The time dependence of photoacoustic waves generated by irradiation of
fluid bodies with optical radiation can be found by solution of the w
ave equation for pressure. Consider the generation of ultrasonic waves
where heat deposition is described by a spatial heating function time
s a delta function in time. Solution of the wave equation in one dimen
sion, shows that the spatial deposition of heat is directly mapped int
o the time profile of the photoacoustic wave. In two dimensions, a cyl
indrically symmetric deposition of heat gives a photoacoustic wave des
cribed by an integral over a spatial source function. In three dimensi
ons, a spherically symmetric deposition of heat gives the photoacousti
c wave as a mapping of the product of the retarded time with the spati
al heating function. For laser pulses long compared with the transit t
ime of sound across the irradiated body, the photoacoustic wave-form i
s found to be proportional to the zero'th time derivative (the time pr
ofile) of the laser pulse in one dimension, the (1/2)'th time derivati
ve of the laser pulse in two dimensions and the first time derivative
of the laser pulse in three dimensions. Formulae for multipole radiati
on in one, two, and three dimensions are derived from the wave equatio
n for sources having arbitrary spatial dependencies.