2008
DOI: 10.1109/tmag.2007.916016
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A Coupled Thermo-Electromagnetic Formulation Based on the Cell Method

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Cited by 12 publications
(10 citation statements)
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“…Applying the energy balance equation to the dual volume of control [15], see Figure 3a, we obtain the following equation:MρCpdTdt+trueD˜(MλGT)=trueW˜,where Wfalse˜ is obtained once the system of equations (1) has been solved, Dfalse˜ represents the discrete divergence associated with the dual volume, being trueD˜=Gt, MρCp is the constitutive matrix in heat transmission in transitory state and Mλ is the thermal conductivity constitutive matrix. In this way, we obtain the heat sources in the disk, which are calculated as follows:trueW˜=1σtrueJ·trueJdtrueV˜,where Jfalse→ is calculated, by the following equation:trueJ=σ(truegrad…”
Section: The Constitutive Convective Matrix In the CMmentioning
confidence: 99%
“…Applying the energy balance equation to the dual volume of control [15], see Figure 3a, we obtain the following equation:MρCpdTdt+trueD˜(MλGT)=trueW˜,where Wfalse˜ is obtained once the system of equations (1) has been solved, Dfalse˜ represents the discrete divergence associated with the dual volume, being trueD˜=Gt, MρCp is the constitutive matrix in heat transmission in transitory state and Mλ is the thermal conductivity constitutive matrix. In this way, we obtain the heat sources in the disk, which are calculated as follows:trueW˜=1σtrueJ·trueJdtrueV˜,where Jfalse→ is calculated, by the following equation:trueJ=σ(truegrad…”
Section: The Constitutive Convective Matrix In the CMmentioning
confidence: 99%
“…(c) Cell method: Another related discretization program, based on general principles originally put forth in [50], [51], [49], is the Cell method [123], [124], [125], [126], [127], [128]. Even though this program does not rely on Whitney forms for constructing discrete Hodge star operators (other geometrically-based constructions are used instead), it is nevertheless still based upon the use of 'domain-integrated' discrete variables that conform to the notion of discrete differential forms or cochains of various degrees and, as such, it is naturally suited for irregular lattices.…”
Section: Appendix E: Overview Of Related Discretization Approachesmentioning
confidence: 99%
“…Multiphysical problems in bulk regions are discretized according to the CM formulation proposed in Alotto et al (2008).…”
Section: Electrical-thermal Model In Bulk Regionsmentioning
confidence: 99%
“…Inhomogeneous Neumann boundary conditions for modeling convective heat transfer are implemented according to Alotto et al (2008). Finally, electric and thermal equations are assembled into the following system of differential algebraic equations which can be solved in terms of electric potentials v and over-temperatures u:…”
Section: Electrical-thermal Model On Contact Interfacesmentioning
confidence: 99%