Solutions 243
where pi is the initial pressure of the gas. Finally,
we obtain
Po+ mg /S
Pi — 1— Ah/h •
2.42. Let us choose the origin as shown in Fig. 205.
Then the force acting on the wedge depends only
Fig. 205
on the x-coordinate of the shock front. The hori
zontal component of this force is
pocxa _ pocavt
Fx = pocx tan a _-
b b '
where x = vt is the wavefront coordinate by the
moment of time t from the beginning of propagation
of the wave through the wedge. The acceleration
imparted to the wedge at this moment of time is
Fx pocavt
a• ...,. — =
' m bm
At the moment of time to when the wavefront
reaches the rear face of the wedge, i.e. when the
wavefront coordinate is b = vto , the acceleration
of the wedge becomes
poca
ato= m •
I 6*