Potential Energy and Conservation of Energy

Slides:



Advertisements
Similar presentations
Physics 111: Mechanics Lecture 7
Advertisements

Work Done by a Constant Force
Conservation of Energy
Gravitational potential energy. Conservation of energy
6-7 Problem Solving Using Conservation of Mechanical Energy
Chapter 6: Conservation of Energy
Copyright © by Holt, Rinehart and Winston. All rights reserved. ResourcesChapter menu Work and Energy Chapter 5 Table of Contents Section 1 Work Section.
AP Physics B Summer Course 年AP物理B暑假班
Work, Energy, And Power m Honors Physics Lecture Notes.
Physics 111 Practice Problem Statements 07 Potential Energy & Energy Conservation SJ 8th Ed.: Chap 7.6 – 7.8, 8.1 – 8.5 Contents: 8-4, 8-5, 8-16, 8-19*,
AP Physics I.C Work, Energy and Power.
Work and Energy Chapter 7.
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.
Lecture notes by Dr. M. S. Kariapper KFUPM - PHYSICS 5-Nov-061/8 Potential Energy and Conservation of Energy. Conservative and non-conservative forces.
PHYSICS 231 INTRODUCTORY PHYSICS I
Conservation of Energy
General Physics 1, Additional questions By/ T.A. Eleyan
1a. Positive and negative work
T101Q7. A spring is compressed a distance of h = 9.80 cm from its relaxed position and a 2.00 kg block is put on top of it (Figure 3). What is the maximum.
Honors Physics Chapter 11
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,
Chapter 5 – Work and Energy If an object is moved by a force and the force and displacement are in the same direction, then work equals the product of.
Chapter 8: Potential Energy and Conservation of Energy
by the normal force acting on a sliding block?
Conservative and Non-Conservative Forces Teacher: Luiz Izola
Copyright © 2010 Pearson Education, Inc. Chapter 7 Work and Kinetic Energy.
Potential Energy and Conservative Forces
Energy m m Physics 2053 Lecture Notes Energy.
Chapter 8 - Potential Energy and Conservation of Energy Conservative vs. Non-conservative Forces Definition of Potential Energy Conservation Of Mechanical.
Physics 203 College Physics I Fall 2012
Work and Energy. Work a force that causes a displacement of an object does work on the object W = Fdnewtons times meters (N·m) or joules (J)
Work and Energy Chapter 7 Conservation of Energy Energy is a quantity that can be converted from one form to another but cannot be created or destroyed.
Energy Transformations and Conservation of Mechanical Energy 8
Energy Transformations and Conservation of Mechanical Energy 8.01 W05D2.
Chapter 6 Work and Energy. Units of Chapter 6 Work Done by a Constant Force Work Done by a Varying Force Kinetic Energy, and the Work-Energy Principle.
Physics 1D03 - Lecture 22 Potential Energy Work and potential energy Conservative and non-conservative forces Gravitational and elastic potential energy.
Conservative Forces: The forces is conservative if the work done by it on a particle that moves between two points depends only on these points and not.
2008 Physics 2111 Fundamentals of Physics Chapter 8 1 Fundamentals of Physics Chapter 8 Potential Energy & Conservation of Energy 1.Potential Energy 2.Path.
Reading Quiz - Work & Energy
NAZARIN B. NORDIN What you will learn: Define work, power and energy Potential energy Kinetic energy Work-energy principle Conservation.
Work and Energy.
Energy Examples Serway and Jewett 8.1 – 8.3 Physics 1D03 - Lecture 22.
Phys211C7 p1 Kinetic Energy: Energy associated with motion K = ½ mv 2 Work done by a force on an object is that forces contribution to  K may only depend.
Conservation of Energy
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.
Advanced Problems 3 These problems will contain:
1 Chapter 7 Potential Energy Potential Energy Potential energy is the energy associated with the configuration of a system of two or more interacting.
Chapter 7 Conservation of Energy (cont’d) Mechanical energy conservation Examples Work by non-conservative forces March 4, 2010.
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.
Lecture 12: Elastic Potential Energy & Energy Conservation.
Physics 1D03 - Lecture 22 Potential Energy Serway and Jewett 8.1 – 8.3 Work and potential energy Conservative and non-conservative forces Gravitational.
Kinetic Energy and Work
Wednesday June 15, PHYS , Summer I 2005 Dr. Andrew Brandt PHYS 1443 – Section 001 Lecture #9 Wednesday June 15, 2005 Dr. Andrew Brandt Lightning.
Conservation of Energy
Examples: Mechanical Energy Conservation
Chapter 7 Conservation of Energy Conservative force Non-conservative force potential energy & potential function March 2, 2010.
 Work  Energy  Kinetic Energy  Potential Energy  Mechanical Energy  Conservation of Mechanical Energy.
WHY DO WE DO WORK? Work transfers energy from one object to another. So, what is energy? –Energy is the ability to do work. Major forms (for our purposes)
Chapter 5 Work and Energy. Question A crate of mass 10 kg is on a ramp that is inclined at an angle of 30⁰ from the horizontal. A force with a magnitude.
Conservative and Nonconservative Forces. A Force is “Conservative” if: The work it does on an object is available for kinetic energy. These forces store.
Warm up – Do old way A boy pulls a large box with a mass of 50 kg up a frictionless incline (
1a. Positive and negative work
Work Done by a Constant Force
Work Done by a Constant Force
Springs & Conservation of Energy pg
Chapter 5 Table of Contents Section 1 Work Section 2 Energy
Energy Problems.
Presentation transcript:

