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International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056
Volume: 09 Issue: 12 | Dec 2022 www.irjet.net p-ISSN: 2395-0072
© 2022, IRJET | Impact Factor value: 7.529 | ISO 9001:2008 Certified Journal | Page 961
Comparison of Thermal Performance of Rankine Cycle, Reheat Cycle,
Regenerative Cycle & One Stage Regenerative & reheat Rankine Cycle
with Same Initial & Final Parameters
Nitin Badhe1, K.S. Gharge2,
1Student, Dept. of Mechanical Engineering, Government College of Engineering Karad, Maharashtra, India
2Ass. Professor, Dept. of Mechanical Engineering, Government College of Engineering Karad, Maharashtra, India
---------------------------------------------------------------------***---------------------------------------------------------------------
Abstract - Vapor power cycles are used in steam power
plants. In a vapour power cycle heat energy (released by the
burning of fuel) is converted into work(shaftwork), inwhicha
working fluid repeatedly performs asuccessionofprocesses. In
a vapour power cycle, the working fluid is water, which
undergoes a change of phase. Among the various types of
vapor power cycles is the Carnot cycle, which is theoretically
the most efficient cycle and sets the limit for the efficiency of
any vapor cycle. This limit is known as the Carnot limit. The
Rankine cycle and its modifications are used widely and are
theoretically the cycles best suited to steam power plants. By
studying these cycles, we know practically what all must be
done to increase the efficiency and cost effectiveness.
Key Words: Vapor powercycle,Carnotcycle,Rankinecycle,
efficiency, Steam power plant, water, heat energy
1. INTRODUCTION
The steam power cycle is a useful method for constantly
converting heat energy into mechanical energy. The Carnot
cycle has the maximum thermal efficiency of all cycles in a
certain temperature range, in accord with the second law of
thermodynamics. We have seen that Carnot cycle is not the
theoretical/ideal cycle for steam turbine power plant
because of the difficulty of pumping a mixture of water and
steam and delivering it as saturated water only. However,
this difficulty is eliminated in Rankin cycle by complete
condensation of water vapor in the condenser, and then,
pumping the waterisentropicallytoboiler pressure.Rankine
cycle is a theoretical/ideal cycle for comparing the
performance of steam power plants.
Therefore, the Rankine cycle has become a basic cycle
generally used in modern thermal power plants.
Additionally, with the progress of science and technology,
based on the Rankine cycle, there are reheat rankine cycle,
regenerative rankine cycle and so on. At present, the actual
cycles of steam power plants are very complex, but they are
all improved based on the primary cycle. What are the
economic differencesoftheseimproved steampowercycles?
Let us compare them with specific examples.
2. Comparison
Example: In a power cycle, the initial parameters of fresh
steamare p1 = 87 bar, t1 = 510˚C, The pressureofcondenseris
pb = 0.1 bar. When the fresh steam expands to p2 = 20 bar in
the steam turbine, a part of the steam is extracted for
regenerative heating, and the rest is senttothereheatertobe
heated to 500˚C, and then return to the steam turbine to do
work. Assume turbine efficiency = 65% and 100 TPH
2.1 Rankine Cycle (ηt = 65%)
T
(510˚C)
87 bar
0.1 bar
S
Fig. 1. T-s diagram of rankine cycle
From h-s diagram, thestateparametersofthecorresponding
state point are as follows:
h1 = 3414.3 kJ/kg = 3414.3* 0.23884 = 815.47 kcal/kg
h2’ = 2119.99 kJ/kg = 506.34 kcal/kg (S1 = S2)
but ηt = 65%
ηt = = 0.65 =
h2 =2573.01 kJ/kg = 614.54 kcal/kg
