A Semi-Analytic Method for Thermal Coupling of Reservoir and Overburden

1972 ◽  
Vol 12 (05) ◽  
pp. 439-447
Author(s):  
H.G. Weinstein

Abstract A semianalytic method of handling the energy balance solution in the overburden has been developed. The method results in a single overburden energy coupling equation applicable at the reservoir - overburden boundary. This feature facilitates simultaneous solution of the pressure and energy equations in the reservoir. Test problems show the semianalytic method to compare favorably with the fully finite-difference technique. Both reservoir - overburden boundary temperature and the important factor of beat transfer into the overburden are accurately predicted by the method. predicted by the method. The semianalytic procedure may have considerable usefulness in the solution of reservoir problems. The method can definitely be applied in thermal simulation programs. Other anticipated applications are to an aquifer underlying a reservoir, an overlying gas cap, or to increasing definition in the vicinity of a wellbore. In each of these applications, the semianalytic procedure is expected to be considerably faster than the finite - difference solution. Introduction In thermal reservoir simulation programs, the material balances are solved over the reservoir; the energy balance is solved over the underburden-reservoir-overburden system. Hence, to avoid excess storage and computation time requirements, the material and energy balances are generally not solved simultaneously. In many cases it would be desirable to solve simultaneously the material balances (or equivalently, the pressure equation obtained by combining the material balances to eliminate saturation) and the energy balance. Problems with solution convergence and the treatment of mass transfer terms could be avoided in this way. This paper describes a semianalytic method of handling the energy balance solution in the overburden (and underburden). This solution results in a single overburden energy coupling equation that can be solved easily in conjunction with the reservoir pressure and energy equations. pressure and energy equations. The paper presents the mathematical development of the method and shows results for several test problems. The problems are similar to those encountered in thermal recovery processes. They compare the semianalytic method with the fully finite-difference procedure and, in one of the problems, with a completely analytic procedure and, in one of the problems, with a completely analytic solution. THEORY GOVERNING EQUATION AND BOUNDARY CONDITIONS Consider the overburden (and underburden) to be a homogeneous medium. The energy balance for the overburden can then be written as follows: (1) where is the density, C is the heat capacity, and khx, khy, khz, are the thermal conductivities in the x, y, z directions, respectively. The initial and boundary conditions for Eq. 1 are (2) Here we assume 0 x a, 0 y b to be the lateral extent of the reservoir and overburden, and 0 z to be the vertical extent of the overburden. SPEJ P. 439

1974 ◽  
Vol 14 (02) ◽  
pp. 152-164 ◽  
Author(s):  
H.G. Weinstein

Abstract A semianalytic method developed earlier couples the overburden energy balance solution to reservoir equations by a single differential equation applicable at the reservoir/overburden boundary. The semi-analytic method is extended in this work to allow temperatures at the reservoir/overburden boundary to decrease, as well as increase, with time. Computer calculations on several test problems show a close agreement of the semianalytic method with the fully finite-difference solution. Both reservoir/overburden boundary temperature and heat flux into the overburden are accurately calculated. Because of its extended generality, the semi-analytic procedure should be quite useful in solving reservoir problems. It is expected that in addition to being useful in thermal simulation programs, it will also be applicable to aquifer, programs, it will also be applicable to aquifer, gas-cap, pseudorelative-permeability, and wellbore problems. The method is faster and requires problems. The method is faster and requires significantly less computer storage than the finite-difference solution. Introduction Thermal reservoir simulation programs, to avoid excessive storage and computation-time requirements, generally do not solve the material balance and energy balance simultaneously, Instead, there an two separate solution steps. First, the material balances are solved over the reservoir; then, with updated pressures and saturations, the energy balance is solved over the underburden/reservoir/ overburden system. However, problems with solution convergence and the treatment of mass transfer terms could be avoided by simultaneously solving the energy balance and the material balances (or equivalently, the pressure equation obtained by combining the material balances to eliminate saturation). A recent paper showed how variational methods could be applied to eliminate the energy-balance solution in the overburden, and thus avoid the problems enumerated above. Included in the model problems enumerated above. Included in the model were a three-dimensional variational principle and an overburden temperature approximation proportional to the solution of the one-dimensional heat conduction equation. However, only the case of a monotonicallyincreasingreservoir/overburden boundary temperature was treated. Using a variational principle complementary to Weinstein's, Chase and O'Dell considered the flow of heat both into and out of the overburden. Their variational equation was one-dimensional, and the assumed overburden temperature function was a one-dimensional cubic polynomial, chosen because of its simplicity. Because the variational model was one-dimensional, no account could be taken of conduction parallel to the reservoir/overburden boundary. Thus, their results are restricted to situations where convection parallel to the reservoir dominates conduction. Chase and O'Dell derived two coupled nonlinear differential equations for the two free parameters of their model. An analytic solution was obtained for increasing boundary temperatures; however, the two equations had to be integrated numerically for decreasing boundary temperatures. To calculate their heat loss vector they had to perform an inner iteration with respect to both perform an inner iteration with respect to both temperature and time. Solving the parameter equations and solving for the heat flux vector were both time-consuming, leading to only a "moderate" savings in computation time over the fully finite-difference model. On the test problems they studied, the model showed increasing errors as the simulation proceeded through the soak and backflow periods. Presumably, these errors would continue to periods. Presumably, these errors would continue to grow if additional heat-flow reversals were invoked. The model to be described here has alleviated the shortcomings in Chase and O'Dell's procedure. This paper describes a generalized semianalytic method paper describes a generalized semianalytic method of handling the energy balance solution in the overburden (and underburden). This solution results in a single overburden energy coupling equation that can be solved easily in conjunction with the reservoir pressure and energy equations. The coupling equation pressure and energy equations. The coupling equation is general, whether reservoir/overburden boundary temperature increases or decreases with time, or increases at some boundary locations while decreasing at others. The paper presents the mathematical development of the extension of the original method to increasing and decreasing temperature problems. SPEJ P. 152