Potential Energy and Conservation of Energy AP Physics Chapter 8 Potential Energy and Conservation of Energy

AP Physics Turn in Chapter 7 Homework, Worksheet, and Lab Lecture: Potential Energy and Conservation of Energy Q&A

Review on Work Done by Gravity Work done by gravity (weight): Interpretation: Object falling down from rest  h < 0  Wg > 0 Wg = K  K > 0  K > 0 (Isn’t obvious?) If you want to stop the object, K: +  0  K < 0  W < 0 by you You are doing _______ work negative  Object doing work to you Object at height has the potential ability to do work (later)

Kinetic and Potential Energy Kinetic energy: ability to do work due to motion One object or system Associated with an object Potential energy: ability to do work due to a relative position System Object and earth Mass and spring Associated with a force

Change in Potential Energy (U) and Work The change of a potential energy is defined to equal to the negative of the work done by its associated force. Not directly defining U W by gravity is the same for same h even when object falls from different initial heights

Conservative and Nonconservative Forces The net work done by a conservative force on a particle moving around any closed path is zero. The work done by a conservative force on a particle moving between two points does not depend on the path taken by the particle. Examples: gravity (weight), spring force Nonconservative Force: The work done by a nonconservative force on a particle moving between two points depends on the path taken by the particle. Example: friction, force you push a table from some initial point to final point

Force and Potential Energy Only conservative forces have potential energies. Gravitational potential energy Spring potential energy Nonconservative forces do not have potential energies associated with them. No pushing or pulling potential energy No frictional potential energy

Gravitational Potential Energy, U or Ug Define Gravitational Potential Energy: m: mass g = 9.8 m/s2 y: vertical position, height (upward has been defined as the positive direction.) Reference point: y = 0  U = 0 Free to choose reference point. (U has no physical significance, only U has physical significance.) Unit:

Elastic or Spring Potential Energy, U or Usp Define Spring Potential Energy: k: spring constant x: displacement from equilibrium (relaxed) position of spring Reference point has been chosen to be at x = 0. Unit:

Example: Pg188-3 In Fig. 8-30, a 2.00 g ice flake is released from the edge of a hemispherical bowl whose radius r is 22.0 cm. The flake-bowl contact is frictionless. How much work is done on the flake by its weight during the flake’s descent to the bottom of the bowl? What is the change in the potential energy of the flake-Earth system during that descent? If that potential energy is taken to be zero at the bottom of the bowl, what is its value when the flake is released? If, instead, the potential energy is taken to be zero at the release point, what is its value when the flake reaches the bottom of the bowl? Ice flake r

Solution: Pg188-3

Practice: Pg189-5 In Fig. 8-32, a frictionless roller coaster of mass m = 825 kg tops the first hill with speed v0 = 17.0 m/s at height h = 42.0 m. How much work does the gravitational force do on the car from that point to a) point A, b) point B, and c) point C? If the gravitational potential energy of the coaster-Earth system is taken to be zero at point C, what is its value when the coaster is at d) point B and e) point A? f) If mass m were doubled, would the change in the gravitational potential energy of the system between points A and B increase, decrease, or remain the same? h A C B h/2 v0 O

h A C B h/2 v0 O Solution: Pg189-5

Solution: Pg189-5 (continued)

Practice: Pg189-6 A 1.50 kg snowball is fired from a cliff 12.5 m high with an initial velocity of 14.0 m/s, directed 41.0o above the horizontal. How much work is done on the snowball by he gravitational force during its flight to the flat ground below the cliff? What is the change in the gravitational potential energy of the snowball-Earth system during the flight? If that gravitational potential energy is take to be zero at the height of the cliff, what is the value when the snowball reaches the ground?