h3 = 191.8 kJ/kg = 45.809 kcal/kg
h4 = 200.57 kJ/kg =47.90 kcal/kg
Heat supplied (qi )= h1 – h4
= 3213.72 kJ/kg = 765.565 kcal/kg
Turbine work ( wt )=h1 – h2
1
4
3 2
International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056
Volume: 09 Issue: 12 | Dec 2022 www.irjet.net p-ISSN: 2395-0072
© 2022, IRJET | Impact Factor value: 7.529 | ISO 9001:2008 Certified Journal | Page 962
= 841.27 kJ/kg = 200.93 kcal/kg
Pump Work (wp )= h4 – h3
=8.77 kJ/kg = 2.096 k cal/kg
Electricity generated = 200.93* 0.860*100/1000
= 17.34 MW=14909716.25 k cal/hr
Firing duty =
= 109652857.1 k cal/hr
ηthermal =
= 25.9%
ηcycle =
= 13.59%
2.2 Reheat Cycle
T
87 bar
0.1 bar
S
Fig. 2. T-s diagram of reheat rankine cycle
From h-s diagram, thestateparametersofthecorresponding
state point are as follows:
h1 = 3414.3 kj/kg = 815.47 kcal/kg
h2 =3147.72 kj/kg = 751.80 kcal/kg (ηHP =60%)
h3 = 3480 kj/kg = 831.16 kcal/kg
h4 = 2745.5 kj/kg = 655.73 kcal/kg (ηLP=65%)
h5 = 191.8 kj/kg = 45.80 kcal/kg
h6 = 193.80 kj/kg = 46.28 kcal/kg
Heat supplied (qi)= (h1 – h6) + (h3 – h2)
=3552.79 Kj/kg = 848.55 k cal/kg
Turbine work (wt) =(h1 – h2) + (h3 – h4)
= 1001.08 Kj/kg = 239.1 kcal/kg
Pump Work (wp) = h6 – h5
= 8.776 Kj/kg = 2.094 kcal/kg
Electricity generated = 239.1 * 0.860 * 100/1000
= 20.56 MW=17678417.88 kcal/hr
Firing duty =
= 121221428.6 kcal/hr
ηthermal =
= 28.12%
ηcycle =
= 14.58 %
2.3 Regeneration Cycle
Fig. 3. T-s diagram of regenerative rankine cycle
From h-s diagram, thestateparametersofthecorresponding
state point are as follows:
h1 = 191.8 kj/kg = 45.80 kcal/kg
h2 =193.80 kj/kg = 46.28 kcal/kg
h3 = 908.5 kj/kg = 216.98 kcal/kg
h4 = 916.38 kj/kg = 218.86 kcal/kg
h5 = 3414.3 kj/kg = 815.47 kcal/kg
h6 = 3121.41 kj/kg = 745.51 kcal/kg (ηHP =65%)
h7 = 2472.35 kj/kg = 590.49 kcal/kg (ηHP =65%)
Energy balance of feed water heater
mh6 + (1-m)h2 = h3
m = 0.2441 kg/kg of steam
Heat supplied (qi)= h5 – h4
= 2497.92 kj/kg = 596.60 k cal/kg
Turbine work (wt)= (h5 – h6) + (1-m) (h6 – h7)
= 783.50 kj/kg = 187.132 kcal/kg
Pump Work (wp)= (h2 – h1) + (h4 - h3)
= 9.88 kj/kg = 2.35 kcal/kg
1 3
2
6
5 4
0.1 bar
20 bar
87 bar
International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056
Volume: 09 Issue: 12 | Dec 2022 www.irjet.net p-ISSN: 2395-0072
© 2022, IRJET | Impact Factor value: 7.529 | ISO 9001:2008 Certified Journal | Page 963
Electricity generated = 187.132* 0.860*100/1000
= 16.09 MW=13834909.72 kcal/ hr
Firing duty =
= 85228571.43 kcal/hr
ηthermal =
= 30.97%
ηcycle =
= 16.20%
2.4 One stage regeneration and one reheat cycle
From h-s diagram, thestateparametersofthecorresponding
state point are as follows:
h1 = 191.8 kj/kg = 45.80 kcal/kg
h2 =193.80 kj/kg = 46.28 kcal/kg
h3 = 908.5 kj/kg = 216.986 kcal/kg
h4 = 916.38 kj/kg = 218.86 kcal/kg
h5 = 3414.3 kj/kg = 815.47 kcal/kg
h6 = 3143.94 kj/kg = 750.89 kcal/kg (ηHP =60%)
h7 = 3467.3 kj/kg = 828.129 kcal/kg
h8 = 2744.29 kj/kg = 655.44 kcal/kg (ηLP=65%)
By energy balance of feed water heater
mh6 + (1 - m) h2 = h3
m = 0.2422 kg/kg of steam
Heat supplied (qi) = (h5 – h4) + (1 - m) (h7 – h6)
=2442.96 Kj/kg = 655.12 kcal/kg
Turbine work (wt)=(h5 – h6) + (1 - m) (h7 – h8)
= 818.256 Kj/kg = 195.43 kcal/kg
Pump Work (wp)=( h2 – h1) + (h3 – h4)
= 9.889 Kj/kg = 2.36 kcal/kg
Electricity generated = 195.43 * 0.860 * 100/1000
= 16.80 MW=144453399.83 kcal/hr
Firing duty =
= 93588571.43 kcal/hr
ηthermal =
= 29.47%
ηcycle =
= 15.43 %
2.5 Calculation Result
Under the same initial and final parameters, we calculated
the thermal efficiency and cycle efficiency of Rankine cycle,
reheat cycle, regenerative cycle, and cycle with one stage
regenerative and one reheat, respectively. The results are
shown in Table 1, 2 and 3.
