Umudike Journal of Engineering and Technology

Michael Okpara University of Agriculture, Umudike


EVALUATION OF THE EFFECTS OF DROPLETS IN OFFSHORE OIL WELLS

Akpan, S. C.
Department of Mechanical Engineering, Michael Okpara University of Agriculture, Umudike, P. M. B 7267, Umuahia, Abia State. Nigeria

Eze, C. C.
Department of Mechanical Engineering, Michael Okpara University of Agriculture, Umudike, P. M. B 7267, Umuahia, Abia State. Nigeria

Ugwu, H. U.
Department of Mechanical Engineering, Michael Okpara University of Agriculture, Umudike, P. M. B 7267, Umuahia, Abia State. Nigeria

Ubani, N. O.
Department of Mechanical Engineering, Michael Okpara University of Agriculture, Umudike, P. M. B 7267, Umuahia, Abia State. Nigeria



ABSTRACT

This study evaluates the effects of droplets in offshore oil well. These droplets are carried to the surface to avoid forming films on the tubing, accumulating at the bottom of the well and resulting into liquid loading as the main effect; which is disastrous. The focus has been on the eradication of liquid loading in the oil well and this streamlined the determination of fluid properties, droplet sizes, velocity, flow rate as well as the critical velocity to lift the droplets from bottom of the well to the surface.The fluid properties were determined using an engineering simulation software called ‘ASPEN HYSYS’ and was done based on a given composition of oil well. The droplets (sizes) were modelled with the assumptions of the droplets being spherical in shape and smooth. Based on the principle that if gas flow provides sufficient energy to hold droplet(s) in suspension; the gravity is equal to the sum of drag force and buoyancy. Also, if the droplet deforms into a regular oblate spheroid of an ellipsoidal cross section as a result of the flow regime and the surface still smooth; Turner’s et al model was applied and the maximum droplet sizes were obtained as 0.001440m, 0.000648m, 0.000645m and 0.000647m at the bottom, middle, surface and separator respectively. The velocities to lift the droplets to the surface were obtained as 5.33 m/s and 5.32m/s while critical velocity was 0.2358m/s. The rates to lift droplets were 0.0336m3/s and 0.0335m3/s. Since liquid loading occurs where producing gas velocity is less than the critical velocity, this means that the velocities at these points are adequate.


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Published
Thursday, December 27, 2018

Issue
Vol. 4 No. 2, DEC 2018

Article Section
GENERAL

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