Lecture 10. Potential energy and conservation of energy

Similar documents
Question 8.1 Sign of the Energy II

ConcepTest PowerPoints

Lecture 10 Mechanical Energy Conservation; Power

Review. Kinetic Energy Work Hooke s s Law Potential Energy Conservation of Energy Power 1/91

Conservation of Energy

5.3. Conservation of Energy

Welcome back to Physics 211

Recall: Gravitational Potential Energy

Name Lesson 7. Homework Work and Energy Problem Solving Outcomes

= 1 2 kx2 dw =! F! d! r = Fdr cosθ. T.E. initial. = T.E. Final. = P.E. final. + K.E. initial. + P.E. initial. K.E. initial =

CHAPTER 6 WORK AND ENERGY

Chapter 6 Energy and Oscillations

Work and energy. 15 m. c. Find the work done by the normal force exerted by the incline on the crate.

Potential Energy & Conservation of Energy

Chapter 6 Work and Energy

Physics 1A, Summer 2011, Summer Session 1 Quiz 3, Version A 1

The content contained in all sections of chapter 6 of the textbook is included on the AP Physics B exam.

Phys101 Lectures 9 and 10 Conservation of Mechanical Energy

Power: Sources of Energy

MECHANICAL (TOTAL) ENERGY

P = dw dt. P = F net. = W Δt. Conservative Force: P ave. Net work done by a conservative force on an object moving around every closed path is zero

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

CPS lesson Work and Energy ANSWER KEY

Chapters 10 & 11: Energy

Name 09-MAR-04. Work Power and Energy

1 1. A spring has a spring constant of 120 newtons/meter. How much potential energy is stored in the spring as it is stretched 0.20 meter?

1) To Work or Not to Work

2 possibilities. 2.) Work is done and... 1.) Work is done and... *** The function of work is to change energy ***

WEP-Energy. 2. If the speed of a car is doubled, the kinetic energy of the car is 1. quadrupled 2. quartered 3. doubled 4. halved

Lesson 5. Luis Anchordoqui. Physics 168. Tuesday, September 26, 17

Conservative vs. Non-conservative forces Gravitational Potential Energy. Conservation of Mechanical energy

Momentum, Impulse, Work, Energy, Power, and Conservation Laws

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

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

Chapter 6: Work and Kinetic Energy

Phys101 Lectures 9 and 10 Conservation of Mechanical Energy

Potential energy functions used in Chapter 7

Unit 4 Work, Power & Conservation of Energy Workbook

D) No, because of the way work is defined D) remains constant at zero. D) 0 J D) zero

Chapters 10 & 11: Energy

Physics 201, Review 2

s_3x03 Page 1 Physics Samples

Lecture 18: Work and Energy. Today s Agenda

Physics 231. Topic 5: Energy and Work. Alex Brown October 2, MSU Physics 231 Fall

Healy/DiMurro. Vibrations 2016

DEVIL PHYSICS THE BADDEST CLASS ON CAMPUS IB PHYSICS

Work changes Energy. Do Work Son!

Work Energy Review. 1. Base your answer to the following question on the information and diagram below and on your knowledge of physics.

Physics 201, Review 2

PSI AP Physics I Work and Energy

WEP-Energy. 2. If the speed of a car is doubled, the kinetic energy of the car is 1. quadrupled 2. quartered 3. doubled 4. halved

Chapter 5: Energy. Energy is one of the most important concepts in the world of science. Common forms of Energy

Chapter 8. Potential Energy & Conservation of Energy

Homework #5. Ph 231 Introductory Physics, Sp-03 Page 1 of 4

Chapter 8: Potential Energy and Conservation of Energy Work and kinetic energy are energies of motion.

5. A car moves with a constant speed in a clockwise direction around a circular path of radius r, as represented in the diagram above.

