Fractional order theory of a perfect conducting thermoelastic medium
Creators
- 1. Alexandria Univ., Faculty of Education, Dept. of Mathematics, Alexandria (Egypt)
- 2. Nizwa Univ., Dept. of Mathematical and Physical Sciences, Nizwa (Oman)
Description
In this work, a new mathematical model of magneto-thermoelasticity theory is constructed in the context of a new consideration of heat conduction law with time-fractional order. This model is applied to a one-dimensional application for a perfect conducting half-space of elastic material, which is thermally shocked in the presence of magnetic field. Laplace transforms and state-space techniques (Ezzat. Can. J. Phys. 86, 1242, (2008)) will be used to obtain the general solution for any set of boundary conditions. According to numerical results and graphs, it is found that introducing a fractional derivative of order α has a significant effect on the temperature, stress, and heat flux distributions as well as the induced electric and magnetic fields; the curves are smoother in the case of 0 < α < 1 due to weak thermal conductivity. Some comparisons are made and shown in figures to estimate the effects of the fractional order parameter on all the studied fields. (author)
Availability note (English)
Available from DOI: https://doi.org/10.1139/P11-022Additional details
Identifiers
- DOI
- 10.1139/P11-022;
Publishing Information
- Journal Title
- Canadian Journal of Physics
- Journal Volume
- 89
- Journal Issue
- 3
- Journal Page Range
- p. 311-318
- ISSN
- 0008-4204
INIS
- Country of Publication
- Canada
- Country of Input or Organization
- Canada
- INIS RN
- 50013066
- Subject category
- S36: MATERIALS SCIENCE;
- Descriptors DEI
- BOUNDARY CONDITIONS; LAPLACE TRANSFORMATION; MAGNETIC FIELDS; MAGNETO-THERMAL EFFECTS; MATHEMATICAL MODELS; THERMAL CONDUCTIVITY; THERMOELASTICITY
- Descriptors DEC
- ELASTICITY; INTEGRAL TRANSFORMATIONS; MECHANICAL PROPERTIES; PHYSICAL PROPERTIES; THERMODYNAMIC PROPERTIES; TRANSFORMATIONS
Optional Information
- Notes
- 44 refs., 1 tab., 5 figs.