332 ENGINEERING THERMODYNAMICSDHARM
M-therm\Th6-2.PM5
(i)The irreversibility ;
(ii)The effectiveness.
Take for air : cp = 1.005 kJ/kg K, cv = 0.718 kJ/kg K, R = 0.287 kJ/kg K.
Solution. Mass of air, m = 1 kg
Initial temperature, T 1 = T 0 = 290 K
Final temperature, T 2 = 400 K
Initial pressure, p 1 = p 0 = 1 bar
Final pressure, p 2 = 6 bar.
(i)The irreversibility, I :
We know that reversible work,
Wrev. = Change in internal energy – T 0 × Change in entropy= (u 2 – u 1 ) – T 0 cT
TR p
p eep
log^2 log
12
1F
HGI
KJ− F
HGI
KJL
NM
MO
QP
P= cv (T 2 – T 1 ) – T 0 cT
TR p
p eep
log^2 log
12
1F
HGI
KJ− F
HGI
KJL
NM
MO
QP
P= 0.718 (400 – 290) – 290 1 005400
2900 287^6
1. logeeF. log
HG
I
KJ
− F
HGI
KJL
N
MO
Q
P
= 78.98 – 290 (0.3232 – 0.5142)
= 134.37 kJ/kg (–) [–ve sign indicates that work is done on the air]
Actual work is given by
Wactual = mR T T
n() 12
1−
−
= RT T
n() 12
1−
−
as m = 1 kg.
The index n for the compression is given by :T
Tp
pn
2 n
12
11
=
F
HGI
KJ−∴^400
2906
11
=F
HGI
KJn−
n or 1.379 = ()6nn−^1loge 1.379 =n
nF −
HGI
KJ1
loge 6 or 0.3213 = 1.7917n
nF −
HGI
KJ1∴
n
n−
=
1 0 3213
17917.
.
= 0.1793 or n = 1.218∴ Wactual =
0 287 290 400
1 218 1.( )
(. )−
−
= – 144.8 kJ
(–ve sign means that the work is done on the air)
Now, irreversibility = Wrev – Wactual
= – 134.37 – (– 144.8) = 10.43 kJ. (Ans.)
(ii)The effectiveness, ∈∈∈∈∈ :
∈ = W
Wrev
actual. = −
−
134.37
144.8= 0.928 or 92.8%. (Ans.)