# Rear-surface integral method for calculating thermal diffusivity: finite pulse time correction and two-layer samples

## TL;DR

This paper extends the rear-surface integral method for calculating thermal diffusivity from laser flash experiments, incorporating realistic heat pulse shapes and two-layer samples, resulting in more accurate and applicable formulas.

## Contribution

It introduces new formulas for thermal diffusivity calculation that account for finite pulse shapes and layered samples, improving upon previous assumptions.

## Key findings

- New formulas accurately estimate thermal diffusivity from realistic pulse shapes.
- Method effectively handles two-layer heterogeneous samples.
- Numerical experiments validate the improved accuracy of the formulas.

## Abstract

We study methods for calculating the thermal diffusivity of solids from laser flash experiments. This experiment involves subjecting the front surface of a small sample of the material to a heat pulse and recording the resulting temperature rise on the opposite (rear) surface. Recently, a method was developed for calculating the thermal diffusivity from the rear-surface temperature rise, which was shown to produce improved estimates compared with the commonly used half-time approach. This so-called rear-surface integral method produced a formula for calculating the thermal diffusivity of homogeneous samples under the assumption that the heat pulse is instantaneously absorbed uniformly into a thin layer at the front surface. In this paper, we show how the rear-surface integral method can be applied to a more physically realistic heat flow model involving the actual heat pulse shape from the laser flash experiment. New thermal diffusivity formulas are derived for handling arbitrary pulse shapes for either a homogeneous sample or a heterogeneous sample comprising two layers of different materials. Presented numerical experiments confirm the accuracy of the new formulas and demonstrate how they can be applied to the kinds of experimental data arising from the laser flash experiment.