Unit 3 Work, Energy & Power Serway Chapters 7 & 8 Glencoe Chapter 10 & 11 1 Unit 3 Section 3 Conservation of Energy.

Slides:



Advertisements
Similar presentations
Part 1 /2 High School by SSL Technologies Physics Ex-39 Click Potential energy is stored energy because it has the “potential” of being used at a future.
Advertisements

ConcepTest Clicker Questions
Gravitational potential energy. Conservation of energy
Reading Quiz A cannonball is dropped from a tower. As it falls,
Warm up problem Frictionless ramp Mass: 5 kg. Angle of ramp: 30 degrees Length of ramp: 20 meters V f = ?
AP Physics C I.C Work, Energy and Power. Amazingly, energy was not incorporated into physics until more than 100 years after Newton.
An object is released from rest on a planet that
Chapter 6: Conservation of Energy
Unit 3 Section 2 Lesson 2 Potential Energy PE Objectives Unit 3 Section 2 Lesson 2 Potential Energy Objectives: ▫ Show understanding of the Physics concept.
Work, Energy, And Power m Honors Physics Lecture Notes.
Energy Physics 11. Types of Energy  Name as many different types of energy as you can. Think of an example to go with each.
Aim: How can we solve problems dealing with the Law of Conservation of Energy? HW #10 due tomorrow Do Now: A 10 kg object free falls off the top of a 100.
Conservation of Energy
Conservation of Energy Energy is Conserved!. The total energy (in all forms) in a “closed” system remains constant The total energy (in all forms) in.
Physics 151: Lecture 16, Pg 1 Physics 151: Lecture 16 Today’s Agenda l Today’s Topics: çConservation of mechanical energy çNonconservative forces and loss.
Physics 151: Lecture 15, Pg 1 Today’s Topics l Potential Energy, Ch. 8-1 l Conservative Forces, Ch. 8-2 l Conservation of mechanical energy Ch.8-4.
Energy.
Chapter 5 Pretest.
1a. Positive and negative work
Conservation of Mechanical Energy Chapter 6. Energy  As you know, energy comes in many forms. Kinetic Energy Potential Energy  Gravitational Potential.
Energy Something that enables an object to work is called energy. What are some different forms of energy? –Potential –Electrical –Mechanical –Kinetic.
Conservation of Energy November The conservation of energy.  In a closed system, energy is neither created nor destroyed. Energy simply changes.
Bellringer 10/25 A 95 kg clock initially at rest on a horizontal floor requires a 650 N horizontal force to set it in motion. After the clock is in motion,
by the normal force acting on a sliding block?
Unit 6 Energy, Work & Power.
Energy and Conservation Physics Chapter 5-2 (p ) Chapter 5-3 (p )
Unit 3 Work, Energy & Power Serway Chapters 7 & 8 Glencoe Chapter 10 & 11 1 Unit 3 Section 2 Energy and the Work-Energy Theorem.
Energy Chapters 7 & 8 10/3/2011. Potential + Kinetic = Total Energy Where P.E = mgh and K.E = ½ mV 2 and E = W = F x d Where Total Energy is conserved.
The Law of Conservation of Energy states: Conservation of Energy Energy cannot be created or destroyed Energy can be transformed from one form to another.
Copyright © 2010 Pearson Education, Inc. Chapter 7 Work and Kinetic Energy.
Units: 1Newton . 1 meter = 1 joule = 1J
Potential Energy and Conservative Forces
Energy m m Physics 2053 Lecture Notes Energy.
AP Physics C I.C Work, Energy and Power. Amazingly, energy was not incorporated into physics until more than 100 years after Newton.
Thursday, June 26, 2014PHYS , Summer 2014 Dr. Jaehoon Yu 1 PHYS 1441 – Section 001 Lecture #13 Thursday, June 26, 2014 Dr. Jaehoon Yu Potential.
Work and Energy. Work, Power, & Energy Energy offers an alternative analysis of motion and its causes. Energy is transformed from 1 type to another in.
Mechanical Energy & It’s Conservation.
1 Work When a force moves something, work is done. Whenever work is done, energy is changed into a different form. Chemical energy → Kinetic energy.
Sect. 6-5: Conservative Forces. Conservative Force  The work done by that force depends only on initial & final conditions & not on path taken between.
Chapter 5 Review Mr. Hauser. Rules of the Game Working in TEAMS, you will be asked to answer questions from the assigned chapters. You have 30 seconds.
Physics 1501: Lecture 14, Pg 1 Physics 1501: Lecture 14 Today’s Agenda l Midterm graded by next Monday (maybe …) l Homework #5: Due Friday Oct. 11:00.
Aim: How can we explain the Law of Conservation of Energy? Do Now: Homework Review.
Section 2: Conservation of Energy
Motion, Forces and Energy Lecture 7: Potential Energy & Conservation The name potential energy implies that the object in question has the capability of.
Work and Energy x Work and Energy 06.
Ch. 6, Work & Energy, Continued. Summary So Far Work-Energy Theorem: W net = (½)m(v 2 ) 2 - (½)m(v 1 ) 2   KE Total work done by ALL forces! Kinetic.
1. Work [W] = N*m = J Units: Work done by forces that oppose the direction of motion will be negative. Work and energy A. PositiveB. NegativeC. Zero Example:
Wednesday June 15, PHYS , Summer I 2005 Dr. Andrew Brandt PHYS 1443 – Section 001 Lecture #9 Wednesday June 15, 2005 Dr. Andrew Brandt Lightning.
Chapter 5.2. What do you think? What is meant when scientists say a quantity is conserved? Describe examples of quantities that are conserved. Are they.
1 Work, Energy & Power Chapter Lesson 1 Feb 10 Specific Instructional Objectives At the end of the lesson, students should be able to: –Show understanding.
Work, Power & Energy How do they relate? (Stone, Ebener, Watkins)
ENERGY Objectives: After completing this module, you should be able to: Define kinetic energy and potential energy, along with the appropriate units.
 Work  Energy  Kinetic Energy  Potential Energy  Mechanical Energy  Conservation of Mechanical Energy.
CHAPTER 5 Work and Energy Work: Work:Work done by an agent exerting a constant force is defined as the product of the component of the force in the direction.
Section 5–3: Conservation of Energy Physics Coach Kelsoe Pages 173 – 178.
Conservation of Energy Aim: How does energy transfer from one form to another?
Wednesday, Oct. 17, 2007 PHYS , Fall 2007 Dr. Jaehoon Yu 1 PHYS 1443 – Section 002 Lecture #13 Wednesday, Oct. 17, 2007 Dr. Jaehoon Yu Potential.
1 Work, Energy & Power CHAPTER Specific Instructional Objectives At the end of the lesson, students should be able to: –Show understanding of the.
Conservation of Energy
PHYS 1443 – Section 001 Lecture #9
Potential Energy and Conservation of Energy
Conservation of Energy
4*3 Spring Potential Energy
Unit 7: Work, Power, and Mechanical Energy.
Today: Work, Kinetic Energy, Potential Energy
General Physics I Work & Energy
PHYS 1443 – Section 001 Lecture #13
Chapter 5 Review.
Efficiency Law of conservation of energy always applies.
Presentation transcript:

Unit 3 Work, Energy & Power Serway Chapters 7 & 8 Glencoe Chapter 10 & 11 1 Unit 3 Section 3 Conservation of Energy

 Unit 3 Section 3 Lesson 1 Conservation of Energy  Conservation of Energy Objectives  Show understanding of conservation & conversion of energy  Correctly distinguish situation involving energy  Conservation & Conversion  Solve related PE and KE problems  Take into account FRICTION  Total Energy = PE + KE - Friction  DO NOW  What is the potential energy of a roller coaster car with a total mass of kg that is at the top of a 65.0 m (measured from the ground) hill?  HOMEWORK: Glencoe Page 308 #’s: 73 – 83 Odd  Physicslab Conservation of Energy: ompilations_CPworkbook_ConservationEnergy.xml ompilations_CPworkbook_ConservationEnergy.xml 2 Unit 3 Section 3 Lesson 1 Conservation of Energy

Conservation of Energy  Energy of an object can be thought of as the sands in an hourglass!  Energy always remain same or fixed in quantity!  But this sand can change position, from the top to bottom and bottom to top! Likewise  energy can change in form  eg. From KE  PE  eg. From KE  Friction (heat) 3

Conservation vs. Conversion of Energy  Conversion of energy is the term used to denote change in energy from one form to another.  Eg.  Burning candle: Chemical  Heat, Light  Fuel: Chemical  Heat  KE  Electricity  Nuclear explosion: Nuclear  Heat, light  Spring: Elastic PE  KE 4

Conversion of Energy  Eg. of KE  PE  Roller-coaster  Falling object 5

Free Falling object model  An object in free fall means the object is falling freely, under the influence of gravity 6 When the object is at the highest position, the GPE is at maximum and KE is zero. When the object is falling, the GPE decreases as it loses height, and the KE increases At the lowest position, the KE is at maximum and GPE is zero. GPE lost = KE gained

