2007
DOI: 10.1080/00102200701386198
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Effects of Entry Conditions on Cracked Kerosene-Fueled Supersonic Combustor Performance

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Cited by 17 publications
(3 citation statements)
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“…In this study, the fuel temperature can vary from 300 to 800 K as a result of convective heat transfer. Although a further increase in fuel temperature is possible, it was not attempted here because significant thermal cracking was noted [21] to occur at fuel temperatures higher than 800 K. In addition, the Reynolds number of the fuel flow, defined by the tube inner diameter and fuel local properties, ranged from 3000 to 500,000 in the present investigation, whereas the wall heat flux was in the range of 1-30 W=cm 2 .…”
Section: Experimental Specifications a Experimental Facilitymentioning
confidence: 79%
“…In this study, the fuel temperature can vary from 300 to 800 K as a result of convective heat transfer. Although a further increase in fuel temperature is possible, it was not attempted here because significant thermal cracking was noted [21] to occur at fuel temperatures higher than 800 K. In addition, the Reynolds number of the fuel flow, defined by the tube inner diameter and fuel local properties, ranged from 3000 to 500,000 in the present investigation, whereas the wall heat flux was in the range of 1-30 W=cm 2 .…”
Section: Experimental Specifications a Experimental Facilitymentioning
confidence: 79%
“…Buoyancy is excluded in order to investigate the basic characteristics of convective heat transfer of the kerosene at supercritical pressure. Since the thermal cracking of the China RP-3 aviation kerosene occurs obviously when the temperature is over 850 K [15], the maximum wall temperature is restricted to below 850 K in this study.…”
Section: Boundary Conditionsmentioning
confidence: 99%
“…The heating system has been used for our previous studies [10,11,13,14] . For the present study, the fuel pressure was in the range of 3.5-4.5 MPa, higher than the critical pressure (~2.4 MPa) of the kerosene and the fuel temperature varied from 700 to 1050 K. The fuel residence time was estimated as approximately 0.5-1.3 s, depending on operation conditions.…”
Section: Introductionmentioning
confidence: 99%