RANKINE CYCLE IMPROVISATIONS BY PRABHAKARAN.T AP/MECH

Slides:



Advertisements
Similar presentations
Use of Regeneration in Vapor Power Cycles
Advertisements

Chapter 10 VAPOR AND COMBINED POWER CYCLES
Rankine Cycle Figures from Cengel and Boles, Thermodynamics, An Engineering Approach, 6th ed., McGraw Hill, 2008.
Chapter 10 Vapor and Combined Power Cycles Study Guide in PowerPoint to accompany Thermodynamics: An Engineering Approach, 6th edition by Yunus.
Reading: Cengel & Boles, Chapter 9
Example 1 - Superheat Rankine Cycle
1 Lec 24: Rankine cycle reheat, deviations, efficiency increases, viscosity, introduction to fluid flow.
Vapor and Combined Power Cycles
9 CHAPTER Vapor and Combined Power Cycles.
ENGR 2213 Thermodynamics F. C. Lai School of Aerospace and Mechanical Engineering University of Oklahoma.
Power Generation OBJECTIVE To examine vapor power plants in which the working fluid is vaporized and condensed.
Thermodynamics Lecture Series Applied Sciences Education.
Department of Mechanical Engineering ME 322 – Mechanical Engineering Thermodynamics Lecture 25 Comparison to Carnot’s Heat Engine Effects of Boiling and.
Chapter 1 VAPOR AND COMBINED POWER CYCLES
Reheat cycle.
Vapor Power Cycles Thermodynamics Professor Lee Carkner Lecture 19.
Vapor and Combined Power Cycles
A Vapor Power Cycle Boiler T Turbine Compressor (pump) Heat exchanger
Thermal_Power_Plant_2 Prepared by: NMG
Power Generation Cycles Vapor Power Generation The Rankine Cycle
Chem. Eng. Thermodynamics (TKK-2137) 14/15 Semester 3 Instructor: Rama Oktavian Office Hr.: M.13-15, Tu , W ,
Thermodynamics II Chapter 1 VAPOR POWER CYCLES
Vapor and Combined Power Cycles (2)
Unit 4 Exercise – Gas Vapour and Combined Power Cycle
Energy and the Environment Spring 2014 Instructor: Xiaodong Chu : Office Tel.: Mobile:
A Vapor Power Cycle Boiler T Turbine Compressor (pump) Heat exchanger
STEAM TURBINE POWER CYCLES. The vast majority of electrical generating plants are variations of vapour power plants in which water is the working fluid.
Chapter 10 VAPOR AND COMBINED POWER CYCLES
Analysis of Rankine Cycle with FWHs P M V Subbarao Professor Mechanical Engineering Department I I T Delhi Engineering solution to Pure Thoughts..…..
Chapter 10 Vapor and Combined Power Cycles Study Guide in PowerPoint to accompany Thermodynamics: An Engineering Approach, 7th edition by Yunus.
The Rankine Cycle: An Alternate Ideal Thermodynamic Model P M V Subbarao Professor Mechanical Engineering Department IIT Delhi A Feasible Mathematical.
ENGR 2213 Thermodynamics F. C. Lai School of Aerospace and Mechanical Engineering University of Oklahoma.
ENGR 2213 Thermodynamics F. C. Lai School of Aerospace and Mechanical Engineering University of Oklahoma.
ENGR 2213 Thermodynamics F. C. Lai School of Aerospace and Mechanical Engineering University of Oklahoma.
1 A 英 Consider a regenerative cycle using steam as the workingfluid. Steam leaves the boiler and enters the turbine at 4 MPaand 400 ℃. After expansion.
T s boiler turbine pump work in work out heat out heat in condenser superheated vapor saturated liquid & vapor compressed liquid critical point.
Superheat Rankine Cycle Example Turbine pump condenser Q out Q in W out W in boiler Consider the superheat Rankine power cycle as we analyzed before.
Vapor And Combined Power Cycles Wrocław, Technical Thermodynamics - Lecture 6.
Chapter 10 VAPOR AND COMBINED POWER CYCLES
Chapter 10 VAPOR AND COMBINED POWER CYCLES
Vapor ,Gas and Combined Power Cycles
Objectives Evaluate the performance of gas power cycles for which the working fluid remains a gas throughout the entire cycle. Analyze vapor power.
BRAYTON CYCLE AND EFFECT OF INTERCOOLING , REHEAT AND REGENRATION
COMBINED CYCLE POWER PLANTS BY SELVAN P AP/MECH
SNS COLLEGE OF ENGINEERING Coimbatore-107 Subject: Thermal Engineering
VARIABLE EFFECTING EFFICIENCY OF RANKINE,REHEAT,REGENERATIVE CYCLE
Thermodynamics Cycles.
Lecture Objectives: Answer question related to Project 1 assignment
prepared by Laxmi institute tech. Mechanical eng. Department.
Chapter: 08 POWER CYCLES.
Simple Thermal Power Plant
TOPIC:- VAPOUR CYCLES CREATED BY:
Vapour Power Systems.
Power and Refrigeration Systems
LAXMI INSTITUTE OF TECHNOLOGY
An iso certified institute
VAPOR & COMBINED POWER CYCLES
Power Plant Technology Steam and Gas Cycle Power Plant (Assignment 1)
Power Plant Technology Steam and Gas Cycle Power Plant (Lecture 1)
UNIT IV- Vapour Power Cycles
Chapter 7 Entropy: A Measure of Disorder
Photo Courtesy of GPU International
Chapter 8 Production of Power from Heat.
9 CHAPTER Vapor and Combined Power Cycles.
Chapter 2 Energy Transfer by Heat, Work & Mass
PAL 4/27/12 Air at 7oC enters a turbojet engine at a rate of 16 kg/s and a velocity of 300 m/s (relative to the engine). The air is heated in the combustion.
Lecture Objectives: Finish with Sorption cooling
Cogen, Regen Combined Cycle
Regenerative Rankine Cycle
Presentation transcript:

