Application of Viper Energy Recovery Expansion Device in Transcritical Carbon Dioxide Refrigeration Cycle

Size: px
Start display at page:

Download "Application of Viper Energy Recovery Expansion Device in Transcritical Carbon Dioxide Refrigeration Cycle"

Transcription

1 Application of Viper Energy Recovery Expansion Device in Transcritical Carbon Dioxide Refrigeration Cycle Riley Barta, Ph.D. Student PI: Prof. Eckhard A. Groll May 16 th,

2 Overview q Introduction q The Viper Expander q Test Stand Design q Theoretical Analysis q Experimental Results q Conclusions and Future Work 2

3 Overview Goal: Recover expansion energy that is not utilized using traditional expansion valves Motivation: Increase understanding of natural refrigerants and devices that can be used to increase efficiency of refrigeration cycles Method: Utilize the Viper Expander to harness expansion work by moving the expansion process from isenthalpic towards isentropic 3

4 Transcritical CO # Cycle 3 2 q Traditional Expansion Valve: h % = h ' (isenthalpic) 4 1 4

5 Transcritical CO # Cycle 3 2 q Traditional Expansion Valve: h % = h ' (isenthalpic) q Isentropic Expansion h % h ') 4s 4 1 5

6 Transcritical CO # Cycle 3 2 q Traditional Expansion Valve: h % = h ' (isenthalpic) q Isentropic Expansion h % h ') 4s 4v 4 1 q Expansion Through Viper h % h '* More Isentropic Expansion Work from 1 st Law W + Q = m h 6

7 Transcritical CO # Cycle 3 2 q Traditional Expansion Valve: h % = h ' (isenthalpic) q Isentropic Expansion h % h ') 4s 4v 4 1 q Expansion Through Viper h % h '* More Isentropic Expansion Work from 1 st Law W + Q = m h η 3),53678 = h % h '* h % h ') W = m (h % h '* ) 7

8 Literature Review q Yang (2009) - CO 2 Refrigeration System Ø Experimentally tested a double acting rotary vane expander/generator Ø Increased COP by 11 14% q Elbel and Hrnjak (2004) Transcritical CO 2 System Ø Tested a prototype ejector with integrated needle for high-side pressure control Ø Improvements in COP and cooling capacity were 7% and 8%, respectively 8

9 Literature Review q Baek and Groll (2005) Transcritical CO 2 System Ø Tested a piston cylinder expander known as the Expansion Device With Output Work (ED-WOW) Ø Improvement in COP was % q He (2009) R410A Refrigeration System Ø Experimentally tested a Pelton-type expander Ø Improvements in COP and cooling capacity were 6.5% and 5.4%, respectively He (2009) 9

10 Overview q Introduction q The Viper Expander q Test Stand Design q Theoretical Analysis q Experimental Results q Conclusions and Future Work 10

11 The Viper Expander q High pressure refrigerant converted to high-velocity stream imparted on an impeller to spin the generator q Utilize energy released from transition from supercritical into 2-phase region Nozzle Impeller Generator Viper Rectifier Motor (ECM) 11

12 The Viper Expander Flow Direction q Currently, impeller utilizes a Pelton Wheel design q Nozzle is fixed-diameter, designed for mass flow rates attainable with current test setup 12

13 Overview q Introduction q The Viper Expander q Test Stand Design q Theoretical Analysis q Experimental Results q Conclusions and Future Work 13

14 Test Stand Design P Hot-gas Bypass Test Stand Ø Independently control all three parameters surrounding compressor 1. P?3)@AB8C7 2. P EF@G3HI 3. T EF@G3HI h 14

15 Test Stand Design P Hot-gas Bypass Test Stand Viper placed here Ø Control all three parameters surrounding compressor Ø Place Viper in liquid expansion line to simulate realistic operating conditions h 15

16 Test Stand Design P Viper placed here Hot-gas Bypass Test Stand, Mass and Energy Balance m Lh L = m Mh M + m Nh N (1) m L = m M + m N (2) Ø Result: Calculate the mass flow rate through the Viper h 16

17 Test Stand Design 17

18 Overview q Introduction q The Viper Expander q Test Stand Design q Theoretical Analysis q Experimental Results q Conclusions and Future Work 18

