Please initial the statement below to show that you have read it

Similar documents
Please initial the statement below to show that you have read it

EN40: Dynamics and Vibrations. Homework 4: Work, Energy and Linear Momentum Due Friday March 1 st

ENGN 40 Dynamics and Vibrations Homework # 7 Due: Friday, April 15

EN40: Dynamics and Vibrations. Homework 7: Rigid Body Kinematics

Chapter 11 Angular Momentum

PHYSICS 231 Review problems for midterm 2

Homework 2: Kinematics and Dynamics of Particles Due Friday Feb 7, 2014 Max Score 45 Points + 8 Extra Credit

Angular Momentum and Fixed Axis Rotation. 8.01t Nov 10, 2004

1.3 Hence, calculate a formula for the force required to break the bond (i.e. the maximum value of F)

Study Guide For Exam Two

Physics 111 Final Exam, Fall 2013, Version A

11. Dynamics in Rotating Frames of Reference

Chapter 8. Potential Energy and Conservation of Energy

Week3, Chapter 4. Position and Displacement. Motion in Two Dimensions. Instantaneous Velocity. Average Velocity

Physics 141. Lecture 14. Frank L. H. Wolfs Department of Physics and Astronomy, University of Rochester, Lecture 14, Page 1

10/23/2003 PHY Lecture 14R 1

Physics 207: Lecture 20. Today s Agenda Homework for Monday

GAUTENG DEPARTMENT OF EDUCATION SENIOR SECONDARY INTERVENTION PROGRAMME PHYSICAL SCIENCES GRADE 12 SESSION 1 (LEARNER NOTES)

= 1.23 m/s 2 [W] Required: t. Solution:!t = = 17 m/s [W]! m/s [W] (two extra digits carried) = 2.1 m/s [W]

Week 11: Chapter 11. The Vector Product. The Vector Product Defined. The Vector Product and Torque. More About the Vector Product

Name: PHYS 110 Dr. McGovern Spring 2018 Exam 1. Multiple Choice: Circle the answer that best evaluates the statement or completes the statement.

Physics 207 Lecture 6

a) No books or notes are permitted. b) You may use a calculator.

A Tale of Friction Basic Rollercoaster Physics. Fahrenheit Rollercoaster, Hershey, PA max height = 121 ft max speed = 58 mph

Chapter 3. r r. Position, Velocity, and Acceleration Revisited

Chapter 11: Angular Momentum

Section 8.1 Exercises

Rotational and Translational Comparison. Conservation of Angular Momentum. Angular Momentum for a System of Particles

First Law: A body at rest remains at rest, a body in motion continues to move at constant velocity, unless acted upon by an external force.

Physics 40 HW #4 Chapter 4 Key NEATNESS COUNTS! Solve but do not turn in the following problems from Chapter 4 Knight

SCHOOL OF COMPUTING, ENGINEERING AND MATHEMATICS SEMESTER 2 EXAMINATIONS 2011/2012 DYNAMICS ME247 DR. N.D.D. MICHÉ

Dynamics 4600:203 Homework 08 Due: March 28, Solution: We identify the displacements of the blocks A and B with the coordinates x and y,

Chapter 3 and Chapter 4

PHYS 1441 Section 002 Lecture #15

Physics 2A Chapter 3 HW Solutions

EN40: Dynamics and Vibrations. Final Examination Wed May : 2pm-5pm

CHAPTER 5 NUMERICAL EVALUATION OF DYNAMIC RESPONSE

Linear Momentum. Center of Mass.

Physics 111: Mechanics Lecture 11

Please review the following statement: I certify that I have not given unauthorized aid nor have I received aid in the completion of this exam.

Please review the following statement: I certify that I have not given unauthorized aid nor have I received aid in the completion of this exam.

Please review the following statement: I certify that I have not given unauthorized aid nor have I received aid in the completion of this exam.

Math1110 (Spring 2009) Prelim 3 - Solutions

Supplemental Instruction sessions next week

Physics 207 Lecture 13. Lecture 13

Recitation: Energy, Phys Energies. 1.2 Three stones. 1. Energy. 1. An acorn falling from an oak tree onto the sidewalk.

Final Examination Thursday May Please initial the statement below to show that you have read it

MEASUREMENT OF MOMENT OF INERTIA

Irregular vibrations in multi-mass discrete-continuous systems torsionally deformed

So far: simple (planar) geometries

Modeling of Dynamic Systems

10/9/2003 PHY Lecture 11 1

coordinates. Then, the position vectors are described by

Physics 207: Lecture 27. Announcements

PHYS 1443 Section 004 Lecture #12 Thursday, Oct. 2, 2014

Moments of Inertia. and reminds us of the analogous equation for linear momentum p= mv, which is of the form. The kinetic energy of the body is.

