Thermodynamics and Atomic Physics II

Size: px
Start display at page:

Download "Thermodynamics and Atomic Physics II"

Transcription

1 Thermodynamics and Atomic Physics II 1. Heat from a source at 550 K is added to the working fluid of an engine operating at a steady rate. The temperature of the surroundings is 300 K. The efficiency of this process is defined as the ratio of the mechanical power produced by the engine to the rate at which heat is provided. The maximum efficiency of this engine is: (a) much greater than 1. (b) about equal to 1. (c) much less than 1. (d) impossible to determine. 2. To determine the efficiency of a piston-and-cylinder based engine that uses air as a working fluid, the properties of which substances need to be known? (a) The air in the engine. (b) The metal of the engines pistons and cylinders. (c) The atmosphere surrounding the engine. (d) Both the engine air and the metal material. (e) All of the engine air, the engine metal, and the surrounding atmosphere. 3. An electric water heater consists of a perfectly-insulated tank filled with water and fitted with an electric heating element. Water enters the tank at 10 C and exits at 50 C at a pressure greater than 1 atm. The efficiency of the water heating process is defined as the energy provided to the water divided by the electrical energy provided to the heating element. The efficiency of the water heating process is: (a) much greater than 1. (b) about equal to 1. (c) much less than 1. (d) impossible to determine. For the next three questions: Air at high pressure and ambient temperature is contained in a perfectly insulated piston-cylinder device. Stops prevent the piston from moving up. The stops are then removed, and the piston quickly rises until a second set of stops (that prevents the piston from leaving the cylinder) is encountered. 4. The temperature of the air: (a) increases. (b) remains the same. (c) decreases. (d) cannot be determined. 5. The energy of the air in the cylinder: (a) increases. (b) remains the same. (c) decreases. (d) cannot be determined. 6. Work is done by the air in this process. (a) True. 1

2 (b) False. (c) Impossible to tell. 7. Three processes compose a thermodynamic cycle (see the pv diagram below). Process 1 2 takes place isothermally. Process 2 3 takes place isochorically, and process 3 1 is adiabatic. During the complete cycle, the total amount of work done is 10 J. During process 2 3, the internal energy decreases by 20 J; and during process 3 1, 20 J of work is done on the system. How much heat is added to the system during process 1 2? (b) 10 J (c) 20 J (d) 30 J (e) 40 J 8. The root mean square velocity of oxygen gas is v at room temperature. What is the root mean square velocity of hydrogen gas at the same temperature? (a) 16v (b) 4v (c) v (d) v/4 (e) v/16 9. A Carnot cycle takes in 1000 J of heat at a high temperature of 400 K. How much heat is expelled at the cooler temperature of 300 K? (b) 250 J (c) 500 J (d) 750 J (e) 1000 J 10. An ideal gas is expanded at constant pressure from an initial volume V i and an initial temperature T i to a final volume V f and final temperature T f. The gas has molar heat capacity C P at constant pressure. The amount of work done by n moles of the gas during the process can be expressed: (b) nrt i ln (V f /V i ) (c) C P n(t f T i ) (d) nk(v f V i ) (e) nr(t f T i ) 2

3 11. To raise the temperature of an ideal gas by 150 K, 6300 joules are required if the gas is heated isochorically, while 8800 joules are required if it is heated isobarically. How much does the internal energy of the gas change when its temperature is raised by 150 K? (a) 2500 J (b) 6300 J (c) 8800 J (d) 11,300 J (e) 15,100 J 12. Which of the following PV plots best represents an isothermal process? (a) (b) (c) (d) (e) 13. One end of a metal rod of length L and cross-sectional area A is held at constant temperature T 1. The other end is held at constant temperature T 2. Which of the following statements about the amount of heat transferred through the rod per unit time are true? I. The rate of heat transfer is proportional to 1/(T 1 T 2 ). II. The rate of heat transfer is proportional to A. III. The rate of heat transfer is proportional to L. (a) II only. (b) III only. (c) I and II only. (d) I and III only. (e) II and III only. 14. A mole of ideal gas at STP is heated in an insulated constant volume container until the average velocity of its molecules doubled. Its pressure would therefore increase by what factor?.5 3

