Simultaneous Solution of Multiphase Reservoir Flow Equations

1970 ◽  
Vol 10 (02) ◽  
pp. 99-110 ◽  
Author(s):  
H.G. Weinstein ◽  
H.L. Stone ◽  
T.V. Kwan

Abstract A strongly implicit iterative procedure has been developed to solve systems of equations arising in multiphase, two-dimensional reservoir flow problems. The two-dimensional, two-phase and problems. The two-dimensional, two-phase and two-dimensional, three-phase algorithms have been evaluated by several test problems and compared with the corresponding alternating direction iterative routines. The strongly implicit procedure (SIP) has been found to have several advantages in the solution of reservoir problems. It is fast, and in problems with extreme anisotropy in the transmissibilities and/or highly irregular geometries it can obtain a solution where the alternating direction procedure many times cannot. For the problems tested, it bas been found that a reliable set of iteration parameters is easily calculated from the coefficient matrix. Finally, SIP appears to be relatively insensitive to the rounding errors inherent in machine computations. Introduction The efficient solution of multidimensional reservoir problems involving the flow of two- or three-fluid phases is essential in petroleum reservoir simulation. Because of nonlinearities and generally complex geometries and boundary conditions, analytic solutions of the differential equations are at present impossible. One must, instead, seek solutions of the finite difference approximations of the equations through iterative techniques. Many iterative methods have been developed. Most of these, including relaxation and successive overrelaxation techniques, require excessive computer effort because they converge rather slowly or fail to converge. The more implicit alternating direction iteration procedure (ADIP) converges faster than the relaxation and overrelaxation schemes and, in general, requires less computational work. More recently, a new iterative technique has been developed. This technique is called the strongly implicit procedure, or simply SIP. It was demonstrated by Scone that SIP achieved greater rates of convergence than ADIP on all problems tested except the simple model problem in which the coefficients in the difference equation were constant and isotropic. Furthermore, the advantage of SIP over ADIP appears to increase as the complexity of the problem increases. SIP was originally developed and tested for the solution of a single equation in two-space dimensions. Its improved convergence over ADIP in this case led naturally to the development of SIP for the simultaneous solution of two or three coupled equations in two dimensions, such as arise in the simultaneous-solution approach to multiphase two-dimensional flow problems. SIP has also been extended to the solution of multiphase reservoir flow problems in three-space dimensions. The development and testing of the latter procedure is discussed elsewhere. In this paper, the SIP algorithms for two-dimensional problems are presented. The algorithms have been evaluated by presented. The algorithms have been evaluated by several test problems and compared with the corresponding ADIP routines. TWO DIMENSIONS: THE MULTIPHASE PROBLEM For purposes of generality, the system to be studied is comprised of coupled, two-dimensional parabolic equations. Employing this system will parabolic equations. Employing this system will facilitate investigation of any problem related to the two-dimensional flow of several fluids in a porous medium. porous medium. SPEJ P. 99

1966 ◽  
Vol 6 (04) ◽  
pp. 350-362 ◽  
Author(s):  
K.H. Coats ◽  
M.H. Terhune

Abstract Analysis and example applications have been performed to compare the accuracy and computing speed of alternating-direction explicit and implicit procedures (ADEP and ADIP) in numerical solution of reservoir fluid flow problems. ADIP yields significantly greater accuracy and requires about 60 per cent more computing time than ADEP, not 300 or 500 per cent more as reported elsewhere. Introduction Several recent papers discuss an alternating-direction explicit difference approximation (ADEP) to the diffusion equation. Example applications of ADEP and ADIP were reported to support conclusions that ADEP is comparable in accuracy to ADIP and requires one-fifth to one-third the computing time of ADIP. Applications of ADEP in calculation of two-phase flow in reservoirs was also proposed. This study was performed to compare further the relative merits of ADEP and ADIP in simulation of two-dimensional flow of one and two fluid phases in reservoirs. Since two-phase flow equations are often essentially elliptic rather than parabolic, the efficiency of ADEP in solving the elliptic equation was also examined. ADIP AND ADEP DIFFERENCE EQUATIONS The diffusion equation: ...................(1) governs heat conduction, molecular diffusion and slightly compressible fluid flow through porous media for the case of homogeneous, isotropic media. The ADEP procedure involves replacement of Eq. 1 at odd time steps by: ,.................(2) and at even time steps by: ,.................(3) where Sweeping a two-dimensional grid from southwest to northeast using Eq. 2 and from northeast to southwest using Eq. 3 allows direct (explicit) calculation of u at the new time step at each grid point. SPEJ P. 350ˆ


2012 ◽  
Vol 9 (1) ◽  
pp. 47-52
Author(s):  
R.Kh. Bolotnova ◽  
V.A. Buzina

The two-dimensional and two-phase model of the gas-liquid mixture is constructed. The validity of numerical model realization is justified by using a comparative analysis of test problems solution with one-dimensional calculations. The regularities of gas-saturated liquid outflow from axisymmetric vessels for different geometries are established.


1979 ◽  
Vol 101 (3) ◽  
pp. 341-347 ◽  
Author(s):  
M. Couston ◽  
J. J. Angelini

An alternating-direction implicit algorithm is applied to solve an improved formulation of the low-frequency, small-disturbance, two-dimensional potential equation. Linear solutions are presented for oscillating trailing edge flaps, plunging and pitching flat-plate airfoils, and compared with results obtained by a doublet-lattice-method. Nonlinear calculations for both steady and unsteady flow problems are then compared with results obtained by using the complete Euler equations. The present procedure allows one to solve complex aerodynamic problems, including flows with shock waves.


Author(s):  
Raymond Lavoie ◽  
Kelley Main ◽  
Anastasia Stuart-Edwards

AbstractThis research advances the conceptualization and measurement of flow. The results of six studies (N = 2809) reveal that flow has two dimensions: “fluency,” which is comprised of experiences related to fluent thought and action; and “absorption,” which is based on sustained full attention. The results also demonstrate that the two dimensions have nuanced relationships with other variables. Specifically, while the fluency dimension is related to antecedents of flow (familiarity, skill, progress), the absorption dimension is not. Conversely, the absorption dimension was found to be strongly related to consequences of flow (behavioral intentions, presence), while the fluency dimension was not. Furthermore, we demonstrate that fluency-related experiences can give rise to the absorption-related experiences, which advances our understanding of how flow emerges. Finally, we develop a refined measure of flow called the two-dimensional-flow scale, and demonstrate its enhanced ability to capture variance in flow and other related variables in leisure contexts.


1993 ◽  
Vol 60 (1) ◽  
pp. 65-69
Author(s):  
D. N. Contractor

An inviscid analysis is conducted of two-dimensional flow between a flat plate pivoting about an external point and falling onto another plate at rest. The motion of the fluid between the two plates is analyzed by the simultaneous solution of the unsteady Bernoulli equation, the equation of continuity, and the equation of motion for the plate. Numerical solution of the equations resulted in velocities and pressures along the plate as a function of time. The pressures were integrated to yield forces and moments on the falling plate. The results are compared with the motion of a horizontal flat plate falling vertically onto a rigid stationary flat plate. The two results are similar to one another.


Sign in / Sign up

Export Citation Format

Share Document