Collisons and close encounters between two massive (1 less than or sim
ilar M/M. less than or similar 100) main-sequence stars have been stud
ied using smooth-particle hydrodynamics (SPH). The stars are represent
ed by Eddington standard models, which have the density profile of a p
olytrope with n = 3 but mass-dependent binding energy and adiabatic in
dex 4/3 < GAMMA1 < 5/3. The equation of state is that of an ideal gas
plus thermal radiation. We have performed a large number of calculatio
ns to obtain extensive coverage of the parameter space. In particular,
the stellar masses, relative velocity, and collision impact parameter
are all varied over wide ranges, representative of the conditions enc
ountered in dense stellar systems such as galactic nuclei. We give app
roximate scaling relations and fitting formulae for the amount of mass
loss and for the critical impact parameters for capture or merging. T
he more massive stars, which have smaller ratios of specific binding e
nergy to the square of escape velocity, are more easily disrupted in c
ollisions. In the limit of small relative velocity, our results for th
e tidal capture radius agree closely with those of linear perturbation
theory, although some nonlinear effects are always apparent. As the r
elative velocity increases, the orbital energy of the colliding stars
can only be dissipated by shock heating, and the critical capture radi
us decreases much faster than predicted by linear theory. We also calc
ulate cross sections and rates of stellar capture, merging, and mass l
oss in a dense star cluster. We find that the average fractional mass
loss per collision in a cluster does not depend sensitively on the ste
llar velocity dispersion. Even when the velocity dispersion is as larg
e as several times the typical escape velocity from a star, collisions
are not very disruptive on the average, with only a few percent of th
e mass liberated per collision. Our results should be useful for futur
e dynamical studies of dense stellar systems incorporating the effects
of stellar collisions and close dissipative encounters.