1998
DOI: 10.2514/2.5278
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Comparison of Physical and Aerodynamic Ramps as Fuel Injectors in Supersonic Flow

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Cited by 121 publications
(39 citation statements)
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“…The aerothermodynamic probing method and data reduction algorithm employed during this research were similar to those used by Fuller et al (1998). They reported estimated uncertainties (within a 95% confidence interval) of the reduced data values as ∆M = ±1.7%, ∆P t = ±2.8%, ∆P = ±2.8%, ∆ρ = ±3.0%, ∆u = ±1.3%, and ∆T = ±0.8%.…”
Section: Appendix Bmentioning
confidence: 76%
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“…The aerothermodynamic probing method and data reduction algorithm employed during this research were similar to those used by Fuller et al (1998). They reported estimated uncertainties (within a 95% confidence interval) of the reduced data values as ∆M = ±1.7%, ∆P t = ±2.8%, ∆P = ±2.8%, ∆ρ = ±3.0%, ∆u = ±1.3%, and ∆T = ±0.8%.…”
Section: Appendix Bmentioning
confidence: 76%
“…They reported estimated uncertainties (within a 95% confidence interval) of the reduced data values as ∆M = ±1.7%, ∆P t = ±2.8%, ∆P = ±2.8%, ∆ρ = ±3.0%, ∆u = ±1.3%, and ∆T = ±0.8%. Fuller et al (1998) accounted for the mixture fractions of a binary gas in their data reduction, whereas this research assumed the flow the probes were exposed to consisted mostly of air alone. The uncertainties for the reduced quantities for this research may actually be lower, but the values used by Fuller et al (1998) provide an established, and possibly conservative, estimation of error.…”
Section: Appendix Bmentioning
confidence: 99%
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“…Various fuelinjection techniques, from different arrangements and shapes of flush-wall injectors to in-stream injection concepts (e.g., ramps, struts, etc. ), have been explored in an attempt to enhance the fuel-air mixing rate [1][2][3][4][5][6][7][8][9][10]. In general, the larger the disruption a fuel injector generates in the supersonic flow, the more effective the mixing of fuel and air.…”
Section: Nomenclaturementioning
confidence: 99%
“…A two-axis computer-controlled traversing mechanism allowed the probes to be positioned in the spatial region bounded by 8 < z=d < 8 and 0 < y=d < 9. These data were used in conjunction with the Raman-scattering data and a computerized solution algorithm developed by Fuller et al [5] to determine the time-averaged aerothermodynamic properties of the flowfield. Fuller et al also conducted an uncertainty analysis for the probe-based measurements; the results of this analysis are reproduced here: the uncertainties in stagnation pressure, Mach number, density, static pressure, static temperature, and velocity were determined to be 2.8, 1.7, 3.0, 2.8, 0.8, and 1.3% of the local values, respectively.…”
Section: In-stream Probingmentioning
confidence: 99%