12 - Conduction - One Dimensional Heat Conduction Equation
5. Thermal Diffusvity α
Thermal Diffusvity (\(\alpha\))
\[\boxed{\alpha = \frac{k}{\rho C_P}}\]
Thermal diffusivity is a measure of the transient thermal response of a material to a change in temperature.
The larger the value of \(\alpha\), the faster will the heat diffuse through the material and its temperature will change with time.
This will result either due to a high value of conductivity \(k\) or a low value of \(\rho, C_P\).
Thermal diffusivity is a convenient collection of physical properties for transient solutions of the heat equation.
Recollect about ‘kinematic viscosity’ (\(\nu=\mu/\rho\)), which is also called as ‘momentum diffusivity’; and \(D_{AB}\).
Material | Thermal Diffusivity |
(cm\(^2\)/s) at 300 K | |
Copper | 1.15 |
Aluminum | 0.97 |
Stainless Steel (304) | 0.042 |
Silicon Dioxide (Polycrystalline) | 0.0083 |
Water | 0.0014 |
Polyvinyl Chloride (PVC) | 0.0008 |
Alcohol | 0.0007 |
Air | 0.19 |
Metals and gases have relatively high value of thermal diffusivity and their response to temperature changes is quite rapid.
The non metallic solids and liquids respond slowly to temperature changes because of their relatively small value of thermal diffusivity.