Abstract
Unlike the shock reflection phenomena in pseudo-steady flows (chapter 2) and in steady flows (chapter 3), where the flow fields basically depend on two independent variables, namely; x/t and y/t in the former and x and y in the latter, here the flow field depends on three parameters x, y and t. For this reason, the analytical consideration of the reflection phenomenon in unsteady flows is much more difficult and as a matter of fact very limited progress has been made.
Keywords
Shock Wave Wedge Angle Incident Shock Wave Mach Stem Mach ReflectionList of Symbols
Latin Letters
- ai
local speed of sound in state (i)
- Aij
ai/aj
- Lm
length of the Mach stem in MR
- Lr
length of the reflected shock wave in TRR
- m3
flow mass in region (3) of a TRR
- Mi
flow Mach number in state (i)
- Mm
Mach stem Mach number
- Ms
incident shock wave Mach number
- R
radius of curvature of cylindrical wedges
- s
coordinate along the cylindrical wedge surface
- S
propagation distance of the corner-generated signals
- t
time
- ui
flow velocity in state (i) with respect to R in RR and TRR andTinMR
- Vi
flow velocity in state (i) in a laboratory frame of reference
- Vij
Vi/aj
- Vn
normal shock wave velocity of a TRR with respect to the reflection point R
- xtr
x coordinate of the MR→RR transition point
- XT
x coordinate of the triple point of an MR
- y
distance from Q to P in a TRR
- YT
y coordinate of the triple point of an MR
- z
distance from R to Q in a TRR
Greek Letters
- α
angle between the incident shock wave and the reflecting wedge surface in a TRR
- β
angle between the slipstream and the reflecting wedge surface in a TRR
- γ
specific heat capacities ratio
- Δt
time interval
- Δθw
change of the slope of the reflecting surface of a double wedge
- θ
angular position of a flow particle
- θT
angular position of the triple point
- θw
reflecting wedge angle
- θw1
wedge angle of the first surface of a double wedge
- θw2
wedge angle of the second surface of a double wedge
- θwinitial
wedge angle of a cylindrical concave or convex wedge
- θwtr
transition wedge angle
- θwMtr
transition wedge angle for shock wave Mach number M
- θw[A⇔B]
transition wedge angle from reflection A to reflection B
- ρi
flow density in state (i)
- Φi
angle of incidence between the flow and the oblique shock wave across which the flow enters state (i) with respect to R in RR and TRR and with respect to T in MR.
- χ
triple point trajectory angle
- χg
triple point trajectory angle at glancing incidence
- χtr
triple point trajectory angle at transition
Subscripts
- 0
flow state ahead of the incident shock wave, i
- 1
flow state behind the incident shock wave, i
- 2
flow state behind the reflected shock wave, r
- 3
flow state behind the Mach stem, m, of an MR or the normal shock wave, n, of a TRR
Preview
Unable to display preview. Download preview PDF.
Reference
- Bazhenova, T. V., Fokeev, V. P. & Gvozdeva, L. G., “Regions of Various Forms of Mach Reflection and Its Transition to Regular Reflection”, Acta Astro., Vol. 3, pp. 131–140, 1976.ADSCrossRefGoogle Scholar
- Ben-Dor, G., “Analytical Solution of a Double-Mach Reflection”, AIAA J., Vol. 18, pp. 1036–1043, 1980.MathSciNetADSMATHCrossRefGoogle Scholar
- Ben-Dor, G., Dewey, J.M., McMillin, D.J. & Takayama, K., “Experimental Investigation of the Asymptotically Approached Mach Reflection over the Second Surface in the Reflection over a Double Wedge”, Experiments in Fluids, Vol. 6, pp. 429–434, 1988.ADSCrossRefGoogle Scholar
- Ben-Dor, G., Dewey, J.M. & Takayama, K., “The Reflection of a Planar Shock Wave over a Double Wedge”, J. Fluid Mech., Vol. 176, pp. 483–520, 1987.ADSCrossRefGoogle Scholar
- Ben-Dor, G. & Takayama, K., “Analytical Prediction of the Transition from Mach to Regular Reflection over Cylindrical Concave Wedges”, J. Fluid Mech., Vol. 158, pp. 365–380, 1985.ADSCrossRefGoogle Scholar
- Ben-Dor, G. & Takayama, K., “Application of Steady Shock Polars to Unsteady Shock Wave Reflections”, AIAA J., Vol. 24, pp. 682–684, 1986.ADSCrossRefGoogle Scholar
