Cyclic Processes. water

Similar documents
Process Nature of Process

1985B4. A kilogram sample of a material is initially a solid at a temperature of 20 C. Heat is added to the sample at a constant rate of 100

TB [103 marks] The damping of the system is now increased. Which describes the change in ƒ 0 and the change in A 0?

Physics 202 Homework 5

The Kinetic Theory of Gases

Chapter 19: The Kinetic Theory of Gases Questions and Example Problems

THERMODYNAMICS CONCEPTUAL PROBLEMS

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

Chapter 19. First Law of Thermodynamics. Dr. Armen Kocharian, 04/04/05

, is placed in thermal contact with object B, with mass m, specific heat c B. and initially at temperature T B

A thermodynamic system is taken from an initial state X along the path XYZX as shown in the PV-diagram.

The first law of thermodynamics continued

Survey of Thermodynamic Processes and First and Second Laws

Chapter 20. Heat Engines, Entropy and the Second Law of Thermodynamics. Dr. Armen Kocharian

Chapter 19 The First Law of Thermodynamics

Unit 05 Kinetic Theory of Gases

The goal of thermodynamics is to understand how heat can be converted to work. Not all the heat energy can be converted to mechanical energy

Speed Distribution at CONSTANT Temperature is given by the Maxwell Boltzmann Speed Distribution

Conservation of Energy

MULTIPLE CHOICE. Choose the one alternative that best completes the statement or answers the question.

AP PHYSICS 2 WHS-CH-15 Thermodynamics Show all your work, equations used, and box in your answers!

Chapter 14 Thermal Physics: A Microscopic View

Heat and Thermodynamics. February. 2, Solution of Recitation 2. Consider the first case when air is allowed to expand isothermally.

Answer: Volume of water heated = 3.0 litre per minute Mass of water heated, m = 3000 g per minute Increase in temperature,

Speed Distribution at CONSTANT Temperature is given by the Maxwell Boltzmann Speed Distribution

CH 15. Zeroth and First Law of Thermodynamics

First Law of Thermodynamics Second Law of Thermodynamics Mechanical Equivalent of Heat Zeroth Law of Thermodynamics Thermal Expansion of Solids

Thermodynamics: The Laws

THERMODYNAMICS. Zeroth law of thermodynamics. Isotherm

Chapter 19. Heat Engines

11/22/11. If you add some heat to a substance, is it possible for the temperature of the substance to remain unchanged?


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

Downloaded from

CHAPTER - 12 THERMODYNAMICS

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

S15--AP Phys Q4--Heat-Thermo Ch13_14_15 PRACTICE

08/26/09 PHYSICS 223 Exam-2 NAME Please write down your name also on the back side of this exam

NOTE: Only CHANGE in internal energy matters

2/18/2019. Ideal-Gas Processes. Thermodynamics systems. Thermodynamics systems

Thermodynamics systems

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

Chapter 19. Heat Engines

a. 4.2x10-4 m 3 b. 5.5x10-4 m 3 c. 1.2x10-4 m 3 d. 1.4x10-5 m 3 e. 8.8x10-5 m 3

Physics 111. Thursday, Dec. 9, 3-5pm and 7-9pm. Announcements. Thursday, December 9, 2004

AP Physics Thermodynamics Wrapup

Physics 4C Chapter 19: The Kinetic Theory of Gases

PHY 206 SPRING Problem #1 NAME: SIGNATURE: UM ID: Problem #2. Problem #3. Total. Prof. Massimiliano Galeazzi. Midterm #2 March 8, 2006

MCQs THERMODYNAMICS. Physics Without Fear.

