First Law of Thermodynamics: Closed Systems
|
|
- Kelley Ball
- 6 years ago
- Views:
Transcription
1 utorial # First Law of hermodynamics: Closed Systems Problem -7 A 0.-m tank contains oxygen initially at 00kPa and 7 C. A paddle wheel within the tank is rotated until the pressure inside rise to 50kPa. During the process KJ of heat is lost to the surroundings. Determine the paddle-wheel work done. Neglect the energy stored in the paddle wheel. Solution: Step : Draw a schematic diagram to represent the system ank Q Paddle Wheel Step : What to determine? he work done by paddle-wheel work, W e Step : he information given in the problem statement. utorial # Page of 5
2 Volume of the tank, V = 0. m, and Volume remains constant during the whole process: V V = V =. Initial condition of the Oxygen in the tank: P = 00 kpa, = 7 C; Final condition of the Oxygen in the tank: P = 50 kpa; Heat loss to the surroundings, Q =! KJ. Step 4: able of all known values and properties Oxygen Pressure (kpa Volume (m emperature (K Initial condition Final condition Heat loss (KJ - Step 5: Assumptions It s a closed system and no mass loss in the whole process; Consider the Oxygen as ideal gas for given conditions; Neglect the energy stored in the paddle wheel; Change in kinetic and potential energy is negligible. Step 6: Solve. According the ideal gas equation, PV = mr From the initial condition, the mass of the Oxygen is determined by PV (00kPa " (0.m m = = = 0.849( kg R (0.598kPa! m / kg! K(00K. he final temperature of the Oxygen can be determined from PV PV = utorial # Page of 5
3 So, PV (50kPa! (0.m = =! (00K = 450( K PV (00kPa! (0.m. he energy conservation equation of this closed system can be described as: where, Q " W =! U +! KE +! PE! KE and! PE are both zero according to the assumptions. As for the work, W = W + W + W e Due to the volume remains constant, the boundary work is zero and there is no other works indicated in the problem. hus the above energy conservation equation became, b Q " We =! U Because it s a constant-volume process, the above equation can be concluded, Q! W other = m( u! u = Cvm( e! Here, the specific heat of Oxygen at the average temperature of avg = ( / = 75( K is, = KJ /( kg (from the able A-b. C v, avg! K So, rearrange the above equation and substitute the values, W = Q! C m( e v! = (! KJ! (0.6745KJ / kg # K " (0.849kg " (450K! 00K =!40.94KJ Step 7: Conclusion statement he work done by the paddle-wheel is KJ. utorial # Page of 5
4 Problem -8 A piston-cylinder device contains 5kg of argon at 400kPa and 0 C. During a quasi-equilibrium, isothermal expansion process, 5KJ of boundary work is done by the system, and KJ of paddle-wheel work is done on the system. Determine the heat transfer for this process. Solution: Step : Draw a schematic diagram to represent the problem W b Q W e Initial Condition Final Condition Step : What to determine? he heat transfer between the system and the surroundings, Q Step : he information given in the problem statement.. Argon in the cylinder: m=5kg, P=400kPa and =0V;. A boundary work done by the system, W b =5KJ;. he paddle-wheel work done on the system, W e =-KJ utorial # Page 4 of 5
5 Step 4: Assumptions. It s a quasi-equilibrium, isothermal expansion process, which means that the temperature remains constant in the whole process;. For the argon in the piston-cylinder system, it s a closed system, no mass enters or leaves.. Change in kinetic and potential energy is negligible. Step 6: Solve We take the argon in the piston-cylinder system as our system, and the energy conservation equation of this closed system can be described as: where, Q " W =! U +! KE +! PE! KE and! PE are both zero according to the assumptions. It s a quasiequilibrium, isothermal expansion process. he temperature remains constant, so is the total internal energy. he change of the total internal energy is zero during the whole process, which give us So, Substituting the works,!u = 0 Q!W = 0 Q = W = We + Wb = (! KJ + (5KJ = KJ he sign is positive, which means that heat transfers from the surroundings to the system. Step 7: Conclusion statement In this process, the argon in the piston-cylinder device will absorb heat with an amount of KJ from the surroundings. utorial # Page 5 of 5
