Pore space hydrate formation in a glass bead sample from methane dissolved in water

[1] An experimental device designed and developed to grow methane hydrate in the pore space of a sediment was successfully used with a glass bead sample. The underlying idea for the experiment is that methane dissolved in water is transported with upward moving fluids from its place of origin at greater depths to formations within the hydrate stability field where the methane is removed from the pore water to form hydrate. This process is simulated in a closed loop flow system where methane charged water from a gas/water reservoir outside the hydrate stability field is pumped into the sediment sample cell in the stability field for methane hydrate. The fluid depleted of methane, then flows back into the gas/water reservoir to be recharged with methane. When the experiment was terminated due to blockage of flow by hydrate formation, hydrate saturation was about 95%.

[1]  M. Lee,et al.  Biot–Gassmann theory for velocities of gas hydrate‐bearing sediments , 2002 .

[2]  W. Waite,et al.  Laboratory synthesis of pure methane hydrate suitable for measurement of physical properties and decomposition behavior , 2000 .

[3]  B. Buffett,et al.  Phase equilibrium of gas hydrate: Implications for the formation of hydrate in the deep sea floor , 1997 .

[4]  J. Murphy,et al.  Acoustic and resistivity measurements on rock samples containing tetrahydrofuran hydrates: Laboratory analogues to natural gas hydrate deposits , 1986 .

[5]  Amos Nur,et al.  Elastic‐wave velocity in marine sediments with gas hydrates: Effective medium modeling , 1999 .

[6]  J. Brooks,et al.  Thermogenic Gas Hydrates in the Gulf of Mexico , 1984, Science.

[7]  Earl E. Davis,et al.  A mechanism for the formation of methane hydrate and seafloor bottom‐simulating reflectors by vertical fluid expulsion , 1992 .

[8]  Y. P. Handa Effect of hydrostatic pressure and salinity on the stability of gas hydrates , 1990 .

[9]  Attila I. Evrenos,et al.  Impermeation of Porous Media by Forming Hydrates In Situ , 1971 .

[10]  P. E. Baker Experiments on Hydrocarbon Gas Hydrates in Unconsolidated Sand , 1974 .

[11]  R. C. Weast CRC Handbook of Chemistry and Physics , 1973 .

[12]  M. Lee,et al.  Seismic velocities for hydrate-bearing sediments using weighted equation , 1996 .

[13]  Ross Anderson,et al.  Visual observation of gas-hydrate formation and dissociation in synthetic porous media by means of glass micromodels , 2001 .

[14]  Carolyn A. Koh,et al.  Clathrate hydrates of natural gases , 1990 .

[15]  M. Lee,et al.  Elastic properties of gas hydrate-bearing sediments , 2001 .

[16]  John A. Hudson,et al.  Elastic properties of hydrate‐bearing sediments using effective medium theory , 2000 .

[17]  K. Kvenvolden Gas hydrates—geological perspective and global change , 1993 .

[18]  E. Spangenberg Modeling of the influence of gas hydrate content on the electrical properties of porous sediments , 2001 .

[19]  D. Staykova,et al.  Ice perfection and onset of anomalous preservation of gas hydrates , 2004 .

[20]  C. Clayton,et al.  A laboratory investigation into the seismic velocities of methane gas hydrate‐bearing sand , 2005 .

[21]  W. Waite,et al.  Methane hydrate formation in partially water-saturated Ottawa sand , 2004 .

[22]  A. Nur,et al.  Sediments with gas hydrates; internal structure from seismic AVO , 1998 .

[23]  Bruce A. Buffett,et al.  Formation and accumulation of gas hydrate in porous media , 1997 .

[24]  William F. Waite,et al.  Physical properties and rock physics models of sediment containing natural and laboratory-formed methane gas hydrate , 2004 .

[25]  W. Durham,et al.  Anomalous Preservation of Pure Methane Hydrate at 1 atm , 2001 .