IJSRD - International Journal for Scientific Research & Development Vol. 4, Issue 03, 2016 ISSN (online):

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IJSRD - International Journal for Scientific Research & Development Vol. 4, Issue 03, 2016 ISSN (online): 2321-0613 Energy & Exergy Analysis of Turbines of Thermal Power Plant Manoj Kumar Attri 1 Dhairya Naryan 2 Rahul Singh 3 Vikas Gangwar 4 1,2 Assistant Professor 3,4 Student 1,3,4 Department of Mechanical Engineering 2 Department of Electrical Engineering 1,2 SITE Subharti University Meerut, India 3,4 Gautam Buddha University Greater Noida, India Abstract Exergy is that the tool, that indicates however suggests that the system departs from equilibrium state. Most of the power plants are designed by the energetic performance criteria supported first law of natural science entirely. The real useful energy loss cannot be even by the first law of natural science, because it cannot differentiate between the quality and quantity of energy. The present study deals with the energy analysis of the power plants. The increasing demand of power has made the power plants of scientific interest, but most of the power plants ar designed by the energetic performance criteria supported first law of natural science entirely. The real useful energy loss cannot be even by the hand law of natural science, because it cannot differentiate between the quality and quantity of energy. Energy analysis presents only quantities results whereas exergy analysis presents qualitative results relating to actual energy consumption. Also presents major losses of out there energy at combustor, superheater, economiser and air-pre heater section. In this article also shown energy efficiency and energy losses comparison charts. This Associate in Nursingalysis provides an completely different prepare to guarantee superior performance of an influence plant. Key words: Power Plant, Energy, Thermodynamics First Law, Efficiency, Exergy I. INTRODUCTION It is the foremost attainable useful work that might be obtained from the system at a given state in fixed atmosphere. The work potential of the energy contained in an passing system at a as state is merely the foremost useful work which is able to be obtained from the system. Work output is maximized once the method between two like states is dead in associate passing reversible manner, as therefore, all the irreversibility s square live overlooked in crucial the work potential. Exergy analysis has sparked interest within the scientific community to need a a lot of in-depth check au courant the energy spoken language devices and to develop new techniques to raised utilize the prevailing restricted resources. First law of physics manage the quantity of energy and asserts that energy cannot be created or destroyed. This law just is a necessary tool for the line of work of energy throughout a technique and offers no challenges to the engineer. The second law, however, deals with the quality of energy. a lot of specifically, it's involved with the degradation of energy throughout a technique, the entropy generation, and also the lost opportunities to strive and work. The second law of physics has tested to be a really powerful tool among the development of sophisticated physics systems. We examine the performance of engineering devices in light-weight of the second law of physics. We begin our discussion with the introduction of exergy (also referred to as availability) that is that the foremost helpful work that may be obtained from the system at a given state in a {very} very given atmosphere, and we continue with the reversible work, that is that the foremost helpful work that will be obtained as a system undergoes a technique between two given state. The exchangeability (also referred to as the exergy destruction or lost work), which is that the wasted work potential throughout a methodology as a results of irreversibilities, and be outlined as second law efficiency. We then develop the exergy balance relation and apply to closed systems and management volumes A. Types of Heat Power Plant: 1) Thermal Power Station: A thermal power station or a coal fired thermal station is far and away, the