19 Theoretical Analysis q Purpose: Understand how expander operating conditions can be simulated in hot-gas bypass test stand q Process: 1. Take design operating conditions 2. Add pressure drop and hot-gas bypass energy and mass balance to model 3. Calculate Viper isentropic efficiency 19

20 Theoretical Results P [kpa] L 7N 4H 5N C 5H 6N 23.5 C p-h, CarbonDioxide, OP4 p Cond C 1H 6H 3N 2H 4N 3H 2N C 2L 3L -0.7 kj/kg-k q 2-stage transcritical CO # cycle q Cycle input into 2 hot-gas bypass stand cycles 1. High-side 2. Low-side 2 x L 8N C Low-Side, "L" High-Side, "H" N. Czapla, "N" h [kj/kg] 9N 1L,N Hot Gas Bypass 6L q Hot-gas bypass and pressure drop shown Ø Predict how well stand can replicate operating conditions 20

21 Theoretical Results From Hot-gas Bypass Valve m N, h N From Liquid Valve m M, h M To Compressor Inlet m L, h L q Parameters of chosen, high-side operating conditions analysis: Ø T TFGUHH8 = 37.8 Ø T YIUHH8 = 1.7 Ø m L = \C ) Ø η 3),]H^687))H8 = 0.7 Ø η 3),53678 = 0.5 q Results: Ø m M = \C ) Ø W = kw Ø COP Improvement of 6.8 % when placed on low-side 21

22 Overview q Introduction q The Viper Expander q Test Stand Design q Theoretical Analysis q Experimental Results q Conclusions and Future Work 22

23 Experimental Results P [kpa] Established Cycle Comparison, mm Nozzle Established Cycle, "e" mm Nozzle, "n" 4e 4n 23.5 C C C 3n C 3e 2n q Testing Method: 2e 1. Establish steadystate cycle with test stand valves 2. Slowly engage Viper, eventually sending 100% of m M through the Viper 3. Adjust superheat to T Eb = 10 ± x C 5n 1n 6n 5e 6e 1e h [kj/kg] 4. Observe Viper outputs, calculate Viper isentropic efficiency 23

24 Experimental Results q m L = 42.0 C ) R744, mm Viper Nozzle C C C q m M = 13.1 C ) q P ef6biu78 = 4489 kpa q W = 11.9 W P [kpa] 23.5 C q Speed = 5790 rpm Ø η is,viper = 6. 5 % C 2 x h [kj/kg] 24

25 Overview q Introduction q The Viper Expander q Test Stand Design q Theoretical Analysis q Experimental Results q Conclusions and Future Work 25

26 Conclusions and Future Work q Test stand is reaching desired operating conditions q Experimental isentropic efficiency is lower than theoretically assumed q Pelton wheel design is not optimal for these operating conditions with CO # Ø Turbine re-design being pursued q Nozzle design is also in question, and further design efforts are being pursued 26

27 Questions? Thank You 27

Choked Flow Characteristics of Subcritical Refrigerant Flowing Through Converging-Diverging Nozzles

Choked Flow Characteristics of Subcritical Refrigerant Flowing Through Converging-Diverging Nozzles Entropy 2014, 16, 5810-5821; doi:10.3390/e16115810 Article OPEN ACCESS entropy ISSN 1099-4300 www.mdpi.com/journal/entropy Choked Flow Characteristics of Subcritical Refrigerant Flowing Through Converging-Diverging

More information

R13 SET - 1 '' ''' '' ' '''' Code No RT21033

R13 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 information

5/6/ :41 PM. Chapter 6. Using Entropy. Dr. Mohammad Abuhaiba, PE

5/6/ :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 information

20 m neon m propane. g 20. Problems with solutions:

20 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 information

Week 8. Steady Flow Engineering Devices. GENESYS Laboratory

Week 8. Steady Flow Engineering Devices. GENESYS Laboratory Week 8. Steady Flow Engineering Devices Objectives 1. Solve energy balance problems for common steady-flow devices such as nozzles, compressors, turbines, throttling valves, mixers, heaters, and heat exchangers

More information

SEM-2017(03HI MECHANICAL ENGINEERING. Paper II. Please read each of the following instructions carefully before attempting questions.

