GAS POWER CYCLES 635
dharm
\M-therm\Th13-3.pm5
Solution. Refer Fig. 13.17.
p (bar)
2 3
Vs
Vs
8
100
Adiabatics
4
1 1 (27°C)
Vc
V(m )^3
Fig. 13.17
Cylinder diameter, D = 200 mm or 0.2 m
Stroke length, L = 300 mm or 0.3 m
Initial pressure, p 1 = 1.0 bar
Initial temperature, T 1 = 27 + 273 = 300 K
Cut-off =
8
100
Vs = 0.08 Vs
(i)Pressures and temperatures at salient points :
Now, stroke volume, Vs = π/4 D^2 L = π/4 × 0.2^2 × 0.3 = 0.00942 m^3
V 1 = Vs + Vc = Vs +
V
r
s
− 1
Q V V
c r
= s
−
L
N
M
O
Q
1 P
= Vs 1
1
11
+
−
F
HG
I
KJ
=
r −
r
r
× Vs
i.e., V 1 =
15
15 1
15
− 14
×=Vs × 0.00942 = 0.0101 m^3. (Ans.)
Mass of the air in the cylinder can be calculated by using the gas equation,
p 1 V 1 = mRT 1
m =
pV
RT
11
1
1 10^5 0 0101
287 300
= ××
×
.
= 0.0117 kg/cycle