Number of extra papers used if any

Size: px
Start display at page:

Download "Number of extra papers used if any"

Transcription

1 Last Name: First Name: Thermo no. ME 200 Thermodynamics 1 Fall 2018 Exam Circle your structor s last name Division 1 (7:0): Naik Division (1:0): Wassgren Division 6 (11:0): Sojka Division 2 (9:0): Choi Division 4 (8:0): Holloway Division 7 (2:0): Vuppuluri Number of extra papers used if any Division 8 (12:0): Buckius INSTRUCTIONS Do not remove staples from any page. If you use extra paper, attach it at the end of the exam with a paper clip and dicate above how many extra sheets were attached. Do not write on the back of any page because it will not be scanned so will not be graded. This is a closed book and closed notes exam. Equation sheets and all needed tables are provided. Significant credit for each problem is given if you identify your and its boundary, draw the relevant energy flows on a diagram i.e. Energy Flow Diagram (EFD), start your analysis with the basic equations, list all relevant assumptions, and have appropriate units and use three significant figures. There is no need to re-write the given and fd. Do not hesitate to ask if you do not comprehend a problem statement. For your own benefit, please write clearly and legibly. You must show your work to receive credit for your answers. IMPORTANT NOTE The use of PDAs, Blackberry-type devices, cell phones, laptop computers, smart watches or any other sources of communication (wireless or otherwise) is strictly prohibited durg examations. Dog so is cheatg. If you brg a smart watch, cell phone, or other communication device to the examation, it must be turned off prior to the start of the exam, placed your backpack, and the backpack must be stored below your seat. It shall be reactivated only after you leave the examation room for the fal time. Otherwise it is a form of cheatg and will be treated as such. SECOND IMPORTANT NOTE The only calculators allowed for use on this exam are those of the TI-0X series. No others. 1

2 1. [20 pots] Circle the correct answer (no partial credit) for (a) to (d). (a) [2 pots] For a constant mass, a reversible and adiabatic process is always isentropic. (True or False) (b) [2 pots] For a constant mass, an isentropic process is always reversible and adiabatic. (True or False) (c) [2 pots] At a given temperature, entropy the liquid phase of a substance is always larger than entropy the vapor phase of the same substance. (True or False) (d) [2 pots] Coefficient of performance is always less than one. (True or False) (e) [6 pots] Liquid water, considered as an compressible substance, enters a reversible and adiabatic pump at 0C and flows with negligible changes KE and PE. The pump has one let and one let and operates at steady state. What is the temperature (C) of liquid water at the exit of the pump? Show supportg calculations. ds Q j ms ms generation s s 0 j Tj,boundary T For an compressible substance: s Cln 0 T T T 0 C T (f) [6 pots] An ventor claims that the maximum efficiency of a power cycle operatg between hot and cold reservoirs of temperatures 1000C and 500C, respectively, is equal to 50%. Is this claim possible? (Yes or No) Justify usg an equation. Maximum efficiency for a reversible power cycle: T K C th, rev TH K It is impossible to atta an efficiency of 50% for a power cycle operatg between hot and cold reservoirs of temperatures 1000C and 500C 2

3 2. [40 pots] Air (m = 0.4 ) contaed a piston-cylder device undergoes a constant pressure process at an absolute pressure of 86.5 kpa. The temperature of air changes from 427C to 77C durg the process. Molecular weight of air: /kmol Use the closest value ideal gas table; do not terpolate. (a) Calculate the itial and fal volume of air. Report your answers m. (b) Fd the work durg the process. Report your answer. (c) Determe the heat transfer durg the process. Report your answer. (d) Calculate the total entropy generation for the and its surroundg. Assume a surroundg temperature of 27C. Report your answer /K. Identify appropriate or s, show mass/energy teractions (EFD), list any assumptions and basic equations, and provide your solution. There is no need to re-write the given and fd. System/EFD Assumptions Quasi-equilibrium Ignore KE change Ignore PE change Air behaves as an ideal gas Neglect friction No other work except boundary work Closed m = constant

4 Extra Space for Problem 2 Basic Equations dm m m Integratg: m constant de Q W m h ke pe m h ke pe Integratg: QW U KE PE ds Q j ms m s T Integratg: generation j j,boundary Q S T boundary Solution (a) PV mr T ; air R air 8.14 R kmol-k MW air K kmol Initial volume of air: V Fal volume of air: V mr T K -K air 1 1 P kpa mr T K -K air 1 2 P kpa V1 1m V2 0.5 m (b) Boundary work durg the process: W PdV W P P V V boundary W kpa 0.5 1m W W < 0 work done on the (c) Considerg energy balance for the : Q12 W12 mu2 u Q Q < 0 heat transfer of the 4

