Compressibility and Consolidation - notes and formulae
av = (e1 - e2)/(σ2 - σ1)
Here, e1 is the void ratio corresponding to effective stress σ1 and e2 is the void ratio corresponding to effective stress σ2. The coefficient of compressibility expresses change of volume (or void ratio) per unit change in effective stress.



Relationship between volume change and thickness change:
ΔV/V0 = ΔH/H0
The coefficient of compression (Cc) is used with void ratio-log stress plots (e-log σ′) to estimate primary consolidation settlement.



O.C.R. = Maximum past effective stress (preconsolidation stress) / Current effective stress


The governing differential equation for one-dimensional consolidation (Terzaghi) is written in terms of excess pore pressure u(z,t):
∂u/∂t = Cv ∂2u/∂z2
where:
Coefficient of volume compressibility mv is related to av by
mv = av / (1 + e0)
where e0 is the initial void ratio.
Compression modulus Ec is the reciprocal of mv:
Ec = 1 / mv
%U = (1 - u/u1) × 100%
Here u is the excess pore pressure at time t and u1 is the initial excess pore pressure (at t = 0). At t = 0, %U = 0%; as t → ∞, u → 0 and %U → 100%.

%U = [(e0 - e)/(e0 - ef)] × 100%
where e is void ratio at time t, e0 is initial void ratio (t = 0) and ef is void ratio at 100% primary consolidation (t = ∞).
%U = (Δh / ΔH) × 100%
where Δh is settlement at time t and ΔH is final total settlement due to primary consolidation (settlement at t = ∞).
The time factor Tv is defined as:
Tv = Cv t / d2
where:
Approximate relations between Tv and degree of consolidation U (useful for hand calculations and laboratory curve fitting):
Cv = (T90 × d2) / t90
where T90 is the time factor corresponding to 90% consolidation and t90 is the observed time for 90% consolidation. d is the drainage path.
Cv = (T50 × d2) / t50
where T50 is the time factor for 50% consolidation and t50 is the observed time for 50% consolidation.
Defined from dial gauge readings; typical notation uses initial reading Ri, zero consolidation reading R0 and final reading Rf after secondary compression.

Measured as the change in dial gauge reading corresponding to 100% primary consolidation (R100).

Ratios for initial, primary and secondary components satisfy ri + rp + rs = 1 for partitioning of total compression.

Total settlement S is the sum of initial, primary and secondary settlements:
S = Si + Sp + Ss
For cohesionless soils, initial settlement may be estimated using empirical bearing capacity or elastic approaches. An approximate factor given is Cs = 1.5 (Cr/σ0) where Cr is a static resistance and σ0 reference stress. H0 denotes the depth of influence.

For cohesive soils, initial elastic settlement may be estimated using a shape (influence) factor It and loaded area A.

Primary consolidation settlement is obtained from e-logσ′ relations or from mv:
S = ΔH = mv H0 Δσ′ for normally consolidated ranges, or by integrating changes in void ratio from initial to final effective stress.






= Settlement for normally consolidation stage
Note: separate plots and formulae are used for normally consolidated and overconsolidated stages; the images above correspond to common consolidation and settlement diagrams.
Secondary compression (creep) occurs after primary consolidation is essentially complete. It is often estimated from a secondary compression index and logarithmic time relations. Typical symbols include H0 ~ H100 (thickness after 100% primary consolidation), e100 (void ratio after 100% consolidation) and t2 the period over which secondary compression is calculated.

Permeability is a measure of the ease with which water flows through a soil. The coefficient of permeability is usually denoted by K (or k).
For laminar flow in a porous medium (Darcy conditions): the discharge per unit time is proportional to the hydraulic gradient and cross-sectional area and inversely proportional to the length.
Rate of flow: q = K i A

K = Q L / (t HL A)
Q = volume collected in time t; L = sample length; HL = head loss; A = cross sectional area.

K = (2.303 a L) / (A t) log10(h1/h2)
a = cross-sectional area of standpipe; A = area of specimen; t = time interval; L = length of specimen; h1, h2 = head readings at start and end of interval.

The Kozeny-Carman type relations connect permeability with particle shape, specific surface and porosity. The general form uses a shape coefficient C and specific surface S:


For spherical particles, relations for specific surface and characteristic dimensions are often simplified; R denotes particle radius. The input images show geometric relations and typical substitutions for S and particle sizes.

K = C × D102
D10 = effective grain size (cm). C ≈ 100 to 150 for clean sands (K in cm/s).
log10(K S2) = a + b n
S = specific surface; n = porosity; a and b are empirical constants.
K = Cv mv γw
This relates permeability with coefficient of consolidation Cv, coefficient of volume compressibility mv and unit weight of water γw.

In partially saturated soils the hydraulic behaviour depends on degree of saturation S; capillary heights and retained suction influence flow. Typical relations include a head distribution i = (h0 + hc)/x for certain simplified geometries where hc is capillary height and x is distance. Permeability K generally increases with saturation and reaches maximum at S = 100%.


Note: Ku (permeability for unsaturated soil) ∝ S; for S = 100% K = maximum.






Seepage pressure is the pressure exerted by moving water on soil particles as a result of flow. Seepage force acts in the direction of flow and is due to frictional drag of water on the soil skeleton.
Seepage pressure: Ps = h γw, where h is head loss and γw is unit weight of water (≈ 9.81 kN/m3).
Seepage force over a volume: Fs = h A γw.
Seepage force per unit volume: fs = i γw, where i is hydraulic gradient (i = h/z).
When upward seepage through a cohesionless soil produces a hydraulic gradient large enough to counteract the effective weight of soil, the net effective vertical stress becomes zero and the soil may behave as quick sand.
Critical hydraulic gradient is given by:
ic = (G - 1)/(1 + e)
To avoid a floating (piping/quick) condition the actual gradient i must satisfy i < ic. A factor of safety against quick condition can be expressed as F.O.S. = ic/i > 1.
The potential function ∅ and total head H are related for seepage in homogeneous isotropic soil: ∅ = k H.


For isotropic homogeneous soil the 2-D Laplace equation applies to H or ∅ and flow nets (orthogonal families of streamlines and equipotential lines) provide graphical solutions.
For unit length in the out-of-plane direction, seepage discharge q is given by:
q = k h (Nf / Nd)
Hydrostatic (pore) pressure at a point: U = hw γw, where hw is pressure head.
An expression for seepage pressure using equipotential drops: Ps = h′ γw, where h′ = h - (2h/Nd) in the specific diagrammatic formulation shown in the images.

The exit gradient at the downstream face of a porous medium (e.g., in an exit flow field of dimensions b × b shown in the figure) is approximated from flow net geometry. The equipotential drop ΔH = h / Nd is used in that evaluation.

The phreatic line is the topmost streamline in an earth dam seepage profile; it represents the free surface of flow and follows a parabolic path in many simple geometries. Pressure on the phreatic line is atmospheric, while pressure below it is hydrostatic.


The phreatic line follows the base parabola; positions and radii of characteristic arcs (e.g., CF as radius of a circular arc) are shown in the figure. Typical notations: C = entry point of base parabola, F = junction of permeable and impermeable surfaces, S = focal length (distance between focus and directrix), FH = S, etc.
Relevant relations from the diagrams and analysis include discharge per unit length q = k s (where s is the seepage path length component shown), and other geometric relations shown in the images.




For a simple dam geometry with downstream slope angle α the approximate discharge expressions shown in the diagrams are:


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