Be. Milton et K. Takayama, CONICAL MACH REFLECTION OF MOVING SHOCK-WAVES - PART 2 - PHYSICAL ANDCFD EXPERIMENTATION, Shock waves, 8(2), 1998, pp. 93-103
Analytical consideration of Mach reflections over cones using the ray-
shock theory showed that they differ from those of the two-dimensional
Mach reflection over wedges. Conical configurations include both self
-similar and non-self-similar cases. However, even when self-similar,
the conical configurations exhibit triple-point locus trajectory angle
s with values which, for any given reflection angle, differ from those
of self-similar, wedge cases. Additionally, within the range of possi
ble conical configurations, different values of self-similar triple-po
int locus angles exist for any given reflection angle depending on the
geometry of the particular reflection process. While the ray-shock th
eory, as discussed in a previous paper on this research. provides a us
eful guide and a means of readily identifying these variations, verifi
cation using both shock tube and numerical simulations is required and
is now available. Results of experimentation for both self-similar an
d non-self-similar axisymmetric cases using these techniques are repor
ted here and comparisons are made with the previous analysis. These su
pport the calculations of the ray-shock theory over much of the reflec
tion angle, Mach number range as well as highlighting some limitations
of the theory.