In many cases the analysis of the consolidation of axi‐symmetric bodies subjected to non axi‐symmetric loading may be carried out without recourse to a full three‐dimensional treatment. Advantage may be taken of the axi‐symmetric nature of the body and field quantities such as displacement and pore pressure can be given a Fourier representation. The problem is then reduced from one in three spatial dimensions (r, θ,z) and the time domain to one in two spatial dimensions (r,z) and the time domain.
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Carter et al. (1983) studied this question.
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