Your Thoughts. Mechanics Lecture 11, Slide 1

Size: px
Start display at page:

Download "Your Thoughts. Mechanics Lecture 11, Slide 1"

Transcription

1 Your Thoughts Honestly, I'm finding this class a bit difficult to keep up with especially coming straight off that midterm, although it wasn't bad. There's a lot going on and I understand that, that's part of the challenge of college, but with quiz, homework, prelecture, checkpoint, prelab, lab, discussion, discussion quiz, opfonal homework, the exam, and studying on top of 14 other credit hours and extracurriculars and drama it seems a bit much. I really like this class and am gonna sfck it out, but I just need some sleep and forgieness from Tony in the 10am lecture. Had exam tonight and a paper to write and an exam tomorrow, had to just click through the prelecture and checkpoint. Going to come back tomorrow night and watch it again and take notes. Please go oer the checkpoints in lecture. It's late and I didn't really think about my answers to the checkpoints, so a clarificafon would help. Is it true that in the center of mass reference frame momentum is ALWAYS consered, or always equals zero? Can we go oer this more in lecture? I'm going to keep menfoning this: please do something about all the disrupfe students during lecture! Maybe they will all drop auer surely doing poorly on the first exam, but it is not fair to allow these students to ruin the quality of lecture for others. Mechanics Lecture 11, Slide 1

2 Physics 211 Lecture 11 Today s Concept: Momentum ConseraFon Mechanics Lecture 11, Slide 2

3 Exam 1 We will post the grades in the next few days. We neer scale anything down. If the aerage is below 75% we will scale the exam up. You will be able to see your answers to each quesfon in the course gradebook. You will get your exam booklets back in discussion next week. We will post the exam (with detailed solufons) on smartphysics Mechanics Lecture 11, Slide 3

4 Recap r P r = m tot i i i Mechanics Lecture 11, Slide 4

5 Can you go oer energy conseration in collisions? That description in the prelecture confused me. Energy (Prelecture 8) Mechanics Lecture 11, Slide 5

6 Comparison of Momentum and Energy Concepts Δ K = Wtotal r r = F Δx net Lecture 7 (2 weeks ago) Work KineFc Energy theorem r r Lecture 14 (next week) Δ P = F Δt total net Impulse- Momentum theorem Mechanics Lecture 11, Slide 6

7 Clicker Question A wood block rests at rest on a table. A bullet shot into the block stops inside, and the bullet plus block start sliding on the fricfonless surface. The horizontal momentum of the bullet plus block remains constant Before AUer A) Before the collision. B) During the collision C) AUer the collision D) All of the aboe E) Only A and C aboe As long as there are no external forces acfng on the system Mechanics Lecture 11, Slide 7

8 It s a ector equation r dp dt p 1 tot = r F Net, External p init p 2 p 2 p 1 p final θ Mechanics Lecture 11, Slide 8

9 CheckPoint Suppose you are on a cart inifally at rest that rides on a fricfonless track. If you throw a ball off the cart towards the leu, will the cart be put into mofon? LeU Right A) Yes, and it moes to the right. B) Yes, and it moes to the leu. ConseraFon of momentum means the cart must moe to the right since the ball moes to the leu. C) No, it remains in place. Mechanics Lecture 11, Slide 9

10 CheckPoint Suppose you are on a cart which is inifally at rest that rides on a fricfonless track. You throw a ball at a erfcal surface that is firmly ajached to the cart. If the ball bounces straight back as shown in the picture, will the cart be put into mofon auer the ball bounces back from the surface? LeU Right A) Yes, and it moes to the right. B) Yes, and it moes to the leu. C) No, it remains in place. Mechanics Lecture 11, Slide 10

11 CheckPoint LeU Right A) Yes, and it moes to the right. B) Yes, and it moes to the leu. C) No, it remains in place. B) The ball ends up moing the right direction so the cart must moe to the left to consere momentum. C) At first the cart will moe right but then when the ball hits the wall the cart will moe back to the left. Mechanics Lecture 11, Slide 11

12 Your Question Say we took the same cart from the first checkpoint problem and put walls on either side of the man. If the man then threw a ball at one of the walls so that it would just bounce between the two walls, would the cart be set in motion and if so, in what direction? LeU Right A) The cart would moe back & forth as the ball bounced. B) The cart would not moe C) The cart would keep moing in the direcfon opposite the throw Mechanics Lecture 11, Slide 12

13 Clicker Question Suppose you are on a cart that is moing at a constant speed toward the leu on a fricfonless track. If you throw a massie ball straight up (relafe to the cart), how will the speed of the cart change? LeU Right A) Increase B) Decrease C) Will not change As long as there are no external forces acfng on the system, P total is consered Mechanics Lecture 11, Slide 13

14 CheckPoint Two balls of equal mass are thrown horizontally with the same inifal elocity. They hit idenfcal stafonary boxes resfng on a fricfonless horizontal surface. The ball hilng box 1 bounces back, while the ball hilng box 2 gets stuck. Which box ends up moing faster? A) Box 1 B) Box 2 C) same 1 2 Lets think about a slightly different ersion of this Mechanics Lecture 11, Slide 14

15 Clicker Question Two equal- mass balls swing down and hit idenfcal bricks while traeling at idenfcal speeds. Ball A bounces back, but ball B just stops when it hits the brick. Which ball is more likely to knock the brick oer? A B A) A B) B C) Equally likely. Mechanics Lecture 11, Slide 15