Part I: Basic Concepts of Thermodynamics

Entropy & the Second Law of Thermodynamics

19-9 Adiabatic Expansion of an Ideal Gas

Physics 5D PRACTICE FINAL EXAM Fall 2013

Chapter 12. The Laws of Thermodynamics

Unified Quiz: Thermodynamics

First Law of Thermodynamics

The laws of Thermodynamics. Work in thermodynamic processes

Physics 115. Specific heats revisited Entropy. General Physics II. Session 13

Irreversible Processes

Classification following properties of the system in Intensive and Extensive

Ideal Gases. 247 minutes. 205 marks. theonlinephysicstutor.com. facebook.com/theonlinephysicstutor. Name: Class: Date: Time: Marks: Comments:

UNIVERSITY COLLEGE LONDON. University of London EXAMINATION FOR INTERNAL STUDENTS. For The Following Qualifications:-

Inconsistency of Carnot Principle and Second Law of Thermodynamics. Charanjeet Singh Bansrao. Abstract

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

ADIABATIC PROCESS Q = 0

HEAT- I Part - A C D A B. Te m p. Heat input

Phys 22: Homework 10 Solutions W A = 5W B Q IN QIN B QOUT A = 2Q OUT 2 QOUT B QIN B A = 3Q IN = QIN B QOUT. e A = W A e B W B A Q IN.

PHYS102 Previous Exam Problems. Temperature, Heat & The First Law of Thermodynamics

Thermal Physics. Topics to be covered. Slide 2 / 105. Slide 1 / 105. Slide 3 / 105. Slide 4 / 105. Slide 5 / 105. Slide 6 / 105.

Renewable Energy. Theory: The Ideal Gas Law The equation of state for an ideal gas is written: PV = nrt

THERMODYNAMICS b) If the temperatures of two bodies are equal then they are said to be in thermal equilibrium.

Simpo PDF Merge and Split Unregistered Version -

Irreversible Processes

Three special ideal gas processes: one of, W or Q is 0

12.1 Work in Thermodynamic Processes

Materials at Equilibrium. G. Ceder Fall 2001 COURSE 3.20: THERMODYNAMICS OF MATERIALS. FINAL EXAM, Dec 18, 2001

Topic 3 &10 Review Thermodynamics

Heat Engines and the Second Law of Thermodynamics

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

UNIVERSITY OF SOUTHAMPTON

THERMODYNAMICS. Chapter Twelve MCQ I

Handout 12: Thermodynamics. Zeroth law of thermodynamics

PhysicsAndMathsTutor.com 1

C e. Negative. In a clockwise cycle, the work done on the gas is negative. Or for the cycle Qnet = +600 J and U = 0 so W = Q = 600 J

First Name: Last Name: Section: 1 December 20, 2004 Physics 201 FINAL EXAM

Lecture 25 Goals: Chapter 18 Understand the molecular basis for pressure and the idealgas

Chapter 17. Work, Heat, and the First Law of Thermodynamics Topics: Chapter Goal: Conservation of Energy Work in Ideal-Gas Processes

Niraj Sir THERMODYNAMICS

Summarizing, Key Point: An irreversible process is either spontaneous (ΔS universe > 0) or does not occur (ΔS universe < 0)

Physics 2 week 7. Chapter 3 The Kinetic Theory of Gases

Unified Thermodynamics Quiz 1

(f ) From the graph, obtain the height of the tube given the mass of the dart is 20 grams and the constant force applied in the tube is 2 newtons.

S6. (a) State what is meant by an ideal gas...

Regents Chemistry: Thermodynamics and Gas Laws Test [Practice]

UNIVERSITY OF SOUTHAMPTON

Chapter 1: FUNDAMENTAL CONCEPTS OF THERMODYNAMICS AND VARIOUS THERMODYMIC PROCESSES

HEAT, WORK, AND THE FIRST LAW OF THERMODYNAMICS

More Thermodynamics. Specific Specific Heats of a Gas Equipartition of Energy Reversible and Irreversible Processes

Handout 12: Thermodynamics. Zeroth law of thermodynamics

(Heat capacity c is also called specific heat) this means that the heat capacity number c for water is 1 calorie/gram-k.

