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Vertical effective stress below a water table

Vertical effective stress at depth beneath a surface surcharge q, through a moist layer of thickness zm and unit weight γm above the water table and a saturated layer of thickness zs and unit weight γsat below it.

Ref
CIV-47
Rev
v1
Field
Civil
Result
σ′v [Pa]

Effective stress is total stress minus pore water pressure, and it is what controls soil strength and compression. Above the water table the soil has its moist unit weight γm. Below it, the soil is saturated, the water supports γw per metre, and the soil skeleton carries γsat − γw. Adding the surcharge, the vertical effective stress at depth zm + zs is q + γm zm + (γsat − γw) zs.

Vertical effective stress at depth beneath a surface surcharge q, through a moist layer of thickness zm and unit weight γm above the water table and a saturated layer of thickness zs and unit weight γsat below it. Below the table the buoyant unit weight γsat − γw applies. Hydrostatic water and negligible suction above the table.

Calculator

Solve for
Pa
Pa
0100,000
N/m³
10,00025,000
m
020
N/m³
10,00025,000
N/m³
9,00010,500
m
020
  • Total vertical stress, q + γmzm + γsat·zs106,000 Pa
  • Pore water pressure, γw·zs29,430 Pa
  • Buoyant unit weight, γsat − γw10,190 N/m³

What drives the result

Each variable is moved across its typical range while the others stay at the values above. The longest bar is the key driver.

Vertical effective stress (Pa) current value 76,570 Pa
zmThickness above the water tableKey driver
40,600401,000
zsSaturated thickness
46,000250,000
qSurface surcharge
66,600167,000
γsatSaturated unit weight
46,60091,600
γmMoist unit weight
60,60090,600
γwUnit weight of water
74,50079,000
  • The effective stress is 76.57 kPa, while the total stress is 106 kPa; the difference is the 29.43 kPa of pore pressure.
  • If the water table rose to the surface the effective stress would fall, which is why flooding and dewatering change settlement and strength.
Chart data as tables

Ranked variables

VariableTypical rangeLowest resultHighest resultSwing (Pa)Local stepChange in result
zm Thickness above the water table0 to 20 m40,570400,600360,000+10%+4.7 %
zs Saturated thickness0 to 20 m46,000249,800203,800+10%+3.99 %
q Surface surcharge0 to 100,000 Pa66,570166,600100,000+10%+1.31 %
γsat Saturated unit weight10,000 to 25,000 N/m³46,57091,57045,000+10%+7.84 %
γm Moist unit weight10,000 to 25,000 N/m³60,57090,57030,000+10%+4.7 %
γw Unit weight of water9,000 to 10,500 N/m³74,50079,0004,500+10%−3.84 %

Sweep of Saturated thickness

Saturated thickness (m)Vertical effective stress (Pa)
046,000
2.571,480
596,950
7.5122,400
10147,900
12.5173,400
15198,900
17.5224,300
20249,800

Sweep one variable

Vertical effective stress (Pa)Hover, touch, or use the arrow keys on the chart
50k100k150k200k250k 05101520 Saturated thickness (m) now 76,570

Variables and how each one contributes

σ′v

Vertical effective stress

Result · Pa

What the equation gives you. Everything else feeds it.

q

Surface surcharge

Pa · typical 0 to 100,000

The uniform surcharge at the surface, in Pa. Adds to the stress at every depth in direct proportion. Raising it by 10 % (to 11,000) moves the result by +1.31 %, from 76,570 to 77,570 Pa.

γm

Moist unit weight

N/m³ · typical 10,000 to 25,000

The moist unit weight above the water table, in N/m³. Raises the stress in proportion to the thickness zm. Raising it by 10 % (to 19,800) moves the result by +4.7 %, from 76,570 to 80,170 Pa.

zm

Thickness above the water table

m · typical 0 to 20

The thickness of soil above the water table, in m. Raises the stress at γm per metre. Raising it by 10 % (to 2.2) moves the result by +4.7 %, from 76,570 to 80,170 Pa.

γsat

Saturated unit weight

N/m³ · typical 10,000 to 25,000

The saturated unit weight below the water table, in N/m³. Raises the buoyant weight in proportion to zs. Raising it by 10 % (to 22,000) moves the result by +7.84 %, from 76,570 to 82,570 Pa.

γw

Unit weight of water

N/m³ · typical 9,000 to 10,500

The unit weight of water, in N/m³ (about 9810). Lowers the effective stress below the table, because of buoyancy. Raising it by 10 % (to 10,790) moves the result by −3.84 %, from 76,570 to 73,630 Pa.

zs

Saturated thickness

m · typical 0 to 20

The thickness of saturated soil, in m. Raises the stress at only γsat − γw per metre, much less than above the table. Raising it by 10 % (to 3.3) moves the result by +3.99 %, from 76,570 to 79,630 Pa.

Worked example with the values above

  1. Above the table: q + γm zm = 10,000 + 18,000 × 2 = 46,000 Pa.
  2. Below the table: (γsat − γw) zs = 10,190 × 3 = 30,570 Pa.
  3. σ′v = 46,000 + 30,570 = 76,570 Pa.

Assumptions and limits

  • A vertical smooth wall, level drained cohesionless backfill, and enough wall movement to mobilise the active or passive state.
  • Effective stresses for soil strength, with water pressure computed separately.

Common mistakes

  • Using total instead of effective stress below the water table.
  • Using the active coefficient where the wall cannot move, when at-rest pressure applies.
  • Entering the friction angle in degrees where the page needs radians.

Statistics and uncertainty

Earth pressure is among the most uncertain quantities in structural design. The effective friction angle is rarely known to better than ±2° to 3°, which alone changes Ka by 10 % to 15 %, and the wall movement needed to reach the active state is rarely checked. Treat the numbers as estimates with generous margins.

Where it is used

  • Designing retaining walls, basement walls and sheet piles.
  • Finding overturning moments and sliding forces on walls.

Maths you need

  • Effective stress: total stress minus pore water pressure
  • Friction angle: the angle whose tangent is the shear to normal stress ratio at failure
  • Active and passive states: minimum and maximum lateral stress at limiting equilibrium

Related formulas

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