Point of maximum depth
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| Series | Geophysical References Series |
|---|---|
| Title | Digital Imaging and Deconvolution: The ABCs of Seismic Exploration and Processing |
| Author | Enders A. Robinson and Sven Treitel |
| Chapter | 2 |
| DOI | http://dx.doi.org/10.1190/1.9781560801610 |
| ISBN | 9781560801481 |
| Store | SEG Online Store |
We have found the parametric equations for the circular raypath that starts at the origin and makes an angle Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://en.wikipedia.org/api/rest_v1/":): {\theta }_0 with the positive y-axis (Figure 13). This raypath represents a diving wave that reaches a maximum depth at point Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://en.wikipedia.org/api/rest_v1/":): D{\rm =}\left(x_D{\rm ,\ }y_D\right) and then returns to the surface. The tangent to the raypath is horizontal at D. Thus, the angle from the vertical is Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://en.wikipedia.org/api/rest_v1/":): {\rm 9}0^{{\rm o}} , that is, Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://en.wikipedia.org/api/rest_v1/":): \theta {\rm =} {\theta }_D{\rm =} \pi {\rm /2} at the depth point. Inserting Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://en.wikipedia.org/api/rest_v1/":): {\rm \ cos\ }\ \theta {\ =\ cos\ }{\theta }_D{\ =\ 0} and Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://en.wikipedia.org/api/rest_v1/":): {\rm \ sin\ }\theta {\ =\ sin\ }{\theta }_D{\ =} {\ 1} in the above parametric equations, we obtain the coordinates of the depth point as
Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://en.wikipedia.org/api/rest_v1/":): \begin{align} x_D&{\rm =}\frac{v_0}{a{\rm \ tan\ }{\theta }_0} \end{align}
Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://en.wikipedia.org/api/rest_v1/":): \begin{align} y_D&{\rm =}\frac{v_0}{a{\rm \ sin\ }{\theta }_0}-\frac{v_0}{a}{\rm =}\frac{v_0}{a}\left(\frac{{\rm l}} {{\rm \ sin\ }{\theta }_0}-{\rm 1}\right) . \end{align} ()
Let Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://en.wikipedia.org/api/rest_v1/":): t_D denote the traveltime along the raypath from the origin to the point of maximum depth. At the point of maximum depth, the angle is Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://en.wikipedia.org/api/rest_v1/":): \theta {\rm =} {\theta }_D{\rm =}\pi {\rm /2} . Thus, the implicit equation for the traveltime Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://en.wikipedia.org/api/rest_v1/":): t_D is
$ {\begin{aligned}e^{at_{D}}&{\rm {=}}{\frac {{\rm {\ tan\ }}{\frac {{\theta }_{D}}{\rm {2}}}}{{\rm {\ tan\ }}{\frac {{\theta }_{0}}{\rm {2}}}}}{\rm {=}}{\frac {{\rm {\ tan\ }}{\frac {\pi }{\rm {4}}}}{{\rm {\ tan\ }}{\frac {{\theta }_{0}}{\rm {2}}}}}{\rm {=}}{\frac {\rm {l}}{{\rm {\ tan\ }}{\frac {{\theta }_{0}}{\rm {2}}}}}{\rm {=}}{\frac {\rm {l}}{\frac {{\rm {1}}-{\rm {\ cos\ }}{\theta }_{0}}{{\rm {\ sin\ }}{\theta }_{0}}}}{\rm {=}}{\frac {{\rm {\ sin\ }}{\theta }_{0}}{{\rm {l}}-{\rm {\ cos\ }}{\theta }_{0}}},\end{aligned}} $ ()

which also can be written as
Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://en.wikipedia.org/api/rest_v1/":): \begin{align} e^{-at_D}&{\rm =\ tan\ }\frac{{\theta }_0}{{\rm 2}} {\rm =}\frac{{\rm l}-{\rm \ cos\ }{\theta }_0}{{\rm \ sin\ }{\theta }_0}. \end{align} ()
These implicit equations involve exponentials. There are two common ways to get rid of exponentials: by logarithms and by hyperbolic functions. We choose the latter. The hyperbolic cosine is defined as $ {\rm {\ cosh\ }}u{\rm {=}}\left(e^{\mathbf {u} }{\rm {+}}e^{-\iota \iota }\right){\rm {/2}} $. Similarly, the hyperbolic sine is defined as Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://en.wikipedia.org/api/rest_v1/":): {\rm \ sinh\ }u{\rm =}\left(e^{\mathbf{u}}-e^{-\mathbf{u}}\right){\rm /2} . We thus have
Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://en.wikipedia.org/api/rest_v1/":): \begin{align} {\rm \ cosh\ }at_D{\rm =}\frac{e^{at_D}{\rm +}e^{-at_D}} {{\rm 2}}{\rm =}\frac{\frac{{\rm \ sin\ }{\theta}_0}{{\rm 1}-{\rm \ cos\ }{\theta }_0}{\rm +}\frac{{\rm 1}-{\rm \ cos\ }{\theta }_0}{{\rm \ sin\ }{\theta }_0}}{{\rm 2}}{\rm =}\frac{{{\rm sin}}^{{\rm 2}}{\theta }_0{\rm +}{\left({\rm 1}-{\rm \ cos\ }{\theta }_0\right)}^{{\rm 2}}}{{\rm 2}\left({\rm l}-{\rm \ cos\ }{\theta }_0\right){\rm \ sin\ }{\theta }_0}{\rm =}\frac{{\rm l}}{{\rm \ sin\ }{\theta }_0} \end{align} ()
and, similarly,
Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://en.wikipedia.org/api/rest_v1/":): \begin{align} {\rm \ sinh\ }at_D&{\rm =}\frac{e^{at_D}-e^{-a{{\rm t}} _O}}{{\rm 2}}{\rm =}\frac{{\rm l}}{{\rm 2}}\left(\frac{{\rm \ sin\ }{\theta }_0}{{\rm 1}-{\rm \ cos\ }{\theta }_0}-\frac{{\rm 1}-{\rm \ cos\ }{\theta }_0}{{\rm \ sin\ }{\theta }_0}\right){\rm =}\frac{{\rm l}}{{\rm \ tan\ }{\theta }_0}. \end{align} ()
In terms of traveltime to the point of maximum depth, the point of maximum depth is given by the coordinates
Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://en.wikipedia.org/api/rest_v1/":): \begin{align} x_D{\rm =}\frac{v_0}{a{\rm \ tan\ }{\theta }_0}{\rm =}\frac{v_0}{a}{\rm \ sinh\ }at_D \end{align}
Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://en.wikipedia.org/api/rest_v1/":): \begin{align} y_D&{\rm =}\frac{v_0}{a{\rm \ sin\ }{\theta }_0}-\frac{v_0}{a}{\rm =}\frac{v_0}{a}\left({\rm \ cosh\ }at_D-{\rm 1}\right) . \end{align} ()
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Also in this chapter
- Reflection seismology
- Digital processing
- Signal enhancement
- Migration
- Interpretation
- Rays
- The unit tangent vector
- Traveltime
- The gradient
- The directional derivative
- The principle of least time
- The eikonal equation
- Snell’s law
- Ray equation
- Ray equation for velocity linear with depth
- Raypath for velocity linear with depth
- Traveltime for velocity linear with depth
- Wavefront for velocity linear with depth
- Two orthogonal sets of circles
- Migration in the case of constant velocity
- Implementation of migration
- Appendix B: Exercises