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Shear Strength: Why and When Does Soil Slide?
Failure in soil almost always happens by shear. The Mohr–Coulomb criterion describes it with a single line — but which stress and which drainage condition it is used with can change the result by 50%. A fill's most dangerous moment can be the end of construction; a cut's, years later.
1. Why does soil slide?
Soils carry no tension and rarely crush under compression; failure in soil almost always happens by shear. A slope sliding, the soil under a footing pushed sideways, the wedge behind a retaining wall moving — all are the shear strength being exceeded. Shear strength is therefore the central quantity of geotechnical engineering; bearing capacity, slope stability and earth pressure all rest on it.
2. The Mohr–Coulomb criterion
The shear strength on a plane increases with the normal effective stress acting on it:
where c' is the effective cohesion and φ' the effective angle of internal friction. In sands c' is practically zero; strength comes entirely from friction. For a sand with φ' = 32° under σ' = 100 kPa, τf = 100 × tan 32° = 62.5 kPa. The criterion is clearest together with the Mohr circle: failure occurs when the Mohr circle touches this line. The site's Mohr circle tool shows the stress transformation.
3. Effective stress: water's share
The σ' in the criterion is effective, not total, stress: σ' = σ − u. Pore water carries no shear; the part with which the grains press on each other — the effective stress — sets the friction. The consequence is striking: at a point with total stress 150 kPa and pore pressure 50 kPa, the correct strength is 100 × tan 32° = 62.5 kPa. Computed with total stress it comes out as 93.7 kPa — 50% too high. This is also why slopes slide after rain: pore pressure rises, effective stress and with it strength fall.
4. Drained and undrained behaviour
Because clay has low permeability, water cannot escape when load is applied quickly; pore pressure changes and the soil behaves undrained. Strength is then expressed by one parameter, the undrained shear strength cu (su), in a total-stress analysis (φu = 0). If the load is applied slowly, or enough time passes, the water equilibrates and the soil behaves drained; an effective-stress analysis with c' and φ' applies.
Which is critical depends on the type of loading:
- Fill or footing on soft clay (loading): the most critical moment is right at the end of construction. Loading raises pore pressure; as water drains, effective stress and strength increase. Undrained analysis governs.
- Excavation or cut slope (unloading): conversely, the long term is most critical. Unloading lowers pore pressure; water gradually returns and strength falls. Drained analysis governs. A cut that stands for years and then suddenly slides is therefore no surprise.
5. The triaxial test
Shear strength parameters are usually measured in the triaxial test. A cylindrical specimen is held under cell pressure σ3 and the axial stress is increased to failure. The test type sets the drainage condition: UU (unconsolidated–undrained) gives cu; CU (consolidated–undrained, with pore pressure measured) and CD (consolidated–drained) give c' and φ'.
The Mohr–Coulomb criterion links the principal stresses at failure:
For a sand with c' = 0 and φ' = 32°, at σ'3 = 100 kPa failure occurs at σ'1 = 325.5 kPa; the failure plane makes 45° + φ'/2 = 61° with the major principal plane. For a clay with c' = 10 kPa and φ' = 25° at the same cell pressure, σ'1 = 277.8 kPa.
6. Uncertainty: how sensitive is φ'?
φ' is never known exactly; sample disturbance, test type and natural variability create an uncertainty of a few degrees. Its effect on strength:
| φ' | τf (kPa), σ' = 100 kPa | Relative to φ' = 32° |
|---|---|---|
| 30° | 57.7 | -7.6 % |
| 32° | 62.5 | 0.0 % |
| 34° | 67.5 | +7.9 % |
±2° means about ±8% in strength. Because bearing capacity factors grow much faster with φ', the same uncertainty becomes a much larger difference in bearing capacity — try changing φ' in the site's bearing capacity tool. Cohesion calls for more caution: a small c' measured in the laboratory is often a by-product of curve fitting, and relying on it in long-term analysis is risky.
All values in this article are checked by tests/v583-shear-strength.test.js.
References
- Terzaghi, K. (1943). Theoretical Soil Mechanics. Wiley. (The effective stress principle.)
- Bishop, A. W. and Bjerrum, L. (1960). The relevance of the triaxial test to the solution of stability problems. Proc. ASCE Research Conference on Shear Strength of Cohesive Soils, 437–501.
- Holtz, R. D., Kovacs, W. D. and Sheahan, T. C. (2011). An Introduction to Geotechnical Engineering, 2nd ed., Chapters 11–12. Pearson.
The numbers in this article were computed with closed-form relations and are checked by the stated test.