Thermal Conductivity

Written by Jerry Ratzlaff on . Posted in Thermodynamics

Thermal conductivity, abbreviated as k, is the ability to transfer heat within a material without any motion of the material.  Depending on the material, the transfer rate will vary.  The lower the conductivity, the slower the transfer.  The higher the conductivity, the faster the transfer.

Typical thermal conductivity values for non-metallic solids can be found here.

Thermal Conductivity formula

\(\large{ k  =  \frac{Q \; l}{A \; \Delta T} }\)

\(\large{ k  =  \frac{Q \; l}{A \;  \left( T_h \;- \; T_l \right)    } }\)

\(\large{ k  =  \alpha \; \rho \; Q   }\)

Where:

\(\large{ k }\) = thermal conductivity

\(\large{ A }\) = area of the object

\(\large{ \rho }\)  (Greek symbol rho) = density

\(\large{ l }\) = length or thickness of material

\(\large{ Q }\) = specific heat capacity

\(\large{ \Delta T }\) = temperature differential

\(\large{ T_h }\) = high temperature

\(\large{ T_l }\) = low temperature

\(\large{ \alpha }\)  (Greek symbol alpha) = thermal diffusity

 

Tags: Equations for Thermal Equations for Heat