Adsorbed and Free Gas

Part 16, Chapter 16: Unconventional and Source-Rock Petrophysics

Learning objectives

  • Distinguish free gas in the pores from adsorbed gas on the kerogen
  • Use the Langmuir isotherm for the adsorbed gas content
  • Add free and adsorbed gas to get total gas-in-place
  • Explain the desorption tail as pressure falls during production

Gas in Two Places

A shale-gas reservoir stores its gas two ways. Some is free gas in the pore space and microfractures, exactly like a conventional reservoir, and its amount grows with pressure. The rest is adsorbed gas, molecules clinging to the enormous internal surface of the kerogen, held there by pressure.

Adsorbed and free gas050100150200250010002000300040005000gas content (scf/ton)pressure (psi)VL 150totaladsorbedfreeadsfreeAdsorbed gas (Langmuir) plateaus at VL; free gas grows with pressure; the total is the sum.

The Langmuir Isotherm

The adsorbed content follows the Langmuir isotherm,

Vads=VLPPL+P,V_{ads} = \frac{V_L\,P}{P_L + P},

which rises steeply at low pressure and then flattens toward the capacity VLV_L, the most the kerogen can hold (more kerogen, higher VLV_L). PLP_L is the pressure at which the rock holds half its capacity. The total gas-in-place is the free gas plus this adsorbed gas.

The Desorption Tail

The split is what makes shale production distinctive. As the well draws the pressure down, the free gas drains first. Then, as the pressure keeps falling, the adsorbed gas desorbs off the kerogen and feeds the well for years, the long, slow tail that conventional reservoirs do not have. A shale with little adsorbed gas declines fast; one rich in kerogen produces gently for a long time.

References

  • Langmuir, I. (1918). The adsorption of gases on plane surfaces of glass, mica and platinum. J. Am. Chem. Soc., 40(9), 1361-1403.
  • Ambrose, R. J. et al. (2012). Shale gas-in-place calculations. SPE Journal, 17(1).

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