2011
DOI: 10.1002/app.34090
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Generalized magneto‐thermoelastic medium with variable material properties subjected to ramp‐type heating

Abstract: The equations of magneto-generalized thermoelasticity with one relaxation time with variable electrical and thermal conductivity for one-dimensional problems are cast into a matrix form using the statespace approach and Laplace transform techniques. The resulting formulation is applied to a problem of a half space where the bounded plane is subjected to a ramptype heating and a traction free. This takes place when a constant magnetic field permeates the medium in the absence of an external electric field. The … Show more

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Cited by 9 publications
(4 citation statements)
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“…For the numerical results, silicon (Si) has been taken as the thermoelastic semiconducting material, for which we take the following values of the different physical constants [7,[33][34][35]: 𝜇 = 5.46×10 10 kg m -1 s -2 , 𝜆 =3.64×10 10 kg m -1 s -2 , 𝜌 = 2330 kg m -3 , 𝐶 = 695 m 2 K -1 s -2 , 𝛼 = 3.0×10 -6 K -1 , 𝐾 = 150 kg m k -1 s -3 , 𝜑 = 1.0.…”
Section: Numerical Resultsmentioning
confidence: 99%
See 1 more Smart Citation
“…For the numerical results, silicon (Si) has been taken as the thermoelastic semiconducting material, for which we take the following values of the different physical constants [7,[33][34][35]: 𝜇 = 5.46×10 10 kg m -1 s -2 , 𝜆 =3.64×10 10 kg m -1 s -2 , 𝜌 = 2330 kg m -3 , 𝐶 = 695 m 2 K -1 s -2 , 𝛼 = 3.0×10 -6 K -1 , 𝐾 = 150 kg m k -1 s -3 , 𝜑 = 1.0.…”
Section: Numerical Resultsmentioning
confidence: 99%
“…Now, we must determine the thermal loading function 𝑓 𝑡 , so we will consider that the thermal loading function is a ramp-type heating which takes the form [7,33,34]:…”
Section: Problem Formulation In the Laplace Transform Domainmentioning
confidence: 99%
“…A constant magnetic field with the components H = (0, H O , 0) is permeating the medium in the absence of an external electric field. Since no external electric field is applied, and the effect of polarization of the ionized medium can be neglected, it follows that the total electric field E vanished identically inside the medium [14]. Now for the one-dimensional problems, all of the considered functions will depend only on the space variable x and the time t. The governing equations for generalized magnetothermo-viscoelasticity (MTVE) (Eqs.…”
Section: Formulation Of the Problemmentioning
confidence: 99%
“…Ezzat and Youssef [13] established a new model for magnetothermoelastic medium with variable electrical and thermal conductivity and solved many problems in this field. Youssef and El Bary [14] solved a problem in the previous medium properties involving ramp-type heating.…”
Section: Introductionmentioning
confidence: 99%