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Upward seepage stress variation diagram

Short answer

Total stress σ increases linearly: slope γw in water, γsat in soil. Pore pressure u is hydrostatic above soil; in soil it increases with excess head h, slope γw(1+i). Effective stress σ' = σ−u is zero at top of soil, increases with slope (γ'−iγw), reaching γ'H1−γw h at base, zero at quick condition.

In the figure, upward seepage is shown. The rate of water supply from the bottom is kept constant. The total loss of head during upward seepage between points B and A is h. Keeping in mind that the total stress at any point in the soil is solely determined by the weight of the soil and the water above it, draw the variation of total stress, pore water pressure and effective stress with depth. Take points A, B and C as reference. [Figure: soil column in a tank with inflow at the bottom and outflow at the top, heights H1 and H2 marked, piezometers showing head h between B and A.]

Assumed figure

C = water surface, B = top of the soil, A = bottom of the soil. Depth of water above the soil =H2= H_2 (C to B). Soil thickness =H1= H_1 (B to A). Water flows upward through the soil with a total head loss hh between A and B. The saturated unit weight of soil is γsat\gamma_{sat} and γ′=γsat−γw\gamma' = \gamma_{sat} - \gamma_w.

Measure depths downward from C.

Stresses at the three points

PointTotal stress σ\sigmaPore pressure uuEffective stress σ′\sigma'
C (water surface)000
B (top of soil)γwH2\gamma_w H_2γwH2\gamma_w H_20
A (bottom of soil)γwH2+γsatH1\gamma_w H_2 + \gamma_{sat}H_1γw(H1+H2+h)\gamma_w (H_1 + H_2 + h)γ′H1−γwh\gamma' H_1 - \gamma_w h

Pore pressure at A is increased by γwh\gamma_w h above the hydrostatic value, since water enters at higher head. The excess head hh is lost uniformly through the soil (linear variation).

Diagrams

 depth   σ            u              σ'
 C  |    0            0              0
    |    ╲            ╲              
 B  |    γw·H2        γw·H2          0
    |      ╲            ╲              ╲
    |       ╲            ╲                ╲  (reduced
 A  |   γwH2+γsatH1  γw(H1+H2+h)   γ'H1 − γw·h   by seepage)
  • Between C and B, σ\sigma and uu increase together with slope γw\gamma_w and σ′=0\sigma' = 0.
  • Between B and A, σ\sigma increases linearly with slope γsat\gamma_{sat}; uu increases linearly with slope γw(1+h/H1)=γw(1+i)\gamma_w(1 + h/H_1) = \gamma_w(1+i); so σ′\sigma' increases linearly with slope γ′−iγw\gamma' - i\gamma_w.
  • When i=h/H1=γ′/γwi = h/H_1 = \gamma'/\gamma_w, σ′\sigma' at A is zero: quick condition.

✓ Answer checked by Claude Opus 5.5 (high effort)

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