Aim: How do we explain conservation of energy in systems under the influence of non-conservative forces?

Slides:



Advertisements
Similar presentations
Wednesday, Nov. 24, 2010 PHYS , Fall 2010 Dr. Jaehoon Yu 1 PHYS 1441 – Section 002 Lecture #20 - Review Wednesday, Nov. 24, 2010 Dr. Jaehoon Yu.
Advertisements

Q07. 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.
Chapter 5 – WORK and ENERGY. 5.2 MECHANICAL 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*,
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.
General Physics 1, Additional questions By/ T.A. Eleyan
A block is launched up a frictionless 40° slope with an initial speed v and reaches a maximum vertical height h. The same block is launched up a frictionless.
Example: The simple pendulum l Suppose we release a mass m from rest a distance h 1 above its lowest possible point. ç What is the maximum speed of the.
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.
Principles of Physics - Foederer. Energy is stored in a spring when work is done to compress or elongate it Compression or elongation= change in length.
Chapter 5 Work and Energy
Conservation of Energy. What Is Energy? Energy makes change possible. Science definition: Energy is the ability to do work Measured in Joules, J. Just.
CONSERVATION OF MECHANICAL ENERGY
Energy By. Jonathan Lee and Harry Chun. What is “energy”? Energy is the ability to do work Potential Energy (PE) is the “possible” ability to do work.
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, Energy, Power Work The work done by force is defined as the product of that force times the parallel distance over which it acts. The.
Chapter 5 Work and Energy. Force, displacement  WORK.
Chapter 5 Work and Energy. Review  x = v i  t + ½ a  t 2  x = ½ (v i + v f )  t v f = v i + a  t v f 2 = v i 2 + 2a  x.
ADV PHYSICS Chapter 5 Sections 2 and 4. Review  Work – force applied over a given distance W = F Δ x [W] = Joules, J  Assumes the force is constant.
Potential Energy and Conservative Forces
Preview Objectives Definition of Work Chapter 5 Section 1 Work.
Review and then some…. Work & Energy Conservative, Non-conservative, and non-constant Forces.
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)
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.
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.
Physics. Session Work, Power and Energy - 3 Session Objectives.
Energy and Energy Conservation. Energy Two types of Energy: 1. Kinetic Energy (KE) - energy of an object due to its motion 2. Potential Energy (PE) -
© Houghton Mifflin Harcourt Publishing Company Preview Objectives Definition of Work Chapter 5 Section 1 Work.
Energy Examples Serway and Jewett 8.1 – 8.3 Physics 1D03 - Lecture 22.
Work, Energy, and Energy Conservation Chapter 5, Sections Pg
A certain pendulum consists of a 2
Chapters 7, 8 Energy. What is energy? Energy - is a fundamental, basic notion in physics Energy is a scalar, describing state of an object or a system.
Motion, Forces and Energy Lecture 7: Potential Energy & Conservation The name potential energy implies that the object in question has the capability of.
Work has a specific definition in physics
A 19-kg block on a rough horizontal surface is attached to a light spring (force constant = 3.0 kN/m). The block is pulled 6.3 cm to the right from.
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.
© Houghton Mifflin Harcourt Publishing Company Preview Objectives Definition of Work Chapter 5 Section 1 Work.
Spring Force and Energy Notes
Chapter 8 Conservation of Energy EXAMPLES. Example 8.1 Free Fall (Example 8.1 Text book) Determine the speed of the ball at y above the ground The sum.
Examples: Mechanical Energy Conservation
Physics 1D03 - Lecture 19 Kinetic Energy. Physics 1D03 - Lecture 19 Then the Work-Energy Theorem says: The total work done by all external forces acting.
Work and Energy. Section Objectives: Define work by relating it to force and displacement. Identify where work is being performed in a variety of situations.
Copyright © by Holt, Rinehart and Winston. All rights reserved. ResourcesChapter menu Section 1 Work Chapter 5 Definition of Work Work is done on an object.
Copyright © by Holt, Rinehart and Winston. All rights reserved. ResourcesChapter menu Section 1 Work Chapter 5 Definition of Work Work is done on an object.
The Physics Energy. Objectives Identify several forms of energy. Calculate kinetic energy for an object. Apply the work–kinetic energy theorem to solve.
Conservation of Energy Aim: How does energy transfer from one form to another?
Copyright © by Holt, Rinehart and Winston. All rights reserved. ResourcesChapter menu Work and Energy Chapter 5 Table of Contents Section 1 Work Section.
60 1. What is the mass M in the system as given in the
Chapter 5 Section 1 Work Objectives
Chapter 5 Section 1 Work Preview Objectives Definition of Work.
Chapter 5 Section 1 Work Preview Objectives Definition of Work.
1a. Positive and negative work
7 Conservation of Energy
Conservation of Energy with Springs AP style
from rest down a plane inclined at an angle q with the horizontal.
Chapter 5 Work and Energy
Do Now: (Yesterday’s Atwood’s Machine)
Aim: How do we apply conservation of energy to solving problems?
Examples: Mechanical Energy Conservation
Chapter 5 Definition of Work
General Physics I Work & Energy
Aim: How do we explain conservation of energy?
Potential Energy Problems
Chapter 8: Potential Energy & Conservation of Energy
Potential Potential Energy
Sect. 7.7: Conservative & Non-Conservative Forces
Projectile Motion and Spring Problems
Presentation transcript:

Aim: How do we explain conservation of energy in systems under the influence of non-conservative forces?

Do Now: The energies indicated on your vertical axis are evenly space; that is E3 – E2 = E2 – E1 . The energy E1 is equal to U(x1 ) and the energy E3 is equal to U(x3 ). a) Determine the numerical values of x1 and x3 . b) Describe the motion of the particle if its total energy is E2 . c) What is the particle’s speed at x = x1 if its total energy E =58 J? d) The particle is released from rest at x =1/2x. Find its speed as it passes through x = x1

Recall Extended Definition of Work and Energy Wtot = Wc + WNC + Wext

When friction is present.. Energy is not conserved. Ei + Wkinetic friction =Ef

Example 1 A child of mass 25 kg slides down a slide of height 3 m. When she reaches the bottom of the slide her speed is 5 m/s. How much internal energy was produced? Mgh-Wf=1/2 Mv2 25(10)(3)-Wf=1/2(25)(5)2 Wf =-437.5 J So 437.5 J of internal energy are produced

Example 2 The particle shown below has a mass of 0.1 kg is released from rest at A and the surface of the bowl is rough. The speed of the particle at B is 1.50 m/s. Assume the radius of the bowl is 0.2m. What is its kinetic energy at B? KE=1/2mv2 KE=1/2(.1) (1.5)2 =0.1125 J How much mechanical energy is transformed due to friction as the particle moves from A to B? Ui -Wf = KE Mgh – Wf =.1125 J .1(10)(.2)-Wf =0.1125 Wf =-0.0875 J so 0.0875 J are lost due to friction Is it possible to determine the coefficient of friction from these results in any simple manner? No

Problem 2

Example 3 A 10 kg block is released from point A. The track is frictionless except for the portion between points B and C, which has a length of 6.00 m. The block travels down the track, hits a spring of force constant 2,250 N/m, and compresses the spring 0.300 m from its equilibrium position before coming to rest momentarily. Determine the coefficient of kinetic friction between the block and the rough surface between B and C. (Solution on next page)

Problem 3 MgH – Wf =1/2kx2 10(10)(3) – Wf =1/2(2250)(.3)2 Wf = -198.75 J So Wf =Ff d 198.75= Ff (6) Ff =33.125 N And Ff = µFN =µmg 33.125=µ(100) µ=0.33

Example 4 A sled of mass m is given a kick on a frozen pond. The kick imparts to it an initial speed of v m/s. The coefficient of kinetic friction between the sled and ice is µ. Use energy considerations to find the distance (d) the sled moves before it stops. ½ mv2 = Wf 1/2mv2 = Ff d 1/2mv2 = µFN d 1/2mv2 =µmgd d= v2 /(2µg)