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Annual Report 2000 - WIT

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256<br />

transport equation. Nevertheless, the result of the ray-propagator-method is noisier<br />

and is superimposed by distortions at isolated gridpoints.<br />

ŽA<br />

0<br />

0.000 0.025 0.050<br />

20 40 60 80 20 40 60 80<br />

0Œ<br />

500<br />

1000<br />

z [m]<br />

1500<br />

<strong>2000</strong><br />

2500<br />

3000 4000 5000 6000 7000 8000 9000<br />

x [m]<br />

Figure 1: Traveltimes and amplitudes for the Marmousi model computed with the FD<br />

solution of the eikonal and the transport equation. The distance between isochrons is<br />

0.075 seconds.<br />

0<br />

500<br />

1000<br />

z [m]<br />

1500<br />

<strong>2000</strong><br />

2500<br />

3000 4000 5000 6000 7000 8000 9000<br />

x [m]<br />

Figure 2: Traveltimes for the Marmousi model computed with the finite difference<br />

solution of the eikonal equation and a wave front construction program. The distance<br />

between isochrons is 0.05 seconds.

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