: SDR – 2

• R/L = 115/4000 = 0.029• From figure SDR = 0.45

Page 70: 2011 PE Review: Michael C. Hirschi, PhD, PE, D.WRE Professor and Assistant Dean University of Illinois mch@illinois.edu.

Channel erosion-deposition modeling

• Process-based small channel models– Foster-Lane model

• H.285-289• Complicated and process-based

– Ephemeral Gully Erosion Model• EGEM• Fit to Foster-Lane Model results

Page 71: 2011 PE Review: Michael C. Hirschi, PhD, PE, D.WRE Professor and Assistant Dean University of Illinois mch@illinois.edu.

Channel erosion-deposition modeling – 2

• Large-channel models– Sediment transport– Channel morphology

Page 72: 2011 PE Review: Michael C. Hirschi, PhD, PE, D.WRE Professor and Assistant Dean University of Illinois mch@illinois.edu.

Sediment transport

• Settling (H.204-209)– Stokes’ Law

• Vs = settling velocity• d = particle diameter• g = accel due to gravity• SG = particle specific gravity• ν = kinematic viscosity

– Simplified Stokes’ Law• SG = 2.65• Quiescent water at 68oF• d in mm, Vs in fps

1

18

1 2

SGgd

Vs

281.2 dVs

Page 73: 2011 PE Review: Michael C. Hirschi, PhD, PE, D.WRE Professor and Assistant Dean University of Illinois mch@illinois.edu.

Calc.: Stokes’ Law settling

• Given:– ISSS soil particle size classification

• Find:– Settling velocities of largest sand, silt, and clay

particles

Page 74: 2011 PE Review: Michael C. Hirschi, PhD, PE, D.WRE Professor and Assistant Dean University of Illinois mch@illinois.edu.

Calc.: Stokes’ Law settling – 2

• ISSS classification– Largest particles size

• Clay = 0.002mm• Silt = 0.2mm• Sand = 2mm

– Vs,clay = 1.12*10-4 fps = 0.04 ft/hr = 0.97 ft/day

– Vs,silt = 0.11 fps = 405 ft/hr = 1.83 mi/day

– Vs,sand = 11.24 fps = 7.66 mph = 184 mi/day

Page 75: 2011 PE Review: Michael C. Hirschi, PhD, PE, D.WRE Professor and Assistant Dean University of Illinois mch@illinois.edu.

Calc.: Stokes’ Law settling

• Given:– Stokes’ Law settling

• Find: particles larger than what size can be assumed to settle 1 ft in one hour?

Page 76: 2011 PE Review: Michael C. Hirschi, PhD, PE, D.WRE Professor and Assistant Dean University of Illinois mch@illinois.edu.

Calc.: Stokes’ Law settling – 2

• Vs = [(1 ft)/(1 hr)](1 hr/3600s) = 2.778*10-4 fps

• d = (Vs/2.81)1/2 = 0.00994mm

Page 77: 2011 PE Review: Michael C. Hirschi, PhD, PE, D.WRE Professor and Assistant Dean University of Illinois mch@illinois.edu.

Other settling

• Flocculant, hindered, compression– Order of increasing concentration– Slower settling with increased conc.

• Settleable solids– Imhoff cone

H.211

Page 78: 2011 PE Review: Michael C. Hirschi, PhD, PE, D.WRE Professor and Assistant Dean University of Illinois mch@illinois.edu.

Sediment transport relationships

• H.223-233• Bedload

– Einstein equation

• Suspended load• Total load

– Yalin total load equation• Vavg, d, SG, r, т, тc

– Yang stream power relationship• Stream power instead of critical shear

Page 79: 2011 PE Review: Michael C. Hirschi, PhD, PE, D.WRE Professor and Assistant Dean University of Illinois mch@illinois.edu.

Channel morphology

• H.391-419• Channel cross-section

– Width B, depth D, avg. vel. U, suspended sediment load qs, flow rate q

– B = Ca * qa, D = Cb * qb, U = Cc * qc,

qs = Cd * qd

– Ca, Cb, Cc, Cd, a, b, c, d = fit coefficients & exponents

Page 80: 2011 PE Review: Michael C. Hirschi, PhD, PE, D.WRE Professor and Assistant Dean University of Illinois mch@illinois.edu.

Channel morphology – 2

• Channel-forming discharge– Greatest impact on channel itself– Return period ≈ 1.5 years

• Channel roughness

Page 81: 2011 PE Review: Michael C. Hirschi, PhD, PE, D.WRE Professor and Assistant Dean University of Illinois mch@illinois.edu.

Channel morphology – 3

• Channel regime– H.405-419

H.416

Page 82: 2011 PE Review: Michael C. Hirschi, PhD, PE, D.WRE Professor and Assistant Dean University of Illinois mch@illinois.edu.

Application of process knowledge to control

• Limit individual parts to limit whole– Limit detachment– Limit transport

• Enhance deposition strategically– Where damage is minimal– Where cleanup is possible

Page 83: 2011 PE Review: Michael C. Hirschi, PhD, PE, D.WRE Professor and Assistant Dean University of Illinois mch@illinois.edu.

Control of Soil Erosion by Water

• Detachment limiting strategies– Reduce raindrop impact (“Stop the Drops”)– Reduce runoff– Reduce detachment capacity of runoff– Increase soil resistance to erosive forces

• Transport limiting strategies– Reduce runoff volume– Reduce runoff transport capacity (“Slow the

Flow”)

Page 84: 2011 PE Review: Michael C. Hirschi, PhD, PE, D.WRE Professor and Assistant Dean University of Illinois mch@illinois.edu.

