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In this Appendix I derive equations 39-45.
mul_sktch9
Figure 21 Sketch to show the computation
of ts1 and ts2 for a non-diffracted multiple from a dipping
water-bottom.
|
| ![mul_sktch9](../Gif/mul_sktch9.gif) |
From triangle ABC in Figure
we immediately get
| ![\begin{displaymath}
t_{s_1}=\frac{\tilde{Z}_s}{\cos(\alpha_s+\varphi)}\end{displaymath}](img101.gif) |
(57) |
and applying the law of sines to triangle ACD we get
| ![\begin{displaymath}
t_{s_2}=\frac{t_{s_1}\cos\alpha_s}{\cos(\alpha_s+2\varphi)}=...
...cos\alpha_s}{V_1\cos(\alpha_s+\varphi)\cos(\alpha_s+2\varphi)}.\end{displaymath}](img102.gif) |
(58) |
mul_sktch10
Figure 22 Sketch to show the computation
of tr2 and tr1 for a non-diffracted multiple from a dipping
water-bottom.
|
| ![mul_sktch10](../Gif/mul_sktch10.gif) |
Similarly, repeated application of the law of sines to triangles CDE and DEF
in Figure
gives
| ![\begin{eqnarray}
t_{r_2}&=&\frac{t_{s_2}\cos(\alpha_s+\varphi)}{\cos(\alpha_s+3\...
...s\cos\alpha_s}{V_1\cos(\alpha_s+3\varphi)\cos(\alpha_s+4\varphi)}.\end{eqnarray}](img103.gif) |
(59) |
| (60) |
mul_sktch11
Figure 23 Sketch to show the computation
of in equation 61.
|
| ![mul_sktch11](../Gif/mul_sktch11.gif) |
These equations are in terms of
, which is not known. However,
from Figure
we see that
| ![\begin{displaymath}
\tilde{Z}_s=\tilde{Z}_D-h_D\sin\varphi,\end{displaymath}](img105.gif) |
(61) |
and
can be computed from the traveltime of the zero
surface-offset trace, since, according to Figure
| ![\begin{displaymath}
t_m(0)=\frac{2\tilde{Z}_D}{V_1\cos\varphi}+\frac{2\tilde{Z}_...
...\varphi}=\frac{2\tilde{Z}_D(1+\cos(2\varphi))}{V_1\cos\varphi},\end{displaymath}](img106.gif) |
(62) |
from which it follows immediately that
| ![\begin{displaymath}
\tilde{Z}_D=\frac{V_1t_m(0)\cos\varphi}{2[1+\cos(2\varphi)]}.\end{displaymath}](img77.gif) |
(63) |
mul_sktch12
Figure 24 Sketch to show the computation
of in equation 63.
|
| ![mul_sktch12](../Gif/mul_sktch12.gif) |
Finally, we need to compute
. Applying the law of sines to
triangle ABC in Figure
we get
| ![\begin{displaymath}
\sin(\alpha_s+2\varphi)=\frac{2h_D\cos(2\varphi)}{V_1t_m},\end{displaymath}](img107.gif) |
(64) |
from which we get
| ![\begin{displaymath}
\alpha_s=\sin^{-1}\left[\frac{2h_D\cos(2\varphi)}{V_1t_m}\right]-2\varphi.\end{displaymath}](img80.gif) |
(65) |
mul_sktch16
Figure 25 Sketch to compute
the takeoff angle of the source ray from a non-diffracted multiple
from a dipping water-bottom.
|
| ![mul_sktch16](../Gif/mul_sktch16.gif) |
D
Next: From dip to no
Up: Alvarez: Multiples in image
Previous: Computation of Image Depth
Stanford Exploration Project
11/1/2005