Preliminary Examination - Day 2 May 16, 2014

Similar documents
Preliminary Examination - Day 2 August 15, 2014

Preliminary Examination - Day 2 August 16, 2013

Preliminary Examination - Day 2 Friday, August 12, 2016

Preliminary Examination - Day 2 Friday, May 11, 2018

Preliminary Examination - Day 1 Thursday, August 9, 2018

Spring 2012 Qualifying Exam. Part I

Thermodynamic Variables and Relations

Preliminary Examination - Day 1 Thursday, May 10, 2018

Candidacy Exam Department of Physics October 6, 2012 Part I

PHY 001 (Physics I) Lecture 7

Graduate Preliminary Examination, Thursday, January 6, Part I 2

General Physics Contest 2012

Practice Examinations Chem 393 Fall 2005 Time 1 hr 15 min for each set.

Graduate Written Examination Spring 2014 Part I Thursday, January 16th, :00am to 1:00pm

Graduate Written Examination Fall 2014 Part I

Preliminary Examination - Day 1 Thursday, August 10, 2017

UNIVERSITY OF LONDON. BSc and MSci EXAMINATION 2005 DO NOT TURN OVER UNTIL TOLD TO BEGIN

August 2013 Qualifying Exam. Part II

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

Joint Entrance Examination for Postgraduate Courses in Physics EUF

Physics 2101, Final Exam, Spring 2007

Chemistry. Lecture 10 Maxwell Relations. NC State University

Final Test for PHYS 2130 section 091 Date: 2 nd May 2007

UNIVERSITY OF SOUTHAMPTON

General Physics I (aka PHYS 2013)

Physics 161 Lecture 17 Simple Harmonic Motion. October 30, 2018

Thermal and Statistical Physics Department Exam Last updated November 4, L π

SIR MICHELANGELO REFALO SIXTH FORM

UNIVERSITY OF MISSOURI-COLUMBIA PHYSICS DEPARTMENT. PART I Qualifying Examination. January 20, 2015, 5:00 p.m. to 8:00 p.m.

Outline Review Example Problem 1 Example Problem 2. Thermodynamics. Review and Example Problems. X Bai. SDSMT, Physics. Fall 2013

(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

Lecture Notes 2014March 13 on Thermodynamics A. First Law: based upon conservation of energy

Outline Review Example Problem 1. Thermodynamics. Review and Example Problems: Part-2. X Bai. SDSMT, Physics. Fall 2014

Qualifying Exam for Ph.D. Candidacy Department of Physics October 11, 2014 Part I

Assignments VIII and IX, PHYS 301 (Classical Mechanics) Spring 2014 Due 3/21/14 at start of class

General Physics 1. School of Science, University of Tehran Fall Exercises (set 07)

Physics 2101, Final Exam, Form A

M04M.1 Particles on a Line

Thermodynamics! for Environmentology!

Lecture 2 - Thursday, May 11 th, 3pm-6pm

GRADUATE WRITTEN EXAMINATION. Fall 2018 PART I

Data Provided: A formula sheet and table of physical constants are attached to this paper.

SPRING 2003 Final Exam, Part A

The Second Law of Thermodynamics (Chapter 4)

FIITJEE Solutions to AIEEE PHYSICS

PHYSICS 221, FALL 2010 FINAL EXAM MONDAY, DECEMBER 13, 2010

Physics 607 Final Exam

i.e. the tighter the curve, the larger the radial acceleration. 56) Which of the following is an accurate statement about circular motion?

Classical Thermodynamics. Dr. Massimo Mella School of Chemistry Cardiff University

Thermal & Statistical Physics Study Questions for the Spring 2018 Department Exam December 6, 2017

PHY101: Major Concepts in Physics I

Identify the intensive quantities from the following: (a) enthalpy (b) volume (c) refractive index (d) none of these

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

Physics 53 Summer Final Exam. Solutions

PHYSICS 221 SPRING FINAL EXAM: May 2, :30pm 6:30pm

Last Name: First Name ID

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

Thermodynamics & Statistical Mechanics SCQF Level 9, U03272, PHY-3-ThermStat. Thursday 24th April, a.m p.m.

UNIVERSITY OF SOUTHAMPTON

Candidacy Exam Department of Physics February 6, 2010 Part I

Department of Physics and Astronomy University of Georgia

Classification following properties of the system in Intensive and Extensive

University of Michigan Physics Department Graduate Qualifying Examination

Old Exams Questions Ch. 8 T072 Q2.: Q5. Q7.

Chapter 14 Oscillations. Copyright 2009 Pearson Education, Inc.

Introduction. Statistical physics: microscopic foundation of thermodynamics degrees of freedom 2 3 state variables!

Exam #: Printed Name: Signature:

PHY218 SPRING 2016 Review for Final Exam: Week 14 Final Review: Chapters 1-11, 13-14

4 A mass-spring oscillating system undergoes SHM with a period T. What is the period of the system if the amplitude is doubled?

