We present a study of the classical limit of nonradiative electronic relaxa
tion in condensed phase systems. The discrete Hamiltonian representing an i
mpurity in a condensed phase environment is mapped onto a continuous form u
sing the Meyer-Miller approach. The classical electronic relaxation rate is
obtained within the framework of the reactive flux formalism and is compar
ed to the fully quantum mechanical result, and to a mixed quantum-classical
approximation. Similar to the case of vibrational relaxation, we find that
the fully classical treatment is closer to the fully quantum mechanical ra
te than the mixed quantum-classical treatment. We provide a time domain ana
lysis of the results.