Table 1. Comparison of calculation results between reheat
cycle and Rankine cycle.
Rankine
cycle
reheat cycle
result Comparison with
Rankinecycle
qi
kJ/kg
3213.72 3552.79 ↑ 339.07
wt
kJ/kg
841.29 1001.08 ↑ 159.79
wp
kJ/kg
8.776 8.776 →
ηthermal 25.90% 27.93% ↑2.03%
ηcycle 13.59% 14.58% ↑0.99%
Table 2. Comparison of calculation results between
regenerative cycle and Rankine cycle.
Rankinecycle
regenerative cycle
result Comparison with
Rankinecycle
qi
kJ/kg
3213.72 2497.92 ↓ 715.8
wt
kJ/kg
841.29 783.507 ↓57.783
wp
kJ/kg
8.776 9.88 ↑ 1.11
ηthermal 25.90% 30.97% ↑5.07%
ηcycle 13.59% 16.20% ↑2.61%
International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056
Volume: 09 Issue: 12 | Dec 2022 www.irjet.net p-ISSN: 2395-0072
© 2022, IRJET | Impact Factor value: 7.529 | ISO 9001:2008 Certified Journal | Page 964
Table 3. Comparison of calculation results between one
stage regeneration and one reheat cycle and Rankine
cycle.
Rankine
cycle
one stage regeneration and one
reheat cycle
result
Comparison with
Rankinecycle
qi
kJ/kg
3213.72 2742.96 ↓ 470.76
wt
kJ/kg
841.29 818.25 ↓23.04
wp
kJ/kg
8.776 9.889 ↑ 1.11
ηthermal 25.90% 29.47% ↑3.57%
ηcycle 13.59% 15.43% ↑1.84%
3. CONCLUSIONS
From the above result it can be seen that thermal efficiency
and cycle efficiency is higher in regenerative rankine cycle
than reheat as well as one stage regeneration reheat rankine
cycle compare with the same parameters.
Heat energy supplied to the boilerishigherin reheatrankine
cycle and heat energy supplied to the boiler is lower in
regenerative rankine cycle.
Work of turbine is higher in reheat rankine cycle i.e.,
electricity production is also high as compare to
regeneration and as one stage regeneration reheat rankine
cycle.
From the above result it can be seen that regeneration
involves the utilization of heat within the system while
reheating or superheating requires additional heat addition
from outside. Thus, the suitable degree of regeneration may
be better over reheating or superheating options.
REFERENCES
[1] YarongWang, and PeirongWang, “Thermal performance
comparison of Rankine cycle, reheat cycle and
regenerative cycle with the same initial and final
parameters” E3S web of conferences 245, 03015(2021)
[2] Gulab Chand Sahu, Manoj Sao, Abhishek Kumar Jain,
“Comparison Between Regenerative , Reheat &
Cogeneration Steam Plant on the basis of Turbine Inlet
Temperature” IJARSET ISSN 2350 – 0328, Vol. 4, Issue 1,
February 2017
[3] R.K. Naradasu, R.K. Konijeti, and V.R. Alluru,
“Thermodynamic analysis of heat recovery steam
generator in combined cycle power plant”, International
Organization Of Science Research, Vol. 11, pp. 143-156,
2007
[4] R.K.Kapooria, S.Kumar, K.S.Kasana, “An analysis of a
thermal power plant working on a Rankine cycle: A
theoretical investigation”, Journal of Energyin Southern
Africa, Vol 19, pp. 77-83, February 2008.
[5] Ivan Sunit Rout, Abhishek Gaikwad, Vinod Kumar
Verma, Mohammad Tariq, “Thermal Analysis of Steam
Turbine Power Plants”, International Organization Of
Science Research, Vol. 7, pp. 28-36, May. - Jun. 2013
[6] Charles Mborah, Abeekuh Brew Hammond, Seth P.
