The way the quantized value of conductance in a quantum wire disappear
s is predicted as a function of temperature and length of the wire by
taking account of both impurity scattering and mutual Coulomb interact
ions, i.e., in the case of a dirty Tomonaga-Luttinger liquid. It is sh
own that quantization of conductance is realized for short wires, whil
e for longer wires the effect of impurity scattering is important and
a deviation from the quantized value becomes apparent especially at lo
w temperatures. In this case the conductance shows a distinctive tempe
rature dependence.