Lectures Chapter 6 (Cutnell & Johnson, Physics 7 th edition)

Physics 201, Midterm Exam 2, Fall Answer Key

Physics 2414 Group Exercise 8. Conservation of Energy

W = F x W = Fx cosθ W = Fx. Work

Potential Energy and Conservation of Energy Chap. 7 & 8

What is Energy? Which has more energy? Who has more energy? 1/24/2017

- Conservation of Energy Notes Teacher Key -

Physics Unit 4:Work & Energy Name:

Work Done by a Constant Force

Potential Energy. Serway 7.6, 7.7;

Old Exam. Question Chapter 7 072

ENERGY. Conservative Forces Non-Conservative Forces Conservation of Mechanical Energy Power

Chapter 7 Potential Energy and Energy Conservation

Physics 1A Lecture 6B. "If the only tool you have is a hammer, every problem looks like a nail. --Abraham Maslow

University of Colorado, Boulder, 2004 CT8-3

Exam #2, Chapters 5-7 PHYS 101-4M MULTIPLE CHOICE. Choose the one alternative that best completes the statement or answers the question.

General Physics I Work & Energy

Page 1. Name:

Extra credit assignment #4 It can be handed in up until one class before Test 4 (check your course outline). It will NOT be accepted after that.

Physics 201 Lecture 16

4.) A baseball that weighs 1.6 N leaves a bat with a speed of 40.0 m/s. Calculate the kinetic energy of the ball. 130 J

Another Method to get a Sine Wave. X = A cos θ V = Acc =

Energy Problem Solving Techniques.

Chapter 7: Energy. Consider dropping a ball. Why does the ball s speed increase as it falls?

Work and the Work-Energy Theorem

= y(x, t) =A cos (!t + kx)

Old Exams Questions Ch. 8 T072 Q2.: Q5. Q7.

Potential Energy & Energy Conservation

Lectures 11-13: From Work to Energy Energy Conservation

Homework 6. problems: 8.-, 8.38, 8.63

Review for Exam 2 S 2019

Harmonic Motion: Exercises

Potential Energy, Conservation of Energy, and Energy Diagrams. Announcements. Review: Conservative Forces. (path independent) 8.

Honor Physics Final Exam Review. What is the difference between series, parallel, and combination circuits?

Concept of Force Concept Questions

P8.14. m 1 > m 2. m 1 gh = 1 ( 2 m 1 + m 2 )v 2 + m 2 gh. 2( m 1. v = m 1 + m 2. 2 m 2v 2 Δh determined from. m 2 g Δh = 1 2 m 2v 2.

Ch 11 ENERGY and its CONSERVATION. work causes a change in the energy of a system KE (an increase or decrease in KE) ket.

Potential energy and conservation of energy

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

PHYSICS 231 INTRODUCTORY PHYSICS I

Lecture 18. Newton s Laws

Welcome to: Physics I. I m Dr Alex Pettitt, and I ll be your guide!

0J2 - Mechanics Lecture Notes 2

Gravitational Potential

Transcription:

Lecture 10 Potential energy and conservation of energy

Today s Topics: Potential Energy and work done by conservative forces Work done by nonconservative forces Conservation of mechanical energy Potential energy curves and equipotentials

Potential Energy Potential Energy has the potential to do work! A change in Potential Energy arises from the work done by a conservative force. The work done by gravity when a ball is lifted to height Δh does work on the ball when it is released. If the work done by gravity in lifting the ball a height Δh is (-mgδh), ΔPE -W conservative mgδh

Example Δh θ m A box of mass m is pushed to the top of a rough board of length L, that is inclined by θ to the horizontal. What is the change in potential energy of the box? F F N mg Same change in potential as raising the box by Δh f Identify the forces acting on the box Identify the conservative forces that do work F N and mgcosθ are perpendicular to the displacement, so they do no work. F and f are not conservative forces, so they can not change the potential energy W mg - mgsinθ L - mgδh ΔPE - W mg mgδh

ACT: Up the Hill Two paths lead to the top of a big hill. One is steep and direct, while the other is twice as long but less steep. How much more potential energy would you gain if you take the longer path? a) the same b) twice as much c) four times as much d) half as much e) you gain no PE in either case Because your vertical position (height) changes by the same amount in each case, the gain in potential energy is the same.

ACT: Sign of the Energy Is it possible for the gravitational potential energy of an object to a) yes b) no be negative? Gravitational PE is mgh, where height h is measured relative to some arbitrary reference level where PE 0. For example, a book on a table has positive PE if the zero reference level is chosen to be the floor. However, if the ceiling is the zero level, then the book has negative PE on the table. Only differences (or changes) in PE have any physical meaning.

