: 2017,, : 2017, < Part I > Zero exergy line < Part II > : h-s
|
|
- William Mosley
- 5 years ago
- Views:
Transcription
1 : : 217,, : 217, < Part I > Zero exergy line < Part II > : h-s
2 : 217, 5, : 217, - 1 / 24 -
3 - 2 / 24 - : : 11-1 = 1 Q = m C ΔT 91-9 = 1
4 = + T P A = + = + Q rev = T ΔS δq ds T rev (= ) T A Q : Amount of change T : Change induction factor S : Entropy P B ΔS =Qrev / T Q T B ΔS ΔS Q S T : (Ex, ) P : (Ex, ) - 3 / 24 -
5 - 4 / 24 - : h > h h < h : : T T x = h - h T (s-s ) Exergy Energy Anergy Value Length Area A B < Maximization > Resource conservation Human development Environmental preservation Isentropic process h h Isothermal process T h 1 1 h w t P h P q w c Ideal Gas T (S-S ) s
6 h Air Exergy destruction Exergy exhaust 86% 72% 1 2 Energy Exergy 1% 3 x 2 h 1 1h 2h Anergy h - h = T (s-s ) + x s h Steam HP 5% IP 4% Energy Exergy 5% 3 2 x Zero exergy line 1 Anergy h Zero enthalpy line 1h 2h s - 5 / 24 -
7 - 6 / 24 - h [ Gibbs free energy : T ref ] h 5h 4h 3h e- a- 5 4x+e+ a- e- a- 3 x- T P x- a+ e- x- Most of systems 2 1 e+ a+ 2h 1h x 1 g = h - Ts Δg = Δh - TΔs Δh < & Δs > Δg Δh > & Δs < Δg Δh < & Δs < Δg? Δh > & Δs > Δg? x s
8 Zero exergy line [kj/kg] Ambient enthalpy [kj/kg] Specific Entropy [kj/kg ] / 24 - Temperature [ ]
9 - 8 / Environment Energy Engineering Economy 1) Environment 2) Energy 3) Engineering 1) Energy 2) Economy 3) Engineering 1) Environment 2) Economy 3) Energy
10 - 9 / 24 -
11 - 1 / 24 - : (?) : 1 : 1% : : Sama, Qian Gaggioli(1989) 13 < > , , 6.,., ( ) 9. T , , /
12 Specific Enthalpy [kj/kg] Specific Entropy [kj/kg ] - 11 / 24 - Exergy Ratio [%] Pressure [bar] Specific Enthalpy [kj/kg] Temperature [ ] Temperature [ ] Pressure [bar] Quality [MW] 1 11 Specific Entropy [kj/kg ] 12
13 Specific Entropy [kj/kg ] / Quality - 12 / 24 - Pressure [bar]
14 Temperature [ ] Specific Entropy [kj/kg ] - 13 / 24 - Pressure [bar] Specific Enthalpy [kj/kg] Quality
15 Temperature [ ] Specific Exergy [kj/kg] Exergy Ratio [%] Specific Entropy [kj/kg ] - 14 / 24 - Pressure [bar] Maximum Power Output Maximum Power Efficiency Saturated State Quality
16 Heat Balance Diagram for Plant Performance Design : 32 m [kg/s] P [bar] T [ ] h [kj/kg] Q, W [kj/s] η [%] HP Steam to Power Block Drain Aux. Condensate from Downstream at GSC Aux-Steam Heater Condansate to Power Block Patial Flow to Condenser Make-Up HP SH#3 RH#2 HP SH#2 RH#1 HP SH#1 HP Evap. HP Eco#3 IP SH HP Eco#2 IP Evap. IP Eco LP SH HP Eco#1 LP Evap. CPH To SSR Recirculation Pump CPH Spray MP Steam to Powerblock HP BFP HP BFW at BL MP BFW at BL IP BFP Water to LP Stean 1 & 2 at BL Attemporation FGH To LP Drum Condensate to Gasfication Combustor HP IP LP STG GSC Drain from Process HP Steam Trubine Comp. GTG Partial Make-up Flow Condensate from Anti-Icing Seal & Misc / 24 -
17 h [kj/kg] Q, W [kj/s] ] [bar] 7. HRSG Inlet 4. Combustor η [%] Pressure [ba r] T[ sur e P [bar] 71 HP SH#3 Pre s m [kg/s] 72. RH#2 73. HP SH#2 74. RH#1 6. HP TBN Inlet 75. HP SH#1 65. HRSG RH Outlet 7. IP TBN Inlet Specific Enthalpy [kj/kg] 41. TBN Outlet 7. HRSG Inlet 3. N2 Mixing Specific Enthalpy [kj/kg] 76. HP Drum 2. Compressure 77. HP Eco# RH#1 78. IP SH 1 8. IP Drum 82. LP SH 543. HP SH#1 83. HP Eco#1 85. HRSG Exhaust 84. LP Drum 61. HP TBN Outlet 63. RH#1 Inlet 54. HP Drum Specific Entropy [kj/kg ] Specific Entropy [kj/kg ] Temperature [ ] 81. IP Eco 1. Fuel Inlet 2. N2 Inlet 544. HP SH#2 79. HP Eco#2 11. Fuel FGH 51. HP Eco#3 As a simulation sample at