5 Extra Space for Problem 2 (d) Considerg entropy balance for the and its surroundg: generation generation Q Q P ms s1 ms2 s1 Rair ln Tboundary Tsurroundg Tboundary Tsurroundg P K generation > 0 irreversible process K 5

6 . [40 pots] A power plant consists of an adiabatic pump, a boiler, an adiabatic turbe, and a condenser. The wor fluid is water/steam, with data at each state provided the table below; all the pressure values are absolute. Q boiler m 2 m W turbe W pump m 1 m Q 1 condenser State P, bar T, C u, / h, / s, /-K P, bar T sat, C u f, / u g, / h f, / h g, / s f, /-K s g, /-K (a) Calculate the isentropic efficiency of the turbe. Report your answer %. (b) Determe the specific heat transfer for the boiler and the condenser. Report your answers /. (c) Fd the specific entropy generation for the entire power cycle. Assume heat transfer occurs to the boiler at a boundary temperature of 500C while heat transfer occurs from the condenser to an environment at a temperature of 0C. Report your answer /-K. (d) Show the cycle on T-s diagram relative to the vapor dome and the relevant les of constant pressure. Label the axes and four states and dicate the process directions with arrows. For water: T critical = 74C, P critical = 221 bar. Identify appropriate or s on the sketch provided, show mass/energy teractions (EFD), list any assumptions and basic equations, and provide your solution. There is no need to re-write the given and fd. m 4 m 4 6

7 Extra Space for Problem Assumptions Steady state, steady flow One-dimensional, uniform flow Ignore KE change Ignore PE change Boiler and condenser: W CV 0 Turbe and pump: Q 0 CV Basic Equations dm m m de ds Q W m h ke pe m h ke pe Q j generation j Tj,boundary ms m s Solution (a) Mass balance for the turbe: m m4 m steam Energy balance for the actual turbe: wactual h h For the isentropic process through the turbe: s s4s K s f,45c < s 4s < s g,45c saturated liquid-vapor mixture s4 s s f,45 C For saturated liquid-vapor mixture: x4s 0.86 s s g,45 C f,45 C h4 h s f,45 C h x s s h4 s h h g,45c f,45c Energy balance for the isentropic turbe: wisentropic h h4s wactual Isentropic efficiency of the turbe: turbe turbe 90% w isentropic

8 Extra Space for Problem (b) Mass balance for the boiler: m2 m m steam Energy balance for the boiler: qboiler h h qboiler 020 q > 0 heat transfer to the Mass balance for the condenser: m4 m1 m steam Energy balance for the condenser: qcondenser h1h qcondenser 2060 q < 0 heat transfer of the (c) Entropy balance for the entire power cycle: qboiler qcondenser cycle T T K 0 27 K boiler condenser cycle K Alternatively Considerg entropy balance for the pump: pump s2 s K Considerg entropy balance for the boiler: 020 qboiler boiler s s Tboiler K -K -K Considerg entropy balance for the turbe: turbe s4 s K Considerg entropy balance for the condenser: 2060 qcondenser condenser s1s Tcondenser 0 27K -K -K Specific entropy generation for the entire heat pump cycle: cycle pump boiler turbe condenser cycle K 8

9 Extra Space for Problem (e) T-s diagram 9

ME 200 Thermodynamics 1 Fall 2017 Exam 3

ME 200 Thermodynamics 1 Fall 2017 Exam 3 ME 200 hermodynamics 1 Fall 2017 Exam Circle your structor s last name Division 1: Naik Division : Wassgren Division 6: Braun Division 2: Sojka Division 4: Goldenste Division 7: Buckius Division 8: Meyer

More information

Circle your instructor s last name

Circle your instructor s last name ME 00 Thermodynamics Fall 07 Exam Circle your structor s last name Division : Naik Division : Wassgren Division 6: Braun Division : Sojka Division 4: Goldenste Division 7: Buckius Division 8: Meyer INSTRUCTIONS

More information

Number of extra papers used if any

Number of extra papers used if any Last Nae: First Nae: Thero no. ME 00 Therodynaics 1 Fall 018 Exa Circle your structor s last nae Diision 1 (7:0): Naik Diision (1:0): Wassgren Diision 6 (11:0): Sojka Diision (9:0): Choi Diision 4 (8:0):

