Dr. Gundersen Phy 206 Test 2 March 6, 2013

Similar documents
A) 120 degrees B) 90 degrees C) 60 degrees D) 45 degrees E) 30 degrees

First major ( 043 ) a) 180 degrees b) 90 degrees c) 135 degrees d) 45 degrees e) 270 degrees

Phys102 Term: 103 First Major- July 16, 2011

Final Review Prof. WAN, Xin

Quiz 3 July 31, 2007 Chapters 16, 17, 18, 19, 20 Phys 631 Instructor R. A. Lindgren 9:00 am 12:00 am

Phys102 First Major-112 Zero Version Coordinator: Wednesday, March 07, 2012 Page: 1

Phys102 First Major-182 Zero Version Coordinator: A A Naqvi Thursday, February 14, 2019 Page: 1

Phys102 First Major- 161 Code: 20 Coordinator: Dr. A. Naqvi Saturday, October 29, 2016 Page: 1

7. (2) Of these elements, which has the greatest number of atoms in a mole? a. hydrogen (H) b. oxygen (O) c. iron (Fe) d. gold (Au) e. all tie.

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

Q1. A) 53.3 cm/s B) 59.8 cm/s C) 77.5 cm/s D) 35.1 cm/s E) 44.7 cm/s. Ans: 1.6 Q2.

Handout 12: Thermodynamics. Zeroth law of thermodynamics

Final Review Solutions

Phys102 First Major-123 Zero Version Coordinator: xyz Sunday, June 30, 2013 Page: 1

Chapter 15 Thermal Properties of Matter

Handout 12: Thermodynamics. Zeroth law of thermodynamics

The first law of thermodynamics continued

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

Q1. For a given medium, the wavelength of a wave is:

Alternate Midterm Examination Physics 100 Feb. 20, 2014

Chapter 19 The First Law of Thermodynamics

Chapter 15. Mechanical Waves

Physics 200a Finals 18 December minutes Formulas and Figures at the end. Do problems in 6 books as indicated. a = 2 g sin θ.

Phys102 First Major-131 Zero Version Coordinator: xyz Saturday, October 26, 2013 Page: 1

Lecture 5. PHYC 161 Fall 2016

Chapter 14 Kinetic Theory

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

Physics 2101, Final Exam, Form A

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

First Law of Thermodynamics

Chapter 16 Mechanical Waves

UNIVERSITY OF SOUTHAMPTON

PHY 206 SPRING Problem #1. Problem #2 NAME: SIGNATURE: Problem #3 UM ID: Problem #4. Problem #5. Problem #6. Total. Prof. Massimiliano Galeazzi

Lecture 30. Chapter 21 Examine two wave superposition (-ωt and +ωt) Examine two wave superposition (-ω 1 t and -ω 2 t)

Sec# Wave Motion - Superposition and Interference of Waves Grade# 50

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

Phys102 First Major-143 Zero Version Coordinator: xyz Sunday, June 28, 2015 Page: 1

Physics 123 Thermodynamics Review

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

Fall 2004 Physics 3 Tu-Th Section

Q1. The displacement of a string carrying a traveling sinusoidal wave is given by:

Thermodynamics continued

Physics 7B Midterm 1 Problem 1 Solution

Chemistry. Lecture 10 Maxwell Relations. NC State University

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

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

Superposition & Interference

Physics Final Exam Formulas

Ch. 19: The Kinetic Theory of Gases

ME 200 Thermodynamics I, Spring 2015, Exam 3, 8 p.m. to 9 p.m. on April 14, 2015

Heat What is heat? Work = 2. PdV 1

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

Week of September 2 Torricelli's Law: The flow velocity from a liquid column of height h is the free fall velocity v = p 2gh. The viscous force transm

Q1. A) 21.0 ms B) 63.1 ms C) 31.5 ms D) 45.2 ms E) 73.1 ms. Ans: Q2.

6. (6) Show all the steps of how to convert 50.0 F into its equivalent on the Kelvin scale.

Chapter 3 - First Law of Thermodynamics

Chapter 15 Mechanical Waves

Chapter 18 Thermal Properties of Matter

Exam 4. P201 Fall 2006, Instructor: Prof. Abanov 11/28/06. (print in big block letters )

General Physics I (aka PHYS 2013)

Downloaded from

Chapter 2 Carnot Principle

Classical Physics I. PHY131 Lecture 36 Entropy and the Second Law of Thermodynamics. Lecture 36 1

PHYS Homework # 10 (Mendes, Fall 2015) due in class on Nov 20. 1) Exercise 15.4, p. 501, University Physics by Young & Freedman

Honors Classical Physics I

UNIVERSITY OF SOUTHAMPTON

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

NOTE: Only CHANGE in internal energy matters

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

Physics 2101 Section 6 November 8 th : finish Ch.16

MidTerm. Phys224 Spring 2008 Dr. P. Hanlet

MCQs THERMODYNAMICS. Physics Without Fear.


