The generation of ultrasound by pulsed lasers is a thermoelastic proce
ss, and in the literature on general thermoelasticity there are presen
tly three different forms of the heat equation in popular use, the cla
ssical, Lord-Schulman (LS), and Green-Lindsay (GL) heat equations. The
question may thus arise as to which heat equation should be used to m
odel laser generated ultrasound. The purpose of this work is to summar
ize the current rationale for using these different heat equations, in
order to provide a basis for choosing one of the forms. A review of t
he classical, LS and GL theories is given, and the potential advantage
s of hyperbolic heat flow theories in laser ultrasonics are discussed.
A numerical example is given that clearly shows the small time differ
ences these theories predict, and also points out potential problems w
ith using hyperbolic heat equations on small time scales.