Chapter #7 Giancoli 6th edition Problem Solutions



Similar documents
Physics 125 Practice Exam #3 Chapters 6-7 Professor Siegel

A uranium nucleus (at rest) undergoes fission and splits into two fragments, one heavy and the other light. Which fragment has the greater speed?

Chapter 7: Momentum and Impulse

Chapter 9. particle is increased.

Work, Energy & Momentum Homework Packet Worksheet 1: This is a lot of work!

Exam 2 is at 7 pm tomorrow Conflict is at 5:15 pm in 151 Loomis

Physics 2A, Sec B00: Mechanics -- Winter 2011 Instructor: B. Grinstein Final Exam

HW Set VI page 1 of 9 PHYSICS 1401 (1) homework solutions

Physics: Principles and Applications, 6e Giancoli Chapter 4 Dynamics: Newton's Laws of Motion

SHORT ANSWER. Write the word or phrase that best completes each statement or answers the question.

Exam Three Momentum Concept Questions

Lecture PowerPoints. Chapter 7 Physics: Principles with Applications, 6 th edition Giancoli

Gravitational Potential Energy

Chapter 7 Momentum and Impulse

Midterm Solutions. mvr = ω f (I wheel + I bullet ) = ω f 2 MR2 + mr 2 ) ω f = v R. 1 + M 2m

8. Potential Energy and Conservation of Energy Potential Energy: When an object has potential to have work done on it, it is said to have potential

AP physics C Web Review Ch 6 Momentum

Name per due date mail box

Problem Set #8 Solutions

Kinetic Energy (A) stays the same stays the same (B) increases increases (C) stays the same increases (D) increases stays the same.

AP Physics - Chapter 8 Practice Test

Work, Power, Energy Multiple Choice. PSI Physics. Multiple Choice Questions

Chapter 8 Conservation of Linear Momentum. Conservation of Linear Momentum

Lecture 07: Work and Kinetic Energy. Physics 2210 Fall Semester 2014

Physical Science Chapter 2. Forces

Work and Conservation of Energy

F N A) 330 N 0.31 B) 310 N 0.33 C) 250 N 0.27 D) 290 N 0.30 E) 370 N 0.26

Chapter 9. is gradually increased, does the center of mass shift toward or away from that particle or does it remain stationary.

9. The kinetic energy of the moving object is (1) 5 J (3) 15 J (2) 10 J (4) 50 J

Giancoli 6th Edition Problem Solutions Chapter #6

The law of conservation of energy, which we discussed in the previous Chapter, Linear Momentum E R CONTENTS

Name Period WORKSHEET: KINETIC AND POTENTIAL ENERGY PROBLEMS. 1. Stored energy or energy due to position is known as energy.

Phys101 Lectures 14, 15, 16 Momentum and Collisions

Newton s Law of Motion

Physics Notes Class 11 CHAPTER 6 WORK, ENERGY AND POWER

PHY231 Section 2, Form A March 22, Which one of the following statements concerning kinetic energy is true?

Physics 41 HW Set 1 Chapter 15

Lab 8: Ballistic Pendulum

WORKSHEET: KINETIC AND POTENTIAL ENERGY PROBLEMS

F f v 1 = c100(10 3 ) m h da 1h 3600 s b =

5. Forces and Motion-I. Force is an interaction that causes the acceleration of a body. A vector quantity.

Conservation of Momentum and Energy

B) 286 m C) 325 m D) 367 m Answer: B

Experiment 7 ~ Conservation of Linear Momentum

PHYSICS 111 HOMEWORK SOLUTION #10. April 8, 2013

Work-Energy Bar Charts

10.1 Quantitative. Answer: A Var: 50+

Tennessee State University

4 Impulse and Impact. Table of contents:

AP Physics C. Oscillations/SHM Review Packet

Serway_ISM_V1 1 Chapter 4

Curso Física Básica Experimental I Cuestiones Tema IV. Trabajo y energía.

Notes on Elastic and Inelastic Collisions

C B A T 3 T 2 T What is the magnitude of the force T 1? A) 37.5 N B) 75.0 N C) 113 N D) 157 N E) 192 N

PRELAB: NEWTON S 3 RD LAW AND MOMENTUM CONSERVATION

Physics 211 Lecture 4

Work, Energy and Power Practice Test 1

Problem Set V Solutions

AP Physics Circular Motion Practice Test B,B,B,A,D,D,C,B,D,B,E,E,E, m/s, 0.4 N, 1.5 m, 6.3m/s, m/s, 22.9 m/s

Chapter 10. Momentum and Collisions

8. As a cart travels around a horizontal circular track, the cart must undergo a change in (1) velocity (3) speed (2) inertia (4) weight

Forces. When an object is pushed or pulled, we say that a force is exerted on it.