ambinet temperature is IP SH 54. HP Eco#2 43. IP Drum 41. IP Eco 71. IP TBN Outlet 72. LP TBN Inlet 21. HRSG LP Outlet 53. HP Eco# FGH Outlet 51. HP BFP 41. IP BFP 14 LP Drum Inlet 13 CPH Outlet 14 LP Drum Inlet 21. LP Drum 51. HP BFP 41. IP BFP 15 LP Drum 12. GSC Outlet 11. BOP Outlet Green lines are simulation values while the ambient temperature changes from -2 to LP TBN Exhaust 1. Condenser Outlet y alit Qu Specific Enthalpy [kj/kg] 13 CPH Outlet Qu ali ty Temperature [ ] 55. HRSG HP Outlet Specific Entropy [kj/kg ] - 16 / 24 -
18 - 17 / 24 - h Air P h Actual work input (A) Received exergy (D) Isentropic work (B) Loss (C) Exergy destruction (G) 1h 1 1e Recovered exergy (I) 1s T Δs (H) Received exergy (E) x Increased anergy = Exergy destruction (F) P ψ T s
19 h h Air 1 P 2h 2e 2s 2 ψ P T s - 18 / 24 - Loss (C) Actual work input (A) Given exergy (D) Isentropic work (B) 1 2 T Δs (H)
20 - 19 / 24 - h Steam 1 ψ 1 2h 2e 2s 2 2 h T Δs (H) s
21 h h 4 1 ψ s - 2 / 24 - Decreased anergy (C) Received exergy (F) 3x 3 2 3h 1x Given exergy (B) Air Received energy (E) 3 ṁ3 4 2 Given energy (A) 1h ṁ1 1 T Δs (H) T Δs (D)
22 - 21 / 24 - h Air Given energy (A) P 2h 2x Given exergy (B) 2 P 3 Received exergy (F) 1x 1 1h Received energy (E) 2 ψ 3 1 Increased anergy (G) h T Δs (H) T Δs (D) s
23 - 22 / 24 - h Air P P Given energy (A) Given exergy (B) 1 2 2e ψ 1 2 Increased anergy (C) h T Δs (D) s
24 h Steam h ψ s - 23 / 24 - Given exergy (B) Increased anergy (G) = Given energy (A) Decreased anergy (C) 1x T Δs (D)
25 - 24 / 24-6 P=P 1 N O Ar.93 CO2.3 1kg/s bar φ=7% 5 P=P+.1 P=P*1 ηs=88% 1 2 T=T4-2 P=.5% loss Heater 12 3 P=.3% loss 4 P=P+.2 ηs=87% Turbine Pressure [bar] 3 Temperature [ ] Exergy balance Air compressor Heat exchanger Combustion Gas turbine Exhaust gas Ė d = ṁ i ψ i - ṁ o ψ o +Ẇ u η II % % Fuel exergy must be analized % x 2x 4h 4e 4s 4 1h 1e 1s 1 1x 5 3o 4o Exergy zero line [kj/kg] Exergy Ratio [%] 5x 5o Ambient enthalpy [kj/kg] 1o 6 6o 2o Specific Entropy [kj/kg ]
Unit Workbook 2 - Level 5 ENG U64 Thermofluids 2018 UniCourse Ltd. All Rights Reserved. Sample
Pearson BTEC Level 5 Higher Nationals in Engineering (RQF) Unit 64: Thermofluids Unit Workbook 2 in a series of 4 for this unit Learning Outcome 2 Vapour Power Cycles Page 1 of 26 2.1 Power Cycles Unit
More informationME 354 THERMODYNAMICS 2 MIDTERM EXAMINATION. Instructor: R. Culham. Name: Student ID Number: Instructions
ME 354 THERMODYNAMICS 2 MIDTERM EXAMINATION February 14, 2011 5:30 pm - 7:30 pm Instructor: R. Culham Name: Student ID Number: Instructions 1. This is a 2 hour, closed-book examination. 2. Answer all questions
More informationME Thermodynamics I
HW-22 (25 points) Given: 1 A gas power cycle with initial properties as listed on the EFD. The compressor pressure ratio is 25:1 Find: 1 Sketch all the processes on a p-h diagram and calculate the enthalpy,
More informationAvailability and Irreversibility
Availability and Irreversibility 1.0 Overview A critical application of thermodynamics is finding the maximum amount of work that can be extracted from a given energy resource. This calculation forms the
More informationME Thermodynamics I
Homework - Week 01 HW-01 (25 points) Given: 5 Schematic of the solar cell/solar panel Find: 5 Identify the system and the heat/work interactions associated with it. Show the direction of the interactions.
More information374 Exergy Analysis. sys (u u 0 ) + P 0 (v v 0 ) T 0 (s s 0 ) where. e sys = u + ν 2 /2 + gz.
