896 ENGINEERING THERMODYNAMICS
dharm
\M-therm\Th16-2.pm5
=
[(.). ][..(.)]
(. ).
141 15 221415 141
14 1 15
29 59
12 96
22
22
−× + × × − −
+×
= × = 1.32
∴ T 2 = 296 × 1.32 = 390.72 K or 117.72°C. Ans.
M 22 =
()
()
γ
γγ
−+
−−
12
21
1
2
12
M
M
...[Eqn. (16.49)]
= (. ).
..(.)
14 1 15 2
21415 141
29
59
2
2
−× +
×× − −
= = 0.49
∴ M 2 = 0.7. Ans.
(ii) Strength of shock :
Strength of shock = p
p
2
1
- 1 = 2.458 – 1 = 1.458. Ans.
Highlights
- A compressible flow is that flow in which the density of the fluid changes during flow.
- The characteristic equation of state is given by :
p
ρ = RT
where p = absolute pressure, N/m^2 ,
ρ = density of gas, kg/m^3 ,
R = characteristic gas constant, J/kg K, and
R = absolute temperature (= t°C + 273). - The pressure and density of a gas are related as :
For isothermal process : p
ρ
= constant
For adiabatic process : p
ργ
= constant.
- The continuity equation for compressible flow is given as :
ρAV = constant
dρ
ρ +
dA
A
dV
V
+ = 0 ... in differential form.
- For compressible fluids Bernoulli’s equation is given as :
(^) ρpg loge p + V
g
2
2
- z = constant ... for isothermal process
γ
γρ−
F
HG
I
KJ
12
p^2
g
V
g
- z = constant ... for adiabatic process.
- Sonic velocity is given by :
C = dp
d
K
ρρ
= ... in terms of bulk modulus