Instructor: Dr. Tatiana Erukhimova

Slides:



Advertisements
Similar presentations
PHYSICS 218 Final Exam Fall, 2006 STEPS __________________________________________________________________ No calculators are allowed in the test. Be sure.
Advertisements

Work Done by a Constant Force
Physics 218, Lecture XV1 Physics 218 Lecture 15 Dr. David Toback.
AP Physics B Summer Course 年AP物理B暑假班
Kinetic energy. Energy Energy is usually defined as the capacity to do work. One type of energy is kinetic 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 218: Mechanics Instructor: Dr. Tatiana Erukhimova Lecture 19.
Physics 218: Mechanics Instructor: Dr. Tatiana Erukhimova Lecture 22.
Physics 218: Mechanics Instructor: Dr. Tatiana Erukhimova Lecture 23.
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: Mechanics Instructor: Dr. Tatiana Erukhimova Lecture 16.
Physics 218: Mechanics Instructor: Dr. Tatiana Erukhimova Lecture 21.
Physics 218: Mechanics Instructor: Dr. Tatiana Erukhimova Lecture 19.
Instructor: Dr. Tatiana Erukhimova
Physics 218 Lecture 14 Dr. David Toback Physics 218, Lecture XIV.
Instructor: Dr. Tatiana Erukhimova
Physics 218: Mechanics Instructor: Dr. Tatiana Erukhimova Lecture 42.
Chapter 7 All forces are CONSERVATIVE or NON-CONSERVATIVE.
Instructor: Dr. Tatiana Erukhimova
Physics 218, Lecture XII1 Physics 218 Lecture 12 Dr. David Toback.
Physics 218: Mechanics Instructor: Dr. Tatiana Erukhimova Lecture 40.
LCROSS crashes into the Moon. Image credit: NASA.
Physics 218: Mechanics Instructor: Dr. Tatiana Erukhimova Lecture 13.
Physics 218, Lecture XI1 Physics 218 Lecture 11 Dr. David Toback.
Physics 218: Mechanics Instructor: Dr. Tatiana Erukhimova Lecture 12.
Physics 218: Mechanics Instructor: Dr. Tatiana Erukhimova Lecture 22.
Physics 218: Mechanics Instructor: Dr. Tatiana Erukhimova Lecture 23.
Physics 218, Lecture XIII1 Physics 218 Lecture 13 Dr. David Toback.
Physics 218 Lecture 15 Dr. David Toback Physics 218, Lecture XV.
General Physics 1, Additional questions By/ T.A. Eleyan
Physics 218, Lecture XIV1 Physics 218 Lecture 14 Dr. David Toback.
Physics 218: Mechanics Instructor: Dr. Tatiana Erukhimova Lecture 23.
Conservation of Energy. What Is Energy? Energy makes change possible. Science definition: Energy is the ability to do work Measured in Joules, J. Just.
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,
Kinetic Energy, Work, Power, and Potential Energy
Kinetic Energy, Work, Power, and Potential Energy
The Law of Conservation of Energy states: Conservation of Energy Energy cannot be created or destroyed Energy can be transformed from one form to another.
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
Energy Transformations and Conservation of Mechanical Energy 8.01 W05D2.
Sect. 7.7: Conservative & Non- Conservative Forces.
Sect. 6-5: Conservative Forces. Conservative Force  The work done by that force depends only on initial & final conditions & not on path taken between.
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.
Conservation of Energy. Forms of Energy Mechanical Energy Thermal Energy Other forms include.
Conservative and non-conservative forces Potential energy Total mechanical energy Energy conservation Lecture 11: Potential energy.
Energy Examples Serway and Jewett 8.1 – 8.3 Physics 1D03 - Lecture 22.
Conservation of Energy
Advanced Problems 3 These problems will contain:
Potential Energy & Energy Conservation. Work Done by Gravity 1 l Example 1: Drop ball Y i = h Y f = 0 mg S y x Y i = h Y f = 0 mg S y x 10.
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.
Potential Energy and Conservation of Energy
 One for which work done does not depend on the path taken only on initial and final positions  Gravity and elastic forces are conservative  Why is.
Examples: Mechanical Energy Conservation
Physics 218: Mechanics Instructor: Dr. Tatiana Erukhimova Lectures 17, 18.
Physics 218: Mechanics Instructor: Dr. Tatiana Erukhimova Lectures 16, 17, 18.
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)
Instructor: Dr. Tatiana Erukhimova
Instructor: Dr. Tatiana Erukhimova
Work Done by a Constant Force
from rest down a plane inclined at an angle q with the horizontal.
Instructor: Dr. Tatiana Erukhimova
Instructor: Dr. Tatiana Erukhimova
Potential Energy Problems
Instructor: Dr. Tatiana Erukhimova
Instructor: Dr. Tatiana Erukhimova
Sect. 7.7: Conservative & Non-Conservative Forces
Instructor: Dr. Tatiana Erukhimova
Energy and Momentum.
Presentation transcript:

Instructor: Dr. Tatiana Erukhimova Physics 218: Mechanics Instructor: Dr. Tatiana Erukhimova Lecture 15

Quiz This is a one-dimensional problem. Suppose a particle is attracted to the origin with a force Find the potential function.

Mechanical energy is conserved! Work-energy theorem: Mechanical energy is conserved!

Examples Strategy: write down the total mechanical energy, E, E = KE + U at the initial and final positions of a particle:

Initial E1=KE1+U1…

Final E2=KE2+U2

Then use or

H

Who hits the bottom with a faster speed? Water Slide Who hits the bottom with a faster speed?

Roller Coaster You are in a roller coaster car of mass M that starts at the top, height H, with an initial speed V0=0. Assume no friction. What is the speed at the bottom? How high will it go again? Would it go as high if there were friction? H

Roller Coaster with Friction A roller coaster of mass m starts at rest at height y1 and falls down the path with friction, then back up until it hits height y2 (y1 > y2). Assuming we don’t know anything about the friction or the path, how much work is done by friction on this path?

Conservative Forces If there are only conservative forces in the problem, then there is conservation of mechanical energy Conservative: Can go back and forth along any path and the potential energy and kinetic energy keep turning into one another Good examples: Gravity and Springs Non-Conservative: As you move along a path, the potential energy or kinetic energy is turned into heat, light, sound etc… Mechanical energy is lost. Good example: Friction (like on Roller Coasters)

Law of Conservation of Energy Mechanical Energy NOT always conserved If you’ve ever watched a roller coaster, you see that the friction turns the energy into heating the rails, sparks, noise, wind etc. Energy = Kinetic Energy + Potential Energy + Heat + Others… Total Energy is what is conserved! K1+U1 = K2+U2+EHeat…

Total Energy is what is conserved! K1+U1= K2+U2+EHeat…

A gun shoots a bullet at angle θ with the x axis with a velocity of magnitude Vm. What is magnitude of the velocity when the bullet returns to the ground? How high it will go?

Spring problem revisited A block of mass M is on a horizontal surface and is attached to a spring, spring constant k. If the spring is compressed an amount A and the block released from rest, how far from unstretched position will it go before stopping if there is no friction between the block and the surface? How will this answer change is the block is not attached to the spring??

Block of mass m has a spring connected to the bottom Block of mass m has a spring connected to the bottom. You release it from a given height H and want to know how close the block will get to the floor. The spring has spring constant k and natural length L. H y=0