RANKINE CYCLE IMPROVISATIONS BY PRABHAKARAN.T AP/MECH SNS COLLEGE OF ENGINEERING Coimbatore-107 SUBJECT: Engineering Thermodynamics RANKINE CYCLE IMPROVISATIONS BY PRABHAKARAN.T AP/MECH

Prabhakaran.T, Ap/Mech,Engineering Thermodynamics Guess the cycle?? Prabhakaran.T, Ap/Mech,Engineering Thermodynamics

Prabhakaran.T, Ap/Mech,Engineering Thermodynamics Rankine cycle The Rankine cycle is the fundamental operating cycle of all power plants where an operating fluid is continuously evaporated and condensed. Prabhakaran.T, Ap/Mech,Engineering Thermodynamics

Prabhakaran.T, Ap/Mech,Engineering Thermodynamics In an ideal Rankine cycle, the system executing the cycle undergoes a series of four processes: two isentropic (reversible adiabatic) processes alternated with two isobaric processes: Prabhakaran.T, Ap/Mech,Engineering Thermodynamics

Prabhakaran.T, Ap/Mech,Engineering Thermodynamics Ideal Rankine Cycle Energy analysis: steady flow process, no generation, neglect KE and PE changes for all four devices, 0 = (net heat transfer in) - (net work out) + (net energy flow in) 0 = (qin - qout) - (Wout - Win) + (hin - hout) 1-2: Pump (q=0)  Wpump = h2 - h1 = v(P2-P1) 2-3: Boiler (W=0)  qin = h3 - h2 3-4: Turbine (q=0)  Wout = h3 - h4 4-1: Condenser (W=0)  qout = h4 - h1 T 1 2 3 4 s Thermal efficiency h = Wnet/qin = 1 - qout/qin = 1 - (h4-h1)/(h3-h2) Wnet = Wout - Win = (h3-h4) - (h2-h1) Prabhakaran.T, Ap/Mech,Engineering Thermodynamics

Prabhakaran.T, Ap/Mech,Engineering Thermodynamics Thermal Efficiency Thermal efficiency can be improved by (a) Lowering the condensing pressure (lower condensing temperature, lower TL) (b) Superheating the steam to higher temperature ( c) Increasing the boiler pressure (increase boiler temperature, increase TH) ( c) increase pressure s T 1 2 3 4 T 3 (b) Superheating 2 s T 1 2 4 1 s Low quality, high moisture content (a) lower pressure(temp) Prabhakaran.T, Ap/Mech,Engineering Thermodynamics

