2022
DOI: 10.1109/tasc.2022.3159302
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Quasi-3D Magneto-Thermal Quench Simulation Scheme for Superconducting Accelerator Magnets

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Cited by 1 publication
(3 citation statements)
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“…where H 1 g (Ω) is the space of square integrable functions with square integrable weak gradient in Ω which fulfill the Dirichlet boundary condition (3). Furthermore, (•, •) Ω denotes the volume integral in Ω of the scalar product of the two arguments while ⟨•, • ′ ⟩ Γneu denotes the surface integral on Γ neu of the two arguments.…”
Section: Weak Formulationmentioning
confidence: 99%
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“…where H 1 g (Ω) is the space of square integrable functions with square integrable weak gradient in Ω which fulfill the Dirichlet boundary condition (3). Furthermore, (•, •) Ω denotes the volume integral in Ω of the scalar product of the two arguments while ⟨•, • ′ ⟩ Γneu denotes the surface integral on Γ neu of the two arguments.…”
Section: Weak Formulationmentioning
confidence: 99%
“…In order to aid the development and analysis of quench detection and protection methods for superconducting devices, appropriate numerical tools are needed (see, e.g. [1][2][3]). When using the finite element (FE) method, the small ratio of thickness of insulation or contact resistance layers to the thickness of the conductor can lead to numerical difficulties [4] since the accuracy of the method depends on the quality of the mesh [5, section 5.3].…”
Section: Introductionmentioning
confidence: 99%
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