Chapter 8 Potential Energy and Conservation of Energy Important Terms (For chapters 7 and 8)

SUMMARY Phys 2113 (General Physics I) Compiled by Prof. Erickson. v = r t. v = lim t 0. p = mv. a = v. a = lim

Displacement at any time. Velocity at any displacement in the x-direction u 2 = v ] + 2 a x ( )

If the solution does not follow a logical thought process, it will be assumed in error.

Please review the following statement: I certify that I have not given unauthorized aid nor have I received aid in the completion of this exam.

Dynamics of Rotational Motion

Week 8: Chapter 9. Linear Momentum. Newton Law and Momentum. Linear Momentum, cont. Conservation of Linear Momentum. Conservation of Momentum, 2

Physics for Scientists and Engineers. Chapter 9 Impulse and Momentum

PHYSICS 203-NYA-05 MECHANICS

I certify that I have not given unauthorized aid nor have I received aid in the completion of this exam.

Problem Points Score Total 100

Physics 5153 Classical Mechanics. Principle of Virtual Work-1

Final Examination Thursday May Please initial the statement below to show that you have read it

LAGRANGIAN MECHANICS

Gravitational Acceleration: A case of constant acceleration (approx. 2 hr.) (6/7/11)

Physics 114 Exam 3 Spring Name:

Part C Dynamics and Statics of Rigid Body. Chapter 5 Rotation of a Rigid Body About a Fixed Axis

PY2101 Classical Mechanics Dr. Síle Nic Chormaic, Room 215 D Kane Bldg

I have not received unauthorized aid in the completion of this exam.

The classical spin-rotation coupling

PHYS 1441 Section 002 Lecture #16

Please review the following statement: I certify that I have not given unauthorized aid nor have I received aid in the completion of this exam.

Chapter 11 Torque and Angular Momentum

ONE-DIMENSIONAL COLLISIONS

Week 9 Chapter 10 Section 1-5

Angular momentum. Instructor: Dr. Hoi Lam TAM ( 譚海嵐 )

Chapter 8: Potential Energy and The Conservation of Total Energy

Conservation of Energy

Lecture 16. Chapter 11. Energy Dissipation Linear Momentum. Physics I. Department of Physics and Applied Physics

where v means the change in velocity, and t is the

Conservation of Angular Momentum = "Spin"

CHAPTER 8 Potential Energy and Conservation of Energy

10/24/2013. PHY 113 C General Physics I 11 AM 12:15 PM TR Olin 101. Plan for Lecture 17: Review of Chapters 9-13, 15-16

Four Bar Linkages in Two Dimensions. A link has fixed length and is joined to other links and also possibly to a fixed point.

Please review the following statement: I certify that I have not given unauthorized aid nor have I received aid in the completion of this exam.

Slide. King Saud University College of Science Physics & Astronomy Dept. PHYS 103 (GENERAL PHYSICS) CHAPTER 5: MOTION IN 1-D (PART 2) LECTURE NO.

Physics 181. Particle Systems

Physics 5153 Classical Mechanics. D Alembert s Principle and The Lagrangian-1

Ph.D. Qualifying Examination in Kinetics and Reactor Design

Effect of loading frequency on the settlement of granular layer

TIME OF COMPLETION NAME SOLUTION DEPARTMENT OF NATURAL SCIENCES. PHYS 2211, Exam 2 Section 1 Version 1 October 18, 2013 Total Weight: 100 points

Spring Force and Power

Chapter 7. Potential Energy and Conservation of Energy

Please review the following statement: I certify that I have not given unauthorized aid nor have I received aid in the completion of this exam.

Transcription:

EN40: Dynamcs and Vbratons Mdterm Examnaton Thursday March 5 009 Dvson of Engneerng rown Unversty NME: Isaac Newton General Instructons No collaboraton of any knd s permtted on ths examnaton. You may brng 3 double sded pages of reference notes. No other materal may be consulted Wrte all your solutons n the space provded. No sheets should be added to the exam. Make dagrams and sketches as clear as possble, and show all your dervatons clearly. Incomplete solutons wll receve only partal credt, even f the answer s correct. If you fnd you are unable to complete part of a queston, proceed to the next part. Please ntal the statement below to show that you have read t `y affxng my name to ths paper, I affrm that I have executed the examnaton n accordance wth the cademc Honor Code of rown Unversty. PLESE WRITE YOUR NME OVE LSO! IN 1 (3 ponts) (4 ponts) 3. (8 ponts) 4. (7 ponts) 5. (8 ponts) TOTL (30 ponts)

a a a (a) V (b) V (c) V 1. The fgure shows a car that travels along a crcular road. In Fg 1(a), the car travels at constant speed In Fg 1(a), the drver s brakng, and the car s speed s decreasng In Fg 1(c), the drver has her foot on the gas and the car s speed s ncreasng. Draw an arrow on each of fgures (a), (b), (c) to show the approxmate drecton of the car s acceleraton vector. [1 POINT ECH]. The fgure shows a vbraton measurement from a velocty transducer. The vbraton may be assumed to be harmonc. Estmate (a) The perod of oscllaton 4 cycles n 0.1sec gves T=0.1/4=0.05s (b) The angular frequency of oscllaton ngular frequency s 80 rad / s T (c) The ampltude of the velocty 5 cm/s (d) The ampltude of the dsplacement. X V / 5 / (80 ) 1/ (16 ) cm 0 0 [1 POINT ECH]