Prabhakaran.T, Ap/Mech,Engineering Thermodynamics Reheating The optimal way of increasing the boiler pressure but not increase the moisture content in the exiting vapor is to reheat the vapor after it exits from a first-stage turbine and redirect this reheated vapor into a second turbine. T high-P turbine 5 3 3 high-P turbine Low-P turbine low-P turbine boiler 4 4 5 2 6 1 6 2 pump 1 condenser s Prabhakaran.T, Ap/Mech,Engineering Thermodynamics

Prabhakaran.T, Ap/Mech,Engineering Thermodynamics Reheat Rankine Cycle Reheating allows one to increase the boiler pressure without increasing the moisture content in the vapor exiting from the turbine. By reheating, the averaged temperature of the vapor entering the turbine is increased, thus, it increases the thermal efficiency of the cycle. Multistage reheating is possible but not practical. One major reason is because the vapor exiting will be superheated vapor at higher temperature, thus, decrease the thermal efficiency. Why? Energy analysis: Heat transfer and work output both change qin = qprimary + qreheat = (h3-h2) + (h5-h4) Wout = Wturbine1 + Wturbine2 = (h3-h4) + (h5-h6) Prabhakaran.T, Ap/Mech,Engineering Thermodynamics

Prabhakaran.T, Ap/Mech,Engineering Thermodynamics Types of Reheating Live steam reheating High pressure steam from the boiler is used to heat the steam coming out from the HP turbine. Prabhakaran.T, Ap/Mech,Engineering Thermodynamics

Prabhakaran.T, Ap/Mech,Engineering Thermodynamics Flue gas reheating Flue gas from the boiler is used to heat the steam coming out from the HP turbine. Prabhakaran.T, Ap/Mech,Engineering Thermodynamics

Prabhakaran.T, Ap/Mech,Engineering Thermodynamics Regeneration From 2-2’, the temperature at 2 is very low, therefore, the heat addition process is at a lower temperature and therefore, the thermal efficiency is lower. Why? Use regenerator to heat up the liquid (feedwater) leaving the pump before sending it to the boiler, therefore, increase the averaged temperature (efficiency as well) during heat addition in the boiler. Lower temp heat addition higher temp heat addition 3 5 T T Extract steam from turbine to provide heat source in the regenerator 2’ 4 6 2 3 2 1 7 1 4 s s Use regenerator to heat up the feedwater Prabhakaran.T, Ap/Mech,Engineering Thermodynamics

Prabhakaran.T, Ap/Mech,Engineering Thermodynamics Regenerative Cycle Improve efficiency by increasing feedwater temperature before it enters the boiler. Open feedwater: Mix steam with the feedwater in a mixing chamber. Closed feedwater: No mixing. Open FWH 5 T 5 boiler 4 6 (y) Open FWH 6 7 (y) (1-y) 2 3 (1-y) 3 4 Pump 2 2 1 7 s Pump 1 Prabhakaran.T, Ap/Mech,Engineering Thermodynamics 1 condenser

Prabhakaran.T, Ap/Mech,Engineering Thermodynamics Regenerative Cycle Improve efficiency by increasing feedwater temperature before it enters the boiler. Open feedwater: Mix steam with the feedwater in a mixing chamber. Closed feedwater: No mixing. Open FWH 5 T 5 boiler 4 6 (y) Open FWH 6 7 (y) (1-y) 2 3 (1-y) 3 4 Pump 2 2 1 7 s Pump 1 Prabhakaran.T, Ap/Mech,Engineering Thermodynamics 1 condenser

Prabhakaran.T, Ap/Mech,Engineering Thermodynamics Regenerative Cycle Assume y percent of steam is extracted from the turbine and is directed into open feedwater heater. Energy analysis: qin = h5-h4, qout = (1-y)(h7-h1), Wturbine, out = (h5-h6) + (1-y)(h6-h7) Wpump, in = (1-y)Wpump1 + Wpump2 = (1-y)(h2-h1) + (h4-h3) = (1-y)v1(P2-P1) + v3(P4-P3) In general, the more feedwater heaters, the better the cycle efficiency. Prabhakaran.T, Ap/Mech,Engineering Thermodynamics

Prabhakaran.T, Ap/Mech,Engineering Thermodynamics THANK U Prabhakaran.T, Ap/Mech,Engineering Thermodynamics