Mechanisms of overpressure

Disequilibrium compaction

  • Ongoing sedimentation increases overburden (vertical stress) faster than fluid diffuses out of zone

Characteristic time of diffusion in porous medium

$${}$$$$ \tau = \frac{(\phi \beta_f + \beta_r) \eta l^2}{k} $$
  • low-permiability sand (~1 md)
    • $\tau$ on the order of years for $l=0.1$km
  • low-permiability shale (~10 nd)
    • $\tau$ on the order of 100,000 years for $l=0.1$km

Common in Gulf of Mexico

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© John Wiley & Sons, Inc. Gordon and Flemmings, 1998

Techtonic compaction

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  • Occurs in areas where large-scale tectonic stress changes occur over geolocgically short periods of time.

Hydrocarbon column heights

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Image Source

Hydrocarbon column heights

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© Cambridge University Press Zoback, Reservoir Geomechanics (Fig. 2.11, pp. 42)

Centroid effects

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© Cambridge University Press Zoback, Reservoir Geomechanics (Fig. 2.12, pp. 43)

Other mechanisms

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Aquathermal pressurization

  • Temperature increases due to radioactive decay and upward heat flow from mantle

Hydrocarbon generation

  • From thermal maturation of kerogen

Direct measurement of pore pressure

  • Via wireline samplers that isolate formation pressure from annular pressure in a small area at the wellbore wall.
  • Mud weight

Estimation of pore pressure at depth

Confined compaction experiment

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© Cambridge University Press Zoback, Reservoir Geomechanics (Fig. 2.13, pp. 46)

Shale compaction relation

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$\phi = \phi_0 e^{-\beta (S_v - P_p)}$

Use with caution!

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© Cambridge University Press Zoback, Reservoir Geomechanics (Fig. 2.14, pp. 48)

Porosity inference from $P$-waves

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$P_p = S_v + \left(\frac{1}{\beta} \ln\left(\frac{\phi}{\phi_0}\right)\right) \quad \quad \phi = 1 - \left(\frac{\Delta t_{ma}}{\Delta t}\right)^{\frac{1}{f}}$

Compaction $P$-wave Pore pressures

© Cambridge University Press Zoback, Reservoir Geomechanics (Figs. 2.16a,b, pp. 48, Fig. 2.8b, pp. 36)