d dt T R m n p 1. (A) 4. (4) Carnot engine T Refrigerating effect W COPref. = 1 4 kw 5. (A)

Size: px
Start display at page:

Download "d dt T R m n p 1. (A) 4. (4) Carnot engine T Refrigerating effect W COPref. = 1 4 kw 5. (A)"

Transcription

1 . (A). (C) 5. (C) 7. ( to 5) 9. (C) 6. (C). (C). (D) 6. (A) 8. (0.6 to 0.66) 50. (D) 6. (C). (A) 5. (C) 7. (A) 9. (C) 5. (D) 6. (C). () 6. (C) 8. (600) 0. (D) 5. (B) 6. (D) 5. (A) 7. (A) 9. (D). (C) 5. (A) 65. (D) 6. (C) 8. (C) 0. (C). (9 to ) 5. (D) 7. (D) 9. (A). (B). (.9 to.) 55. (A) 8. (5.8 to 5.9) 0. (B, C). ( to ). (0. to 0.6) 56. (C) 9. (D). (D). (B) 5. (A) 57. (B) 0. (A). (B). (D) 6. (0.88 to 0.9) 58. (D). (C). (A) 5. (A) 7. (88 to 9) 59. (C). (C). (B) 6. (C) 8. (50 to 5) 60. (D). (A) Carnot engine E d d c Similarly, d d c d d d c d c Hence decreasing has a higher eiciency.. (C). (A) (Note sign indicates only direction) at constant temperature ranserring units to zero ealuated cells ater reaching optimality gies an alternatie solution with the same transportation cost to the problem. I artiicial ariable which does not hae any physical signiicance is in solution then it is ineasible.. () 5. (A) 6. (C) 7. (D) COre. COH 5 Rerigerating eect COre. = k For minimizing mean tardiness EDD rule is used, or minimizing aerage in process inentory S rule is used. 8. (5.86 [5.8 to 5.9]) 9. (D) 0. (A). (C) x x 5.86 In a regeneratie steam cycle, a part o steam is extracted rom the turbine and utilized to heat up condensate. So temperature at which eed water is supplied in boiler is high. As a result aerage heat addition temperature o steam is increased whereas aerage heat rejection temperature is same so oerall gape between aerage heat addition temperature and aerage heat rejection temperature increase, thereore, thermal eiciency o cycle increases. As we hae less amount o steam remaining in steam turbine at lower stages, the work output will decreases. Rerigerant nomenclature is gien as R m n p where m is number o carbon atoms

2 and. (C). (C). (D) 5. (C) 6. (C) 7. (A) 8. (C) 9. (A) n is number o hydrogen atoms p is number o luorine atoms R can be written as R0 thereore m 0 m and p Number o clorine atom = = C H F CHFCl emperature can be increased by supplying heat or by doing work. Extent o irreersibility o any process is determined by the entropy increase o the unierse. he mixture o air and liquid air is not a pure substance, because the relatie proportions o oxygen and nitrogen dier in gas and liquid phases in equilibrium. Extent o irreersibility o any process is determined by the entropy increase o the unierse. he exergy o a closed system is either positie or zero. (C) cannot be the alue o exergy. 0. (B, C). (D). (B). (A) n n Maximum useul work in a closed system U E E S S V V On rearrangement 0 0 U E S E S V V et Vapour Increase CO (B) 5. (C) 6. (A) 7. (A) Aboe the Critical emperature Increase the CO Ammonia is toxic in nature Since electrical energy is high grade energy and heat is low grade energy. In 00K is gien to electric heater it would conert whole 00K into work to perorm the task but i 00K is gien to hearth it can not conert 00K to work 00K to work. In the context o question exergy input to electrical heater is more than exergy input to the hearth but exergy output is same. Hence second law eiciency o hearth is more than second law eiciency o electric heater. So rom the aboe reason we can conclude that electrical heater is more irreersible. 8. (600) Loss in aailable energy = Irreersibility I 0 S 00 uni (D) 0. (C) I 600kJ Reheating S Rankine cycle with Reheating 7 06K 7 7K C R - C Q For Carnot Rerigerator Q=.6 k

3 . (B) Q CO k 00 Heat lost by hot water mc p mc p hot water C K S S sys+ S gen S S = Heat gained by cold water surr cold water S 0, surr sys gen perect insulation mc ln mc ln i i.8 ln.8 ln 0 5. J / K. ( [ to ]) Johnson's rule says to identiy the shortest processing time. I it is at the irst work center, place (the entire) job as early as possible. I it is at second work centre, place the job as late as possible. Eliminate that job rom urther consideration and apply the decision rule to the remaining jobs. Following the algorithm, we get B E D A C he sequential times are as ollows. B E D A C Baking Decoration 9 Job Baking Decoration In Out In Out B 0 E 0 D A C 0 So, the minimum total elapsed time or optimum sequence in hours is.. (B). (D) Applying st law o thermodynamics or closed system Q U Q mc d kJ Actual work =.6kJ Reersible work == change in aailable energy U U S S 0 here, S S mc ln Reersible work kJ State- 500 C 600ka State- 90ka ln 7 0 For highest possible elocity at nozzle exit, system, must be reersible. S gen 0 S S C p ln R ln ln.07 ln S S S S gen sur system gen ln.07 ln K 89.7C Now steady low energy equation between & is h h C 5. (A) V 000 C V 000 V C 000 V 06 m / s

4 By steady low energy equation or unit mass Q = heat transerred per unit mass. = work done per unit mass 5 bar bar Q dq ds (i) O (m /kg) ds dh dp Q h h dp (ii) From equation (i) & (ii) 6. (C) V dp V Now dp = Area under - cure projected on axis kj / kg V V j / kg 7 kj / kg 7 kj / kg kj / kg (by compressor) dq du + d dq 0 d 0 du 0 mcd 0 constant (insulated) (ree expansion) V S C ln R ln V Air S R ln V constant V V V h Q h R ln 0.87 ln 0.98 kj / kg. K Membrane 7. (. [ to 5]) From st law o thermodynamics Q U F.B.D. o piston A mg A o o A i A where, Inside air pressure i o o i Outside air pressure Outside air pressure A 0. Soling, we get 90.5a i ia oa mg ork done by gas in raising piston by 0. m J Q U U J 8. (0.65[ ]) 9. (C) For imum work min 00 Brayton Cycle min 00 Carnot Now Brayton Cycle Carnot For imum work engine should be reersible Q Q Q 0K K II law 0. (D) actual 00 II law 00 8% 80 Gien: dq 0.8 kj / s dt d 0. kj / s dt 500K HE Q 00K 600 kj/s

5 . (C) otal heat transer in 0 min dq 0 60 kj kJ dt otal work done in 0 min d kJ dt Applying irst law o thermodynamics or closed system. dq d du mc i C ME ork done per cycle stroke olume V V V V. (0 [9 to ]) m i.e. B I F I I d I I 00 k I B I F k Brake power 80 pth 0% Heat supplied 00. (.06 [.9 to.]) Speciic humidity 0.6 because air is saturated] t is negatie.7ka kg o water apor/kg o dry air otal mass o water apour = =.06 kg. (0.5 [0. to 0.6]) ' ' h h h x h h h u p Now, h c p s mass o dry air c ( p is small or liquid phase) Similarly h ' c 5. (A) c.5 55 x 0.5 h 0 g eaporator K 57.7C (0.9 [0.88 to 0.9]) 0.6 atm a.065. ka 0.6 Rs Ra a atm artial pressure o air a a s atm m / kg d. a 7. (90.5 [88 to 9]) From data gien h 9.5 kj / kg hs 89. kj / kg h 07. kj / kg compressor s c h s h h h actual

6 s h h s h h comp kj / kg Condenser load in / = = 90.5 kj 8. (50.8 [50 to 5]) s kj kg h h 5C.698ka sat sat sat ; ka speciic humidity kg Vap kg dry air h enthalpy o air sts C p h a c C g p kj / kg dry air Vc / n Vs /.5 V V (D) V 58cm Now, V V cm Now olumetric eiciency, V V % V 000 s Combustion equation can be written as: C H ao.76an CO O CO x 5. (D) y Equating moles or Nitrogen.76a 8 a.00 8N bh O Oxygen.00 b b.0 Carbon x Hydrogen y b.0 Gien equation becomes CH Z x 5x Z 0,0 0 x (0,5) (0,) 9. (C) Vs 000cm V Vc 0.05 Vs 00cm n n V V Z 0 0, ,0,0,0 5 x

7 Z x 5. (B) /5, , x Z In case o degenerate solution one o the decision ariable will get zero alue and one o the constraint becomes redundant type howeer it is ully consumed or utilized. Z x 0x Statement: x 6x 8 x x 8 x ; x 0 x, x 6 optimal 0,9 0,8 x x x 8 Z x 0x,6 Z C x C x x C Z x C C y mx c C slope, m C,0 x 9,0 x 6x 8 Slope o the objectie unction 0 Slope o constraint 6 Slope o constraint C C C 0 Fix C 0 C ; C (A) C ; 0 C 0 Range o alues o coeicient Cast matrix is to be minimized x 6.67 to Row ransaction Column ransaction (D) H F F Solution = =9 No. o lines = No. o rows so, solution is optimal are Houses Supply 00- F F F Demand he eect o this on transportation cost is 55. (A) 56. (C) 57. (B) 58. (D) ransport cost increases by `. Aerage in-process inentory = (5 jobs st hour + jobs nd hour + jobs rd hour + jobs 5 th hour + job 5 th hour)/( ) AI. 5 5 ankaj SE 5 km 0 km ankaj

8 59. (C) 60. (D) 6. (C) 6. (C) otal age o students and principals is 5 5 = 75 Ater excluding the principal's age, the total age o students become = 6 age o principal = 75 6 age o principal = 75 6 = 9 A V S...() A V 9 V S 8 A V S 7...() Equation () () gies V now, A 5 5 Salary o A is 59 5 he ratio o the number o coins is : : or the 50 paise and `.50 coins, respectiely. In terms o monetary alue, the ratio becomes 0.5 : 0.5 :.5 hich equals 0.5 : 0.5 :.5 or :: 9 th o the total alues comes rom 5 paise coins (i.e.) 6600 = `600 is in the orm o 5 paise otal number o 5 paise coins he basic diagram or the gien statements is Females Football players = Ground Males From the aboe basic diagram Choice (a), does not ollow Choice (b), does not ollow Choice (c), ollow Choice (d), not Hence, option (c) is correct (A + B + C) = 50% o the work. 6. (D) 65. (D) Means A, B and C can do the ull work in hour. hus, (A + B + C) = 00% From this point it is better to sole through options. Option (C) gies the correct answer based on the ollowing thought process. I c = 50% work per hour, it means C takes hours to complete the work. Consequently, A would take hours and hence do.% work per hour. Since, A + B + C = 00%, this gies as B's hourly work rate = 6.66%. For this option to be correct these numbers should match the second instance and the inormation gien there. According to the second condition: A + B should be equal to 00%. utting A =.% and B = 6.66% we see that he condition is satisied. Hence, this option is correct. 9 In 99, In 96, Required robability = 8. = 9% A = Getting a Leap year B = Getting 5 Sunday in a year 5 ; A 00 A C Required probability A B A C B B A A C A A B C Selections

9

Introduction to Thermodynamic Cycles Part 1 1 st Law of Thermodynamics and Gas Power Cycles

Introduction to Thermodynamic Cycles Part 1 1 st Law of Thermodynamics and Gas Power Cycles Introduction to Thermodynamic Cycles Part 1 1 st Law of Thermodynamics and Gas Power Cycles by James Doane, PhD, PE Contents 1.0 Course Oeriew... 4.0 Basic Concepts of Thermodynamics... 4.1 Temperature

More information

Chapter 4: Properties of Pure Substances. Pure Substance. Phases of a Pure Substance. Phase-Change Processes of Pure Substances

Chapter 4: Properties of Pure Substances. Pure Substance. Phases of a Pure Substance. Phase-Change Processes of Pure Substances Chapter 4: roperties o ure Substances ure Substance A substance that has a ixed chemical composition throughout is called a pure substance such as water, air, and nitrogen A pure substance does not hae

More information

Chapter 7: The Second Law of Thermodynamics

Chapter 7: The Second Law of Thermodynamics Chapter 7: he Second Law of hermodynamics he second law of thermodynamics asserts that processes occur in a certain direction and that the energy has quality as well as quantity he first law places no

More information

CRITICAL MASS FLOW RATE THROUGH CAPILLARY TUBES

CRITICAL MASS FLOW RATE THROUGH CAPILLARY TUBES Proceedings o the ASME 010 rd Joint US-European Fluids Engineering Summer Meeting and 8th International Conerence FESM-ICNMM010 August 1-5, 010, Montreal, Canada Proceedings o ASME 010 rd Joint US-European

More information

ENERGY ANALYSIS: CLOSED SYSTEM

ENERGY ANALYSIS: CLOSED SYSTEM ENERGY ANALYSIS: CLOSED SYSTEM A closed system can exchange energy with its surroundings through heat and work transer. In other words, work and heat are the orms that energy can be transerred across the

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

Outline. Example. Solution. Property evaluation examples Specific heat Internal energy, enthalpy, and specific heats of solids and liquids Examples

Outline. Example. Solution. Property evaluation examples Specific heat Internal energy, enthalpy, and specific heats of solids and liquids Examples Outline Property ealuation examples Specific heat Internal energy, enthalpy, and specific heats of solids and liquids s A piston-cylinder deice initially contains 0.5m of saturated water apor at 00kPa.

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

LECTURE NOTE THERMODYNAMICS (GEC 221)

LECTURE NOTE THERMODYNAMICS (GEC 221) LETURE NOTE ON THERMODYNAMIS (GE ) Thermodynamics is the branch of science that treats the arious phenomena of energy and related properties of matter especially the relationship between heat, work and

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

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

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

Chapter 1 Solutions Engineering and Chemical Thermodynamics 2e Wyatt Tenhaeff Milo Koretsky

Chapter 1 Solutions Engineering and Chemical Thermodynamics 2e Wyatt Tenhaeff Milo Koretsky Chapter 1 Solutions Engineering and Chemical Thermodynamics 2e Wyatt Tenhaeff Milo Koretsky School of Chemical, Biological, and Enironmental Engineering Oregon State Uniersity 1.1 (b) The olume of water

More information

Answer 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.

Answer 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 information

Chapter 1 Introduction and Basic Concepts

Chapter 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 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

UNIVERSITY OF CALIFORNIA - SANTA CRUZ DEPARTMENT OF PHYSICS PHYS 112. Homework #4. Benjamin Stahl. February 2, 2015

UNIVERSITY OF CALIFORNIA - SANTA CRUZ DEPARTMENT OF PHYSICS PHYS 112. Homework #4. Benjamin Stahl. February 2, 2015 UIERSIY OF CALIFORIA - SAA CRUZ DEPARME OF PHYSICS PHYS Homework #4 Benjamin Stahl February, 05 PROBLEM It is given that the heat absorbed by a mole o ideal gas in a uasi-static process in which both its

More information

Chem142 Introduction to Physical Chemistry

Chem142 Introduction to Physical Chemistry Chem4 Introduction to hysical Chemistry Exam # (50 minutes) Name 00 points September 5, 07 Units and Constants R = 8.34 J/K*mol = 0.0834 L*bar/K*mol = 0.0806 L*atm/K*mol dm 3 = L K = 73.5 + C bar = 00

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

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

CHAPTER - 12 THERMODYNAMICS

CHAPTER - 12 THERMODYNAMICS CHAPER - HERMODYNAMICS ONE MARK QUESIONS. What is hermodynamics?. Mention the Macroscopic variables to specify the thermodynamics. 3. How does thermodynamics differ from Mechanics? 4. What is thermodynamic

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

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

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

Paper-II Chapter- TS-equation, Maxwell s equation. z = z(x, y) dz = dx + dz = Mdx + Ndy. dy Now. = 2 z

Paper-II Chapter- TS-equation, Maxwell s equation. z = z(x, y) dz = dx + dz = Mdx + Ndy. dy Now. = 2 z aper-ii Chapter- S-equation, Maxwell s equation Let heorem: Condition o exact dierential: Where M Hence, z x dz dx and N Q. Derive Maxwell s equations z x z zx, z dx + dz Mdx + Nd z d Now 2 z x M N x x

More information

General Physical Chemistry I

General Physical Chemistry I General Physical Chemistry I Lecture 11 Aleksey Kocherzhenko March 12, 2015" Last time " W Entropy" Let be the number of microscopic configurations that correspond to the same macroscopic state" Ø Entropy

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

Earlier Lecture. Basics of Refrigeration/Liquefaction, coefficient of performance and importance of Carnot COP.

Earlier Lecture. Basics of Refrigeration/Liquefaction, coefficient of performance and importance of Carnot COP. 9 1 Earlier Lecture Basics o Rerigeration/Liqueaction, coeicient o perormance and importance o Carnot COP. Throttling, heat exchanger, compression/expansion systems. Deinition o a rerigerator, liqueier

More information

II/IV B.Tech (Regular) DEGREE EXAMINATION. (1X12 = 12 Marks) Answer ONE question from each unit.

II/IV B.Tech (Regular) DEGREE EXAMINATION. (1X12 = 12 Marks) Answer ONE question from each unit. Page 1 of 8 Hall Ticket Number: 14CH 404 II/IV B.Tech (Regular) DEGREE EXAMINATION June, 2016 Chemical Engineering Fourth Semester Engineering Thermodynamics Time: Three Hours Maximum : 60 Marks Answer

More information

AP* Bonding & Molecular Structure Free Response Questions page 1

AP* Bonding & Molecular Structure Free Response Questions page 1 AP* Bonding & Molecular Structure Free Response Questions page 1 Essay Questions 1991 a) two points ΔS will be negative. The system becomes more ordered as two gases orm a solid. b) two points ΔH must

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

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 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 8 THERMODYNAMICS. Common Data For Q. 3 and Q.4. Steam enters an adiabatic turbine operating at steady state with an enthalpy of 3251.

CHAPTER 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 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. 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

Spectral Techniques for Reversible Logic Synthesis

Spectral Techniques for Reversible Logic Synthesis Spectral Techniques or Reersible Logic Synthesis D. Michael Miller Gerhard W. Dueck Department o Computer Science Faculty o Computer Science Uniersity o Victoria Uniersity o New Brunswick Victoria, BC,

More information

AME 436. Energy and Propulsion. Lecture 7 Unsteady-flow (reciprocating) engines 2: Using P-V and T-s diagrams

AME 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 information

Chemical Engineering Thermodynamics

Chemical Engineering Thermodynamics Chemical Engineering Thermodynamics P Liquid P x 1 sat P 1 T sat T 2 T x 1 T x 1 T y 1 Liquid Vapour sat P 2 P x 1 P y 1 P y 1 Vapour sat T 1 x, y 1 1 x, y 1 1 Pradeep Ahuja Contents CHEMICAL ENGINEERING

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

Kinetic Theory. Reading: Chapter 19. Ideal Gases. Ideal gas law:

Kinetic Theory. Reading: Chapter 19. Ideal Gases. Ideal gas law: Reading: Chapter 19 Ideal Gases Ideal gas law: Kinetic Theory p nrt, where p pressure olume n number of moles of gas R 831 J mol -1 K -1 is the gas constant T absolute temperature All gases behae like

More information

MAHALAKSHMI ENGINEERING COLLEGE

MAHALAKSHMI ENGINEERING COLLEGE MAHALAKSHMI ENGINEERING COLLEGE TIRUCHIRAPALLI 621 213. Department: Mechanical Subject Code: ME2202 Semester: III Subject Name: ENGG. THERMODYNAMICS UNIT-I Basic Concept and First Law 1. What do you understand

More information

Outline. Property diagrams involving entropy. Heat transfer for internally reversible process

Outline. Property diagrams involving entropy. Heat transfer for internally reversible process Outline roperty diagrams involving entropy What is entropy? T-ds relations Entropy change of substances ure substances (near wet dome) Solids and liquids Ideal gases roperty diagrams involving entropy

More information

EDEXCEL NATIONAL CERTIFICATE/DIPLOMA. PRINCIPLES AND APPLICATIONS of THERMODYNAMICS NQF LEVEL 3 OUTCOME 2 -ENERGY TRANSFER

EDEXCEL NATIONAL CERTIFICATE/DIPLOMA. PRINCIPLES AND APPLICATIONS of THERMODYNAMICS NQF LEVEL 3 OUTCOME 2 -ENERGY TRANSFER EDEXCEL NATIONAL CERTIFICATE/DIPLOMA PRINCIPLES AND APPLICATIONS of THERMODYNAMICS NQF LEEL OUTCOME -ENERGY TRANSFER TUTORIAL - CLOSED THERMODYNAMIC SYSTEMS CONTENT Be able to quantify energy transfer

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

Lect-19. In this lecture...

Lect-19. In this lecture... 19 1 In this lecture... Helmholtz and Gibb s functions Legendre transformations Thermodynamic potentials The Maxwell relations The ideal gas equation of state Compressibility factor Other equations of

More information

Phys102 First Major-162 Zero Version Coordinator: Saleem Rao Sunday, March 19, 2017 Page: 1

Phys102 First Major-162 Zero Version Coordinator: Saleem Rao Sunday, March 19, 2017 Page: 1 Phys0 First Major-6 Zero Version Coordinator: Saleem Rao Sunday, March 9, 07 Page: Q. A transverse wave travelling along a string (x-axis) has a orm given by equation y ym sin( kxt). FIGURE shows the displacement

More information

The Second Law of Thermodynamics (Chapter 4)

The Second Law of Thermodynamics (Chapter 4) The Second Law of Thermodynamics (Chapter 4) First Law: Energy of universe is constant: ΔE system = - ΔE surroundings Second Law: New variable, S, entropy. Changes in S, ΔS, tell us which processes made

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

The Laws of Thermodynamics

The Laws of Thermodynamics MME 231: Lecture 06 he Laws of hermodynamics he Second Law of hermodynamics. A. K. M. B. Rashid Professor, Department of MME BUE, Dhaka oday s opics Relation between entropy transfer and heat Entropy change

More information

Phase Changes and Latent Heat

Phase Changes and Latent Heat Review Questions Why can a person remove a piece of dry aluminum foil from a hot oven with bare fingers without getting burned, yet will be burned doing so if the foil is wet. Equal quantities of alcohol

More information

Thermodynamics Introduction and Basic Concepts

Thermodynamics Introduction and Basic Concepts Thermodynamics Introduction and Basic Concepts by Asst. Prof. Channarong Asavatesanupap Mechanical Engineering Department Faculty of Engineering Thammasat University 2 What is Thermodynamics? Thermodynamics

More information

Lecture 25: Heat and The 1st Law of Thermodynamics Prof. WAN, Xin

Lecture 25: Heat and The 1st Law of Thermodynamics Prof. WAN, Xin General Physics I Lecture 5: Heat and he 1st Law o hermodynamics Pro. WAN, Xin xinwan@zju.edu.cn http://zimp.zju.edu.cn/~xinwan/ Latent Heat in Phase Changes Latent Heat he latent heat o vaporization or

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. Basic state values of matter

1. 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 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

MARIA COLLEGE OF ENGINEERING AND TECHNOLOGY

MARIA 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 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

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

Aljalal-Phys March 2004-Ch21-page 1. Chapter 21. Entropy and the Second Law of Thermodynamics

Aljalal-Phys March 2004-Ch21-page 1. Chapter 21. Entropy and the Second Law of Thermodynamics Aljalal-Phys.102-27 March 2004-Ch21-page 1 Chapter 21 Entropy and the Second Law of hermodynamics Aljalal-Phys.102-27 March 2004-Ch21-page 2 21-1 Some One-Way Processes Egg Ok Irreversible process Egg

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

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

MME 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 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 information

AAE COMBUSTION AND THERMOCHEMISTRY

AAE COMBUSTION AND THERMOCHEMISTRY 5. COMBUSTIO AD THERMOCHEMISTRY Ch5 1 Overview Definition & mathematical determination of chemical equilibrium, Definition/determination of adiabatic flame temperature, Prediction of composition and temperature

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

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

+ 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

Problem Set #10 Assigned November 8, 2013 Due Friday, November 15, 2013 Please show all work for credit. To Hand in

Problem Set #10 Assigned November 8, 2013 Due Friday, November 15, 2013 Please show all work for credit. To Hand in Problem Set #10 Assigned November 8, 013 Due Friday, November 15, 013 Please show all work or credit To Hand in 1. 1 . A least squares it o ln P versus 1/T gives the result 3. Hvaporization = 5.8 kj mol

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

Differential Equations

Differential Equations LOCUS Dierential Equations CONCEPT NOTES 0. Motiation 0. Soling Dierential Equations LOCUS Dierential Equations Section - MOTIVATION A dierential equation can simpl be said to be an equation inoling deriaties

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

Thermochemistry deals with the heat involved in chemical and physical changes. 2 H2(g) + O2(g) 2 H2O(g) + energy. Two types of energy

Thermochemistry deals with the heat involved in chemical and physical changes. 2 H2(g) + O2(g) 2 H2O(g) + energy. Two types of energy All course materials, including lectures, class notes, quizzes, exams, handouts, presentations, and other materials provided to students or this course are protected intellectual property. As such, the

More information

Thermodynamic Properties are Measurements p,t,v, u,h,s - measure directly -measure by change

Thermodynamic Properties are Measurements p,t,v, u,h,s - measure directly -measure by change Thermodynamic Proerties are Measurements,T,, u,h,s - measure directly -measure by change s Tables T T Proerty Data Cure its Tables Correlation's, Boyles Law Tables c@tc limited hand calculations Equations

More information

SECOND ENGINEER REG. III/2 APPLIED HEAT

SECOND ENGINEER REG. III/2 APPLIED HEAT SECOND ENGINEER REG. III/2 APPLIED HEAT LIST OF TOPICS A B C D E F G H I J K Pressure, Temperature, Energy Heat Transfer Internal Energy, Thermodynamic systems. First Law of Thermodynamics Gas Laws, Displacement

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

FOCUS ON CONCEPTS Section 7.1 The Impulse Momentum Theorem

FOCUS ON CONCEPTS Section 7.1 The Impulse Momentum Theorem WEEK-6 Recitation PHYS 3 FOCUS ON CONCEPTS Section 7. The Impulse Momentum Theorem Mar, 08. Two identical cars are traeling at the same speed. One is heading due east and the other due north, as the drawing

More information

The International Association for the Properties of Water and Steam

The International Association for the Properties of Water and Steam he International Association for the Properties of Water and Steam Kyoto, Japan September 2004 Reised Supplementary Release on Backward Equations for the Functions (p,h), (p,h) and (p,s), (p,s) for Region

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

Applied Thermodynamics for Marine Systems Prof. P. K. Das Department of Mechanical Engineering Indian Institute of Technology, Kharagpur

Applied Thermodynamics for Marine Systems Prof. P. K. Das Department of Mechanical Engineering Indian Institute of Technology, Kharagpur Applied Thermodynamics for Marine Systems Prof. P. K. Das Department of Mechanical Engineering Indian Institute of Technology, Kharagpur Lecture - 8 Introduction to Vapour Power Cycle Today, we will continue

More information

4 Fundamentals of Continuum Thermomechanics

4 Fundamentals of Continuum Thermomechanics 4 Fundamentals of Continuum Thermomechanics In this Chapter, the laws of thermodynamics are reiewed and formulated for a continuum. The classical theory of thermodynamics, which is concerned with simple

More information

The International Association for the Properties of Water and Steam

The International Association for the Properties of Water and Steam IAPWS SR3-03(2014) he International Association for the Properties of Water and Steam Moscow, Russia June 2014 Reised Supplementary Release on Backward Equations for the Functions (h), (h) and (s), (s)

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

What is thermodynamics? and what can it do for us?

What is thermodynamics? and what can it do for us? What is thermodynamics? and what can it do for us? The overall goal of thermodynamics is to describe what happens to a system (anything of interest) when we change the variables that characterized the

More information

CHEM* Physical Chemistry FALL Assignment #1: SOLUTIONS. Gases. Thermodynamics: heat and work

CHEM* Physical Chemistry FALL Assignment #1: SOLUTIONS. Gases. Thermodynamics: heat and work CHEM*2880 - hysical Chemistry FALL 2005 Assignment #1: SOLUTIONS Gases. Thermodynamics: heat and work 1. 1 mol o nitrogen and mol o hydrogen are injected into a container o volume 10 dm at 298K. What are

More information

CHAPTER (i) No. For each coefficient, the usual standard errors and the heteroskedasticity-robust ones are practically very similar.

CHAPTER (i) No. For each coefficient, the usual standard errors and the heteroskedasticity-robust ones are practically very similar. SOLUTIONS TO PROBLEMS CHAPTER 8 8.1 Parts (ii) and (iii). The homoskedasticity assumption played no role in Chapter 5 in showing that OLS is consistent. But we know that heteroskedasticity causes statistical

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

Physical Chemistry. Chapter 3 Second Law of Thermodynamic

Physical Chemistry. Chapter 3 Second Law of Thermodynamic Physical Chemistry Chapter 3 Second Law of hermodynamic by Izirwan Bin Izhab FKKSA izirwan@ump.edu.my Chapter Description Aims Develop the calculational path for property change and estimate enthalpy and

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

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

Chemical Thermodynamics

Chemical Thermodynamics Quiz A 42.8 ml solution of ammonia (NH 3 ) is titrated with a solution of 0.9713 M hydrochloric acid. The initial reading on the buret containing the HCl was 47.13 ml and the final reading when the endpoint

More information

Thermodynamics Qualifying Exam Study Material

Thermodynamics Qualifying Exam Study Material Thermodynamics Qualifying Exam Study Material The candidate is expected to have a thorough understanding of undergraduate engineering thermodynamics topics. These topics are listed below for clarification.

More information

Theoretical & Derivation based Questions and Answer. Unit Derive the condition for exact differentials. Solution:

Theoretical & Derivation based Questions and Answer. Unit Derive the condition for exact differentials. Solution: Theoretical & Derivation based Questions and Answer Unit 01 1. Derive the condition for exact differentials. Solution: 2*. Derive the Maxwell relations and explain their importance in thermodynamics. Solution:

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

(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

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

This follows from the Clausius inequality as a consequence of the second law of thermodynamics. Therefore. (for reversible process only) (22.

This follows from the Clausius inequality as a consequence of the second law of thermodynamics. Therefore. (for reversible process only) (22. Entropy Clausius inequality can be used to analyze the cyclic process in a quantitative manner. The second law became a law of wider applicability when Clausius introduced the property called entropy.

More information

Aerodynamic Admittance Function of Tall Buildings

Aerodynamic Admittance Function of Tall Buildings Aerodynamic Admittance Function o Tall Buildings in hou a Ahsan Kareem b a alou Engineering Int l, Inc., 75 W. Campbell Rd, Richardson, T, USA b Nataz odeling Laboratory, Uniersity o Notre Dame, Notre

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

Handout 12: Thermodynamics. Zeroth law of thermodynamics

Handout 12: Thermodynamics. Zeroth law of thermodynamics 1 Handout 12: Thermodynamics Zeroth law of thermodynamics When two objects with different temperature are brought into contact, heat flows from the hotter body to a cooler one Heat flows until the temperatures

More information