Final Exam for Physics 176. Professor Greenside Wednesday, April 29, 2009

Thermodynamics Free E and Phase D. J.D. Price

Fall 2012 Qualifying Exam. Part I

Physics 221. Exam III Spring f S While the cylinder is rolling up, the frictional force is and the cylinder is rotating

Candidacy Exam Department of Physics February 5, 2011 Part I

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

PHYS 1303 Final Exam Example Questions

Physics 408 Final Exam

24/06/13 Forces ( F.Robilliard) 1

Chapter 12. Recall that when a spring is stretched a distance x, it will pull back with a force given by: F = -kx

Physics 117A Final Exam Fall 2006

Classical thermodynamics

PY205N Spring The vectors a, b, and c. are related by c = a b. The diagram below that best illustrates this relationship is (a) I

Do not fill out the information below until instructed to do so! Name: Signature: Student ID: Section Number:

PHYSICS DEPARTMENT UNIVERSITY OF OREGON Unified Graduate Examination Part I Analytical Mechanics Friday, January 6, 2017, 10:00 to 12:40

A amplitude. k stiffness m mass δ phase angle x 0 initial displacement v 0 initial velocity T period f frequency. A amplitude. ω angular frequency

Sample Final Questions: Solutions Math 21B, Winter y ( y 1)(1 + y)) = A y + B

Physics 5A Final Review Solutions

Some physical constants:

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

The Gibbs Phase Rule F = 2 + C - P

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

Grade XI. Physics Exam Preparation Booklet. Chapter-wise Important Questions. #GrowWithGreen

Chapter 7. Entropy. by Asst.Prof. Dr.Woranee Paengjuntuek and Asst. Prof. Dr.Worarattana Pattaraprakorn

Oscillations. Oscillations and Simple Harmonic Motion

Padua, Italy. Theoretical competition

Study Guide Final Exam Solutions. Part A: Kinetic Theory, First Law of Thermodynamics, Heat Engines

Thermodynamic system is classified into the following three systems. (ii) Closed System It exchanges only energy (not matter) with surroundings.

Some properties of the Helmholtz free energy

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

Gibb s free energy change with temperature in a single component system

Transcription:

UNL - Department of Physics and Astronomy Preliminary Examination - Day May 6, 04 This test covers the topics of Thermodynamics and Statistical Mechanics (Topic ) and Mechanics (Topic ) Each topic has 4 A questions and 4 B questions Work two problems from each group Thus, you will work on a total of 8 questions today, 4 from each topic WRITE YOUR ANSWERS ON ONE SIDE OF THE PAPER ONLY

Thermodynamics and Statistical Mechanics Group A - Answer only two Group A questions A Two editors work independently and examine a manuscript that contains N typos They are both equally well-trained and spot typos with probability equal to p What is the expected number of typos that neither of the editors will spot? A A gas can be taken from the initial state i to the final state f along the four different paths shown on a p-v diagram in the figure Which of the paths corresponds to the highest amount of heat absorbed by the gas? Explain your reasoning A3 A reversible Carnot cycle is used as a heat pump to heat a room at temperature 0 C, while outside air at 0 C serves as a heat source How much power must be supplied in order to provide the heat to the room at kw? A4 In a first experiment, a certain gas expands into vacuum after an internal partition in an enclosing thermally insulating vessel is punctured It was found that the temperature of the gas has decreased In a second experiment, the gas slowly expands isothermally as it absorbs heat Q and does work W Based on the result of the first experiment, predict whether Q is greater, smaller, or equal to W

Thermodynamics and Statistical Mechanics Group B - Answer only two Group B questions B Consider a mole of ideal gas taken through a process with the initial state at ( p, V, T ) and the final state at ( p, V, T ) a Show that for any two states and, the following holds: T p S S = C ln Rln p T p b Show that if the states and lie on an adiabatic curve, the difference S S vanishes Assume C = C + R, but do not assume any particular value of C p V V B In a statistics course you have learned to solve an assortment of easy and hard problems For the final exam the professor prepares closed envelopes of 3 types: () with two easy problems, () with two hard problems, and (3) with one easy and one hard problem There are an equal number of envelopes () () (3) of each type, and you pull a closed envelope at random After opening your envelope, you examine one of the problems and it turns out to be hard What is the probability that the other problem in your envelope is also hard? B3 A 3 kg bronze brick heated to 90 C is placed in a thermally insulated vessel with 600 g of ice, which is initially at 5 C The whole system is then allowed to reach equilibrium a What is the final temperature of the system? b What was the entropy change of the whole system in this process? Reference data: Specific heat of water: 486 J / (kg K); ice: 050 J / (kg K); bronze: 435 J / (kg K) It takes 334 joules to melt gram of ice B4 Show that if a system s initial and final temperature and pressure are that of a bath that is both isothermal and isobaric, then the maximum useful work W done by this system is W = G, that is, the negative change in the Gibbs free energy of the system max

Mechanics Group A - Answer only two Group A questions A In the figure, a block weighing 40 N, which can slide without friction on an incline at angle θ = 40, is connected to the top of the incline by a massless spring of un-stretched length 045 m and spring constant k = 0 N/m k a How far from the top of the incline is the block s equilibrium point? b If the block is pulled slightly down the incline and released, what is the period of the resulting oscillations? block A Consider a mass shell of finite thickness with inner radius r and outer radius r, as shown in the figure The shell has uniform volume mass density ρ Calculate the gravitational force on a mass m a at r< r b at r < r< r c at r > r A3 This problem is -dimensional Consider the two force functions F = xiˆ+ yˆ j, and F = yiˆ xˆ j The adjacent diagram shows two different paths (A and B) from the origin to the point (,) a Calculate F dr and F dr path A path B Is F conservative? Explain b Calculate F dr and F dr path A path B Is F conservative? Explain

A4 See diagram We wrap a massless, flexible cable around a solid uniform cylinder with mass M and radius R The cylinder rotates without friction about a stationary horizontal axis We tie the free end of the cable to a block of mass m and release the object with no initial velocity at a distance h above the floor As the block falls, the cable unwinds without stretching or slipping, turning the cylinder Find the speed of the falling block and the angular speed of the cylinder just as the block strikes the floor

Mechanics Group B - Answer only two Group B questions B Consider a particle subject to an attractive central force of magnitude f() r, where r is the distance between the particle and the center of the force Find the explicit form f() r if all circular orbits are to have identical areal velocities A (Note: areal velocity, aka sectorial velocity, is the rate at which area is swept out by a particle as it moves along the orbit) B A thin, uniform stick of length is initially in unstable equilibrium with its bottom end resting on a frictionless table A small disturbance makes the stick fall Find the velocity of the center of mass when it reaches the table B3 A point mass m slides frictionlessly, under the influence of gravity, along a massive ring of radius a and mass M The ring is affixed by horizontal springs to two fixed vertical surfaces, as depicted in the figure All motion is within the plane of the figure Except for the point mass, there is no motion in the vertical direction: the ring is constrained without friction to move horizontally X k M k θ a m Choose as generalized coordinates the horizontal displacement X of the center of the ring with respect to equilibrium, and the angle θ a radius to the mass m makes with respect to the vertical (see fig ) You may assume that at X = 0 the springs are both unstretched a Find the Lagrangian LX (, θ, X, θ, t ) b Find the momenta conjugate to X and θ c Derive the equations of motion (but don t solve them)

B4 A particle of mass m is performing one-dimensional motion subject to the force function F( x) = F 0 sin( cx ) At some instant the particle's position is x = 0 and its velocity v= v 0 a Find the potential energy as a function of x and sketch it b Find the velocity as a function of x c Find the condition on the initial velocity v 0 for which the motion is periodic ( v <? 0 ) d Suppose that v 0 is so small that the periodic motion can be treated as a harmonic oscillation Find the period of this oscillation

Physical Constants speed of light 8 c = 998 0 m/s electrostatic constant k = πε = 9 (4 0) 8988 0 m/f 34 3 Planck s constant h = 666 0 J s electron mass m el = 909 0 kg 34 7 Planck s constant / π = 055 0 J s proton mass m p = 673 0 kg 3 Boltzmann constant k = 38 0 J/ K bohr a B 0 = 059 Å 9 elementary charge e = 60 0 C hartree E h = 7 ev electric permittivity ε 0 = 8854 0 F/m Avogrado constant N A = 60 0 mol 3 N 6 magnetic permeability µ 0 = 57 0 H/m gravitational constant G = 6674 0 m / kg s molar gas constant R = 834 J / mol o K 3 EQUATIONS THAT MAY BE HELPFUL MECHANICS: Gravitational acceleration on Earth: g = 98 m/s Moments of Inertia of Various Bodies

THERMODYNAMICS General efficiency η of a heat engine producing work W while taking in heat Q is η = h For a Carnot cycle operating as a heat engine between reservoirs at T and at T the efficiency h c T T becomes η = h c C T Clausius theorem: h N i= Qi 0, which becomes T i For adiabatic processes in an ideal gas with constant heat capacity, dp λ = dt T Δ V N i= Qi = 0 for a reversible cyclic process of N steps T i PV γ = constant W Q h specific heat of water: latent heat of ice melting: 486 J/(kg K) 334 J/g H = E + PV F = E TS G = F + PV Ω= F µ de = TdS PdV + µ d ds = de / T + PdV / T µ d / T dh = TdS + VdP + µ d df = SdT PdV + µ d dg = SdT + VdP + µ d dω= SdT PdV dµ δq S δq S S C = = T C = = T TdS = C dt + T dv dt T dt T V V p V V V p p T

INTEGRALS 0 + ay dy = π /a / 0 y e dy = n! a n ya / n+