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LECTURE UNIT 009
    3. Second Law of Thermodynamics is concerned with the availability of energy from a thermodynamic
                    cycle and shows the impossibility of a perpetual motion machine.
                A. Kelvin-Plank Statement (Concept of thermal efficiency)
                         It is impossible to operate an engine in a cycle that will have no other effect than to extract heat from a
                                   reservoir and produce an equivalent amount
                                      ILLUSTRATION: Rankine Cycle Steam Power Plant
                                                                                                                   STEAM
                                                                                                .                  TURBINE
                                                                                                ms
                                                                                                              1                                        Pi
                                                              QA
                                                                                                                                2


                                                                                                                                                    QR

                                                                     BOILER                     BOILER FEED PUMP                        CONDENSER
                                                                                                                                    3
                                                                                      B   .                         .
                                                                                          ms                        ms




                                                                                                       WP

                                                    Thermal Efficiency, e:

                                                                                   WNET
                                                                         e=        QA          * 100%

                  B. Reeves Statement
                          Heat flows readily from a region of high temperature to region of lower temperature.
                  C. Clausius statement
                          It is impossible for a self-acting machine, unaided by an external agency to convey heat from one body
                          to another at a higher temperature.
                                    ILLUSTRATION: Refrigeration Cycle
                                                                                                  QR




                                                                                                                         .
                                                                                                                         mR
                                                                              .                CONDENSER
                                                                              mR                                                          COMPRESSOR

                                                                              EXPANSION
                                                                              VALVE
                                                                                                                                                            WC
                                                                              .                EVAPORATOR                  .
                                                                              mR                                           mR




                                                                                                  QA         ROOM




     4. Third Law of Thermodynamics states that the entropy of any pure substance in thermodynamic equilibrium tends to approach
                     zero as the absolute temperature approaches zero.
                                                        T2
                                        S2 - S1 =        dQ
                                                        T T
                                                        1
   CYCLE ANALYSIS
         is a series of processes that a system undergoes, whereby the system’s starting state is also its final state.
               1. Use Pv and Ts diagram to illustrate the cycle.
               2. PVT relationship
                          a.)        PV = mRT                                 (for any ideal gas processes)

                                     P1V1       P2V2
                          b.)               =                                 (for P=C, V=C or T=C only)
                                      T1         T2

                                                  k-1              k-1
                                                   k
                                     T2   P2              V1
                          c.)           =               =                     (for PVk=C or S=C)
                                     T1   P1              V2

                                            Note: Change k to n for Special polytropic process (PVn=C)

                 “God gives us the ingredients for our daily bread, but He expects us to do the baking.”
3. Heat Added, QA

                            QA =         +Q
                                                 CYCLE

              4. Heat Rejected, QR

                            QR =         -Q      CYCLE

              5. Net Work, WNET


                             WNET = QA - QR =                            WNF =             P dV

              6. Cycle thermal efficiency, e
                                        WNET
                             e   =                     * 100%                  (for any cycle)
                                        QA

              7. Cycle mean effective pressure, Pm
                                              Network
                              Pm =
                                        Volumetric displacement
                                         WNET                       e QA
                              Pm =                     =
                                            VD                   (Vmax - Vmin)
CARNOT CYCLE
    The most efficient cycle and basis of comparison for Rankine Cycle.
            ILLUSTRATION:                                                              QA



                                                                               Heat Source
                                                            .                                                   .    2
                                                            ma                                                  ma
                                                   1
                                                                                   TH = C
                                                                                                        WT
                          ADIABATIC                                                                                            ADIABATIC TURBINE
                          COMPRESSOR        S=C                                                                          S=C   OR EXPANDER




                                                                                   TL = C
                                                       .                                                        .
                                                       ma                                                       ma
                                                                                Cold Souce                       3
                                                        4




                                                                                      QR

                   P-v diagram                                                                    T-s diagram
                        P                                                                                   T
                                        1