3. The goal of ths problem s to estmate the shortest stoppng dstance for a bcycle durng rear-wheel brakng. ssume that t tme t=0 the bcycle has velocty V. t ths nstant, the rder brakes hard enough to lock the rear wheel, causng t to skd. The coeffcent of frcton between the rear wheel and the ground s denoted by The front wheel rolls freely. r resstance may be neglected. h d L 3.1 Draw the forces actng on the bcycle and rder, usng the fgure shown. The bcycle and rder together may be dealzed as a partcle on a massless frame. T mg N N [ POINTS] 3. Wrte down Newton s law of moton F=ma and the moment balance equaton M=0 about the center of mass, expressng your answer as components n the bass shown. T ( N N mg) ma N ( L d) N d T h k 0 3.3 Hence, calculate an expresson for the acceleraton of the bcycle n terms of, g, d and h. [ POINTS] The frcton law gves T N. The moment equaton and vertcal component of Newtons law are N N mg 0 Elmnate N : N ( L d) N ( d h) 0 ( L d) N N ( d h) mg( L d) 0 N mg( L d) / ( L h) Fnally the component of F=ma shows that a T / m N / m mg( L d) / ( L h) [ POINTS] 3

3.4 Deduce a formula for the stoppng dstance n terms of V,, g, d and h. The constant acceleraton formulas gve 0 V at V 1 d Vt at V ( L h) / mg( L d) a [ POINTS] 4. The fgure shows an expermental apparatus for measurng the resttuton coeffcent of, e.g. a golfball or a bowlng ball. It uses the followng procedure pendulum (a golf-club head, e.g.) s swung to a known ntal angle 1 and then dropped from rest so as to strke the ball The angle of follow-through of the pendulum s recorded Your goal s to derve a formula that can be used to determne the resttuton coeffcent e from the measured data. m 1 l v m 1 m m 4.1 Usng energy conservaton, derve an expresson for the speed V of the mass on the end of the pendulum ust before t strkes the ball, n terms of 1, l and the gravtatonal acceleraton. Energy conservaton gves 1 mgl(1 cos 1) mv V gl(1 cos 1) [ POINTS] 4. Smlarly, derve an expresson for the speed v 1 of the mass on the end of the pendulum ust after t strkes the ball, n terms of, l and the gravtatonal acceleraton. v gl(1 cos ) 1 [1 POINT] 4.3 Use momentum conservaton to calculate an expresson for the velocty v of the ball ust after t s struck, n terms of V and v 1, and any other necessary parameters. Momentum conservaton durng the collson requres that m V m v m v v m V v / m 1 1 1 1 1 [ POINTS] 4

4.4 Hence, deduce a formula for the coeffcent of resttuton, n terms of 1,, l, and g, and any other necessary parameters. The resttuton coeffcent formula gves v v e(0 V ) e ( v v ) / V 1 1 e m V v / ( Vm ) v / V 1 1 1 m1 ( m1 m (1 cos ) v1 m1 ( m1 m ) gl ) e m m V m m gl(1 cos ) 1 m1 ( m1 m ) m m (1 cos ) 1 (1 cos ) [ POINTS] 5. The fgure shows an dealzaton of a motor mounted on a flexble vbraton-solaton support. The motor turns the shaft at constant angular speed, so that t. The motor s free to move vertcally, but s prevented from movng horzontally or rotatng. The vbraton solator can be dealzed as a sprng wth stffness k and unstretched length L 0. The mass of the motor and the shaft may be neglected. The goal of ths problem s to derve an equaton of moton for the vertcal poston of the motor h(t). d motor m k,l 0 h 5.1 Wrte down an expresson for the poston vector of the mass m n terms of h, d, and r d cos h d sn 5. Hence, calculate a formula for the acceleraton of the mass m n terms of d, and and the tme dervatves of h. [1 POINT] d h a d cos d sn dt [ POINTS] 5

5.3 Draw a free body dagram for the solated porton of the system shown n the fgure (you can draw forces and moments drectly on the fgure). Idealze the motor and shaft as a massless frame. Note that the motor s prevented from movng horzontally and s also prevented from rotatng. N M m mg F s [3 POINTS] 5.4 Hence, show that the equaton of moton for h s gven by d h k k h L 0 g d snt dt m m Newton s law gves d h N ( Fs mg) md cos m d sn dt The sprng force law s Fs k( h L0 ). Take the component and re-arrange to get the answer stated. [ POINTS] 6