More information

ME 200 Thermodynamics 1 Spring Exam 2

ME 200 Thermodynamics 1 Spring Exam 2 Last Name: First Name: Thermo no. ME 200 Thermodynamics 1 Sprg 2017 - Exam 2 Circle your structor s last name Ardekani Fisher Hess Naik Sojka (onle and on campus) INSTRUCTIONS This is a closed book and

More information

Number of extra papers used if any

Number of extra papers used if any Last Nae: First Nae: Thero no. ME 00 Therodynaics 1 Fall 018 Exa 1 Circle your instructor s last nae Division 1 (7:0): Naik Division (1:0): Wassgren Division 6 (11:0): Sojka Division (9:0): Choi Division

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

ME 200 Final Exam December 14, :00 a.m. to 10:00 a.m.

ME 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 information

ME 200 Thermodynamics 1 Fall 2016 Final Exam

ME 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 information

ME 200 Thermodynamics I, Spring 2015, Exam 3, 8 p.m. to 9 p.m. on April 14, 2015

ME 200 Thermodynamics I, Spring 2015, Exam 3, 8 p.m. to 9 p.m. on April 14, 2015 ME 200 Thermodynamics I, Spring 2015, Exam 3, 8 p.m. to 9 p.m. on April 14, 2015 CIRCLE YOUR LECTURE BELOW: 7:30 a.m. 10:30 a.m. 12:30 p.m. 2:30 p.m. 4:30 p.m. Joglekar Chen Chen Kittel Naik INSTRUCTIONS

More information

ME 200 Exam 2 October 22, :30 p.m. to 7:30 p.m.

ME 200 Exam 2 October 22, :30 p.m. to 7:30 p.m. CIRCLE YOUR LECTURE BELOW: First Name Solution Last Name 7:0 a.m. 8:0 a.m. 10:0 a.m. 11:0 a.m. Boregowda Boregowda Braun Bae :0 p.m. :0 p.m. 4:0 p.m. Meyer Naik Hess ME 00 Exam October, 015 6:0 p.m. to

More information

ME 200 Exam 2 October 16, :30 p.m. to 7:30 p.m.

ME 200 Exam 2 October 16, :30 p.m. to 7:30 p.m. CIRCLE YOUR LECTURE BELOW: First Name Solution Last Name 7:30 am 8:30 am 10:30 am 11:30 am Joglekar Bae Gore Abraham 1:30 pm 3:30 pm 4:30 pm Naik Naik Cheung ME 200 Exam 2 October 16, 2013 6:30 p.m. to

More information

EXAM # 1 CIRCLE YOUR LECTURE BELOW: 8:30 am 11:30 am 2:30 pm Prof. Memon Prof. Naik Prof. Lucht INSTRUCTIONS

EXAM # 1 CIRCLE YOUR LECTURE BELOW: 8:30 am 11:30 am 2:30 pm Prof. Memon Prof. Naik Prof. Lucht INSTRUCTIONS Last Name First Name CIRCLE YOUR LECTURE BELOW: 8: am : am : pm Prof. Memon Prof. Naik Prof. Lucht EXAM # INSTRUCTIONS. This is a closed book examination. An equation sheet and all needed property tables

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

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

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

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

Last Name: First Name: Purdue ID: Please write your name in BLOCK letters. Otherwise Gradescope may not recognize your name.

Last Name: First Name: Purdue ID: Please write your name in BLOCK letters. Otherwise Gradescope may not recognize your name. Solution Key Last Name: First Name: Purdue ID: Please write your name in BLOCK letters. Otherwise Gradescope may not recognize your name. CIRCLE YOUR LECTURE BELOW: MWF 10:30 am MWF 3:30 pm TR 8:30 am

More information

I. (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. 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 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

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

Delft University of Technology DEPARTMENT OF AEROSPACE ENGINEERING

Delft University of Technology DEPARTMENT OF AEROSPACE ENGINEERING Delft University of Technology DEPRTMENT OF EROSPCE ENGINEERING Course: Physics I (E-04) Course year: Date: 7-0-0 Time: 4:00-7:00 Student name and itials (capital letters): Student number:. You have attended

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

ENERGY TRANSFER BY WORK: Electrical Work: When N Coulombs of electrical charge move through a potential difference V

ENERGY TRANSFER BY WORK: Electrical Work: When N Coulombs of electrical charge move through a potential difference V Weight, W = mg Where m=mass, g=gravitational acceleration ENERGY TRANSFER BY WOR: Sign convention: Work done on a system = (+) Work done by a system = (-) Density, ρ = m V kg m 3 Where m=mass, V =Volume