Transcription:

Name Cyclic Processes Cyclic Processes A fixed quantity of ideal gas is contained within a metal cylinder that is sealed with a movable, frictionless, insulating piston. (The piston can move up or down without the slightest resistance from friction, but no gas can enter or leave the cylinder. The piston is heavy, but there can be no heat transfer to or from the piston itself.) The cylinder is surrounded by a large container of water with high walls as shown. We are going to describe two separate processes, Process #1 and Process #2. movable piston Time A ideal gas water Entire system at room temperature. At initial time A, the gas, cylinder, and water have all been sitting in a room for a long period of time, and all of them are at room temperature. Step 1. We now begin Process #1: The water container is gradually heated, and the piston very slowly moves upward. At time B the heating of the water stops, and the piston stops moving when it is in the position shown in the diagram below: Time B Piston in new position. Temperature of system has changed. Question #1: During the process that occurs from time A to time B, which of the following is true: (a) positive work is done on the gas by the environment, (b) positive work is done by the gas on the environment, (c) no net work is done on or by the gas. Question #2: During the process that occurs from time A to time B, the gas absorbs x joules of energy from the water. Which of the following is true: The total kinetic energy of all of the gas molecules (a) increases by more than x joules; (b) increases by x joules; (c) increases, but by less than x joules; (d) remains unchanged; (e) decreases by less than x joules; (f) decreases by x joules; (g) decreases by more than x joules. Explain your answer: 1

Step 2. Now, empty containers are placed on top of the piston as shown. Small lead weights are gradually placed in the containers, one by one, and the piston is observed to move down slowly. While this happens, the temperature of the water is nearly unchanged, and the gas temperature remains practically constant. (That is, it remains at the temperature it reached at time B, after the water had been heated up.) containers lead weight weights being added Piston moves down slowly. Temperature remains same as at time B. Step 3. At time C we stop adding lead weights to the container and the piston stops moving. (The weights that we have already added up until now are still in the containers.) The piston is now found to be at exactly the same position it was at time A. Time C Weights in containers. Piston in same position as at time A. Temperature same as at time B. Question #3: During the process that occurs from time B to time C, does the total kinetic energy of all the gas molecules increase, decrease, or remain unchanged? Question #4: During the process that occurs from time B to time C, is there any net energy flow between the gas and the water? If no, explain why not. If yes, is there a net flow of energy from gas to water, or from water to gas? Explain your answer: 2

Step 4. Now, the piston is locked into place so it cannot move; the weights are removed from the piston. The system is left to sit in the room for many hours, and eventually the entire system cools back down to the same room temperature it had at time A. When this finally happens, it is time D. Time D Piston in same position as at time A. Temperature same as at time A. Question #5: During the process that occurs from time C to time D, the water absorbs y joules of energy from the gas. Which of the following is true: The total kinetic energy of all of the gas molecules (a) increases by more than y joules; (b) increases by y joules; (c) increases, but by less than y joules; (d) remains unchanged; (e) decreases, by less than y joules; (f) decreases by y joules; (g) decreases by more than y joules. Question #6: Consider the entire process from time A to time D. (i) Is the net work done by the gas on the environment during that process (a) greater than zero, (b) equal to zero, or (c) less than zero? Explain your answer: (ii) Is the total heat transfer to the gas during that process (a) greater than zero, (b) equal to zero, or (c) less than zero? Explain your answer: 3

