Rear-surface integral method for calculating thermal diffusivity from laser flash experiments

TL;DR

This paper introduces a new integral-based method for calculating thermal diffusivity from laser flash experiments, providing more accurate and less variable estimates than the standard half-rise time approach.

Contribution

The paper develops an exact integral formula for thermal diffusivity using rear-surface temperature data, improving accuracy over traditional methods.

Findings

New formula yields more accurate diffusivity estimates

Method reduces variability in measurements

Effective with synthetic experimental data

Abstract

The laser flash method for measuring thermal diffusivity of solids involves subjecting the front face of a small sample to a heat pulse of radiant energy and recording the resulting temperature rise on the opposite (rear) surface. For the adiabatic case, the widely-used standard approach estimates the thermal diffusivity from the rear-surface temperature rise history by calculating the half rise time: the time required for the temperature rise to reach one half of its maximum value. In this article, we develop a novel alternative approach by expressing the thermal diffusivity exactly in terms of the area enclosed by the rear-surface temperature rise curve and the steady-state temperature over time. Approximating this integral numerically leads to a simple formula for the thermal diffusivity involving the rear-surface temperature rise history. Using synthetic experimental data we demonstrate that the new formula produces estimates of the thermal diffusivity - for a typical test case - that are more accurate and less variable than the standard approach. The article concludes by briefly commenting on extension of the new method to account for heat losses from the sample.