most conventional technique of generating power with fairly high potency. It uses coal as the primary fuel to boil the water available to superheated steam for driving the turbine. The steam turbine is then automatically coupled to associate generator rotor, the rotation of which results within the generation of electrical power. Generally in Asian country, bituminous coal or wood coal square measure used as fuel of boiler that has volatile content starting from eight to thirty three try to ash content five to Sixteen Personality Factor Questionnaire. To enhance the thermal efficiency of the plant, the coal is used within the boiler in its pulverized kind. 2) Nuclear Power Station: The nuclear power generating stations are just like the thermal stations in additional ways in which than one. However, the exception here is that, radioactive parts like metallic element and metallic element area unit used as the primary fuel in situ of coal. Also in a Nuclear station the chamber and also the boiler area unit replaced by the setup and also the device tubes. For the process of atomic energy generation, the radioactive fuels area unit created to bear fission reaction at intervals the nuclear reactors. The fission reaction, propagates like a controlled chain reaction and is amid unprecedented quantity of energy made, which is manifested in the type of heat. This heat is then transferred to the water present in the device tubes. As a result, superheated steam at very high temperature is made. Once the process of steam formation is accomplished, the remaining process is precisely just like a thermal station, as this steam will more drive the rotary engine blades to generate electricity. 3) Hydro-Electric Power Station: In Hydro-electric plants the energy of the falling water is utilized to drive the rotary engine that successively runs the generator to provide electricity. Rain falling upon the earth s surface has potential energy relative to the oceans towards which it flows. This energy is converted to shaft work wherever the water falls through associate degree considerable vertical distance. This power is utilized for rotating the generator shaft, to convert it to equivalent electrical energy. A vital purpose to be noted is that, the hydro-electric plants are of abundant lower capability compared to their thermal or nuclear counterpart. For this All rights reserved by www.ijsrd.com 2047

reason hydro plants are typically used in programing with thermal stations, to serve the load during peak hours. They in a way assist the thermal or the nuclear plant to deliver power with efficiency during times of peak hours. II. LITERATURE REVIEW Energy will neither be created nor destroyed. It simply changes form such as potential, chemical, power, heat and work. Exergy is that the helpful work potential of the energy. Exergy isn't preserved. Once the exergy is wasted, it will never be recovered. We tend to use energy we don't seem to be destroying any energy; we are just changing it to a less helpful kind, a kind of less exergy. The useful work potential of a system is that the quantity of energy we tend to extract as useful work. The helpful work potential of a system at the desired state is referred to as exergy (also called availableness). Exergy could be a property and is related to the state of the system and therefore the atmosphere. Galal Mohammed Zaki, Rahim Kadhim Jassim, Majed Moalla Alhazmy [1] in YEAR=2011 showed that Gas turbine (GT) power plants operating in arid climates suffer a decrease in output power during the hot summer months because of the high specific volume of air drawn by the compressor. Energy and exergy analysis of a GT Brayton cycle coupled to a refrigeration air cooling unit shows a promise for increasing the output power with a little decrease in thermal efficiency. The performance analysis of the GT shows that the intake air temperature decreases by 12 to 22 K. Power output increase 12.5% & thermal efficiency decrease 8-9% Mali Sanjay, Dr. Mehta [2] in YEAR = 2012 presents energy and exergy analysis method for thermal power plant and analysis carried out on coal base thermal power plant. 