374 Exergy Analysis The value of the exergy of the system depends only on its initial and final state, which is set by the conditions of the environment The term T 0 P S is always positive, and it does
More informationFundamentals of Thermodynamics. Chapter 8. Exergy
Fundamentals of Thermodynamics Chapter 8 Exergy Exergy Availability, available energy Anergy Unavailable energy Irreversible energy, reversible work, and irreversibility Exergy analysis : Pure Thermodynamics
More informationME 200 Final Exam December 14, :00 a.m. to 10:00 a.m.
CIRCLE YOUR LECTURE BELOW: First Name Last Name 7:30 a.m. 8:30 a.m. 10:30 a.m. 11:30 a.m. Boregowda Boregowda Braun Bae 2:30 p.m. 3:30 p.m. 4:30 p.m. Meyer Naik Hess ME 200 Final Exam December 14, 2015
More informationRefrigeration. 05/04/2011 T.Al-Shemmeri 1
Refrigeration is a process of controlled removal of heat from a substance to keep it at a temperature below the ambient condition, often below the freezing point of water (0 O C) 05/04/0 T.Al-Shemmeri
More informationTurbomachinery & Turbulence. Lecture 2: One dimensional thermodynamics.
Turbomachinery & Turbulence. Lecture 2: One dimensional thermodynamics. F. Ravelet Laboratoire DynFluid, Arts et Metiers-ParisTech February 3, 2016 Control volume Global balance equations in open systems
More informationECE309 THERMODYNAMICS & HEAT TRANSFER MIDTERM EXAMINATION. Instructor: R. Culham. Name: Student ID Number:
ECE309 THERMODYNAMICS & HEAT TRANSFER MIDTERM EXAMINATION June 19, 2015 2:30 pm - 4:30 pm Instructor: R. Culham Name: Student ID Number: Instructions 1. This is a 2 hour, closed-book examination. 2. Permitted
More informationI. (20%) Answer the following True (T) or False (F). If false, explain why for full credit.
I. (20%) Answer the following True (T) or False (F). If false, explain why for full credit. Both the Kelvin and Fahrenheit scales are absolute temperature scales. Specific volume, v, is an intensive property,
More informationThe exergy of asystemis the maximum useful work possible during a process that brings the system into equilibrium with aheat reservoir. (4.
Energy Equation Entropy equation in Chapter 4: control mass approach The second law of thermodynamics Availability (exergy) The exergy of asystemis the maximum useful work possible during a process that
More informationSustainable Power Generation Applied Heat and Power Technology. Equations, diagrams and tables
Sustainable Power Generation Applied Heat and Power Technology Equations, diagrams and tables 1 STEAM CYCLE Enthalpy of liquid water h = c p,liquid (T T ref ) T ref = 273 K (normal conditions). The specific
More information20 m neon m propane. g 20. Problems with solutions:
Problems with solutions:. A -m tank is filled with a gas at room temperature 0 C and pressure 00 Kpa. How much mass is there if the gas is a) Air b) Neon, or c) Propane? Given: T7K; P00KPa; M air 9; M
More informationIn the next lecture...
16 1 In the next lecture... Solve problems from Entropy Carnot cycle Exergy Second law efficiency 2 Problem 1 A heat engine receives reversibly 420 kj/cycle of heat from a source at 327 o C and rejects
More informationExisting Resources: Supplemental/reference for students with thermodynamics background and interests:
Existing Resources: Masters, G. (1991) Introduction to Environmental Engineering and Science (Prentice Hall: NJ), pages 15 29. [ Masters_1991_Energy.pdf] Supplemental/reference for students with thermodynamics
More informationLecture 35: Vapor power systems, Rankine cycle
ME 00 Thermodynamics I Spring 015 Lecture 35: Vapor power systems, Rankine cycle Yong Li Shanghai Jiao Tong University Institute of Refrigeration and Cryogenics 800 Dong Chuan Road Shanghai, 0040, P. R.
More informationSPC 407 Sheet 5 - Solution Compressible Flow Rayleigh Flow
SPC 407 Sheet 5 - Solution Compressible Flow Rayleigh Flow 1. Consider subsonic Rayleigh flow of air with a Mach number of 0.92. Heat is now transferred to the fluid and the Mach number increases to 0.95.