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

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

ECE309 INTRODUCTION TO THERMODYNAMICS & HEAT TRANSFER. 12 June 2006

ECE309 INTRODUCTION TO THERMODYNAMICS & HEAT TRANSFER. 12 June 2006 ECE309 INTRODUCTION TO THERMODYNAMICS & HEAT TRANSFER 1 June 006 Midterm Examination R. Culham This is a hour, closed-book examination. You are permitted to use one 8.5 in. 11 in. crib sheet (one side

More information

Lecture 35: Vapor power systems, Rankine cycle

Lecture 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 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

Previous lecture. Today lecture

Previous lecture. Today lecture Previous lecture ds relations (derive from steady energy balance) Gibb s equations Entropy change in liquid and solid Equations of & v, & P, and P & for steady isentropic process of ideal gas Isentropic

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

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

ECE309 INTRODUCTION TO THERMODYNAMICS & HEAT TRANSFER. 13 June 2007

ECE309 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 information

ME 300 Thermodynamics II

ME 300 Thermodynamics II ME 300 Thermodynamics II Prof. S. H. Frankel Fall 2006 ME 300 Thermodynamics II 1 Week 1 Introduction/Motivation Review Unsteady analysis NEW! ME 300 Thermodynamics II 2 Today s Outline Introductions/motivations

More information

King Fahd University of Petroleum & Minerals

King Fahd University of Petroleum & Minerals King Fahd University of Petroleum & Minerals Mechanical Engineering Thermodynamics ME 04 BY Dr. Haitham Bahaidarah My Office Office Hours: :00 0:00 am SMW 03:00 04:00 pm UT Location: Building Room # 5.4

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

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

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

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

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

Entropy and the Second Law of Thermodynamics

Entropy 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 information

Name: Discussion Section:

Name: Discussion Section: CBE 141: Chemical Engineering Thermodynamics, Spring 2017, UC Berkeley Midterm 2 FORM A March 23, 2017 Time: 80 minutes, closed-book and closed-notes, one-sided 8 ½ x 11 equation sheet allowed Please show

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

ENT 254: Applied Thermodynamics

ENT 254: Applied Thermodynamics ENT 54: Applied Thermodynamics Mr. Azizul bin Mohamad Mechanical Engineering Program School of Mechatronic Engineering Universiti Malaysia Perlis (UniMAP) azizul@unimap.edu.my 019-4747351 04-9798679 Chapter

More information

8:30 am 11:30 am 2:30 pm Prof. Memon Prof. Naik Prof. Lucht

8:30 am 11:30 am 2:30 pm Prof. Memon Prof. Naik Prof. Lucht 1 Last Name First Name CIRCLE YOUR LECTURE BELOW: 8:3 am 11:3 am :3 pm Prof. Memon Prof. Naik Prof. Luht EXAM # 3 INSTRUCTIONS 1. This is a losed book examination. An equation sheet and all needed property

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

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

Course: MECH-341 Thermodynamics II Semester: Fall 2006

Course: 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 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 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

Engineering Thermodynamics. Chapter 6. Entropy: a measure of Disorder 6.1 Introduction

Engineering 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 information

PROBLEM 6.3. Using the appropriate table, determine the indicated property. In each case, locate the state on sketches of the T-v and T-s diagrams.

PROBLEM 6.3. Using the appropriate table, determine the indicated property. In each case, locate the state on sketches of the T-v and T-s diagrams. PROBLEM 63 Using the appropriate table, determine the indicated property In each case, locate the state on sketches of the -v and -s diagrams (a) water at p = 040 bar, h = 147714 kj/kg K Find s, in kj/kg

More information

Lecture 29-30: Closed system entropy balance

Lecture 29-30: Closed system entropy balance ME 200 Thermodynamics I Spring 2016 Lecture 29-30: Closed system entropy balance Yong Li Shanghai Jiao Tong University Institute of Refrigeration and Cryogenics 800 Dong Chuan Road Shanghai, 200240, P.

More information

Find: a) Mass of the air, in kg, b) final temperature of the air, in K, and c) amount of entropy produced, in kj/k.