47.43% exergy loss occurs in combustor (furnace) which shows combustor is not fully adiabatic. HP and IP turbine have best performance show it tends to adiabatic and LP turbine have poor performance need maintenance. The major energy destruction occurs in the heat recovery system which leads to inefficient heat transfer between hot stream (flue gas) and cold stream (water & air). Karim Maghsoudi, Abdollah Mehrpanahi [3] in Year =2013 showed that exergy and energy analysis of Shahid Rajaee Steam Power plant, located at Km 25 of Karaj- Qazvin road is presented. The highest losses of exergy in the power plant occurred in boiler, which accounted for 87.91% of irreversibility, following by turbine and condenser, which accounted for 6.69% and 2.23% of irreversibility. Thus, it was concluded that to improve efficiency, we should look for a way to reduce irreversibility in boiler, because this component had a high contribution to exergy destruction. ANKUR GEETE & A. I. KHANDWAWALA [4] in Year =2014 analysis different inlet temperature conditions are (1) 507.78 C, (2) 517.78 C, (3) 527.78 C, (4) 537.78 C, (5) 547.78 C, (6) 557.78 C and (7) 567.78 C.Exergy analysis has been done for boiler, for steam turbines for condenser and for feed water heaters with different inlet temperature conditions. When inlet temperature increases then exergy for boiler increases, steam turbine and condenser, feed water decrease Maximum second law efficiency can be achieved at 507.78 C inlet temperature. Ali Mousafarash, Mohammad Ameri [5] in Year = 2013 Exergo-economic analysis of Montazer Ghaem gas turbine power plant which is located near Tehran, capital city of Iran. The highest exergy destruction occurs in the combustion chamber (CC). Load variation reduces exergy efficiency. Ambient temperature increases so the Exergy efficiency decreases. Raviprakash kurkiya, Sharad chaudhary [6] in Year=2012 presented Energy analysis helps designers to find ways to improve the performance of a system in a many way. Most of the conventional energy losses optimization method are iterative in nature and require the interpretation of the designer at each iteration. T. Ganapathy, N. Alagumurthi, R. P.Gakkhar and K.Murugesan [7] inyear = 2009 presented the exergy analysis assesses the energy on quantity as well as the quality. The exergy losses occurred in the various subsystems of the plant and their components have been calculated using the mass, energy and exergy balance equations. The maximum exergy losses of 42.73% occur in the combustor. Exergy analysis results show that over 57% of exergy losses take place within the boiler system. The first law efficiency of the plant is 27%. Mukesh Gupta, Raj Kumar, Bhupender Singh [8] in Year = 2013 analysis. The study points out that the boiler, combustor and turbine are the critical components where maximum exergy losses occur. The first law analysis shows major energy loss has been found to occur in condenser. The second law (Exergy) analysis shows that combustion chamber in both steam and gas turbine thermal power plants are main source of Irreversibility. The Irreversibility in condenser is insignificant, because in the condenser the low quality energy is lost. Sarang j gulhane, Amit kumar Thakur [9] in Year = 2013. The aim of this paper is to be finding out amount and source of irreversibilities gererated in boiler of 35 TPH boiler in 6MW captive power plant. The exergy of feed water Before entering the water into the economizer, the water is allowed to get heated in the deratator thus the temp of feed water is increased to higher temperature. Vosough Amir [10] in Year 2012 presented the useful concept of energy and exergy utilization is analyzed, and applied to the boiler system. Energy and exergy flows in a boiler have been shown in this paper. The energy and exergy efficiencies have been determined as well. In a boiler, the energy and exergy efficiencies are found to be 89.21% and 45.48%, respectively. A boiler energy and exergy efficiencies are compared with others work as well. III. THERMAL POWER PLANT: COMPONANTS A. Turbine: A turbine (from the Latin turbo, a vortex, related to the Greek τύρβη, tyrbē, meaning "turbulence"), is a rotary machine that extracts energy from a fluid flow and converts it into useful work. A turbine is a turbomachine with a minimum of one moving half known as a rotor assembly, which is a shaft or drum with blades hooked up. Moving fluid acts on the blades so that they move and impart move energy to the rotor. Early turbine examples square measure windmills and waterwheels. HPT, IPT, LPT There are three sections to a steam rotary engine viz. high pressure, intermediate pressure and low pressure turbine. All three square measure mounted on the same shaft that rotates at 3600 rate in a very generator All rights reserved by www.ijsrd.com 2048