SEM-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 information

CHAPTER 5 MASS AND ENERGY ANALYSIS OF CONTROL VOLUMES

CHAPTER 5 MASS AND ENERGY ANALYSIS OF CONTROL VOLUMES Thermodynamics: An Engineering Approach 8th Edition in SI Units Yunus A. Çengel, Michael A. Boles McGraw-Hill, 2015 CHAPTER 5 MASS AND ENERGY ANALYSIS OF CONTROL VOLUMES Lecture slides by Dr. Fawzi Elfghi

More information

Chapter 5. Mass and Energy Analysis of Control Volumes. by Asst. Prof. Dr.Woranee Paengjuntuek and Asst. Prof. Dr.Worarattana Pattaraprakorn

Chapter 5. Mass and Energy Analysis of Control Volumes. by Asst. Prof. Dr.Woranee Paengjuntuek and Asst. Prof. Dr.Worarattana Pattaraprakorn Chapter 5 Mass and Energy Analysis of Control Volumes by Asst. Prof. Dr.Woranee Paengjuntuek and Asst. Prof. Dr.Worarattana Pattaraprakorn Reference: Cengel, Yunus A. and Michael A. Boles, Thermodynamics:

More information

MAE 11. Homework 8: Solutions 11/30/2018

MAE 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

c 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)

c 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 information

Content. Entropy and principle of increasing entropy. Change of entropy in an ideal gas.

Content. Entropy and principle of increasing entropy. Change of entropy in an ideal gas. Entropy Content Entropy and principle of increasing entropy. Change of entropy in an ideal gas. Entropy Entropy can be viewed as a measure of molecular disorder, or molecular randomness. As a system becomes

More information

Lecture 44: Review Thermodynamics I

Lecture 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 information

CHAPTER INTRODUCTION AND BASIC PRINCIPLES. (Tutorial). Determine if the following properties of the system are intensive or extensive properties: Property Intensive Extensive Volume Density Conductivity

More information

CHAPTER 7 ENTROPY. Copyright Hany A. Al-Ansary and S. I. Abdel-Khalik (2014) 1

CHAPTER 7 ENTROPY. Copyright Hany A. Al-Ansary and S. I. Abdel-Khalik (2014) 1 CHAPTER 7 ENTROPY S. I. Abdel-Khalik (2014) 1 ENTROPY The Clausius Inequality The Clausius inequality states that for for all cycles, reversible or irreversible, engines or refrigerators: For internally-reversible

More information

THE VAPOR COMPRESSION REFRIGERATION PROCESS

THE VAPOR COMPRESSION REFRIGERATION PROCESS SUSTAINABLE ENERGY UTILIZATION - COMPUTER LAB 2 SEU-CL2 THE VAPOR COMPRESSION REFRIGERATION PROCESS OBJECTIVES The primary objective of this computer lab is to develop a simple model of the vapour compression

More information

Lecture 38: Vapor-compression refrigeration systems

Lecture 38: Vapor-compression refrigeration systems ME 200 Termodynamics I Lecture 38: Vapor-compression refrigeration systems Yong Li Sangai Jiao Tong University Institute of Refrigeration and Cryogenics 800 Dong Cuan Road Sangai, 200240, P. R. Cina Email

More information

MAE 320 HW 7B. 1e. For an isolated system, please circle the parameter which will change with time. (a) Total energy;

MAE 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 information

ME 354 THERMODYNAMICS 2 MIDTERM EXAMINATION. Instructor: R. Culham. Name: Student ID Number: Instructions

ME 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 information

In the next lecture...

In 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 information

ME Thermodynamics I. Lecture Notes and Example Problems

ME 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 information

Pure Substances Phase Change, Property Tables and Diagrams

Pure Substances Phase Change, Property Tables and Diagrams Pure Substances Phase Change, Property Tables and Diagrams In this chapter we consider the property values and relationships of a pure substance (such as water) which can exist in three phases - solid,

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.