PHY231 Section 1, Form B March 22, 2012

Lesson 3 - Understanding Energy (with a Pendulum)

B Answer: neither of these. Mass A is accelerating, so the net force on A must be non-zero Likewise for mass B.

Motion of a Leaky Tank Car

v v ax v a x a v a v = = = Since F = ma, it follows that a = F/m. The mass of the arrow is unchanged, and ( )

Momentum Crash Course

PHY121 #8 Midterm I

PHYSICS 111 HOMEWORK SOLUTION, week 4, chapter 5, sec 1-7. February 13, 2013

momentum change per impact The average rate of change of momentum = Time interval between successive impacts 2m x 2l / x m x m x 2 / l P = l 2 P = l 3

2 ONE- DIMENSIONAL MOTION

P211 Midterm 2 Spring 2004 Form D

Unit 3 Work and Energy Suggested Time: 25 Hours

Free Fall: Observing and Analyzing the Free Fall Motion of a Bouncing Ping-Pong Ball and Calculating the Free Fall Acceleration (Teacher s Guide)

Practice Test SHM with Answers

Review Vocabulary force: a push or a pull. Vocabulary Newton s third law of motion

The Bullet-Block Mystery

Chapter 15 Collision Theory

Problem Set 1. Ans: a = 1.74 m/s 2, t = 4.80 s

9. Momentum and Collisions in One Dimension*

A) N > W B) N = W C) N < W. speed v. Answer: N = W

Ch 7 Kinetic Energy and Work. Question: 7 Problems: 3, 7, 11, 17, 23, 27, 35, 37, 41, 43

Exercises on Work, Energy, and Momentum. A B = 20(10)cos98 A B 28

G U I D E T O A P P L I E D O R B I T A L M E C H A N I C S F O R K E R B A L S P A C E P R O G R A M

EDUH SPORTS MECHANICS

WATCH THIS ICON: View this short clip from the Insurance Institute for Highway Safety DVD called Understanding Car Crashes It s basic physics.

Lecture 6. Weight. Tension. Normal Force. Static Friction. Cutnell+Johnson: , second half of section 4.7

Physics: Principles and Applications, 6e Giancoli Chapter 2 Describing Motion: Kinematics in One Dimension

Displacement (x) Velocity (v) Acceleration (a) x = f(t) differentiate v = dx Acceleration Velocity (v) Displacement x

Projectile motion simulator.

SQA Higher Physics Unit 1 Mechanics and Properties of Matter

Resistance in the Mechanical System. Overview

Conceptual Questions: Forces and Newton s Laws

THE COLLISION PHENOMENON BETWEEN CARS

Chapter 4. Forces and Newton s Laws of Motion. continued

Science Standard Articulated by Grade Level Strand 5: Physical Science

Answer: Same magnitude total momentum in both situations.

Weight The weight of an object is defined as the gravitational force acting on the object. Unit: Newton (N)

Transcription:

Chapter #7 Giancoli 6th edition Problem Solutions ü Problem #8 QUESTION: A 9300 kg boxcar traveling at 5.0 m/s strikes a second boxcar at rest. The two stick together and move off with a speed of 6.0 m/s. What is the mass of the second car? ANSWER: 5 m/sec at rest Before Collision 6 m/s After Collision Momentum is conserved since there is no external force acting on the system of two boxcars in the horizontal direction. (There is an external force (gravity) in the y-direction but there is no motion in the y direction.) Momentum is NOT conserved for each boxcar separately. The two boxcars stick together and this usually means energy is NOT conserved or at least cannot be assumed to be conserved. The initial momentum is p 0 = 9300 kg ä 5 mês and the final momentum is p f = H9300 kg + ML ä 6 mês if we knew the mass M of the second boxcar. Conservation of momentum means p 0 = p f that is 9300 kg ä 5 m/s = (9300 kg + M) ä 6 m/s 39500 kg-m/s = 55800 kg-m/s + M ä 6 m/s 9300 * 5 39 500 930 086 9300 * 6 55 800 H39 500-55 800L ê 6. 3 950. ü Problem #: M=3,950 kg. QUESTION: A 3-gm (=0.03 kg) bullet traveling 30 m/s penetrates at.0 kg block of wood and emerges cleanly at 70 m/s If the block is stationary on a frictionless surface when hit, how fast does it move after the bullet emerges? ANSWER:

Giancoli 6th ed chap.7 problem solutions Rev.nb 30 m/s kg block bullet Before 70 m/s bullet After Momentum is conserved for the system of the bullet and.0 kg block since there is no external force acting on the system in the horizontal direction. (Gravity is an external force which acts in the vertical direction but there is no motion in the vertical direction.) Momentum is not conserved for the bullet separately or the block of wood separately. The initial momentum of the system (bullet plus block) is 0.03 * 30 p 0 = 0.03 kg ä 30 mês = 5.9 kg-m/s 5.9 The final momentum of the system p f = 0.03 kg ä 70 mês +.0 kg ä V f = 3.9 kg-m/s + kg ä V f 70 * 0.03 3.9 Assuming conservation of momentum p 0 = p f means that 5.9 kg-m/s= 3.9 kg-m/s + kg ä V f Solving for V f yields 5.9-3.9 0.69.0 ü Problem #6 V f = 5.9 kg-mês - 3.9 kg-mês kg = 0.69 m/s QUESTION: A kg hammer strikes a nail at a velocity of 8.5 m/s and comes to rest in a time interval of 8.0 sec. (a) What is the impulse given to the nail? (b) What is the average force acting on the nail? ANSWER: The change in momentum of the hammer is Dp=p f - p 0 where the final momentum of the hammer is zero p f =0 since the hammer comes to rest. The initial momentum of the hammer is p 0 = kg ä 8.5 m/s = 0 kg-m/s. So the change in momentum of the hammer is Dp=p f - p 0 = (0-0 kg-m/s) = -0 kg-m/s. (The positive x direction is in the direction of the motion of the hammer so the initial velocity of the hammer 8.5 m/s is positive.) The change in momentum of the hammer equals the impulse due to the nail on the hammer which by Newton's nd law impulse of the nail on the hammer = F Dt= Dp = -0 Nt-sec where F is the average force of the nail on the hammer and Dt=8.0 msec. (msec=0-3 sec.) It is the force of the nail on the hammer that changes the momentum of the hammer. (The impulse of the hammer on the nail is equal in size to this but opposite in direction due to Newton's 3rd law and because the time of contact Dt is the same for the hammer and the nail.) So the average force of the nail on the hammer F is F = Dp Dt = -0 kg-mês 8.0 ä 0-3 s = -,750 Nt.

in the direction of the motion of the hammer so the initial velocity of the hammer 8.5 m/s is positive.) The change in momentum of the hammer equals the impulse due to the nail on the hammer which by Newton's nd law Giancoli 6th ed chap.7 problem solutions Rev.nb 3 impulse of the nail on the hammer = F Dt= Dp = -0 Nt-sec where F is the average force of the nail on the hammer and Dt=8.0 msec. (msec=0-3 sec.) It is the force of the nail on the hammer that changes the momentum of the hammer. (The impulse of the hammer on the nail is equal in size to this but opposite in direction due to Newton's 3rd law and because the time of contact Dt is the same for the hammer and the nail.) So the average force of the nail on the hammer F is F = Dp Dt = -0 kg-mês 8.0 ä 0-3 s = -,750 Nt. By Newton's 3rd law, the force of the hammer on the nail is equal in size and opposite in direction to F so the force of the hammer on the nail is +,750 Nt. and this is in the positive x direction as expected. * 8.5 0. 0. ê.008. 750 ü Problem #4 QUESTION: Two billiard balls of equal mass undergo a perfectly elastic head-on collision. If one ball's initial speed was.0 m/s and the other's was 3.0 m/s in the opposite direction, what will be their speeds after the collision? ANSWER: M M m/s 3 m/s Before the Collison M M X Vb Va After the Collision Va is the velocity of the ball on the right after the collision and Vb is the velocity of the ball on the left after the collision. Assuming momentum is conserved M ä m/s + M ä (-3 m/s) = Mä(-Vb) + MäVa and after cancellation of M's we get - 3 = -Vb + Va or - = -Vb + Va = Vb- (Equation #) The positive x direction is to the right and it is assumed the velocity of the ball on the right is positive after the collision so Va is positive and the ball on the left is assumed moving to the left with negative velocity (-Vb) after the collision since Vb>0. If these assumptions are incorrect, in the process of solving the problem Va and/or Vb may turn out to be negative and that will tell us our assumption(s) is/are incorrect and the balls are actually moving in the reverse directions after the collision. Assuming energy is conserved we get and after cancellation of Ms and / we get M ä H mêsl + M ä H-3 mêsl = MäH-VbL + MäVa 4 + 9 = Vb + Va or 3 = Vb + Va (Equation #) Equations # and # have two unknowns which we solve for by first writing equation # as Va = Vb - and using this