- Ben-Dor, G. & Takayama, K., “The Dynamics of the Transition from Mach to Regular Reflection over Concave Cylinders”, Israel J. Tech., Vol. 23, pp. 71–74, 1986/7.Google Scholar
- Ben-Dor, G., Takayama, K. & Dewey, J.M., “Further Analytical Considerations of the Reflection of Weak Shock Waves over a Concave Wedge”, Fluid Dyn. Res., Vol. 2, pp. 77–85, 1987.ADSCrossRefGoogle Scholar
- Courant, R. & Friedrichs, K.O., Hypersonic Flow and Shock Waves, Wiley Interscience, New York, U.S.A., 1948.Google Scholar
- Dewey, J.M. & McMillin, D.J., “An Analysis of the Particle Trajectories in Spherical Blast Waves Reflected from Real and Ideal Surfaces”, Canadian J. Phys., Vol. 59, pp. 1380–1390, 1981.ADSCrossRefGoogle Scholar
- Dewey, J.M., McMillin, D.J. & Classen, D.F., “Photogrammetry of Spherical Shocks Reflected from Real and Ideal Surfaces”, J. Fluid Mech., Vol. 81, pp. 701–717, 1977.ADSCrossRefGoogle Scholar
- Ginzburg, I.P. & Markov, Y.S., “Experimental Investigation of the Reflection of a Shock Wave from a Two-Facet Wedge”, Fluid Mech.-Soviet Res., Vol. 4, pp. 167–172, 1975.Google Scholar
- Heilig, W.H., “Diffraction of Shock Wave by a Cylinder”, Phys. Fluids Supll. I., Vol. 12, pp. 154–157, 1969.ADSGoogle Scholar
- Henderson, L.F. & Lozzi, A., “Experiments on Transition of Mach Reflection”, J. Fluid Mech., Vol. 68, pp. 139–155, 1975.ADSCrossRefGoogle Scholar
- Hornung, H.G., Oertel, H. Jr. & Sandeman, R.J., “Transition to Mach Reflection of Shock Waves in Steady and Pseudo-Steady Flow with and without Relaxation”, J. Fluid Mech., Vol. 90, pp. 541–560, 1979.ADSCrossRefGoogle Scholar
- Hu, T.C.J. & Glass, I.I., “Blast Wave Reflection Trajectories from a Height of Burst”, AIAA J., Vol. 24, pp. 607–610, 1986.ADSCrossRefGoogle Scholar
- Itoh, S. & Raya, M., “On the Transition Between Regular and Mach Reflection” in “Shock Tubes and Waves”, Ed. A. Lifshitz and J. Rom, Magnes Press, Jerusalem, pp. 314–323, 1980.Google Scholar
- Itoh, S., Okazaki, N. & Itaya, M., “On the Transition Between Regular and Mach Reflection in Truly Non-Stationary Flows”, J. Fluid Mech., Vol. 108, pp. 383–400, 1981.ADSCrossRefGoogle Scholar
- Law, C.K. & Glass, I.I., “Diffraction of Strong Shock Waves by a Sharp Compressive Corner”, CASI Trans., Vol. 4, pp. 2–12, 1971.Google Scholar
- Marconi, F., “Shock Reflection Transition in Three-Dimensional Flow About Interfering Bodies”, AIAA J., Vol. 21, pp. 107–113, 1983.CrossRefGoogle Scholar
- Milton, B.E., “Mach Reflection Using Ray-Shock Theory”, AIAA J., Vol. 13, pp. 1531–1533, 1975.ADSCrossRefGoogle Scholar
- Reichenbach, H., “Roughness and Heated Layer Effects on Shock Wave Propagation and Reflection — Experimental Results”, Ernst Mach Institute Rep. E 24/85, Freiburg, West Germany, 1985.Google Scholar
- Srivastava, R.S. & Deschambault R.L., “Pressure Distribution Behind a Nonstationary Reflected-Diffracted Oblique Shock Wave”, AIAA J., Vol. 22, pp. 305–306, 1984.ADSCrossRefGoogle Scholar
- Takayama, K. & Ben-Dor, G., “A Reconsideration of the Transition Criterion from Mach to Regular Reflection over Cylindrical Concave Surfaces”, KSME J., Vol. 3, pp. 6–9, 1989.Google Scholar
- Takayama, K., Ben-Dor, G. & Gotoh, J., “Regular to Mach Reflection Transition in Truly Nonstationary Flows — Influence of Surface Roughness”, AIAA J., Vol. 19, pp. 1238–1240, 1981.ADSCrossRefGoogle Scholar
- Takayama, K. & Sasaki, M., “Effects of Radius of Curvature and Initial Angle on the Shock Transition over Concave and Convex Walls”, Rep. Inst. High Speed Mech., Tohoku Univ., Sendai, Japan, Vol. 46, pp. 1–30, 1983.Google Scholar
- Takayama, K. & Sekiguchi, H., “Triple-Point Trajectory of Strong Spherical Shock Wave”, AIAA J., Vol. 19, pp. 815–817, 1981a.ADSCrossRefGoogle Scholar
- Takayama, K. & Sekiguchi, H., “Formation and Diffraction of Spherical Shock Waves in Shock Tube”, Rep. Inst. High Speed Mech., Tohoku Univ., Sendai, Japan, Vol. 43, pp. 89–119, 1981b.Google Scholar
- Whitham, G.B., “A New Approach to Problems of Shock Dynamics. Part 1. Two Dimensional Problems”, J. Fluid Mech., Vol. 2, pp. 145–171, 1957.MathSciNetADSMATHCrossRefGoogle Scholar