More informationME Thermodynamics I. Lecture Notes and Example Problems
ME 227.3 Thermodynamics I Lecture Notes and Example Problems James D. Bugg September 2018 Department of Mechanical Engineering Introduction Part I: Lecture Notes This part contains handout versions of
More informationAn introduction to thermodynamics applied to Organic Rankine Cycles
An introduction to thermodynamics applied to Organic Rankine Cycles By : Sylvain Quoilin PhD Student at the University of Liège November 2008 1 Definition of a few thermodynamic variables 1.1 Main thermodynamics
More informationHeat Integration - Introduction
Heat Integration - Introduction Sub-Topics Design of Heat Exchanger Networks Selection of Utilities Ø Consumption and Production Correct Integration Ø Distillation and Evaporation Ø Heat Pumps Ø Turbines
More informationDishwasher. Heater. Homework Solutions ME Thermodynamics I Spring HW-1 (25 points)
HW-1 (25 points) (a) Given: 1 for writing given, find, EFD, etc., Schematic of a household piping system Find: Identify system and location on the system boundary where the system interacts with the environment
More informationIsentropic Efficiency in Engineering Thermodynamics
June 21, 2010 Isentropic Efficiency in Engineering Thermodynamics Introduction This article is a summary of selected parts of chapters 4, 5 and 6 in the textbook by Moran and Shapiro (2008. The intent
More informationR13. II B. Tech I Semester Regular Examinations, Jan THERMODYNAMICS (Com. to ME, AE, AME) PART- A
SET - 1 II B. Tech I Semester Regular Examinations, Jan - 2015 THERMODYNAMICS (Com. to ME, AE, AME) Time: 3 hours Max. Marks: 70 Note 1. Question Paper consists of two parts (Part-A and Part-B) 2. Answer
More informationChapter 7. Dr Ali Jawarneh. Department of Mechanical Engineering Hashemite University
Chapter 7 ENTROPY Dr Ali Jawarneh Department of Mechanical Engineering Hashemite University Objectives Apply the second law of thermodynamics to processes. Define a new property called entropy to quantify
More informationSUMMARY AND CONCEPTS FOR. Introduction to Engineering Thermodynamics by Sonntag and Borgnakke First edition. Wiley 2001
SUMMARY AND CONCEPTS FOR Introduction to Engineering Thermodynamics by Sonntag and Borgnakke First edition Wiley 2001 This is a collection of end of chapter summaries and main concepts and concept problems
More informationConsequences of Second Law of Thermodynamics. Entropy. Clausius Inequity
onsequences of Second Law of hermodynamics Dr. Md. Zahurul Haq Professor Department of Mechanical Engineering Bangladesh University of Engineering & echnology BUE Dhaka-000, Bangladesh zahurul@me.buet.ac.bd
More informationME 200 Thermodynamics 1 Fall 2016 Final Exam
Last Name: First Name: Thermo no. ME 200 Thermodynamics 1 Fall 2016 Final Exam Circle your instructor s last name Ardekani Bae Fisher olloway Jackson Meyer Sojka INSTRUCTIONS This is a closed book and
More informationChapter 7. Entropy: A Measure of Disorder
Chapter 7 Entropy: A Measure of Disorder Entropy and the Clausius Inequality The second law of thermodynamics leads to the definition of a new property called entropy, a quantitative measure of microscopic
More informationTHERMODYNAMICS, FLUID AND PLANT PROCESSES. The tutorials are drawn from other subjects so the solutions are identified by the appropriate tutorial.
THERMODYNAMICS, FLUID AND PLANT PROCESSES The tutorials are drawn from other subjects so the solutions are identified by the appropriate tutorial. THERMODYNAMICS TUTORIAL 2 THERMODYNAMIC PRINCIPLES SAE
More informationTHE METHOD OF THE WORKING FLUID SELECTION FOR ORGANIC RANKINE CYCLE (ORC) SYSTEM WITH VOLUMETRIC EXPANDER. * Corresponding Author ABSTRACT
Paper ID: 79, Page 1 THE METHOD OF THE WORKING FLUID SELECTION FOR ORGANIC RANKINE CYCLE (ORC) SYSTEM WITH VOLUMETRIC EXPANDER Piotr Kolasiński* 1 1 Wrocław University of Technology, Department of Thermodynamics,
More informationTHERMODYNAMICS NOTES. These notes give a brief overview of engineering thermodynamics. They are based on the thermodynamics text by Black & Hartley.
THERMODYNAMICS NOTES These notes give a brief overview of engineering thermodynamics. They are based on the thermodynamics text by Black & Hartley. Topics covered include: concepts; properties; conservation
More informationME Thermodynamics I
HW-6 (5 points) Given: Carbon dioxide goes through an adiabatic process in a piston-cylinder assembly. provided. Find: Calculate the entropy change for each case: State data is a) Constant specific heats
More informationCourse: MECH-341 Thermodynamics II Semester: Fall 2006
FINAL EXAM Date: Thursday, December 21, 2006, 9 am 12 am Examiner: Prof. E. Timofeev Associate Examiner: Prof. D. Frost READ CAREFULLY BEFORE YOU PROCEED: Course: MECH-341 Thermodynamics II Semester: Fall
More informationConsequences of Second Law of Thermodynamics. Entropy. Clausius Inequity
onsequences of Second Law of hermodynamics Dr. Md. Zahurul Haq Professor Department of Mechanical Engineering Bangladesh University of Engineering & echnology BUE Dhaka-000, Bangladesh zahurul@me.buet.ac.bd
More informationc Dr. Md. Zahurul Haq (BUET) Entropy ME 203 (2017) 2 / 27 T037
onsequences of Second Law of hermodynamics Dr. Md. Zahurul Haq Professor Department of Mechanical Engineering Bangladesh University of Engineering & echnology BUE Dhaka-000, Bangladesh zahurul@me.buet.ac.bd
More information1. (10) Calorically perfect ideal air at 300 K, 100 kpa, 1000 m/s, is brought to rest isentropically. Determine its final temperature.