IN CLASS Conservation of Energy  A fresh durian of mass 5 kg is found growing at the end of a tree branch 20 m above ground. When ripe, the durian will by itself drop to the ground below. Let gravity = 10m/s 2.  Find the energy of the fresh durian just before it drops? What form is it?  GPE = mgh = 5 x 10 x 20 = 1000JGPE  Find the GPE and KE of the durian when it is 5m above ground. Sum up both the GPE and KE and compare the value with above. What can you infer from the results?  GPE = 5 x 10 x 5 = 250J.  Vf 2 = Vi 2 + 2gd  0 +2(10)15 = 300  Vf 2 = 300  V = m/s  KE = ½ mv 2 = ½ (5)(17.321) 2 = 750 J  OR ….KE = GPE original – GPE 5m = 750 J  Sum of energies = PE:250 + KE:750 = 1000J  Same as above => energy is conserved. 7

Conversion of Energy  A car of 800 kg is moving at an average speed of 5 m/s. The traffic light changed to red and so the driver stepped on the brakes to bring the car to a quick, sudden and screeching halt.  Find energy of moving car and what form of energy is this?  KE. KE = ½ mv 2 = ½ x 800 x 5 2 = 10,000 J.  What energy does the car possesses when it stops?  None.  What happened to the original energy of the moving car?  KE has changed to Sound and Heat Energy. 8

Conservation of Energy  Energy cannot be made or destroyed but it can change form, total energy stays constant  Consider a marble at the top of a ramp with 2.5 J of energy… GPE GPE = 2.5 J KE KE = 0 J GPE GPE = 0 J KE KE = 2.5 J GPE GPE = 1.25J KE KE = 1.25 J Total Energy- 2.5 J 2.5 J2.5 J a b c cb a Ignoring heat energy losses!

More Example Questions AA stone of mass 3 kg is dropped from a height of 60 cm onto the ground. a) Calculate its GPE before it is dropped GGPE = Weight x height = mgh = (3 x 10) x 0.6 = 18 J b) When it hits the ground how much GPE does it have? How much KE does it have? GPE is zero as its height off the ground is zero. KE is 18 J, all the GPE has been converted into KE c) At what speed will it hit the ground? KE = ½ mv 2 18 = (½) (3)(v 2 ) 12 = v m/s = v

 Unit 3 Section 3 Lesson 2 Conservation of Energy  Conservation of Energy Objectives  Solve related PE and KE problems  Take into account FRICTION  Total Energy = PE + KE - Friction  Potential Energy Curves  DO NOW  What is the potential energy of a roller coaster car with a total mass of kg that is at the top of a 65.0 m (measured from the ground) hill and neglecting friction, how fast will it be traveling at the bottom of the hill if the track has a 55 degree incline from the horizontal and is meters long?  HOMEWORK: Glencoe Page 309 #’s: 84– 93 All 11 Unit 3 Section 3 Lesson 2 Conservation of Energy

FRICTION and WORK and ENERGY  Total Energy usually = PE at start  PE initial + KE initial = PE final + KE final – F friction *d  F friction = μ mg COS{ Ɵ }ramp  Or F friction = μ m(v 2 /r) curve 12

Examples  A ball of mass 2 kg is dropped from a height of 5.0 m above the floor. Find the velocity of the ball as it strikes the floor?  E 0 = KE i + PE i = KE f + PE f  0 + mgh = ½ mv  0 + 2(10)(5.0 ) = ½ (2) v 2  v = √ (100) = 10m/s  A box is pushed UP an inclined plane with an angle of 37 degrees with an initial velocity of 10.0 m/s. If the surface is frictionless, how high up the ramp will the box go when it stops?  E 0 = KE i + PE i = KE f + PE f  ½ mv = 0 + mgh  ½ = 0 + gh  h = 50/10 = 5 m  How far up the ramp {distance} will it slide?  Sin Ɵ = h / d  d = h / Sin Ɵ =8.3 m 13 h d Ɵ

 A skier starts from rest at the top of a 20.0 º incline and skis in a straight line to the bottom of the slope over a distance of m. If the coefficient of friction between the skis and the snow is 0.2, calculate the skier’s speed at the bottom of the hill.  E 0 = KE i + PE i – 1 Work friction = KE f + PE f  E 0 = 0 + mgh – μ mgcos ( Ɵ ) * d = ½ mv  g( d * Sin Ɵ ) – μ gcos ( Ɵ ) * d = ½ v 2  V = √{2g( d * Sin Ɵ ) – 2 μ gcos ( Ɵ ) * d } = 35 m/s 14 Friction Examples h d Ɵ

Potential Energy Curves  E 0 = KE i + PE i – 1 Work friction = KE f + PE f  E 0 = KE i + U(x) i – 1 Work friction = KE f + U(x) f   v = + √ { (2/m) [E 0 – U(x)]}  F(x) = dU/dx  Example Hooks Law  F(x) = d/dx (1/2 kx 2 ) = kx 15 Potential Energy Curves and Questions PHYSLAB