chapter 3 soil mechanics part i

52
Priyantha Jayawickrama, Ph.D. Associate Professor Chapter 3: Soil Mechanics/Review Texas Tech University Department of Civil and Environmental Engineering

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Page 1: Chapter 3 Soil Mechanics Part I

Priyantha Jayawickrama,

Ph.D.Associate Professor

Chapter 3: Soil Mechanics/Review

Texas Tech UniversityDepartment of Civil and Environmental Engineering

Page 2: Chapter 3 Soil Mechanics Part I

CE 4321: Geotechnical Engineering Design

Chapter 3: Soil Mechanics

Lecture No.1 3.1 Soil Composition

Soil-a 3-phase material Soil Characterization (particle size,

soil plasticity) 3.2 Soil Classification 3.3 Groundwater 3.4 Stress (Total vs. Effective)

Page 3: Chapter 3 Soil Mechanics Part I

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Chapter 3: Soil Mechanics

Lecture No.2 3.5 Compressibility and

settlementLecture No.3 3.6 Strength

Page 4: Chapter 3 Soil Mechanics Part I

CE 4321: Geotechnical Engineering Design

Soil: A 3-Phase Material

Solid

WaterAir

Page 5: Chapter 3 Soil Mechanics Part I

CE 4321: Geotechnical Engineering Design

The Mineral Skeleton

Volume

Solid Particles

Voids (air or water)

Page 6: Chapter 3 Soil Mechanics Part I

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Three Phase Diagram

Solid

Air

Water

Mineral Skeleton Idealization:Three Phase Diagram

Page 7: Chapter 3 Soil Mechanics Part I

CE 4321: Geotechnical Engineering Design

Fully Saturated Soils

Fully Saturated

Water

Solid

Mineral Skeleton

Page 8: Chapter 3 Soil Mechanics Part I

CE 4321: Geotechnical Engineering Design

Dry Soils

Mineral Skeleton Dry Soil

Air

Solid

Page 9: Chapter 3 Soil Mechanics Part I

CE 4321: Geotechnical Engineering Design

Partly Saturated Soils

Solid

Air

Water

Mineral Skeleton Partly Saturated Soils

Page 10: Chapter 3 Soil Mechanics Part I

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Three Phase System

Volume Weight

Solid

Air

WaterWT

Ws

Ww

Wa~0

Vs

Va

Vw

Vv

VT

Page 11: Chapter 3 Soil Mechanics Part I

CE 4321: Geotechnical Engineering Design

Weight Relationships Weight Components:

Weight of Solids = Ws

Weight of Water = Ww

Weight of Air ~ 0

%100(%), s

w

W

WwContentWater

Page 12: Chapter 3 Soil Mechanics Part I

CE 4321: Geotechnical Engineering Design

Volumetric Relationships Volume Components:

Volume of Solids = Vs

Volume of Water = Vw

Volume of Air = Va

Volume of Voids = Va + Vw = Vv

s

v

V

VeRatioVoid ,

%100(%), T

v

V

VnPorosity

Page 13: Chapter 3 Soil Mechanics Part I

CE 4321: Geotechnical Engineering Design

Volumetric Relationships Volume Components:

Volume of Solids = Vs

Volume of Water = Vw

Volume of Air = Va

Volume of Voids = Va + Vw = Vv

%100(%), V

w

V

VSSaturationofDegree

Page 14: Chapter 3 Soil Mechanics Part I

CE 4321: Geotechnical Engineering Design

Specific Gravity

Unit weight of Water, w w = 1.0 g/cm3 (strictly accurate at 4° C) w = 62.4 pcf w = 9.81 kN/m3

WaterofVolumeEqualanofWeight

ceSubsaofWeightGravitySpecific

tan

WaterofWeightUnit

ceSubsaofWeightUnitGravitySpecific

tan

Page 15: Chapter 3 Soil Mechanics Part I

CE 4321: Geotechnical Engineering Design

Specific Gravity Iron 7.86 Aluminum2.55-2.80 Lead 11.34 Mercury 13.55

Granite 2.69 Marble 2.69 Quartz 2.60 Feldspar 2.54-2.62

Page 16: Chapter 3 Soil Mechanics Part I

CE 4321: Geotechnical Engineering Design

Specific Gravity, Gs

Page 17: Chapter 3 Soil Mechanics Part I

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Example: Volumetric Ratios

Determine void ratio, porosity and degree of saturation of a soil core sample

Data: Weight of soil sample = 1013g Vol. of soil sample = 585.0cm3

Specific Gravity, Gs = 2.65 Dry weight of soil = 904.0g

Page 18: Chapter 3 Soil Mechanics Part I

CE 4321: Geotechnical Engineering Design

Solid

Air

Water

Wa~0

Volumes Weights

1013.0g585.0cm3

904.0g

s =2.65

109.0g

341.1cm3

109.0cm3

243.9cm3

134.9cm3

W =1.00

Example

Page 19: Chapter 3 Soil Mechanics Part I

CE 4321: Geotechnical Engineering Design

585.0cm3

Solid

Air

Water

Volumes

s =2.65341.1cm3

109.0cm3

243.9cm3

134.9cm3

W =1.00

%7.441009.243

0.109%100(%)

%7.411000.585

9.243%100(%)

72.01.341

9.243

v

w

T

v

s

v

V

VS

V

Vn

V

Ve

Example

Page 20: Chapter 3 Soil Mechanics Part I

CE 4321: Geotechnical Engineering Design

Soil Unit weight (lb/ft3 or kN/m3)

Bulk (or Total) Unit weight = WT / VT

Dry unit weightd = Ws / VT

Buoyant (submerged) unit weightb = - w

Page 21: Chapter 3 Soil Mechanics Part I

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Typical Unit weights

Page 22: Chapter 3 Soil Mechanics Part I

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TWO KINDS of Soil...