Solution Pg189-6 :

(Total) Mechanical Energy, E Sum of kinetic and potential energy: or simply,

Conservation of Mechanical Energy When only conservative forces are doing work within a system, the kinetic energy and potential energy can change. However, their sum, the mechanical energy E of the system, remains unchanged.

Example: Pg199-116 A 70.0 kg man jumping from a widow lands in an elevated fire rescue net 11.0 m below the window. He momentarily stops when he has stretched the net by 1.50 m. Assuming that mechanical energy is conserved during this process and that the net functions like an ideal spring, find the elastic potential energy of the net when it is stretched by 1.50 m. Let y = 0 after the net is stretched 1.5 m, then i y = 1.5m + 11m =12.5 m yi = 12.5 m, yf = 0, m = 70.0kg, Us.f = ? y = 1.50 m f y = 0

Practice: Pg197-96 A volcanic ash flow is moving across horizontal ground when it encounters a 10o upslope. The front of the flow then travels 920 m on the upslope before stopping. Assume that the gases entrapped in the flow lift the flow and thus make the frictional force from the ground negligible; assume also that mechanical energy of the front of the flow is conserved. What was the initial speed of the front of the flow? Let y = 0 at bottom, then yi = 0, yf = 920m sin10o = 160m, vf = 0, f vi = ? i y = 0

Practice: Pg191-31 k m  A block with mass m = 2.00 kg is placed against a spring on a frictionless incline with angle  = 30.0o (Fig. 8-43). (The block is not attached to the spring.) The spring, with spring constant 19.6 N/cm, is compress 20.0 cm and then released. What is the elastic potential energy of the compressed spring? What is the change in the gravitational potential energy of the block-Earth system as the block moves from the release point to its highest point on the incline? How far along the incline is the highest point from the release point?

f • L h Solution: Pg191-31 i • y = 0 

Practice: Pg190-18 A block of mass m = 2 Practice: Pg190-18 A block of mass m = 2.0 kg is dropped from a height h = 40 cm onto a spring of spring constant k = 1960 N/m (Fig. 8-36). Find the maximum distance the spring is compressed. yi = x + h Let the maximum compression be x, and let y = 0 at maximum compression, then h k i y = x f y = 0

What if the block is slowly lowered to the top of the spring What if the block is slowly lowered to the top of the spring? How much will it be compressed? Conservation of Energy? No, hand is doing negative work when lowering the block. i h f Then how? N = Fsp W

Force and Potential Energy For each potential energy, there is a conservative force associated with it. Nonconservative forces have no potential energies.

Work Done By External Force Work done by external force will change the total mechanical energy of the system: If there is also kinetic friction, where is the heat gain (change in thermal energy) Total Energy: Eint = Chemical Energy & Nuclear Energy

all external forces, normally including spring force and gravity. Work and Energy Change all external forces (excluding spring force and gravity) Total work done by __________________________. Work-Kinetic Energy Theorem: all external forces, normally including spring force and gravity. Total work done by _______________________________.

Practice: Pg198-105 The temperature of a plastic cube is monitored while the cube is pushed 3.0 m across a floor at constant speed by a horizontal force of 15 N. The monitoring reveals that the thermal energy of the cube increases by 20 J. What is the increase in the thermal energy of the floor along which the cube slides?

Practice: Pg198-111 A 0.63 kg ball thrown directly upward with an initial speed of 14 m/s reaches a maximum height of 8.1 m. What is the change in the mechanical energy of the ball-Earth system during the ascent of the ball to that maximum height?

1 2 3 Practice: Pg193-51 No friction d (k) In Fig. 8-51, a 3.5 kg block is accelerated from rest by a compressed spring of spring constant is 640 N/m. The block leaves the spring at the spring’s relaxed length and then travels over a horizontal floor with a coefficient of kinetic friction k = 0.25. The frictional forces stops the block in distance d = 7.8 m. What are the increase in the thermal energy of the block-floor system, the maximum kinetic energy of the block, and the original compression distance of the spring.

Solution: Pg193-51 During distance d (2 3), No friction d (k) 1 2 3 Solution: Pg193-51 During distance d (2 3), During uncompressing of spring, (1 2)