850 | Thermodynamics
Differentiating, we have
Solving for dVgives
Combining this with the energy equation, we have
which is the equation for the Fanno line in differential form. At point a
(the point of maximum entropy) ds0. Then from the second T dsrelation
(T dsdhvdP) we have dhvdPdP/r. Substituting yields
Solving for V, we have
which is the relation for the speed of sound, Eq. 17–9. Thus the proof is
complete.
Va
0 P
0 r
b
1 > 2
s
dP
r
V^2
dr
r
0 ¬¬at sconstant
dhV^2
dr
r
0
dVV
dr
r
r dVV dr 0
EXAMPLE 17–9 Shock Wave in a Converging–Diverging Nozzle
If the air flowing through the converging–diverging nozzle of Example 17–7
experiences a normal shock wave at the nozzle exit plane (Fig. 17–35), deter-
mine the following after the shock: (a) the stagnation pressure, static pres-
sure, static temperature, and static density; (b) the entropy change across the
shock; (c) the exit velocity; and (d) the mass flow rate through the nozzle.
Assume steady, one-dimensional, and isentropic flow with k1.4 from the
nozzle inlet to the shock location.
Solution Air flowing through a converging–diverging nozzle experiences a
normal shock at the exit. The effect of the shock wave on various properties
is to be determined.
Assumptions 1 Air is an ideal gas with constant specific heats at room
temperature. 2 Flow through the nozzle is steady, one-dimensional, and
isentropic before the shock occurs. 3 The shock wave occurs at the exit
plane.
Properties The constant-pressure specific heat and the specific heat ratio of
air are cp1.005 kJ/kg · K and k1.4. The gas constant of air is 0.287
kJ/kg K (Table A–2a).
Analysis (a) The fluid properties at the exit of the nozzle just before the
shock (denoted by subscript 1) are those evaluated in Example 17–7 at the
nozzle exit to be
P 01 1.0 MPa¬P 1 0.1278 MPa T 1 444.5 K¬r 1 1.002 kg>m^3
T = 444.5 K
Ma 1 = 2
P 01
1
1
1
= 1.0 MPa
P = 0.1278 MPa
r = 1.002 kg/m^3
Shock wave
12
m· = 2.86 kg/s
FIGURE 17–35
Schematic for Example 17–9.
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