Behaviour of laser induced incandescence signal with long laser pulse duration and high fluence

TL;DR

This study investigates unexpected secondary peaks in Laser Induced Incandescence signals when using long laser pulses, highlighting a phenomenon that could impact soot measurement techniques and sensor development.

Contribution

It reports the observation of a secondary peak in LII signals with long laser pulses and discusses potential physical or experimental origins of this phenomenon.

Findings

Secondary peak observed at fluences around 1.1 J/cm2

Phenomenon independent of pulse duration

Potential link to particle creation during high fluence

Abstract

Laser Induced Incandescence (LII) is an experimental technique that has been extensively used for in-flame measurement of soot properties. The traditional laser used for LII has been Nd:YAG laser with 5-10 ns pulse durations. The present study investigates an unexpected LII signal behaviour in the form of a secondary peak observed when using long laser pulse duration in the range of hundreds of ns. Temporal LII signals at varying fluences (up to 4.5 J/cm2) and pulse durations are presented and discussed. Although an explanation based on theoretical grounds has not been found, the study shows that the phenomenon is independent of pulse duration and that its appearance correlates with laser fluences of approximately 1.1 J/cm2. Artificial signal generated by the experimental procedures cannot be excluded, but if so could not be identified. One suggestion is an amplified effect of the phenomenon observed in the literature where new particles were created from the molecular cloud during high laser fluence LII. Since LII using long pulse durations are not widely used, but present a true potential in relation to sensor technology, this unexpected LII behaviour, either physically linked to the laser-soot interaction or induced by experimental flaw, should be further watched and understood.