                                                PV = C
                                                                                                                           1        T=C            2
                              PVk = C                                                        TH = T1 = T2
                                                            2
                                                 WNET                                                                            WNET
                                                                 PVk = C                                             S=C          or                   S=C
                                                                                                                                 QNET
                                            4
                                             PV = C                        3
                                                                                             TL = T4 = T3                                          3
                                                                                                                           4        T=C
                     Pm                           WNET


                                                                                   v                                                                         s
                  Definitions
                                                                               Vmax
                           a.) Expansion Ratio, re =
                                                                               Vmin
                                                                                   Vmax
                           b.) Compression Ratio, rk =
                                                                                   Vmin
                                                                           Vmax
                           c.) Cut-off Ratio,                     rc =
                                                                           Vmin
                                                                            Pmax
                           d.) Pressure Ratio, rp =
                                                                            Pmin

                                        “Practice random acts of kindness and senseless acts of beauty.”
Equations:
     1. PVT Relationships
              Process 1-2 (T = C)
                       P1   V2
                          =    = re(T=C)                 isothermal expansion ratio
                       P2   V1
              Process 2-3 (S = C)
                                                              1
                                    k-1                k-1   k-1
                                     k
                      T3   P3                     V2
                         =                =
                      T2   P2                     V3

                             1                1
                             k-1              k
                       T2            P2                V3
                                   =              =       = re(S=C)       isentropic expansion ratio
                       T3            P3                V2

              Process 3-4 (T = C)
                      V3   P4
                         =    = rk(T=C)                 isothermal compression ratio
                      V4   P3

             Process 4-1 (S = C)
                             1                1
                             k-1              k
                       T1            P1                V4
                                   =              =       = rk(S=C)      isentropic compression ratio
                       T4            P4                V1

                              Since T2 = T1 and T4 = T3, Hence;
                                                                   V3   V4
                                                                      =
                                                                   V2   V1
                              Isentropic expansion ratio = Isentropic compression ratio
                                                             re(S=C) = rk(S=C)

                                    And;                           V3   V2
                                                                      =
                                                                   V4   V1

                                                             re(T=C) = rk(T=C)

                              Isothermal expansion ratio = Isothermal compression ratio


     2. Heat Added, QA
             Process 1-2 (T = C)
                      QA =     +Q
                                              P1           P1
                      QA = mRT1 ln               = mRT2 ln
                                              P2           P2

     3. Heat Rejected, QR

             Process 3-4 (T = C)
                      QR =     -Q

                                              P3           P3
                      QR = mRT3 ln               = mRT4 ln
                                              P4           P4

     4. Net Work, WNET
             WNET = QA - -QR

                                              P1
             WNET = mR (T1 - T4) ln
                                              P2


                         “Everything is created twice - first mentally, then physically.”
5. Carnot cycle thermal efficiency,         e cc
                           WNET
                    e cc = Q      * 100%
                             A

                              T1 - T4
                     e cc =               * 100%
                                 T1
                              TH - TL
                     e cc =           * 100%
                                 TH

       6. Mean effective pressure, Pm
                           WNET
                    Pm =
                             VD
                              e cc   QA
                     Pm =
                              (V3 - V1)

