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)

Similar documents
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

Chapter 11 Angular Momentum

Chapter 3 and Chapter 4

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

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

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

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

Chapter 11 Torque and Angular Momentum

Conservation of Angular Momentum = "Spin"

Chapter 7: Conservation of Energy

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

Collisions! Short, Sharp Shocks

Linear Momentum and Collisions

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

Physics for Scientists and Engineers. Chapter 9 Impulse and Momentum

Momentum. Momentum. Impulse. Momentum and Collisions

Study Guide For Exam Two

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

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

Chapter 8: Potential Energy and The Conservation of Total Energy

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

Physics 207, Lecture 13, Oct. 15. Energy

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

Physic 231 Lecture 14

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

EMU Physics Department

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

10/23/2003 PHY Lecture 14R 1

Conservation of Energy

Chapter 11: Angular Momentum

Important Dates: Post Test: Dec during recitations. If you have taken the post test, don t come to recitation!

Dynamics of Rotational Motion

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

PHYS 1441 Section 002 Lecture #15

PHYSICS 231 Review problems for midterm 2

10/9/2003 PHY Lecture 11 1

Physics 105: Mechanics Lecture 13

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

PHYS 1443 Section 002

total If no external forces act, the total linear momentum of the system is conserved. This occurs in collisions and explosions.

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

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

Conservation of Energy

Physics 101 Lecture 9 Linear Momentum and Collisions

Chapter 07: Kinetic Energy and Work

EMU Physics Department.

WYSE Academic Challenge 2004 State Finals Physics Solution Set

Lecture 09 Systems of Particles and Conservation of Linear Momentum

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

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

ONE-DIMENSIONAL COLLISIONS

Physics 2A Chapter 9 HW Solutions

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.

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

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

Linear Momentum. Center of Mass.

Conservation Laws (Collisions) Phys101 Lab - 04

Rotational Dynamics. Physics 1425 Lecture 19. Michael Fowler, UVa

Physics 207: Lecture 27. Announcements

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

PHYSICS 231 Lecture 18: equilibrium & revision

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?

Chapter Seven - Potential Energy and Conservation of Energy

So far: simple (planar) geometries

RETURN ONLY THE SCANTRON SHEET!

CHAPTER 8 Potential Energy and Conservation of Energy

Week 9 Chapter 10 Section 1-5

CHAPTER 10 ROTATIONAL MOTION

Class: Life-Science Subject: Physics

PHYSICS 203-NYA-05 MECHANICS

Physics 131: Lecture 16. Today s Agenda

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.

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

Physics 207 Lecture 13. Lecture 13

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

MEASUREMENT OF MOMENT OF INERTIA

Chapter 9 Linear Momentum and Collisions

PHYS 1441 Section 002 Lecture #16

CHAPTER 9 LINEAR MOMENTUM, IMPULSE AND COLLISIONS

Momentum and Collisions. Rosendo Physics 12-B

Physics 111: Mechanics Lecture 11

Spring Force and Power

11. Dynamics in Rotating Frames of Reference

Physics 181. Particle Systems

Rigid body simulation

Chapter 7. Potential Energy and Conservation of Energy

Supplemental Instruction sessions next week

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

Physics 2A Chapter 3 HW Solutions

Chapter 12 Equilibrium & Elasticity

Experiment 5 Elastic and Inelastic Collisions

K = 100 J. [kg (m/s) ] K = mv = (0.15)(36.5) !!! Lethal energies. m [kg ] J s (Joule) Kinetic Energy (energy of motion) E or KE.

University of Bahrain College of Science Dept. of Physics PHYCS 102 FINAL EXAM

Chapter 21 - The Kinetic Theory of Gases

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.

PHYS 705: Classical Mechanics. Newtonian Mechanics

Force = F Piston area = A

Physics 231. Topic 8: Rotational Motion. Alex Brown October MSU Physics 231 Fall

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

NEWTON S LAWS. These laws only apply when viewed from an inertial coordinate system (unaccelerated system).

Transcription:

We..7 -.9, (.) Moton Wth & Wthout Torque E. ab r. otaton ab Evals.0 Quantzaton, Quz, ect Evals E.e Mon. evew or nal (-) HW: Pr s 39, 57, 64, 74, 78 Sat. 9 a.m. nal Exam (Ch. -)

Usng ngular Momentum The measure o moton about a pont r p r Magntue p r p r p r sn p Magntue an Drecton =r p = (p z r y p y r z ), (p x r z p z r x ), (p y r x p x r y ) Drecton Orent ght han so ngers curl rom the axs an wth moton, then thump ponts n recton o angular momentum.

ngular Momentum Prncple rbll pole ball rope p ball han pole Magntue (yet another cross prouct) r r sn r r t ( ) about Quantes moton about a pont sn r sn ( about) where, ( Torque about) Interacton that changes moton about a pont r ( rom) Drecton (yet another cross prouct) r

Mult-Partcle ngular Momentum Prncple Wth Mult-Partcle ngular Momentum c s ext ext 3ext... t where r, etc. cs cs cms transs ext Star cm s ext rotcm or rg objects rotcm I cm cm r s r s r 3s Clou o Dust ext 3 3ext ext

Example: unorm sol sk wth raus 9 cm has mass 0.9 kg (moment o nerta I = ½M ). constant orce N s apple as shown. t the nstant shown, the angular velocty o the sk s 45 raans/s n the z recton. The length o the strng s 8 cm. t ths nstant, what are the magntue an recton o the angular momentum about the center o the sk? y z (z-axs ponts out o page) x What are the magntue an recton o the torque on the sk, about the center o mass o the sk? The strng s pulle or 0. s. What are the magntue an recton o the angular mpulse apple to the sk urng ths tme? ter the torque has been apple or 0. s, what are the magntue an recton o the angular momentum about the center o the sk? t ths later tme, what are the magntue an recton o the angular velocty o the sk?

Spnnng Skater Zero-Torque Systems Demo: spnnng umb bells Solar system ormaton Intal rot. rot. rot rot.. rot. rot. mass arther I rom axs: I larger smaller I 0 ave t nal mass closer to axs: I smaller larger What about the energy? K rot E I I I I nt. other E E E 0 0 K rot Ent. other nt. other nt. other Increase kc energy uele by change n nternal energy (Wheates) http://leng.lamost.org/courses/astrotoay/ CHISSON/T35/HTM/T350.HTM Increase rotatonal kc energy uele by change n nternal energy (gravtatonal potental) lso conser: ver, St-spn & lp spnnng wheel

y Completely Inelastc Collson & ngular Moton z (z-axs ponts out o page) x Chl runs an jumps on playgroun merry-goroun. or the system o the chl + sk (exclung the axle an the Earth), whch statement s true rom just beore to just ater mpact? K s total (macroscopc) kc energy P s total (lnear) momentum s total angular momentum (about the axle) What s the ntal angular momentum o the chl + sk about the axle? a. K, P, an o not change b. P, an o not change c. oes not change. K an P o not change e. K an o not change a) < 0, 0, 0 > b) < 0, mv, 0 > c) < 0, mv, 0 > ) < 0, 0, mv > e) < 0, 0, mv >

y Completely Inelastc Collson & ngular Moton z (z-axs ponts out o page) x The sk has moment o nerta I, an ater the collson t s rotatng wth angular spee. The rotatonal angular momentum o the sk alone (not countng the chl) s ter the collson, what s the spee (n m/s) o the chl? a. < 0, 0, 0 > b. < 0, I, 0 > c. < 0, I, 0 >. < 0, 0, I > e. < 0, 0, I > a. b. c.. / e. ter the collson, what s translatonal angular momentum o the chl about the axle? a. < 0, 0, 0 > b. < 0, m, 0 > c. < 0, m, 0 >. < 0, m(), 0 > e. < 0, m(), 0 >

y Completely Inelastc Collson & ngular Moton What s the nal angular spee o the merry-go-roun ater the k jumps on? z (z-axs ponts out o page).. t m,0 0,, 0 0, I.,0 0, mv 0, sk I cm m. g. r. chl. chl. M,0 0, m,0 0, mv,0 sk. cm M x System: chl + merry-go-roun ctve envronment: none that change angular momentum pproxmatons: neglgble rctonal torque at axel xs: xle 0, m M,0 0, mv, 0 m M mv m mv M M m v easonable?

Two-Step Example: blob o clay (mass m) s roppe a stance h to lan on an stck to a wheel (mass M, raus ) horzontally ½ o axs. What s the wheel s angular spee just ater the collson? Step : Ball alls to wheel; use energy E E K & B 0 E B B. nt EE U E, B mv mv mgh 0 B. B.0 0 v B. gh Step : Ball & wheel colle; use angular momentum System: Ball + Earth ctve envronment: none pproxmatons: neglgble rag Moment 0 m xs: C System: Ball + Wheel ctve envronment: no torques pproxmatons: tme nterval small enough axel rcton an Earth s gravtaton have neglgble eect W & BC. By rght-han-rule, all n the +z BC. recton IW & B. C mvbr Beore collson, r I W & B. C Irng. cm I. IW & B. C m gh IW & B. C M m m m gh M M m m gh m gh M m easonable? m cm gh M m M h Moment Moment / v B.

ngular Momentum: t ( ) about Three unamental Prncples ( about) (lnear) Momentum: t p E Energy: W Example all three together! Say we have a unorm 0.4 kg puck wth an 8 cm raus. 4 cm strng s ntally wrappe aroun ts crcumerence. I t s on a rctonless surace an a 0 N orce s apple to the en o the strng untl t s unwoun l = 0.4 m I puck = 0.08m m =? =? v cm =? a. What wll be ts rate o rotaton when the strng s ully unwoun? Energy Prncple K r E total W E trans nt r cm K rot l I I l I l t? l I l m l m K cm " W cm "

ngular Momentum: t ( ) about Example all three together! Say we have a unorm 0.4 kg puck wth an 8 cm raus. 4 cm strng s ntally wrappe aroun ts crcumerence. I t s on a rctonless surace an a 0 N orce s apple to the en o the strng untl t s unwoun l = 0.4 m = 0.08m Three unamental Prncples ( about) (lnear) Momentum: t v cm =? I puck =? m t? a. What wll be ts rate o rotaton when the strng s ully unwoun? b. How long was the orce apple? ngular Momentum Prncple (axs through nal locaton o cm) t t trans rot trans rot.. ) (.. ) t I r a t Torque an nal angular velocty n z recton l I I m m t t m m p E Energy: W l m ml K " " cm W cm

ngular Momentum: t ( ) about Example all three together! Say we have a unorm 0.4 kg puck wth an 8 cm raus. 4 cm strng s ntally wrappe aroun ts crcumerence. I t s on a rctonless surace an a 0 N orce s apple to the en o the strng untl t s unwoun l = 0.4 m I puck = 0.08m m Three unamental Prncples ( about) =? (lnear) Momentum: t t v cm =? a. What wll be ts rate o rotaton when the strng s ully unwoun? ml b. How long was the orce apple? t You try: c. How quckly s the puck nally slng, v cm?? p E Energy: W l m K " " cm W cm. How ar has the puck move,?

Mon. Tues. We. ab r..4-.6, (.3) ngular Momentum Prncple & Torque.7 -.9, (.) Moton Wth & Wthout Torque otaton Course Evals.0 Quantzaton, Quz E.c EP E. E.e Mon. evew or nal (-) HW: Pr s 39, 57, 64, 74, 78 Sat. 9 a.m. nal Exam (Ch. -)