+ 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 information

THE METHOD OF THE WORKING FLUID SELECTION FOR ORGANIC RANKINE CYCLE (ORC) SYSTEM WITH VOLUMETRIC EXPANDER. * Corresponding Author ABSTRACT

THE 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 information

BME-A PREVIOUS YEAR QUESTIONS

BME-A PREVIOUS YEAR QUESTIONS BME-A PREVIOUS YEAR QUESTIONS CREDITS CHANGE ACCHA HAI TEAM UNIT-1 Introduction: Introduction to Thermodynamics, Concepts of systems, control volume, state, properties, equilibrium, quasi-static process,

More information

Introduction to Chemical Engineering Thermodynamics. Chapter 7. KFUPM Housam Binous CHE 303

Introduction to Chemical Engineering Thermodynamics. Chapter 7. KFUPM Housam Binous CHE 303 Introduction to Chemical Engineering Thermodynamics Chapter 7 1 Thermodynamics of flow is based on mass, energy and entropy balances Fluid mechanics encompasses the above balances and conservation of momentum

More information

Name: I have observed the honor code and have neither given nor received aid on this exam.

Name: I have observed the honor code and have neither given nor received aid on this exam. ME 235 FINAL EXAM, ecember 16, 2011 K. Kurabayashi and. Siegel, ME ept. Exam Rules: Open Book and one page of notes allowed. There are 4 problems. Solve each problem on a separate page. Name: I have observed

More information

Readings for this homework assignment and upcoming lectures

Readings 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 information

ME 200 Final Exam December 12, :00 a.m. to 10:00 a.m.

ME 200 Final Exam December 12, :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. 1:30 p.m. 3:30 p.m. Mongia Abraham Sojka Bae Naik ME 200 Final Exam December 12, 2011 8:00 a.m. to 10:00 a.m. INSTRUCTIONS

More information

Chapter 5. Mass and Energy Analysis of Control Volumes

Chapter 5. Mass and Energy Analysis of Control Volumes Chapter 5 Mass and Energy Analysis of Control Volumes Conservation Principles for Control volumes The conservation of mass and the conservation of energy principles for open systems (or control volumes)

More information

Chapter 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 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 information

The exergy of asystemis the maximum useful work possible during a process that brings the system into equilibrium with aheat reservoir. (4.

The 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 information

THE FIRST LAW APPLIED TO STEADY FLOW PROCESSES

THE 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 information

Characteristics of CO2 Transcritical Expansion Process

Characteristics of CO2 Transcritical Expansion Process Purdue University Purdue e-pubs International Refrigeration and Air Conditioning Conference School of Mechanical Engineering 1 Characteristics of CO Transcritical Expansion Process Mitsuhiro Fukuta tmmfuku@ipc.shizuoka.ac.jp

More information

Chemical Engineering Thermodynamics Spring 2002

Chemical Engineering Thermodynamics Spring 2002 10.213 Chemical Engineering Thermodynamics Spring 2002 Test 2 Solution Problem 1 (35 points) High pressure steam (stream 1) at a rate of 1000 kg/h initially at 3.5 MPa and 350 ºC is expanded in a turbine

More information

ME 316: Thermofluids Laboratory

ME 316: Thermofluids Laboratory ME 316 Thermofluid Laboratory 6.1 KING FAHD UNIVERSITY OF PETROLEUM & MINERALS ME 316: Thermofluids Laboratory PELTON IMPULSE TURBINE 1) OBJECTIVES a) To introduce the operational principle of an impulse

More information

ME Thermodynamics I

ME 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 information

Thermodynamic Analysis of the Effect of Generator Temperature on the Performance of a Single-Effect Absorption Refrigeration Cycle

Thermodynamic Analysis of the Effect of Generator Temperature on the Performance of a Single-Effect Absorption Refrigeration Cycle Thermodynamic Analysis of the Effect of Generator Temperature on the Performance of a Single-Effect Absorption Refrigeration Cycle Abstract Debendra Nath Sarkar 1, Dipankar Narayan Basu 2 1 UG 4 th Year

More information

Two mark questions and answers UNIT I BASIC CONCEPT AND FIRST LAW SVCET

Two mark questions and answers UNIT I BASIC CONCEPT AND FIRST LAW SVCET Two mark questions and answers UNIT I BASIC CONCEPT AND FIRST LAW 1. What do you understand by pure substance? A pure substance is defined as one that is homogeneous and invariable in chemical composition

More information

Chapter Four fluid flow mass, energy, Bernoulli and momentum

Chapter Four fluid flow mass, energy, Bernoulli and momentum 4-1Conservation of Mass Principle Consider a control volume of arbitrary shape, as shown in Fig (4-1). Figure (4-1): the differential control volume and differential control volume (Total mass entering

More information

Dishwasher. Heater. Homework Solutions ME Thermodynamics I Spring HW-1 (25 points)

