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Annual Report 2000 - WIT

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69<br />

(a)<br />

(b)<br />

Depth (m)<br />

600<br />

800<br />

Depth (m)<br />

600<br />

800<br />

1000<br />

-1000 0 1000<br />

Distance (m)<br />

1000<br />

-1000 0 1000<br />

Distance (m)<br />

Figure 7: (a) Kirchhoff depth migrated section, (b) Kirchhoff demodeled section, of<br />

noise-free common-offset data for Model II.<br />

Reflection Coefficient<br />

0.1<br />

0.05<br />

(a)<br />

Relative Error (%)<br />

0<br />

-1000 0 1000<br />

Distance (m)<br />

50<br />

0<br />

-50<br />

(b)<br />

-100<br />

-1000 0 1000<br />

Distance (m)<br />

Figure 8: (a) Amplitudes along the reflector from demodeling (solid line) and Kirchhoff<br />

migration (dashed line) in comparison to reflection coefficients (bold line). (b)<br />

Relative errors.<br />

CONCLUSIONS<br />

We have presented a numerical analysis of a new migration method based on the<br />

Kirchhoff-Helmholtz integral. Since the process under investigation represents an<br />

(asymptotic) inverse to Kirchhoff modeling, we have termed it Kirchhoff demodeling.<br />

The demodeling integral is completely analogous to the modeling integral in the<br />

sense that it does exactly the same procedure along the reflection traveltime surface<br />

that the modeling integral does along the reflector.

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