First Law of Thermodynamics Closed Systems
First Law of Thermodynamics Closed Systems Content The First Law of Thermodynamics Energy Balance Energy Change of a System Mechanisms of Energy Transfer First Law of Thermodynamics in Closed Systems Moving
More informationPhysics 111. Lecture 39 (Walker: 17.6, 18.2) Latent Heat Internal Energy First Law of Thermodynamics May 8, Latent Heats
Physics 111 Lecture 39 (Walker: 17.6, 18.2) Latent Heat Internal Energy First Law of Thermodynamics May 8, 2009 Lecture 39 1/26 Latent Heats The heat required to convert from one phase to another is called
More informationCHAPTER 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 informationKNOWN: 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 informationa) The minimum work with which this process could be accomplished b) The entropy generated during the process
ENSC 46 Tutorial, Week#6 Exergy: Control Mass Analysis An insulated piston-cylinder device contains L of saturated liquid water at a pressure of 50 kpa which is constant throughout the process. An electric
More informationExergy 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 informationME Thermodynamics I
HW-03 (25 points) i) Given: for writing Given, Find, Basic equations Rigid tank containing nitrogen gas in two sections initially separated by a membrane. Find: Initial density (kg/m3) of nitrogen gas
More informationPROBLEM 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 informationUNIT 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 informationCircle your instructor s last name
ME 00 Thermodynamics Fall 07 Exam Circle your structor s last name Division : Naik Division : Wassgren Division 6: Braun Division : Sojka Division 4: Goldenste Division 7: Buckius Division 8: Meyer INSTRUCTIONS
More informationSCHOOL OF COMPUTING, ENGINEERING AND MATHEMATICS SEMESTER 2 EXAMINATIONS 2014/2015 ME258. Thermodynamics
s SCHOOL OF COMPUING, ENGINEERING AND MAHEMAICS SEMESER EXAMINAIONS 04/05 ME58 hermodynamics ime allowed: WO hours Answer: Any FOUR Questions Items permitted: Any approved calculator Items supplied: Steam
More informationFind: a) Mass of the air, in kg, b) final temperature of the air, in K, and c) amount of entropy produced, in kj/k.
PROBLEM 6.25 Three m 3 of air in a rigid, insulated container fitted with a paddle wheel is initially at 295 K, 200 kpa. The air receives 1546 kj of work from the paddle wheel. Assuming the ideal gas model,
More informationIII. 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 informationPTT 277/3 APPLIED THERMODYNAMICS SEM 1 (2013/2014)
PTT 77/3 APPLIED THERMODYNAMICS SEM 1 (013/014) 1 Energy can exist in numerous forms: Thermal Mechanical Kinetic Potential Electric Magnetic Chemical Nuclear The total energy of a system on a unit mass:
More informationME Thermodynamics I = = = 98.3% 1
HW-08 (25 points) i) : a) 1 Since ν f < ν < ν g we conclude the state is a Saturated Liquid-Vapor Mixture (SLVM) 1, from the saturation tables we obtain p 3.6154 bar. 1 Calculating the quality, x: x ν
More informationChapter 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 informationChapter 7. Entropy. by Asst.Prof. Dr.Woranee Paengjuntuek and Asst. Prof. Dr.Worarattana Pattaraprakorn
Chapter 7 Entropy by Asst.Prof. Dr.Woranee Paengjuntuek and Asst. Prof. Dr.Worarattana Pattaraprakorn Reference: Cengel, Yunus A. and Michael A. Boles, Thermodynamics: An Engineering Approach, 5th ed.,
More informationfirst law of ThermodyNamics
first law of ThermodyNamics First law of thermodynamics - Principle of conservation of energy - Energy can be neither created nor destroyed Basic statement When any closed system is taken through a cycle,
More information- Apply closed system energy balances, observe sign convention for work and heat transfer.
CHAPTER : ENERGY AND THE FIRST LAW OF THERMODYNAMICS Objectives: - In this chapter we discuss energy and develop equations for applying the principle of conservation of energy. Learning Outcomes: - Demonstrate
More informationTHERMODYNAMICS, FLUID AND PLANT PROCESSES. The tutorials are drawn from other subjects so the solutions are identified by the appropriate tutorial.
