The derivation of a Green's function for steady-state heat conduction in an
isotropic bimaterials is presented. The Green's function is obtained throug
h a Fourier representation to obtain both free-space, singular parts and re
gion-dependent, regular parts. To obtain the region-dependent parts of the
Green's function, the homogeneous solution is written using the virtual for
ce method. Full details of the necessary inversion integrals are provided.
The Green's function is shown to degenerate to the usual logarithmic potent
ial for steady-state heat conduction in isotropic solids. The normal deriva
tives necessary for implementation of the Green's function in boundary inte
gral equations are provided, and an example calculation of the Green's func
tion in a quartz-copper material system is presented.