4 (b) 1 (c) 2 (d) 4 (e) The momentum p of a photon is given by the equation p = h λ where h is Plancks constant and λ is the photons wavelength. In terms of p, the photon s energy is (a) E γ = phc (b) E γ = ph/c (c) E γ = p/c (d) E γ = pc (e) E γ = h/pc 16. The photoelectric work function of a metal surface is Φ. The thermionic work function of the same metal surface will be (a) less than Φ. (b) equal to Φ. (c) greater than Φ. (d) independent of Φ. (e) dependent on the heating method. 17. In an experiment, light of a particular wavelength is incident on a metal surface, and electrons are emitted from the surface as a result. To produce more electrons per unit time but with less kinetic energy per electron, the experimenter should do which of the following? (a) Increase the intensity and decrease the wavelength of the light. (b) Increase the intensity and the wavelength of the light. (c) Decrease the intensity and the wavelength of the light. (d) Decrease the intensity and increase the wavelength of the light. (e) None of the above would produce the desired result. 18. The classical planetary model of the hydrogen atom is unacceptable because (a) the Coulomb force is too week to hold the electron. (b) the nuclear force is too strong to allow the electrons to orbit. (c) the electron is accelerating and must radiate away its energy. (d) the electron s angular momentum is not conserved, as it should be. (e) of some other reason. 19. When a photon is Compton-scattered, the (a) minimum shift λ will be twice the Compton wavelength. (b) minimum shift λ will be h times the Compton wavelength. (c) maximum shift λ will be h times the Compton wavelength. (d) maximum shift λ will be twice the Compton wavelength. 4

5 (e) shift λ will be impossible to predict. 20. The energy per unit area per unit time radiate by a blackbody (a) depends on the mass of the blackbody. (b) depends on the color of the blackbody. (c) depends on its temperature. (d) depends on its total surface area. (e) depends on something other than the things mentioned. 5

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

A thermodynamic system is taken from an initial state X along the path XYZX as shown in the PV-diagram. AP Physics Multiple Choice Practice Thermodynamics 1. The maximum efficiency of a heat engine that operates between temperatures of 1500 K in the firing chamber and 600 K in the exhaust chamber is most

More information

Physics 5D PRACTICE FINAL EXAM Fall 2013

Physics 5D PRACTICE FINAL EXAM Fall 2013 Print your name: Physics 5D PRACTICE FINAL EXAM Fall 2013 Real Exam is Wednesday December 11 Thimann Lecture 3 4:00-7:00 pm Closed book exam two 8.5x11 sheets of notes ok Note: Avogadro s number N A =

More information

The first law of thermodynamics continued

The 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 information

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

AP PHYSICS 2 WHS-CH-15 Thermodynamics Show all your work, equations used, and box in your answers! AP PHYSICS 2 WHS-CH-15 Thermodynamics Show all your work, equations used, and box in your answers! Nicolas Léonard Sadi Carnot (1796-1832) Sadi Carnot was a French military engineer and physicist, often

More information

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

Speed 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 information

Chapter 19 The First Law of Thermodynamics

Chapter 19 The First Law of Thermodynamics Chapter 19 The First Law of Thermodynamics The first law of thermodynamics is an extension of the principle of conservation of energy. It includes the transfer of both mechanical and thermal energy. First

More information

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

Chapter 17. Work, Heat, and the First Law of Thermodynamics Topics: Chapter Goal: Conservation of Energy Work in Ideal-Gas Processes Chapter 17. Work, Heat, and the First Law of Thermodynamics This false-color thermal image (an infrared photo) shows where heat energy is escaping from a house. In this chapter we investigate the connection

More information

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

MULTIPLE CHOICE. Choose the one alternative that best completes the statement or answers the question. CH. 19 PRACTICE Name MULTIPLE CHOICE. Choose the one alternative that best completes the statement or answers the question. 1) When a fixed amount of ideal gas goes through an isobaric expansion, A) its

