Transient heat conduction in a slab

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SUMMARY

The discussion focuses on transient heat conduction in an infinitely wide slab of solid material with a thickness of 2L, emphasizing the derivation of the temperature equation T at a distance z from the central plane over time t. The governing equation is established as dT/dt = A ∂²T/∂η², where η = z/L and A represents a group of parameters. Participants highlight the importance of performing an energy balance and suggest that the control volume area Δa will cancel out during derivation, ultimately leading to the Fourier equation. The discussion also clarifies that the problem is one-dimensional and advises against non-dimensionalizing until after the derivation is complete.

PREREQUISITES
  • Understanding of transient heat conduction principles
  • Familiarity with the Fourier heat conduction equation
  • Basic knowledge of energy balance concepts in thermodynamics
  • Ability to work with partial derivatives in multi-variable calculus
NEXT STEPS
  • Study the derivation of the Fourier heat conduction equation in detail
  • Learn about energy balance techniques in thermodynamic systems
  • Explore the concept of lumped capacity and its applications
  • Investigate the implications of semi-infinite solids in heat conduction problems
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Students and professionals in thermodynamics, mechanical engineers, and anyone involved in heat transfer analysis, particularly those focusing on transient heat conduction in solid materials.

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Homework Statement



Consider unsteady state heat conduction through an infinitely wide slab of solid material of thickness 2L. There is no internal heat generation and the thermal properties of the material are independent of temperature and position. Starting from an energy balance, show that the temperature T at a distance z from the central plane at time t is described by an equation of the form

\frac{dT}{dt} = A \frac{\partial^{2}T}{\partial\eta^{2}}where η = z/L and A is a group of parameters. Define A.

The Attempt at a Solution



I want to perform a energy balance, which should come out in the form:

aq = a(q+dq)+\frac{\partial H}{\partial t}

where a is the area and then I can probably solve it from there
However, in this case I can't do so as because the slab is infinitely wide I can't get a. Is there a problem with the way I'm visualising it in three dimensions or should I be taking a different approach to the energy balance?
 
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I'm no expert and have just started with thermodynamics but I think you should look at lumped capacity and semi-infinite solids
 
Based on the equation you cite, the problem is one dimensional and you are being asked to derive the Fourier equation. Call your control volume area Δa. The areas will all cancel out once you finish the derivation. The derivative with respect to time should be a partial derivative because you have two independent variables, time and space.

I would not worry about non-dimensionalizing until after you complete the derivation.
 

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