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Numerical Model of a PDRE
Michael Hoyt
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The Pulse Detonation Rocket Engine
What is it? Rocket engine where the combustion process involves a detonation wave Uses shock wave to generate high pressures
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Purpose Attempting to simulate a single pulse detonation wave
Based upon the process set by C. I. Morris who emphasize the importance of nozzle selection for the PDRE Also compared with steady state rocket engine in terms of performance
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System Model Constant volume reactor governs the timestep
Plug flow reactor governs the spacestep
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Governing Equations Stoichiometric reaction of kerosene in oxygen
Model the products as a whole instead of carbon dioxide and water
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Governing Equations Quasi 1-D Euler equations
Assumes adiabatic, no viscosity, ideal conditions
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Governing Equations
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Other Equations
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Chemistry Model Assume global chemistry model
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Numerical Model Solved in split form
Timestep splitting approach by Strang[2].
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Numerical Model Uses ghost cells as the means to evaluate the conditions in each timestep and spacestep Similar to the finite elements on a solid model Allows for proper boundary conditions to be applied
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Initial and Boundary conditions
Initial conditions Basic state initial conditions, nothing all that special Example T(x,0) = T0 Boundary conditions Reflective boundary conditions to simulate walls Method of characteristics to model exit flow boundary conditions, determined by interior flow
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Expected Results Mach number contour plot (space-time diagram)[1]
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Quick Comparison Taken from Morris[1].
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References [1]Morris, C. I., “Numerical Modeling of Single-Pulse Gasdynamics and Performance of Pulse Detonation Rocket Engines,” Journal of Propulsion and Power, Vol. 21, No. 3, 2005, pp [2]Strang, G., “On the Construction and Comparison of Difference Schemes,” SIAM Journal on Numerical Analysis, Vol. 5, No. 3, 1968, pp
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