In this chapter the finite element method for the solution of problems of one-dimensional consolidation is presented. The purpose is to develop a method for the analysis of consolidation of a soil consisting of several layers having different properties. 16.1 Basic equation The basic equation of one-dimensional consolidation is (16.1) where pis the excess pore pressure, and where n is the compressibility of the soil, k is the hydraulic conductivity (or permeability), and 'Y is the volumetric weight of the fluid. The initial condition is t = 0 : p =Po, (16.2) and the boundary conditions are supposed to be z = 0 : p = 0, (16.3) ap z = h : az = 0. (16.4) This means that the upper boundary z = 0 is supposed to be fully drained, and the lower boundary z =his impermeable. As an alternative the lower boundary may also be drained, in which case the excess pore pressure p is zero for z = h. In order to eliminate the time derivative the differential equation (16.1) is integrated over a small time intervalll.t. This gives n(p+-p-) = ll.t .!!._(~ dp), dz 'Y dz (16.5) where p-is the value of p at the beginning of the time interval, p+ is the value at the end of the interval, and p is the average value during that interval. It is assumed that this average value can be expressed as (16.6) 280 A. Verruijt, Computational Geomechanics
CITATION STYLE
Verruijt, A. (1995). Finite Elements for Two-Dimensional Consolidation (pp. 291–307). https://doi.org/10.1007/978-94-017-1112-8_17
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