2010 ◽  
Vol 7 ◽  
pp. 182-190
Author(s):  
I.Sh. Nasibullayev ◽  
E.Sh. Nasibullaeva

In this paper the investigation of the axisymmetric flow of a liquid with a boundary perpendicular to the flow is considered. Analytical equations are derived for the radial and axial velocity and pressure components of fluid flow in a pipe of finite length with a movable right boundary, and boundary conditions on the moving boundary are also defined. A numerical solution of the problem on a finite-difference grid by the iterative Newton-Raphson method for various velocities of the boundary motion is obtained.


Mathematics ◽  
2019 ◽  
Vol 7 (10) ◽  
pp. 923 ◽  
Author(s):  
Abdul Ghafoor ◽  
Sirajul Haq ◽  
Manzoor Hussain ◽  
Poom Kumam ◽  
Muhammad Asif Jan

In this paper, a wavelet based collocation method is formulated for an approximate solution of (1 + 1)- and (1 + 2)-dimensional time fractional diffusion wave equations. The main objective of this study is to combine the finite difference method with Haar wavelets. One and two dimensional Haar wavelets are used for the discretization of a spatial operator while time fractional derivative is approximated using second order finite difference and quadrature rule. The scheme has an excellent feature that converts a time fractional partial differential equation to a system of algebraic equations which can be solved easily. The suggested technique is applied to solve some test problems. The obtained results have been compared with existing results in the literature. Also, the accuracy of the scheme has been checked by computing L 2 and L ∞ error norms. Computations validate that the proposed method produces good results, which are comparable with exact solutions and those presented before.


Robotica ◽  
2021 ◽  
pp. 1-12
Author(s):  
Xu-Qian Fan ◽  
Wenyong Gong

Abstract Path planning has been widely investigated by many researchers and engineers for its extensive applications in the real world. In this paper, a biharmonic radial basis potential function (BRBPF) representation is proposed to construct navigation fields in 2D maps with obstacles, and it therefore can guide and design a path joining given start and goal positions with obstacle avoidance. We construct BRBPF by solving a biharmonic equation associated with distance-related boundary conditions using radial basis functions (RBFs). In this way, invalid gradients calculated by finite difference methods in large size grids can be preventable. Furthermore, paths constructed by BRBPF are smoother than paths constructed by harmonic potential functions and other methods, and plenty of experimental results demonstrate that the proposed method is valid and effective.


1978 ◽  
Vol 45 (4) ◽  
pp. 812-816 ◽  
Author(s):  
B. S. Berger ◽  
B. Alabi

A solution has been derived for the Navier equations in orthogonal cylindrical curvilinear coordinates in which the axial variable, X3, is suppressed through a Fourier transform. The necessary coordinate transformation may be found either analytically or numerically for given geometries. The finite-difference forms of the mapped Navier equations and boundary conditions are solved in a rectangular region in the curvilinear coordinaties. Numerical results are given for the half space with various surface shapes and boundary conditions in two and three dimensions.


Symmetry ◽  
2018 ◽  
Vol 10 (10) ◽  
pp. 499 ◽  
Author(s):  
Chih Tso ◽  
Chee Hor ◽  
Gooi Chen ◽  
Chee Kok

The heat induced by viscous dissipation in a microchannel fluid, due to a small oscillating motion of the lower plate, is investigated for the first time. The methodology is by applying the momentum and energy equations and solving them for three cases of standard thermal boundary conditions. The first two cases involve symmetric boundary conditions of constant surface temperature on both plates and both plates insulated, respectively. The third case has the asymmetric conditions that the lower plate is insulated while the upper plate is maintained at constant temperature. Results reveal that, although the fluid velocity is only depending on the oscillation rate of the plate, the temperature field for all three cases show that the induced heating is dependent on the oscillation rate of the plate, but strongly dependent on the parameters Brinkman number and Prandtl number. All three cases prove that the increasing oscillation rate or Brinkman number and decreasing Prandtl number, when it is less than unity, will significantly increase the temperature field. The present model is applied to the synovial fluid motion in artificial hip implant and results in heat induced by viscous dissipation for the second case shows remarkably close agreement with the experimental literature.


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