138 ENGINEERING THERMODYNAMICS
dharm
/M-therm/Th4-3.pm5
(ii)Index of expansion, n :
If the work done by the polytropic process is the same,
W1–2–3 = W1–3 =
pV pV
n
11 33
1
−
−
85454 =
4 10 0 02 10 0
1
336
1
××− ××^55
−
=^5
−
.2 1. .732
()nn
∴ n= 854545336 + 1
i.e., n = 1.062
Hence, value of index = 1.062. (Ans.)
Example 4.24. The following is the equation which connects u, p and v for several gases
u = a + bpv
where a and b are constants. Prove that for a reversible adiabatic process,
pvγ = constant, where γ =
b1
b
+
.
Solution. Consider a unit mass.
For a reversible adiabatic process, first law gives
0 = du + pdv
∴ dudv = – p ...(i)
Also, u = a + bpv
∴ dudv = da bpv()dv+ = bv dpdv + bp
= b pv
dp
+ dv
F
H
I
. K ...(ii)
Equating (i) and (ii), we get
b pv
dp
+ dv
F
H
I
. K = – p
bp + b. v. dpdv = – p
bp + p + bv. dp
dv
= 0
p(b + 1) + bv. dpdv = 0
Multiplying both sides by dv
bpv
, we get
b
b
dv
v
dp
p
F +
HG
I
KJ +
1
= 0
or
dp
p
b
b
dv
+ v
F +
H
I
K
1
= 0
d(loge p) +
b
b
F +
H
I
K
1
d(loge v) = 0