Quick Concept Review and Fact Check

Slides:



Advertisements
Similar presentations
Potential Energy, Conservation of Energy
Advertisements

ConcepTest Clicker Questions
Conservation of Energy
6-7 Problem Solving Using Conservation of Mechanical Energy
Physics 218, Lecture XV1 Physics 218 Lecture 15 Dr. David Toback.
AP Physics B Summer Course 年AP物理B暑假班
Chapter 9 Potential Energy & Conservation of Energy
Dynamics and transportation 1) Review of work, energy; 2) PRS questions on work; 2) Introduction to transportation.
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.
Department of Physics and Applied Physics , F2010, Lecture 13 Physics I LECTURE 13 10/20/10.
Physics 218, Lecture XIII1 Physics 218 Lecture 13 Dr. David Toback.
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.
Physics 218 Lecture 14 Dr. David Toback Physics 218, Lecture XIV.
Physics 218, Lecture XII1 Physics 218 Lecture 12 Dr. David Toback.
Physics 218, Lecture XI1 Physics 218 Lecture 11 Dr. David Toback.
8-1 Conservative and Nonconservative Forces Definition 1: The total work around a closed path is zero for a conservative force. Work done by gravity =
Physics 218 Lecture 11 Dr. David Toback Physics 218, Lecture XI.
Physics 218, Lecture XIII1 Physics 218 Lecture 13 Dr. David Toback.
1a. Positive and negative work
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.
Copyright © 2007, Pearson Education, Inc., Publishing as Pearson Addison-Wesley. Important forms of energy How energy can be transformed and transferred.
Work and Energy. Work Done by a Constant Force Definition of Work: The work done by a constant force acting on an object is equal to the the displacement.
The power of Niagra Falls Height: 167 ft Flow: 600,000 U.S. gallons per second.
Chapter 6 Work and Energy.
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.
2/19/03Physics 103, Spring 2004, U. Wisconsin1 Physics 103: Lecture 9 Energy Conservation, Power Today’s lecture will cover Potential Energy Conservation.
Chapter 8: Potential Energy and Conservation of Energy
Work, Energy, and Momentum Tanya Liu. Notes All my slides will be uploaded to Professor Dodero’s site:
Conservative and Non-Conservative Forces Teacher: Luiz Izola
Physics for Scientists and Engineers, 6e Chapter 8 – Potential Energy.
Chapter 6 Work and Energy.
Potential Energy and Conservative Forces
Energy m m Physics 2053 Lecture Notes Energy.
Gravitational Potential Energy p extra p ,7 Conservation of Energy p , 7(tricky)extra p Chapter Review for above p. 226.
Chapter 8 - Potential Energy and Conservation of Energy Conservative vs. Non-conservative Forces Definition of Potential Energy Conservation Of Mechanical.
Energy Transformations and Conservation of Mechanical Energy 8
Copyright © 2010 Pearson Education, Inc. Chapter 8 Potential Energy and Conservation of Energy.
Work has a specific definition in physics. Work is done anytime a force is applied through a distance.
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.
Chapter 6 Work and Energy. Units of Chapter 6 Work Done by a Constant Force Kinetic Energy, and the Work-Energy Principle Potential Energy Conservative.
Work & Energy Chapters 7-8 Work Potential Energy Kinetic Energy Conservation of Mechanical Energy.
2008 Physics 2111 Fundamentals of Physics Chapter 8 1 Fundamentals of Physics Chapter 8 Potential Energy & Conservation of Energy 1.Potential Energy 2.Path.
© 2010 Pearson Education, Inc. Lecture Outline Chapter 5 College Physics, 7 th Edition Wilson / Buffa / Lou.
Work and Energy. Work Done by a Constant Force The work done by a constant force is defined as the distance moved multiplied by the component of the force.
Physics 6A Work and Energy examples Prepared by Vince Zaccone For Campus Learning Assistance Services at UCSB.
Energy Examples Serway and Jewett 8.1 – 8.3 Physics 1D03 - Lecture 22.
Chapter 6: Work and Energy Essential Concepts and Summary.
Physics 111: Lecture 11, Pg 1 Physics 111: Lecture 11 Today’s Agenda l Review l Work done by variable force in 3-D ç Newton’s gravitational force l Conservative.
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
Lecture 10: Work & Energy.
 E is always constant, but KE and PE can change  If PE and KE change, they must change in such a way as to keep E constant Example Consider the 1D free-fall.
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.
Physics 1D03 - Lecture 22 Potential Energy Serway and Jewett 8.1 – 8.3 Work and potential energy Conservative and non-conservative forces Gravitational.
Work = Force x Displacement …when F and D are in the same direction (The block would be accelerating !)
Conservation of Energy
Energy 1. Work 2. Kinetic Energy 3. Work-Energy Principle 4. Friction 5. Potential Energy 6. Conservation of Energy ©2013 Robert Chuckrow.
Examples: Mechanical Energy Conservation
UB, Phy101: Chapter 6, Pg 1 Physics 101: Chapter 6 Work and Kinetic Energy l New stuff: Chapter 6, sections
Energy and Work. Work done by a Force Distance x Force x Distance x Force x Distance x Force x Textbook defines work due to a force as the product of.
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.
Warm up – Do old way A boy pulls a large box with a mass of 50 kg up a frictionless incline (
© 2010 Pearson Education, Inc. Lecture Outline Chapter 5 College Physics, 7 th Edition Wilson / Buffa / Lou.
Potential Energy and Conservation of Energy
Conservative and Nonconservative Forces
Classical Mechanics Midterm 2 Review Force and Energy
Presentation transcript:

