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Physics 218 Lecture 15

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Title: Physics 218 Lecture 15


1
Physics 218Lecture 15
  • Dr. David Toback

2
Notes
  • Exam Next Tuesday
  • Here. Usual class time Covering
  • Exam 1 material
  • Chapter 3(9)
  • Chapter 4(1-8)
  • Chapter 5(1-3)
  • Chapter 6(1-8)
  • Chapter 7(1-4)
  • Calculus 2
  • Today Rest of Chapter 8 NOT ON EXAM

3
Overview of Chapter 8
  • Chapter 8 is a mish-mash of topics
  • The basic idea is to learn about energy so you
    can do a new set of problems that you cant do
    using previous ideas. This means understanding
  • Potential Energy, Mechanical Energy and when
    there is Conservation of Mechanical Energy
    (conservative forces)

4
Today
  • Topics
  • Potential Energy, Mechanical Energy and when
    there is Conservation of Mechanical Energy
    (conservative forces).
  • Conservation of Energy
  • Conservative and non-Conservative Forces
  • How to back and forth between types of problems
  • In many ways this is a review for the exam

5
(No Transcript)
6
Potential Energy
  • Amount of energy that could be released
  • Gravitation potential energy
  • If you lift up a ball it has the potential to do
    damage.
  • Raise it a height h gt U mgh
  • Compress a spring
  • Spring potential energy U ½kx2
  • Doing External Work can change the potential
    energy

7
Forces Potential Energy
  • Another definition

8
Mechanical Energy Conservative Systems
  • If there is net work on an object, it changes the
    kinetic energy of the object (Gravity forces a
    ball falling from height h to speed up. Work
    done.)
  • Wnet DK
  • If there is a change in the potential energy,
    there is net work done on an object (ball
    falling from height h speeds up. Work done, loss
    of potential energy)
  • DUTotal -Wnet

9
Conservation of Mechanical Energy
  • DK DU 0
  • K2U2 K1U1
  • E K U
  • ½mv2 (mgy ½kx2)

10
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
  • Gravity
  • Springs
  • Others
  • Non-Conservative As you move along a path, the
    potential energy or kinetic energy is turned into
    heat, light, sound etc.
  • Friction
  • Others

11
Old Problems
  • Lets do some old problems in some new ways

12
Example with Gravity
  • A rock is held at height h and dropped.
  • What is the speed when it hits the ground?
  • A rock, at any height y relative to the ground,
    has potential energy of Umgy.
  • What must be the force on the rock?

13
Law of Conservation of Energy
  • Even if there is friction, Energy is conserved
  • Friction turns the energy into heat
  • Total Energy Kinetic Energy Potential Energy
    Heat Others
  • This is what is conserved
  • Can use lost mechanical energy to estimate
    things about friction

14
Spherical Roller Coaster
  • A roller coaster of mass m starts at rest at
    height y1 and falls down the path, then back up
    until it hits height y2 (y1 gt y2). An odometer
    tells us that the total scalar distance traveled
    is d.
  • Assuming we dont know anything about the
    friction or the path, how much work is done by
    friction on this path?
  • Assuming a constant force of friction, F, between
    the car and the track is constant, find F.

15
Friction and Springs
A block of mass m is traveling on a rough
surface. It reaches a spring (spring constant k)
with speed vo and compresses it by an amount X.
Determine m
16
Gravitational Potential Energy
  • If I move to outer space, does is it still true
    that Umgh?
  • What is U in outer space?

17
Escape Velocity
  • What happens if I throw a ball up in the air?
    Will it fall down?
  • What if I throw it up really fast?
  • What if I throw it up REALLY fast?
  • Can I throw it up so fast that it will never come
    down? How fast would that be?

18
Package Dropped from a Rocket
  • Drop a package with speed V at a height r0 so far
    above the earths surface, the mgh approximation
    doesnt work. Eventually, the package falls to
    the surface of the earth.
  • What is the final speed of the package?
  • Why doesnt the answer depend on the direction of
    the initial velocity?

19
Exam
  • Tuesday, here at the regular time
  • 4 Problems
  • Problems similar to those in the
    book/homework/lecture
  • No numbers

20
Next Thursday
  • Reading Conservation of Linear Momentum

21
Advice 1
  • How to prepare
  • Do all the homework problems and keep doing them
    until they are easy!
  • How do you know when you are ready to take the
    exam?
  • Pick the hardest problems from the lecture,
    examples and HW.
  • You are ready when you can do any of those
    problems without looking at ANY
    notes/books/examples etc.
  • My Advice 2 ?

22
My Advice II Dont come underprepared
23
Conservative Forces
  • Conservative Work doesnt depend on the path
    taken
  • A force is conservative if the net work done by
    the force on an object moving around any closed
    path is zero
  • Friction is an example of a non-conservative Force

24
Law of Conservation of Energy
  • Even if there is friction, Energy is conserved
  • Friction turns the energy into heat
  • Total Energy Kinetic Energy Potential Energy
    Heat Others
  • This is what is conserved

25
Power Potential Energy
  • Definition Power is the rate at which work is
    done.
  • P dw/dt
  • Pavg Dw/Dt
  • Name the unit after James Watt
  • 1 Watt 1Joule/sec
  • Definition

26
Gravitational Potential Energy
  • What is the change in potential energy as you
    move from one point in space to another?
  • What is a useful coordinate axis to define the
    gravitational potential energy?
  • What is the potential energy in that reference
    point?
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