THERMODYNAMICS, FLUID AND PLANT PROCESSES The tutorials are drawn from other subjects so the solutions are identified by the appropriate tutorial. THERMODYNAMICS TUTORIAL 2 THERMODYNAMIC PRINCIPLES SAE
More informationTwo 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 informationSpeed Distribution at CONSTANT Temperature is given by the Maxwell Boltzmann Speed Distribution
Temperature ~ Average KE of each particle Particles have different speeds Gas Particles are in constant RANDOM motion Average KE of each particle is: 3/2 kt Pressure is due to momentum transfer Speed Distribution
More information5/6/ :41 PM. Chapter 6. Using Entropy. Dr. Mohammad Abuhaiba, PE
Chapter 6 Using Entropy 1 2 Chapter Objective Means are introduced for analyzing systems from the 2 nd law perspective as they undergo processes that are not necessarily cycles. Objective: introduce entropy
More informationGAS. Outline. Experiments. Device for in-class thought experiments to prove 1 st law. First law of thermodynamics Closed systems (no mass flow)
Outline First law of thermodynamics Closed systems (no mass flow) Device for in-class thought experiments to prove 1 st law Rubber stops GAS Features: Quasi-equlibrium expansion/compression Constant volume
More informationPhysics 111. Lecture 35 (Walker: ) Latent Heat Internal Energy First Law of Thermodynamics. Latent Heats. Latent Heat
Physics 111 Lecture 35 (Walker: 17.4-5) Latent Heat Internal Energy First Law of Thermodynamics Latent Heats The heat required to convert from one phase to another is called the latent heat. The latent
More informationFirst Law of Thermodynamics
First Law of Thermodynamics During an interaction between a system and its surroundings, the amount of energy gained by the system must be exactly equal to the amount of energy lost by the surroundings.
More informationRelationships between WORK, HEAT, and ENERGY. Consider a force, F, acting on a block sliding on a frictionless surface. x 2
Relationships between WORK, HEAT, and ENERGY Consider a force, F, acting on a block sliding on a frictionless surface x x M F x Frictionless surface M dv v dt M dv dt v F F F ; v mass velocity in x direction
More informationKNOWN: 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 informationMAE 110A. Homework 3: Solutions 10/20/2017
MAE 110A Homework 3: Solutions 10/20/2017 3.10: For H 2O, determine the specified property at the indicated state. Locate the state on a sketch of the T-v diagram. Given a) T 140 C, v 0.5 m 3 kg b) p 30MPa,
More informationCONCEPTS AND DEFINITIONS. Prepared by Engr. John Paul Timola
CONCEPTS AND DEFINITIONS Prepared by Engr. John Paul Timola ENGINEERING THERMODYNAMICS Science that involves design and analysis of devices and systems for energy conversion Deals with heat and work and
More informationName: 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 informationWhere 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 informationThe Kinetic Theory of Gases
PHYS102 Previous Exam Problems CHAPTER 19 The Kinetic Theory of Gases Ideal gas RMS speed Internal energy Isothermal process Isobaric process Isochoric process Adiabatic process General process 1. Figure
More informationThermodynamics 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 informationMAE 320 Thermodynamics HW 4 Assignment
MAE 0 Thermodynamics HW 4 Assignment The homework is de Friday, October 7 th, 06. Each problem is worth the points indicated. Copying of the soltion from any sorce is not acceptable. (). Mltiple choice
More informationWeek 5. Energy Analysis of Closed Systems. GENESYS Laboratory
Week 5. Energy Analysis of Closed Systems Objectives 1. Examine the moving boundary work or PdV work commonly encountered in reciprocating devices such as automotive engines and compressors 2. Identify
More informationChapter 3 First Law of Thermodynamics and Energy Equation
Fundamentals of Thermodynamics Chapter 3 First Law of Thermodynamics and Energy Equation Prof. Siyoung Jeong Thermodynamics I MEE0-0 Spring 04 Thermal Engineering Lab. 3. The energy equation Thermal Engineering
More informationRelationships between WORK, HEAT, and ENERGY. Consider a force, F, acting on a block sliding on a frictionless surface
Introduction to Thermodynamics, Lecture 3-5 Prof. G. Ciccarelli (0) Relationships between WORK, HEAT, and ENERGY Consider a force, F, acting on a block sliding on a frictionless surface x x M F x FRICTIONLESS
More informationLast Name: First Name: Purdue ID: Please write your name in BLOCK letters. Otherwise Gradescope may not recognize your name.
