2010
DOI: 10.2514/1.42368
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Modeling, Simulation, and Controller Design for an Air-breathing Combustion System

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Cited by 25 publications
(16 citation statements)
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“…(15) and the one feasible solution from the quadratic equation can be used as the equivalence ratio command. Here, the fuel supply actuation by this command is assumed to be the 1 st order dynamics, with a cutoff frequency of approximately 0.8 Hz [13], which is equivalent to a time constant of 0.2 sec, and it is realized by a transfer function.…”
Section: (16)mentioning
confidence: 99%
“…(15) and the one feasible solution from the quadratic equation can be used as the equivalence ratio command. Here, the fuel supply actuation by this command is assumed to be the 1 st order dynamics, with a cutoff frequency of approximately 0.8 Hz [13], which is equivalent to a time constant of 0.2 sec, and it is realized by a transfer function.…”
Section: (16)mentioning
confidence: 99%
“…A change in the nozzle throat area takes a small but finite time to influence the combustor pressure, as modeled by the B parameter in [14,15]. Then the upstream propagating pressure wave from the combustor affects the intake shock position, which then generates a new total pressure at node 3 behind the terminal shock.…”
Section: Terminal Shock Dynamic Modelmentioning
confidence: 99%
“…A model that couples the intake with the combustor and exhaust nozzle for a ramjet was first realized recently by our coworkers [14], and it was used [15] to derive a control law for the intake shock location using the nozzle throat area as input. A significant feature of the model in [14] was the use of time lags to capture the physics of upstream and downstream propagating waves between the intake and combustor.…”
Section: Introductionmentioning
confidence: 99%
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