AME 5053 Intermediate Thermodynamics Examination Prof J M Powers 30 September 0 0 Calorically perfect ideal air at 300 K, 00 kpa, 000 m/s, is brought to rest isentropically Determine its final temperature
More information10. Heat devices: heat engines and refrigerators (Hiroshi Matsuoka)
10 Heat devices: heat engines and refrigerators (Hiroshi Matsuoka) 1 In this chapter we will discuss how heat devices work Heat devices convert heat into work or work into heat and include heat engines
More informationR13 SET - 1 '' ''' '' ' '''' Code No RT21033
SET - 1 II B. Tech I Semester Supplementary Examinations, June - 2015 THERMODYNAMICS (Com. to ME, AE, AME) Time: 3 hours Max. Marks: 70 Note: 1. Question Paper consists of two parts (Part-A and Part-B)
More informationMAE 11. Homework 8: Solutions 11/30/2018
MAE 11 Homework 8: Solutions 11/30/2018 MAE 11 Fall 2018 HW #8 Due: Friday, November 30 (beginning of class at 12:00p) Requirements:: Include T s diagram for all cycles. Also include p v diagrams for Ch
More information+ m B1 = 1. u A1. u B1. - m B1 = V A. /v A = , u B1 + V B. = 5.5 kg => = V tot. Table B.1.
5.6 A rigid tank is divided into two rooms by a membrane, both containing water, shown in Fig. P5.6. Room A is at 200 kpa, v = 0.5 m3/kg, VA = m3, and room B contains 3.5 kg at 0.5 MPa, 400 C. The membrane
More informationEntropy Generation Analysis of Desalination Technologies
Entropy 2011, 13, 1829-1864; doi:10.3390/e13101829 OPEN ACCESS entropy ISSN 1099-4300 www.mdpi.com/journal/entropy Article Entropy Generation Analysis of Desalination Technologies Karan H. Mistry 1, Ronan
More informationChapter 7. Entropy. by Asst.Prof. Dr.Woranee Paengjuntuek and Asst. Prof. Dr.Worarattana Pattaraprakorn
Chapter 7 Entropy by Asst.Prof. Dr.Woranee Paengjuntuek and Asst. Prof. Dr.Worarattana Pattaraprakorn Reference: Cengel, Yunus A. and Michael A. Boles, Thermodynamics: An Engineering Approach, 5th ed.,
More informationReading Problems , 8-34, 8-50, 8-53, , 8-93, 8-103, 8-118, 8-137
Availability Readg Problems 8-1 8-8 8-9, 8-34, 8-50, 8-53, 8-63 8-71, 8-93, 8-103, 8-118, 8-137 Second Law Analysis of Systems AVAILABILITY: the theoretical maximum amount of work that can be obtaed from
More information5/6/ :41 PM. Chapter 6. Using Entropy. Dr. Mohammad Abuhaiba, PE
Chapter 6 Using Entropy 1 2 Chapter Objective Means are introduced for analyzing systems from the 2 nd law perspective as they undergo processes that are not necessarily cycles. Objective: introduce entropy
More information1. Basic state values of matter
1. Basic state values of matter Example 1.1 The pressure inside a boiler is p p = 115.10 5 Pa and p v = 9.44.10 4 Pa inside a condenser. Calculate the absolute pressure inside the boiler and condenser
More informationBasic Thermodynamics Prof. S K Som Department of Mechanical Engineering Indian Institute of Technology, Kharagpur. Lecture - 21 Vapors Power Cycle-II
Basic Thermodynamics Prof. S K Som Department of Mechanical Engineering Indian Institute of Technology, Kharagpur Lecture - 21 Vapors Power Cycle-II Good morning to all of you. Today, we will be continuing
More informationc Dr. Md. Zahurul Haq (BUET) Thermodynamic Processes & Efficiency ME 6101 (2017) 2 / 25 T145 = Q + W cv + i h 2 = h (V2 1 V 2 2)
Thermodynamic Processes & Isentropic Efficiency Dr. Md. Zahurul Haq Professor Department of Mechanical Engineering Bangladesh University of Engineering & Technology (BUET Dhaka-1000, Bangladesh zahurul@me.buet.ac.bd
More informationMARIA COLLEGE OF ENGINEERING AND TECHNOLOGY
MARIA COLLEGE OF ENGINEERING AND TECHNOLOGY ATTOOR ENGINEERING THERMODYNAMICS (TWO MARK QUESTION BANK) UNIT 1 (BASIC COMCEPTS AND FIRST LAW) 1. Define the term thermal engineering. Thermal engineering
More informationfirst law of ThermodyNamics
first law of ThermodyNamics First law of thermodynamics - Principle of conservation of energy - Energy can be neither created nor destroyed Basic statement When any closed system is taken through a cycle,
More informationThermodynamics. For the process to occur under adiabatic conditions, the correct condition is: (iii) q = 0. (iv) = 0
Thermodynamics Choose the correct answer. A thermodynamic state function is a quantity (i) used to determine heat changes (ii) whose value is independent of path (iii) used to determine pressure volume
More informationENGR Thermodynamics
ENGR 224 - hermodynamics #1 - Diagram for a Cascade VCR Cycle (21 ts) Baratuci Final 13-Jun-11 On a full sheet of paper, construct a complete Diagram for the cascade cascade vapor-compression refrigeration
More informationSEM-2017(03HI MECHANICAL ENGINEERING. Paper II. Please read each of the following instructions carefully before attempting questions.
