Lecture 09: Work and Potential Energy II. Physics 2210 Fall Semester 2014

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1 Lecture 09: Work and Potential Energy II Physics 2210 Fall Semester 2014

2 Today's Concepts: a) Energy and Friction b) Potential Energy and Force Mechanics Lecture 8, Slide 2

3 Unit 9: Prelecture Feedback Block sliding down the ramp checkpoint. Macroscopic work Connection between force and potential energy. Please keep going through problems like the homework Mechanics Lecture 8, Slide 3

4 Energy and Friction Last time: Mechanical Energy (K+U) is a constant of the motion for conservative forces. Today: Change in mechanical energy is equal to work done by nonconservative forces.

5 Last Time: Generalize mechanical energy conservation to conservative systems including springs: Spring P.E. K.E. Gravitational P.E.

6 Energy and Friction Last time: Mechanical Energy (K+U) is a constant of the motion for conservative forces. Today: Change in mechanical energy is equal to work done by nonconservative forces.

7 Macroscopic Work done by Friction Mechanics Lecture 9, Slide 7

8 Macroscopic Work: This is not a new idea it s the same work you are used to. W b = F dl a Applied to big (i.e. macroscopic) objects rather than point particles (picky detail) We call it macroscopic to distinguish it from microscopic. Mechanics Lecture 9, Slide 8

9 Mechanics Lecture 9, Slide 9

10 Mechanics Lecture 9, Slide

11 f f Mechanics Lecture 9, Slide

12 Heat is just the kinetic energy of the atoms! Mechanics Lecture 9, Slide 12

13 Heat is just the kinetic energy of the atoms! This is how the conservative fundamental forces (gravity, electromagnetism...) give rise to nonconservative macroscopic forces Mechanics Lecture 9, Slide 13

14 Example: A block of mass 12 kg has an initial velocity of 1.0 m/s to the right as it slides across the floor with a coefficient of kinetic friction k = How far does it travel before coming to rest? Solve via: a) 2 nd law and kinematics equations b) Work-energy theorem

15 Conservative and Nonconservative Forces N 1 m must be negative N 2 H mg µ mg mg Mechanics Lecture 9, Slide 15

16 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 r from the bottom of the ramp. The coefficient of kinetic friction between the box and the floor is µ k. What is the macroscopic work done on the block by friction during this process? m CheckPoint A) mgh B) mgh C) µ k mgd D) 0 H D Mechanics Lecture 9, Slide 16

17 What is the macroscopic work done on the block by friction during this process? A) mgh B) mgh C) µ k 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. m CheckPoint H D Mechanics Lecture 9, Slide 17

18 CheckPoint 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 µ k. What is the total macroscopic work done on the block by all forces during this process? m A) mgh B) mgh C) µ k mgd D) 0 H K = W tot D Mechanics Lecture 9, Slide 18

A) mgh B) mgh C) µ k mgd D) 0 D) total work is equal to the change in

19 CheckPoint What is the total macroscopic work done on the block by all forces during this process? A) mgh B) mgh C) µ k mgd D) 0 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 K = W tot D Mechanics Lecture 9, Slide 19

20 Potential Energy vs. Force F( x) = du ( x) dx Mechanics Lecture 9, Slide 20

21 CheckPoint 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) Mechanics Lecture 9, Slide 21

22 CheckPoint 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) F( x) = du ( x) dx Mechanics Lecture 9, Slide 22

23 Flashcard Question 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) F( x) = du ( x) dx Mechanics Lecture 9, Slide 23

24 Flashcard Question 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) F( x) = du ( x) dx Mechanics Lecture 9, Slide 24

25 HW Example What is work done by tension before the incline? What is the speed of the block before the incline? What is the work done by friction after traveling up the incline? What is the work done by gravity after traveling up the incline? How far does the block travel before coming to rest?

26 Homework Example How far will you get with some initial speed? If you have the minimum speed 11,068 m/s required, what is your speed when you reach the moon? Which effects minimum speed? m earth, r earth, m ship?

27 HW Example: Potential Energy in Earth-Moon System

28 HW Example: Potential Energy in Earth-Moon System

Lecture 07: Work and Kinetic Energy. Physics 2210 Fall Semester 2014

Lecture 07: Work and Kinetic Energy Physics 2210 Fall Semester 2014 Announcements Schedule next few weeks: 9/08 Unit 3 9/10 Unit 4 9/15 Unit 5 (guest lecturer) 9/17 Unit 6 (guest lecturer) 9/22 Unit 7,