a cfd model for a progressing cavity pump · 2010. 7. 9. · 4th latin american cfd workshop...
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4th Latin American CFD Workshop
Applied to the Oil and Gas Industry
July 12-13, 2010 - Rio de Janeiro - Brazil
Organization: Support:
A CFD Model for a Progressing Cavity Pump
Emilio E. Paladino*, João Alves de Lima
†
PPGEM - Graduate Program in Mechanical Engineering,
Federal University of Rio Grande do Norte, CEP 59072-970- Natal - RN
*e-mail: [email protected]
†e-mail:[email protected]
ABSTRACT
The growth of Progressing Cavity Pump as artificial lift system in the last years lead to the development of
models for the flow behavior within these devices. Based on the ideas of the system creator, Rene Moineau, usual
flow models attempt to establish relations between differential pressure and flow rate by considering a Poiseuille
flow along the seal lines between cavities in order to predict the internal slip which is subtracted from the
displaced volumetric flow rate. In addition, some attempts for more detailed models including computational
solutions for the flow in static simplified geometries can be encountered in previous works. Nevertheless no models considering the solution for the full transient 3D Navier-Stokes equations and relative motion rotor and
stator were found in literature. This work presents a computational model for the unsteady 3D flow, using an
element based finite volume method, which includes the relative motion between rotor and stator, in a Progressing Cavity Pumps. The computational model for the flow in a Progressing Cavity Pump was
implemented in CFX11 [1]. This software is based on a discretization of the governing equations using and
Element Based Finite Volume Method ([2]; [3]; [4]) and a coupled approach for solving the pressure-velocity
decoupling ([5]).
The numerical flow computation within positive displacement pumps is, in general, a challenging task as it
normally requires moving mesh simulations. Furthermore, depending on the pump type, the need of discretization
of small clearances between rotor and stator introduces serious difficulties into the mesh generation process. In
addition, for the specific case of PCPs, the pump kinematics are very complex (when compared with a
reciprocating pump, for instance). , the main challenge in this work was the imposition of the mesh motion and mesh generation process, mainly, because of the need of mesh quality control (element distortion) in regions near
the seal lines
The model developed is capable of the accurate prediction of volumetric efficiency and viscous looses as well as provide detailed information of pressure and velocity field inside this device. This could allow, for example, the
prediction of local stator deformation in order to predict how this influences on slip, the accurate treatment of
turbulence effects, by using advanced turbulence models, and the model extension for the case of multiphase flows, which is a common case in artificial lift.
The model was validated against experimental results from literature, as can be seen in Figure 1. The model
successfully predicts the performance for high (oil 42 cP) and low (Water) viscosity fluids. For the caso of low
viscosity fluids, simplified models based on Pouseuille flow in seal regions, use to fail [6]. Some aspects related
to the dynamic behavior of the flow, not captured by the simplified models, are analyzed using this model. In
Figure 2, the pressure distribution along the pump stator is showed. This information, no available in simplified
models, allows the calculation of the stator deformation, in the case of elastomeric stators.
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4th Latin American CFD Workshop
Applied to the Oil and Gas Industry
July 12-13, 2010 - Rio de Janeiro - Brazil
Organization: Support:
0 25 50 75 100 125 150 175 200
∆P [psig]
0
50
100
150
200
250
300
QNET [bpd]
Present Work: Model
Gamboa et al. (2003): Exper
300 rpm
100 rpm
400 rpm
200 rpm
0 10 20 30 40 50 60
∆P [psig]
0
50
100
150
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Q [bpd]
WaterPresent work: Model
Gamboa et al (2003) : Exper.
400 rpm
300 rpm
Figure 1 - Comparison of model results with experimental results from [7]
Figure 2 - Pressure distibution along the stator for different rotor positions
References
[1] ANSYS CFX 11 Theory Manual , ANSYS Inc., Cannonsbourg, PA, USA (2008)
[2] Baliga, B. R. and Patankar, S. V., A New Finite Element Formulation for Convection-
Diffusion Problems, Numerical Heat Tranfer, 3, (1980) 393-409.
[3] Ferziger, J. H. & Peric, M., Computational Methods for Fluid Dynamics, Springer-Verlag Telos, (2001).
[4] Maliska, C. R., Transferência De Calor e Mecânica Dos Fluidos Computacional (in
Portuguese), LTC Editora, (2004). [5] Raw, M. J., A New Control-Volume-Based Finite Element Procedure for Numerical
Solution of the Fluid Flow and Scalar Transport Equations , University of Waterloo,
Canada (1985). [6] Gamboa, J.; Olivet, J.; Espin, S.. New Approach for Modelling Progressive Cavity Pumps
Performance, Proceedings of SPE Annual Technical Conference and Exhibition, Denver,
Colorado, USA, (2003).
[7] Olivet, J.; Gamboa, J.; Kenyery, F.. Experimental Study of Two-Phase Pumping in a
Progressive Cavity Pump Metal to Metal, Proceedings of SPE Annual Technical
Conference and Exhibition, San Antonio, Texas, SPE 77730 (2002).