NO. 07 · Petrophysics & Reservoir

Porosity: The Space Between

Nothing on earth is worth more per cubic meter than properly counted emptiness. Density, neutron, and sonic each count the pore space through different physics and disagree instructively; NMR listens to the fluids living inside it; gas announces itself by fooling two tools in opposite directions; carbonates hide their porosity in vugs and molds that break the sonic's rules; and in the end the count must travel from the borehole to the whole field before it becomes barrels.

You can compute porosity from density, neutron, and sonic and explain each tool's lie, read gas crossover as a feature rather than an error, correct to effective porosity, read pore size from an NMR T2 distribution, explain why two carbonates at equal porosity flow like different rocks, place a rock against the critical-porosity ceiling, spread porosity per facies between wells, and carry the count into the volumetric equation with its uncertainty intact.

13 competencies · 3 interactive widget challenges · 3.5 to 5.5 hours of guided study
For petrophysicists and reservoir modelers who count the space for a living

Counting it

The space in the rock

Total, effective, connected: porosity is several numbers wearing one name, and the definitions decide which barrels are real before any tool gets a vote.

Density counts the mass deficit

The density log weighs the rock and the missing mass is the pore space; one honest linear equation, hostage only to the matrix density you assumed.

The neutron counts hydrogen

The neutron tool counts hydrogen and calls it porosity, which is true exactly when the pores hold water or oil and instructively false when they hold gas or the rock holds clay.

The neutron-density crossplot

Plot the two lies against each other and the truth appears: the crossplot reads porosity and lithology simultaneously, the single most used picture in petrophysics.

Gas crossover: the useful disagreement

Gas makes density read too high a porosity and neutron too low, and the curves cross over; the tool disagreement is the gas detector, error as signal.

The sonic counts the slowness

Wyllie's time average turns transit time into porosity, and its failures, compaction, gas, vugs, are each diagnostic; the third count completes the triangulation.

Applied: NMR and the T2 distributionwidget challenge

NMR skips the matrix entirely and listens to the fluids: the T2 distribution is a pore-size spectrum, splitting bound from free fluid, porosity that comes pre-sorted by usefulness.

Where it comes from, where it goes

The critical-porosity ceiling

Above critical porosity the sediment is a suspension, below it a frame; every rock's porosity history is a walk down from that ceiling, and the ceiling anchors the modulus trends.

Secondary porosity

Dissolution opens vugs and molds after burial, porosity the sonic cannot see because it rides the fast matrix path around them; the density-sonic gap becomes a measurement of the invisible.

The carbonate pore zoo

Interparticle, moldic, vuggy, microporous: carbonates hold one porosity in many architectures, and the architecture, not the amount, sets the stiffness and the flow.

Applied: the carbonate porosity paradoxwidget challenge

Two carbonates, same porosity, velocities a kilometer per second apart: pore shape is the hidden variable, and resolving the paradox is the capstone of porosity literacy.

From the count to the barrels

Applied: porosity between the wellswidget challenge

The borehole counted centimeters; the field needs every cell. Simulating porosity within each facies, honoring the histogram and the variogram, is how the count travels between wells without losing its statistics.

Porosity becomes barrels

The volumetric equation multiplies the counted space through area, thickness, saturation, and shrinkage; the path's every correction and caveat survives into this one line of arithmetic, which is why it was worth being careful.

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