dc.contributor.author |
Zathiha, M. M. |
|
dc.contributor.author |
Faham, M. A. A. M. |
|
dc.date.accessioned |
2022-11-30T04:40:26Z |
|
dc.date.available |
2022-11-30T04:40:26Z |
|
dc.date.issued |
2022-11-15 |
|
dc.identifier.citation |
Proceedings of the 11th Annual Science Research Sessions, FAS, SEUSL, Sri Lanka 15th November 2022 pp.38. |
en_US |
dc.identifier.isbn |
978-624-5736-60-7 |
|
dc.identifier.isbn |
978-624-5736-59-1 |
|
dc.identifier.uri |
http://ir.lib.seu.ac.lk/handle/123456789/6283 |
|
dc.description.abstract |
In a variety of scientific domains, the heat equation has many fundamental
importance. Heat is a type of energy that can be found in any substance. The
physical phenomena of the one-dimensional heat equation were investigated in this
research study by generating the model with Dirichlet boundary conditions and
initial conditions. This model was solved using the numerical method of finite
difference of the explicit Forward Time Centered Space (FTCS) and implicit
Backward Time Centered Space (BTCS) schemes, derived from the Taylor series
expansion for the required orders. Then we have interpreted the basic behaviour of
the numerical solutions of the derived model with diverse initial conditions of
trigonometric function, polynomial function, exponential function, and piece-wise
function. For these four illustrative test example problems, we also have
considered and compared on the stability criteria of the numerical results for the
produced solutions using the Von-Neumann stability analysis techniques. From
the solutions, we have found that the explicit FDM – FTCS method is very easy to
calculate numerically and show the stability only for 𝑟 ≤ 0.5. Whereas implicit
FDM - BTCS method is unconditionally stable and computer time required at each
step is higher. In addition, the simulation method is utilized to assess performance
based on accuracy and programming implementations in MATLAB with twodimensional and three-dimensional graphical representations employed for various
time steps and stability requirements. Where we can conclude the stability criteria
are met when the parameters are changed to meet the desired criteria. |
en_US |
dc.language.iso |
en_US |
en_US |
dc.publisher |
Faculty of Applied Sciences, South Eastern University of Sri Lanka, Sammanthurai. |
en_US |
dc.subject |
one-dimensional heat equation |
en_US |
dc.subject |
Explicit and implicit finite difference method |
en_US |
dc.subject |
Von-Neumann stability analysis |
en_US |
dc.title |
Numerical solution and stability analysis of one-dimensional heat equation |
en_US |
dc.type |
Article |
en_US |