A NOTE ON THE SOLUTION TO THE DIFFUSION EQUATION
β Scribed by WANG, Y.
- Publisher
- John Wiley and Sons
- Year
- 1996
- Tongue
- English
- Weight
- 498 KB
- Volume
- 20
- Category
- Article
- ISSN
- 0363-9061
No coin nor oath required. For personal study only.
β¦ Synopsis
Three methods (Gauss-Legendre method, Stehfest method and Laplace transform method) are used to evaluate a solution of a coupled heat-fluid linear diffusion equation. Comparing with the results by Jaeger, the accuracy and efficiency of the Stehfest and Gauss-Legendre methods and the limitations of the truncated solutions obtained by Laplace transformation are discussed. It is concluded that the Stehfest method gives accurate results and is numerically more efficient than the other two methods, particularly for the solutions in early time. Two transformations with u = -In(x) and u = arctan(xn/2), where u is the original integral variable, are considered in the Gauss-Legendre method.
π SIMILAR VOLUMES
We present a new strategy to accelerate the convergence rate of a high-accuracy multigrid method for the numerical solution of the convection-diffusion equation at the high Reynolds number limit. We propose a scaled residual injection operator with a scaling factor proportional to the magnitude of t
Plane radial flow of water in a closed aquifer towards a circular well or heat flow through a homogeneous conducting solid from a circular hole to infinity are well known problems that were solved long ago. The solution is expressed in terms of an integral of ordinary Bessel functions. A new solutio
The solution of the linear system Ax = b by iterative methods requires a splitting of the coefficient matrix in the form A = M -N where M is usually chosen to be a diagonal or a triangular matrix. In this article we study relaxation methods induced by the Hermitian and skew-Hermitian splittings for
Weak solution of the Euler equations is defined as an L 2 -vector field satisfying the integral relations expressing the mass and momentum balance. Their general nature has been quite unclear. In this work an example of a weak solution on a 2-dimensional torus is constructed that is identically zero
## A general analytical solution to the finite-difference time-( ) domain FDTD scalar-wa¨e equation is deri¨ed in terms of its initial conditions using Fourier analysis. The fundamental sources of FDTD modeling error, namely, phase and sampling errors, are demonstrated by comparing this expression