Heat flow rate with non-constant k through plane wall

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SUMMARY

The discussion focuses on calculating the heat flow rate through a plane wall with variable thermal conductivity defined by the equation k(T) = k0(1 + βT). The two methods presented for solving the problem involve applying Fourier's law and integrating under boundary conditions. The final expression for heat transfer rate, Q̇, is derived as Q̇ = -k0A/L [T2 + (β/2)T22 - T1 - (β/2)T12]. The discussion also clarifies the implications of negative heat flow rates and the behavior of thermal conductivity in different materials.

PREREQUISITES
  • Understanding of Fourier's law of heat conduction
  • Knowledge of thermal conductivity and its temperature dependence
  • Ability to perform integration with boundary conditions
  • Familiarity with steady-state heat transfer concepts
NEXT STEPS
  • Study the derivation of heat conduction equations in non-homogeneous materials
  • Learn about the implications of variable thermal conductivity in heat transfer analysis
  • Explore numerical methods for solving heat transfer problems with variable properties
  • Investigate the physical significance of boundary conditions in thermal analysis
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Students and professionals in mechanical engineering, thermal engineering, and materials science who are involved in heat transfer analysis and thermal management of materials.

  • #31
Yes and the equation agrees with the plot for a large finite beta
 

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