Full model for

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Full model for $\gamma(\omega)$

The high- and low-frequency limits are again causally connected via the simple function

$\begin{displaymath} \gamma(\omega) = \gamma_{sq} \sqrt{1-\frac{i\omega}{\omega_{sq}}}\end{displaymath}$ (124)

but now the parameters are defined as

$\begin{eqnarray} \gamma_{sq}&=&\frac{v_2 k_2}{\eta L_2^2} \\ \omega_{sq} &=& \fr... ...ta \alpha_2} \frac{k_2}{L_2^2} \left(\frac{v_2 V/S}{L_2}\right)^2.\end{eqnarray}$ (125)

(126)

Stanford Exploration Project
10/14/2003

	$\begin{eqnarray} \gamma_{sq}&=&\frac{v_2 k_2}{\eta L_2^2} \\ \omega_{sq} &=& \fr... ...ta \alpha_2} \frac{k_2}{L_2^2} \left(\frac{v_2 V/S}{L_2}\right)^2.\end{eqnarray}$	(125)
		(126)