2 dT Figure 8-13 8-28 Figure 8-13, which is similar to Fig. 8-9(b), shows a Carn
ID: 2076490 • Letter: 2
Question
2 dT Figure 8-13 8-28 Figure 8-13, which is similar to Fig. 8-9(b), shows a Carnot cycle in the liquid vapor region. The working substance is 1 kg of water, and T 453 K, T. 313 K Steam tables list values of T, P, u, s, and h at points on the saturation lines and these are tabulated below, in MKS units, for points a, b, e, and f. e wish to make a complete analysis of the cycle. Point TOK) PON m 2) uo kg 1) s kg 1 K-1) 180 453 7.82 x 105 10 x 105 7.60 x 105 2140 180 453 27.7 x 103 10 x 105 25.8 x 105 6590 40 313 074 x 105 1.67 x 105 1.67 x 105 572 400 313 074 x 105 24.3 x 105 25.6 x 105 8220Explanation / Answer
(e) Mass fraction or vapour quality is,
x = havg-hf / hfg
For point c,
x2 = havg - he / hf - he
Also, TdS = dh - VdP
and if pressure is assumed constant, TdS = dh
So, x2 = Sb-Se / Sf-Se
Similarly, at point d,
x1 = Sa-Se / Sf-Se
(f) Now,
x2 = Sb-Se / Sf-Se
At constant volume, dh = TdS = dU
So, x2 = Ub-Ue / Uf -Ue
Internal energy is same at constant pressure, so Ub = Uc
x2 = Uc-Ue / Uf -Ue
or Uc = Ue+x2(Uf-Ue)
In terms of specific heat,
hc = he+x2(hf-he)
From the quality at point c, we have
x1 = Sa-Se / Sf-Se
Similarly as above, we get
Ud = Ue+x1(Uf-Ue)
and hd = he+x1(hf-he)
(g)
Work done in expansion,
W = -nRdT
= -1*8.314*(453-313)
= - 1163.96 J
(h)
Work done in comression,
W = nRdT
= 1163.96 J
So the ratio of exapansion work to compression work is unity.
(i)
Net work done,
W = Wexpansion + Wcompression
= -1163.96 + 1163.96
= 0 J
so, no work is done throughout the cycle.
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