TITLE.PM5

(Ann) #1

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


  1. A compressible flow is that flow in which the density of the fluid changes during flow.

  2. 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).

  3. The pressure and density of a gas are related as :
    For isothermal process : p
    ρ
    = constant


For adiabatic process : p
ργ

= constant.


  1. The continuity equation for compressible flow is given as :
    ρAV = constant

    ρ +


dA
A

dV
V
+ = 0 ... in differential form.


  1. 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.



  1. Sonic velocity is given by :


C = dp
d

K
ρρ
= ... in terms of bulk modulus
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