Article | REF: BE8200 V1

Thermal energy transmission - Conduction

Author: Alain DEGIOVANNI

Publication date: April 10, 1999

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2. Application: unidirectional conduction

2.1 Continuous operation

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2.1.1 General

The transfer equation reduces to :

div ( λgradT ) + p = 0

In the case of dead conduction (no internal source), the system is flux-conserving since :

div ( λgradT ) = 0 → divϕ = 0

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Application: unidirectional conduction