More information

Kinetic Theory continued

Kinetic Theory continued Chapter 12 Kinetic Theory continued 12.4 Kinetic Theory of Gases The particles are in constant, random motion, colliding with each other and with the walls of the container. Each collision changes the

More information

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

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

More information

Kinetic Theory continued

Kinetic Theory continued Chapter 12 Kinetic Theory continued 12.4 Kinetic Theory of Gases The particles are in constant, random motion, colliding with each other and with the walls of the container. Each collision changes the

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

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

The Kinetic Theory of Gases

The 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 information

The laws of Thermodynamics. Work in thermodynamic processes

The 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 information

CHEM Thermodynamics. Work. There are two ways to change the internal energy of a system:

CHEM 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 information

Process Nature of Process

Process 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 information

Chapter 12. The Laws of Thermodynamics

Chapter 12. The Laws of Thermodynamics Chapter 12 The Laws of Thermodynamics First Law of Thermodynamics The First Law of Thermodynamics tells us that the internal energy of a system can be increased by Adding energy to the system Doing work

More information

Thermodynamics I - Enthalpy

Thermodynamics I - Enthalpy Thermodynamics I - Enthalpy Tinoco Chapter 2 Secondary Reference: J.B. Fenn, Engines, Energy and Entropy, Global View Publishing, Pittsburgh, 2003. 1 Thermodynamics CHEM 2880 - Kinetics An essential foundation

More information

Unit 05 Kinetic Theory of Gases

Unit 05 Kinetic Theory of Gases Unit 05 Kinetic Theory of Gases Unit Concepts: A) A bit more about temperature B) Ideal Gas Law C) Molar specific heats D) Using them all Unit 05 Kinetic Theory, Slide 1 Temperature and Velocity Recall:

More information

Physics Fall Mechanics, Thermodynamics, Waves, Fluids. Lecture 32: Heat and Work II. Slide 32-1

Physics Fall Mechanics, Thermodynamics, Waves, Fluids. Lecture 32: Heat and Work II. Slide 32-1 Physics 1501 Fall 2008 Mechanics, Thermodynamics, Waves, Fluids Lecture 32: Heat and Work II Slide 32-1 Recap: the first law of thermodynamics Two ways to raise temperature: Thermally: flow of heat Energy

More information

Downloaded from

Downloaded from Chapter 13 (Kinetic Theory) Q1. A cubic vessel (with face horizontal + vertical) contains an ideal gas at NTP. The vessel is being carried by a rocket which is moving at a speed of500 ms in vertical direction.

More information

A) 2.0 atm B) 2.2 atm C) 2.4 atm D) 2.9 atm E) 3.3 atm

A) 2.0 atm B) 2.2 atm C) 2.4 atm D) 2.9 atm E) 3.3 atm Name: Date: 1. On a cold day ( 3 C), the gauge pressure on a tire reads 2.0 atm. If the tire is heated to 27 C, what will be the absolute pressure of the air inside the tire? A) 2.0 atm B) 2.2 atm C) 2.4

More information

Conservation of Energy

Conservation of Energy Conservation of Energy Energy can neither by created nor destroyed, but only transferred from one system to another and transformed from one form to another. Conservation of Energy Consider at a gas in

More information

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

(Heat capacity c is also called specific heat) this means that the heat capacity number c for water is 1 calorie/gram-k. Lecture 23: Ideal Gas Law and The First Law of Thermodynamics 1 (REVIEW) Chapter 17: Heat Transfer Origin of the calorie unit A few hundred years ago when people were investigating heat and temperature

More information

Handout 12: Thermodynamics. Zeroth law of thermodynamics

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

More information

UNIVERSITY OF SOUTHAMPTON

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

More information

(prev) (top) (next) (Throughout, we will assume the processes involve an ideal gas with constant n.)

(prev) (top) (next) (Throughout, we will assume the processes involve an ideal gas with constant n.) 1 of 9 8/22/12 9:51 PM (prev) (top) (next) Thermodynamics 1 Thermodynamic processes can be: 2 isothermal processes, ΔT = 0 (so P ~ 1 / V); isobaric processes, ΔP = 0 (so T ~ V); isovolumetric or isochoric

More information

CHAPTER 3 TEST REVIEW

CHAPTER 3 TEST REVIEW IB PHYSICS Name: Period: Date: # Marks: 52 Raw Score: IB Curve: DEVIL PHYSICS BADDEST CLASS ON CAMPUS CHAPTER 3 TEST REVIEW 1. Water at a temperature of 0 C is kept in a thermally insulated container.

