Time-distance helioseismology measures the time for acoustic wave packets t
o travel, through the solar interior, from one location on the solar surfac
e to another. Interpretation of travel times requires an understanding of t
heir dependence on subsurface inhomogeneities. Traditionally, time-distance
measurements have been modeled in the ray approximation. Recent efforts ha
ve focused on the Born approximation, which includes finite-wavelength effe
cts. In order to understand the limitations and ranges of validity of the r
ay and Born approximations, we apply them to a simple problem-adiabatic aco
ustic waves in a uniform medium with a spherical inclusion-for which a nume
rical solution to the wave equation is computationally feasible. We show th
at, for perturbations with length scales large compared to the size of the
first Fresnel zone, both the Born and first-order ray approximations yield
the same result and that the fractional error in the travel time shift, com
puted by either approximation, is proportional to the fractional strength o
f the sound speed perturbation. Furthermore, we demonstrate that for pertur
bations with length scales smaller than the first Fresnel zone the ray appr
oximation can substantially overestimate travel time perturbations while th
e Born approximation gives the correct order of magnitude. The main cause o
f the inaccuracy of the Born approximation travel times is the appearance o
f a diffracted wave. This wave, however, has not yet been observed in the s
olar data.