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| where <math> a = \frac{1}{2\cos^{2}\theta}, b = 0.5-\left [ 2\left ( \frac{Vs}{Vp} \right )^{2}\sin^{2}\theta \right ], c = -4\left ( \frac{Vs}{Vp} \right )^{2}\sin^{2}\theta </math> | | where <math> a = \frac{1}{2\cos^{2}\theta}, b = 0.5-\left [ 2\left ( \frac{Vs}{Vp} \right )^{2}\sin^{2}\theta \right ], c = -4\left ( \frac{Vs}{Vp} \right )^{2}\sin^{2}\theta </math> |
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− | and <math> \rho = \frac{\rho_2+\rho_1}{2}, \Delta \rho = \rho_2 - \rho_1 </math> | + | and |
| + | <math> \rho = \frac{\rho_2+\rho_1}{2}, \Delta \rho = \rho_2 - \rho_1 </math> |
| <math> Vp = \frac{Vp_2+Vp_1}{2}, \Delta Vp = Vp_2 - Vp_1 </math> | | <math> Vp = \frac{Vp_2+Vp_1}{2}, \Delta Vp = Vp_2 - Vp_1 </math> |
| <math> Vs = \frac{Vs_2+Vs_1}{2}, \Delta Vs = Vs_2 - Vs_1 </math> | | <math> Vs = \frac{Vs_2+Vs_1}{2}, \Delta Vs = Vs_2 - Vs_1 </math> |
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| '''c) Hilterman (1983)''' | | '''c) Hilterman (1983)''' |
| Hilterman simplified Bortfeld equations by separating the reflection coefficients into the form of acoustic and elastic : | | Hilterman simplified Bortfeld equations by separating the reflection coefficients into the form of acoustic and elastic : |
| + | |
| + | <math> R(\theta_1) = \frac{Vp_2\rho_2\cos\theta_1 - Vp_1\rho_1\cos\theta_2}{Vp_2\rho_2\cos\theta_1 + Vp_1\rho_1\cos\theta_2 }+ \left ( \frac{\sin\theta_1 }{Vp_1}\right )\left ( Vs_1+Vs2 \right )\left [ 3\left ( Vs_1-Vs2 \right ) + \frac{2\left ( Vs_2\rho_1 - Vs_1\rho_2 \right )}{\rho_2 + \rho_1} \right ] </math> |
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| '''d) Shuey Approximation (1985)''' | | '''d) Shuey Approximation (1985)''' |
| Shuey modified Aki and Richard equation by using variable of poisson ratio as follows: | | Shuey modified Aki and Richard equation by using variable of poisson ratio as follows: |
| + | |
| + | <math> R(\theta_1) = R_p + \left [ R_p A_o + \frac {\Delta\sigma}{1-\sigma^{2}} \right ]\sin^{2}\theta + \frac{\Delta\alpha }{2\alpha}\left ( \tan^{2}\theta-\sin^{2}\theta \right ) </math> |
| + | |
| + | where |
| + | <math> \sigma =\frac{\left ( \sigma _1+\sigma _2 \right )}{2}, \Delta \sigma = \left ( \sigma _2-\sigma _1 \right )</math> |
| + | <math> A_o = B-2\left ( 1+B \right )\frac{1-2\sigma }{1-\sigma } </math> |
| + | <math> B = \frac{\frac{\Delta \alpha }{\alpha }}{\frac{\Delta \alpha }{\alpha }+ \frac{\Delta \rho }{\rho }}</math> |
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