16 demo A B ΔP A ΔP B ΔP A > ΔP B The change in the momentum of the ball is bigger in A So the block gets a bigger kick in A Mechanics Lecture 11, Slide 16

17 CheckPoint Two balls of equal mass are thrown horizontally with the same inifal elocity. They hit idenfcal stafonary boxes resfng on a fricfonless horizontal surface. The ball hilng box 1 bounces back, while the ball hilng box 2 gets stuck. Which box ends up moing faster? A) Box 1 B) Box 2 C) same 1 2 Mechanics Lecture 11, Slide 17

18 Ballistic Pendulum m M H A projecfle of mass m moing horizontally with speed strikes a stafonary mass M suspended by strings of length L. Subsequently, m + M rise to a height of H. Gien H, what is the inifal speed of the projecfle? Mechanics Lecture 11, Slide 18

19 Breaking it down into steps before during auer m M H splat Which quanffes are consered before the collision? A) momentum (horizontal) B) mechanical energy C) both momentum and mechanical energy Mechanics Lecture 11, Slide 19

20 Breaking it down into steps before during auer m M H splat Which quanffes are consered during the collision? A) Momentum (horizontal) B) mechanical energy C) both momentum and mechanical energy m = ( m + M ) V Mechanics Lecture 11, Slide 20

21 Breaking it down into steps before during auer m M H splat Which quanffes are consered auer the collision A) momentum (horizontal) B) mechanical energy C) both momentum and mechanical energy 2 (1/ 2)( + ) = ( + ) M m V M m gh V 2 = 2gH Mechanics Lecture 11, Slide 21

22 Ballistic Pendulum m M H m = ( m + M ) V V 2 = 2gH V = m ( m+ M) m+ M = 2gH m = 2gH 1+ M m Mechanics Lecture 11, Slide 22

23 Ballistic Pendulum Demo L L L L m M H M + m d In the demo we measure forward displacement d, not H: L-H H d L L 2 H = = d 2 L + ( L H) L 2 d 2 2 = 1+ M m d g L (mph) = 3d(cm) for d << L Physics 211 Lecture 11, Slide 23

Your Thoughts. What is the difference between elastic collision and inelastic collision?

Your Thoughts. What is the difference between elastic collision and inelastic collision? Your Thoughts This seemed pretty easy...before we got the checkpoint questions What is the difference between elastic collision and inelastic collision? The most confusing part of the pre lecture was the

More information

Classical Mechanics Lecture 11

Classical Mechanics Lecture 11 Classical Mechanics Lecture 11 Today s Examples Center of Mass Today s Concept: Conservation of Momentum Inelastic Collisions Mechanics Lecture 11, Slide 1 Unit 10 Homework Problems Mechanics Lecture 10,

More information

Lecture 11: Conservation of Momentum

Lecture 11: Conservation of Momentum Lecture 11: Conservation of Momentum Today s Concept: Inelastic Collisions How did the chicken cross the frictionless road? It laid an egg and threw it backwards. Mechanics Lecture 11, Slide 1 Announcements

More information

Classical Mechanics Lecture 13

Classical Mechanics Lecture 13 Classical Mechanics Lecture 13 Today s Concepts: a) More on Elas5c Collisions b) Average Force during Collisions Mechanics Lecture 13, Slide 1 Your comments: This section was pretty good. Easy to understand.

More information

Physics 211: Lecture 14. Today s Agenda

Physics 211: Lecture 14. Today s Agenda Physics 211: Lecture 14 Today s Agenda Systems of Particles Center of mass Linear Momentum Example problems Momentum Conservation Inelastic collisions in one dimension Ballistic pendulum Physics 211: Lecture

More information

Classical Mechanics Lecture 13

Classical Mechanics Lecture 13 Classical Mechanics Lecture 13 Today s Concepts: a) More on Elas5c Collisions b) Average Force during Collisions Mechanics Lecture 13, Slide 1 Your comments: good I'd like to go over the energy of a system

More information

Last 6 lectures are easier

Last 6 lectures are easier Your Comments I love you. Seriously. I do. And you never post it. I felt really bad whilst completing the checkpoint for this. This stuff is way above my head and I struggled with the concept of precession.

More information

Hour Exam 1 Average 76.5% (no scaling) Mechanics Lecture 12, Slide 2

Hour Exam 1 Average 76.5% (no scaling) Mechanics Lecture 12, Slide 2 Your Comments This entire prelecture/checkpoint confused me, but especially the double mass but half speed checkpoint. Hey kid in Seat D23, your shoe is untied! Switching reference frames makes this way

More information

Announcements - 9 Oct 2014

Announcements - 9 Oct 2014 Announcements - 9 Oct 2014 1. Prayer 2. Exam 2 results a. Median Score: b. Curve: c. Exams will be returned soon, our office assistant should put them in the boxes near N357 ESC sometime today. d. I'll

More information

Today s topic: IMPULSE AND MOMENTUM CONSERVATION

Today s topic: IMPULSE AND MOMENTUM CONSERVATION Today s topic: IMPULSE ND MOMENTUM CONSERVTION Reiew of Last Week s Lecture Elastic Potential Energy: x: displacement from equilibrium x = 0: equilibrium position Work-Energy Theorem: W tot W g W el W

More information

Welcome back to Physics 211

Welcome back to Physics 211 Welcome back to Physics 211 The room is very full please move toward the center and help others find a seat. Be patient. The registration database is only updated twice per week. Get to know the people

More information

Physics 110 Homework Solutions Week #6 - Wednesday

Physics 110 Homework Solutions Week #6 - Wednesday Physics 110 Homework Solutions Week #6 - Wednesday Friday, May3, 2013 Chapter 6 Questions - none Multiple-Choice 66 C 67 D 68 B 69 C Problems 612 It s velocity as the ball hits the ground is found from

More information

Welcome to Kinematics!

