2004
DOI: 10.1016/j.icheatmasstransfer.2004.05.011
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Dual-Phase-Lag Heat Conduction Model in Thin Slab Under the Effect of a Moving Heating Source

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Cited by 7 publications
(4 citation statements)
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“…To obtain their corresponding expression in the time domain, we take their respective Laplace inverses. These, however, could be obviously difficult hence we employed a numerical method; the Riemann-Sum Approximation Method used by Khadrawi et al 29 and later by Jha and Isa. 30 This approach requires that the Laplace inverse of any function U y p ̅ ( , ) can be obtained from…”
Section: Riemann-sum Approximation Methodsmentioning
confidence: 99%
See 1 more Smart Citation
“…To obtain their corresponding expression in the time domain, we take their respective Laplace inverses. These, however, could be obviously difficult hence we employed a numerical method; the Riemann-Sum Approximation Method used by Khadrawi et al 29 and later by Jha and Isa. 30 This approach requires that the Laplace inverse of any function U y p ̅ ( , ) can be obtained from…”
Section: Riemann-sum Approximation Methodsmentioning
confidence: 99%
“…To obtain their corresponding expression in the time domain, we take their respective Laplace inverses. These, however, could be obviously difficult hence we employed a numerical method; the Riemann‐Sum Approximation Method used by Khadrawi et al 29 and later by Jha and Isa 30 . This approach requires that the Laplace inverse of any function trueU̅(y,p) $\mathop{U}\limits^{̅}(y,p)$ can be obtained from U(y,t)=eεtt][12trueU¯(y,ε)+Rek=1ntrueU¯y,ε+italicikπt(1)k, $U(y,t)=\frac{{e}^{\varepsilon t}}{t}\left[\frac{1}{2}\bar{U}(y,\varepsilon )+Re\sum _{k=1}^{n}\bar{U}\left(y,\varepsilon +\frac{{ik}\pi }{t}\right){(-1)}^{k}\right],$ where Re $Re$ is the real part of the expression, i=1 $i=\sqrt{-1}$ is the imaginary number, and n $n$ is the number of iterations used while ε $\varepsilon $ is the real part of the Bromwich contour used for inverting a function from the Laplace domain to its corresponding time domain.…”
Section: Mathematical Analysismentioning
confidence: 99%
“…Bioheat application [133,134] Laplace transformation technique [71,92,93,135,136] Cartesian, Cylindrical, Spherical 1-D, 2-D CV, DPL Hybrid method [93]. Moving heating source [136] Other analytical methods [137][138][139][140][141][142][143][144][145][146][147] Cartesian 1-D, 2-D, 3-D CV, DPL Fourier series [137]: Constant heat flux and constant temperature BC, [138,139]: fluctuating harmonic heating source. Spectral [140]: CV model, Chebyshev polynomials.…”
Section: Uniquenessmentioning
confidence: 99%
“…The axisymmetric problem of the CV non-Fourier model for the regions interior and exterior to a circular cylinder is investigated by using the methods of Laplace transformation and asymptotic analysis [135]. Also, the Laplace transformation technique is used to obtain the solution of the DPL model under the effect of a moving heat source [136] and the CV model in a radial one-dimensional heat conduction process for a hollow sphere [71].…”
Section: Laplace Transformation Techniquementioning
confidence: 99%