Fractal Viscous Fingers

Fragmentation of viscous fingers in porous media: A three dimensional video microscopic study

Soft Matter ◽

10.1039/c2sm06803f ◽

2012 ◽

Vol 8 (21) ◽

pp. 5791 ◽

Cited By ~ 3

Author(s):

Prerna Sharma ◽

P Aswathi ◽

Anit Sane ◽

Shankar Ghosh ◽

Sabyasachi Bhattacharya

Keyword(s):

Porous Media ◽

Microscopic Study ◽

Three Dimensional ◽

Viscous Fingers

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'Peacock' viscous fingers

Nature ◽

10.1038/356113a0 ◽

1992 ◽

Vol 356 (6365) ◽

pp. 113-113 ◽

Cited By ~ 5

Author(s):

J. M. GARCíA-RUIZ

Keyword(s):

Viscous Fingers

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Dynamics and Structure of Viscous Fingers in Porous Media

Time-Dependent Effects in Disordered Materials ◽

10.1007/978-1-4684-7476-3_10 ◽

1987 ◽

pp. 111-138 ◽

Cited By ~ 13

Author(s):

Knut Jørgen Måløy ◽

Finn Boger ◽

Jens Feder ◽

Torstein Jøssang

Keyword(s):

Porous Media ◽

Viscous Fingers

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Stability Considerations in Downward Miscible Displacements

Society of Petroleum Engineers Journal ◽

10.2118/961-pa ◽

1964 ◽

Vol 4 (04) ◽

pp. 356-362 ◽

Cited By ~ 23

Author(s):

J.M. Dumore

Keyword(s):

Transition Zone ◽

Viscous Fingering ◽

Favorable Effect ◽

Homogeneous Layer ◽

Oil Viscosity ◽

Critical Rate ◽

Miscible Displacements ◽

Viscous Fingers ◽

The Stability ◽

Definition Of

Abstract If, in a vertical, downward miscible displacement, the transition zone between the displacing and displaced fluids is neglected, a criterion for stable displacement can be obtained by considering a small hypothetical protrusion of one of the fluids into the other. This criterion leads to the definition of the well-known critical rate, uc = kg ??/?µ. The consideration is further extended by taking into account the transition zone that develops as a result of diffusion and mixing. A generalization of the previous criterion leads to the definition of another characteristic rate, the stable rate, which in actual miscible drives will be less than the critical rate. In such drives, the entire transition zone is stable at rates less than the stable rate. At rates between the stable and critical rates, the displacement is only partly stable, i.e. part of the transition zone adjacent to the displaced fluid is in an unstable position. From that part of the transition zone viscous fingers will develop. At rates greater than the critical rate the entire displacement is unstable and viscous fingers will develop more strongly. Results of laboratory experiments are in agreement with the expected behavior based on the theoretically deduced stability of the displacement. INTRODUCTION The simplest form of miscible drive in an oil-bearing formation is the injection of a fluid that is completely miscible* with the oil under reservoir conditions. In general, such a fluid, a solvent for example, is less dense and less viscous than the oil present in the formation. If it is injected into a horizontal homogeneous layer, gravitational forces will lead to the formation of a gravity tongue of solvent in the upper part of the layer and the adverse solvent-oil viscosity ratio will cause viscous fingers to develop. If, however, the solvent is injected up-structure into a dipping layer, gravity has a favorable effect, because it tends to keep the less dense solvent up-structure. Tongue formation and viscous fingering are consequently reduced and it is even possible that they will be suppressed completely. Viscous fingering and gravity tonguing are the consequences of the instability of the displacement. A stable displacement cannot result in growing viscous fingers and/or growing gravity tongues. Since large amounts of oil can be bypassed if there is viscous fingering and/or gravity tonguing, the stability of a miscible drive is very important with respect to the recovery efficiency of the drive. The stability is of particular importance in miscible-slug drives, as it determines how quickly the miscible slug between the displaced and displacing fluids will be distorted and broken up, after which the drive is no longer completely miscible. Stability is thus a most important factor in determining the success of a miscible drive, and it is considered that the aspects of stability considered in this paper will make a useful contribution to existing theories. Consideration is given only to vertical downward displacements, in which no gravity tongues can develop and which are therefore simpler than downward displacements in sloping layers.

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