Agbomadzi, “Thermodynamic Analysis of the Gas and
Steam Turbines at Takoradi Thermal Power Station”,
European Journal of Technology and Advanced
Engineering Research, Vol.1, pp.62-72, 2010.
[7] Raviprakash kurkiya, Sharad chaudhary, “Energy
Analysis of Thermal Power Plant”, International Journal
of Scientific & Engineering Research, Vol.3,pp.1-7,July-
2012.
[8] M. A. Jegadeswaran, V. Sam Daniel, G.
Thamaraikkannan,“AnalysisforEfficiencyImprovement
and Fuel Savings Opportunities in Thermal Power
Plant”, The International Journal Of Science &
Technoledge, Vol 3, pp. 9-15, September, 2015.
[9] Adeyinka O. Adeoye, Christian O. Osueke, Anthony O.
Onokwai, Chinedu A.K Ezugwu, “Enhancing the
Performance of 75mw Steam Power Plant with Second
Law Efficiency, Condenser Pressure andRankineCycle”,
The International Journal Of Engineering And Science,
Vol. 4, pp. 18-29, 2015.
[10] P.Srinivasarao, Dr. P. Ravinder Reddy, Dr.K.Vijaya
Kumar Reddy, “Advance Power Plant Technologies and
Steam CycleforSuperCritical Application”,International
Journal of Scientific and Research, Vol. 2, pp. 1-10,
September 2012.
[11] Onkar Singh, “Applied Thermodynamics” third editon
ISBN (13): 978-81-224-2916-9
[12] P K Nag, “Basic and Applied Thermodynamics” eight
editon ISBN 0-07-047338-2
[13] Xu, Y.P., Ke, X.Y. (2012) Thermal Engineering. China
Electric Power Press, Beijing
International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056
Volume: 09 Issue: 12 | Dec 2022 www.irjet.net p-ISSN: 2395-0072
© 2022, IRJET | Impact Factor value: 7.529 | ISO 9001:2008 Certified Journal | Page 965
[14] Cheng, G.T., Wang, Y.Z. (2007) Engineering
Thermodynamics (SecondEdition). BeijingUniversityof
Technology Press, Beijing.
[15] Chen, Z.H. (2009) Basic Thermal Engineering, China
Electric Power Press, Beijing.
[16] Shen, W.D., Geng, T.J. (2007) Engineering
Thermodynamics, Higher Education Press, Beijing

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Comparison of Thermal Performance of Rankine Cycle, Reheat Cycle, Regenerative Cycle & One Stage Regenerative & reheat Rankine Cycle with Same Initial & Final Parameters

  • 1. International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 09 Issue: 12 | Dec 2022 www.irjet.net p-ISSN: 2395-0072 © 2022, IRJET | Impact Factor value: 7.529 | ISO 9001:2008 Certified Journal | Page 961 Comparison of Thermal Performance of Rankine Cycle, Reheat Cycle, Regenerative Cycle & One Stage Regenerative & reheat Rankine Cycle with Same Initial & Final Parameters Nitin Badhe1, K.S. Gharge2, 1Student, Dept. of Mechanical Engineering, Government College of Engineering Karad, Maharashtra, India 2Ass. Professor, Dept. of Mechanical Engineering, Government College of Engineering Karad, Maharashtra, India ---------------------------------------------------------------------***--------------------------------------------------------------------- Abstract - Vapor power cycles are used in steam power plants. In a vapour power cycle heat energy (released by the burning of fuel) is converted into work(shaftwork), inwhicha working fluid repeatedly performs asuccessionofprocesses. In a vapour power cycle, the working fluid is water, which undergoes a change of phase. Among the various types of vapor power cycles is the Carnot cycle, which is theoretically the most efficient cycle and sets the limit for the efficiency of any vapor cycle. This limit is known as the Carnot limit. The Rankine cycle and its modifications are used widely and are theoretically the cycles best suited to steam power plants. By studying these cycles, we know practically what all must be