to form electricity. Here's a simplified steam flow path through HP, IP and L-P turbines. (highlighted red). We can specialise in solely the rotary engine. Forget about condenser and feedwater heaters and boiler for currently. Main steam or live steam as shown above leaves the boiler at concerning one thousand F and 2300 psig and goes to air mass rotary engine (HP) recess. Main steam goes over multistage blades and expands reducing the temperature as it leaves the horsepower. The turbine size is the smallest because the recess steam is beneath air mass requiring lesser volume than expanded steam. Steam leaving the horsepower is known as cold heat (CRH). CRH goes to another section of the boiler called the re-heater. Re-heater heats the CRH back to about one thousand F however at a a lot of lower pressure of four hundred psig compared to main steam/live steam. This steam is called Hot Re-reheat steam (HRH). HRH goes to IP rotary engine recess. Since HRH is at lower pressure than main steam, it occupies larger volume. Hence larger piping, larger turbine is needed to handle the steam flow. IP section of the rotary engine is larger than horsepower rotary engine for this reason. IP rotary engine outlet is connected with one or 2 L-P rotary engine rotors. LP rotary engine more expands the steam generating additional energy. LPs are the biggest in size since they need rock bottom steam pressures therefore need larger space to handle the steam rate. Temperature varies from 1000 F to saturation temperature at the L-P outlet. As the steam expands it becomes wetter and wetter. Wetter steam is harmful for blades. Hence blade style for horsepower, IP and L-P is completely different. Also, thermal expansion of rotary engine shaft, casings prompts more issues. 2) The First Law Efficiency: Energy loss ƞ HPT = 1 m 12 (h 12 h 23 ) + (m 12 m 23 )(h 23 h 13 ) Exergy balance for the HPT W HPT = m 12 (φ 12 φ 23 ) + (m 12 m 23 )(φ 23 φ 13 ) T 0 S gen T 0 S gen = m 12 (φ 12 φ 23 ) + (m 12 m 23 )(φ 23 φ 13 ) W HPT I destroyed = T 0 S gen = m 12 (φ 12 φ 23 ) + (m 12 m 23 )(φ 23 φ 13 ) W HPT 3) The Second Law Efficiency: I destroyed ƞ HPT = 1 m 12 (φ 12 φ 23 ) + (m 12 m 23 )(φ 23 φ 13 ) Fig. 2: B. Intermediate Pressure Turbine: 1) Energy Balance for IPT: W IPT = m 14 (h 14 h 24 ) + (m 14 m 24 )(h 24 h 25 ) + (m 14 m 24 m 25 )(h 25 h 15 ) Energy loss Energy loss = m 14 (h 14 h 24 ) + (m 14 m 24 )(h 24 h 25 ) + (m 14 m 24 m 25 )(h 25 h 15 ) W IPT 2) The First Law Efficiency: Fig. 1: IV. ENERGY & EXERGY ANALYSIS OF VARIOUS PRESSURE TURBINES OF THERMAL POWER PLANT A. High Pressure Turbine: 1) Energy Balance For HPT: W HPT = m 12 (h 12 h 23 ) + (m 12 m 23 )(h 23 h 13 ) Energy loss Energy loss = m 12 (h 12 h 23 ) 3) Exergy Balance for IPT: W IPT = m 14 (φ 14 φ 24 ) + (m 14 m 24 )(φ 24 φ 25 ) + (m 14 m 24 m 25 )(φ 25 φ 15 ) T 0 S gen T 0 S gen = m 14 (φ 14 φ 24 ) + (m 14 m 24 )(φ 24 φ 25 ) + (m 14 m 24 m 25 )(φ 25 φ 15 ) W IPT + (m 12 m 23 )(h 23 h 13 ) W HPT All rights reserved by www.ijsrd.com 2049

