A comparison is undertaken of theories for the gravity wave induced fl
uctuations in the intensity of airglow emissions and the associated te
mperature of the source region. The comparison is made in terms of Kra
ssovsky's ratio eta(E) for a vertically extended emission region (eta(
E)) is the ratio of the vertically integrated normalized intensity per
turbation to the vertically integrated normalized intensity-weighted t
emperature perturbation). It is shown that the formulas for eta(E) in
the works by Tarasick and Hines (1990) and Schubert et al. (1991) are
in agreement for the case of an inviscid atmosphere. The calculation o
f eta(E) using the theory of Tarasick and Hines (1990) requires determ
ination of their function chi; we show that chi is simply related to t
he ''single-level'' Krassovsky's ratio eta of Schubert et al. (1991).
The general relationship between chi and eta is applied to a simple ch
emical-dynamical model of the O2 atmospheric airglow and the altitude
dependence of these quantities is evaluated for nonsteady state chemis
try. Though the Tarasick and Hines (1990) formula for eta(E) does not
explicitly depend on the scale heights of the minor constituents invol
ved in airglow chemistry, eta(E) implicitly depends upon these scale h
eights through its dependences on chemical production and loss contain
ed in chi. We demonstrate this dependence of eta(E) for the OH nightgl
ow on atomic oxygen scale height by direct numerical evaluation of eta
(E); in this case the dependence originates in the chemical production
of perturbed ozone.