More information

The First Law of Thermodynamics

The First Law of Thermodynamics Thermodynamics The First Law of Thermodynamics Thermodynamic Processes (isobaric, isochoric, isothermal, adiabatic) Reversible and Irreversible Processes Heat Engines Refrigerators and Heat Pumps The Carnot

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

On my honor as a Texas A&M University student, I will neither give nor receive unauthorized help on this exam.

On my honor as a Texas A&M University student, I will neither give nor receive unauthorized help on this exam. Physics 201, Exam 4 Name (printed) On my honor as a Texas A&M University student, I will neither give nor receive unauthorized help on this exam. Name (signed) The multiple-choice problems carry no partial

More information

Each of the following 50 questions are worth 2 points each. Answer a = true b = false

Each of the following 50 questions are worth 2 points each. Answer a = true b = false PHY 262 Exam 3-----preview----- 8/7/2012 NAME This exam is closed book and closed notes, but open calculator. You have about 80 minutes to complete the exam (~ 9:30 10:50). The actual exam will be 50 questions

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

Explain how Planck resolved the ultraviolet catastrophe in blackbody radiation. Calculate energy of quanta using Planck s equation.

Explain how Planck resolved the ultraviolet catastrophe in blackbody radiation. Calculate energy of quanta using Planck s equation. Objectives Explain how Planck resolved the ultraviolet catastrophe in blackbody radiation. Calculate energy of quanta using Planck s equation. Solve problems involving maximum kinetic energy, work function,

More information

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

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 1985B4. A 0.020-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 joules per second until the temperature increases to 60

More information

CHEMISTRY Matter and Change. Chapter 13: Gases

CHEMISTRY Matter and Change. Chapter 13: Gases CHEMISTRY Matter and Change Chapter 13: Gases CHAPTER 13 Table Of Contents Section 13.1 Section 13.2 Section 13.3 The Gas Laws The Ideal Gas Law Gas Stoichiometry Click a hyperlink to view the corresponding

More information

Reversible Processes. Furthermore, there must be no friction (i.e. mechanical energy loss) or turbulence i.e. it must be infinitely slow.

Reversible Processes. Furthermore, there must be no friction (i.e. mechanical energy loss) or turbulence i.e. it must be infinitely slow. Reversible Processes A reversible thermodynamic process is one in which the universe (i.e. the system and its surroundings) can be returned to their initial conditions. Because heat only flows spontaneously

More information

Lecture 24. Paths on the pv diagram

Lecture 24. Paths on the pv diagram Goals: Lecture 24 Chapter 17 Apply heat and energy transfer processes Recognize adiabatic processes Chapter 18 Follow the connection between temperature, thermal energy, and the average translational kinetic

More information

Phase Changes and Latent Heat

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

More information

Niraj Sir THERMODYNAMICS

Niraj Sir THERMODYNAMICS THERMODYNAMICS Thermal Equilibrium:- Two systems are said to be in thermal equilibrium with each other if they have the same temperature. Thermo dynamical system:- An assembly of large numbers of particles

More information

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

Chapter 20. Heat Engines, Entropy and the Second Law of Thermodynamics. Dr. Armen Kocharian Chapter 20 Heat Engines, Entropy and the Second Law of Thermodynamics Dr. Armen Kocharian First Law of Thermodynamics Review Review: The first law states that a change in internal energy in a system can

More information

Physics 202 Homework 5

Physics 202 Homework 5 Physics 202 Homework 5 Apr 29, 2013 1. A nuclear-fueled electric power plant utilizes a so-called boiling water reac- 5.8 C tor. In this type of reactor, nuclear energy causes water under pressure to boil

