Conservative and Nonconservative Forces. A Force is “Conservative” if: The work it does on an object is available for kinetic energy. These forces store.

Slides:



Advertisements
Similar presentations
Physics 111: Mechanics Lecture 7
Advertisements

Work Done by a Constant Force
Gravitational potential energy. Conservation of energy
Work Done by Non-conservative Forces
6-7 Problem Solving Using Conservation of Mechanical 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.
Conservative Forces & Potential Energy
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*,
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.
Chapter 9:Linear Momentum 8-4 Problem Solving Using Conservation of Mechanical Energy 8-5 The Law of Conservation of Energy 8-6 Energy conservation with.
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.
General Physics 1, Additional questions By/ T.A. Eleyan
1a. Positive and negative work
Copyright © 2007, Pearson Education, Inc., Publishing as Pearson Addison-Wesley. Important forms of energy How energy can be transformed and transferred.
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.
Example: A 20 kg block is fired horizontally across a frictionless surface. The block strikes a platform that is attached to a spring at its equilibrium.
PHYSICS InClass by SSL Technologies with S. Lancione Exercise-42
WORK In order for work to be done, three things are necessary:
Work and Energy. Work Done by a Constant Force.
Chapter 6 Energy and Oscillations
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 6 Conservation of Energy. MFMcGrawCh06 - Energy - Revised: 2/20/102 Conservation of Energy Work by a Constant Force Kinetic Energy Potential Energy.
Chapter 8: Potential Energy and Conservation of Energy
College Physics, 7th Edition
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.
Chapter 8 - Potential Energy and Conservation of Energy Conservative vs. Non-conservative Forces Definition of Potential Energy Conservation Of Mechanical.
Review and then some…. Work & Energy Conservative, Non-conservative, and non-constant Forces.
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.
Work-2 & Power. Work and Area If the force is constant, we can graphically interpret the work done ( W = F d ) as the area of a rectangle F tall and d.
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.
Nonconservative Forces. When conservative forces act on a system ΔK + ΔU = 0 Most moving objects experience nonconservative forces – forces that remove.
Introduction to Simple Harmonic Motion Unit 12, Presentation 1.
Energy Examples Serway and Jewett 8.1 – 8.3 Physics 1D03 - Lecture 22.
Conservation of Energy
A certain pendulum consists of a 2
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.
Work and Energy Physics Mr. Day. Work F Work - the product of the magnitudes of the component of a force along the direction of displacement and the displacement.
Advanced Problems 3 These problems will contain:
Work and Energy x Work and Energy 06.
WHITE BOARD TIME !! CONSERVE ENERGY. E T = PE G + KE + PE S When comparing the energy at two different positions on a system, the total energy at one.
Potential Energy and Conservation of Energy
Lecture 12: Elastic Potential Energy & Energy Conservation.
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:
FOR SCIENTISTS AND ENGINEERS physics a strategic approach THIRD EDITION randall d. knight © 2013 Pearson Education, Inc. Chapter 10 Lecture.
Examples: Mechanical Energy Conservation
Copyright © 2007, Pearson Education, Inc., Publishing as Pearson Addison-Wesley. Important forms of energy How energy can be transformed and transferred.
Energy and its Conservation Physics Mrs. Coyle. Part I Mechanical Energy – Potential – Kinetic Work Energy Theorem.
Chapter 6 Work and Energy © 2014 Pearson Education, Inc. No need to write information in red.
Energy of Simple Harmonic Motion
Chapter 7 WORK, ENERGY, AND ENERGY RESOURCES
Chapter 7 WORK, ENERGY, AND ENERGY RESOURCES
1a. Positive and negative work
Chapter 7 Work and Energy
Kinetics of a particle: Work & Energy
Hooke's Law When a springs is stretched (or compressed), a force is applied through a distance. Thus, work is done. W=Fd. Thus elastic potential energy.
Last Time: Work, Kinetic Energy, Work-Energy Theorem Today:
Chapter 5 Table of Contents Section 1 Work Section 2 Energy
Potential Energy Problems
Potential Potential Energy
Energy Problems.
Projectile Motion and Spring Problems
T101-Q-1 Figure 1 shows the spring force as a function of position x for a spring-block system resting on a frictionless table. The block is released at.
Presentation transcript:

Conservative and Nonconservative Forces

A Force is “Conservative” if: The work it does on an object is available for kinetic energy. These forces store energy The work done by conservative forces is the negative of the potential energy change. W = -ΔU Force of gravity and Spring force are examples of conservative forces W c = F  x (if force is constant) W c =  Fdx = -  dU = -  U (if force varies)  Fdx = -  dU Fdx = -dU F = -dU/dx

Review Springs

Springs Elastic Potential Energy Energy stored in a compressed or extended spring. U s = ½ kx 2 k is the spring constant. x is the distance the spring is compressed or stretched.

A special spring is constructed in which the restoring force is in the opposite direction to the displacement, but is proportional to the cube of the displacement; i.e., F = -kx 3 This spring is placed on a horizontal frictionless surface. One end of the spring is fixed, and the other end is fastened to a mass M. The mass is moved so that the spring is stretched a distance A and then released. Determine each of the following in terms of k, A, and M. a. The potential energy in the spring at the instant the mass is released

b. The maximum speed of the mass c. The displacement of the mass at the point where the potential energy of the spring and the kinetic energy of the mass are equal

A 2 kg block is dropped from a height of 0.45 m above an uncompressed spring, as shown above. The spring has an elastic constant of 200 n/m and negligible mass. The block strikes the end of the spring and sticks to it. (a)Determine the speed of the block at the instant it hits the end of the spring (b) Determine the period of the simple harmonic motion that ensues

(c) Determine the distance that the spring is compressed at the instant the speed of the block is maximum (d) Determine the maximum compression of the spring (e) Determine the amplitude of the simple harmonic motion

Block A of mass 4.0 kg is on a horizontal, frictionless tabletop and is placed against a spring of negligible mass and spring constant 650 N/m. The other end of the spring is attached to a wall. The block is pushed toward the wall until the spring has been compressed a distance x, as shown. The block is released and follows the trajectory shown, falling 0.80 m vertically and striking a target on the floor that is a horizontal distance of 1.2 m from the edge of the table.

(a)Calculate the time elapsed from the instant block A leaves the table to the instant it strikes the floor. (b)Calculate the speed of the block as it leaves the table (c)Calculate the distance x the spring was compressed

A Force is “Non-Conservative” if: The work done by these forces causes energy to be lost to the system. They “steal” energy from the system Examples of this type of force is friction and air resistance The energy they remove from the system is no longer available for kinetic energy

Conservation of energy and conservative and nonconservative forces When conservative forces act on a system E i = E f When nonconservative forces act on a system Our Energy formula becomes E i – W nc = E f **Work done is negative. It removes energy from the system. It is in the form of heat lost to the system.

Example : One of the tallest and fastest roller coasters in the world is the Steel Dragon in Mie, Japan. The ride includes a vertical drop of 93.5 m. The coaster has a speed of 3.0 m/s at the top of the drop. The speed at the bottom is 41.0 m/s. Find the work done by the nonconservative forces on a 55.0 kg rider during the descent.

Example: A 60 kg sledder starts from rest and slides down a 20 o incline 100 m long. (a) If the coefficient of friction is 0.090, what is the sledder’s speed at the base of the incline.

(b) If the snow is level at the foot of the incline and has the same coefficient of friction, how far will the sledder travel along the level snow?

© 2013 Pearson Education, Inc. Power  The rate at which energy is transferred or transformed is called the power P.  The SI unit of power is the watt, which is defined as: 1 watt = 1 W = 1 J/s Slide Highly trained athletes have a tremendous power output. If the particle moves at velocity while acted on by force, the power delivered to the particle is:

© 2013 Pearson Education, Inc. Example Choosing a Motor Slide ,800 W

© 2013 Pearson Education, Inc. Example Power Output of a Motor Slide W

© 2013 Pearson Education, Inc. Four students run up the stairs in the time shown. Which student has the largest power output? QuickCheck Slide

© 2013 Pearson Education, Inc. Four students run up the stairs in the time shown. Which student has the largest power output? QuickCheck Slide