The diffusion rate in polycrystals is higher than in single crystals due to
the fact that diffusion in solids is known to occur along grain boundaries
and over free surfaces more rapidly than through the lattice. The diffusio
n mechanism in a polycrystalline medium has been discussed and analyzed ext
ensively since Fisher first studied this subject in 1951, by assuming high
diffusivity along the grain boundaries [1-5]. Most of the experimental data
was produced by thin layers and free surface bars with a finite source of
the element to be diffused. Whipple modified the Fisher model and Levine-Ma
cCallum based their theories upon the constant source in which the concentr
ation did not change during the diffusion time [3-4]. Since the experimenta
l sources usually consist of a finite amount, the validity of the models is
confined to the low temperature range where the diffusion is slow such tha
t the source is practically invariant.
The suggested technique adopts the instantaneous source model developed by
Suzuoka [2]. In addition, the concentration of the source at the medium sur
face does not change during the diffusion time, due to the sample design ha
ving a constant source.