done to increase the efficiency and cost effectiveness. Key Words: Vapor powercycle,Carnotcycle,Rankinecycle, efficiency, Steam power plant, water, heat energy 1. INTRODUCTION The steam power cycle is a useful method for constantly converting heat energy into mechanical energy. The Carnot cycle has the maximum thermal efficiency of all cycles in a certain temperature range, in accord with the second law of thermodynamics. We have seen that Carnot cycle is not the theoretical/ideal cycle for steam turbine power plant because of the difficulty of pumping a mixture of water and steam and delivering it as saturated water only. However, this difficulty is eliminated in Rankin cycle by complete condensation of water vapor in the condenser, and then, pumping the waterisentropicallytoboiler pressure.Rankine cycle is a theoretical/ideal cycle for comparing the performance of steam power plants. Therefore, the Rankine cycle has become a basic cycle generally used in modern thermal power plants. Additionally, with the progress of science and technology, based on the Rankine cycle, there are reheat rankine cycle, regenerative rankine cycle and so on. At present, the actual cycles of steam power plants are very complex, but they are all improved based on the primary cycle. What are the economic differencesoftheseimproved steampowercycles? Let us compare them with specific examples. 2. Comparison Example: In a power cycle, the initial parameters of fresh steamare p1 = 87 bar, t1 = 510˚C, The pressureofcondenseris pb = 0.1 bar. When the fresh steam expands to p2 = 20 bar in the steam turbine, a part of the steam is extracted for regenerative heating, and the rest is senttothereheatertobe heated to 500˚C, and then return to the steam turbine to do work. Assume turbine efficiency = 65% and 100 TPH 2.1 Rankine Cycle (ηt = 65%) T (510˚C) 87 bar 0.1 bar S Fig. 1. T-s diagram of rankine cycle From h-s diagram, thestateparametersofthecorresponding state point are as follows: h1 = 3414.3 kJ/kg = 3414.3* 0.23884 = 815.47 kcal/kg h2’ = 2119.99 kJ/kg = 506.34 kcal/kg (S1 = S2) but ηt = 65% ηt = = 0.65 = h2 =2573.01 kJ/kg = 614.54 kcal/kg h3 = 191.8 kJ/kg = 45.809 kcal/kg h4 = 200.57 kJ/kg =47.90 kcal/kg Heat supplied (qi )= h1 – h4 = 3213.72 kJ/kg = 765.565 kcal/kg Turbine work ( wt )=h1 – h2 1 4 3 2
  • 2. International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 09 Issue: 12 | Dec 2022 www.irjet.net p-ISSN: 2395-0072 © 2022, IRJET | Impact Factor value: 7.529 | ISO 9001:2008 Certified Journal | Page 962 = 841.27 kJ/kg = 200.93 kcal/kg Pump Work (wp )= h4 – h3 =8.77 kJ/kg = 2.096 k cal/kg Electricity generated = 200.93* 0.860*100/1000 = 17.34 MW=14909716.25 k cal/hr Firing duty = = 109652857.1 k cal/hr ηthermal = = 25.9% ηcycle = = 13.59% 2.2 Reheat Cycle T 87 bar 0.1 bar S Fig. 2. T-s diagram of reheat rankine cycle From h-s diagram, thestateparametersofthecorresponding state point are as follows: h1 = 3414.3 kj/kg = 815.47 kcal/kg h2 =3147.72 kj/kg = 751.80 kcal/kg (ηHP =60%) h3 = 3480 kj/kg = 831.16 kcal/kg h4 = 2745.5 kj/kg = 655.73 kcal/kg (ηLP=65%) h5 = 191.8 kj/kg = 45.80 kcal/kg h6 = 193.80 kj/kg = 46.28 kcal/kg Heat supplied (qi)= (h1 – h6) + (h3 – h2) =3552.79 Kj/kg = 848.55 k cal/kg Turbine work (wt) =(h1 – h2) + (h3 – h4) = 1001.08 Kj/kg = 239.1 kcal/kg Pump Work (wp) = h6 – h5 = 8.776 Kj/kg = 2.094 kcal/kg Electricity generated = 239.1 * 0.860 * 100/1000 = 20.56 MW=17678417.88 kcal/hr Firing duty = = 121221428.6 kcal/hr ηthermal = = 28.12% ηcycle = = 14.58 % 2.3 Regeneration Cycle Fig. 3. T-s diagram of regenerative rankine cycle From h-s