We RoU No. 700095 Candidate should write his/her Roll No. here. Total No. of Questions : 7 No. of Printed Pages : 7 SEM-2017(03HI MECHANICAL ENGINEERING Paper II Time ; 3 Hours ] [ Total Marks : 0 Instructions
More informationToday lecture. 1. Entropy change in an isolated system 2. Exergy
Today lecture 1. Entropy change in an isolated system. Exergy - What is exergy? - Reversible Work & Irreversibility - Second-Law Efficiency - Exergy change of a system For a fixed mass For a flow stream
More informationAME 436. Energy and Propulsion. Lecture 7 Unsteady-flow (reciprocating) engines 2: Using P-V and T-s diagrams
AME 46 Energy and ropulsion Lecture 7 Unsteady-flow (reciprocating) engines : Using - and -s diagrams Outline! Air cycles! What are they?! Why use - and -s diagrams?! Using - and -s diagrams for air cycles!!!!!!
More information5.2. The Rankine Cycle
Figure 5.1. Illustration of a Carnot cycle based on steam in T-S coordinates. The Carnot cycle has a major advantage over other cycles. It operates at the highest temperature available for as long as possible,
More informationTeaching schedule *15 18
Teaching schedule Session *15 18 19 21 22 24 Topics 5. Gas power cycles Basic considerations in the analysis of power cycle; Carnot cycle; Air standard cycle; Reciprocating engines; Otto cycle; Diesel
More informationME 2322 Thermodynamics I PRE-LECTURE Lesson 23 Complete the items below Name:
Lesson 23 1. (10 pt) Write the equation for the thermal efficiency of a Carnot heat engine below: 1 L H 2. (10 pt) Can the thermal efficiency of an actual engine ever exceed that of an equivalent Carnot
More informationTHE FIRST LAW APPLIED TO STEADY FLOW PROCESSES
Chapter 10 THE FIRST LAW APPLIED TO STEADY FLOW PROCESSES It is not the sun to overtake the moon, nor doth the night outstrip theday.theyfloateachinanorbit. The Holy Qur-ān In many engineering applications,
More informationCHEMICAL ENGINEERING THERMODYNAMICS. Andrew S. Rosen
CHEMICAL ENGINEERING THERMODYNAMICS Andrew S. Rosen SYMBOL DICTIONARY 1 TABLE OF CONTENTS Symbol Dictionary... 3 1. Measured Thermodynamic Properties and Other Basic Concepts... 5 1.1 Preliminary Concepts
More informationmodel.lst Thu Jul 05 21:13:
model.lst Thu Jul 05 21:13:36 2018 1 model.lst Thu Jul 05 21:13:36 2018 2 07/05/18 21:13:34 Page 1 C o m p i l a t i o n INCLUDE /var/www/html/interfaces/cgi-bin/steam/ex1.dat 2 Scalars 3 4 AmbT Ambient
More information(1)5. Which of the following equations is always valid for a fixed mass system undergoing an irreversible or reversible process:
Last Name First Name ME 300 Engineering Thermodynamics Exam #2 Spring 2008 March 28, 2008 Form A Note : (i) (ii) (iii) (iv) Closed book, closed notes; one 8.5 x 11 sheet allowed. 60 points total; 60 minutes;
More informationTwo mark questions and answers UNIT II SECOND LAW 1. Define Clausius statement. It is impossible for a self-acting machine working in a cyclic process, to transfer heat from a body at lower temperature
More informationFundamentals of Thermodynamics Applied to Thermal Power Plants
Fundamentals of Thermodynamics Applied to Thermal Power Plants José R. Simões-Moreira Abstract In this chapter it is reviewed the fundamental principles of Thermodynamics aiming at its application to power
More informationME 201 Thermodynamics
ME 0 Thermodynamics Solutions First Law Practice Problems. Consider a balloon that has been blown up inside a building and has been allowed to come to equilibrium with the inside temperature of 5 C and
More information7. Development of the 2nd Law
7-1 7. Development of the 2nd Law 7.1 1st Law Limitations The 1 st Law describes energy accounting. Once we have a process (or string of processes) we can calculate the relevant energy interactions. The
More informationOVERVIEW. Air-Standard Power Cycles (open cycle)
OVERVIEW OWER CYCLE The Rankine Cycle thermal efficiency effects of pressure and temperature Reheat cycle Regenerative cycle Losses and Cogeneration Air-Standard ower Cycles (open cycle) The Brayton cycle
More information10 minutes reading time is allowed for this paper.
