Gas Power Systems Nick DiFilippo. Spark Ignition Compression Ignition Compression Ratio.

Slides:



Advertisements
Similar presentations
Department of Mechanical Engineering ME 322 – Mechanical Engineering Thermodynamics Review for Exam 3.
Advertisements

EGR 334 Thermodynamics Chapter 9: Sections 3-4 Lecture 32: Gas Power Systems: The Diesel Cycle Quiz Today?
Problem Ideal and Actual Gas-Turbine (Brayton) Cycles 9–73
Copyright © 2011 by Oxford University Press, Inc. Energy and the Environment James A. Fay / Dan S. Golomb FIGURE 3.4 The Otto cycle comprises two isentropic.
Gas Power Cycles Cengel & Boles, Chapter 8 ME 152.
GAS POWER CYCLES Chapter 9. Introduction Two important areas of application for thermodynamics are power generation and refrigeration. Two important areas.
Energy Conversion CHE 450/550. Ideal Gas Basics and Heat Capacities - I Ideal gas: – a theoretical gas composed of a set of non-interacting point particles.
Diesel / Brayton Cycles
CHAPTER 9 Gas Power Cycles.
Thermodynamics Professor Lee Carkner Lecture 18
Ideal Cycles, Air-Standard Assumptions, and The Otto Cycle
Dr Roger Bennett Rm. 23 Xtn Directed Reading.
Lec 22: Diesel cycle, Brayton cycle
GAS TURBINE POWER PLANTS
For next time: Read: § 8-6 to 8-7 HW11 due Wednesday, November 12, 2003 Outline: Isentropic efficiency Air standard cycle Otto cycle Important points:
MAE431-Energy System Presentation
Applied Thermodynamics
Microturbines Recuperator Exhaust Natural Gas Air Combustion Chamber
EGR 334 Thermodynamics Chapter 9: Sections 7-8
INTERNAL COMBUSTION ENGINES (reciprocating). Geometry.
Thermodynamic Cycles Air-standard analysis is a simplification of the real cycle that includes the following assumptions: 1) Working fluid consists of.
ENGR 2213 Thermodynamics F. C. Lai School of Aerospace and Mechanical Engineering University of Oklahoma.
Department of Mechanical Engineering ME 322 – Mechanical Engineering Thermodynamics Lecture 27 Gas Power Generation The Brayton Cycle.
EGR 334 Thermodynamics Chapter 9: Sections 5-6
Thermodynamic Cycles for CI engines In early CI engines the fuel was injected when the piston reached TC and thus combustion lasted well into the expansion.
Chapter 9 GAS POWER CYCLES
Gas Power Cycle - Jet Propulsion Technology, A Case Study
8 CHAPTER Gas Power Cycles.
Gas Power Cycles.
CHAPTER 8 Gas Power Cycles. Copyright © The McGraw-Hill Companies, Inc. Permission required for reproduction or display. 8-1 FIGURE 8-1 Modeling is a.
chapter 8 Gas Power Cycle 8-1 The Analysis of a Cycle The average temperature of a process We define: That is: 1 2 T s s1s1 s2s2 T.
Chapter10 Refrigeration Cycle 10-1 Vapor-Compression Cycle The Reversed Carnot Cycle T s THTH TLTL Coefficient of Performance.
CHAPTER 9 GAS POWER CYCLES
The Diesel Cycle By Marcus Low. What is the difference? The Diesel engine takes in JUST air. The compression ratio is higher, thus higher efficiency.
Thermodynamic Cycles for CI engines
GAS TURBINE POWER PLANT
ENGR 2213 Thermodynamics F. C. Lai School of Aerospace and Mechanical Engineering University of Oklahoma.
TEKNIK PERMESINAN KAPAL II (Minggu – 3) LS 1329 ( 3 SKS) Jurusan Teknik Sistem Perkapalan ITS Surabaya.
Chapter 9 GAS POWER CYCLES