Solution Key Last Name: First Name: Purdue ID: Please write your name in BLOCK letters. Otherwise Gradescope may not recognize your name. CIRCLE YOUR LECTURE BELOW: MWF 10:30 am MWF 3:30 pm TR 8:30 am
More informationTeaching schedule *15 18
Teaching schedule Session *15 18 19 21 22 24 Topics 5. Gas power cycles Basic considerations in the analysis of power cycle; Carnot cycle; Air standard cycle; Reciprocating engines; Otto cycle; Diesel
More informationME 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 informationSHRI 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 informationEngineering Thermodynamics. Chapter 3. Energy Transport by Heat, Work and Mass
Chapter 3 Energy Transport y Heat, ork and Mass 3. Energy of a System Energy can e viewed as the aility to cause change. Energy can exist in numerous forms such as thermal, mechanical, kinetic, potential,
More informationU = 4.18 J if we heat 1.0 g of water through 1 C. U = 4.18 J if we cool 1.0 g of water through 1 C.
CHAPER LECURE NOES he First Law of hermodynamics: he simplest statement of the First Law is as follows: U = q + w. Here U is the internal energy of the system, q is the heat and w is the work. CONVENIONS
More informationDishwasher. Heater. Homework Solutions ME Thermodynamics I Spring HW-1 (25 points)
HW-1 (25 points) (a) Given: 1 for writing given, find, EFD, etc., Schematic of a household piping system Find: Identify system and location on the system boundary where the system interacts with the environment
More informationThe 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 informationChapter 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 informationChapter 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 informationTo 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 informationSpeed Distribution at CONSTANT Temperature is given by the Maxwell Boltzmann Speed Distribution
Temperature ~ Average KE of each particle Particles have different speeds Gas Particles are in constant RANDOM motion Average KE of each particle is: 3/2 kt Pressure is due to momentum transfer Speed Distribution
More informationHence. The second law describes the direction of energy transfer in spontaneous processes
* Heat and Work The first law of thermodynamics states that: Although energy has many forms, the total quantity of energy is constant. When energy disappears in one form, it appears simultaneously in other
More information2013, 2011, 2009, 2008 AP
Lecture 15 Thermodynamics I Heat vs. Temperature Enthalpy and Work Endothermic and Exothermic Reactions Average Bond Enthalpy Thermodynamics The relationship between chemical reactions and heat. What causes
More informationThe first law of thermodynamics continued
Lecture 7 The first law of thermodynamics continued Pre-reading: 19.5 Where we are The pressure p, volume V, and temperature T are related by an equation of state. For an ideal gas, pv = nrt = NkT For
More informationCHAPTER. The First Law of Thermodynamics: Closed Systems
CHAPTER 3 The First Law of Thermodynamics: Closed Systems Closed system Energy can cross the boundary of a closed system in two forms: Heat and work FIGURE 3-1 Specifying the directions of heat and work.
More informationME 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 informationDual 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 informationCHAPTER - 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 informationCHEMISTRY. CHM201 Class #10 CHEMISTRY. Chapter 5. Particulate Review. Thermochemistry: Energy Changes in Reactions
CHEMISTRY Fifth Edition Gilbert Kirss Foster Bretz Davies CHM201 Class #10 Chemistry, 5 th Edition Copyright 2017, W. W. Norton & Company CHEMISTRY Fifth Edition Gilbert Kirss Foster Bretz Davies Chapter
More information+ m B1 = 1. u A1. u B1. - m B1 = V A. /v A = , u B1 + V B. = 5.5 kg => = V tot. Table B.1.
5.6 A rigid tank is divided into two rooms by a membrane, both containing water, shown in Fig. P5.6. Room A is at 200 kpa, v = 0.5 m3/kg, VA = m3, and room B contains 3.5 kg at 0.5 MPa, 400 C. The membrane
More informationFINAL 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 information12/21/2014 7:39 PM. Chapter 2. Energy and the 1st Law of Thermodynamics. Dr. Mohammad Suliman Abuhaiba, PE
Chapter 2 Energy and the 1st Law of Thermodynamics 1 2 Homework Assignment # 2 Problems: 1, 7, 14, 20, 30, 36, 42, 49, 56 Design and open end problem: 2.1D Due Monday 22/12/2014 3 Work and Kinetic Energy
More informationThermodynamics. Internal Energy. Study of energy and its transformations Thermochemistry
Internal Energy 5.1- Thermodynamics Study of energy and its transformations Thermochemistry Study of energy changes that accompany chemical and physical changes. Energy the capacity to do work or transfer
More informationIdeal Gases. 247 minutes. 205 marks. theonlinephysicstutor.com. facebook.com/theonlinephysicstutor. Name: Class: Date: Time: Marks: Comments:
Ideal Gases Name: Class: Date: Time: 247 minutes Marks: 205 marks Comments: Page 1 of 48 1 Which one of the graphs below shows the relationship between the internal energy of an ideal gas (y-axis) and
More informationContent. 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 informationChapters 17 &19 Temperature, Thermal Expansion and The Ideal Gas Law
Chapters 17 &19 Temperature, Thermal Expansion and The Ideal Gas Law Units of Chapter 17 & 19 Temperature and the Zeroth Law of Thermodynamics Temperature Scales Thermal Expansion Heat and Mechanical Work
More informationChapter 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 informationCHAPTER 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 informationENERGY 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 informationIntroduction 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 informationProcess Nature of Process
AP Physics Free Response Practice Thermodynamics 1983B. The pv-diagram above represents the states of an ideal gas during one cycle of operation of a reversible heat engine. The cycle consists of the following
More informationT s change via collisions at boundary (not mechanical interaction)
Lecture 14 Interaction of 2 systems at different temperatures Irreversible processes: 2nd Law of Thermodynamics Chapter 19: Heat Engines and Refrigerators Thermal interactions T s change via collisions
More informationThe 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 informationMAE 320 HW 7B. 1e. For an isolated system, please circle the parameter which will change with time. (a) Total energy;
MAE 320 HW 7B his comprehensive homework is due Monday, December 5 th, 206. Each problem is worth the points indicated. Copying of the solution from another is not acceptable. Multi-choice, multi-answer
More information1.4 Perform the following unit conversions: (b) (c) s. g s. lb min. (d) (e) in. ft s. m 55 h. (f) ft s. km h. (g)
1.4 Perform the following unit conversions: 0.05 ft 1 in. (a) 1L 61in. 1L 1ft (b) 1kJ 650 J 10 J 1Btu 1.0551kJ 0.616 Btu (c) 41 Btu/h 0.15 kw 1kW 1h 600 s 778.17 ft lbf 1Btu ft lbf 99.596 s (d) g 78 s
More informationThis 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 informationChapter 10: Thermal Physics
Chapter 10: hermal Physics hermal physics is the study of emperature, Heat, and how these affect matter. hermal equilibrium eists when two objects in thermal contact with each other cease to echange energy.
More informationUNIVERSITY COLLEGE LONDON. University of London EXAMINATION FOR INTERNAL STUDENTS. For The Following Qualifications:-
UNIVERSITY COLLEGE LONDON University of London EXAMINATION FOR INTERNAL STUDENTS For The Following Qualifications:- B.Sc. M.Sci. Physics 1B28: Thermal Physics COURSE CODE : PHYSIB28 UNIT VALUE : 0.50 DATE
More informationDr 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 informationME Thermodynamics I. Lecture Notes and Example Problems
ME 227.3 Thermodynamics I Lecture Notes and Example Problems James D. Bugg September 2018 Department of Mechanical Engineering Introduction Part I: Lecture Notes This part contains handout versions of
More informationThermodynamics 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 informationAP Physics Thermodynamics Wrapup
AP Physics hermodynamics Wrapup Here are your basic equations for thermodynamics. here s a bunch of them. l l 0 Q ml Q his is the equation for the change in length of an object as a function of temperature.
More informationThermodynamics II. Week 9
hermodynamics II Week 9 Example Oxygen gas in a piston cylinder at 300K, 00 kpa with volume o. m 3 is compressed in a reversible adiabatic process to a final temperature of 700K. Find the final pressure
More informationClassification 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 informationME 201 Thermodynamics
ME 0 Thermodynamics Solutions First Law Practice Problems. Consider a balloon that has been blown up inside a building and has been allowed to come to equilibrium with the inside temperature of 5 C and
More informationNumber of extra papers used if any
Last Nae: First Nae: Thero no. ME 00 Therodynaics 1 Fall 018 Exa 1 Circle your instructor s last nae Division 1 (7:0): Naik Division (1:0): Wassgren Division 6 (11:0): Sojka Division (9:0): Choi Division
More informationME 200 Exam 2 October 16, :30 p.m. to 7:30 p.m.
CIRCLE YOUR LECTURE BELOW: First Name Solution Last Name 7:30 am 8:30 am 10:30 am 11:30 am Joglekar Bae Gore Abraham 1:30 pm 3:30 pm 4:30 pm Naik Naik Cheung ME 200 Exam 2 October 16, 2013 6:30 p.m. to
More informationChapter Four fluid flow mass, energy, Bernoulli and momentum
4-1Conservation of Mass Principle Consider a control volume of arbitrary shape, as shown in Fig (4-1). Figure (4-1): the differential control volume and differential control volume (Total mass entering
More informationCHEM Thermodynamics. Work. There are two ways to change the internal energy of a system:
There are two ways to change the internal energy of a system: Thermodynamics Work 1. By flow of heat, q Heat is the transfer of thermal energy between and the surroundings 2. By doing work, w Work can
More informationTwo mark questions and answers UNIT II SECOND LAW 1. Define Clausius statement. It is impossible for a self-acting machine working in a cyclic process, to transfer heat from a body at lower temperature
More informationConsequences of Second Law of Thermodynamics. Entropy. Clausius Inequity
onsequences of Second Law of hermodynamics Dr. Md. Zahurul Haq Professor Department of Mechanical Engineering Bangladesh University of Engineering & echnology BUE Dhaka-000, Bangladesh zahurul@me.buet.ac.bd
More information(a) How much work is done by the gas? (b) Assuming the gas behaves as an ideal gas, what is the final temperature? V γ+1 2 V γ+1 ) pdv = K 1 γ + 1
P340: hermodynamics and Statistical Physics, Exam#, Solution. (0 point) When gasoline explodes in an automobile cylinder, the temperature is about 2000 K, the pressure is is 8.0 0 5 Pa, and the volume
More informationChapter 8. The increased awareness that the world s energy EXERGY: A MEASURE OF WORK POTENTIAL. Objectives
Chapter 8 EXERGY: A MEASURE OF WORK POTENTIAL The increased awareness that the world s energy resources are limited has caused many countries to reexamine their energy policies and take drastic measures
More informationFirst Law of Thermodynamics
CH2303 Chemical Engineering Thermodynamics I Unit II First Law of Thermodynamics Dr. M. Subramanian 07-July-2011 Associate Professor Department of Chemical Engineering Sri Sivasubramaniya Nadar College
More informationME 200 Thermodynamics 1 Fall 2017 Exam 3
ME 200 hermodynamics 1 Fall 2017 Exam Circle your structor s last name Division 1: Naik Division : Wassgren Division 6: Braun Division 2: Sojka Division 4: Goldenste Division 7: Buckius Division 8: Meyer
More information19-9 Adiabatic Expansion of an Ideal Gas
19-9 Adiabatic Expansion of an Ideal Gas Learning Objectives 19.44 On a p-v diagram, sketch an adiabatic expansion (or contraction) and identify that there is no heat exchange Q with the environment. 19.45
More informationThermodynamic Systems
Thermodynamic Systems For purposes of analysis we consider two types of Thermodynamic Systems: Closed System - usually referred to as a System or a Control Mass. This type of system is separated from its
More informationLecture 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 informationThe laws of Thermodynamics. Work in thermodynamic processes
The laws of Thermodynamics ork in thermodynamic processes The work done on a gas in a cylinder is directly proportional to the force and the displacement. = F y = PA y It can be also expressed in terms
More informationFinal Examination ( )
Ministry of high education& scientific Research University of echnology Materials engineering department Class: Second Year Subject: Chemical Metallurgy Examiner: Final Examination (0-0) وزارة التعليم
More information20 m neon m propane. g 20. Problems with solutions:
Problems with solutions:. A -m tank is filled with a gas at room temperature 0 C and pressure 00 Kpa. How much mass is there if the gas is a) Air b) Neon, or c) Propane? Given: T7K; P00KPa; M air 9; M
More information