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Rankine Cycle
Ideal cycle for vapor power plants
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Process 1-2
isentropic compression in a pump
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process 2-3
constant pressure heat addition in a boiler
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process 3-4
isentropic expansion in a turbine
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process 4-1
constant pressure heat rejection in a condenser
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internal irreversibilities?
NO!
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Pump
- enters as - saturated liquid
- during: compressed isentropically; T increases, brought to operating pressure of boiler
- leaves as - compressed liquid
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boiler
- enters as - compressed liquid
- during: heat exchanger, T increase, no P change
- leaves as - superheated vapor
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turbine
- enters as - superheated vapor
- during - expands isentropically; T and P drop
- leaves as - saturated liquid-vapor mix
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condenser
- enters as - saturated liquid-vapor mix
- during - Heat exchanger, reject heat to cooling medium, no P change
- dropleaves as - saturated liquid
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steady-flow energy equation
(qin-qout) + (win-wout) = he-hi
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simple - Pump eq.
- (q=0)
- wpump,in=h2-h1 = v(P2-P1)
- h1=hf@P1 and v=v1=vf@p1
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thermal efficiency
nth=wnet/qin =1 - qout/qin
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wnet
wnet = qin-qout=wturb,out-wpump,in
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simple - state 1
- saturated liquid
- Find h and v - given P, look @ Table A-5 (saturated water)
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simple - state 2
- compressed liquid
- Find h - apply conservation of energy eq.
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simple - state 2 cons. of energy equation
- wpump,in = wturb,out
- h2-h1=v(P2-P1)
- h2 = v(P2-P1)+h1
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simple - state 3
- superheated vapor
- Find h and s - given T and P, look @ Table A-6 (superheated water)
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simple - state 4
- saturated liquid-vapor mix
- Find h - given P; apply quality equations
- get values from A-5
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quality equations
- x# = x# - sf / sfg
- h# = hf+x#hfg
- h# = hf + (s# - sf / sfg)hfg
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wturb,out w/ efficiency
wturb,out = ntws turb,out
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wpump,in w/ efficiency
wpump,in = ws, pump in / np
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linear interpolate
- y = y0 + (x-x0)(y1-y0 / x1-x0)
- x - given
- 0 and 1; table #'s
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double linear interpolate
- Using ex. from hw
- 1) Btwn two P's, linear interpolation for each T, get ha and hb
- 2) Btwn two T's, linear interpolate with ha and hb for final h
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net power
W*dot*net = (mass flow rate)Wnet
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Increase efficiency
- increase T for superheated steam
- increase boiler pressure, at same T (but quality decreases)
- decrease T heat is rejected from condenser
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reheat rankine cycle
two stage turbine to solve excessive moisture problem after increasing boiler pressure
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reheat - qin
qin = qprimary + qreheat = (h3-h2) + (h5-h4)
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reheat - wturb,out
wturb,out = wturb,I + wturb,II = (h3-h4)+(h5-h6)
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Find Preheat
- T3 = T5 - to maintain heat
- find entropy at state 6 - s6 = sf + x6sfg
- use T5 and s5/6 , look @ Table A-6 to find P
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reheat - state 1
- saturated liquid
- find h and v = given P, look @ table A-5
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reheat - state 2
- compressed liquid
- apply conservation of energy eq. (use h1 and v1)
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reheat - state 3
- superheated vapor
- find h3 and s3, given P and T look @ Table A-6
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reheat - state 4
- saturated liquid-vapor mix
- Calculate P4, s4 (s3)
- Look @ Table A-6
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reheat- state 5
- Superheated vapor
- Given T and s5(s4), look @ Table A-6
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reheat - state 6
- Saturated mixture
- Given P, look @ A-5
- apply quality equations, h6 = hf + x6hfg
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Ideal Regen. Rankine cycle w/ open FWH
FHW - device that heats feedwater by regeneration
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regeneration
transfer heat to the feedwater from the expanding steam, in counterflow exchanger built into the turbine
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FWH - qout
qout = (1-y)(h7-h1)
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FWH - wturb,out
wturb,out = (h5-h6) + (1-y)(h6-h7)
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FWH - wpump,in
wpump,in = (1-y)wpumpI,in + wpumpII,in
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fraction of heat extracted
y = m6/m5 (mass flow) = h3-h2 / h6-h2
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FWH - state 1
- saturated liquid
- Find h and v - given P, look @ Table A-5
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FWH - state 2
- compressed liquid
- apply conservation energy
- Find h
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FWH - state 3
- saturated liquid
- find h and v, given P (same as 2 and 6), look @ Table A-5
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FWH - state 4
- compressed liquid
- apply conservation energy
- find h
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FWH - state 5
- superheated vapor
- find h and s, given P and T, look @ Table A-6
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FWH - state 6
- saturated liquid-vapor mix
- find h, given P, apply quality equation
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FWH - state 7
- saturated liquid-vapor mix
- find h, given P appy quality equation
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