The energetics of cavity formation in proteins is evaluated with two d
ifferent approaches and results are analyzed and compared to experimen
tal data. In the first approach, free energy of cavity formation is ex
tracted by RMS fitting from the distribution of numbers of cavities, N
, with different volumes, V-cav, in 80 high-resolution protein structu
res. It is assumed that the distribution of number of cavities accordi
ng to their volume follows the Boltzmann law, N(V-cav)=exp[(-a.V-cav-b
)/kT], or its simplified form. Specific energy cost of cavity formatio
n, a, extracted by RMS fitting from these distributions is compared to
a values extracted from experimental free energies of cavity formatio
n in T4 lysozyme fitted to similar expressions. It is found that fitti
ng of both sets of data leads to similar magnitudes and uncertainties
in the calculated foe energy values. It is shown that Boltzmann-like d
istribution of cavities can be derived for a simple model of an equili
brium interconversion between mutants in an extracellular system. We,
however, suggest that a partitioning into cavity-dependent and cavity-
independent terms may lose meaning when one attempts to describe mutat
ion effects on protein stability in terms of specific free energy cont
ributions. As an alternative approach, a direct molecular mechanics ev
aluation is attempted of T4 lysozyme destabilization by five single ca
vity-creating mutations. The calculations are based on the approach us
ed in calculations of the energetics of packing defects in crystals. F
or all mutations calculated destabilizations agree with the correspond
ing experimental values within +/-0.6 kcal/mol. A computational relaxa
tion of the mutant was most difficult to achieve for the mutation prod
ucing the smallest cavity. However, calculations do not always reprodu
ce crystallographically observed contraction/expansion of cavities. It
is suggested that this may be related to usually observed large RMS d
ifferences (>1 Angstrom) between crystallographic and energy-minimized
protein structures, and thus correct energetics might be easier to ca
lculate than the correct geometry.