Welcome to Kinematics! Welcome to Kinematics! Classical Mechanics Mechanics Lecture 1, Slide 1 Modus Operandi SmartPhysics Protocol Online Prelectures (animated textbook, before lecture) Online Checkpoints (check knowledge,

More information

Impulse and Momentum continued

Impulse and Momentum continued Chapter 7 Impulse and Momentum continued 7.2 The Principle of Conservation of Linear Momentum External forces Forces exerted on the objects by agents external to the system. Net force changes the velocity

More information

Your Comments. Mechanics Lecture 19, Slide 1

Your Comments. Mechanics Lecture 19, Slide 1 Your Comments i studied so hard for exam... and i did so bad :'( why physics u no love me. When we say a system will conserve angular momentum, does the solar system count? Say the sun suddenly expands

More information

Welcome back to PHY101: Major Concepts in Physics I. Photo: J. M. Schwarz

Welcome back to PHY101: Major Concepts in Physics I. Photo: J. M. Schwarz Welcome back to PHY101: Major Concepts in Phsics I Photo: J. M. Schwarz Announcements Course Website: jmschwarztheorgroup.org/ph101/ HW on Chapter is due at the beginning of lecture on Wednesda. HW 3 on

More information

Lecture 12! Center of mass! Uniform circular motion!

Lecture 12! Center of mass! Uniform circular motion! Lecture 1 Center of mass Uniform circular motion Today s Topics: Center of mass Uniform circular motion Centripetal acceleration and force Banked cures Define the center of mass The center of mass is a

More information

Classical Mechanics Lecture 4

Classical Mechanics Lecture 4 Classical Mechanics Lecture 4 Homework 3 and Midterm Exam 1 Today's Concepts: Newton s Laws a) Acceleration is caused by forces b) Force changes momentum c) Forces always come in pairs d) Good reference

More information

PHYS 100: Lecture 4 PROJECTILE MOTION. y = (v 0 /v T ) x (g/2v T2 )x 2. Velocity of Train v T. Physics 100 Lecture 4, Slide y(m)

PHYS 100: Lecture 4 PROJECTILE MOTION. y = (v 0 /v T ) x (g/2v T2 )x 2. Velocity of Train v T. Physics 100 Lecture 4, Slide y(m) PHYS : Lecture 4 PROJECTILE MOTION.4. Velocity of Train T y(m).8.6.4. 5 5 x(m) y ( / T ) x (/ T )x Physics Lecture 4, Slide Music Who is the Artist? A) Miles Dais B) Wynton Marsalis C) Chris Botti D) Nina

More information

Frames of Reference, Energy and Momentum, with

Frames of Reference, Energy and Momentum, with Frames of Reference, Energy and Momentum, with Interactie Physics Purpose: In this lab we will use the Interactie Physics program to simulate elastic collisions in one and two dimensions, and with a ballistic

More information

PHYSICS. Chapter 11 Lecture FOR SCIENTISTS AND ENGINEERS A STRATEGIC APPROACH 4/E RANDALL D. KNIGHT Pearson Education, Inc.

PHYSICS. Chapter 11 Lecture FOR SCIENTISTS AND ENGINEERS A STRATEGIC APPROACH 4/E RANDALL D. KNIGHT Pearson Education, Inc. PHYSICS FOR SCIENTISTS AND ENGINEERS A STRATEGIC APPROACH 4/E Chapter 11 Lecture RANDALL D. KNIGHT Chapter 11 Impulse and Momentum IN THIS CHAPTER, you will learn to use the concepts of impulse and momentum.

More information

Page 1. t F t m v. N s kg s. J F t SPH4U. From Newton Two New Concepts Impulse & Momentum. Agenda

Page 1. t F t m v. N s kg s. J F t SPH4U. From Newton Two New Concepts Impulse & Momentum. Agenda SPH4U Agenda Fro Newton Two New Concepts Ipulse & oentu Ipulse Collisions: you gotta consere oentu! elastic or inelastic (energy consering or not) Inelastic collisions in one diension and in two diensions

More information

October 24. Linear Momentum: - It is a vector which may require breaking it into components

October 24. Linear Momentum: - It is a vector which may require breaking it into components October 24 Linear Momentum: - It is a vector which may require breaking it into components Newton s First Law: A body continues with Constant Linear Momentum unless it is acted upon by a Net External Force.

More information

Momentum. Physics 1425 Lecture 15. Michael Fowler, UVa

Momentum. Physics 1425 Lecture 15. Michael Fowler, UVa Momentum Physics 1425 Lecture 15 Michael Fowler, UVa Physics Definition of Momentum Momentum is another word (like work, energy, etc.) from everyday life that has a precise meaning when used in physics.

More information

Welcome back to Physics 211

Welcome back to Physics 211 Welcome back to Physics 211 Today s agenda: Circular motion Impulse and momentum 08-2 1 Current assignments Reading: Chapter 9 in textbook Prelecture due next Thursday HW#8 due NEXT Friday (extension!)

More information

Momentum. Physics 211 Syracuse University, Physics 211 Spring 2017 Walter Freeman. February 28, W. Freeman Momentum February 28, / 15

Momentum. Physics 211 Syracuse University, Physics 211 Spring 2017 Walter Freeman. February 28, W. Freeman Momentum February 28, / 15 Momentum Physics 211 Syracuse University, Physics 211 Spring 2017 Walter Freeman February 28, 2017 W. Freeman Momentum February 28, 2017 1 / 15 Announcements Extra homework help hours today: 5:10-6:50

More information

Linear Momentum and Collisions Conservation of linear momentum

Linear Momentum and Collisions Conservation of linear momentum Unit 4 Linear omentum and Collisions 4.. Conseration of linear momentum 4. Collisions 4.3 Impulse 4.4 Coefficient of restitution (e) 4.. Conseration of linear momentum m m u u m = u = u m Before Collision

More information

Physics 131: Lecture 15. Today s Agenda

Physics 131: Lecture 15. Today s Agenda Physics 131: Lecture 15 Today s Agenda Impulse and Momentum (or the chapter where physicists run out of letters) Non-constant t forces Impulse-momentum thm Conservation of Linear momentum External/Internal

More information

Ch 7 Impulse-Momentum Theorem, Conservation of Momentum, and Collisions

Ch 7 Impulse-Momentum Theorem, Conservation of Momentum, and Collisions Ch 7 Impulse-Momentum Theorem, Conservation of Momentum, and Collisions Momentum and its relation to force Momentum describes an object s motion. Linear momentum is the product of an object s mass and

More information

Welcome back to Physics 211

Welcome back to Physics 211 Welcome back to Physics 211 Today s agenda: Rotations What s on the exam? Relative motion Physics 211 Fall 2012 Lecture 04-1 1 Assignments due this week: Prelecture 4-2: Ch 5.1-5.7 Complete short quiz

More information

Final EXAM. Physics 203. Prof. Daniel A. Martens Yaverbaum. John Jay College of Criminal Justice, the CUNY. Sections 1, 2. Wednesday, 5/21/14

Final EXAM. Physics 203. Prof. Daniel A. Martens Yaverbaum. John Jay College of Criminal Justice, the CUNY. Sections 1, 2. Wednesday, 5/21/14 Final EXAM Physics 203 Prof. Daniel A. Martens Yaverbaum John Jay College of Criminal Justice, the CUNY Sections 1, 2 Wednesday, 5/21/14 (Revised, Clarified, 5/28/14) Name: Section # : SCORE: DIRECTIONS

More information

Classical Mechanics Lecture 3

Classical Mechanics Lecture 3 Classical Mechanics Lecture 3 Today's Concepts: Newton s Laws a) Accelera=on is caused by forces b) Force changes momentum c) Forces always come in pairs d) Good reference frames Mechanics Lecture 3, Slide

More information

Purpose of the experiment

Purpose of the experiment Impulse and Momentum PES 116 Adanced Physics Lab I Purpose of the experiment Measure a cart s momentum change and compare to the impulse it receies. Compare aerage and peak forces in impulses. To put the

More information

Physics 231 Lecture 14

Physics 231 Lecture 14 Physics 231 Lecture 14 Impulses: forces that last a short time Momentum: p = mv Impulse-Momentum theorem: FΔt = Δp = mδv = m( v f v i ) Momentum conservation: p tot,f p 1,f + p 2,f = p 1,i + p 2,i p tot,i

More information

AP Physics Ch 6 Day 4

AP Physics Ch 6 Day 4 Textbook Reference: Goal/Objectives: Sections 6.3 (Collisions) - Understand how momentum and kinetic energy relate to the 3 types of collisions: elastic, inelastic, and perfectly inelastic - Use projectile

More information

Momentum Review. Lecture 13 Announcements. Multi-step problems: collision followed by something else. Center of Mass

Momentum Review. Lecture 13 Announcements. Multi-step problems: collision followed by something else. Center of Mass Lecture 13 Announcements 1. While you re waiting for class to start, please fill in the How to use the blueprint equation steps, in your own words.. Exam results: Momentum Review Equations p = mv Conservation

More information

New Course Webpage (To be setup by this weekend) h>p://people.physics.tamu.edu/tyana/phys218/

New Course Webpage (To be setup by this weekend) h>p://people.physics.tamu.edu/tyana/phys218/ Important Informa+on Instructor: Dr. Ty S(egler Office: ENPH 211 (Office Hours TBD) Email: tyana@physics.tamu.edu New Course Webpage (To be setup by this weekend) h>p://people.physics.tamu.edu/tyana/phys218/

More information

Chapter 7. Impulse and Momentum

Chapter 7. Impulse and Momentum Chapter 7 Impulse and Momentum Chaper 6 Review: Work and Energy Forces and Displacements Effect of forces acting over a displacement Work W = (F cos)s Work changes the Kinetic Energy of a mass Kinetic

More information

Your Comments. Nutcracker

Your Comments. Nutcracker Nutcracker Your Comments I don't understand the pressure differences in different sized pipes. To me, I would think that a pipe with a larger diameter has the smaller pressure and a skinnier pipe has a

More information

Announcements 2 Oct 2014

Announcements 2 Oct 2014 Announcements 2 Oct 2014 1. Prayer 2. Exam 1 starts today! a. Thursday Oct 2 Tuesday Oct 7 (2 pm) in the Testing Center, late fee after Oct 6, 2 pm b. Covers through today's lecture (unless we don't quite

More information

Physics 103, Practice Midterm Exam 2

Physics 103, Practice Midterm Exam 2 Physics 103, Practice Midterm Exam 2 1) A rock of mass m is whirled in a horizontal circle on a string of length L. The period of its motion is T seconds. If the length of the string is increased to 4L

More information

Problem Set 9: Momentum and Collision Theory. Nov 1 Hour One: Conservation Laws: Momentum and Collision Theory. Reading: YF

Problem Set 9: Momentum and Collision Theory. Nov 1 Hour One: Conservation Laws: Momentum and Collision Theory. Reading: YF MASSACHUSETTS INSTITUTE OF TECHNOLOGY Department of Physics Physics 8.0T Fall Term 2004 Problem Set 9: Momentum and Collision Theory Available on-line October 29; Due: November 9 at 4:00 p.m. Please write

More information

PHYS 1441 Section 002 Lecture #6

PHYS 1441 Section 002 Lecture #6 PHYS 1441 Section 00 Lecture #6 Monday, Feb. 4, 008 Examples for 1-Dim kinematic equations Free Fall Motion in Two Dimensions Maximum ranges and heights Today s homework is homework #3, due 9pm, Monday,

More information

Your Comments. That s the plan

Your Comments. That s the plan Your Comments I love physics as much as the next gal, but I was wondering. Why don't we get class off the day after an evening exam? What if the ladder has friction with the wall? Things were complicated

More information

Welcome back to Physics 211

Welcome back to Physics 211 Welcome back to Physics 211 Today s agenda: Impulse and momentum 09-2 1 Current assignments Reading: Chapter 10 in textbook Prelecture due next Tuesday HW#8 due this Friday at 5 pm. 09-2 2 9-2.1 A crash

More information

Physics 2210 Fall smartphysics 10 Center-of-Mass 11 Conservation of Momentum 10/21/2015

Physics 2210 Fall smartphysics 10 Center-of-Mass 11 Conservation of Momentum 10/21/2015 Physics 2210 Fall 2015 smartphysics 10 Center-of-Mass 11 Conservation of Momentum 10/21/2015 Collective Motion and Center-of-Mass Take a group of particles, each with mass m i, position r i and velocity

More information

Physics 2112 Unit 16

Physics 2112 Unit 16 Physics 2112 Unit 16 Concept: Motional EMF Unit 16, Slide 1 Your Comments Hopefully I will understand more after lecture. May be time to open the book. can we go over the conducting loop moving toward

More information

Welcome to Physics 212

Welcome to Physics 212 Welcome to Physics 212 http://online.physics.uiuc.edu/courses/phys212 This lecture is VERY full. Please sit next to someone nice. Find out the best thing that happened to them during the winter break!

More information

Stuff you asked about:

Stuff you asked about: Stuff you asked about: Instrumental illness Can you go over the change in momentum with respect to the change in time being used to calcuate the net force in depth more during the lecture. We never really

More information

A. unchanged increased B. unchanged unchanged C. increased increased D. increased unchanged

A. unchanged increased B. unchanged unchanged C. increased increased D. increased unchanged IB PHYSICS Name: DEVIL PHYSICS Period: Date: BADDEST CLASS ON CAMPUS CHAPTER B TEST REVIEW. A rocket is fired ertically. At its highest point, it explodes. Which one of the following describes what happens

More information

Unit 08 Work and Kinetic Energy. Stuff you asked about:

Unit 08 Work and Kinetic Energy. Stuff you asked about: Unit 08 Work and Kinetic Energy Today s Concepts: Work & Kinetic Energy Work in a non-constant direction Work by springs Mechanics Lecture 7, Slide 1 Stuff you asked about: Can we go over the falling,

More information

AP Physics C 2015 Summer Assignment

AP Physics C 2015 Summer Assignment AP Physics C 2015 Summer Assignment College Board (the people in charge of AP exams) recommends students to only take AP Physics C if they have already taken a 1 st year physics course and are currently

More information

So now that we ve mentioned these terms : kinetic, potential, work we should try to explain them more. Let s develop a model:

So now that we ve mentioned these terms : kinetic, potential, work we should try to explain them more. Let s develop a model: Lecture 12 Energy e are now at the point where we can talk about one of the most powerful tools in physics, energy. Energy is really an abstract concept. e hae indicators of energy (temperature, elocity

More information

Welcome to Physics 212

Welcome to Physics 212 Welcome to Physics 212 http://online.physics.uiuc.edu/courses/phys212 01 Physics 212 Lecture 1, Slide 1 Physics 212 Lecture 1 Today's Concepts: a) Coulomb s Law b) Superposition 03 Physics 212 Lecture

More information

Physic 602 Conservation of Momentum. (Read objectives on screen.)

Physic 602 Conservation of Momentum. (Read objectives on screen.) Physic 602 Conservation of Momentum (Read objectives on screen.) Good. You re back. We re just about ready to start this lab on conservation of momentum during collisions and explosions. In the lab, we

More information

EF 151 Exam #3 - Spring, 2016

EF 151 Exam #3 - Spring, 2016 Name: Section: Instructions: Sit in assigned seat; failure to sit in assigned seat results in a 0 for the eam. Put name and section on your eam. Put seating label on your equation sheet. Do not open the

More information

Physics 201: Lecture 14, Pg 1

Physics 201: Lecture 14, Pg 1 Physics 201: Lecture 14, Pg 1 Physics 131: Lecture 15 Today s Agenda Impulse and Momentum (or the chapter where physicists run out of letters) Non-constant forces Impulse-momentum thm Conservation of Linear

More information

Lecture 02: 2D Kinematics. Physics 2210 Fall Semester 2014

Lecture 02: 2D Kinematics. Physics 2210 Fall Semester 2014 Lecture 02: 2D Kinematics Physics 2210 Fall Semester 2014 Announcements Note that all Prelectures, Checkpoint Quizzes, and Homeworks are available one week before due date. You should have done Prelecture

More information

Lecture 11. Linear Momentum and Impulse. Collisions.

Lecture 11. Linear Momentum and Impulse. Collisions. Lecture 11 Linear Momentum and Impulse. Collisions. Momentum and Newton s Second Law F net = m a= m Δ v Δ t = Δ (m v ) Δ t = Δ p Δ t Linear momentum p = m v Newton s second law in terms of linear momentum:

More information

FTF Day 1. Feb 2, 2012 HW: Ch 3 Review Q s and Key Terms (Friday) Topic: Newton s 2 nd and 3 rd Laws Questions

FTF Day 1. Feb 2, 2012 HW: Ch 3 Review Q s and Key Terms (Friday) Topic: Newton s 2 nd and 3 rd Laws Questions Motion pt 2 Table of Contents 1. FTF s 2. Forces and Motion Phet Lab 3. Bill Nye: Gravity 4. Brainpop (Forces) 5. Lab: What Law Is It? 6. HW: Ch 3 7. Cartoon or Poem (2 nd Law) 8. Explorations Ch 2 & 3

More information

Stuff you asked about:

Stuff you asked about: Stuff you asked about: I'm so excited to walk to Loomis in -25 degree weather. I can't wait. I might not even fall asleep tonight out of anticipation. Oh centripetal acceleration, my old nemesis. Will

More information

Welcome back to Physics 211. Physics 211 Spring 2014 Lecture ask a physicist

Welcome back to Physics 211. Physics 211 Spring 2014 Lecture ask a physicist Welcome back to Physics 211 Today s agenda: Forces in Circular Motion Impulse Physics 211 Spring 2014 Lecture 07-1 1 ask a physicist My question is on sonoluminescence, which is supposed to be when a sound

More information

A ballistic pendulum

A ballistic pendulum A ballistic pendulum A ballistic pendulum is a device used to measure the speed of a bullet. A bullet of mass m is fired at a block of wood (mass M) hanging from a string. The bullet embeds itself in the

More information

Today: Scalars and vectors Coordinate systems, Components Vector Algebra

Today: Scalars and vectors Coordinate systems, Components Vector Algebra PHY131H1F - Class 6 Today: Scalars and vectors Coordinate systems, Components Vector Algebra Clicker Question The ball rolls up the ramp, then back down. Which is the correct acceleration graph? [Define

More information

LECTURE 26: Work- Kinetic Energy

LECTURE 26: Work- Kinetic Energy Lectures Page 1 LECTURE 26: Work- Kinetic Energy Select LEARNING OBJECTIVES: i. ii. iii. iv. v. vi. vii. viii. ix. Introduce and define linear kinetic energy. Strengthen the ability to perform proportional

More information

Topic 1: 2D Motion PHYSICS 231

Topic 1: 2D Motion PHYSICS 231 Topic 1: 2D Motion PHYSICS 231 Current Assignments Homework Set 1 due this Thursday, Jan 20, 11 pm Homework Set 2 due Thursday, Jan 27, 11pm Reading: Chapter 4,5 for next week 2/1/11 Physics 231 Spring

More information

Announcements 8 Oct 2013

Announcements 8 Oct 2013 Announcements 8 Oct 2013 1. Exam 2 still going on a. ends tomorrow 2 pm, late fee after 2 pm today Colton - Lecture 11 - pg 1 Where are we now? Topics Kinematics (velocity, acceleration) Vectors & 2D Motion

More information

Lecture 11. Impulse/Momentum. Conservation of Momentum. Cutnell+Johnson: Impulse and Momentum

Lecture 11. Impulse/Momentum. Conservation of Momentum. Cutnell+Johnson: Impulse and Momentum Lecture 11 Impulse/Momentum Conservation of Momentum Cutnell+Johnson: 7.1-7.3 Impulse and Momentum We learned about work, which is the force times distance (times the cosine of the angle in between the

More information

AP Physics 1 Momentum and Impulse Practice Test Name

AP Physics 1 Momentum and Impulse Practice Test Name AP Physics 1 Momentum and Impulse Practice Test Name MULTIPLE CHOICE. Choose the one alternative that best completes the statement or answers the question. 1) A rubber ball and a lump of clay have equal

More information

Center of Mass & Linear Momentum

Center of Mass & Linear Momentum PHYS 101 Previous Exam Problems CHAPTER 9 Center of Mass & Linear Momentum Center of mass Momentum of a particle Momentum of a system Impulse Conservation of momentum Elastic collisions Inelastic collisions

More information

Lecture 18: Work and Energy. Today s Agenda

Lecture 18: Work and Energy. Today s Agenda Lecture 18: Work and Energy Work and Energy Definition of work Examples Today s Agenda Definition of Mechanical Energy Conservation of Mechanical Energy Conservative forces Physics 201: Lecture 10, Pg

More information

Note on Posted Slides. Motion Is Relative

Note on Posted Slides. Motion Is Relative Note on Posted Slides These are the slides that I intended to show in class on Tue. Jan. 9, 2014. They contain important ideas and questions from your reading. Due to time constraints, I was probably not

More information

Phys101 Lectures 14, 15, 16 Momentum and Collisions

Phys101 Lectures 14, 15, 16 Momentum and Collisions Phys101 Lectures 14, 15, 16 Momentum and Collisions Key points: Momentum and impulse Condition for conservation of momentum and why How to solve collision problems Centre of mass Ref: 9-1,2,3,4,5,6,7,8,9.

More information

Physics 218 Lecture 14

Physics 218 Lecture 14 Physics 218 Lecture 14 Dr. David Toback Physics 218, Lecture XIV 1 Checklist for Today Things due awhile ago: Read Chapters 7, 8 & 9 Things that were due Yesterday: Problems from Chap 7 on WebCT Things

More information

Contents. Contents. Contents

Contents. Contents. Contents Physics 121 for Majors Schedule HW #5 is due Friday Quiz #2 is due 9/29 Lab #2 is due Monday Midterm 1 is 10/2 in the classroom. Class 6 and Collisions Relative Velocity Last Class Natural motion is straight-line

More information

PHY131H1F Class 3. From Knight Chapter 1:

PHY131H1F Class 3. From Knight Chapter 1: PHY131H1F Class 3 Today: Error Analysis Significant Figures Unit Conversion Normal Distribution Standard Deviation Reading Error Propagation of Errors Error in the Mean From Knight Chapter 1: 1 Significant

More information

Physics 111: Week 8 10 Review

Physics 111: Week 8 10 Review Physics 111: Week 8 10 Review Bin Chen NJIT Physics Department Announcements q Common Exam #3 on Nov 19 (Next Monday) from 4:15 pm to 5:45 pm in KUPF 107 q Must bring your NJIT ID q Cell phone and electronic

More information

Physics 1: Mechanics

Physics 1: Mechanics Physics 1: Mechanics Đào Ngọc Hạnh Tâm Office: A1.53, Email: dnhtam@hcmiu.edu.n HCMIU, Vietnam National Uniersity Acknowledgment: Most of these slides are supported by Prof. Phan Bao Ngoc credits (3 teaching

More information

Energy in Collisions Problems AP Physics C

Energy in Collisions Problems AP Physics C 1. A bullet of mass m and velocity v 0 is fired toward a block of mass 4m. The block is initially at rest on a v frictionless horizontal surface. The bullet penetrates the block and emerges with a velocity

More information

Welcome to Physics 211! General Physics I

Welcome to Physics 211! General Physics I Welcome to Physics 211! General Physics I Physics 211 Fall 2015 Lecture 01-1 1 Physics 215 Honors & Majors Are you interested in becoming a physics major? Do you have a strong background in physics and

More information

EXPERIMENT 8 BALLISTIC PENDULUM. Figure 1 Setup to determine the initial speed of the projectile using the Blackwood Pendulum

EXPERIMENT 8 BALLISTIC PENDULUM. Figure 1 Setup to determine the initial speed of the projectile using the Blackwood Pendulum EXPERIMENT 8 BALLISTIC PENDULUM I. Introduction. The objectie of this eperiment is to determine the initial elocity of a projectile fired from a gun by two methods. In the first the projectile undergoes

More information

Physics 141. Lecture 15. No lecture on Tuesday 10/28. I will be across the Atlantic.

Physics 141. Lecture 15. No lecture on Tuesday 10/28. I will be across the Atlantic. Physics 141. Lecture 15. No lecture on Tuesday 10/28. I will be across the Atlantic. Frank L. H. Wolfs Department of Physics and Astronomy, University of Rochester, Lecture 15, Page 1 Physics 141. Lecture

More information

Rutgers University Department of Physics & Astronomy. 01:750:271 Honors Physics I Fall Lecture 4. Home Page. Title Page. Page 1 of 35.

Rutgers University Department of Physics & Astronomy. 01:750:271 Honors Physics I Fall Lecture 4. Home Page. Title Page. Page 1 of 35. Rutgers Uniersit Department of Phsics & Astronom 01:750:271 Honors Phsics I Fall 2015 Lecture 4 Page 1 of 35 4. Motion in two and three dimensions Goals: To stud position, elocit, and acceleration ectors

More information

Last-night s Midterm Test. Last-night s Midterm Test. PHY131H1F - Class 10 Today, Chapter 6: Equilibrium Mass, Weight, Gravity

Last-night s Midterm Test. Last-night s Midterm Test. PHY131H1F - Class 10 Today, Chapter 6: Equilibrium Mass, Weight, Gravity PHY131H1F - Class 10 Today, Chapter 6: Equilibrium Mass, Weight, Gravity Clicker Question 1 Which of the following objects described below is in dynamic equilibrium? A. A 100 kg barbell is held at rest

More information

Announcements 9 Sep 2014

Announcements 9 Sep 2014 Announcements 9 Sep 2014 1. Prayer 2. Course homepage via: physics.byu.edu Class web pages Physics 105 (Colton J) Colton - Lecture 3 - pg 1 Which of the problems from last night's HW assignment would you

More information

Collisions. Of classical objects like collisions of motor vehicles. Of subatomic particles collisions allow study force law.

Collisions. Of classical objects like collisions of motor vehicles. Of subatomic particles collisions allow study force law. Collision Theory Collisions Any interaction between (usually two) objects which occurs for short time intervals Δt when forces of interaction dominate over external forces. Of classical objects like collisions

More information

Physics 231. Topic 6: Momentum and Collisions. Alex Brown October MSU Physics 231 Fall

Physics 231. Topic 6: Momentum and Collisions. Alex Brown October MSU Physics 231 Fall Physics 231 Topic 6: Momentum and Collisions Alex Brown October 7 2015 MSU Physics 231 Fall 2015 1 Momentum F = m a Newton s 2nd law F = m v/ t a= v/ t F = m (v final - v inital )/ t Define p = mv p: momentum

More information

LECTURE 15. Prof. Paul

LECTURE 15. Prof. Paul LECTURE 15 Prof. Paul Review Clicker Questions: Review Clicker Questions: (You can talk with others) Mark and David are loading identical cement blocks onto a truck. Mark lifts his block straight up from

More information

Physics 201, Review 3

Physics 201, Review 3 Physics 0, Reiew Important Notes: This reiew does not replace your own preparation efforts Exercises used in this reiew do not form a test problem pool. Please practice more with end of chapter problems.

More information

Mechanics. Time (s) Distance (m) Velocity (m/s) Acceleration (m/s 2 ) = + displacement/time.

Mechanics. Time (s) Distance (m) Velocity (m/s) Acceleration (m/s 2 ) = + displacement/time. Mechanics Symbols: Equations: Kinematics The Study of Motion s = distance or displacement v = final speed or velocity u = initial speed or velocity a = average acceleration s u+ v v v u v= also v= a =

More information

PHY131H1F - Class 9. Today, finishing Chapter 5: Kinetic Friction Static Friction Rolling without slipping (intro) Drag

PHY131H1F - Class 9. Today, finishing Chapter 5: Kinetic Friction Static Friction Rolling without slipping (intro) Drag PHY131H1F - Class 9 Today, finishing Chapter 5: Kinetic Friction Static Friction Rolling without slipping (intro) Drag Microscopic bumps and holes crash into each other, causing a frictional force. Kinetic

More information

On my honor, I have neither given nor received unauthorized aid on this examination.

On my honor, I have neither given nor received unauthorized aid on this examination. Instructor(s): Field/Furic PHYSICS DEPARTENT PHY 2053 Exam 1 October 5, 2011 Name (print, last first): Signature: On my honor, I hae neither gien nor receied unauthorized aid on this examination. YOUR

More information

Name ID Section. 1. One mile is equal to 1609 m; 1 hour is equal to 3600 s. The highway speed limit of 65 mph is equivalent to the speed of:

Name ID Section. 1. One mile is equal to 1609 m; 1 hour is equal to 3600 s. The highway speed limit of 65 mph is equivalent to the speed of: The exam is closed book and closed notes. There are 30 multiple choice questions. Make sure you put your name, section, and ID number on the SCANTRON form. The answers for the multiple choice Questions

More information

November 16, 2006 PHYS101 Test2 - Free Response Section Page 3

November 16, 2006 PHYS101 Test2 - Free Response Section Page 3 Last Name: First Name: Print your LAST and FIRST name on the front of your blue book, on this question sheet, the multiple-choice question sheet and the multiple-choice answer sheet. TIME ALLOWED 90 MINUTES

More information

phy 3.1.notebook September 19, 2017 Everything Moves

phy 3.1.notebook September 19, 2017 Everything Moves Eerything Moes 1 2 \ Diagrams: Motion 1) Motion (picture) no reference! time lapsed photo Type Motion? 3 origin Diagrams: reference pt. Motion reference! 1) Motion (picture) diagram time lapsed photo by

More information

Clickers Registration Roll Call

Clickers Registration Roll Call Clickers Registration Roll Call If you do not see your name then either: 1) You successfully registered your clicker during the roll call on tuesday OR 2) You added the course and your name was not yet

More information

Conservation of Energy Lab Packet

Conservation of Energy Lab Packet Conservation of Energy Lab Packet Unit # 3 Main Topic: Pendulum Duration: 10 days NAME: Contents/Page Number Day 2 (2/1/16): The Pendulum Lab Day 1 (2/2/16): The Physics of Pendulum Day 3 (2/3/16): The

More information

PHYS 1443 Section 004 Lecture #4 Thursday, Sept. 4, 2014

PHYS 1443 Section 004 Lecture #4 Thursday, Sept. 4, 2014 PHYS 1443 Section 004 Lecture #4 Thursday, Sept. 4, 014 One Dimensional Motion Motion under constant acceleration One dimensional Kinematic Equations How do we sole kinematic problems? Falling motions

More information

Chapter 7. Impulse and Momentum

Chapter 7. Impulse and Momentum Chapter 7 Ipulse and Moentu 7. The Ipulse-Moentu Theore There are any situations when the force on an object is not constant. 7. The Ipulse-Moentu Theore DEFINITION OF IMPULSE The ipulse of a force is

More information