out to be negative and that will tell us our assumption(s) is/are incorrect and the balls are actually moving in the reverse directions after the collision. Assuming energy is conserved we get 4 Giancoli 6th ed chap.7 problem solutions Rev.nb and after cancellation of Ms and / we get M ä H mêsl + M ä H-3 mêsl = MäH-VbL + MäVa 4 + 9 = Vb + Va or 3 = Vb + Va (Equation #) Equations # and # have two unknowns which we solve for by first writing equation # as Va = Vb - and using this to eliminate Va in equation # obtaining 3 = (Vb - L + Vb or Vb - Vb - = 0 This is a quadratic equation for Vb which is easily solved to get + 4 + 4** ± 4+4** Vb= * 3 * - 4 + 4** - * Using Mathematica to check the results above: Solve@8 * X * X - * X - ã 0<, 8X<D 88X Ø -<, 8X Ø 3<< So there are two possible solution for Vb: st solution is Vb = - m/s and returning to Va = Vb- we get Va =-3m/s. Since both Va and Vb are minus it means we guessed wrong about the directions after the collisions. More importantly, this result says the particle b on the left passes through the particle a on the right and particle b has it's velocity unchanged. (and similarly for particle a). This is not possible physically so we reject this solution. nd solution is Vb= 3m/s and returning to Va = Vb- we get Va =m/s. Since both Va and Vb are positive we know we guessed right as to their directions. The st solution means that after the collision particle a has the same velocity it started with and the same for particle b. The only way this could happen is if the particles pass through each other but this is not physically possible. So the st solution is ruled out on physical grounds. As a check Mathematica can be used to solve the two equations: SolveA9-3 ã -Vb + Va, 3 ã Vb + Va =, 8Va, Vb<E 88Va Ø -3, Vb Ø -<, 8Va Ø, Vb Ø 3<< ü Problem #35 QUESTION: A m=90 kg sports car collides into the rear end of a M=300 kg SUV stopped at a red light. The bumpers lock, the brakes are locked, and the two cars skid forward.8 m before stopping. The police officer, knowing that the coefficient of kinetic friction between tires and road is 0.80 calculates the speed of the sports car at impact. What was that speed? ANSWER: The physical problem is similar to problem # above and we use the same diagram except the masses are different and the initial speed V 0 of the sports car is not known in problem #35.

Giancoli 6th ed chap.7 problem solutions Rev.nb 5 V 0 sports car SUV at rest Before Collision V f After Collision Momentum is conserved since there is no external force acting on the system (the sports car plus SUV) in the horizontal direction. (There is an external force (gravity) in the y-direction but there is no motion in the y direction.) Momentum is NOT conserved for the sports car and SUV separately. The sports car and SUV stick together and this usually means energy is NOT conserved or at least cannot be assumed conserved. The kinetic energy lost winds up as heat energy so energy is still conserved just kinetic energy of the center of mass is NOT. The initial momentum is p 0 = m V 0 = 90 kg ä V 0 and the final momentum is p f = Hm + ML ä V f =H90 kg + 300 kglä V f. Conservation of momentum means p 0 = p f so in this case, this means 90 kg ä V 0 = H90 kg + 300 kgl ä V f 90 + 300 3.5 90. V 0 = 3.5 V f So if we knew the final velocity V f of the sports car plus SUV right after the collision, then we would find the initial speed of the sports car V 0. The sports car plus SUV system travels a distance X=.8 m before stopping. Assume the initial kinetic energy of the sports car plus SUV equals the work done against friction mnx where N=(m+M)g is the normal force of the sports car plus SUV system and m=0.80 is the coefficient of friction. Thus Hm + ML ä V f = m Hm + MLg x The mass (m+m) cancels in the above equation and we solve for V f obtaining V f = m g x = ä0.80ä9.8 mës ä.8 m = 6.63 m/s

