10. in-situ stress (das, chapter 9) sections: all except 9.5, 9.6, 9.7, 9.8, 9.9

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10. In-Situ Stress (Das, Chapter 9) Sections: All except 9.5, 9.6, 9.7, 9.8, 9.9

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Page 1: 10. In-Situ Stress (Das, Chapter 9) Sections: All except 9.5, 9.6, 9.7, 9.8, 9.9

10. In-Situ Stress(Das, Chapter 9)

Sections: All except 9.5, 9.6, 9.7, 9.8, 9.9

Page 2: 10. In-Situ Stress (Das, Chapter 9) Sections: All except 9.5, 9.6, 9.7, 9.8, 9.9

Stress in a Soil MassStress in a Soil Mass

TopicsTopics

IntroductionIntroduction

Geostatic StressGeostatic Stress

Stresses due to external loadsStresses due to external loads

Page 3: 10. In-Situ Stress (Das, Chapter 9) Sections: All except 9.5, 9.6, 9.7, 9.8, 9.9

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IntroductionIntroduction

Page 4: 10. In-Situ Stress (Das, Chapter 9) Sections: All except 9.5, 9.6, 9.7, 9.8, 9.9

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IntroductionIntroduction

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IntroductionIntroduction

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Hydrostatic and Total stress

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• When a load is applied to soil, it is carried by the water in the pores as well as the solid grains. The increase in pressure within the porewater causes drainage (flow out of the soil), and the load is transferred to the solid grains. The rate of drainage depends on the permeability of the soil. The strength and compressibility of the soil depend on the stresses within the solid granular fabric. These are called effective stresses

Page 8: 10. In-Situ Stress (Das, Chapter 9) Sections: All except 9.5, 9.6, 9.7, 9.8, 9.9

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Pore Water Pressure

Page 9: 10. In-Situ Stress (Das, Chapter 9) Sections: All except 9.5, 9.6, 9.7, 9.8, 9.9

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Effective Stress – General Expression

Page 10: 10. In-Situ Stress (Das, Chapter 9) Sections: All except 9.5, 9.6, 9.7, 9.8, 9.9

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Methods of Computations Effective Stress

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Diagram

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Total stress in multi-layered soil

Page 13: 10. In-Situ Stress (Das, Chapter 9) Sections: All except 9.5, 9.6, 9.7, 9.8, 9.9

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EXAMPLE Plot the variation of total and effective vertical stresses, and

pore water pressure with depth for the soil profile shown

below in Fig.

Page 14: 10. In-Situ Stress (Das, Chapter 9) Sections: All except 9.5, 9.6, 9.7, 9.8, 9.9

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Solution: Within a soil layer, the unit weight is constant, and therefore the stresses vary

linearly. Therefore, it is adequate if we compute the values at the layer interfaces

and water table location, and join them by straight lines.

Page 15: 10. In-Situ Stress (Das, Chapter 9) Sections: All except 9.5, 9.6, 9.7, 9.8, 9.9

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Solution

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Example 1t ’

Page 17: 10. In-Situ Stress (Das, Chapter 9) Sections: All except 9.5, 9.6, 9.7, 9.8, 9.9

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Example 2t ’

Page 18: 10. In-Situ Stress (Das, Chapter 9) Sections: All except 9.5, 9.6, 9.7, 9.8, 9.9

Other Examples

Example 9.1 Das, Chapter 9

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Page 19: 10. In-Situ Stress (Das, Chapter 9) Sections: All except 9.5, 9.6, 9.7, 9.8, 9.9

Stresses in Saturated Soils without Seepage (No flow)At A,

•Total Stress: A = H1 w

•Pore water pressure: uA = H1 w

•Effective stress: ’A= 0

At B,

•Total Stress: B = H1 w + H2 sat

•Pore water pressure: uB = (H1 + H2) w

•Effective stress: ’B= H2(sat – w) = H2 ’

At C,

•Total Stress: C = H1 w + z sat

•Pore water pressure: uC = (H1 + z) w

•Effective stress: ’C= z(sat – w) = z ’

Page 20: 10. In-Situ Stress (Das, Chapter 9) Sections: All except 9.5, 9.6, 9.7, 9.8, 9.9

Stresses in Saturated Soils without Seepage (No flow)

Variations of the total stress, pore water pressure, and effective stress, respectively, with depth for a soil layer without seepage

Page 21: 10. In-Situ Stress (Das, Chapter 9) Sections: All except 9.5, 9.6, 9.7, 9.8, 9.9

Stresses in Saturated Soils with Upward SeepageIf water is seeping, the effective stress at any point in a soil mass will differ from that in the static case. It will increase or decrease,

depending on the direction of seepage.

Page 22: 10. In-Situ Stress (Das, Chapter 9) Sections: All except 9.5, 9.6, 9.7, 9.8, 9.9

Stresses in Saturated Soils with Upward Seepage

Variations of the total stress, pore water pressure, and effective stress, respectively, with depth for a soil layer with upward seepage

Page 23: 10. In-Situ Stress (Das, Chapter 9) Sections: All except 9.5, 9.6, 9.7, 9.8, 9.9

• Note that h/H2 is the hydraulic gradient I caused by the flow, and therefore:

• If the rate of seepage and thereby the hydraulic gradient gradually are increased, a limiting condition will be reached, at which ’ is zero:

Where icr: critical hydraulic gradient (for zero effective stress).

• Under such a situation, soil stability is lost. This situation generally is referred to as boiling, or a quick condition.

• For most soils, the value of icr varies from 0.9 to 1.1, with an average of 1.

Stresses in Saturated Soils with Upward Seepage

wizz

wcr ziz 0

wcri

Page 24: 10. In-Situ Stress (Das, Chapter 9) Sections: All except 9.5, 9.6, 9.7, 9.8, 9.9

Stresses in Saturated Soils with Downward Seepage

At B,

•Total Stress: B = H1 w + H2 sat

•Pore water pressure: uB = (H1 + H2 - h) w

•Effective stress: ’B= H2(sat – w) + h w

Page 25: 10. In-Situ Stress (Das, Chapter 9) Sections: All except 9.5, 9.6, 9.7, 9.8, 9.9

Stresses in Saturated Soils with Downward Seepage

Variations of the total stress, pore water pressure, and effective stress, respectively, with depth for a soil layer with downward seepage

Page 26: 10. In-Situ Stress (Das, Chapter 9) Sections: All except 9.5, 9.6, 9.7, 9.8, 9.9

Seepage Force

Page 27: 10. In-Situ Stress (Das, Chapter 9) Sections: All except 9.5, 9.6, 9.7, 9.8, 9.9

Seepage Force per unit volume

See Example 9.3 Das, chapter 9