Dishwasher. 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 information

Chapter 6. Using Entropy

Chapter 6. Using Entropy Chapter 6 Using Entropy Learning Outcomes Demonstrate understanding of key concepts related to entropy and the second law... including entropy transfer, entropy production, and the increase in entropy

More information

ME 300 Thermodynamics II Spring 2015 Exam 3. Son Jain Lucht 8:30AM 11:30AM 2:30PM

ME 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 information

Two 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 information

Refrigeration. 05/04/2011 T.Al-Shemmeri 1

Refrigeration. 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 information

ME 201 Thermodynamics

ME 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 information

CHAPTER 8 ENTROPY. Blank

CHAPTER 8 ENTROPY. Blank CHAPER 8 ENROPY Blank SONNAG/BORGNAKKE SUDY PROBLEM 8-8. A heat engine efficiency from the inequality of Clausius Consider an actual heat engine with efficiency of η working between reservoirs at and L.

More information

1. (10) Calorically perfect ideal air at 300 K, 100 kpa, 1000 m/s, is brought to rest isentropically. Determine its final temperature.

1. (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 information

1 st Law Analysis of Control Volume (open system) Chapter 6

1 st Law Analysis of Control Volume (open system) Chapter 6 1 st Law Analysis of Control Volume (open system) Chapter 6 In chapter 5, we did 1st law analysis for a control mass (closed system). In this chapter the analysis of the 1st law will be on a control volume

More information

Engineering Thermodynamics Solutions Manual

Engineering Thermodynamics Solutions Manual Engineering Thermodynamics Solutions Manual Prof. T.T. Al-Shemmeri Download free books at Prof. T.T. Al-Shemmeri Engineering Thermodynamics Solutions Manual 2 2012 Prof. T.T. Al-Shemmeri & bookboon.com

More information

ECE309 THERMODYNAMICS & HEAT TRANSFER MIDTERM EXAMINATION. Instructor: R. Culham. Name: Student ID Number:

ECE309 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 information

Chapter 7. Entropy: A Measure of Disorder

Chapter 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 information

first law of ThermodyNamics

first 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 information

ME 2322 Thermodynamics I PRE-LECTURE Lesson 23 Complete the items below Name:

ME 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 information

Spring_#7. Thermodynamics. Youngsuk Nam.

Spring_#7. Thermodynamics. Youngsuk Nam. Spring_#7 Thermodynamics Youngsuk Nam ysnam1@khu.ac.kr You can t connect the dots looking forward; you can only connect them looking backwards. So you have to trust that the dots will somehow connect in

More information

UBMCC11 - THERMODYNAMICS. B.E (Marine Engineering) B 16 BASIC CONCEPTS AND FIRST LAW PART- A

UBMCC11 - 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 information

(1)5. Which of the following equations is always valid for a fixed mass system undergoing an irreversible or reversible process:

(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 information

ECE309 INTRODUCTION TO THERMODYNAMICS & HEAT TRANSFER. 20 June 2005

ECE309 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 information

Availability and Irreversibility

Availability 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 information

Thermodynamics is the Science of Energy and Entropy

Thermodynamics is the Science of Energy and Entropy Definition of Thermodynamics: Thermodynamics is the Science of Energy and Entropy - Some definitions. - The zeroth law. - Properties of pure substances. - Ideal gas law. - Entropy and the second law. Some

More information

Applied Fluid Mechanics

Applied Fluid Mechanics Applied Fluid Mechanics 1. The Nature of Fluid and the Study of Fluid Mechanics 2. Viscosity of Fluid 3. Pressure Measurement 4. Forces Due to Static Fluid 5. Buoyancy and Stability 6. Flow of Fluid and

More information

Version 001 HW 15 Thermodynamics C&J sizemore (21301jtsizemore) 1

Version 001 HW 15 Thermodynamics C&J sizemore (21301jtsizemore) 1 Version 001 HW 15 Thermodynamics C&J sizemore 21301jtsizemore 1 This print-out should have 38 questions. Multiple-choice questions may continue on the next column or page find all choices before answering.

