GASES AND VAPOUR MIXTURES 431
dharm
\M-therm\Th9-2.pm5
Solution. Using the relation, n =
pV
RT 0
∴ nO 2 =
810 18
8 314 10 323
5
3
××
××
.
(. )
= 0.536 (where TO 2 = 50 + 273 = 323 K)
and nCO =
110 36
8 314 10 293
5
3
××
××
.
(. )
= 0.1478 (where TCO = 20 + 273 = 293 K).
(i)Final temperature (T) and pressure (p) of the mixture :
Before mixing :
U 1 = Σ niCviTi = 0.536 × 21.07 × 323 + 0.1478 × 20.86 × 293
i.e., U 1 = 4551.15 kJ
After mixing :
U 2 = T Σ niCvi = T (0.536 × 21.07 + 0.1478 × 20.86)
i.e., U 2 = 14.37 T
For adiabatic mixing,
U 1 = U 2
∴ 4551.15 = 14.37 T
∴ T =
455115
14 37
.
.
= 316.7 K
∴ Temperature of the mixture = 316.7 – 273 = 43.7°C. (Ans.)
Now p =
nR T
V
0
∴ p =
(.. )..
(.. )
0 536 01478 8 314 10 316 7
18 36 10
3
5
+×××
+×
= 3.33 bar
i.e., Pressure after mixing = 3.33 bar. (Ans.)
(ii)Change of entropy of the system :
Change of entropy of the system = change of entropy of the O 2 + change of entropy of CO
...... Gibbs-Dalton law
Referring to Fig. 9.7, the change of entropy of O 2 can be calculated by replacing the process
undergone by the oxygen by the two processes 1 to A and A to 2.
V 2
V 1
1
T^2
2
T 1 B
R loge
C logve
T
S
V 2
V (^1) V 1
V 2
1 Isothermal
2
A
T
S
C logve
R loge
V 2
V 1 Constant volume T
T
1
2
T
T
2
1
Fig. 9.7 Fig. 9.8