Effect of Pressure on Soot Morphology in Laminar Diffusion Flames PDF Download
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Author: Ben Gigone
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Languages : en
Pages : 0
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The effect of pressure on soot aggregate morphology in laminar diffusion flames, specifically pertaining to primary soot particle size and soot aggregate fractal parameters, was investigated in methane-air and nitrogen-diluted ethylene flames. Soot aggregate samples were collected by thermophoretic sampling within a high-pressure combusting chamber. Soot samples were imaged via transmission electron microscopy followed by an automated imaging detection method. The experiments covered pressures from 7 to 30 bar at vertical flame heights of 3, 6, and 8 mm in methane-air flames, and 3 to 6 bar at heights of 2, 5, 10, and 15 mm in nitrogen-diluted ethylene flames. It was observed that mean primary soot particle size increased with increasing pressure for both fuel types at virtually all flame locations. The fractal dimension was found to vary with pressure for both fuel cases, suggesting that a universal soot aggregate fractal value may not be justified in high-pressure flames.
Author: Ben Gigone
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ISBN:
Category :
Languages : en
Pages : 0
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Book Description
The effect of pressure on soot aggregate morphology in laminar diffusion flames, specifically pertaining to primary soot particle size and soot aggregate fractal parameters, was investigated in methane-air and nitrogen-diluted ethylene flames. Soot aggregate samples were collected by thermophoretic sampling within a high-pressure combusting chamber. Soot samples were imaged via transmission electron microscopy followed by an automated imaging detection method. The experiments covered pressures from 7 to 30 bar at vertical flame heights of 3, 6, and 8 mm in methane-air flames, and 3 to 6 bar at heights of 2, 5, 10, and 15 mm in nitrogen-diluted ethylene flames. It was observed that mean primary soot particle size increased with increasing pressure for both fuel types at virtually all flame locations. The fractal dimension was found to vary with pressure for both fuel cases, suggesting that a universal soot aggregate fractal value may not be justified in high-pressure flames.
Author: Adel Maurice Iskander
Publisher:
ISBN:
Category : Flame
Languages : en
Pages : 440
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Author: L. L. McCrain
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Category :
Languages : en
Pages :
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Author: Chul Han Kim
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Category :
Languages : en
Pages : 408
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Author: Robert J. Santoro
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Category :
Languages : en
Pages : 67
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Studies emphasizing the effects of fuel concentration and operating pressure on the formation of soot particles have been conducted in a series of laminar diffusion flames. These experiments have shown that fuel concentration has a measurable effect on the amount of soot formed in the flame. However, a simple, constant proportionality between the fuel concentration and soot volume fraction has not been found to apply for the range of flow conditions studied. This observation is believed to be a result of flame residence time and diffusion effects which mitigate the consequences of reduced initial fuel concentration. Comparisons with simple laminar diffusion flame models are currently being used to investigate the relationship between initial fuel concentration and local flame concentration fields. Similar studies of soot formation in laminar diffusion flames as a function of operating pressure have also been completed for ethene, ethane and propene fuel species. Keywords: Soot formation, Soot particles, Diffusion flames. (JES).
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Languages : en
Pages :
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Soot volume fraction (f[subscript sv]) is measured quantitatively in a laminar diffusion flame at elevated pressures up to 25 atmospheres as a function of fuel type in order to gain a better understanding of the effects of pressure on the soot formation process. Methane and ethylene are used as fuels; methane is chosen since it is the simplest hydrocarbon while ethylene represents a larger hydrocarbon with a higher propensity to soot. Soot continues to be of interest because it is a sensitive indicator of the interactions between combustion chemistry and fluid mechanics and a known pollutant. To examine the effects of increased pressure on soot formation, Laser Induced Incandescence (LII) is used to obtain the desired temporally and spatially resolved, instantaneous f[subscript sv] measurements as the pressure is incrementally increased up to 25 atmospheres. The effects of pressure on the physical characteristics of the flame are also observed. A laser light extinction method that accounts for signal trapping and laser attenuation is used for calibration that results in quantitative results. The local peak f[subscript sv] is found to scale with pressure as p[superscript 1.2] for methane and p[superscript 1.7] for ethylene.
Author: Laura Lynne McCrain
Publisher:
ISBN:
Category :
Languages : en
Pages : 69
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Keywords: diffusion flame, high pressure, soot formation.
Author: Guozheng Lin
Publisher:
ISBN:
Category : Flame
Languages : en
Pages : 568
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![Soot Formation in Propane-air Laminar Diffusion Flames at Elevated Pressures [microform] PDF](https://books.google.com/books/content/images/frontcover/j8uMtgAACAAJ?fife=w80-h100)
Author: Decio S. (Decio Santos) Bento
Publisher: Library and Archives Canada = Bibliothèque et Archives Canada
ISBN: 9780494024430
Category : Combustion
Languages : en
Pages : 158
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Laminar axisymmetric propane air diffusion flames were studied at pressures 0.1 to 0.725 MPa (1 to 7.25 atm). To investigate the effect of pressure on soot formation, radially resolved soot temperatures and soot volume fractions were deduced from soot radiation emission scans collected at various pressures using spectral soot emission (SSE). Overall flame stability was quite good as judged by the naked eye. Flame heights varied by 15% and flame axial diameters decreased by 30% over the entire pressure range.Analysis of temperature sensitivity to variations in E lambda(m) revealed that a change in E lambda(m) of +/-20% produced a change in local temperature values of about 75 to 100 K or about 5%.Temperatures decreased and soot concentration increased with increased pressure. More specifically, the peak soot volume fraction showed a power law dependence, fv ∝ Pn where n = 2.0 over the entire pressure range. The maximum integrated soot volume fraction also showed a power law relationship with pressure, f ̄v ∝ Pn where n = 3.4 for 1 ≤ P ≤ 2 atm and n = 1.4 for 2 ≤ P ≤ 7.25 atm. The percentage of fuel carbon converted to soot increased with pressure at a rate, etas ∝ Pn where n = 3.3 and n = 1.1 for 1 ≤ P ≤ 2 atm and 2 ≤ P ≤ 7.25 atm respectively.
Author: Marc Robert Joseph Charest
Publisher:
ISBN: 9780494777626
Category :
Languages : en
Pages :
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