Calculations of models for the dust shell of Nova Aql 1993 show that t
he period of its isothermal expansion, i.e., the period during which t
he shape of the energy distribution in its spectrum remains unchanged,
is related to perceptible destruction of dust particles. In order for
the computed light curves to coincide with the observed ones, the des
truction of grains must be complex in nature, incorporating their frag
mentation, in which the total mass of the dust shell is preserved, and
destruction as a result of bombardment of their surface by particles
of the gaseous phase (sputtering), in which the grain size, i.e., thei
r total mass, decreases, but their total number is preserved. It seems
quite reasonable to suppose that both these processes proceed simulta
neously in clumpy nova shells with a large scatter of internal velocit
ies. Within similar to 110 days after the condensation, the originally
optically thick (tau(v) similar or equal to 2.5) dust shell of Nova A
ql 1993 becomes essentially transparent (tau(v) similar or equal to 0.
04). By this time, the destruction of grains had led to a similar to 2
5-fold increase in their number and similar to 7-fold decrease in thei
r total mass. The grain size is reduced by a factor less than or equal
to 6. It is noted that during the expansion of an optically thick dus
t shell, the partial stabilization of its color properties may be caus
ed by optical effects arising from a decrease in its opacity, with the
grain temperature at its inner boundary actually decreasing.