I destroyed = T 0 S gen = m 14 (φ 14 φ 24 ) + (m 14 m 24 )(φ 24 φ 25 ) + (m 14 m 24 m 25 )(φ 25 φ 15 ) W IPT 4) The second law efficiency: Fig. 4: Fig. 3: C. Low Pressure Turbine: 1) Energy Balance for LPT: W LPT = m 15 (h 15 h 26 h 27 h 28 ) + (m 15 m 26 m 27 m 28 )(h 26 + h 27 + h 28 h 16 ) Energy loss Energy loss = m 15 (h 15 h 26 h 27 h 28 ) + (m 15 m 26 m 27 m 28 )(h 26 + h 27 + h 28 h 16 ) W LPT 2) The First Law Efficiency: 3) Exergy Balance for The LPT: W LPT = m 15 (φ 15 φ 26 φ 27 φ 28 ) + (m 15 m 26 m 27 m 28 )(φ 26 + φ 27 + φ 28 φ 16 ) T 0 S gen T 0 S gen = m 15 (φ 15 φ 26 φ 27 φ 28 ) + (m 15 m 26 m 27 m 28 )(φ 26 + φ 27 + φ 28 φ 16 ) W LPT I destroyed = T 0 S gen = m 15 (φ 15 φ 26 φ 27 φ 28 ) + (m 15 m 26 m 27 m 28 )(φ 26 + φ 27 + φ 28 φ 16 ) W LPT 4) The Second Law Efficiency: V. RESULTS AND DISCUSSION Thermodynamic Properties of Various Components (Mundra Thermal Power Plant) condition. Ma ss Spe Exer Po Pres flo Enth Entr cific Tempe gy int sure w alpy opy exer rature flow N ( o. (MP rate (kj/ (kj/k gy C) rate a) (to kg) g/k) (kj/ (kw) n/h kg) ) 12 539 13.9 478 345 6.81 143 1903.2 8.5 5 2.99 48.83 13 364 4 434 206 4.47 733. 8847.34 2.36 8 282 0.47 14 539 3.9 434 345 6.81 143 1728.34 8.5 5 2.99 15 307 0.8 396 160 3.71 505..1 7.62 7 32 16 42.7 0.07 336 183. 0.61.3 14 2 6.13 23 382 4.9 44. 306 6.83 102 76 0.4 4 9.23 24 442 1.9 19. 334 7.45 113 82 7.55 3 1.92 25 311.1 0.73 20. 299 945. 6.88 24 0.6 726 26 246 0.54 24. 256 827. 5.86 45 8.86 946 27 156 0.21 18. 248 801. 5.68 36 8.4 126 28 102 0.04 19. 239 5.43 779. 5 26 4.88 8 722 Table 1: Thermodynamic Properties of Various Points (Mundra Thermal Power Plant) The main results of this study are summarized below. Compone nts Energ y loss Irreversibil ity Exerg y loss % ƞ I % 90.24 5559 9.23 572.6 44 1279 6.75 6231. 84 5317. 081 5623. 133 4085. 742 4171. 512 ƞ II % 82.5 85.7 HPT 4479 27153 7.54 2 2 2687. 81.5 84.6 IPT 16291.8 4.52 43 6 1 1791. 80.3 84.7 LPT 6516.72 1.81 6 5 9 Table 2: Exergy and Energy Loss of Various Turbines All rights reserved by www.ijsrd.com 2050

Table 2 shows the energy loss, exergy loss, first law efficiency and second law efficiency of each component in thermal power plant. The result shows that HPT has higher energy loss then other component. LPT has higher exergetic loss Fig. 8: Exergy Efficiency for Various Turbines Fig. 5: Energy Loss of Various Turbines Fig. 6: Exegetic Loss of Various Turbines Fig. 7: Energy Efficiency for Various Turbines VI. CONCLUSIONS Energy and Exergy analysis is presented for various turbines of thermal power plant. Following conclusions are given below 1) Energy & Exergy loss is higher for HPT. 2) Exergetic efficiency is high for HPT about 85.7 % 3) Irreversibility is higher for HPT about 27153 KW and lower for LPT about 6516.72 KW REFERENCES [1] Galal Mohammed Zaki, Rahim Kadhim Jassim, Majed Moalla Alhazmy Energy, Exergy and Thermoeconomics Analysis of Water Chiller Cooler for Gas Turbines Intake Air Cooling May 30, 2011. [2] Mali Sanjay, Dr. Mehta N.S Easy Method Of Exergy Analysis For Thermal Power Plant IJAERS/Vol. I/ Issue III/April-June, 2012/245-247 [3] Karim Maghsoudi, Abdollah Mehrpanahi Energy and Exergy Analysis of 250MW Steam Power Plant Vol. 102, No. 11; November 2013 [4] Ankur Geete & A. I. Khandwawala Exergy Analysis for 120MW Thermal Power Plant With Different Inlet Temperature Conditions IMPACT: IJRET) ISSN(E):2321-8843; ISSN(P): 2347-4599 Vol. 2, Issue 1, Jan 2014, 21-30 [5] Ali Mousafarash, Mohammad Ameri Exergy and exergo-economic based analysis of a gas turbine power generation system Journal of Power Technologies 93 (1) (2013) 44 51 [6] Raviprakash kurkiya, Sharad chaudhary Energy Analysis of Thermal Power Plant International Journal of Scientific & Engineering Research Volume 3, Issue 7, July-2012 1 ISSN 2229-5518 [7] T. Ganapathy, N. Alagumurthi, R. P. Gakkhar and K. Murugesan Exergy Analysis of Operating Lignite Fired Thermal Power Plant Journal of Engineering Science and Technology Review 2 (1) (2009) 123-130 [8] Mukesh Gupta, Raj Kumar, Bhupender Singh Exergy Based Evaluation of Coal Based Thermal Power Plants Volume 3, Special Issue 2, January 2013 All rights reserved by www.ijsrd.com 2051

[9] Sarang j gulhane, Prof.Amit kumar Thakur Exergy Analysis of Boiler In cogeneration Thermal Power Plant American Journal of Engineering Research 2013 [10] Vosough Amir, Improving Steam Power Plant Efficiency Through Exergy Analysis: AmbientTemperature, 2nd International Conference on Mechanical, Production and Automobile Engineering (ICMPAE'2012) Singapore April 28-29, 2012 [11] Yunus A. Cengel, Michael A. Boles Thermodynamics and engineering approach fifth edition [12] P.K. Nag, (2008). Power Plant Engineering, by Tata McGraw-Hill Publishing Company Limited, 7 West Patel Nagar, New Delhi 110 008 All rights reserved by www.ijsrd.com 2052