Quick Concept Review and Fact Check

Which of the following processes are due to non-conservative forces? 0 / 100 Hockey puck slides over ice at constant speed. Golf ball rolls to a stop over rough grass. Car moves at constant speed with constant power from engine. A only B only C only A and B B and C Cross-Tab Label

Name the following terms in the correct order. 0 / 100 Name the following terms in the correct order. Gravitational potential, Kinetic energy, Spring Potential Spring potential, Kinetic energy, gravitational potential. Kinetic energy, gravitational potential, Spring potential. Cross-Tab Label

Work, Force and Energy redux. Chapter 8.4-8.5 Work, Force and Energy redux. The most important messages are these: Mechanical energy is given by: E = K + U Energy changes only if there are non-conservative forces: DE = Ef – Ei = Wnc This means that Mechanical Energy is CONSERVED if Wnc = 0. SUMMARY RELATIONSHIPS: Wtotal = Wc + Wnc = DK Wc = - DU Wnc = DE

This is a type of “book-keeping” for energy. Starting with the definition of mechanical energy… E = K + U Then the changes in the energy terms are also related…. DE = DK + DU Each energy change is associated with a type of work…. DE = DK + DU Wnc = Wtot - Wc And if we re-arrange the terms, we get… Wtot = Wc + Wnc

What does this mean, “in words”? DE = DK + DU Wnc = Wtot - Wc The non-conservative work, Wnc, goes into heat (or sound, etc.), and is “lost” from the mechanical system. Wnc is NEGATIVE! (almost always) Example is friction. The force of friction acts opposite to the direction of motion, so W = F x D is NEGATIVE. In words….. The mechanical energy is CHANGED by the amount of non-conservative work done by the forces in the system. (Heat energy going into or out of the system) The Kinetic Energy is INCREASED by the amount of total work done by forces in the system (conservative plus non-conservative). The potential energy changes OPPOSITE to the work done by conservative forces in the system. (Potential stores energy of conservative forces)

Conservative Work: Atwood’s machine Q: An “Atwood’s Machine” is shown in Fig. 1 at the left. What is the speed of the two masses just before mass #2 hits the ground? Potential DECREASES E INIT= 0 (my choice of potential) DE = 0 (conservative forces) So, Efinal = Einit Potential INCREASES CHECK: Suppose m1 was equal to zero? What if masses are equal?

How much does spring compress? DX K V M V=0 Solve using energy conservation: What is initial mechanical energy? (Kinetic and potential) What is final mechanical energy? (Kinetic and potential) Set them equal. Solve in class (next slide).

How much does the spring compress? 0 / 100 M V V=0 K DX A mass M moving at speed V hits an initially relaxed spring of constant K. What is the maximum compression of the spring, DX? B C A A. B. C. Cross-Tab Label

Non-conservative Work L V0 M M Rough spot, coefficient of friction m. A block of mass M is moving initially with speed V0. It passes over a rough patch of table of length L. Given the mass M, the initial speed V0, and the coefficient of friction, find the final speed of the block. 1. Draw the picture. 2. What is given? 3. What are the relationships? Non-conservative work: Work-energy: DE = E1 – E0

Set up the problem V1 L V0 M M Rough spot, coefficient of friction m. A block of mass M is moving initially with speed V0. It passes over a rough patch of table of length L. Given the mass M, the initial speed V0, and the coefficient of friction, find the final speed of the block. What is the initial total energy? What is the final total energy? What is the change in energy? What is the non-conservative work (Force x distance)? Use WNC = DE. Solve in class (next slide).

What is the final speed? Cross-Tab Label 0 / 100 V1 L V0 M M Rough spot, coefficient of friction m. A. B. C. Cross-Tab Label

Hard by force, easy by energy. M Ball of mass M slides without friction down the ramp, and then slides WITH friction (m) on the grass. How far does it slide, L? H L What is the initial energy? What is the final energy? What is the work done? (Hint: non-conservative) Use Wnc = DE.

Ball rolling down slide. 0 / 100 Ball rolling down slide. Ball of mass M slides without friction down the ramp, and then slides WITH friction (m) on the grass. How far does it slide, L? H L A. B. C. Cross-Tab Label

Combo problem. Ball slides down ramp, and then falls by free-fall a height Y. What is range X? H V Y X Kinematics: Conservation of energy: