  We investigate the kinetics of constant-kernel aggregation which is augmented
by either: (a) evaporation of monomers from finite-mass clusters, or (b)
continuous cluster growth -- \ie, condensation. The rate equations for these
two processes are analyzed using both exact and asymptotic methods. In
aggregation-evaporation, if the evaporation is mass conserving, \ie, the
monomers which evaporate remain in the system and continue to be reactive, the
competition between evaporation and aggregation leads to several asymptotic
outcomes. For weak evaporation, the kinetics is similar to that of aggregation
with no evaporation, while equilibrium is quickly reached in the opposite case.
At a critical evaporation rate, the cluster mass distribution decays as
$k^{-5/2}$, where $k$ is the mass, while the typical cluster mass grows with
time as $t^{2/3}$. In aggregation-condensation, we consider the process with a
growth rate for clusters of mass $k$, $L_k$, which is: (i) independent of $k$,
(ii) proportional to $k$, and (iii) proportional to $k^\mu$, with $0<\mu<1$. In
the first case, the mass distribution attains a conventional scaling form, but
with the typical cluster mass growing as $t\ln t$. When $L_k\propto k$, the
typical mass grows exponentially in time, while the mass distribution again
scales. In the intermediate case of $L_k\propto k^\mu$, scaling generally
applies, with the typical mass growing as $t^{1/(1-\mu)}$. We also give an
exact solution for the linear growth model, $L_k\propto k$, in one dimension.