EGT1 ENGINEERING TRIPOS PART IB Tuesday 31 May 2016 2 to 4 Paper 4 THERMOFLUID MECHANICS Answer not more than four questions. Answer not more than two questions from each section. All questions carry the
More informationEntropy and the Second Law of Thermodynamics
Entropy and the Second Law of Thermodynamics Reading Problems 7-1 7-3 7-88, 7-131, 7-135 7-6 7-10 8-24, 8-44, 8-46, 8-60, 8-73, 8-99, 8-128, 8-132, 8-1 8-10, 8-13 8-135, 8-148, 8-152, 8-166, 8-168, 8-189
More informationEngineering Thermodynamics
David Ng Summer 2017 Contents 1 July 5, 2017 3 1.1 Thermodynamics................................ 3 2 July 7, 2017 3 2.1 Properties.................................... 3 3 July 10, 2017 4 3.1 Systems.....................................
More informationClass XI Chapter 6 Thermodynamics Chemistry
Class XI Chapter 6 Chemistry Question 6.1: Choose the correct answer. A thermodynamic state function is a quantity (i) used to determine heat changes (ii) whose value is independent of path (iii) used
More informationFirst Law of Thermodynamics
CH2303 Chemical Engineering Thermodynamics I Unit II First Law of Thermodynamics Dr. M. Subramanian 07-July-2011 Associate Professor Department of Chemical Engineering Sri Sivasubramaniya Nadar College
More informationUBMCC11 - THERMODYNAMICS. B.E (Marine Engineering) B 16 BASIC CONCEPTS AND FIRST LAW PART- A
UBMCC11 - THERMODYNAMICS B.E (Marine Engineering) B 16 UNIT I BASIC CONCEPTS AND FIRST LAW PART- A 1. What do you understand by pure substance? 2. Define thermodynamic system. 3. Name the different types
More information3 Energy Exchange in Turbomachines
3 Energy Exchange in Turbomachines Problem 1 The solved and unsolved examples of this chapter are meant to illustrate the various forms of velocity triangles and the variety of the turbomachines. In addition,
More informationCHAPTER 8 THERMODYNAMICS. Common Data For Q. 3 and Q.4. Steam enters an adiabatic turbine operating at steady state with an enthalpy of 3251.
CHAPER 8 HERMODYNAMICS YEAR 0 ONE MARK MCQ 8. MCQ 8. Steam enters an adiabatic turbine operating at steady state with an enthalpy of 35.0 kj/ kg and leaves as a saturated mixture at 5 kpa with quality
More informationEngineering Thermodynamics. Chapter 6. Entropy: a measure of Disorder 6.1 Introduction
Engineering hermodynamics AAi Chapter 6 Entropy: a measure of Disorder 6. Introduction he second law of thermodynamics leads to the definition of a new property called entropy, a quantitative measure of
More informationECE309 INTRODUCTION TO THERMODYNAMICS & HEAT TRANSFER. 20 June 2005
ECE309 INTRODUCTION TO THERMODYNAMICS & HEAT TRANSFER 20 June 2005 Midterm Examination R. Culham & M. Bahrami This is a 90 minute, closed-book examination. You are permitted to use one 8.5 in. 11 in. crib
More informationAnswer Key THERMODYNAMICS TEST (a) 33. (d) 17. (c) 1. (a) 25. (a) 2. (b) 10. (d) 34. (b) 26. (c) 18. (d) 11. (c) 3. (d) 35. (c) 4. (d) 19.
HERMODYNAMICS ES Answer Key. (a) 9. (a) 7. (c) 5. (a). (d). (b) 0. (d) 8. (d) 6. (c) 4. (b). (d). (c) 9. (b) 7. (c) 5. (c) 4. (d). (a) 0. (b) 8. (b) 6. (b) 5. (b). (d). (a) 9. (a) 7. (b) 6. (a) 4. (d).
More informationHow much work is lost in an irreversible turbine?
Exergy, an International Journal 00) 15 158 www.exergyonline.com How much work is lost in an irreversible turbine? H. Struchtrup a,,m.a.rosen b a Department of Mechanical Engineering, University of Victoria,
More informationLecture 44: Review Thermodynamics I
ME 00 Thermodynamics I Lecture 44: Review Thermodynamics I Yong Li Shanghai Jiao Tong University Institute of Refrigeration and Cryogenics 800 Dong Chuan Road Shanghai, 0040, P. R. China Email : liyo@sjtu.edu.cn
More informationSTEADY STATE SIMULATION AND EXERGY ANALYSIS OF SUPERCRITICAL COAL-FIRED POWER PLANT (SCPP) WITH CO 2 CAPTURE
10 th European Conference on Coal Research and its Application () STEADY STATE SIMULATION AND EXERGY ANALYSIS OF SUPERCRITICAL COAL-FIRED POWER PLANT (SCPP) WITH CO 2 CAPTURE Akeem K Olaleye Process and
More informationDepartment of Mechanical Engineering ME 322 Mechanical Engineering Thermodynamics. Lecture 26. Use of Regeneration in Vapor Power Cycles
Department of Mechanical Engineering ME 322 Mechanical Engineering Thermodynamics Lecture 2 Use of Regeneration in Vapor Power Cycles What is Regeneration? Goal of regeneration Reduce the fuel input requirements
More informationProf. Dr.-Ing. F.-K. Benra. ISE batchelor course
University Duisburg-Essen Campus Duisburg Faculty of engineering Science Department of Mechanical Engineering Examination: Fluid Machines Examiner: Prof. Dr.-Ing. F.-K. Benra Date of examination: 06.03.2006
More informationThermal Energy Final Exam Fall 2002
16.050 Thermal Energy Final Exam Fall 2002 Do all eight problems. All problems count the same. 1. A system undergoes a reversible cycle while exchanging heat with three thermal reservoirs, as shown below.
