S. Apte et V. Yang, Unsteady flow evolution in porous chamber with surface mass injection, part 1: Free oscillation, AIAA J, 39(8), 2001, pp. 1577-1586
Unsteady flow evolution in a porous chamber with surface mass injection sim
ulating a nozzleless rocket motor has been investigated numerically. The an
alysis is based on a large-eddy-simulation technique in which the spatially
filtered and Favre averaged conservation equations for large, energy-carry
ing turbulent structures are solved explicitly. The effect of the unresolve
d scales is modeled semi-empirically by considering adequate dissipation ra
tes for the energy present in the resolved scale motions. The flowfield is
basically governed by the balance between the inertia force and pressure gr
adient, as opposed to viscous effects and pressure gradient corresponding t
o channel flows without transpiration. It accelerates from zero at the head
end and becomes supersonic in the divergent section of the nozzle. Three s
uccessive regimes of development, laminar, transitional, and fully turbulen
t flow, are observed. Transition to turbulence occurs away from the porous
wall in the midsection of the motor, and the peak in the turbulence intensi
ty moves closer to the wall farther downstream as the local Reynolds number
increases. Increase in pseudoturbulence level at the injection surface cau
ses early transition to turbulence. As the flow develops farther downstream
, the velocity profile transits into the shape of a fully developed turbule
nt pipe flow with surface transpiration. The compressibility effect also pl
ays an important role, causing transition of the mean velocity profiles fro
m their incompressible flow counterparts as the local Mach number increases
. The flow evolution is characterized primarily by three nondimensional num
bers: injection Reynolds number, centerline Reynolds number, and momentum f
lux coefficient.