Now let us begin Process #2. The piston is unlocked so it is again free to move. We start from the same initial situation as shown at time A and D (i.e., same temperature and position of the piston). Just as before, we heat the water and watch as the piston rises. However, this time, we will heat the water for a longer period of time. As a result, the piston ends up higher than it was at time B. Step 5. Step 6. Now, weights are added to the piston and it begins to move down. (Temperature does not change during this process.) However, this time, more weights than before must be added to get the piston back to the position it had at time C. Again, the piston is locked and the weights are removed. After many hours, the system returns to the same temperature that it had at time A and time D (and the piston is in the same position as it was at those times). This final state occurs at time E. Question #7: Consider the total kinetic energy of all of the gas molecules at times A, D, and E; call those E A, E D, and E E. Rank these in order of magnitude (greatest to least, using > or < signs). If two or more of these are equal, indicate that with an = sign. Explain your answer: Question #8: Consider the following positive quantities: Q 1, Q2, W1, W2. These represent the absolute values of the total heat transfer to the gas during Process #1 and Process #2, and of the net work done by the gas during Processes #1 and #2. Rank these four quantities from largest to smallest. If two or more are equal, indicate with = sign. Explain your answer: Question #9: Sketch a P-V diagram of Process #1 and Process #2 on the same set of axes; label (with the appropriate letter) the states that occur at times A, B, C, D, and E. (Use the other side of this sheet if necessary.) Explain how you can use the diagram to justify your answer to Question #8. 4

Question #10: A. For the process A B: i. Is the work done by the system (W AB ) positive, negative, or zero? ii. Is heat transferred to the system, away from the system, or is there no heat transfer? iii. Does the internal energy increase, decrease, or remain the same? Explain. B. For the process B C: i. Is the work done by the system (W BC ) positive, negative, or zero? ii. Is heat transferred to the system, away from the system, or is there no heat transfer? iii. Does the internal energy increase, decrease, or remain the same? Explain. C. For the process C D: i. Is the work done by the system (W CD ) positive, negative, or zero? ii. Is heat transferred to the system, away from the system, or is there no heat transfer? iii. Does the internal energy increase, decrease, or remain the same? Explain. 5

Question #11: Rank the absolute values W AB, W BC, and W CD from largest to smallest; if two or more are equal, indicate with an = sign. largest smallest Explain your reasoning. Question #12: Rank the absolute values of internal energy change U AB, U BC, and U CD from largest to smallest; if two or more are equal, indicate with an = sign. largest smallest Explain your reasoning. Question #13: Rank the absolute values of heat transfer Q AB, Q BC, and Q CD from largest to smallest; if two or more are equal, indicate with an = sign. Assume that the low temperature is 300 K, and the high temperature is 600 K. largest smallest Explain your reasoning. 6

Question #14: Are your answers to Questions #11, 12, and 13 consistent with your answers to parts (i) and (ii) of Question #6? Explain. Question #15: Is the net change in volume from time A to time D (V D V A ) greater than zero, equal to zero, or less than zero? Is this consistent with your answers to Questions #6(i) and #14? Explain. Question #16: Is the net change in temperature from time A to time D (T D T A ) greater than zero, equal to zero, or less than zero? Is this consistent with your answers to Questions #6(ii) and #14? Explain. 7

A Sample Cyclic Process A thermodynamic system undergoes a three-step process. An adiabatic expansion takes it from state 1 to state 2; heat is added at constant pressure to move the system to state 3; and an isothermal compression returns the system to state 1. The system consists of a diatomic ideal gas with C V = 5R/2. The number of moles is chosen so nr = 100 J/K. The following information is known about states 2 and 3. Pressure: P 2 = P 3 = 100 kpa Volume: V 3 = 0.5 m 3 What is the temperature of the system in state 3? The system does 20000 J of work in the constant pressure process that takes it from state 2 to state 3. What is the volume and temperature of the system in state 2? V 2 = T 2 = Complete the table below, filling in the missing numerical values, with units of joules. The total work done by the system in the cycle is 19400 J. Note that there is a way to do this without integrating or using logarithms. Process Q E W int 1 2 2 3 20000 3 1 Complete cycle -19400 Step 1: First fill in all the terms that are zero. Remember that each row in the table satisfies the First Law of Thermodynamics. Also remember that Eint = ncv T. Chapter 15 The Laws of Thermodynamics Page 9