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 dv in the time dt is du, the element releases the amount
-ducϱdv=-u′tdtcϱdv |
of heat, which is the heat flux through the surface of dv. Thus if there are no sources and sinks of heat in v, the heat flux through the surface a in dt is
-dt∫vcϱu′t𝑑v. | (1) |
On the other hand, the flux through da in the time dt must be proportional to a, to dt and to the derivative of the temperature in the direction of the normal line of the surface element da, i.e. the flux is
-k∇u⋅d→adt, |
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
-dt∮ak∇u⋅d→a, |
which is, by the Gauss’s theorem, same as
-dt∫vk∇⋅∇udv=-dt∫vk∇2udv. | (2) |
Equating the expressions (1) and (2) and dividing by dt, one obtains
∫vk∇2udv=∫vcϱu′t𝑑v. |
Since this equation is valid for any region v in the matter, we infer that
k∇2u=cϱu′t. |
Denoting kcϱ=α2, we can write this equation as
α2∇2u=∂u∂t. | (3) |
This is the differential equation 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 |
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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 |