PROBLEM SET:
1.    Consider a three-process air standard power cycle in which process 1-2 is an isothermal compression, 2-3 is a constant-
               pressure heat addition, and 3-1 is an isentropic expansion. Given that P1 = 100 kPa, t1 = 20oC, and P2 = 600 kPa,
                        determine:
               (a) The work and heat transfer for each process and the thermal efficiency of the cycle. [
                                                                                       ]
               (b) Show the cycle on Ts and Pv coordinates.
2.       Consider a three-process air-standard power cycle in which process 1-2 is an isentropic compression, 2-3 is a constant
                  pressure heat addition, and 3-1 is a constant-volume heat rejection. Given that P1 = 100 kPa, T1 = 330 K, and P2 =
800               kPa, determine:
                  (a) The work and heat transfer for each process and the thermal efficiency of the cycle. [
                                                                               ]
                  (b) Show the cycle on Ts and Pv coordinates.
3.       A three-process cycle operating with nitrogen as the working substance has: constant temperature 1-2 (t1 = 40oC, P1 = 110
                  kPa); constant volume heating 2-3; and polytropic expansion 3-1 (n=1.35). The isothermal compression requires -
67 kJ/kg                    of work. Determine:
                  (a) P, T, and v around the cycle
                  (b) The heat in and out [                                  ]
                  (c) The net work [           ]
4.       Two and half kg of an ideal gas with R = 296.9 J/kg.K and cv = 0.7442 kJ/kg.K at a pressure of 827.4 kPa and a
                  temperature of 677oC reject 132.2 kJ of heat at constant pressure. The gas is then expanded according to PV1.25 =
C to a            point where a constant volume process will bring the gas back to its original state. Determine P3, QA, and the
power in kJ.                [                              ]
5.       An air-standard Carnot cycle is executed in a closed system between the temperature limits of 350 and 1200 K. The
                   pressures before and after the isothermal compression are 150 kPa and 300 kPa, respectively. If the net work
output per                  cycle is 400 kJ, determine.
                   (a) The maximum pressure in the cycle [              ]
                   (b) The heat transferred to air [        ]
                   (c) The mass of air [        ]
6.       Consider a three-process thermodynamic cycle which operates on 0.5 kg/s of air is composed of the following reversible
                  processes:
                  (1) constant volume heating process             1-2;
                  (2) isentropic expansion process                2-3;
                  (3) constant pressure heat rejection            3-1
         Given that P1 = 345 kPa, t1 = 38oC and P2 = 4P1, determine:
                             (a) the heat transfer for each process [                          ]
                             (b) the network [           ]
                             (c) and the thermal efficiency [    ]
7.       A thermodynamic cycle is composed of the following processes: isothermal expansion 1-2; isometric 2-3; isentropic 3-1. The
                  cycle runs on 0.125 kg of air and has an expansion ratio of 5.4. For P3 = 100 kPaa and t3 = 27oC, find
                  (a) P,V and t for each point of the cycle.
                  (b) Qin and Qout
                  (c) WNET [       ]
                  (d) ecyc [         ]
                  (e) mean effective pressure [               ]
8.       The following thermodynamic cycle operating at 30 Hz is composed of the following reversible process; isothermal
                  expansion 1-2; polytropic 2-3; isometric 3-1. The cycle uses 0.725 kg of air, for which P2 = 105 kPaa, t2 = 735oC,
and t3 =          37oC, n = 0.75 for the polytropic process. Determine (a) the volume at each corner of the cycle (b) Qin and Qout (c)
the               power [                ] (d) the Pm.
9.        A Carnot engine rejects 1000 Btu/min at 50oF and produces 40 hp. Determine the temperature of heat addition and the
                   amount of heat flow into the engine. [                       ]
10.       A Carnot cycle uses air as the working substance. The heat supplied is 50 Btu. The temperature of the heat rejected is 70oF,
                   and the isentropic compression ratio V4/V1 = 10. Determine (a) the cycle efficiency [     ] (b) the temperature of
heat               added [          ] (c) the work [       ]

                                               “Either you run the day or the day runs you.”

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011 second law_cycle_analysis

