derivation of heat equation


Let us consider the heat conduction in a ϱ and specific heat capacity c.  Denote by  u⁢(x,y,z,t)  the temperature in the point  (x,y,z)  at the time t.  Let a be a surface in the matter and v the spatial region by it.

When the growth of the temperature of a volume element d⁢v in the time d⁢t is d⁢u, the element releases the amount

-d⁢u⁢c⁢ϱ⁢d⁢v=-ut′⁢d⁢t⁢c⁢ϱ⁢d⁢v

of heat, which is the heat flux through the surface of d⁢v.  Thus if there are no sources and sinks of heat in v, the heat flux through the surface a in d⁢t is

-d⁢t⁢∫vc⁢ϱ⁢ut′⁢𝑑v. (1)

On the other hand, the flux through d⁢a in the time d⁢t must be proportional to a, to d⁢t and to the derivative of the temperature in the direction of the normal line of the surface element d⁢a, i.e. the flux is

-k⁢∇⁡u⋅d⁢a→⁢d⁢t,

where k is a positive (because the heat always from higher temperature to lower one).  Consequently, the heat flux through the whole surface a is

-d⁢t⁢∮ak⁢∇⁡u⋅d⁢a→,

which is, by the Gauss’s theorem, same as

-d⁢t⁢∫vk⁢∇⋅∇⁡u⁢d⁢v=-d⁢t⁢∫vk⁢∇2⁡u⁢d⁢v. (2)

Equating the expressions (1) and (2) and dividing by d⁢t, one obtains

∫vk⁢∇2⁡u⁢d⁢v=∫vc⁢ϱ⁢ut′⁢𝑑v.

Since this equation is valid for any region v in the matter, we infer that

k⁢∇2⁡u=c⁢ϱ⁢ut′.

Denoting  kc⁢ϱ=α2,  we can write this equation as

α2⁢∇2⁡u=∂⁡u∂⁡t. (3)

This is the differential equationMathworldPlanetmath of heat conduction, first derived by Fourier.

References

  • 1 K. Väisälä: Matematiikka IV.  Handout Nr. 141. Teknillisen korkeakoulun ylioppilaskunta, Otaniemi, Finland (1967).
Title derivation of heat equation
Canonical name DerivationOfHeatEquation
Date of creation 2013-03-22 18:45:04
Last modified on 2013-03-22 18:45:04
Owner pahio (2872)
Last modified by pahio (2872)
Numerical id 9
Author pahio (2872)
Entry type Derivation
Classification msc 35K05
Classification msc 35Q99
Related topic DerivationOfWaveEquation