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THERMODYNAMICS - CASE STUDY SOLUTION

   

A steam power plant operates on an ideal reheat-regenerative Rankine cycle with one open feedwater heater, one closed feedwater heater, and one reheater. The fractions of stream extracted from turbines and the thermal efficiency of the cycle are to be determined.

Assumptions:

  • All the components in the cycle operate at steady state.
  • Kinetic and potential energy changes are negligible.
The schematic and the T-s diagram of the power plant are shown below.
     

Schematic of the Power Plant and Its T-s Diagram

     
Saturated Water Temperature Table
Saturated Water Pressure Table
Superheated Steam Table
 

(1) Determine the fraction of steam extracted from the turbines

The enthalpies at various states and the pump work per unit mass of fluid flowing through them can be determined by using the water tables.

State1: saturated water
      P1 = 10 kPa ( given)
      h1 = 191.83 kJ/kg
      v1 = 0.00101 m3/kg

State 2: compressed water
      P2 = 1 MPa (given)
      wpump,in = v1 (P2 - P1)
                   = 0.00101(1,000 - 10) = 1.0 kJ/kg
      h2 = h1 + wpump,in = 192.83 kJ/kg

State 3: saturated water
      P3 = 1 MPa (given)
      h3 = 762.81 kJ/kg
      v3 = 0.00113 m3/kg

State 4: compressed water
      P4 = 16 MPa (given)
      wpump,in = v3 (P4 - P3)
                   = 0.00113(16,000 - 1,000) = 16.9 kJ/kg
      h4 = h3 + wpump,in = 762.81+ 16.9 = 779.71 kJ/kg

State 5: saturated water
      P5 = 16 MPa (given)
      h5 = 1,650.1 kJ/kg

     
   

State 6: superheated vapor
      P6 = 16 MPa (given)
      T6 = 600oC (given)
      h6 = 3,569.8 kJ/kg
      s6= 6.6988 kJ/(kg-K)

State7: superheated vapor
      P7 = 5 MPa (given)
      s7 =s6= 6.6988 kJ/(kg-K)
      h7 = 3,222.4 kJ/kg

State 8: superheated vapor
      P8 = 5 MPa (given)
      T8 = 600oC (given)
      h8 = 3,665.6 kJ/kg
      s8= 7.2731 kJ/(kg-K)

State 9: superheated vapor
      P9 = 1 MPa (given)
      s9 =s8= 7.2731 kJ/(kg-K)
      h9 = 3,138.1 kJ/kg

State 10: saturated mixture
      P10 = 10 kPa (given)
      s10 =s8= 7.2731 kJ/(kg-K)
      x8 = (s8 - sf@10 kPa)/sfg@10 kPa = 88.3%
      h10 = hf@10 kPa+ x8hfg@10 kPa = 2,304.76 kJ/kg

State 11: saturated water
      P11 = 5 MPa (given)
      h11 = 1,154.2 kJ/kg

State 12: The trap is an throttling device
      h12 = h11 = 1,154.2 kJ/kg

     


Open Feedwater Heater


Closed Feedwater Heater

 

Assume y kg steam is extracted from the high-pressure turbine per kg mass of water flowing through the boiler. Also assume z kg steam is extracted from the low-pressure turbine per kg mass of water flowing through the boiler. Then y and z can be determined from the energy balance of the closed and open feedwater heaters.

Closed feedwater heater:
      y(h7 - h11) = 1(h5 - h4)
      y = (1650.1 - 779.71)/(3222.4 -1154.2 )
         = 0.42 kg/kg

Open feedwater heater:
      (1)h3 = (z)h9 + (1 - y - z)h2 + (y)h12
      z =0.056 kg/kg

(2) Determine the thermal efficiency of the cycle

The power output from the high-pressure and low-pressure turbine for 1 kg of mass flowing through the boiler is:

      wturb,out = (1)(h6 - h7) + (1 - y)(h8 - h9)
                      + (1 -y - z )(h9 - h10)
                  = (1)( 3,569.8 - 3,222.4) +
                         (1 -0.42)(3,665.6 - 3,138.1)+
                         (1 - 0.42 - 0.056)(3,138.1 - 2,304.7)
                  = 1,090.0 kJ/kg

The pump input works have been determined in (1) as

      wpump,in = (1 - y -z)1.0 + 16.9
                   = 17.4 kJ/kg

So the total net work output fro 1 kg mass of water flowing through the boiler is
      wnet,out = wturb,out - wpump,in
                 = 1,090.0 - 17.4 = 1,072.6 kJ/kg

The total heat input to the cycle equals the sum of the heat input in the boiler and the heat input from the reheater.

      qin = (1)(h6 - h5) + (1 - y)(h8 - h7)
           = (1)(3,569.8 - 1,650.1) +
             (1 - 0.42)(3,665.6 - 3,222.44)
           = 2,176.7 kJ/kg

The thermal efficiency is
ηth = wnet,out/qin = 1,072.6/ 2,176.7 = 49.3%