diagram, thestateparametersofthecorresponding state point are as follows: h1 = 191.8 kj/kg = 45.80 kcal/kg h2 =193.80 kj/kg = 46.28 kcal/kg h3 = 908.5 kj/kg = 216.98 kcal/kg h4 = 916.38 kj/kg = 218.86 kcal/kg h5 = 3414.3 kj/kg = 815.47 kcal/kg h6 = 3121.41 kj/kg = 745.51 kcal/kg (ηHP =65%) h7 = 2472.35 kj/kg = 590.49 kcal/kg (ηHP =65%) Energy balance of feed water heater mh6 + (1-m)h2 = h3 m = 0.2441 kg/kg of steam Heat supplied (qi)= h5 – h4 = 2497.92 kj/kg = 596.60 k cal/kg Turbine work (wt)= (h5 – h6) + (1-m) (h6 – h7) = 783.50 kj/kg = 187.132 kcal/kg Pump Work (wp)= (h2 – h1) + (h4 - h3) = 9.88 kj/kg = 2.35 kcal/kg 1 3 2 6 5 4 0.1 bar 20 bar 87 bar
  • 3. International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 09 Issue: 12 | Dec 2022 www.irjet.net p-ISSN: 2395-0072 © 2022, IRJET | Impact Factor value: 7.529 | ISO 9001:2008 Certified Journal | Page 963 Electricity generated = 187.132* 0.860*100/1000 = 16.09 MW=13834909.72 kcal/ hr Firing duty = = 85228571.43 kcal/hr ηthermal = = 30.97% ηcycle = = 16.20% 2.4 One stage regeneration and one reheat cycle From h-s diagram, thestateparametersofthecorresponding state point are as follows: h1 = 191.8 kj/kg = 45.80 kcal/kg h2 =193.80 kj/kg = 46.28 kcal/kg h3 = 908.5 kj/kg = 216.986 kcal/kg h4 = 916.38 kj/kg = 218.86 kcal/kg h5 = 3414.3 kj/kg = 815.47 kcal/kg h6 = 3143.94 kj/kg = 750.89 kcal/kg (ηHP =60%) h7 = 3467.3 kj/kg = 828.129 kcal/kg h8 = 2744.29 kj/kg = 655.44 kcal/kg (ηLP=65%) By energy balance of feed water heater mh6 + (1 - m) h2 = h3 m = 0.2422 kg/kg of steam Heat supplied (qi) = (h5 – h4) + (1 - m) (h7 – h6) =2442.96 Kj/kg = 655.12 kcal/kg Turbine work (wt)=(h5 – h6) + (1 - m) (h7 – h8) = 818.256 Kj/kg = 195.43 kcal/kg Pump Work (wp)=( h2 – h1) + (h3 – h4) = 9.889 Kj/kg = 2.36 kcal/kg Electricity generated = 195.43 * 0.860 * 100/1000 = 16.80 MW=144453399.83 kcal/hr Firing duty = = 93588571.43 kcal/hr ηthermal = = 29.47% ηcycle = = 15.43 % 2.5 Calculation Result Under the same initial and final parameters, we calculated the thermal efficiency and cycle efficiency of Rankine cycle, reheat cycle, regenerative cycle, and cycle with one stage regenerative and one reheat, respectively. The results are shown in Table 1, 2 and 3. Table 1. Comparison of calculation results between reheat cycle and Rankine cycle. Rankine cycle reheat cycle result Comparison with Rankinecycle qi kJ/kg 3213.72 3552.79 ↑ 339.07 wt kJ/kg 841.29 1001.08 ↑ 159.79 wp kJ/kg 8.776 8.776 → ηthermal 25.90% 27.93% ↑2.03% ηcycle 13.59% 14.58% ↑0.99% Table 2. Comparison of calculation results between regenerative cycle and Rankine cycle. Rankinecycle regenerative cycle result Comparison with Rankinecycle qi kJ/kg 3213.72 2497.92 ↓ 715.8 wt kJ/kg 841.29 783.507 ↓57.783 wp kJ/kg 8.776 9.88 ↑ 1.11 ηthermal 25.90% 30.97% ↑5.07% ηcycle 13.59% 16.20% ↑2.61%
  • 4. International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 09 Issue: 12 | Dec 2022 www.irjet.net p-ISSN: 2395-0072 © 2022, IRJET | Impact Factor value: 7.529 | ISO 9001:2008 Certified Journal | Page 964 Table 3. Comparison of calculation results between one stage regeneration and one reheat cycle and Rankine cycle. Rankine cycle one stage regeneration and one reheat cycle result Comparison with Rankinecycle qi kJ/kg 3213.72 2742.96 ↓ 470.76 wt kJ/kg 841.29 818.25 ↓23.04 wp kJ/kg 8.776 9.889 ↑ 1.11 ηthermal 25.90% 29.47% ↑3.57% ηcycle 13.59% 15.43% ↑1.84% 3. CONCLUSIONS From the above result it can be seen that thermal efficiency and cycle efficiency is higher in regenerative rankine cycle than reheat as well as one stage regeneration reheat rankine cycle compare with the same