Find: a) Mass of the air, in kg, b) final temperature of the air, in K, and c) amount of entropy produced, in kj/k. PROBLEM 6.25 Three m 3 of air in a rigid, insulated container fitted with a paddle wheel is initially at 295 K, 200 kpa. The air receives 1546 kj of work from the paddle wheel. Assuming the ideal gas model,

More information

Thermodynamics [ENGR 251] [Lyes KADEM 2007]

Thermodynamics [ENGR 251] [Lyes KADEM 2007] CHAPTER V The first law of thermodynamics is a representation of the conservation of energy. It is a necessary, but not a sufficient, condition for a process to occur. Indeed, no restriction is imposed

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

ME Thermodynamics I = = = 98.3% 1

ME Thermodynamics I = = = 98.3% 1 HW-08 (25 points) i) : a) 1 Since ν f < ν < ν g we conclude the state is a Saturated Liquid-Vapor Mixture (SLVM) 1, from the saturation tables we obtain p 3.6154 bar. 1 Calculating the quality, x: x ν

More information

Name: Discussion Section:

Name: Discussion Section: CBE 141: Chemical Engineering Thermodynamics, Spring 2018, UC Berkeley Midterm 1 February 13, 2018 Time: 80 minutes, closed-book and closed-notes, one-sided 8 ½ x 11 equation sheet allowed Please show

More information

Consequences of Second Law of Thermodynamics. Entropy. Clausius Inequity

Consequences 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 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

Distinguish between an isothermal process and an adiabatic process as applied to an ideal gas (2)

Distinguish between an isothermal process and an adiabatic process as applied to an ideal gas (2) 1. This question is about thermodynamic processes. (a) Distinguish between an isothermal process and an adiabatic process as applied to an ideal gas.......... An ideal gas is held in a container by a moveable

More information

ME Thermodynamics I

ME Thermodynamics I HW-03 (25 points) i) Given: for writing Given, Find, Basic equations Rigid tank containing nitrogen gas in two sections initially separated by a membrane. Find: Initial density (kg/m3) of nitrogen gas

More information

The First Law of Thermodynamics. By: Yidnekachew Messele

The First Law of Thermodynamics. By: Yidnekachew Messele The First Law of Thermodynamics By: Yidnekachew Messele It is the law that relates the various forms of energies for system of different types. It is simply the expression of the conservation of energy

More information

Entropy and the Second Law of Thermodynamics

Entropy and the Second Law of Thermodynamics Entropy and the Second Law of hermodynamics Reading Problems 6-, 6-2, 6-7, 6-8, 6-6-8, 6-87, 7-7-0, 7-2, 7-3 7-39, 7-46, 7-6, 7-89, 7-, 7-22, 7-24, 7-30, 7-55, 7-58 Why do we need another law in thermodynamics?

More information

ME6301- ENGINEERING THERMODYNAMICS UNIT I BASIC CONCEPT AND FIRST LAW PART-A

ME6301- ENGINEERING THERMODYNAMICS UNIT I BASIC CONCEPT AND FIRST LAW PART-A ME6301- ENGINEERING THERMODYNAMICS UNIT I BASIC CONCEPT AND FIRST LAW PART-A 1. What is meant by thermodynamics system? (A/M 2006) Thermodynamics system is defined as any space or matter or group of matter

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 Thermodynamics I

ME 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 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

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

ME 2322 Thermodynamics I PRE-LECTURE Lesson 10 Complete the items below Name:

ME 2322 Thermodynamics I PRE-LECTURE Lesson 10 Complete the items below Name: Lesson 10 1. (5 pt) If P > P sat (T), the phase is a subcooled liquid. 2. (5 pt) if P < P sat (T), the phase is superheated vapor. 3. (5 pt) if T > T sat (P), the phase is superheated vapor. 4. (5 pt)

More information

Thermodynamics Lecture Series

Thermodynamics Lecture Series Thermodynamics Lecture Series Second Law uality of Energy Applied Sciences Education Research Group (ASERG) Faculty of Applied Sciences Universiti Teknologi MARA email: drjjlanita@hotmail.com http://www.uitm.edu.my/faculties/fsg/drjj.html

More information

Consequences of Second Law of Thermodynamics. Entropy. Clausius Inequity

Consequences 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 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

Spring_#8. Thermodynamics. Youngsuk Nam

Spring_#8. Thermodynamics. Youngsuk Nam Spring_#8 Thermodynamics Youngsuk Nam ysnam1@khu.ac.krac kr Ch.7: Entropy Apply the second law of thermodynamics to processes. Define a new property called entropy to quantify the secondlaw effects. Establish

More information

wb Thermodynamics 2 Lecture 9 Energy Conversion Systems

wb Thermodynamics 2 Lecture 9 Energy Conversion Systems wb1224 - Thermodynamics 2 Lecture 9 Energy Conversion Systems Piero Colonna, Lecturer Prepared with the help of Teus van der Stelt 8-12-2010 Delft University of Technology Challenge the future Content

More information

The first law of thermodynamics. U = internal energy. Q = amount of heat energy transfer

The first law of thermodynamics. U = internal energy. Q = amount of heat energy transfer Thermodynamics Investigation of the energy transfer by heat and work and how natural systems behave (Q) Heat transfer of energy due to temp differences. (W) Work transfer of energy through mechanical means.