  • 1. LECTURE UNIT 009 3. Second Law of Thermodynamics is concerned with the availability of energy from a thermodynamic cycle and shows the impossibility of a perpetual motion machine. A. Kelvin-Plank Statement (Concept of thermal efficiency) It is impossible to operate an engine in a cycle that will have no other effect than to extract heat from a reservoir and produce an equivalent amount ILLUSTRATION: Rankine Cycle Steam Power Plant STEAM . TURBINE ms 1 Pi QA 2 QR BOILER BOILER FEED PUMP CONDENSER 3 B . . ms ms WP Thermal Efficiency, e: WNET e= QA * 100% B. Reeves Statement Heat flows readily from a region of high temperature to region of lower temperature. C. Clausius statement It is impossible for a self-acting machine, unaided by an external agency to convey heat from one body to another at a higher temperature. ILLUSTRATION: Refrigeration Cycle QR . mR . CONDENSER mR COMPRESSOR EXPANSION VALVE WC . EVAPORATOR . mR mR QA ROOM 4. Third Law of Thermodynamics states that the entropy of any pure substance in thermodynamic equilibrium tends to approach zero as the absolute temperature approaches zero. T2 S2 - S1 = dQ T T 1 CYCLE ANALYSIS is a series of processes that a system undergoes, whereby the system’s starting state is also its final state. 1. Use Pv and Ts diagram to illustrate the cycle. 2. PVT relationship a.) PV = mRT (for any ideal gas processes) P1V1 P2V2 b.) = (for P=C, V=C or T=C only) T1 T2 k-1 k-1 k T2 P2 V1 c.) = = (for PVk=C or S=C) T1 P1 V2 Note: Change k to n for Special polytropic process (PVn=C) “God gives us the ingredients for our daily bread, but He expects us to do the baking.”
  • 2. 3. Heat Added, QA QA = +Q CYCLE 4. Heat Rejected, QR QR = -Q CYCLE 5. Net Work, WNET WNET = QA - QR = WNF = P dV 6. Cycle thermal efficiency, e WNET e = * 100% (for any cycle) QA 7. Cycle mean effective pressure, Pm Network Pm = Volumetric displacement WNET e QA Pm = = VD (Vmax - Vmin) CARNOT CYCLE The most efficient cycle and basis of comparison for Rankine Cycle. ILLUSTRATION: QA Heat Source . . 2 ma ma 1 TH = C WT ADIABATIC ADIABATIC TURBINE COMPRESSOR S=C S=C OR EXPANDER TL = C . . ma ma Cold Souce 3 4 QR P-v diagram T-s diagram P T 1 PV = C 1 T=C 2 PVk = C TH = T1 = T2 2 WNET WNET PVk = C S=C or S=C QNET 4 PV = C 3 TL = T4 = T3 3 4 T=C Pm WNET v s Definitions Vmax a.) Expansion Ratio, re = Vmin Vmax b.) Compression Ratio, rk = Vmin Vmax c.) Cut-off Ratio, rc = Vmin Pmax d.) Pressure Ratio, rp = Pmin “Practice random acts of kindness and senseless acts of beauty.”
  • 3. Equations: 1. PVT Relationships Process 1-2 (T = C) P1 V2 = = re(T=C) isothermal expansion ratio P2 V1 Process 2-3 (S = C) 1 k-1 k-1 k-1 k T3 P3 V2 = = T2 P2 V3 1 1 k-1 k T2 P2 V3 = = = re(S=C) isentropic expansion ratio T3 P3 V2 Process 3-4 (T = C) V3 P4 = = rk(T=C) isothermal compression ratio V4 P3 Process 4-1 (S = C) 1 1 k-1 k T1 P1 V4 = = = rk(S=C) isentropic compression ratio T4 P4 V1 Since T2 = T1 and T4 = T3, Hence; V3 V4 = V2 V1 Isentropic expansion ratio = Isentropic compression ratio re(S=C) = rk(S=C) And; V3 V2 = V4 V1 re(T=C) = rk(T=C) Isothermal expansion ratio = Isothermal compression ratio 2. Heat Added, QA Process 1-2 (T = C) QA = +Q P1 P1 QA = mRT1 ln = mRT2 ln P2 P2 3. Heat Rejected, QR Process 3-4 (T = C) QR = -Q P3 P3 QR = mRT3 ln = mRT4 ln P4 P4 4. Net Work, WNET WNET = QA - -QR P1 WNET = mR (T1 - T4) ln P2 “Everything is created twice - first mentally, then physically.”