Chapter 9 Gas Power Cycles Study Guide in PowerPoint to accompany Thermodynamics: An Engineering Approach, 8th edition by Yunus A. Çengel and Michael.
MT 313 IC ENGINES LECTURE NO: 04 (24 Feb, 2014) Khurram Yahoo Group Address: ICE14.
Chapter 9 POWER AND REFRIGERATION CYCLES
ChemE 260 The Brayton Power Cycle and Variations
ENGINES, REFRIGERATORS, AND HEAT PUMPS This lecture highlights aspects in Chapters 9,10,11 of Cengel and Boles. Every thermodynamic device has moving parts.
ENGINES, REFRIGERATORS, AND HEAT PUMPS This lecture highlights aspects in Chapters 9,10,11 of Cengel and Boles. Every thermodynamic device has moving parts.
A pplied Thermodynamics Air Standard Power Cycles Introduction Two important applications of thermodynamics are power generation and refrigeration.
Diesel Cycle and the Brayton Cycle Chapter 9b. Rudolph Diesel  German inventor who is famous for the development of the diesel engine  The diesel engine.
Mechanical Engineering Department C. Prapti Mahandari What is Thermodynamics.
MT 313 IC ENGINES LECTURE NO: 03 (19 Feb, 2014) Khurram Yahoo Group Address: ICE14.
Wind Turbine Power Plant. Sources ●
Cycles  A series of processes which return a system to its initial state  Heat engine: receives heat; does work  Reversed cycle: cool or heat when work.
8. GAS POWER CYCLES. Objectives Evaluate the performance of gas power cycles for which the working fluid remains a gas throughout the entire cycle. Develop.
THERMODYNAMICS CYCLES RELATED TO POWER PLANTS
Basic Mechanical Engineering, First Edition by Dr Pravin Kumar Copyright © 2013 Dorling Kindersley (India) Pvt. Ltd. Chapter 6 Internal Combustion Engines.
Prepared by, Brijrajsinh Sarvaiya(13ME548) Jaypalsinh Jadeja(13ME517) Pradipsinh Jadeja(13ME518) Virendrasinh Parmar(13ME539) Gas power cycle.
Brayton cycle with intercooling and reheating HARIKISHNAN PILLAI ENGG THERMODYNAMICS.
Real Heat Engines Stirling heat engine
Gas Power Cycles.
A. Diesel cycle : The ideal cycle for CI engines
SNS COLLEGE OF ENGINEERING THERMAL ENGINEERING
Chapter 9 GAS POWER CYCLES
BRAYTON CYCLE AND EFFECT OF INTERCOOLING , REHEAT AND REGENRATION
THERMAL ENGINEERING SYSTEMS
Date of download: 12/28/2017 Copyright © ASME. All rights reserved.
GAS TURBINE POWER PLANT
Dual Fuel Engines.
Gas Power Cycle - Internal Combustion Engine
Engineering Thermodynamics ME-103
Copyright © John Wiley & Sons Ltd.
Lec 28: Final Review.
Presentation transcript:

Gas Power Systems Nick DiFilippo

Spark Ignition Compression Ignition Compression Ratio

Air Standard Otto Cycle Q Q Q Q

Air Standard Diesel Cycle Q Q Q Q Cold air standard Air standard

Comparison of Otto and Diesel Cycle

Air Standard Dual Cycle Q Q Q Q Q Q

Gas Turbine Power Plants

Air Standard Brayton Cycle

Actual Gas Turbine

T1 = 300K h1 = kJ/kg Pr1 = State 1 T2s = 540K h2s = kJ/kg State 2s State 3 T3 = 1300K h3 = kJ/kg Pr3 = T4s = 720.2K h4s = kJ/kg State 4s

Brayton With Regeneration T4>T2

T1 = 300K h1 = kJ/kg Pr1 = State 1 T2s = 540K h2s = kJ/kg State 2s State 3 T3 = 1300K h3 = kJ/kg Pr3 = T4s = 720.2K h4s = kJ/kg State 4s State 2State 4 T4 = 853K h4 = kJ/kg T2 = 598K h2 = kJ/kg

Brayton with Intercooling, Reheating and Regeneration Reheat