More information

Ph.D. Qualifying Examination In Thermodynamics

Ph.D. Qualifying Examination In Thermodynamics Ph.D. Qualifying Examination In Thermodynamics May 2014 University of Texas at Austin Department of Chemical Engineering The exam is a closed book examination. There are five equally weighed problems on

More information

KNOWN: Data are provided for a closed system undergoing a process involving work, heat transfer, change in elevation, and change in velocity.

KNOWN: Data are provided for a closed system undergoing a process involving work, heat transfer, change in elevation, and change in velocity. Problem 44 A closed system of mass of 10 kg undergoes a process during which there is energy transfer by work from the system of 0147 kj per kg, an elevation decrease of 50 m, and an increase in velocity

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

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

Unit Workbook 2 - Level 5 ENG U64 Thermofluids 2018 UniCourse Ltd. All Rights Reserved. Sample

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 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

SCHOOL OF COMPUTING, ENGINEERING AND MATHEMATICS SEMESTER 2 EXAMINATIONS 2014/2015 ME258. Thermodynamics

SCHOOL OF COMPUTING, ENGINEERING AND MATHEMATICS SEMESTER 2 EXAMINATIONS 2014/2015 ME258. Thermodynamics s SCHOOL OF COMPUING, ENGINEERING AND MAHEMAICS SEMESER EXAMINAIONS 04/05 ME58 hermodynamics ime allowed: WO hours Answer: Any FOUR Questions Items permitted: Any approved calculator Items supplied: Steam

More information

c Dr. Md. Zahurul Haq (BUET) Entropy ME 203 (2017) 2 / 27 T037

c 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 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

(SP 1) DLLL. Given: In a closed rigid tank,

(SP 1) DLLL. Given: In a closed rigid tank, (SP 1) Given: In a closed rigid tank, State 1: m 1,ice = 1, m 1,g = 0.05 P1= 0.0381 kpa, T1= -30 o C State 2: the liquid vapor equilibrium line, either saturated liquid or saturated vapor Find: (a) The

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

Unified Quiz: Thermodynamics

Unified Quiz: Thermodynamics Fall 004 Unified Quiz: Thermodynamics November 1, 004 Calculators allowed. No books allowed. A list of equations is provided. Put your name on each page of the exam. Read all questions carefully. Do all

More information

PHYSICS 221 Fall 2013 EXAM 2: November 6, :15pm 10:15pm. Name (printed): Recitation Instructor: Section #:

PHYSICS 221 Fall 2013 EXAM 2: November 6, :15pm 10:15pm. Name (printed): Recitation Instructor: Section #: PHYSICS 221 Fall 2013 EXAM 2: November 6, 2013 8:15pm 10:15pm Name (printed): Recitation Instructor: Section #: INSTRUCTIONS: This exam contains 25 multiple choice questions, plus two extra credit questions,

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

+ 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

UNIVERSITY OF SOUTHAMPTON

UNIVERSITY OF SOUTHAMPTON UNIVERSITY OF SOUTHAMPTON PHYS1013W1 SEMESTER 2 EXAMINATION 2014-2015 ENERGY AND MATTER Duration: 120 MINS (2 hours) This paper contains 8 questions. Answers to Section A and Section B must be in separate

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

6-5. H 2 O 200 kpa 200 C Q. Entropy Changes of Pure Substances

6-5. H 2 O 200 kpa 200 C Q. Entropy Changes of Pure Substances Canges f ure Substances 6-0C Yes, because an ternally reversible, adiabatic prcess vlves n irreversibilities r eat transfer. 6- e radiatr f a steam eatg system is itially filled wit supereated steam. e

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

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

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

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

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

Physics 121, April 29, The Second Law of Thermodynamics.

Physics 121, April 29, The Second Law of Thermodynamics. Physics 121, April 29, 2008. The Second Law of Thermodynamics. http://www.horizons.uc.edu/masterjuly1998/oncampus.htm Physics 121. April 29, 2008. Course Information Topics to be discussed today: The Second

More information