Abstract
It is shown that, if thermal phonons are scattered by both processes which conserve and also by those which do not conserve wave number, then the thermal conductivity K may be expressed as a power series of the form
Here τ, C, v and α are respectively the relaxation time for normal processes, the specific heat, the phonon velocity and a numerical constant. K0 is inversely proportional to the strength of those processes which do not conserve wave number and hence, by measuring experimentally how K varies with the strength of these processes, the value of τ may be found. The method is applied to lithium fluoride giving results which are in reasonable agreement with those obtained in earlier work by more complicated analysis.