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Titlebook: Computational Micromagnetism; Andreas Prohl Textbook 2001 Springer Fachmedien Wiesbaden 2001 Direct Minimization.Micromagnetism.Nematic Li

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楼主: Helmet
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Direct Minimization of existing exchange energy contributions; this effect will be illustrated here for uniaxial materials, for the case of absent exterior fields .: . → ℝ., and . = 0. All results will be presented for . ⊂ ℝ., but can be generalized to . ⊂ ℝ. as well.
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Sucrose and osmotic dehydration,; electromagnetic coupling effects are incorporated in the (MLLG) equation. Part II closes with the numerical analysis for the nematic liquid crystal problem which also imposes a non-convex constraint onto its solution.
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Direct Minimizationtions can by rather costly, due to diverse patterns and scales of minimizing magnetizations. Moreover, they can blurr physical information in the case of existing exchange energy contributions; this effect will be illustrated here for uniaxial materials, for the case of absent exterior fields .: . →
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Relaxed Micromagnetism using Young Measures non-convex, it is not weakly closed in ..(.; ℝ.), and a solution to (I.4) does not have to exist for uniaxial materials; cf. for instance [71]. An implication is that highly oscillatory minimizing sequences of . do not have weak limits in .. One way to overcome this problem is to convexify the anis
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Summary and Outlookn magnetic recording, can have an enormous impact on future technologies. Their mathematical theory started with the introduction of the Landau-Lifshitz free energy; a numerical analysis of existing strategies to solve the corresponding minimization problem is presented in part I of this monograph.
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