GAS POWER CYCLES 635
dharm
\M-therm\Th13-3.pm5
Solution. Refer Fig. 13.17.p (bar)2 3VsVs8
100
Adiabatics41 1 (27°C)VcV(m )^3Fig. 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 KCut-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^3V 1 = Vs + Vc = Vs +
V
rs
− 1Q V V
c r
= s
−L
N
MO
Q
1 P= Vs 1
1
11+
−F
HGI
KJ=
r −r
r
× Vsi.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 1m =
pV
RT11
11 10^5 0 0101
287 300
= ××
×.
= 0.0117 kg/cycle