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

Statistical Mechanics

Specific Heat of Diatomic Gases and. The Adiabatic Process

PRACTICE FINAL EXAM SOLUTIONS

ABCD42BEF F2 F8 5 4D6589 CC8 9

a) The process is isobaric, or it occurs at constant pressure. We know this because the pressure is supplied entirely by the weight of the piston:

Kinetic Theory continued

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

Name: Discussion Section:

The First Law of Thermodynamics

Chapter 16 Waves in One Dimension

Kinetic Theory continued

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

Topic 3 &10 Review Thermodynamics

Miami-Dade Community College PHY 2053 College Physics I

Old Exams - Questions Ch-16

Learning Objectives for Final Exam Fall, 2012 Physics 2210

Chapter 19 The First Law of Thermodynamics

Honors Physics. Notes Nov 16, 20 Heat. Persans 1

Answers to test yourself questions

P V T 1 P 1 V 1 T 1. Question 3 : Find the efficiency of the triangular cycle.

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

Enthalpy and Adiabatic Changes

Unit 05 Kinetic Theory of Gases

Thermodynamics of solids 5. Unary systems. Kwangheon Park Kyung Hee University Department of Nuclear Engineering

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

1. (10) Calorically perfect ideal air at 300 K, 100 kpa, 1000 m/s, is brought to rest isentropically. Determine its final temperature.

Transcription:

Signature: Idnumber: Name: You must do all four questions. There are a total of 100 points. Each problem is worth 25 points and you have to do ALL problems. A formula sheet is provided on the LAST page which you can tear off. TO GET PARTIAL CREDIT, SHOW YOUR WORK ON PROBLEMS 2-4. 1 2 3 4 CHECK DISCUSSION SECTION ATTENDED: [ ] Dr. Barnes 1P, 11:00-11:50 a.m. [ ] Dr. Barnes 1Q, 12:30-1:20 p.m. [ ] Dr. Zuo 1R, 2:00-2:50 p.m. [ ] Dr. Ghandour 1S, 3:30-4:20 p.m. [ ] Dr. Ghandour 1T, 5:00-5:50 p.m. [ ] Dr. Zuo 2P, 11:00-11:50 a.m. [ ] Dr. Van Vliet 2R, 2:00-2:50 p.m

[1.] This problem has five multiple choice questions. Circle the best answers. [1A.] An ideal gas may expand from an initial pressure p i and volume V i to a final volume V f isothermally, adiabatically, or isobarically. For which type of process is the heat that is added to the gas the largest? (Assume that p i, V i, and V f are the same for each process.) [A] isothermal [B] adiabatic [C] isobaric [E] not enough information [1B.] A refrigerator operates by [D] all the processes have the same heat flow [A] doing work to move heat from a low-temperature thermal reservoir to a high-temperature thermal reservoir. [B] doing work to move heat from a high-temperature thermal reservoir to a low-temperature thermal reservoir. [C] using thermal energy to produce useful work. [D] moving heat from a low-temperature thermal reservoir to a high-temperature thermal reservoir without doing work. [E] moving heat from a high-temperature thermal reservoir to a low-temperature thermal reservoir without doing work. [1C.] Which of the following statements about the Carnot cycle is incorrect? [A] The maximum efficiency of a Carnot engine is 100% since the Carnot cycle is an ideal process. [B] The Carnot cycle consists of two isothermal processes and two adiabatic processes. [C] The Carnot cycle consists of two isothermal processes and two constant entropy (isentropic) processes. [D] The efficiency of the Carnot cycle depends solely on the temperature of the two thermal reservoirs. [E] The Carnot cycle is reversible. [1D.] Which of the following processes always results in an increase in the internal energy of the system? [A] The system loses heat and does work on the surroundings. [B] The system gains heat and does work on the surroundings. [C] The system loses heat and has work done on it by the surroundings. [D] The system gains heat and has work done on it by the surroundings. [E] None of the above will always increase the internal energy of the system. [1E.] Which statement is not true about a string instrument? [A] Longer strings give rise to lower resonant frequencies. [B] The resonant frequencies are proportional to the square root of the string s tension. [C] Strings with higher linear mass densities yield lower resonant frequencies. [D] The resonant frequency is proportional to the wave speed. [E] The resonant frequency is proportional to the amplitude of the string s motion.

