critical ratio. Also illustrated on this figure is the effect of back pressure on
the nozzle exit pressure Pe. We observe that
To summarize, for all back pressures lower than the critical pressure P*,
the pressure at the exit plane of the converging nozzle Peis equal to P*, the
Mach number at the exit plane is unity, and the mass flow rate is the maxi-
mum (or choked) flow rate. Because the velocity of the flow is sonic at the
throat for the maximum flow rate, a back pressure lower than the critical
pressure cannot be sensed in the nozzle upstream flow and does not affect
the flow rate.
The effects of the stagnation temperature T 0 and stagnation pressure P 0 on
the mass flow rate through a converging nozzle are illustrated in Fig. 17–22
where the mass flow rate is plotted against the static-to-stagnation pressure
ratio at the throat Pt/P 0. An increase in P 0 (or a decrease in T 0 ) will increase
the mass flow rate through the converging nozzle; a decrease in P 0 (or an
increase in T 0 ) will decrease it. We could also conclude this by carefully
observing Eqs. 17–24 and 17–25.
A relation for the variation of flow area Athrough the nozzle relative to
throat area A* can be obtained by combining Eqs. 17–24 and 17–25 for the
same mass flow rate and stagnation properties of a particular fluid. This
yields
(17–26)
Table A–32 gives values of A/A* as a function of the Mach number for air
(k1.4). There is one value of A/A* for each value of the Mach number,
but there are two possible values of the Mach number for each value of
A/A*—one for subsonic flow and another for supersonic flow.
A
A*
1
Ma
ca
2
k 1
ba 1
k 1
2
Ma^2 bd
1 k 1 2> 3 21 k 124
Pee
Pb for PbP*
P* for Pb 6 P*
838 | Thermodynamics
0
Pt
Decrease in ,
P* 1.0
P 0
m
P 0
P 0
P 0 , T 0
increase in T 0 ,
or both
Increase in ,P 0
decrease inT 0 ,
or both
Mat = 1 Mat< 1
⋅
FIGURE 17–22
The variation of the mass flow rate
through a nozzle with inlet stagnation
properties.
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