A uniqueness theorem is proved for two theories of thermoelasticity capable
of admitting finite speed thermal waves, the theories having been proposed
by Green & Naghdi. Uniqueness is proved under the weak assumption of requi
ring only major symmetry of the elasticity tensor; no definiteness whatsoev
er is postulated. It is shows how to demonstrate uniqueness by a Lagrange i
dentity method and also by producing a novel functional to which to apply t
he technique of logarithmic convexity. It is remarked on how to extend the
result to an unbounded spatial domain without requiring decay restrictions
on the solution at infinity. Finally, conditions are derived which show hop
i a suitable measure of the solution will grow at least exponentially in ti
me if the initial 'energy' satisfies appropriate conditions. This complemen
ts the fundamental work of Knops & Payne, who produced corresponding growth
results in the isothermal elasticity case.