More informationECE309 INTRODUCTION TO THERMODYNAMICS & HEAT TRANSFER. 13 June 2007
ECE309 INTRODUCTION TO THERMODYNAMICS & HEAT TRANSFER 13 June 2007 Midterm Examination R. Culham This is a 2 hour, open-book examination. You are permitted to use: course text book calculator There are
More informationLecture 43: Aircraft Propulsion
Lecture 43: Aircraft Propulsion Turbojet Engine: 1 3 4 fuel in air in exhaust gases Diffuser Compressor Combustor Turbine Nozzle 43.1 T Ideal Ccle: w T,s = w C,s s 1 s w T,s w C,s 3 4 s s Processes: 1:
More informationME 300 Thermodynamics II Spring 2015 Exam 3. Son Jain Lucht 8:30AM 11:30AM 2:30PM
NAME: PUID#: ME 300 Thermodynamics II Spring 05 Exam 3 Circle your section (-5 points for not circling correct section): Son Jain Lucht 8:30AM :30AM :30PM Instructions: This is a closed book/note exam.
More informationThermodynamics II. Week 9
hermodynamics II Week 9 Example Oxygen gas in a piston cylinder at 300K, 00 kpa with volume o. m 3 is compressed in a reversible adiabatic process to a final temperature of 700K. Find the final pressure
More informationMAE 320 HW 7B. 1e. For an isolated system, please circle the parameter which will change with time. (a) Total energy;
MAE 320 HW 7B his comprehensive homework is due Monday, December 5 th, 206. Each problem is worth the points indicated. Copying of the solution from another is not acceptable. Multi-choice, multi-answer
More informationReadings for this homework assignment and upcoming lectures
Homework #3 (group) Tuesday, February 13 by 4:00 pm 5290 exercises (individual) Thursday, February 15 by 4:00 pm extra credit (individual) Thursday, February 15 by 4:00 pm Readings for this homework assignment
More informationSEM-2016(03)-II MECHANICAL ENGINEERING. Paper -11. Please read each of the following instructions carefully before. attempting questions.
Roll No. Candidate should write his/her Roll No. here. Total No. of Questions : 7 No. of Printed Pages : 8 SEM-2016(03)-II MECHANICAL ENGINEERING Paper -11 Time : 3 Hours ] [ Total Marks : 300 Instructions
More informationChapter 1 Introduction and Basic Concepts
Chapter 1 Introduction and Basic Concepts 1-1 Thermodynamics and Energy Application Areas of Thermodynamics 1-2 Importance of Dimensions and Units Some SI and English Units Dimensional Homogeneity Unity
More informationMECA-H-402: Turbomachinery course Axial compressors
MECA-H-40: Turbomachinery course Axial compressors Pr. Patrick Hendrick Aero-Thermo-Mecanics Year 013-014 Contents List of figures iii 1 Axial compressors 1 1.1 Introduction...............................
More informationGestão de Sistemas Energéticos 2017/2018
Gestão de Sistemas Energéticos 2017/2018 Exergy Analysis Prof. Tânia Sousa taniasousa@tecnico.ulisboa.pt Conceptualizing Chemical Exergy C a H b O c enters the control volume at T 0, p 0. O 2 and CO 2,
More informationMME 2010 METALLURGICAL THERMODYNAMICS II. Fundamentals of Thermodynamics for Systems of Constant Composition
MME 2010 METALLURGICAL THERMODYNAMICS II Fundamentals of Thermodynamics for Systems of Constant Composition Thermodynamics addresses two types of problems: 1- Computation of energy difference between two
More informationExcercise: Steam superheating
Steam superheating Excercise: Steam superheating Calculate the efficiency of thermodynamic cycle in optimum working conditions for: a) the system without repeated steam superheating; b) the system with
More informationThermochemistry Chapter 8
Thermochemistry Chapter 8 Thermochemistry First law of thermochemistry: Internal energy of an isolated system is constant; energy cannot be created or destroyed; however, energy can be converted to different
More informationChapter 19. Chemical Thermodynamics. Chemical Thermodynamics
Chapter 19 Enthalpy A thermodynamic quantity that equal to the internal energy of a system plus the product of its volume and pressure exerted on it by its surroundings; Enthalpy is the amount of energy
More informationSummary for TEP 4215 E&P/PI
R S H U Summary for TEP 4215 E&P/PI Reactor System (R) Endothermic vs. Exothermic Reactions Equilibrium vs. Kinetics Temperature Dependence of Equilibrium Constants and Reaction Rates (Arrhenius) Reactors
More information