drilling · pressure

Eaton Pore Pressure (Resistivity)

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MODE:
Inputs
psi/ft
psi/ft
Ω·m
Ω·m
ft
Description
Predicts formation pore pressure from a deep resistivity log by comparing observed resistivity to a normal compaction trend, using the Eaton (1975) exponent method's resistivity form. A sibling of the sonic-based Eaton method (eaton_pp) — same paper, same normal-compaction-trend logic, but resistivity rises with compaction where sonic slowness falls, so the ratio and the direction of the overpressure signal are inverted relative to the sonic form.
Variables
Variable symbols, units, and descriptions for this calculation
SymbolUnitDescription
PPpsi/ftPore Pressure Gradient
PPpsiPore Pressure
EMWlb/galEquivalent Mud Weight
OBGpsi/ftOverburden (lithostatic) pressure gradient from an integrated bulk density log or regional model — typically 0.90-1.05 psi/ft.
Pnpsi/ftNormal (hydrostatic) pore pressure gradient for the basin — typically 0.433-0.465 psi/ft depending on water salinity.
RnΩ·mShale resistivity expected for a normally compacted, normally pressured section at this depth, read from a calibrated normal resistivity trend line. Fitted independently from the sonic normal trend (DTn) — resistivity and sonic normal trends are calibrated against different log responses and are not interchangeable.
RobsΩ·mObserved shale resistivity from a deep resistivity log at this depth. Values lower than the normal trend (Rn) indicate undercompaction and overpressure — the opposite direction from the sonic method, since resistivity rises with compaction while sonic slowness falls.
nEmpirical exponent in the Eaton resistivity equation. The default of 1.2 is Eaton's (1975) commonly cited value — distinct from the sonic method's n=3.0 default — and should be recalibrated to local offset wells with MDT/RFT data where possible.
TVDftTrue vertical depth of the point of interest, used to convert the predicted pressure gradient into an absolute pressure and equivalent mud weight.
Assumptions
  • The normal resistivity compaction trend (Rn) has been correctly established from offset wells or regional shale trends in normally pressured sections — fitted independently from any sonic normal trend
  • The lithology is predominantly shale — the Eaton resistivity method is calibrated for shale and is less reliable in sands, carbonates, or evaporites
  • The Eaton resistivity exponent n is appropriate for the basin; the default n=1.2 should be recalibrated against direct pressure measurements (MDT/RFT) where available
Limitations
  • Resistivity-derived pore pressure is an estimate, not a measurement — always calibrate against direct pressure data (MDT, RFT, kicks, mud weight history) where available
  • Hydrocarbon effect (resistivity increases in a hydrocarbon-bearing zone independent of pressure) can produce a spurious high-resistivity reading that mimics normal or under-pressure
  • The method assumes a single compaction mechanism (disequilibrium compaction); other overpressure mechanisms (fluid expansion, lateral transfer, hydrocarbon generation) may not follow the same resistivity-pressure relationship
Use Cases
  • Cross-check against sonic-based Eaton prediction: Compare the resistivity-based and sonic-based (eaton_pp) pore pressure estimates at the same depth as an independent confirmation, since the two logs respond to compaction through different physical mechanisms.
  • Pre-drill pore pressure prediction where sonic is unavailable: Build a pre-drill pore pressure profile from offset well resistivity logs when sonic data is sparse or of poor quality.
  • Real-time geopressure monitoring while drilling: Continuously update the pore pressure estimate using LWD resistivity data to detect developing overpressure ahead of the bit.
  • Mud weight window design: Establish the safe mud weight window between pore pressure and fracture gradient for the planned well path, cross-checked against the sonic-based estimate.
Related Calculations
Region Notes
Gulf of Mexico
Classic Eaton application area — the resistivity form is the traditional cross-check against the sonic form in Plio-Pleistocene shale sections below major sand bodies.
Haynesville
Severely overpressured shale gas play; the default n=1.2 often under-predicts pressure here, similar to the sonic form's n=3.0 needing upward recalibration after MDT calibration.
References
Primary source
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