p (bar) h (kJ/kg) v (m'/kg) s (kJ/kg-K) State 60 2784 1 5.888 1.5 2262 0.8064 6.102 1.5 467.3 0.001053 4 60 476.8 Determine: (a) the percent isentropic turbine efficiency. (b) the rate of exergy destruction per unit mass of steam flowing in the turbine, in kJ/kg. (c) the percent isentropic pump efficiency. (d) the percent thermal efficiency. 2. 3.

Elements Of Electromagnetics
7th Edition
ISBN:9780190698614
Author:Sadiku, Matthew N. O.
Publisher:Sadiku, Matthew N. O.
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p (bar)
h (kJ/kg)
v (m?/kg)
s (kJ/kg-K)
State
1
60
2784
1
5.888
2
1.5
2262
0.8064
6.102
3
1.5
467.3
0.001053
60
476.8
Determine:
(a) the percent isentropic turbine efficiency.
(b) the rate of exergy destruction per unit mass of steam flowing in the turbine, in kJ/kg.
(c) the percent isentropic pump efficiency.
(d) the percent thermal efficiency.
4-
Transcribed Image Text:p (bar) h (kJ/kg) v (m?/kg) s (kJ/kg-K) State 1 60 2784 1 5.888 2 1.5 2262 0.8064 6.102 3 1.5 467.3 0.001053 60 476.8 Determine: (a) the percent isentropic turbine efficiency. (b) the rate of exergy destruction per unit mass of steam flowing in the turbine, in kJ/kg. (c) the percent isentropic pump efficiency. (d) the percent thermal efficiency. 4-
Steam is the working fluid in the Rankine cycle 1-2-3-4-1, shown in the T-s diagram below, which includes the effects of
irreversibilities in the adiabatic expansion and compression processes. The cycle operates with steady flow devices between the
pressures of 60 bar and 1.5 bar. Let To = 300 K, po = 1 bar.
T
p= 60 bar
p = 1.5 bar
Transcribed Image Text:Steam is the working fluid in the Rankine cycle 1-2-3-4-1, shown in the T-s diagram below, which includes the effects of irreversibilities in the adiabatic expansion and compression processes. The cycle operates with steady flow devices between the pressures of 60 bar and 1.5 bar. Let To = 300 K, po = 1 bar. T p= 60 bar p = 1.5 bar
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