PHYS16 – Lecture 18 Energy Conservation: Sleds and Rollercoasters October 20, 2010.

Slides:



Advertisements
Similar presentations
PHYS16 – Lecture 16 Ch. 8 Energy Conservation. Energy Pre-question Clyde, the dinosaur, is sick of his doll-sized roller coaster and decides to ride the.
Advertisements

Chapter 7 Potential Energy and Energy Conservation
Review Chap. 7 Potential Energy and Energy Conservation
ConcepTest Clicker Questions
Conservation of Energy
Gravitational potential energy. Conservation of energy
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
Physics 7C lecture 07 Potential Energy
PHYSICS 50: Lecture 7-1 RICHARD CRAIG. Homework #6 Read Chapter 7 Exercises and Problems: 7.5, 7.14, 7.29,7.38, 7.46, 7.55 Due Thursday, 3/13.
Conservation of mechanical energy Lecture Conservation of Mechanical Energy Under the influence of conservative forces only (i.e. no friction or.
Conservation of Energy
PHYS16 – Lecture 20 Review: Ch. 1-7 October 25, 2010.
PHYS16 – Lecture 17 Energy Conservation: Springs October 18, 2010.
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.
Chapter 8 Potential Energy and Conservation of Energy.
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.
Potential Energy. Height  Work is a process.  When a box is lifted, work is done on the box.  At the end, the box is resting – no kinetic energy. 
Physics 218: Mechanics Instructor: Dr. Tatiana Erukhimova Lecture 13.
Physics 218, Lecture XI1 Physics 218 Lecture 11 Dr. David Toback.
Physics 218 Lecture 11 Dr. David Toback Physics 218, Lecture XI.
Conservation of Energy
1a. Positive and negative work
Work and Energy Definition of Work Kinetic Energy Potential Energy
Chapter 6 Work and Energy. 6.1 Work Done by a Constant Force.
Copyright © 2012 Pearson Education Inc. PowerPoint ® Lectures for University Physics, Thirteenth Edition – Hugh D. Young and Roger A. Freedman Lectures.
WORK In order for work to be done, three things are necessary:
Chapter 7 The Conservation of Energy. Consider an object dropped near the surface of the earth. If the distance is small then the gravitational force.
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.
AP Physics C I.C Work, Energy and Power. Amazingly, energy was not incorporated into physics until more than 100 years after Newton.
Kinetic Energy Chap 5 associated with motion, velocity.
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.
Conservation of mechanical energy
Copyright © 2010 Pearson Education, Inc. Chapter 8 Potential Energy and Conservation of Energy.
 Types of Forces ◦ Contact Forces:  Frictional force: F f  Tensional force: F T  Normal force: F N  Air resistance force: F a  Applied force (push.
L-9 Conservation of Energy, Friction and Circular Motion Kinetic energy, potential energy and conservation of energy What is friction and what determines.
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.
Monday, Mar. 24, 2008 PHYS , Spring 2008 Dr. Jaehoon Yu 1 PHYS 1441 – Section 002 Lecture #16 Monday, Mar. 24, 2008 Dr. Jaehoon Yu Potential Energy.
Chapter 6 Work and Energy. Force,displacement  WORK.
Energy Examples Serway and Jewett 8.1 – 8.3 Physics 1D03 - Lecture 22.
Lecture 11: Potential Energy & Energy Conservation.
332 – UNIT 6 WORK & ENERGY.
Lecture 10: Work & Energy.
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.
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:
Copyright © 2010 Pearson Education, Inc. Lecture Outline Chapter 8 Physics, 4 th Edition James S. Walker.
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
Everyone grab a small whiteboard and a dry erase marker.
Chapter 7 Conservation of Energy Conservative force Non-conservative force potential energy & potential function March 2, 2010.
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)
Mechanics Topic 2.3 Work, Energy and Power. Learning Outcomes 2.3.1Outline what is meant by work Determine the work done by a non-constant force.
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.
Copyright © 2010 Pearson Education, Inc. Lecture Outline Chapter 8 Physics, 4 th Edition James S. Walker.
Energy and its Conservation Physics Mrs. Coyle. Part I Mechanical Energy – Potential – Kinetic Work Energy Theorem.
Chapter 5 Work and Energy.
 Gravity is 9.8 or ~10 m/s 2  If dropped from rest: y = -½ gt 2.
Kinetic Energy (E K ) Energy an object has due to its motion Potential Energy (E P ) Energy an object has due to its position/location Mechanical Energy.
Potential Energy and Conservation of Energy
1a. Positive and negative work
Work and energy 1. Work Wf = |fk| |Δx| cos(180°) = -|fk| |Δx| < 0
Work Who does the most work? Definition of work in physics:
Presentation transcript:

PHYS16 – Lecture 18 Energy Conservation: Sleds and Rollercoasters October 20, 2010

Administration TA Help Sessions – Su 8-9 pm, W 8-9 pm, Sa 3-5pm – Merrill 116 (around the corner from my office) Course Website – Lectures posted – Assignments + Solutions posted – Announcements posted (in class, by , on website)

This Week Spring Force and Energy Conservative vs. Nonconservative Forces Conservation of Energy – Sleds and Rollercoasters – Springs – Pendulums

Questions from Last time

When is work negative? Work is (+) when done on system, (-) when done by system Work is (+) when force and displacement in the same direction, (-) when in opposite directions Examples of some problems with Work…

P16 is Bulking up… Becca decides to move couches and applies 200 N of force and moves a couch 5 m. – What is the work done by Becca to the couch? 1000 J – What is the work done by gravity to the couch? 0 J – What is the work done by the normal force to couch? 0 J – What is the work done by friction to couch if couch moves at constant speed? J

P16 is Bulking up… Peter builds a weight system where he has to move a weight attached to a spring 5 m. He applies 5 N of force. – What is the work done by Peter to the weight? 25 J – Let’s say that the spring constant is variable so that Peter ends up moving the weight at a constant speed, then what is the work done by the spring? -25 J In this instance the spring force would be constant so W=-F spring x where the magnitude of F spring equals 5 N

P16 is Bulking up… Tim uses Peter’s weight system except he applies 10 N of force to move the weight 5 m. – What is the work done by Tim to the weight? 50 J – The weight system hasn’t changed so what is the work done by the spring? -25 J, the weight is accelerating, so the rest of Tim’s work goes to increasing kinetic energy of weight!

P16 is Bulking up… Jorge decides to slow down large moving crates. He pushes a crate with 500 N of force for 100 m, slowing the crate down. – What is the work done by Jorge to the crate? -50,000 J

P16 is Bulking up… Who did the most work? – Becca = 1000 J – Peter = 25 J – Tim = 50 J – Jorge = -50,000 J – Jorge used the most calories, so if you asked which person did the most biological work within their body, it would be Jorge… – However, if you asked who did the most mechanical work to their particular system, it would be Becca

Zero point of Gravitational Potential For gravitational potential energy where you set the zero point is arbitrary. However, once choice is made you have to stick with it. Examples for Gravitational Potential

Sledding… 5 m 10 m 20 m What is the change in energy for the sledder from the top to current position?

Energy Conservation

Conservative vs. Nonconservative Forces Conservative Forces– force where work done over ANY closed path is zero W AtoB = -W BtoA W AtoB, path 1 = W AtoB, path 2 Nonconservative force – not conservative

Conservative – Spring Force – Gravity – Buoyant Force Nonconservative – Friction – Air resistance/Drag – Fluid resistance – Applied Forces Conservative vs. Nonconservative Forces Situation Dependent Tension Normal Force

When is normal force conservative? FNFN FGFG Situation #1 Block slides down frictionless inclined plane at constant velocity. Conservative system – Normal force is Conservative, but not doing work anyway… Situation #2 Block on table. Table is lifted by person at constant acceleration. FNFN FGFG F applied Nonconservative system – Normal force is not conservative, normal force is doing work

When is tension conservative? Situation #1 Block being lifted by weight at constant velocity. Conservative system – Tension is conservative Situation #2 Block being lifted by person. T FGFG F applied Nonconservative system – Tension is not conservative T FGFG

Energy Conservation For Conservative Forces and an Isolated System: For Nonconservative Forces:

Sledding Ignore friction. What is the velocity of our sledder at the current position if they started from top? 5 m 10 m 20 m Ground

Clyde on the Rollercoaster Our favorite green dinosaur, Clyde, wants to take a ride on the rollercoaster. What is his speed at the end, if he starts at 62 cm and ends at 18 cm? Does it matter that he went over a loop? No

Discussion Question 1 Why is the second hill in a roller coaster ride always shorter than the first? (Hint: there are two answers.)

Discussion Question 2 A 0.5 kg ball is on a 0.5 m platform. There is a straight ramp down to the bottom or a ramp that looks more like a slide. Ignore friction. – What is the velocity of the ball at the end of each ramp? – Which ramp will be the quickest way down?