Linear Momentum and Collisions

Similar documents
Chapter 3 and Chapter 4

Physics for Scientists and Engineers. Chapter 9 Impulse and Momentum

EMU Physics Department.

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

Physics 105: Mechanics Lecture 13

Page 1. Physics 131: Lecture 14. Today s Agenda. Things that stay the same. Impulse and Momentum Non-constant forces

PHYS 1443 Section 002

Momentum. Momentum. Impulse. Momentum and Collisions

How does the momentum before an elastic and an inelastic collision compare to the momentum after the collision?

Physics 101 Lecture 9 Linear Momentum and Collisions

Chapter 8: Potential Energy and The Conservation of Total Energy

Energy and Energy Transfer

Physics 207, Lecture 13, Oct. 15. Energy

ONE-DIMENSIONAL COLLISIONS

Lecture 09 Systems of Particles and Conservation of Linear Momentum

PHYS 1441 Section 002 Lecture #15

p p +... = p j + p Conservation Laws in Physics q Physical states, process, and state quantities: Physics 201, Lecture 14 Today s Topics

Chapter 07: Kinetic Energy and Work

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

Period & Frequency. Work and Energy. Methods of Energy Transfer: Energy. Work-KE Theorem 3/4/16. Ranking: Which has the greatest kinetic energy?

EMU Physics Department

Chapter 11 Angular Momentum

Physic 231 Lecture 14

Physics 207 Lecture 13. Lecture 13

Chapter 9 Linear Momentum and Collisions

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

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

Conservation of Energy

Linear Momentum. Center of Mass.

Ground Rules. PC1221 Fundamentals of Physics I. Linear Momentum, cont. Linear Momentum. Lectures 17 and 18. Linear Momentum and Collisions

Momentum and Collisions. Rosendo Physics 12-B

RE 11.e Mon. Review for Final (1-11) HW11: Pr s 39, 57, 64, 74, 78 Sat. 9 a.m. Final Exam (Ch. 1-11)

Conservation of Energy

Physics 2A Chapter 9 HW Solutions

Chapter Seven - Potential Energy and Conservation of Energy

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

Conservation Laws (Collisions) Phys101 Lab - 04

Physics 106 Lecture 6 Conservation of Angular Momentum SJ 7 th Ed.: Chap 11.4

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

10/9/2003 PHY Lecture 11 1

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

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

CHAPTER 9 LINEAR MOMENTUM, IMPULSE AND COLLISIONS

Chapter 8. Momentum Impulse and Collisions. Analysis of motion: 2 key ideas. Newton s laws of motion. Conservation of Energy

Physics 2A Chapter 3 HW Solutions

CHAPTER 8 Potential Energy and Conservation of Energy

Week 9 Chapter 10 Section 1-5

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

Page 1. Clicker Question 9: Physics 131: Lecture 15. Today s Agenda. Clicker Question 9: Energy. Energy is Conserved.

Collisions! Short, Sharp Shocks

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

RETURN ONLY THE SCANTRON SHEET!

Spring Force and Power

Study Guide For Exam Two

9/19/2013. PHY 113 C General Physics I 11 AM-12:15 PM MWF Olin 101

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

Linear Momentum. Equation 1

You will analyze the motion of the block at different moments using the law of conservation of energy.

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

PHYSICS 203-NYA-05 MECHANICS

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

10/23/2003 PHY Lecture 14R 1

Physics 115. Molecular motion and temperature Phase equilibrium, evaporation

PHYS 1441 Section 002 Lecture #16

Center of Mass and Linear Momentum

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

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

Phys102 General Physics II

Chapter 8. Momentum, Impulse and Collisions (continued) 10/22/2014 Physics 218

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

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

AP Physics Enosburg Falls High School Mr. Bushey. Week 6: Work, Energy, Power

From Newton s 2 nd Law: v v. The time rate of change of the linear momentum of a particle is equal to the net force acting on the particle.

Chapter 5. Answers to Even Numbered Problems m kj. 6. (a) 900 J (b) (a) 31.9 J (b) 0 (c) 0 (d) 31.9 J. 10.

2.00 kg 4.00 kg 3.00 kg m. y com. (2.00 kg)(0.500 m) 4.00 kg m 3.00 kg m m m kg 4.00 kg 3.00 kg m.

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

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.

1. The number of significant figures in the number is a. 4 b. 5 c. 6 d. 7

τ rf = Iα I point = mr 2 L35 F 11/14/14 a*er lecture 1

Physics 131: Lecture 16. Today s Agenda

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

v c motion is neither created nor destroyed, but transferred via interactions. Fri. Wed (.18,.19) Introducing Potential Energy RE 6.

Physics 111 Final Exam, Fall 2013, Version A

Physics 111: Mechanics Lecture 11

PHYSICS 231 Lecture 18: equilibrium & revision

Experiment 5 Elastic and Inelastic Collisions

Linear Momentum. Center of Mass.

Force = F Piston area = A

Chapters 18 & 19: Themodynamics review. All macroscopic (i.e., human scale) quantities must ultimately be explained on the microscopic scale.

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

Physics 2A Chapters 6 - Work & Energy Fall 2017

5/24/2007 Collisions ( F.Robilliard) 1

Chapter 4: Linear Momentum and Collisions

= 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]

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

Chapter 2. Pythagorean Theorem. Right Hand Rule. Position. Distance Formula

So far: simple (planar) geometries

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.

Problem While being compressed, A) What is the work done on it by gravity? B) What is the work done on it by the spring force?

Physics 4B. Question and 3 tie (clockwise), then 2 and 5 tie (zero), then 4 and 6 tie (counterclockwise) B i. ( T / s) = 1.74 V.

Transcription:

Lnear Momentum and Collsons Chater 9 Lnear Momentum [kg m/s] x y mv x mv y Newton s nd Law n terms o momentum:

Imulse I - [kg m/s] I t t Fdt I = area under curve bounded by t axs Imulse-Momentum Theorem Proo:

Queston Fnd the ollowng usng the estmated orce-tme curve shown below or an object subjected to a orce F over a tme nterval o 5.00 s.: o The mulse delvered by the orce. o The average orce F avg. Queston A tenns layer receves a shot wth the ball (0.060 kg) ntally travelng horzontally at 0.0 m/s and returns the ball horzontally at 40.0 m/s n the ooste drecton. I the racket s n contact wth the ball or 4.00 x 0-3 s, determne the ollowng: The mulse delvered by the tenns racket The magntude o the average orce on the ball? 3

Conservaton o Lnear Momentum and Collsons Momentum s conserved whenever a system o nteractng artcles s solated (.e., no net external orces act on the system and thereore there s no net mulse) When there are no external orces (F ext = 0) on a system, ts mulse I = 0, and ts momentum s conserved! 4

Momentum and Auto Collsons In any collson, the total o the system s always conserved Elastc Collson - no hyscal contact occurs Inelastc Collson - hyscal contact occurs 5

6 Elastc Collson (-D) conserves both the momentum and knetc energy o the system K K K K v = m - m m + m æ è ç ö ø v + m m + m æ è ç ö ø v v = m m + m æ è ç ö ø v + m - m m + m æ è ç ö ø v Inelastc collson (-D) conserves only the momentum o the system and not ts knetc energy v m m ( ) Perectly nelastc: Inelastc:

Queston 3 Two blocks are ree to slde along the rctonless wooden track below. The masses o the blocks are m =.00 kg and m = 4.0o kg. Both masses are released rom rest at a heght o h = 5.00 m. When they meet at the bottom, they undergo an elastc-head on collson (although they don t touch). Calculate: (a) The seed o m and m just beore the collson (b) The seed o m and m just ater the collson (c) The maxmum heght that m and m rse ater the collson. Queston 4 An m = 0.0 kg wad o clay s hurled horzontally at an m = 0.00 kg wooden block ntally at rest on a horzontal rough surace. Just beore the nelastc collson, the clay strkes the block wth v c and stcks to t. Just ater the collson they both move wth v cb. The clay-block system then slde a dstance Δr = 7.50 m beore comng to rest v cb = 0 due to the orce o rcton (μ k = 0.650). o What s the magntude o ther velocty v cb just ater the collson? o What was the magntude o the clay s velocty v c just beore the collson? v c m m + m m v cb 7

Inelastc Collsons (-D) x y x y x y x y Queston 5 A car m = 500 kg s travelng due east at v = 5.0 m/s. A van m = 500 kg s travelng due north at v = 0.0 j m/s. They collde and move together wth a common seed v at an angle θ, N o E (as shown). o Fnd θ and v 8

The Center o Mass ont where the total mass o a system s concentrated CM can move as mass dstrbuton changes athlete usng hyscs 9

cm o a system o ont artcles x cm xm xm... m m... x m m M x m tot In -D: Queston 6 Fnd the CM o the system shown below where m = m =.0 kg, and m 3 =.0 kg. 0

cm o an extended symmetrc object o unorm mass dstrbuton Queston 7 A unorm sheet o steel s shaed as shown. o Fnd the x and y coordnates o the center o mass o the sheet

cm o an extended object x cm M tot xdm and y cm M tot ydm where M tot dm I the mass s unorm, we relate dm to a constant mass densty. lnear mass densty area mass densty volume mass densty M dm L d M dm A da M dm V dv I the mass o the object s non-unorm then the mass densty wll have a satal deendence,.e., λ = ax, that must be ntegrated. Queston 8 Show that the CM o a unorm rod o total mass M and length L les mdway between ts ends. x cm L xdm M 0 L x dx M 0 L xdx M 0 M L xdx M L 0 L L L

Queston 9 Suose a rod o length L = 0.30 m has a non-unorm mass dstrbuton, so that ts mass er unt length vares as λ(x) = (50 + 0x) g/m. a) Determne ts mass: M. b) Fnd ts cm: x cm CM o a trangle o unorm mass x cm = (/3)a and y cm = (/3)b 3