Back to the Work-Energy Theorem In normal situations both conservative and nonconservative forces act simultaneously on an object, so the work done by the net external force can be written as W W c + W nc W KE f - KE o DKE W c -DPE DKE -DPE +W nc THE WORK-ENERGY THEOREM W nc DKE + DPE

Conservation of Mechanical Energy W nc ( KE - KE ) + ( PE PE ) DKE + DPE - f o f o W nc ( KE + PE )- ( KE + PE ) f f o o W nc Ef - E o If the net work on an object by non-conservative forces is zero, then its energy does not change:

The Pendulum A simple pendulum consists of a mass m (of negligible size) suspended by a string or rod of length L (and negligible mass). The angle it makes with the vertical varies with time as a sine or cosine. DEMO: Bowling ball pendulum If we displace a pendulum by an angle, q, away from equilibrium, it rises by an amount: Dh L - Lcosq L(1 -cosq ) aboveits initial position. DPE mgdh mgl(1 -cosq )

ACT: Down the Hill Three blocks of equal mass start from rest and slide down different frictionless ramps. All ramps have the same height. Which block has the greatest speed at the bottom of its ramp? d) same speed for all blocks a b c All of the blocks have the same initial gravitational PE, because they are all at the same height (PE mgh). Thus, when they get to the bottom, they all have the same final KE, and hence the same speed (KE mv ). 1

ACT: Water Slide I Paul and Kathleen start from rest at the same time on frictionless water slides with different shapes. At the bottom, whose velocity is greater? a) Paul b) Kathleen c) both the same Conservation of Energy: E i mgh E f mv 1 1 therefore: gh v Because they both start from the same height, they have the same velocity at the bottom.

ACT: Water Slide II Paul and Kathleen start from rest at the same time on frictionless water slides with different shapes (but equal lengths). Who makes it to the bottom first? a) Paul b) Kathleen c) both the same Even though they both have the same final velocity, Kathleen is at a lower height than Paul for most of her ride. Thus, she always has a larger velocity during her ride and therefore arrives earlier!

ACT: Runaway Truck A truck, initially at rest, rolls down a frictionless hill and attains a speed of 0 m/s at the bottom. To achieve a speed of 40 m/s at the bottom, how many times higher must the hill be? a) half the height b) the same height c) times the height d) twice the height e) four times the height Use energy conservation: Ø initial energy: E i PE g mgh Ø final energy: E f KE mv Conservation of Energy: E i mgh E f mv 1 therefore: gh v So if v doubles, H quadruples! 1 1

Let s continue our Example Δh m θ Now our box is at rest at the top of the inclined plane and we release it. First, let s ignore friction. What is it s initial and final KE? What is its initial and final PE? What is its final velocity? KE 0 0 since box is at rest PE 0 mgδh PE f 0 since box is at bottom KE F mgδh since we are ignoring friction and, so, the total mechanical energy is conserved PE 0 + KE 0 mgdh + 0 mgdh v PE 0 + 1 F 1 mv + mv gdh KE F

If we included friction: f m Δh θ Then work is done by friction, and the final velocity is smaller W W NC NC E 1 F - mv E 0 - mgdh

Storing potential energy in a spring: PE spring 1 kx

ACT: Elastic Potential Energy How does the work required to stretch a spring cm compare with the work required to stretch it 1 cm? a) same amount of work b) twice the work c) four times the work d) eight times the work The elastic potential energy is kx. So in the second case, the elastic PE is four times greater than in the first case. Thus, the work required to stretch the spring is also four times greater. 1

ACT: Springs and Gravity A mass attached to a vertical spring causes the spring to stretch and the mass to move downwards. What can you say about the spring s potential energy (PE s ) and the gravitational potential energy (PE g ) of the mass? a) both PE s and PE g decrease b) PE s increases and PE g decreases c) both PE s and PE g increase d) PE s decreases and PE g increases e) PE s increases and PE g is constant The spring is stretched, so its elastic PE increases, because PE s 1 kx. The mass moves down to a lower position, so its gravitational PE decreases, because PE g mgh.

Potential Energy Curves and Equipotentials The curve of a hill or a roller coaster is itself essentially a plot of the gravitational potential energy: DEMO: Wavy track

The potential energy curve for a spring:

Contour maps are also a form of potential energy curve: