2002
DOI: 10.1023/a:1015446919301
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Cited by 6 publications
(4 citation statements)
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“…5b–d) presumably because of cavitation produced by the laser pulse in the liquid. 16 Because the bubble generated by a single laser pulse collapses after a period of hundreds of microseconds, 17 semi-adiabatic compression occurs during bubble collapse, resulting in a hot spot with a temperature of the order of 10 000 K. At the end of this period, the bubble can emit a short pulse of light for a picosecond–nanosecond duration, which is known as sonoluminescence. 18,19 This phenomenon typically has broad spectral emission, which can be attributed to ion-electron recombination occurring at the high temperature of the compressed bubbles.…”
Section: Resultsmentioning
confidence: 99%
“…5b–d) presumably because of cavitation produced by the laser pulse in the liquid. 16 Because the bubble generated by a single laser pulse collapses after a period of hundreds of microseconds, 17 semi-adiabatic compression occurs during bubble collapse, resulting in a hot spot with a temperature of the order of 10 000 K. At the end of this period, the bubble can emit a short pulse of light for a picosecond–nanosecond duration, which is known as sonoluminescence. 18,19 This phenomenon typically has broad spectral emission, which can be attributed to ion-electron recombination occurring at the high temperature of the compressed bubbles.…”
Section: Resultsmentioning
confidence: 99%
“…In a previous study of hydrogen-bonding systems the activation energy, E b , in eq 23 was attributed to the energy barrier that molecules have to take when detaching and rejoining clusters of hydrogen-bonded molecules. 79 Furthermore, in a SAFT study of Tong et al, 80 the activation energy was assumed to be related to the bonded fraction (1 -X A ), i.e.,…”
Section: Resultsmentioning
confidence: 99%
“…The kinetic gas theory allows the derivation of a model for the self-diffusion coefficients of gases at infinite dilution. For low-density gases, the Chapman–Enskog equation satisfactorily describes the self-diffusion coefficients; however, for high-density and nonspherical chain fluids, this equation requires modification by combining other theories, such as the contrasting volume model, rough hard sphere model, and free-volume model, or by choosing the potential energy model and introducing correction terms, such as the hard sphere chain model and Lennard-Jones chain model . The universal coefficients of the correction terms can be obtained by fitting data from molecular dynamics simulations, , and the parameters of the structural properties can be obtained by fitting the experimental data of the self-diffusion coefficients.…”
Section: Introductionmentioning
confidence: 99%