Today's Concepts: a) Energy and Friction b) Potential energy & force

Slides:



Advertisements
Similar presentations
Chapter 6: Conservation of Energy
Advertisements

Work, Energy, And Power m Honors Physics Lecture Notes.
Chapter 9 Potential Energy & Conservation of Energy
Conservation of mechanical energy Lecture Conservation of Mechanical Energy Under the influence of conservative forces only (i.e. no friction or.
AP Physics I.C Work, Energy and Power.
SPH4U: Introduction to Work Work & Energy Work & Energy Discussion Discussion Definition Definition Dot Product Dot Product Work of a constant force Work.
Frank L. H. WolfsDepartment of Physics and Astronomy, University of Rochester Physics 121. Tuesday, February 26, 2008.
Physics 218, Lecture XIII1 Physics 218 Lecture 13 Dr. David Toback.
Physics 218 Lecture 14 Dr. David Toback Physics 218, Lecture XIV.
PHYSICS 231 INTRODUCTORY PHYSICS I
Physics 218, Lecture XII1 Physics 218 Lecture 12 Dr. David Toback.
Physics 218: Mechanics Instructor: Dr. Tatiana Erukhimova Lecture 13.
Classical Mechanics Lecture 8
1a. Positive and negative work
Example: The simple pendulum l Suppose we release a mass m from rest a distance h 1 above its lowest possible point. ç What is the maximum speed of the.
Classical Mechanics Lecture 9 Today's Examples: a) Conservative Forces b) Potential and Mechanical energy Today's Concepts : a) Energy and Friction b)
Classical Mechanics Lecture 9 Today's Concepts and Examples: a) Energy and Friction b) Potential energy & force Mechanics Lecture 9, Slide 1 Midterm 2.
Unit 6 Friction Today’s Concept: Friction UP.
Frank L. H. WolfsDepartment of Physics and Astronomy, University of Rochester Physics 121. Thursday, February 21, Conservation of energy! Changing.
Potential Energy and Conservative Forces
Energy m m Physics 2053 Lecture Notes Energy.
Review and then some…. Work & Energy Conservative, Non-conservative, and non-constant Forces.
Physics 2112 Unit 5: Electric Potential Energy
Physics 215 – Fall 2014Lecture Welcome back to Physics 215 Today’s agenda: Work Non-conservative forces Power.
Conservation of mechanical energy
Energy Transformations and Conservation of Mechanical Energy 8
Energy Transformations and Conservation of Mechanical Energy 8.01 W05D2.
Physics 215 – Fall 2014Lecture Welcome back to Physics 215 Today’s agenda: More gravitational potential energy Potential energy of a spring Work-kinetic.
Physics 111: Lecture 11, Pg 1 Physics 111: Lecture 11 Today’s Agenda l Review l Work done by variable force in 3-D ç Newton’s gravitational force l Conservative.
332 – UNIT 6 WORK & ENERGY.
Motion, Forces and Energy Lecture 7: Potential Energy & Conservation The name potential energy implies that the object in question has the capability of.
Chapter 8 Potential Energy and Conservation of Energy In this chapter we will introduce the following concepts: Potential energy Conservative and nonconservative.
Catching up from Yesterday
Your comments I feel like this could work brilliantly in a nice sized stadium seating lecture hall. Point to a student in the back/upper seats, say they.
Physics 211 Lecture 18 Today’s Concepts: a) Static Equilibrium
Stuff you asked about: I thought I understood the concepts in the pre-lecture until they went over the three examples. I felt that it moved too fast especially.
Your Comments Mechanics Lecture 9, Slide 1 Just a thought, in the prelectures, when whoever is narrating them says "this all makes sense", it makes me.
Your Comments The checkpoint problems about the spinning disk are slightly confusing to me still. What material does the third exam cover?? Both this unit.
Mechanics Lecture 1, Slide 1 Welcome to Physics 211! Classical Mechanics.
Physics 101: Lecture 9, Pg 1 Physics 101: Lecture 9 Work and Kinetic Energy l Today’s lecture will be on Textbook Sections  Hour Exam 1, Monday.
Your Comments I understand the concepts, but the math formulas being spat out like machine gun bullets are really confusing me. Is there a way we can see.
Today’s Concepts: Work & Kinetic Energy
Physics 211 Lecture 12 Today’s Concepts: a) Elastic Collisions
Problem with Work done by “other” forces Relationship between force and potential energy Potential energy diagrams Lecture 12: Potential energy diagrams.
Mechanics Lecture 11, Slide 1 Physics 211 Lecture 11 Today’s Concept: Inelastic Collisions.
 Work  Energy  Kinetic Energy  Potential Energy  Mechanical Energy  Conservation of Mechanical Energy.
Physics 101: Lecture 9, Pg 1 Physics 101: Lecture 9 Work and Kinetic Energy  Hour Exam 1, Tomorrow! – Exam 2.
Physics 101: Lecture 9, Pg 1 Physics 101: Lecture 9 Work and Kinetic Energy l Today’s lecture will be on Textbook Sections Exam II.
Physics 101: Lecture 9, Pg 1 Physics 101: Lecture 9 Work and Kinetic Energy l Today’s lecture will be on Textbook Sections
UB, Phy101: Chapter 6, Pg 1 Physics 101: Chapter 6 Work and Kinetic Energy l New stuff: Chapter 6, sections
Physics 101: Lecture 9, Pg 1 Physics 101: Lecture 9 Work and Kinetic Energy l Today’s lecture will be on Textbook Sections Exam II.
Today’s Concept: Simple Harmonic Motion: Mass on a Spring
Question C1.01 Description: Eliciting prior conceptions about "work" and introducing the physics definition. Source: A2L: UMPERG-ctqpe50.
More Fun Energy Examples 1. Santa Claus is at the top of a chimney 8.5 m from the floor below. He slips and falls all the way down (ouch!). With what speed.
Lecture 09: Work and Kinetic Energy
1a. Positive and negative work
Conservative and Nonconservative Forces
Work Done by a Constant Force
Physics 111: Lecture 9 Today’s Agenda
Work and Kinetic Energy
from rest down a plane inclined at an angle q with the horizontal.
Classical Mechanics Midterm 2 Review Force and Energy
Potential Energy and Conservation of Energy
Work and Kinetic Energy
Work and Kinetic Energy
AP 1 Energy practice.
Work Who does the most work? Definition of work in physics:
Potential Energy Problems
1 By what factor does the kinetic energy of a car change when its speed is tripled? 1) no change at all 2) factor of 3 3) factor of 6 4) factor of.
Potential Energy and Conservation of Energy
Presentation transcript:

