\[ \sigma_{\theta \theta}^{min} = 3 S_{hmin} - S_{Hmax} - 2 P_p - \Delta P - \sigma^{\Delta T} = -T_0 \]
© Cambridge University Press Zoback, Reservoir Geomechanics (Fig. 7.2, pp. 211)
© Cambridge University Press Zoback, Reservoir Geomechanics (Fig. 7.3, pp. 213)
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© Cambridge University Press Zoback, Reservoir Geomechanics (Fig. 7.3, pp. 213)
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© Cambridge University Press Zoback, Reservoir Geomechanics (Fig. 7.5, pp. 216)
When \(S_3 \sim S_v\) integrate density logs
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© Cambridge University Press Zoback, Reservoir Geomechanics (Fig. 7.4, pp. 214)
\[ \Delta P = P_b - P_p \]
so
\[ S_{Hmax} = 3 S_{hmin} - P_b - P_p + T_0 \]
or
\[ S_{Hmax} = 3 S_{hmin} - P_b(T=0) - P_p \]
Consider a system with compressibility \(\beta_s\)
\[ \beta_s = \frac{\Delta V_s}{V_s} \frac{1}{\Delta P} \]
\[ \Delta P = \frac{1}{\beta_s V_s} \Delta V_s \]
\[ \frac{\Delta P}{\Delta t} = \frac{1}{\beta_s V_s} \frac{\Delta V_s}{\Delta t} \]
Answer: Not very well.
Shortcourse on Reservoir Geomechanics - John T. Foster - May 2023