More information

THERMODYNAMICS. Zeroth law of thermodynamics. Isotherm

THERMODYNAMICS. Zeroth law of thermodynamics. Isotherm 12 THERMODYNAMICS Zeroth law of thermodynamics Two systems separately in thermal equilibrium with a third system are in thermal equilibrium with each other. Isotherm It is the graph connecting pressure

More information

People s Physics book 3e

People s Physics book 3e The Big Ideas Heat is a form of energy transfer. It can change the kinetic energy of a substance. For example, the average molecular kinetic energy of gas molecules is related to temperature. A heat engine

More information

Simpo PDF Merge and Split Unregistered Version -

Simpo PDF Merge and Split Unregistered Version - 74. The rate of heat flow by conduction through a slab does NOT depend upon the: A. temperature difference between opposite faces of the slab B. thermal conductivity of the slab C. slab thickness D. cross-sectional

More information

CHAPTER - 12 THERMODYNAMICS

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

More information

Chapter 19. Heat Engines

Chapter 19. Heat Engines Chapter 19 Heat Engines Thermo Processes Eint = Q+ W Adiabatic No heat exchanged Q = 0 and E int = W Isobaric Constant pressure W = P (V f V i ) and E int = Q + W Isochoric Constant Volume W = 0 and E

More information

(2) The volume of molecules is negligible in comparison to the volume of gas. (3) Molecules of a gas moves randomly in all direction.

(2) The volume of molecules is negligible in comparison to the volume of gas. (3) Molecules of a gas moves randomly in all direction. 9.1 Kinetic Theory of Gases : Assumption (1) The molecules of a gas are identical, spherical and perfectly elastic point masses. (2) The volume of molecules is negligible in comparison to the volume of

More information

Preliminary Examination - Day 2 August 16, 2013

Preliminary Examination - Day 2 August 16, 2013 UNL - Department of Physics and Astronomy Preliminary Examination - Day August 16, 13 This test covers the topics of Quantum Mechanics (Topic 1) and Thermodynamics and Statistical Mechanics (Topic ). Each

More information

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

11/22/11. If you add some heat to a substance, is it possible for the temperature of the substance to remain unchanged? Physics 101 Tuesday 11/22/11 Class 26" Chapter 17.2, 17.5, 17.6, 18.1, 18.2" Kinetic Theory" Latent Heat" Phase changes" 1 st law of thermodynamics" " Which one is not the assumption in kinetic theory

More information

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

More Thermodynamics. Specific Specific Heats of a Gas Equipartition of Energy Reversible and Irreversible Processes More Thermodynamics Specific Specific Heats of a Gas Equipartition of Energy Reversible and Irreversible Processes Carnot Cycle Efficiency of Engines Entropy More Thermodynamics 1 Specific Heat of Gases

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

Test Exchange Thermodynamics (C) Test Answer Key

Test Exchange Thermodynamics (C) Test Answer Key 1 Test Exchange Thermodynamics (C) Test Answer Key Made by Montgomery High School montyscioly@gmail.com 2 Questions are worth between 1 to 3 points. Show calculations for all open-ended math questions

More information

CHAPTER 17 WORK, HEAT, & FIRST LAW OF THERMODYNAMICS

CHAPTER 17 WORK, HEAT, & FIRST LAW OF THERMODYNAMICS CHAPTER 17 WORK, HEAT, and the FIRST LAW OF THERMODYNAMICS In this chapter, we will examine various thermal properties of matter, as well as several mechanisms by which energy can be transferred to and

More information

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

Speed 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 information

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

Chapter 19: The Kinetic Theory of Gases Questions and Example Problems Chapter 9: The Kinetic Theory of Gases Questions and Example Problems N M V f N M Vo sam n pv nrt Nk T W nrt ln B A molar nmv RT k T rms B p v K k T λ rms avg B V M m πd N/V Q nc T Q nc T C C + R E nc

More information

Physics 4C Chapter 19: The Kinetic Theory of Gases

Physics 4C Chapter 19: The Kinetic Theory of Gases Physics 4C Chapter 19: The Kinetic Theory of Gases Whether you think you can or think you can t, you re usually right. Henry Ford The only thing in life that is achieved without effort is failure. Source

