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Determination of gas-diffusion and interface-mass-transfer coefficients in fracture-heavy oil saturated porous matrix system

Ehsan Zamanian ; Petroleum Engineering Department, Amirkabir University of Technology, Tehran, Iran, Research Institution of Petroleum Industry (R.I.P.I.)-Polymer Division
Mahmoud Hemmati ; Research Institution of Petroleum Industry (R.I.P.I.)-Polymer Division
Mahmoud Safar Beiranvand


Puni tekst: hrvatski pdf 103 Kb

str. 359-363

preuzimanja: 875

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Puni tekst: engleski pdf 1.128 Kb

str. 351-358

preuzimanja: 2.488

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Sažetak

For the modeling and simulation of oil recovery from naturally fractured reservoirs during the gas injection process, an accurate value of the molecular diffusion coefficient (MDC) of gases from a gas filled fracture into the oil matrix is essential. During the injection of miscible fluids with oil, transport of the injectant and oil are controlled by fracture and matrix properties. Diffusion is a significant-oil recovery mechanism between matrix and fracture. However, experimentally determined data concerning to gas transfer between fracture-matrix systems by diffusion mechanism are relatively rare.
In this study the pressure-decay method is applied to obtain effective molecular diffusion coefficient of CO2 and CH4 in heavy oil saturated porous matrix media at different conditions of temperatures. Gas-diffusion and interface-mass-transfer coefficients are determined by applying a transient-state equilibrium diffusion model. The effect of porous media presence on these coefficients has also been investigated.
It is expected that the experimental results will be useful in deriving the matrix-fracture transfer function by diffusion, which is required for simulation of recovery in naturally fractured reservoirs.

Ključne riječi

molecular diffusion coefficient; interface-mass-transfer; fracture; porous matrix; heavy oil; fractured reservoir

Hrčak ID:

95410

URI

https://hrcak.srce.hr/95410

Datum izdavanja:

31.12.2012.

Podaci na drugim jezicima: hrvatski

Posjeta: 4.087 *