More information

3 Energy Exchange in Turbomachines

3 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 information

An introduction to thermodynamics applied to Organic Rankine Cycles

An 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 information

ENGR Thermodynamics

ENGR 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 information

Thermodynamic Cycles

Thermodynamic Cycles Thermodynamic Cycles Content Thermodynamic Cycles Carnot Cycle Otto Cycle Rankine Cycle Refrigeration Cycle Thermodynamic Cycles Carnot Cycle Derivation of the Carnot Cycle Efficiency Otto Cycle Otto Cycle

More information

Introduction to Engineering thermodynamics 2 nd Edition, Sonntag and Borgnakke. Solution manual

Introduction to Engineering thermodynamics 2 nd Edition, Sonntag and Borgnakke. Solution manual Introduction to Engineering thermodynamics 2 nd Edition, Sonntag and Borgnakke Solution manual Chapter 6 Claus Borgnakke The picture is a false color thermal image of the space shuttle s main engine. The

More information

QUESTION BANK UNIT-1 INTRODUCTION. 2. State zeroth law of thermodynamics? Write its importance in thermodynamics.

QUESTION BANK UNIT-1 INTRODUCTION. 2. State zeroth law of thermodynamics? Write its importance in thermodynamics. QUESTION BANK UNIT-1 INTRODUCTION 1. What do you mean by thermodynamic equilibrium? How does it differ from thermal equilibrium? [05 Marks, June-2015] 2. State zeroth law of thermodynamics? Write its importance

More information

TOLERANCES AND UNCERTAINTIES IN PERFORMANCE DATA OF REFRIGERANT COMPRESSORS JANUARY 2017

TOLERANCES AND UNCERTAINTIES IN PERFORMANCE DATA OF REFRIGERANT COMPRESSORS JANUARY 2017 TOLERANCES AND UNCERTAINTIES IN PERFORMANCE DATA OF REFRIGERANT COMPRESSORS JANUARY 017 111 Wilson Blvd, Suite 500 Arlington, Virginia 01 USA +001 (703) 54-8800 Published by: TABLE OF CONTENTS SECTION

More information

MAHALAKSHMI ENGINEERING COLLEGE

MAHALAKSHMI ENGINEERING COLLEGE MAHALAKSHMI ENGINEERING COLLEGE TIRUCHIRAPALLI-621213. Department: Mechanical Subject Code: ME2202 U N IT - 1 Semester: III Subject Name: ENGG. THERMODYNAMICS 1. 1 kg of gas at 1.1 bar, 27 o C is compressed

More information

Pumped Thermal Exergy Storage Past, Present and Future

Pumped Thermal Exergy Storage Past, Present and Future Pumped Thermal Exergy Storage Past, Present and Future Alexander White Josh McTigue, Pau Farres-Antunez, Haobai Xue Caroline Willich, Christos Markides (Imperial), Chris Dent (Durham) Department of Engineering

More information

Earlier Topics. Introduction to Cryogenic Engineering An introductory knowledge of Cryogenic Engineering.

Earlier Topics. Introduction to Cryogenic Engineering An introductory knowledge of Cryogenic Engineering. 8 1 Earlier Topics Introduction to Cryogenic Engineering An introductory knowledge of Cryogenic Engineering. Properties of Cryogenic Fluids Properties of Cryogens, T s diagram, Hydrogen, Helium. Properties

More information

1. INTRODUCTION TO REFRIGERATION AND AIR CONDITION

1. INTRODUCTION TO REFRIGERATION AND AIR CONDITION CHAPTER ONE 1. INTRODUCTION TO REFRIGERATION AND AIR CONDITION Refrigeration may be defined as the process of reducing and maintaining a temperature of a space or material below that of the surroundings.

More information

Feasibility Study of Replacing Steam Ejector with Liquid Ring Vacuum Pump (LRVP) in 210 MW Plant of Vijayawada Thermal Power Station (V.T.P.

