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Eduardo Kausel-Fundamental solutions in elastodynamics_ a compendium-Cambridge University Press (2006)

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82 Three-dimensional problems <strong>in</strong> homogeneous half-spaces<br />

0.2<br />

µru rx<br />

0.1<br />

0<br />

-0.1<br />

Figure 6.2a: Radial displacement at<br />

surface due to suddenly applied horizontal<br />

po<strong>in</strong>t load, ν = 0.25 (Chao’s<br />

problem). Varies as cos θ.<br />

-0.2<br />

tβ<br />

τ =<br />

r<br />

-0.3<br />

0 0.5 1.0 1.5 2.0<br />

Displacementsonthe epicentral axis (r= 0, z ≠ 0)<br />

At all times, u xx (0, z, t) = u rx (0, z, t), u θ x (0, z, t) =−u rx (0, z, t), u z (0, z, t) = 0. Def<strong>in</strong>e the<br />

auxiliary functions<br />

( )√<br />

τ τ 2 − 1 τ<br />

3<br />

2 + 2 3<br />

f (τ) = ( ) 2 ( )√<br />

2τ 2 + 1 3 − 4τ τ 2 − 1 τ<br />

3<br />

2 + 2 3<br />

( √<br />

)<br />

τ 2 (τ 2 − 1) 2τ τ 2 − 2 3 − (2τ 2 − 1)<br />

g(τ) =<br />

√<br />

(2τ 2 − 1) 2 − 4τ(τ 2 − 1) τ 2 − 2 3<br />

(6.17)<br />

(6.18)<br />

0.07<br />

µru θx<br />

0<br />

-0.07<br />

Figure 6.2b: Tangential displacement at<br />

surface due to suddenly applied horizontal<br />

po<strong>in</strong>t load, ν = 0.25 (Chao’s<br />

problem). Varies as −s<strong>in</strong> θ.<br />

tβ<br />

τ =<br />

r<br />

-0.14<br />

0 0.5 1.0 1.5 2.0

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