2008
DOI: 10.1016/j.ijheatmasstransfer.2007.11.021
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Thermal and chemical kinetic characterization of multiphase and multicomponent substances by laser heating

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Cited by 17 publications
(58 citation statements)
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“…The system was originally designed to limit effects of a nonuniform temperature distribution in the middle of the sphere. The uniformity in temperature of heating a sample placed within the center of the sphere (for a volume with dimensions of about 10 mm diameter by 5 mm height) is of the order of 1 K. 28 Within the sample, heat transfer is by conduction. The lumped-capacitance approximation 30 is invoked, in which the sample is spatially uniform in temperature at any instant of time during the transient process, as long as the Biot number < 0.1, which is satisfied to be for this investigation.…”
Section: Methodsmentioning
confidence: 99%
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“…The system was originally designed to limit effects of a nonuniform temperature distribution in the middle of the sphere. The uniformity in temperature of heating a sample placed within the center of the sphere (for a volume with dimensions of about 10 mm diameter by 5 mm height) is of the order of 1 K. 28 Within the sample, heat transfer is by conduction. The lumped-capacitance approximation 30 is invoked, in which the sample is spatially uniform in temperature at any instant of time during the transient process, as long as the Biot number < 0.1, which is satisfied to be for this investigation.…”
Section: Methodsmentioning
confidence: 99%
“…The mode of thermal analysis for these experiments is based on heating the reactor to a steady-state temperature (referred to as the 'heating-rate' approach). 28 Experiments were initially carried out for the 'baseline thermogram' (i.e., sample and reactor temperature measurements with respect to time including the pan substrate and no sample), and then repeated with the sample ('sample thermogram'). From these thermograms, we also define the 'sample-baseline temperature difference' profiles (i.e., subtracting the sample thermogram and that of the baseline for either the sample or reactor temperatures), and the 'sample' or 'reactor' derivative profiles (i.e., variation of the sample or reactor temperature-time derivative with time or sample/reactor temperature for either the sample or baseline thermograms).…”
Section: Methodsmentioning
confidence: 99%
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“…To fabricate a graphene-based sensing device, the surface graphene can be ablated at the same low threshold fluence via a laser patterning route by using a multiple pass in-motion technique. This study used a long-pulse UV nanosecond laser (1 > ns), because even laser ablation at a low energy fluence may induce thermal effects (plasma heating) [33,34]. Because the laser energy in this study was absorbed by the graphene surface ( Fig.…”
Section: Laser-ablated Multiyear Graphene Characterizationmentioning
confidence: 99%