Example – No-Till• Detachment

– Raindrop impact detachment is very low due to high surface cover percentage

– Flow shear detachment is low due to low velocities caused by tortuous flow path

– Soil is resistant to erosion because of low disturbance• Transport

– Raindrop transport is limited by surface residue– Flow transport is limited by increased infiltration,

lessening runoff– Flow transport is further limited by small dams created by

surface residue

Page 85: 2011 PE Review: Michael C. Hirschi, PhD, PE, D.WRE Professor and Assistant Dean University of Illinois mch@illinois.edu.

Example – Mulch on newly seeded area

• Detachment– Raindrop impact detachment is very low due to high

surface cover percentage– Flow shear detachment is low due to low velocities caused

by tortuous flow path• Transport

– Raindrop transport is limited by surface residue– Flow transport is limited by increased infiltration,

lessening runoff– Flow transport is further limited by small dams created by

surface residue

Page 86: 2011 PE Review: Michael C. Hirschi, PhD, PE, D.WRE Professor and Assistant Dean University of Illinois mch@illinois.edu.

Comparison of no-till vs. mulch• Detachment

– Likely higher with mulch for same surface cover fraction because of higher soil disturbance for seedbed preparation

– Likely higher for no-till following dry years because amount of residue cover is dictated by prior year crop growth

• Transport– Likely higher for mulch, unless “cut” in because no-till

residue is effectively “cut” in during planting, at least for a small area, hopefully across slope

– Likely higher for mulch situation because seedbed prep likely reduced average aggregate diameter

Page 87: 2011 PE Review: Michael C. Hirschi, PhD, PE, D.WRE Professor and Assistant Dean University of Illinois mch@illinois.edu.

Control of Sediment in Runoff

• Reduce transport capacity of flow• Enhance deposition of sediment

Page 88: 2011 PE Review: Michael C. Hirschi, PhD, PE, D.WRE Professor and Assistant Dean University of Illinois mch@illinois.edu.

Reduce transport capacity

• Slow the flow– Barriers

• Must let water pass, though slowly• Must be flow-stable, even after use• Must be where maintenance is possible

– Reduce slope steepness• Channel must be of adequate capacity

• Increase infiltration

Page 89: 2011 PE Review: Michael C. Hirschi, PhD, PE, D.WRE Professor and Assistant Dean University of Illinois mch@illinois.edu.

Enhance deposition of sediment

• Use flocculant to increase sedimentation– Usually in sedimentation ponds when other

methods are not adequate– Expensive…

Page 90: 2011 PE Review: Michael C. Hirschi, PhD, PE, D.WRE Professor and Assistant Dean University of Illinois mch@illinois.edu.

90

Slope stability & failurePossible forms of Failure

McCarthy (1982) page 440

McCarthy (1982) page 437-455

I.B Mohtar

Page 91: 2011 PE Review: Michael C. Hirschi, PhD, PE, D.WRE Professor and Assistant Dean University of Illinois mch@illinois.edu.

91

Slope stability & failure – 2

• Terms– β=max. slope angle before sliding– Φ=angle of internal friction

• Cohesionless soil– tan(β) = tan(Φ)

– Saturated: tan(β) = (1/2)tan(Φ)

I.B Mohtar

Page 92: 2011 PE Review: Michael C. Hirschi, PhD, PE, D.WRE Professor and Assistant Dean University of Illinois mch@illinois.edu.

92

Slope stability & failure – 3

• Cohesive soil–γ*z*sin(β)*cos(β) = c + σ*tan(Φ)

• z = assumed depth• c = cohesive force• σ = effective compressive stress

–Rotational or sliding block

I.B Mohtar

Page 93: 2011 PE Review: Michael C. Hirschi, PhD, PE, D.WRE Professor and Assistant Dean University of Illinois mch@illinois.edu.

93

Slope stability & failure – 4For clay soil

For soil with cohesion and internal friction > 0

McCarthy (1982) page 474I.B Mohtar

Page 94: 2011 PE Review: Michael C. Hirschi, PhD, PE, D.WRE Professor and Assistant Dean University of Illinois mch@illinois.edu.

94

Slope stability & failure – 5

• Ns = c / (γ * Hmax)–c = cohesion force–γ = soil unit weight–Hmax = max depth without sliding

I.B Mohtar

Page 95: 2011 PE Review: Michael C. Hirschi, PhD, PE, D.WRE Professor and Assistant Dean University of Illinois mch@illinois.edu.

95

Calc.: slope stability

Example 8:• Given:

– Cohesion strength = 500 lb/ft2

– Unit weight = 110 lb/ft3

– Slope steepness = 50o

– Internal friction angle = 15o

• Find:– Max. slope height

I.B Mohtar

Page 96: 2011 PE Review: Michael C. Hirschi, PhD, PE, D.WRE Professor and Assistant Dean University of Illinois mch@illinois.edu.

96

Calc.: slope stability – 2

• Fig. b, φ = 15o, i = 50o

• Hmax = c / (γ * Ns) =

(500 lb/ft2)(1ft3/ 10)(1/ 0.095) = 48 ft

I.B Mohtar

Page 97: 2011 PE Review: Michael C. Hirschi, PhD, PE, D.WRE Professor and Assistant Dean University of Illinois mch@illinois.edu.

Questions?