TUTORIAL 4: CONSERVATION OF ENERGY. Instructors: Kazumi Tolich and Sheh Lit Chang

Similar documents
Announcements. If you think there was an error in the scoring, fill out a regrade form and had back to ME (not TAs)

LECTURE 12 FRICTION, STRINGS & SPRINGS. Instructor: Kazumi Tolich

14.4 Change in Potential Energy and Zero Point for Potential Energy

a. Determine the potential energy of the spring as a function of displacement.

A Question about free-body diagrams

Work and Potential Energy

Work, energy, power, and conservation of energy

W = F x W = Fx cosθ W = Fx. Work

Physics 2211 M Quiz #2 Solutions Summer 2017

1 of 6 10/21/2009 6:33 PM


LECTURE 12 FRICTION & SPRINGS. Instructor: Kazumi Tolich

LECTURE 9 FRICTION & SPRINGS. Instructor: Kazumi Tolich

Which, if any, of the velocity versus time graphs below represent the movement of the sliding box?

End-of-Chapter Exercises

Find the acceleration of the train B Find the distance traveled during this 20 s? C D

Physics 111. Thursday, Dec. 9, 3-5pm and 7-9pm. Announcements. Thursday, December 9, 2004

When you throw a ball, increasing the speed of your hand increases the speed of the ball. Does the same apply to a wave pulse?

LECTURE 22 EQUILIBRIUM. Instructor: Kazumi Tolich

PHYS 154 Practice Test 3 Spring 2018

Physics Mechanics. Lecture 11 Newton s Laws - part 2

General Physics I Spring Applying Newton s Laws

Physics 2210 Fall Review for Midterm Exam 2 10/07/2015

1- A force F = ( 6ˆ i 2ˆ j )N acts on a particle that undergoes a displacement

Chapter 11 Vibrations and Waves

8.01x Classical Mechanics, Fall 2016 Massachusetts Institute of Technology. Problem Set 2

Mechanics and Heat. Chapter 5: Work and Energy. Dr. Rashid Hamdan

Phys101 Second Major-131 Zero Version Coordinator: Dr. A. A. Naqvi Sunday, November 03, 2013 Page: 1

Ch 10 HW: Problem Spring Force

Lecture 6 Force and Motion. Identifying Forces Free-body Diagram Newton s Second Law

Isaac Newton ( ) 1687 Published Principia Invented Calculus 3 Laws of Motion Universal Law of Gravity

PHYS 101 Previous Exam Problems. Force & Motion I

Physics 2211 ABC Quiz #3 Solutions Spring 2017

i. Indicate on the figure the point P at which the maximum speed of the car is attained. ii. Calculate the value vmax of this maximum speed.

F on stone by rope F on box by rope. F on stone by Earth

( ) = ( ) W net = ΔKE = KE f KE i W F. F d x. KE = 1 2 mv2. Note: Work is the dot product of F and d. Work-Kinetic Energy Theorem

Chapter 8. Conservation of Energy

Simple Harmonic Oscillator Challenge Problems

TUTORIAL 1 SIMPLE HARMONIC MOTION. Instructor: Kazumi Tolich

4 A mass-spring oscillating system undergoes SHM with a period T. What is the period of the system if the amplitude is doubled?

Newton s 3 Laws of Motion

Chapter 5 Force and Motion

(A) 10 m (B) 20 m (C) 25 m (D) 30 m (E) 40 m

Physics 221. Exam III Spring f S While the cylinder is rolling up, the frictional force is and the cylinder is rotating

CONTENTS (BOOK PAGES )

(A) 10 m (B) 20 m (C) 25 m (D) 30 m (E) 40 m

PSI AP Physics B Dynamics

PHY 101. Work and Kinetic Energy 7.1 Work Done by a Constant Force

EXAM 3 MECHANICS 40% of the final grade

Friction Can Be Rough

AP Physics 1 Review. On the axes below draw the horizontal force acting on this object as a function of time.

Section /07/2013. PHY131H1F University of Toronto Class 9 Preclass Video by Jason Harlow. Based on Knight 3 rd edition Ch. 5, pgs.

General Physics I Forces

Chapter 8. Potential Energy and Energy Conservation

Name Student ID Phys121 Win2011

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

HATZIC SECONDARY SCHOOL

Math Review Night: Work and the Dot Product

Finishing Chapter 26 on dipoles.. Electric Potential Energy of: Point Charges Dipoles Electric Potential: V Voltage: ΔV

Pulling force $ % 6 Least

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:

PHYSICS. Chapter 10 Lecture FOR SCIENTISTS AND ENGINEERS A STRATEGIC APPROACH 4/E RANDALL D. KNIGHT Pearson Education, Inc.

Solving two-body problems with Newton s Second Law. Example Static and Kinetic Friction. Section 5.1 Friction 10/15/13

Chapter 13. Simple Harmonic Motion

Physics B Newton s Laws AP Review Packet

Energy present in a variety of forms. Energy can be transformed form one form to another Energy is conserved (isolated system) ENERGY

Virbations and Waves

Potential Energy & Conservation of Energy

Chapter 14 Oscillations. Copyright 2009 Pearson Education, Inc.

PHY131H1S Class 17. Pre-class Reading Quiz 1. The transfer of energy to a system by the application of a force is called

Q4.2.a Approximately what is the radius of a copper atom? 1) 1 e -15 m 2) 1 e -12 m 3) 1 e -10 m 4) 1 e-8 m 5) 1 e-6 m

Chapter 14 Oscillations

LECTURE 3 ENERGY AND PENDULUM MOTION. Instructor: Kazumi Tolich

Name Period Date. 75 kg. Horizontal, frictionless surface. Label a coordinate system, write the formula, substitute and solve.

Phys101 Second Major-162 Zero Version Coordinator: Dr. Kunwar S. Saturday, March 25, 2017 Page: 1

Forces & Newton s Laws FR Practice Problems

A. B. C. D. E. v x. ΣF x

Chapter 15 Periodic Motion

The dot product and work

Potential energy and conservation of energy

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

Old Exam. Question Chapter 7 072

Figure 1: Doing work on a block by pushing it across the floor.

AP Physics C - Mechanics

You may use g = 10 m/s 2, sin 60 = 0.87, and cos 60 = 0.50.

General Physics I Work & Energy

Chapter 5 Newton s Laws of Motion. Copyright 2010 Pearson Education, Inc.

Chapter 3, Section 3

Fundamentals Physics

Chapter 3 The Laws of motion. The Laws of motion

PHYSICS - CLUTCH CH 07: WORK & ENERGY.

General Physics Physics 101 Test #2 Spring 2017 Wednesday 3/1/17 Prof. Bob Ekey

Chapter 8. Potential Energy & Conservation of Energy

Physics 2111 Unit 7. Today s Concepts: Work & Kinetic Energy Power. Mechanics Lecture 7, Slide 1

Name Student ID Score Last First. I = 2mR 2 /5 around the sphere s center of mass?

Chapter 7 Energy of a System

PHYSICS. Chapter 5 Lecture FOR SCIENTISTS AND ENGINEERS A STRATEGIC APPROACH 4/E RANDALL D. KNIGHT Pearson Education, Inc.

Lesson 14: Friction. a) Fill in the table that follows by constructing a force diagram for the block (the system) for these five situations.

RELEASED FORM RELEASED. North Carolina Test of Physics

Exercises on Newton s Laws of Motion

Transcription:

TUTORIL 4: CONSERVTION OF ENERGY Instructors: Kazumi Tolich and Sheh Lit Chang

2 Relating work and changes in energy: experiments 1 and 2 Two experiments are conducted with identical blocks on a level, frictionless surface. Each block is pushed through the same distance by the same force. In experiment 1 both blocks end at rest and in 2 both blocks have a final speef v f2. System 1: Two blocks and spring in experiment 1. System 2: Two blocks in experiment 2.

3 Relating work and changes in energy: Checkpoint 1 1. Determine whether the quantities in the table are positive, negative, or zero for each system. System 1 System 2 W net ext ΔK ΔU ΔE tot 2. With which of the following students, if any, do you agree? Student 1 The net work done on a system is always equal to the change in kinetic energy of that system. Student 2 The total energy of a system can change if something is doing work on that system. The net work done on a system by external forces is equal to the change in total energy of the system. Student 3 In the absence of friction, the total energy of a system must remain constant. In other words, K i + U i = K f + U f or ΔK + ΔU = 0

Relating work and changes in energy: experiments 1, 2, and 3 4 Experiment 3 is similar to experiment 1, but the spring in experiment 3 is weaker than in experiment 1 (k 3 < k 1 ). t the enf experiment 3, each block has a speef v f3. System 3 consists of the two blocks and the spring in experiment 3. ll three experiments are shown together below. Experiment 1 Experiment 2 Experiment 3 t = t 1 Each hand pushes with a constant force of magnitude F o t = t 3 Each hand pushes with a constant force of magnitude F o t = t 5 Each hand pushes with a constant force of magnitude F o k 1 k 3 t = t 2 t = t 4 t = t 6 v f 1 = 0 v f 2 > 0 v f 3 > 0

5 Relating work and changes in energy: Checkpoint 2 Consider systems 1 3. 3. Rank these systems according to the net work done on each system by external forces, from smallest to largest. If the net work done on any system is zero, state so explicitly. 4. Rank these systems according to the change in total energy of the system, from smallest to largest. If the change in total energy of any system is zero, state so explicitly.

6 Relating work and changes in energy: Checkpoint 3 5. Rank these systems according to the change in kinetic energy of the system, from smallest to largest. If the change in kinetic energy of any system is zero, state so explicitly. 6. Rank these systems according to the change in potential energy of the system, from smallest to largest. If the change in potential energy of any system is zero, state so explicitly.

Work and energy in systems 7 block of mass m on a level, frictionless surface is attached to an ideal massless spring of constant k, as shown at right. t time t i, the block is released from rest, and at time t f the spring is at its equilibrium position. We will account for the change in kinetic energy of the block, ΔK block by considering 2 different systems: System, which consists of the block alone System S, which consists of the spring and the block

8 Work and energy in systems: Discussion questions 7. Sketch a free-body diagram for system and system S during the interval from t i to t f (after the hand releases the block). 8. For each force on your diagrams, determine whether it does positive, negative, or zero work. 9. For each system, determine whether the net external work is positive, negative, or zero.

Work and energy in systems: Checkpoint 4 9 10. Two students are considering the work done on the two systems: Student 1: I think that the spring does positive work on the block, and the wall does positive work on the spring-block system. Student 2: ut the point where the wall exerts a force on the spring-block system doesn t move, so how can the wall do work? The displacement is zero. With which student, if either, do you agree?

Work and energy in systems: Checkpoint 5 10 11. For each system, determine whether ΔU over the interval from t i to t f is positive, negative, or zero. 12. Two students are considering an energy analysis of system (the block alone): Student 1: The spring does work on system, so system s spring potential energy changes. Student 2: I agree that the spring does work on system, but there aren t any springs in system, so how could it have spring potential energy? It s just a block. With which student, if either, do you agree?

11 Work and energy in systems: Discussion questions 13. For which system, if either, is the total energy unchangever the interval from t i to t f? Explain how you can use the principle of conservation of energy to account for the change in kinetic energy of the block in this system. 14. For the system for which the total energy changes, explain how you can account for the change in kinetic energy of the block in that system.