QUIZZES RIEPJCPIγPJEJJJY

Size: px
Start display at page:

Download "QUIZZES RIEPJCPIγPJEJJJY"

Transcription

1 Che 3021 Thermodynamics I QUIZZES RIEPJCPIγPJEJJJY

2 QUIZ 1. Find Molecular Weights: 1 1 CO 2 2 NaCl 3 Aspirin C 9 H 8 O 4 CO2 = NaCl = C9H8O4 = PIgPJC

3 Quiz 1. Temperature conversion 1 Convert 94 o F, to (a). Rankine, o R (b). Kelvin, K (c).. Celsius, o C (a). Rankine, o R = (b). Kelvin, K = (c).. Celsius, o C = PIgPJC

4 Quiz 1. Carnot Efficiency 1 In a Carnot engine, the high temperature is 975 o C, and low temperature is 20 o C; what is its thermal efficiency, η? η = PIgPJC

5 Quiz 2. PV Expansion work of ideal gas: PV = nrt For an ideal gas of 0.7 gmol in a cylinder initially at v 1 = 5 liters and P 1 = 5 atm. What is its temperature T 1 (K)? Expansion at constant temperature takes place until v 2 = 10 liters. What is the final pressure P 2 (atm)? What work has been done, W (in J)? T1 = P2 = W = PJE 2 Hints: Find the gas constant, R PJE

6 Quiz 2. Ideal gas calculations: PJE 2 Calculate the volume (in liter) of air (assuming ideal gas, i.e. PV=nRT) at T= 70 o F, and P = 1 atm for one lbmol. Calculate the temperature of nitrogen (ideal gas) at 20 psia and 102 cuft/lbmol. Calculate the specific volume (m 3 /kmol) of CO2 (ideal gas) at bar and -195 o F.

7 Piston-Cylinder Heat Transfer pas donne PJE 2 Air is contained in a vertical piston cylinder assembly by a piston of mass 50 kg and having a face area of 0.01 m 2. The mass of the air is 5 g, and initially the air occupies a volume of 5 liters. The atmosphere exerts a pressure of 100 kpa on the top of the piston. The volume of the air slowly decreases to m 3 as the specific internal energy of the air decreases by 260 kj/kg. Neglecting friction between the piston and the cylinder wall, determine the heat transfer to the air, in kj. OJG

8 Quiz 3. Read Steam Tables & Mollier Charts For water PJJ-3 (ST) Find the enthalpy (kj/kg) and internal energy (kj/kg), and specific volume (m3/kg) for steam at (a) T = 120 o C and P = 1bar, and (b) T = 440 o C and P = 320 bar. (MC) Find the enthalpy (Btu/lb m ) and entropy (Btu/(lb m,or) for steam at (a) T = 800 o F and P = 100 psia, and (b) T = 450 o F and P = 60 psia.

9 QUIZ 3. Read Steam Tables and Mollier Chart Find specific volume (m 3 /kg) and enthalpy (kj/kg) for Steam at T= 520 o C and P= 200 bar. T.A-5 Find the enthalpy, H, from the Mollier chart at T= 700 o F, and P=60 psia. PJJ-3

10 QUIZ 3. Read Steam Tables: PJJ-3 Find specific volume (m3/kg) and enthalpy (kj/kg) for subcooled liquid water at T= 200 o C and P= 25 bar. T.A-5 At T= 50 o C, what is the saturate pressure (bar)? What are the saturated liquid and vapor volumes (m3/kg). T.A-2 At P= 4 bar, what is the saturate temperature (oc)? What are the saturated liquid and vapor volumes (m3/kg). T.A-3

11 Quiz 4. (1) Ideal gas calculations: Given a classroom of size: 25 x30 x12, find the air mass (in lb m ) at T = 75 o F and P= 14.7 psia. PV = nrt. (Choose the right value of R). Air s average MW is RIN (2) Use steam tables: What is the specific volume (in m 3 /kg) of water at saturated pressure of 7.85 psia.

12 lbm

13 QUIZ 5. Calculate the Heat Capacity, Cp, of nitrogen at T =298 K RIQ (1) Use the text formula for N 2. For N 2 : Cp/R = α + βt + γt 2 + δt 3 + εt 4.α= β= e-3.γ= 2.324e-6.δ= e-9.ε= e-12 (2) Use the API formula for N 2. For N 2 : Cp* in cal/(gmol.k) B= , C= , D= , E= ,, F=

14 QUIZ #1. OAKRKb11.98 Find the pressure (atm) of a mixture of CH 4 (0. 5 lbmol) + n-c 3 H 8 (0.5 lbmol) at T=194 F and V= 7.65 ft 3. Use the van der Waals EOS. Table A-24E. (R= atm.ft 3 /(lbmol. o R)) CH4 n-c 3 H 8 a atm.(ft3/lbmol)^2 b ft3/lbmol

15 Ans RKb.a= b= T= = o R P=49.9 atm

16 QUIZ #2 OAK Find the pressure of a mixture of CH 4 (0.18 kmol) + n-c 4 H 10 (0.274 kmol) at T=238 C and V= m 3. Use the Redlich-Kwong EOS. (R= bar.m3/kmol.k) CH4 nc4h10 a b

17 QUIZ 5. Calculate the Heat Capacity, Cp, of nitrogen at T =298 K RIQ (1) Use the text formula for N 2. For N 2 : Cp/R.α= β= e-3.γ= 2.324e-6.δ= e-9.ε= e-12 (2) Use the API formula for N 2. For N 2 : Cp* in cal/(gmol.k) B= , C= , D= , E=

18 QUIZ 5. Calculate the enthalpy of steam PJM-4 For 1 kg of steam at P = 15 bar, and T = 280 o C, the specific volume v = m3/kg. The internal energy is u= kj/kg. Use the formula (Definition) of enthalpy to calculate H = U + PV What is this H-value (kj)? kj

19 QUIZ 5. Calculate the enthalpy of steam RIQ H = U + PV What is this H-value (kj)? kj

20 QUIZ 6. PJQ-5

21 QUIZ 4. Use generalized compressibility chart for nitrogen PJM-4 For 1 kmol of nitrogen (N2) at P = 35 bar, and T = 280 o C, what is its compressibility, Z? Use Figure A1 or A2 in the appendix. Z = 1.05

22 QUIZ 7. RIXPJT Applying the Maxwell Relations Evaluate the partial derivative ( T/ v) H for van der Waals equation in terms of P,v,T, Cp, Cv, and their derivatives. Using the RABbit rule and the Maxwell relations.

23 QUIZ 6. Applying the Maxwell Relations Evaluate the partial derivative ( s/ P) T (in J/(bar.K)) for water vapor at a state fixed by a temperature of 240 C and a specific volume of m 3 /kg. Use the Redlich Kwong equation of state and an appropriate Maxwell relation. PJT

24 QUIZ 6.

25 Quiz F18 Express the derivative [ T/ V]H [ H/ T]v in terms of P,V,T,Cp,Cv and their derivatives. Use Maxwell and other derivative relations Plus dh = TdS + VdP

26 Quiz F18 Express the derivatives [ T/ V]S [ H/ T]v in terms of P,V,T,Cp,Cv and their derivatives. Use Maxwell and other derivative relations Plus dh = TdS + VdP

27 Quiz F18 Use graphical differentiation and Clapeyron eq. to find the heat of vaporization of saturated steam at 120 o C Steam Given the vapor pressure curve of steam. T,C VP

28 QUIZ 7. Find the heat of vaporization (kj/kg) by the Clausius-Claperon equation at 220 o C from the vapor pressures using graphical differentiation.

29 QUIZ 7. Find the heat of vaporization (kj/kg) by the Clausius-Claperon equation at 140 o C from the vapor pressures using graphical differentiation.

30

31

32 QUIZ 10. Find the velocity of sound in air (in ft/s) at - 40 o F (below 0 o F) using the ideal gas equation Pv = RT. Use k = 1.4. RJE PJZ

33 Example: Velocity of Sound in Air

34 RJH Quiz 11. Change in entropy, ΔS 10 kmol of Ethylene (C2H4) is compressed from 1 bar to 100 bar at constant T= 400K. Find its entropy change in (kj/k). Use the Redlich-Kwong equation. ΔS = S2-S1 =

35 4.2

36 Quiz 11. Turbine Work output Winnick <133> PKG+PKH Steam at 1000 o F and 1000 psia is fed steadily to an adiabatic turbine (Q=0) at a rate of 125 lb/min. If the outlet steam is 450 o F and 100 psia, what is the work output in (Btu/min, and kw). (Negligible PE and KE changes). Note that 1 Btu/min = watts.

37 Q11: Ans Winnick <133> PKG kw Btu/min

38 QUIZ 12: Pump Heat capacity: C= 1 Btu/(lb*Δ o F)

39 QUIZ 12 (continued)

40 QUIZ 13. Carnot Efficiency In a Carnot engine, the high temperature is 975 o C, and low temperature is 20 o C; what is its thermal efficiency, η? If the Qc = kj, what is the net entropy change (in kj/k) due to heat transfers Q H and Qc in the Cycle? Calculate the work produced in this cycle: W net =? η = 76.5 % RJSPIg

41 QUIZ 14. Entropy change for Id.g. An ideal gas is compressed from T 1 =300 K, v 1 = 10 m 3 /kg to T 2 = 400 K, v 2 = 2 m 3 /kg. Find the Δs in (kj/(kg.k). Constant heat capacity is assumed at C v =1.008 kj/(kg.k). RJSPIg

42 QUIZ 15: Hot/Cold Isentropic Processes: (1) T 1 = 230K, P 1 =100 bar, T 2 = 350K, find P 2? (a) Use Isentropy (Cold): P2/P1 = (b) Use Tables (A22) (Hot): Pr2=?, Pr1=? P2= P1*(Pr2/Pr1)=

43 Quiz 15b Using Cold & Hot Processes RJZPKN <451> Otto In a compressor, air goes through an adiabatic and reversible compression from P1= 1 atm, and V1 = 0.2 cuft to V2=0.025 cuft at T1 = 540 o R. The hat capacity ratio k= Cp/Cv=1.4. (a) Use the cold equations to find T2 ( o R), and P2 (atm). (b) Use table A-22E (the hot process) to find T2 ( o R), and P2 (atm). (Interpolate if needed!)

44 QUIZ 16: Hot/Cold Isentropic Processes: (1) T 1 = 230K, P 1 =100 bar, T 2 = 350K, find P 2? (a) Use Isentropy (Cold): P2/P1 = (b) Use Tables (A22) (Hot): Pr2=?, Pr1=? P2= P1*(Pr2/Pr1)=

45 QUIZ 17: Otto Cycle (Hot) for unit mass (1 kg of working fluid) flowing through. Heat addition Q H is 1400 kj/kg during combustion. (a) Compression Stroke (1-2): T 1 = 300K, P 1 =1 bar, r=8.5 (b) Find T2(K), u2(kj/kg) from Table A-22. (c) Use 1 st law for Combust (2-3) : m(u3-u2) = Q H +0 find u3 and T3! (interpolate!) Vr1, Vr2,V2 8.5

46 QUIZ 18: Otto Cycle (Cold) for unit mass (1 kg of working fluid) flowing through. Heat addition Q H is 1400 kj/kg during combustion. (a) Compression Stroke (1-2): T 1 = 300K, P 1 =1 bar, r=8.5 (b) Find T2(K) & u2(kj/kg) =Cv*T2 (c) Use 1 st law for Combustion (2-3) : m(u3-u2) = Q H +0 find u3 =Cv*T3 (kj/kg). Use k=1.4! Cv=0.713 (kj/(kg.δkelvin)) 8.5

47 QUIZ #19. OAKRKb11.98 Find the pressure (atm) of a mixture of CH 4 (0. 5 lbmol) + n-c 3 H 8 (0.5 lbmol) at T=194 F and V= 7.65 ft 3. Use the van der Waals EOS. Table A-24E. (R= atm.ft 3 /(lbmol. o R)) CH4 n-c 3 H 8 a atm.(ft3/lbmol)^2 b ft3/lbmol

48 Ans RKb.a= b= T= = o R P=49.9 atm

49 QUIZ #20 OAK Find the pressure of a mixture of CH 4 (0.18 kmol) + n-c 4 H 10 (0.274 kmol) at T=238 C and V= m 3. Use the Redlich-Kwong EOS. (R= bar.m3/kmol.k) CH4 nc4h10 a b

50 Quiz 21: H-x: Water+H 2 SO 4 Mx Find the partial molar enthalpies at 93.3 o C! water and Hacid at mass frac. w acid =0.60. H Also find H Total at w Acid =0.60 from the relation between PMH and total H T. H

51 QUIZ 22: Fugacity of steam PAMRLE Calculate the fugacity of steam at P=60 bar, and T= 500 o C using the steam tables h s h s

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

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

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

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

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 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 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

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

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

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

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

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

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

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

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 4. Energy Analysis of Closed Systems

Chapter 4. Energy Analysis of Closed Systems Chapter 4 Energy Analysis of Closed Systems The first law of thermodynamics is an expression of the conservation of energy principle. Energy can cross the boundaries of a closed system in the form of heat

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

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

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

Basic Thermodynamics Module 1

Basic Thermodynamics Module 1 Basic Thermodynamics Module 1 Lecture 9: Thermodynamic Properties of Fluids Thermodynamic Properties of fluids Most useful properties: Properties like pressure, volume and temperature which can be measured

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

EVALUATING PROPERTIES FOR A PURE SUBSTANCES. By Ertanto Vetra

EVALUATING PROPERTIES FOR A PURE SUBSTANCES. By Ertanto Vetra EVALUATING PROPERTIES FOR A PURE SUBSTANCES 1 By Ertanto Vetra Outlines - TV, PV, PT, PVT Diagram - Property Tables - Introduction to Enthalpy - Reference State & Reference Values - Ideal Gas Equation

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

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

Dr Ali Jawarneh. Hashemite University

Dr Ali Jawarneh. Hashemite University Dr Ali Jawarneh Department of Mechanical Engineering Hashemite University Examine the moving boundary work or P d work commonly encountered in reciprocating devices such as automotive engines and compressors.

More information

Thermodynamics I Chapter 2 Properties of Pure Substances

Thermodynamics I Chapter 2 Properties of Pure Substances Thermodynamics I Chapter 2 Properties of Pure Substances Mohsin Mohd Sies Fakulti Kejuruteraan Mekanikal, Universiti Teknologi Malaysia Properties of Pure Substances (Motivation) To quantify the changes

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

KNOWN: Pressure, temperature, and velocity of steam entering a 1.6-cm-diameter pipe.

KNOWN: Pressure, temperature, and velocity of steam entering a 1.6-cm-diameter pipe. 4.3 Steam enters a.6-cm-diameter pipe at 80 bar and 600 o C with a velocity of 50 m/s. Determine the mass flow rate, in kg/s. KNOWN: Pressure, temperature, and velocity of steam entering a.6-cm-diameter

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

(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

INSTITUTE OF AERONAUTICAL ENGINEERING (Autonomous) Dundigal, Hyderabad

INSTITUTE OF AERONAUTICAL ENGINEERING (Autonomous) Dundigal, Hyderabad INSTITUTE OF AERONAUTICAL ENGINEERING (Autonomous) Dundigal, Hyderabad -500 043 MECHANICAL ENGINEERING TUTORIAL QUESTION BANK Name : THERMODYNAMICS Code : A30306 Class : II B. Tech I Semester Branch :

More information

Dual Program Level 1 Physics Course

Dual Program Level 1 Physics Course Dual Program Level 1 Physics Course Assignment 15 Due: 11/Feb/2012 14:00 Assume that water has a constant specific heat capacity of 4190 J/kg K at all temperatures between its melting point and boiling

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

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

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

Common Terms, Definitions and Conversion Factors

Common Terms, Definitions and Conversion Factors 1 Common Terms, Definitions and Conversion Factors 1. Force: A force is a push or pull upon an object resulting from the object s interaction with another object. It is defined as Where F = m a F = Force

More information

MAE 320 THERODYNAMICS FINAL EXAM - Practice. Name: You are allowed three sheets of notes.

MAE 320 THERODYNAMICS FINAL EXAM - Practice. Name: You are allowed three sheets of notes. 50 MAE 320 THERODYNAMICS FINAL EXAM - Practice Name: You are allowed three sheets of notes. 1. Fill in the blanks for each of the two (Carnot) cycles below. (a) 5 a) Heat engine or Heat pump/refrigerator

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

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

4. All questions are NOT ofequal value. Marks available for each question are shown in the examination paper.

4. All questions are NOT ofequal value. Marks available for each question are shown in the examination paper. THE UNIVERSITY OF NEW SOUTH WALES SCHOOL OF PHYSICS \1111~11\llllllllllllftllll~flrllllllllll\11111111111111111 >014407892 PHYS2060 THER1\1AL PHYSICS FINAL EXAMINATION SESSION 2 - NOVEMBER 2010 I. Time

More information

S.E. (Chemical Engineering) (Second Semester)EXAMINATION, 2012 THERMODYNAMICS-I (2008 PATTERN) Time : Three Hours Maximum Marks : 100

S.E. (Chemical Engineering) (Second Semester)EXAMINATION, 2012 THERMODYNAMICS-I (2008 PATTERN) Time : Three Hours Maximum Marks : 100 Total No. of Questions 12] [Total No. of Printed Pages 7 Seat No. [4162]-189 S.E. (Chemical Engineering) (Second Semester)EXAMINATION, 2012 THERMODYNAMICS-I (2008 PATTERN) Time : Three Hours Maximum Marks

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

+ 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

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

INSTITUTE OF AERONAUTICAL ENGINEERING (Autonomous) Dundigal, Hyderabad

INSTITUTE OF AERONAUTICAL ENGINEERING (Autonomous) Dundigal, Hyderabad INSTITUTE OF AERONAUTICAL ENGINEERING (Autonomous) Dundigal, Hyderabad - 500 04 AERONAUTICAL ENGINEERING TUTORIAL QUESTION BANK Course Name : THERMODYNAMICS Course Code : AME00 Regulation : IARE - R1 Year

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

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

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

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

Name: Discussion Section:

Name: Discussion Section: CBE 141: Chemical Engineering Thermodynamics, Spring 2018, UC Berkeley Midterm 2 March 22, 2018 Time: 80 minutes, closed-book and closed-notes, one-sided 8 ½ x 11 equation sheet allowed Please show all

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

9.1 Basic considerations in power cycle analysis. Thermal efficiency of a power cycle : th = Wnet/Qin

9.1 Basic considerations in power cycle analysis. Thermal efficiency of a power cycle : th = Wnet/Qin Chapter 9 GAS POWER CYCLES 9.1 Basic considerations in power cycle analysis. Thermal efficiency of a power cycle : th = Wnet/Qin Gas-power cycles vs. vapor-power cycles: T p 1 p 2 p 3 Vapor cycle Gas cycle

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

Chapter 1: Basic Definitions, Terminologies and Concepts

Chapter 1: Basic Definitions, Terminologies and Concepts Chapter : Basic Definitions, Terminologies and Concepts ---------------------------------------. UThermodynamics:U It is a basic science that deals with: -. Energy transformation from one form to another..

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

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

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

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

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

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

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

Thermodynamics I Spring 1432/1433H (2011/2012H) Saturday, Wednesday 8:00am - 10:00am & Monday 8:00am - 9:00am MEP 261 Class ZA

Thermodynamics I Spring 1432/1433H (2011/2012H) Saturday, Wednesday 8:00am - 10:00am & Monday 8:00am - 9:00am MEP 261 Class ZA Thermodynamics I Spring 1432/1433H (2011/2012H) Saturday, Wednesday 8:00am - 10:00am & Monday 8:00am - 9:00am MEP 261 Class ZA Dr. Walid A. Aissa Associate Professor, Mech. Engg. Dept. Faculty of Engineering

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

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

Physics 231. Topic 14: Laws of Thermodynamics. Alex Brown Dec MSU Physics 231 Fall

Physics 231. Topic 14: Laws of Thermodynamics. Alex Brown Dec MSU Physics 231 Fall Physics 231 Topic 14: Laws of Thermodynamics Alex Brown Dec 7-11 2015 MSU Physics 231 Fall 2015 1 8 th 10 pm correction for 3 rd exam 9 th 10 pm attitude survey (1% for participation) 10 th 10 pm concept

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

UNIVESITY OF SWAZILAND FACl.JLTY OF SCIENCE AND ENGINEERING DEPARTMENT OF PHYSICS

UNIVESITY OF SWAZILAND FACl.JLTY OF SCIENCE AND ENGINEERING DEPARTMENT OF PHYSICS UNIVESITY OF SWAZILAND FACl.LTY OF SCIENCE AND ENGINEERING DEPARTMENT OF PHYSICS Main Examination 2016/2017. COURSE NAME: Thermodynamics/Thermofluids COURSE CODE: PHY242/EEE202 TIME ALLOWED: 3 hours ANSWER

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

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 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

MAE 110A. Homework 6: Solutions 11/9/2017

MAE 110A. Homework 6: Solutions 11/9/2017 MAE 110A Hoework 6: Solutions 11/9/2017 H6.1: Two kg of H2O contained in a piston-cylinder assebly, initially at 1.0 bar and 140 C undergoes an internally ersible, isotheral copression to 25 bar. Given

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

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

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

Today lecture. 1. Entropy change in an isolated system 2. Exergy

Today lecture. 1. Entropy change in an isolated system 2. Exergy Today lecture 1. Entropy change in an isolated system. Exergy - What is exergy? - Reversible Work & Irreversibility - Second-Law Efficiency - Exergy change of a system For a fixed mass For a flow stream

More 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

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

III. Evaluating Properties. III. Evaluating Properties

III. Evaluating Properties. III. Evaluating Properties F. Property Tables 1. What s in the tables and why specific volumes, v (m /kg) (as v, v i, v f, v g ) pressure, P (kpa) temperature, T (C) internal energy, u (kj/kg) (as u, u i, u f, u g, u ig, u fg )

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

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

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

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

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

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

Temperature Thermal Expansion Ideal Gas Law Kinetic Theory Heat Heat Transfer Phase Changes Specific Heat Calorimetry Heat Engines

Temperature Thermal Expansion Ideal Gas Law Kinetic Theory Heat Heat Transfer Phase Changes Specific Heat Calorimetry Heat Engines Temperature Thermal Expansion Ideal Gas Law Kinetic Theory Heat Heat Transfer Phase Changes Specific Heat Calorimetry Heat Engines Zeroeth Law Two systems individually in thermal equilibrium with a third

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

Chapter One Reviews of Thermodynamics Update on 2013/9/13

Chapter One Reviews of Thermodynamics Update on 2013/9/13 Chapter One Reviews of Thermodynamics Update on 2013/9/13 (1.1). Thermodynamic system An isolated system is a system that exchanges neither mass nor energy with its environment. An insulated rigid tank

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 1 LIQUIDS VAPOURS - GASES SAE

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

Non-Newtonian fluids is the fluids in which shear stress is not directly proportional to deformation rate, such as toothpaste,

Non-Newtonian fluids is the fluids in which shear stress is not directly proportional to deformation rate, such as toothpaste, CHAPTER1: Basic Definitions, Zeroth, First, and Second Laws of Thermodynamics 1.1. Definitions What does thermodynamic mean? It is a Greeks word which means a motion of the heat. Water is a liquid substance

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

Pure Substance. Properties of Pure Substances & Equations of State. Vapour-Liquid-Solid Phase Equilibrium

Pure Substance. Properties of Pure Substances & Equations of State. Vapour-Liquid-Solid Phase Equilibrium Pure Substance Properties of Pure Substances & Equations of State Dr. d. Zahurul Haq Professor Department of echanical Engineering Bangladesh University of Engineering & Technology (BUET) Dhaka-1000, Bangladesh

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

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

CHEMICAL ENGINEERING THERMODYNAMICS. Andrew S. Rosen

CHEMICAL ENGINEERING THERMODYNAMICS. Andrew S. Rosen CHEMICAL ENGINEERING THERMODYNAMICS Andrew S. Rosen SYMBOL DICTIONARY 1 TABLE OF CONTENTS Symbol Dictionary... 3 1. Measured Thermodynamic Properties and Other Basic Concepts... 5 1.1 Preliminary Concepts

More 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

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

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

Pure Substance. Properties of Pure Substances & Equations of State. Vapour-Liquid-Solid Phase Equilibrium

Pure Substance. Properties of Pure Substances & Equations of State. Vapour-Liquid-Solid Phase Equilibrium Pure Substance Properties of Pure Substances & Equations of State Dr. d. Zahurul Haq Professor Department of echanical Engineering Bangladesh University of Engineering & Technology (BUET) Dhaka-1000, Bangladesh

More information