6 Giancoli 6th ed chap.7 problem solutions Rev.nb * 0.80 * 9.8 *.8 6.660 This value of V f =6.63 m/s can now be used to compute V 0 using the result from conservation of momentum V 0 = 3.5 V f so that V 0 = 3.5 * 6.63 mês 3.05 m s ü Problem #46 Calculate the center of mass or COM of the three-mass system shown below. Specify the COM relative the left-hand.0 kg mass Y.0 kg.5 kg. kg X 0.5 m 0.75 m X =.0 kg ä 0 m +.5 kg ä 0.5 m +. kg ä 0.75 m.0 kg +.5 kg +. kg = 0.44 m since using Mathematica to compute the numbers yields * 0 +.5 * 0.5 +. * 0.75 0.4375 ü Problem # 76.0 +.5 +. Two balls of masses m A = 40 gm = 0.04 kg and m B = 60 gm = 0.06 kg are suspended as show in the diagram below. The lighter ball is pulled away to a 60 angle with the vertical and released. (a) What is the velocity of the lighter ball before impact? (b) What will be the maximum height of each ball after the elastic collision?

Giancoli 6th ed chap.7 problem solutions Rev.nb 7 Energy is conserved from the release of mass m A until just before it hits mass m B. So the initial potential energy equals the kinetic energy of m A just before impact when it has a velocity V m A g h = m A V or V = g h The height h the mass rises vertically is given by and using this to compute V yields h= 30 cm - 30 cmäcos[60 ] = 5 cm = 0.5 m V = g h =.7 m/s Using Mathematica to check the calculation h = 0.30-0.30 * Cos@60 D 0.5 g = 9.8; V = * g * h.7464 Part b: Momentum is conserved when mass m A hits mass m B so we write p 0 = m V as the initial momentum and p f = m A V A + m B V B where V A is the velocity of m A after the collision and V B is the velocity of m B after the collision. Conservation of momentum yields m A V = m A V A + m B V B Using V=7. m/s in equation above together with m A = 40 gm = 0.04 kg and m B = 60 gm = 0.06 kg yields 0.04 kg ä.7 m/s = 0.04 kg ä V A + 0.06 kgäv B Simplifying this equation 0.0684 = 0.04ä V A + 0.06äV B equation # Assume kinetic energy K.E. is conserved for the collision process of m A with m B so m A V = m A V A + m B V B Utilization of the numerical values for m A, m B, and V in the above equation yields 0.04 kg ä H.7 mêsl = 0.04 kg äv A + 0.06 kg ä V B

Simplifying this equation 8 Giancoli 6th ed chap.7 problem solutions Rev.nb 0.0684 = 0.04ä V A + 0.06äV B equation # Assume kinetic energy K.E. is conserved for the collision process of m A with m B so m A V = m A V A + m B V B Utilization of the numerical values for m A, m B, and V in the above equation yields 0.04 kg ä H.7 mêsl = 0.04 kg äv A + 0.06 kg ä V B or a little more simply 0.8 = 0.04äV A + 0.06 ä V B equation # Equation # and # have two unknowns V A and V B. First solve equation # for V A = 0.684-0.06 V B then use this last 0.04 equation to eliminate V A in equation # and what results is a quadratic equation for V A which is easily solved. Mathematica can do the work for us: SolveA90.068 == 0.04 * VA + 0.06 * VB, 0.8 ã 0.04 * VA + 0.06 * VB =, 8VA, VB<E 88VA Ø -0.357497, VB Ø.3766<, 8VA Ø.775, VB Ø -0.06647<< The first solution VA=-0.36 m/s and VB=.37 m/s is the valid solution. The second solution makes no physical sense since it says mass m A passes through mass m B and m A continues on with the same velocity it had before the collision that is,.7 m/s and mass m B remains at rest (0.0 m/s is zero in comparison with.7 m/s) throughout. Mass A will rise up a distance ha =.0066 m determined from conservation of energy m A V A = m A g h A which after cancellation yields h A = V A =0.0066 m and something similar for mass B, that is, hb=0.096 m. Mathematica gives for the two heights g = 9.8; ha = 0.36 * g 0.00664 hb =.37 * g 0.095760 g