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CHAPTER 3
3.1 From Table A.1, for M = 0.7; po/p = 1.387 and To/T = 1.098. Hence,
= 1096 ft/sec
M = V/a = 3000/1096 = (2.74)
3.4 From Table A.2, for M1 = 3; p2/p1 = 10.33, 2/1 = 3.857,
= 0.3283, and
M2 =0.4752. Thus,
p2 = p1 (p2/p1) = (1)(1.01 x 105)(10.33) = 1.043 x 106 N/m2 (or 10.33 atm)
Thus,
T T T T
T
p
R
T
T
x
o o
o o
2 1
1 1
1
1
1
1 1
5
101 10
287 123
= =
=
=
.
()( . )
(2.8) = 801K
3.5 (a) po/p =
122 10
101 10
5
5
.
.
x
x
= 1.21. From Table A.1: M = 0.53
3.6 For the shock compression, use M1 as a parameter, along with Table A.2. For the
isentropic compression, use p2/p1 = (v1/v1)–
Note that:
3.7 From Table A.1 for M = 38, To/T = 289.9; To = (289.8)(270) = 78246K
This temperature is almost 8 times the surface temperature of the sun. Long before this
3.8 (a) From Table A.3 for M1 = 2.0:
= 0.7934
From Table A.1 for M1 = 2.0:
T
T
o
o
*
1
(1.8)(288) = 653.4K
This is the total temperature at the exit, since for choked conditions at the exit, M2 = 1 and hence
= To*, p2 = p*, etc. At the inlet,
= 1.8 T1 = (1.8)(288) = 518.4K.
q = cp (
) = 1005 (653.4 – 581.4)
q = 1.357 x 105 joule/kg
p2 = p* = p1/0.3636 =
= 2.75 atm
T2 = T* = T1/0.5289 =
= 544.4K
(b) From Table A.3, for M1 = 0.2:
p1/p* = 2.273, T1/T* = 0.2066,
/To* = 0.1736
From Table A.1, for M1 = 0.2:
3.9 1 slug air + 0.06 slug fuel = 1.06 slug of mixture
Eq. (3.95) becomes
p
u
dp
p
T
du
u
dp
du
Substitute (A4) into (A1).
u
dT
du
u
dT
du
u
dT
du
u
Substitute (A6) and (A8) into (A5)
3.16 q = cp (T0,2 – To,1)
q
c T
T
T
p 0 1
0 2
0 1,
,
,
=
– 1
At M = 2.5, from Table A.3,
= 0.7101.
Since cp T0,1 is the total enthalpy of the gas entering the duct, and q is given as 30% of this total
enthalpy, we have