Feasibility Study of Replacing Steam Ejector with Liquid Ring Vacuum Pump (LRVP) in 210 MW Plant of Vijayawada Thermal Power Station (V.T.P. Feasibility Study of Replacing Steam Ejector with Liquid Ring Vacuum Pump (LRVP) in 210 MW Plant of Vijayawada Thermal Power Station (V.T.P.S) V.SAIRAM M.Tech student, Department of Mechanical Engineering

More information

Classification following properties of the system in Intensive and Extensive

Classification following properties of the system in Intensive and Extensive Unit I Classification following properties of the system in Intensive and Extensive Extensive : mass, weight, volume, potential energy, Kinetic energy, Internal energy, entropy, exergy, energy, magnetization

More information

FINAL EXAM. ME 200 Thermodynamics I, Spring 2013 CIRCLE YOUR LECTURE BELOW:

FINAL EXAM. ME 200 Thermodynamics I, Spring 2013 CIRCLE YOUR LECTURE BELOW: ME 200 Thermodynamics I, Spring 2013 CIRCLE YOUR LECTURE BELOW: Div. 5 7:30 am Div. 2 10:30 am Div. 4 12:30 am Prof. Naik Prof. Braun Prof. Bae Div. 3 2:30 pm Div. 1 4:30 pm Div. 6 4:30 pm Prof. Chen Prof.

More information

CENTRIFUGAL PUMP SELECTION, SIZING, AND INTERPRETATION OF PERFORMANCE CURVES

CENTRIFUGAL PUMP SELECTION, SIZING, AND INTERPRETATION OF PERFORMANCE CURVES CENTRIFUGAL PUMP SELECTION, SIZING, AND INTERPRETATION OF PERFORMANCE CURVES 4.0 PUMP CLASSES Pumps may be classified in two general types, dynamic and positive displacement. Positive displacement pumps

More information

CLASS Fourth Units (Second part)

CLASS Fourth Units (Second part) CLASS Fourth Units (Second part) Energy analysis of closed systems Copyright The McGraw-Hill Companies, Inc. Permission required for reproduction or display. MOVING BOUNDARY WORK Moving boundary work (P

More information

THERMODYNAMICS, 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, 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 information

Chapter 5: The First Law of Thermodynamics: Closed Systems

Chapter 5: The First Law of Thermodynamics: Closed Systems Chapter 5: The First Law of Thermodynamics: Closed Systems The first law of thermodynamics can be simply stated as follows: during an interaction between a system and its surroundings, the amount of energy

More information

7. Development of the 2nd Law

7. 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 information

SATHYABAMA UNIVERISTY. Unit III

SATHYABAMA UNIVERISTY. Unit III Unit III UNIT III STEAM NOZZLES AND TURBINES Flow of steam through nozzles, shapes of nozzles, effect of friction, critical pressure ratio,supersaturated flow.impulse and reaction principles, compounding,

More information

Thermodynamics of solids 5. Unary systems. Kwangheon Park Kyung Hee University Department of Nuclear Engineering

Thermodynamics of solids 5. Unary systems. Kwangheon Park Kyung Hee University Department of Nuclear Engineering Thermodynamics of solids 5. Unary systems Kwangheon ark Kyung Hee University Department of Nuclear Engineering 5.1. Unary heterogeneous system definition Unary system: one component system. Unary heterogeneous

More information

First Law of Thermodynamics

First 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 information

Hydraulic Turbines. Table 6.1 Parameters of hydraulic turbines. Power P (kw) Speed N (rpm)

Hydraulic Turbines. Table 6.1 Parameters of hydraulic turbines. Power P (kw) Speed N (rpm) 6 Hydraulic Turbines Problem 1 There are 10 solved examples and 7 exercise problems (exclude Problems 1, 2, and 10) in this chapter. Prepare a table to mention the values of all the parameters, such as

More information

Where F1 is the force and dl1 is the infinitesimal displacement, but F1 = p1a1

Where F1 is the force and dl1 is the infinitesimal displacement, but F1 = p1a1 In order to force the fluid to flow across the boundary of the system against a pressure p1, work is done on the boundary of the system. The amount of work done is dw = - F1.dl1, Where F1 is the force

More information

Performance Comparison in Retrofit

Performance Comparison in Retrofit Influence of Heat Transfer Fluid Conditions in an Evaporator on Refrigerant Performance Comparison in Retrofit (Part 2: Evaporator) Influence of Heat Transfer Fluid Conditions in an Evaporator on Refrigerant

More information

To receive full credit all work must be clearly provided. Please use units in all answers.

