Understanding NMR relaxometry of partially water-saturated rocks

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Abstract

Nuclear magnetic resonance (NMR) relaxometry measurements are commonly used to characterize the storage and transport properties of water-saturated rocks. Estimations of these properties are based on the direct link of the initial NMR signal amplitude to porosity (water content) and of the NMR relaxation time to pore size. Herein, pore shapes are usually assumed to be spherical or cylindrical. However, the NMR response at partial water saturation for natural sediments and rocks may differ strongly from the responses calculated for spherical or cylindrical pores, because these pore shapes do not account for water menisci remaining in the corners of desaturated angular pores. Therefore, we consider a bundle of pores with triangular cross sections. We introduce analytical solutions of the NMR equations at partial saturation of these pores, which account for water menisci of desaturated pores. After developing equations that describe the water distribution inside the pores, we calculate the NMR response at partial saturation for imbibition and drainage based on the deduced water distributions. For this pore model, the NMR amplitudes and NMR relaxation times at partial water saturation strongly depend on pore shape, i.e., arising from the capillary pressure and pore shape-dependent water distribution in desaturated pores with triangular cross sections. Even so, the NMR relaxation time at full saturation only depends on the surface-to-volume ratio of the pore. Moreover, we show the qualitative agreement of the saturation-dependent relaxation-time distributions of our model with those observed for rocks and soils.

Figures

  • Figure 1. (a) NMR decay time distributions at different water saturation levels for a classical cylindrical capillary pore distribution. (b) Concept sketch of saturated (gray) and desaturated capillaries, e.g., during drainage.
  • Figure 2. (a) Complex pore structure of a Rotliegend tight gas sandstone. Pore spaces are filled with tangential and hairly illite and exhibit different pore types with elongated or slit-shaped, triangular, and multi-angular cross sections. (b) T1 decay time distributions calculated from inverse Laplace transform performed on Rotliegend sandstone (porosity 13 %, permeability 0.1 mD) at different water saturations (Sw = 21 %–100 %).
  • Figure 3. Cross sections of a partially saturated triangular tube. The arc meniscus of radius rAM separates the invading non-wetting phase (white) from the adsorbed wetting phase (gray). (a) Original triangle ABC with side lengths LAB, LBC, LCA, and radius R0 of its inscribing circle. (b) Reduced triangle A′B′C′ of similar geometry. The wetting phase resides in the three corners (gray) with r ′ = rAM being the radius of both the three interface arc menisci of ABC and of the inscribing circle of A′B′C′.
  • Figure 4. (a) Modeled distribution of water (gray) and gas (white) phases in an equilateral triangular tube with a side length of 1 µm during imbibition (top) and drainage (bottom). (b) Water saturation versus capillary pressure during imbibition (©) and drainage (N).
  • Figure 5. (a) Modeled distribution of water (gray) and gas (white) phases in a right-angled triangular capillary (G= 0.39) with side lengths L= 1, 0.81, 0.58 µm, and perimeter P = 2.39 µm during imbibition (top) and drainage (bottom). (b) Water saturation versus capillary pressure during imbibition (©) and drainage (N).
  • Figure 7. Saturated corner with active boundaries, i.e., ρs = ρ1 > 0 at the corner’s perimeter Pγ and a passive boundary at the air–water interface (meniscus), i.e., ρs = ρ = 0.
  • Figure 6. Longitudinal relaxation times T1 of fully saturated triangular pores with constant cross-sectional areaA= 4.33×10−13 m2 versus shape factor G= A P 2 and perimeter P . NMR parameters: ρs = 10 µ m s −1, T1B = 3.
  • Figure 8. Water (black) and air (white) distributions within a triangular pore (A0 = 4.33× 10 −13 m2, ρs = 10 µm s −1) at different capillary pressures for imbibition (a) with corresponding evolution of the (longitudinal) magnetization (b) and NMR T1 relaxation times (c).

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APA

Mohnke, O., Jorand, R., Nordlund, C., & Klitzsch, N. (2015). Understanding NMR relaxometry of partially water-saturated rocks. Hydrology and Earth System Sciences, 19(6), 2763–2773. https://doi.org/10.5194/hess-19-2763-2015

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