In Figure (5.3), the Mach number after the shock,
My,
and the ratio of the total pressure,
P0y/P0x,
are plotted as a function of the entrance Mach number.
The working equations were presented earlier.
Note that the
has a minimum value which depends on the specific
heat ratio.
It can be noticed that the density ratio (velocity ratio) also has
a finite value regardless of the upstream Mach number.
The typical situations in which these equations can be used
also include the moving shocks.
The equations should be used with the Mach number (upstream or
downstream) for a given pressure ratio or density ratio (velocity
ratio).
This kind of equations requires examining Table
(5.1) for
or utilizing Potto-GDC for
for value of the specific heat ratio.
Finding the Mach number for a pressure ratio of
8.30879 and
k=1.32 and
is only a few mouse clicks away from the following table.
This table was generated by Potto-GDC (in HTML)
Normal Shock
Input: Py/Px
k = 1.32
Mx
My
Ty/Tx
ρy/ρx
Py/Px
P0y/P0x
2.7245
0.476422
2.111
3.93596
8.30879
0.381089
Now the velocity downstream is determined by the inverse ratio of
ρy = 993.6 / 3.85714 = 257.6
[m/sec].
Analysis:
First, the known information
Mx=3, Px=1.5[bar] and T=273 K.
Using these data, the total pressure can be obtained (through an
isentropic relationship Table
(4.2), i.e.
P0x
is known).
Also with the temperature,
Tx
the velocity can readily be calculated.
The relationship that was calculated will be utilized to obtain
the ratios for downstream of the normal shock.
Normal Shock
Input: Mx
k = 1.4
Mx
My
Ty/Tx
ρy/ρx
Py/Px
P0y/P0x
3
0.475191
2.67901
3.85714
10.3333
0.328344