Two kinds of soil in this world… COARSE FINE

Basis for division is...

Page 23: Chapter 3 Soil Mechanics Part I

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Fine-Grained vs. Coarse-Grained Soils

U.S. Standard Sieve - No. 200 0.0029 inches 0.074 mm

“No. 200” means...

Page 24: Chapter 3 Soil Mechanics Part I

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Sieve Analysis (Mechanical Analysis)

This procedure is suitable for coarse grained soils

e.g. No.10 sieve …. has 10 apertures per linear inch

Page 25: Chapter 3 Soil Mechanics Part I

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Hydrometer Analysis

Also called Sedimentation Analysis

Stoke’s Law

18

)(2Lsw GGD

v

Page 26: Chapter 3 Soil Mechanics Part I

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Grain Size Distribution Curves

Page 27: Chapter 3 Soil Mechanics Part I

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Soil Plasticity

Further classification within fine-grained soils (i.e. soil that passes #200 sieve) is done based on soil plasticity.

Albert Atterberg, Swedish Soil Scientist (1846-1916)…..series of tests for evaluating soil plasticity

Arthur Casagrande adopted these tests for geotechnical engineering purposes

Page 28: Chapter 3 Soil Mechanics Part I

CE 4321: Geotechnical Engineering Design

Consistency of fine-grained soil varies in proportion to the water content

Atterberg Limits

Shrinkage limit

Plastic limit

Liquid limit

solid

semi-solid

plastic

liquid

PlasticityIndex

(cheese)

(pea soup)

(pea nut butter)

(hard candy)

Page 29: Chapter 3 Soil Mechanics Part I

CE 4321: Geotechnical Engineering Design

Liquid Limit (LL or wL)

Empirical Definition

The moisture content at which a 2 mm-wide groove in a soil pat will close for a distance of 0.5 in when dropped 25 times in a standard brass cup falling 1 cm each time at a rate of 2 drops/sec in a standard liquid limit device

Page 30: Chapter 3 Soil Mechanics Part I

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Engineering Characterization of Soils

Soil Properties that Control its Engineering Behavior

Particle Size

Particle/Grain Size DistributionParticle Shape

Soil Plasticity

fine-grained

coarse-grained

Page 31: Chapter 3 Soil Mechanics Part I

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Clay Morphology Scanning

Electron Microscope (SEM)

Shows that clay particles consist of stacks of plate-like layers

Page 32: Chapter 3 Soil Mechanics Part I

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Soil Consistency Limits Albert Atterberg

(1846-1916) Swedish Soil Scientist ….. Developed series of tests for evaluating consistency limits of soil (1911)

Arthur Casagrande (1902-1981)

……Adopted these tests for geotechnical engineering purposes

Page 33: Chapter 3 Soil Mechanics Part I

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Arthur Casagrande (1902-1981)

Joined Karl Terzaghi at MIT in 1926 as his graduate student

Research project funded by Bureau of Public Roads

After completion of Ph.D at MIT Casagrande initiated Geotechnical Engineering Program at Harvard

Soil Plasticity and Soil Classification (1932)

Page 34: Chapter 3 Soil Mechanics Part I

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Casagrande Apparatus

Page 35: Chapter 3 Soil Mechanics Part I

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Casagrande Apparatus

Page 36: Chapter 3 Soil Mechanics Part I

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Casagrande Apparatus

Page 37: Chapter 3 Soil Mechanics Part I

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Liquid Limit Determination

Page 38: Chapter 3 Soil Mechanics Part I

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The moisture content at which a thread of soil just begins to crack and crumble when rolled to a diameter of 1/8 inches

Plastic Limit (PL, wP)

Page 39: Chapter 3 Soil Mechanics Part I

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Plastic Limit (PL, wP)

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Plasticity Index ( PI, IP )

PI = LL – PL

or IP=wL-wP

Note: These are water contents, but the percentage sign is not typically shown.

Page 41: Chapter 3 Soil Mechanics Part I

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Plasticity Chart

Page 42: Chapter 3 Soil Mechanics Part I

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USCS Classification Chart

Page 43: Chapter 3 Soil Mechanics Part I

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USCS Classification Chart

Page 44: Chapter 3 Soil Mechanics Part I

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Plasticity Chart

Page 45: Chapter 3 Soil Mechanics Part I

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Groundwater

U = porewater pressure = wZw

Zw

+

Page 46: Chapter 3 Soil Mechanics Part I

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Stresses in Soil Masses

Area = A

= P/A

X X

Soil Unit

P

Assume the soil is fully saturated, all voids are filled with water.

Page 47: Chapter 3 Soil Mechanics Part I

CE 4321: Geotechnical Engineering Design

Effective Stress

From the standpoint of the soil skeleton, the water carries some of the load. This has the effect of lowering the stress level for the soil.

Therefore, we may define effective stress = total stress minus pore pressure

′ = - u where, ′ = effective stress = total stressu = pore pressure

Page 48: Chapter 3 Soil Mechanics Part I

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Effective Stress

′ = - u The effective stress is the force carried by

the soil skeleton divided by the total area of the surface.

The effective stress controls certain aspects of soil behavior, notably, compression & strength.

Page 49: Chapter 3 Soil Mechanics Part I

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Effective Stress Calculations

′z = iHi - u where,

H = layer thicknesssat = saturated unit weight

U = pore pressure = w Zw

When you encounter a groundwater table, you must use effective stress principles; i.e., subtract the pore pressure from the total stress.

Page 50: Chapter 3 Soil Mechanics Part I

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Geostatic Stresses

Page 51: Chapter 3 Soil Mechanics Part I

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See p.79

Page 52: Chapter 3 Soil Mechanics Part I

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See p.79