More information

Lecture 7, 8 and 9 : Thermodynamic process by: Asst. lect. Karrar Al-Mansoori CONTENTS. 7) Thermodynamic process, path and cycle 2

Lecture 7, 8 and 9 : Thermodynamic process by: Asst. lect. Karrar Al-Mansoori CONTENTS. 7) Thermodynamic process, path and cycle 2 CONTENTS Topics pages 7) Thermodynamic process, path and cycle 8) Reversibility and irreversibility 4 9) Thermodynamic processes and calculation of work 5 9.: Constant pressure process or isobaric process

More information

International Academy Invitational Tournament Keep the Heat Test Team Name. Team Number. Predicted Water Temp C

International Academy Invitational Tournament Keep the Heat Test Team Name. Team Number. Predicted Water Temp C International Academy Invitational Tournament Keep the Heat Test 2-4-2012 Team Name Team Number Predicted Water Temp C Circle the all of the correct answer to the below questions. One or more of the answers

More information

Name: Discussion Section:

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

More information

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

First Law of Thermodynamics Second Law of Thermodynamics Mechanical Equivalent of Heat Zeroth Law of Thermodynamics Thermal Expansion of Solids Slide 1 / 66 1 What is the name of the following statement: "When two systems are in thermal equilibrium with a third system, then they are in thermal equilibrium with each other"? A B C D E First Law

More information

Molar Specific Heat of Ideal Gases

Molar Specific Heat of Ideal Gases Molar Specific Heat of Ideal Gases Since Q depends on process, C dq/dt also depends on process. Define a) molar specific heat at constant volume: C V (1/n) dq/dt for constant V process. b) molar specific

More information

Chapter 12. The Laws of Thermodynamics. First Law of Thermodynamics

Chapter 12. The Laws of Thermodynamics. First Law of Thermodynamics Chapter 12 The Laws of Thermodynamics First Law of Thermodynamics The First Law of Thermodynamics tells us that the internal energy of a system can be increased by Adding energy to the system Doing work

More information

16-1. Sections Covered in the Text: Chapter 17. Example Problem 16-1 Estimating the Thermal Energy of a gas. Energy Revisited

16-1. Sections Covered in the Text: Chapter 17. Example Problem 16-1 Estimating the Thermal Energy of a gas. Energy Revisited Heat and Work Sections Covered in the Text: Chapter 17 In this note we continue our study of matter in bulk. Here we investigate the connection between work and heat in bulk matter. Work and heat are both

More information

CH 15. Zeroth and First Law of Thermodynamics

CH 15. Zeroth and First Law of Thermodynamics CH 15 Zeroth and First Law of Thermodynamics THERMODYNAMICS Thermodynamics Branch of Physics that is built upon the fundamental laws that heat and work obey. Central Heating Objectives: After finishing

More information

Stellar Astrophysics: The Interaction of Light and Matter

Stellar Astrophysics: The Interaction of Light and Matter Stellar Astrophysics: The Interaction of Light and Matter The Photoelectric Effect Methods of electron emission Thermionic emission: Application of heat allows electrons to gain enough energy to escape

More information

Chapter 15 Thermal Properties of Matter

Chapter 15 Thermal Properties of Matter Chapter 15 Thermal Properties of Matter To understand the mole and Avogadro's number. To understand equations of state. To study the kinetic theory of ideal gas. To understand heat capacity. To learn and

More information

Thermodynamics. Internal Energy. Study of energy and its transformations Thermochemistry

Thermodynamics. 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 information

Entropy & the Second Law of Thermodynamics

Entropy & the Second Law of Thermodynamics PHYS102 Previous Exam Problems CHAPTER 20 Entropy & the Second Law of Thermodynamics Entropy gases Entropy solids & liquids Heat engines Refrigerators Second law of thermodynamics 1. The efficiency of

More information

KINETIC THEORY. was the original mean square velocity of the gas. (d) will be different on the top wall and bottom wall of the vessel.

KINETIC THEORY. was the original mean square velocity of the gas. (d) will be different on the top wall and bottom wall of the vessel. Chapter Thirteen KINETIC THEORY MCQ I 13.1 A cubic vessel (with faces horizontal + vertical) contains an ideal gas at NTP. The vessel is being carried by a rocket which is moving at a speed of 500m s 1

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

Thermodynamics Test Wednesday 12/20

Thermodynamics Test Wednesday 12/20 Thermodynamics Test Wednesday 12/20 HEAT AND TEMPERATURE 1 Temperature Temperature: A measure of how hot (or cold) something is Specifically, a measure of the average kinetic energy of the particles in

More information

Handout 12: Thermodynamics. Zeroth law of thermodynamics

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

More information

Lesson 12. Luis Anchordoqui. Physics 168. Tuesday, November 28, 17

Lesson 12. Luis Anchordoqui. Physics 168. Tuesday, November 28, 17 Lesson 12 Physics 168 1 Temperature and Kinetic Theory of Gases 2 Atomic Theory of Matter On microscopic scale, arrangements of molecules in solids, liquids, and gases are quite different 3 Temperature

More information

Physics 221: Optical and Thermal Physics Final Exam, Sec. 500, 9 May Please fill in your Student ID number (UIN): IMPORTANT

Physics 221: Optical and Thermal Physics Final Exam, Sec. 500, 9 May Please fill in your Student ID number (UIN): IMPORTANT Physics 221: Optical and Thermal Physics Final Exam, Sec. 500, 9 May 2005 Instructor: Dr. George R. Welch, 415 Engineering-Physics, 845-7737 Print your name neatly: Last name: First name: Sign your name:

More information

Lecture Outline Chapter 30. Physics, 4 th Edition James S. Walker. Copyright 2010 Pearson Education, Inc.

Lecture Outline Chapter 30. Physics, 4 th Edition James S. Walker. Copyright 2010 Pearson Education, Inc. Lecture Outline Chapter 30 Physics, 4 th Edition James S. Walker Chapter 30 Quantum Physics Units of Chapter 30 Blackbody Radiation and Planck s Hypothesis of Quantized Energy Photons and the Photoelectric

More information

Chapter 1: FUNDAMENTAL CONCEPTS OF THERMODYNAMICS AND VARIOUS THERMODYMIC PROCESSES

Chapter 1: FUNDAMENTAL CONCEPTS OF THERMODYNAMICS AND VARIOUS THERMODYMIC PROCESSES Chapter 1: FUNDAMENTAL CONCEPTS OF THERMODYNAMICS AND VARIOUS THERMODYMIC PROCESSES Thermodynamics is that branch of science which deals with energy transfer A system may be closed, open or isolated system

More information

THE SECOND LAW OF THERMODYNAMICS. Professor Benjamin G. Levine CEM 182H Lecture 5

THE SECOND LAW OF THERMODYNAMICS. Professor Benjamin G. Levine CEM 182H Lecture 5 THE SECOND LAW OF THERMODYNAMICS Professor Benjamin G. Levine CEM 182H Lecture 5 Chemical Equilibrium N 2 + 3 H 2 2 NH 3 Chemical reactions go in both directions Systems started from any initial state

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

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

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

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

Ideal 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 information

Properties of Gases. Molecular interactions van der Waals equation Principle of corresponding states

Properties of Gases. Molecular interactions van der Waals equation Principle of corresponding states Properties of Gases Chapter 1 of Atkins and de Paula The Perfect Gas States of gases Gas laws Real Gases Molecular interactions van der Waals equation Principle of corresponding states Kinetic Model of

More information

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

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 Thermodynamics The goal of thermodynamics is to understand how heat can be converted to work Main lesson: Not all the heat energy can be converted to mechanical energy This is because heat energy comes

More information

Topic 3 &10 Review Thermodynamics

Topic 3 &10 Review Thermodynamics Name: Date: Topic 3 &10 Review Thermodynamics 1. The kelvin temperature of an object is a measure of A. the total energy of the molecules of the object. B. the total kinetic energy of the molecules of

More information

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

THERMODYNAMICS b) If the temperatures of two bodies are equal then they are said to be in thermal equilibrium. THERMODYNAMICS Important Points:. Zeroth Law of Thermodynamics: a) This law gives the concept of temperature. b) If the temperatures of two bodies are equal then they are said to be in thermal equilibrium.