Today's Concepts: a) Energy and Friction b) Potential energy & force Physics 211 Lecture 9 Today's Concepts: a) Energy and Friction b) Potential energy & force

Hour Exam One on THIS Thursday This is a 50 minute exam. Most of the practice exams online were 90 minute exams. Don’t wait until Wednesday. But bring questions to Wednesday’s review. Wednesday’s review will be working on homework questions that you raise.

Macroscopic Work done by Friction

Macroscopic Work: do not understand the concept of macroscopic work. Kindaa confused. Help me please??/ This is not a new idea – it’s the same “work” you are used to. Applied to big (i.e. macroscopic) objects rather than point particles (picky detail) We call it “macroscopic” to distinguish it from “microscopic”. You will deal with this in Physics 213 Macroscopic work changes only macroscopic (mechanical) energy, not heat.

f f

“Heat” is just the kinetic energy of the atoms! Demo: cork popper

Checkpoint/ACT A block of mass m, initially held at rest on a frictionless ramp a vertical distance H above the floor, slides down the ramp and onto a floor where friction causes it to stop a distance D from the bottom of the ramp. The coefficient of kinetic friction between the box and the floor is mk. What is the total macroscopic work done on the block by all forces during this process? A) mgH B) –mgH C) mk mgD D) 0 m H D

CheckPoint What is the total macroscopic work done on the block by all forces during this process? A) mgH B) –mgH C) mk mgD D) 0 A) the only work there is the potential energy initially B) work= change in potential energy C) The only work being done on the object is by the friction force. D) total work is equal to the change in kinetic energy. since the box starts and ends at rest, the change in kinetic energy is zero. m H D

CheckPoint/ACT A block of mass m, initially held at rest on a frictionless ramp a vertical distance H above the floor, slides down the ramp and onto a floor where friction causes it to stop a distance D from the bottom of the ramp. The coefficient of kinetic friction between the box and the floor is mk. What is the macroscopic work done on the block by friction during this process? A) mgH B) –mgH C) mk mgD D) 0 m H D

CheckPoint/ACT What is the macroscopic work done on the block by friction during this process? A) mgH B) –mgH C) mk mgD D) 0 B) All of the potential energy goes to kinetic as it slides down the ramp, then the friction does negative work to slow the box to stop C) Since the floor has friction, the work done by the block by friction is the normal force times the coefficient of kinetic friction times the distance. Work done by friction is negative. m H D

Ouch! They’re perpendicular. I don’t understand this. no Any better understanding by now? What forces?

must be negative N1 mg m N2 mg m mg H

Potential Energy vs. Force

Potential Energy vs. Force Demo: car on track

ACT Suppose the potential energy of some object U as a function of x looks like the plot shown below. Where is the force on the object zero? A) (a) B) (b) C) (c) D) (d) U(x) x (a) (b) (c) (d)

ACT Suppose the potential energy of some object U as a function of x looks like the plot shown below. Where is the force on the object in the +x direction? A) To the left of (b) B) To the right of (b) C) Nowhere U(x) x (a) (b) (c) (d)

CheckPoint – BAD WORDING Suppose the potential energy of some object U as a function of x looks like the plot shown below. Where is the force on the object biggest in the –x direction? A) (a) B) (b) C) (c) D) (d) U(x) x (a) (b) (c) (d)

ACT – BETTER WORDING Suppose the potential energy of some object U as a function of x looks like the plot shown below. Where is the force on the object in the –x direction & of the largest magnitude? A) (a) B) (b) C) (c) D) (d) U(x) x (a) (b) (c) (d)

ACT – BETTER WORDING Suppose the potential energy of some object U as a function of x looks like the plot shown below. Where is the force on the object in the –x direction & of the largest magnitude? A) (a) B) (b) C) (c) D) (d) U(x) x (a) (b) (c) (d)

Your Comments Careful! A negative slope means a positive force! good At A) slope is neg so force is positive. At A) slope is neg so force is positive. Careful: F = - dU/dx At C) slope is pos so force is negative.

More Comments from this Morning

L v Conserve Energy from initial to final position

mg T L

mg T

h h Conserve Energy from initial to final position

h mg T r