parameters. Heat energy supplied to the boilerishigherin reheatrankine cycle and heat energy supplied to the boiler is lower in regenerative rankine cycle. Work of turbine is higher in reheat rankine cycle i.e., electricity production is also high as compare to regeneration and as one stage regeneration reheat rankine cycle. From the above result it can be seen that regeneration involves the utilization of heat within the system while reheating or superheating requires additional heat addition from outside. Thus, the suitable degree of regeneration may be better over reheating or superheating options. REFERENCES [1] YarongWang, and PeirongWang, “Thermal performance comparison of Rankine cycle, reheat cycle and regenerative cycle with the same initial and final parameters” E3S web of conferences 245, 03015(2021) [2] Gulab Chand Sahu, Manoj Sao, Abhishek Kumar Jain, “Comparison Between Regenerative , Reheat & Cogeneration Steam Plant on the basis of Turbine Inlet Temperature” IJARSET ISSN 2350 – 0328, Vol. 4, Issue 1, February 2017 [3] R.K. Naradasu, R.K. Konijeti, and V.R. Alluru, “Thermodynamic analysis of heat recovery steam generator in combined cycle power plant”, International Organization Of Science Research, Vol. 11, pp. 143-156, 2007 [4] R.K.Kapooria, S.Kumar, K.S.Kasana, “An analysis of a thermal power plant working on a Rankine cycle: A theoretical investigation”, Journal of Energyin Southern Africa, Vol 19, pp. 77-83, February 2008. [5] Ivan Sunit Rout, Abhishek Gaikwad, Vinod Kumar Verma, Mohammad Tariq, “Thermal Analysis of Steam Turbine Power Plants”, International Organization Of Science Research, Vol. 7, pp. 28-36, May. - Jun. 2013 [6] Charles Mborah, Abeekuh Brew Hammond, Seth P. Agbomadzi, “Thermodynamic Analysis of the Gas and Steam Turbines at Takoradi Thermal Power Station”, European Journal of Technology and Advanced Engineering Research, Vol.1, pp.62-72, 2010. [7] Raviprakash kurkiya, Sharad chaudhary, “Energy Analysis of Thermal Power Plant”, International Journal of Scientific & Engineering Research, Vol.3,pp.1-7,July- 2012. [8] M. A. Jegadeswaran, V. Sam Daniel, G. Thamaraikkannan,“AnalysisforEfficiencyImprovement and Fuel Savings Opportunities in Thermal Power Plant”, The International Journal Of Science & Technoledge, Vol 3, pp. 9-15, September, 2015. [9] Adeyinka O. Adeoye, Christian O. Osueke, Anthony O. Onokwai, Chinedu A.K Ezugwu, “Enhancing the Performance of 75mw Steam Power Plant with Second Law Efficiency, Condenser Pressure andRankineCycle”, The International Journal Of Engineering And Science, Vol. 4, pp. 18-29, 2015. [10] P.Srinivasarao, Dr. P. Ravinder Reddy, Dr.K.Vijaya Kumar Reddy, “Advance Power Plant Technologies and Steam CycleforSuperCritical Application”,International Journal of Scientific and Research, Vol. 2, pp. 1-10, September 2012. [11] Onkar Singh, “Applied Thermodynamics” third editon ISBN (13): 978-81-224-2916-9 [12] P K Nag, “Basic and Applied Thermodynamics” eight editon ISBN 0-07-047338-2 [13] Xu, Y.P., Ke, X.Y. (2012) Thermal Engineering. China Electric Power Press, Beijing
  • 5. International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 09 Issue: 12 | Dec 2022 www.irjet.net p-ISSN: 2395-0072 © 2022, IRJET | Impact Factor value: 7.529 | ISO 9001:2008 Certified Journal | Page 965 [14] Cheng, G.T., Wang, Y.Z. (2007) Engineering Thermodynamics (SecondEdition). BeijingUniversityof Technology Press, Beijing. [15] Chen, Z.H. (2009) Basic Thermal Engineering, China Electric Power Press, Beijing. [16] Shen, W.D., Geng, T.J. (2007) Engineering Thermodynamics, Higher Education Press, Beijing