2010
DOI: 10.1007/s10543-010-0287-z
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Convergence analysis of finite element approximations of the Joule heating problem in three spatial dimensions

Abstract: In this paper we present a finite element discretization of the Joule-heating problem. We prove existence of solution to the discrete formulation and strong convergence of the finite element solution to the weak solution, up to a sub-sequence. We also present numerical examples in three spatial dimensions. The first example demonstrates the convergence of the method in the second example we consider an engineering application.

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Cited by 12 publications
(11 citation statements)
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“…Theoretical analyses for the nonlinear thermistor system have been done extensively, see, e.g., [3,5,9,19,32,33]. Numerical methods and analysis for the time-dependent nonlinear thermistor system (1.1)-(1.4) can be found in [2,4,12,31,34,35].…”
Section: Introductionmentioning
confidence: 99%
“…Theoretical analyses for the nonlinear thermistor system have been done extensively, see, e.g., [3,5,9,19,32,33]. Numerical methods and analysis for the time-dependent nonlinear thermistor system (1.1)-(1.4) can be found in [2,4,12,31,34,35].…”
Section: Introductionmentioning
confidence: 99%
“…An application of Grönwall's lemma then shows that the left-hand side is bounded by Ck 2 . Using Equation (16) From these preliminary bounds, we may deduce the desired regularity of Θ n and Φ n and then test (17) with −∆e n θ to acquire e n θ 2…”
Section: Error Analysismentioning
confidence: 99%
“…(1) In the analysis of similar coupled problems in the field of Joule heating, the difficulties with the right-hand side data not having sufficient regularity in order to ensure uniqueness of the weak solution are also encounted. By following a similar approach to [32,33] and imposing boundedness on the solution to weak form of the electrostatics problem we can (22) thus ensuring uniqueness of the solution to (24).…”
Section: Electrostrictionmentioning
confidence: 99%
“…In the case of linearised electrostriction, the weak forms of electrostatics (32) and linearised elasticity (using either the displacement (33) or the mixed formulation (34)) are coupled in the sense that the deformation dependent permittivity tensor OEOE r .u/ becomes a function of the small strain tensor OEOE".u/, and the Cauchy stress tensor OEOE Q becomes a function of the electric field E . For materials with a weak electrostrictive coupling, Knops [3] has proposed a simplified mathematical model in which the permittivity tensor is assumed to be invariant to the linearised strain tensor, so that the electrostatic and linearised elasticity problems decouple resulting in OEOE r .u/ D r I.…”
Section: Coupled Strategymentioning
confidence: 99%