BOILER--------------------(3)high pressure vapor⇒-----------------------------TURBINE
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⇑(2)high pressure water-------------------------------------------(4)low pressure steam⇓
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PUMP-----------------------⇐(1)low pressure water------------------------CONDENSER
Noting the clockwise sequence above (with states and pressures of
the water between the components), first establish the pump work
as [P2 − P1] ÷ ρwater or [3500 − 10] kPa ÷ 1000 kg/m3 which goes to
3.49 kJ/kg. A unit mass of working fluid is assumed here since only
efficiency is sought.
Next guide on h2 = h1 + win. A Properties Table Of Saturated Water By Pressure
at 10 kPa (or 0.01 MPa) gives h1 as hf = 191.8 kJ/kg. Then evaluate h2 as
(191.8 + 3.49) or 195.29 kJ/kg.
For heat input, go to a Properties Table Of Superheated Steam under 3.5 MPa and
across 350°C to gain (h3, s3) as (3104.0 kJ/kg, 6.6579 kJ/kg•K). Then heat input is
qB = h3 − h2 or (3104.0 − 195.29) or 2908.71 kJ/kg.
A T-s diagram shows that entropy at State 4 is s4 equal to s3 or 6.6579 kJ/kg•K. Then
build s4 = sf + x4sfg; this enumerates to 6.6579 kJ/kg•K = (0.6491 + 7.5019x4) kJ/kg•K
[with values for sf & sfg taken from the Properties Table Of Saturated Water By Pressure
across from 0.01 MPa]. This will isolate the dryness fraction (or quality) as x4 = 0.8009704208.
Now return to Properties Table Of Saturated Water By Pressure to gain (at P = 0.01 MPa)
h4 = hf + x4hfg or 191.8 kJ/kg + (0.8009704208)(2392.8 kJ/kg) equal to 2108.362023 kJ/kg.
Then work output from the turbine is wT = h3 − h4 or (3104.0 − 2108.362023) or 995.637977 kJ/kg.
As a result, the efficiency is (including pump work) η = (wT − wP) ÷ qB
or (995.637977 − 3.49) kJ/kg ÷ 2908.71 kJ/kg which reduces to
0.3410955293 (or roughly 34.1%).