To receive full credit all work must be clearly provided. Please use units in all answers. Exam is Open Textbook, Open Class Notes, Computers can be used (Computer limited to class notes, lectures, homework, book material, calculator, conversion utilities, etc. No searching for similar problems

More information

Chapter 8. The increased awareness that the world s energy EXERGY: A MEASURE OF WORK POTENTIAL. Objectives

Chapter 8. The increased awareness that the world s energy EXERGY: A MEASURE OF WORK POTENTIAL. Objectives Chapter 8 EXERGY: A MEASURE OF WORK POTENTIAL The increased awareness that the world s energy resources are limited has caused many countries to reexamine their energy policies and take drastic measures

More information

SHRI RAMSWAROOP MEMORIAL COLLEGE OF ENGG. & MANAGEMENT

SHRI RAMSWAROOP MEMORIAL COLLEGE OF ENGG. & MANAGEMENT B.Tech. [SEM III (ME-31, 32, 33,34,35 & 36)] QUIZ TEST-1 Time: 1 Hour THERMODYNAMICS Max. Marks: 30 (EME-303) Note: Attempt All Questions. Q1) 2 kg of an ideal gas is compressed adiabatically from pressure

More information

Thermodynamics II. Week 9

Thermodynamics 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 information

UNIT I Basic concepts and Work & Heat Transfer

UNIT I Basic concepts and Work & Heat Transfer SIDDHARTH GROUP OF INSTITUTIONS :: PUTTUR Siddharth Nagar, Narayanavanam Road 517583 QUESTION BANK (DESCRIPTIVE) Subject with Code: Engineering Thermodynamics (16ME307) Year & Sem: II-B. Tech & II-Sem

More information

Teaching schedule *15 18

Teaching 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 information

FUNDAMENTAL THERMO-ECONOMIC APPROACH TO SELECTING SCO2 POWER CYCLES FOR CSP APPLICATIONS

FUNDAMENTAL THERMO-ECONOMIC APPROACH TO SELECTING SCO2 POWER CYCLES FOR CSP APPLICATIONS FUNDAMENTAL THERMO-ECONOMIC APPROACH TO SELECTING SCO2 POWER CYCLES FOR CSP APPLICATIONS F. Crespi, D. Sánchez, J.M. Rodríguez, G. Gavagnin, Department of Energy Engineering University of Seville (Spain)

More information

EXAM # 1 ME 300 SP2017

EXAM # 1 ME 300 SP2017 CIRCLE YOUR LECTURE BELOW: 8:3 am :3 am 3:3 pm Prof. Lucht Prof. Chen Prof. Goldenstein EXAM # ME 3 SP7 INSTRUCTIONS. Please place all your electronics, including but not limited to cell phones, computers,

More information

Unified Quiz: Thermodynamics

Unified Quiz: Thermodynamics Unified Quiz: Thermodynamics October 14, 2005 Calculators allowed. No books or notes allowed. A list of equations is provided. Put your ID number on each page of the exam. Read all questions carefully.

More information

R13. II B. Tech I Semester Regular Examinations, Jan THERMODYNAMICS (Com. to ME, AE, AME) PART- A

R13. 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 information

ME 300 Thermodynamics II Exam 1 September 27, :00 p.m. 9:00 p.m.

ME 300 Thermodynamics II Exam 1 September 27, :00 p.m. 9:00 p.m. ME 00 Thermodynamics II Exam 1 September 7, 01 8:00 p.m. 9:00 p.m. Name: Solution Section (Circle One): Sojka Naik 11:0 a.m. 1:0 p.m. Instructions: This is a closed book/notes exam. You may use a calculator.

More information

Exergy and the Dead State

Exergy and the Dead State EXERGY The energy content of the universe is constant, just as its mass content is. Yet at times of crisis we are bombarded with speeches and articles on how to conserve energy. As engineers, we know that

More information

CHAPTER EIGHT P U M P I N G O F L I Q U I D S

CHAPTER EIGHT P U M P I N G O F L I Q U I D S CHAPTER EIGHT P U M P I N G O F L I Q U I D S Pupmps are devices for supplying energy or head to a flowing liquid in order to overcome head losses due to friction and also if necessary, to raise liquid

More information

The Otto Cycle. Presented by: Jason Rako, Mike Nee and Ralph Spolander

The Otto Cycle. Presented by: Jason Rako, Mike Nee and Ralph Spolander The Otto Cycle Presented by: Jason Rako, Mike Nee and Ralph Spolander Our Agenda A brief history of Nicolaus Otto The Otto Engine The Otto Cycle Explained Formulas to Calculate an Otto Cycle Critical Error

More information