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Hybrid method for the computation of dynamic soil-structure ...

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Asymptotic expansion <strong>for</strong> ω → ∞<strong>Hybrid</strong> domain <strong>method</strong>Introduction<strong>Hybrid</strong> <strong>method</strong>Time Domain BEMFE-BEConclusions■ Force-displacement relationship <strong>for</strong> ω → ∞:ũ x (k x , ω) = iωρC s˜t x (k x , ω) (7)ũ y (k x , ω) = iωρC s˜t y (k x , ω) (8)ũ z (k x , ω) = iωρC p˜t z (k x , ω) (9)■ The stiffnesses are independent <strong>of</strong> <strong>the</strong> wavenumber:û x (x, ω) = iωρC sˆt x (x, ω) (10)û y (x, ω) = iωρC sˆt y (x, ω) (11)û z (x, ω) = iωρC pˆt z (x, ω) (12)■ The result is extended to <strong>the</strong> 3D-case, using a Fourier series in <strong>the</strong> circumferentialdirection. The results remain valid.LMSSMat <strong>Hybrid</strong> <strong>method</strong> <strong>for</strong> <strong>the</strong> <strong>computation</strong> <strong>of</strong> <strong>dynamic</strong> <strong>soil</strong>-<strong>structure</strong> interaction in <strong>the</strong> time domain - p. 13/44

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