  • 4. 5. Carnot cycle thermal efficiency, e cc WNET e cc = Q * 100% A T1 - T4 e cc = * 100% T1 TH - TL e cc = * 100% TH 6. Mean effective pressure, Pm WNET Pm = VD e cc QA Pm = (V3 - V1) PROBLEM SET: 1. Consider a three-process air standard power cycle in which process 1-2 is an isothermal compression, 2-3 is a constant- pressure heat addition, and 3-1 is an isentropic expansion. Given that P1 = 100 kPa, t1 = 20oC, and P2 = 600 kPa, determine: (a) The work and heat transfer for each process and the thermal efficiency of the cycle. [ ] (b) Show the cycle on Ts and Pv coordinates. 2. Consider a three-process air-standard power cycle in which process 1-2 is an isentropic compression, 2-3 is a constant pressure heat addition, and 3-1 is a constant-volume heat rejection. Given that P1 = 100 kPa, T1 = 330 K, and P2 = 800 kPa, determine: (a) The work and heat transfer for each process and the thermal efficiency of the cycle. [ ] (b) Show the cycle on Ts and Pv coordinates. 3. A three-process cycle operating with nitrogen as the working substance has: constant temperature 1-2 (t1 = 40oC, P1 = 110 kPa); constant volume heating 2-3; and polytropic expansion 3-1 (n=1.35). The isothermal compression requires - 67 kJ/kg of work. Determine: (a) P, T, and v around the cycle (b) The heat in and out [ ] (c) The net work [ ] 4. Two and half kg of an ideal gas with R = 296.9 J/kg.K and cv = 0.7442 kJ/kg.K at a pressure of 827.4 kPa and a temperature of 677oC reject 132.2 kJ of heat at constant pressure. The gas is then expanded according to PV1.25 = C to a point where a constant volume process will bring the gas back to its original state. Determine P3, QA, and the power in kJ. [ ] 5. An air-standard Carnot cycle is executed in a closed system between the temperature limits of 350 and 1200 K. The pressures before and after the isothermal compression are 150 kPa and 300 kPa, respectively. If the net work output per cycle is 400 kJ, determine. (a) The maximum pressure in the cycle [ ] (b) The heat transferred to air [ ] (c) The mass of air [ ] 6. Consider a three-process thermodynamic cycle which operates on 0.5 kg/s of air is composed of the following reversible processes: (1) constant volume heating process 1-2; (2) isentropic expansion process 2-3; (3) constant pressure heat rejection 3-1 Given that P1 = 345 kPa, t1 = 38oC and P2 = 4P1, determine: (a) the heat transfer for each process [ ] (b) the network [ ] (c) and the thermal efficiency [ ] 7. A thermodynamic cycle is composed of the following processes: isothermal expansion 1-2; isometric 2-3; isentropic 3-1. The cycle runs on 0.125 kg of air and has an expansion ratio of 5.4. For P3 = 100 kPaa and t3 = 27oC, find (a) P,V and t for each point of the cycle. (b) Qin and Qout (c) WNET [ ] (d) ecyc [ ] (e) mean effective pressure [ ] 8. The following thermodynamic cycle operating at 30 Hz is composed of the following reversible process; isothermal expansion 1-2; polytropic 2-3; isometric 3-1. The cycle uses 0.725 kg of air, for which P2 = 105 kPaa, t2 = 735oC, and t3 = 37oC, n = 0.75 for the polytropic process. Determine (a) the volume at each corner of the cycle (b) Qin and Qout (c) the power [ ] (d) the Pm. 9. A Carnot engine rejects 1000 Btu/min at 50oF and produces 40 hp. Determine the temperature of heat addition and the amount of heat flow into the engine. [ ] 10. A Carnot cycle uses air as the working substance. The heat supplied is 50 Btu. The temperature of the heat rejected is 70oF, and the isentropic compression ratio V4/V1 = 10. Determine (a) the cycle efficiency [ ] (b) the temperature of heat added [ ] (c) the work [ ] “Either you run the day or the day runs you.”