More information

UNIVERSITY 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:- 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 information

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

Physics 115. Specific heats revisited Entropy. General Physics II. Session 13 Physics 115 General Physics II Session 13 Specific heats revisited Entropy R. J. Wilkes Email: phy115a@u.washington.edu Home page: http://courses.washington.edu/phy115a/ 4/22/14 Physics 115 1 Lecture Schedule

More information

2. Estimate the amount of heat required to raise the temperature of 4 kg of Aluminum from 20 C to 30 C

2. Estimate the amount of heat required to raise the temperature of 4 kg of Aluminum from 20 C to 30 C 1. A circular rod of length L = 2 meter and diameter d=2 cm is composed of a material with a heat conductivity of! = 6 W/m-K. One end is held at 100 C, the other at 0 C. At what rate does the bar conduct

More information

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

Lecture 25 Goals: Chapter 18 Understand the molecular basis for pressure and the idealgas Lecture 5 Goals: Chapter 18 Understand the molecular basis for pressure and the idealgas law. redict the molar specific heats of gases and solids. Understand how heat is transferred via molecular collisions

More information

Specific Heat of Diatomic Gases and. The Adiabatic Process

Specific Heat of Diatomic Gases and. The Adiabatic Process Specific Heat of Diatomic Gases and Solids The Adiabatic Process Ron Reifenberger Birck Nanotechnology Center Purdue University February 22, 2012 Lecture 7 1 Specific Heat for Solids and Diatomic i Gasses

More information

Lecture 5. PHYC 161 Fall 2016

Lecture 5. PHYC 161 Fall 2016 Lecture 5 PHYC 161 Fall 2016 Ch. 19 First Law of Thermodynamics In a thermodynamic process, changes occur in the state of the system. Careful of signs! Q is positive when heat flows into a system. W is

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

PARTICLES AND WAVES CHAPTER 29 CONCEPTUAL QUESTIONS

PARTICLES AND WAVES CHAPTER 29 CONCEPTUAL QUESTIONS CHAPTER 29 PARTICLES AND WAVES CONCEPTUAL QUESTIONS 1. REASONING AND SOLUTION A monochromatic light source emits photons of a single frequency. According to Equation 29.2, the energy, E, of a single photon

More information

BCIT Fall Chem Exam #1

BCIT Fall Chem Exam #1 BCIT Fall 2012 Chem 3615 Exam #1 Name: Attempt all questions in this exam. Read each question carefully and give a complete answer in the space provided. Part marks given for wrong answers with partially

More information

Outline of the Course

Outline of the Course Outline of the Course 1) Review and Definitions 2) Molecules and their Energies 3) 1 st Law of Thermodynamics 4) 2 nd Law of Thermodynamics 5) Gibbs Free Energy 6) Phase Diagrams and REAL Phenomena 7)

More information

Physical Biochemistry. Kwan Hee Lee, Ph.D. Handong Global University

Physical Biochemistry. Kwan Hee Lee, Ph.D. Handong Global University Physical Biochemistry Kwan Hee Lee, Ph.D. Handong Global University Week 3 CHAPTER 2 The Second Law: Entropy of the Universe increases What is entropy Definition: measure of disorder The greater the disorder,

More information

Real Gases 1. The value of compressibility factor for one mole of a gas under critical states is 1) 3/8 2) 2/3 3) 8/27 4) 27/8 2. an der Waal s equation for one mole of CO2 gas at low pressure will be

More information

Gases. Section 13.1 The Gas Laws Section 13.2 The Ideal Gas Law Section 13.3 Gas Stoichiometry

Gases. Section 13.1 The Gas Laws Section 13.2 The Ideal Gas Law Section 13.3 Gas Stoichiometry Gases Section 13.1 The Gas Laws Section 13.2 The Ideal Gas Law Section 13.3 Gas Stoichiometry Click a hyperlink or folder tab to view the corresponding slides. Exit Section 13.1 The Gas Laws State the

More information