[2.] A three step heat engine cycle consists of an adiabatic expansion (process AB), an isobaric compression (process BC) and an isochoric process (process CA). The working substance consists of n moles of an ideal gas with a molar heat capacity at constant volume of C V and a molar heat capacity at constant pressure C p. The cycle operates between pressures (p 1,p 2 ) and volumes (V 1,V 2 ) as shown in the figure below. [a] Label the points on graph with A, B, or C, connect the points with properly shaped lines representing each process, and indicate arrows on the lines showing the direction of the cycle. (7 points) [b] Calculate the heat Q, the work W, and the change in internal energy U for each process in the cycle and enter your results in the table below. Express your answers in terms of p 1, p 2, V 1, V 2, C p, C V and the gas constant R. (18 points)

[3.] This problem concerns the cycle described in problem 2. [a] Compute the efficiency of the cycle described in problem 2. Express your answer in terms of the compression ratio r = V 2 /V 1 and γ = C p /C V. (10 points) [b] Compute the change in entropy for each of the processes shown in problem 2, i.e. S AB, S BC, and S CA. Express your answer in terms of n, C p, C V, r, and γ.(9 points) [c] Show that the change in entropy for the complete cycle is 0. (6 points)

[4.] A string is attached to a wall at x = 0 and x = L. The string is oscillating in its fourth harmonic and its shape is described by the standing wave y(x,t) = 3sin(5x)sin(7t). The numbers in the wave function are in terms of standard MKS units. Give units for your answers in parts b) and c). [a] In the diagram above, draw the standing wave pattern at times t = π/14 seconds and t = 3π/14 seconds and indicate the positions of the nodes and antinodes. (9 points) [b] As described in class, standing waves consist of the sum of two counter-propagating traveling waves. What is the amplitude, wavelength, frequency, period and speed of the traveling waves that make up the standing wave? (10 points) [c] What is the length (L) of the string, what is its transverse velocity, v y (x,t), and what is its transverse acceleration, a y (x,t)? (6 points)

Fluid Mechanics: ρ = m V, p = df da, p 2 p 1 = ρg(y 2 y 1 ), p = p 0 + ρgh, B = m disp g A 1 v 1 = A 2 v 2, dv dt = Av, p 1 + ρgy 1 + 1 2 ρv2 1 = p 2 + ρgy 2 + 1 2 ρv2 2 Temperature and Heat: T C = 5 9 (T F 32 ), T K = T C +273.15, L = αl 0 T, V = βv 0 T, Q = mc T, Q = nc T, Q = ±ml, H = dq dt = kat H T C L Thermal Properties of Matter: F A = Y α T = ka dt dx, H net = Aeσ(T 4 T 4 s ) m tot = nm, pv = nrt, M = N A m, K tr = 3 2 nrt, 1 2 m(v2 ) av = 3 2 kt, C V = #DOF R 2 v rms = 3kT 3RT (v 2 ) av = m = M, f(v) = 4π( m 2πkT )3/2 v 2 e mv 2 /2kT W = V2 First Law of Thermodynamics: V 1 pdv, U = Q W, U = nc V T, C p = C V + R, γ = C p C V T 1 V γ 1 1 = T 2 V γ 1 2, p 1 V γ 1 = p 2V γ 2, W = C V R (p 1V 1 p 2 V 2 ) Second Law of Thermodynamics: e = W = 1 + Q C = 1 Q C Q H Q H Q H, e Carnot = 1 T C, K = Q C T H W K Carnot = T 2 C dq, S rev = T H T C 1 T, S = k lnw Mechanical Waves: v = λf = ω/k, f = ω/2π = 1/T, λ = 2π/k, y(x,t) = Acos(kx ωt), v = = Q C Q H Q C 2 y(x,t) x 2 = 1 v 2 2 y(x,t) t 2 F µ, P(x,t) = µfω 2 A 2 sin 2 (kx ωt), P av = 1 µfω 2 A 2, v y (x,t) = y(x,t) 2 t a y (x,t) = v y(x,t), y(x,t) = y 1 (x,t)+y 2 (x,t), y(x,t) = A SW sinkxsin ωt, λ n = 2L t n, f n = nv 2L