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Physics 218, Lecture XII 1 Physics 218 Lecture 12 Dr. David Toback

Physics 218 Lecture 12tobackgroup.physics.tamu.edu/toback/218/LastSemester/Lecture12.… · Physics 218, Lecture XII 18 Energy Summary If there is net work on an object, it changes

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  • Physics 218, Lecture XII 1

    Physics 218Lecture 12Dr. David Toback

  • Physics 218, Lecture XII 2

    This week…

    • This week we will finish up Chapters 6 & 7–Last set of topics for Exam 2

    • Exam 2: Thurs, October 26th

    • Covers chapters 1-7

  • Physics 218, Lecture XII 3

    The ScheduleThis week: (10/9) • Finish up Chapters 6&7 in lecture• Chapter 6 in recitationNext week: (10/16) • Chapter 6 HW due• Chapter 8 in lecture (reading questions due)• Chapter 7 in recitationFollowing week: (10/23)• HW 7 due• Chapter 9 in lecture on Tuesday (reading questions due)• Chapter 8 in Recitation• Exam 2 on Thursday October 26th

  • Physics 218, Lecture XII 4

    Energy• Conservation of

    Mechanical Energy problems

    • Conservative Forces• Conservation of Energy

  • Physics 218, Lecture XII 5

  • Physics 218, Lecture XII 6

    Potential EnergyA brick held 6 feet in the air has potential energy• Subtlety: Gravitational potential energy is

    relative to somewhere!Example: What is the potential energy of a book 6 feet

    above a 4 foot high table? 10 feet above the floor?• ∆U = U2-U1 = Wext = mg (h2-h1)• Write U = mgh• U=mgh + ConstOnly change in potential energy is really

    meaningful

  • Physics 218, Lecture XII 7

    Other Potential Energies: Springs

    Last week we calculated that it took ½kx2 of work to compress a spring by a distance xHow much potential energy does it now how have?

    U(x) = ½kx2

  • Physics 218, Lecture XII 8

    Problem Solving

    For Conservation of Energy problems:

    BEFORE and AFTER diagrams

  • Physics 218, Lecture XII 9

    Conservation of Energy Problems

    Before…

  • Physics 218, Lecture XII 10

    After

  • Physics 218, Lecture XII 11

    Z Z

    Before After

    C

    Falling onto a Spring

    We want to measure the spring constant of a certain spring. We drop a ball of known mass mfrom a known height Zabove the uncompressed spring. Observe it compresses a distance C.

    What is the spring constant?

  • Physics 218, Lecture XII 12

    Roller CoasterYou are in a roller coaster car of mass M that

    starts at the top, height Z, with an initial speed V0=0. Assume no friction.

    a) What is the speed at the bottom?b)How high will it go again?c) Would it go as high if there were friction?

    Z

  • Physics 218, Lecture XII 13

    Non-Conservative Forces• In this problem there are three different

    types of forces acting:1. Gravity: Conserves mechanical energy2. Normal Force: Conserves mechanical

    energy3. Friction: Doesn’t conserve mechanical

    energy• Since Friction causes us to lose

    mechanical energy (doesn’t conserve mechanical energy) it is a Non-Conservative force!

  • Physics 218, Lecture XII 14

    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!

  • Physics 218, Lecture XII 15

    Conservative ForcesIf 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)

  • Physics 218, Lecture XII 16

    Law of Conservation of Energy• Even if there is friction, Energy is conserved• Friction does work

    – Can turn the energy into heat– Changes the kinetic energy

    • Total Energy = Kinetic Energy + Potential Energy + Heat + Others…– This is what is conserved

    • Can use “lost” mechanical energy to estimate things about friction

  • Physics 218, Lecture XII 17

    Roller Coaster with FrictionA 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?

  • Physics 218, Lecture XII 18

    Energy SummaryIf 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 = ∆KIf there is a change in the potential energy, some one

    had to do some work: (Ball falling from height hspeeds up→ work done → loss of potential energy. I raise a ball up, I do work which turns into potential energy for the ball)

    ∆UTotal = WPerson =-WGravity

  • Physics 218, Lecture XII 19

    Energy Summary

    If work is done by a non-conservative force it does negative work (slows something down), and we get heat, light, sound etc.

    EHeat+Light+Sound.. = -WNCIf work is done by a non-conservative force, take this

    into account in the total energy. (Friction causes mechanical energy to be lost)

    K1+U1 = K2+U2+EHeat…K1+U1 = K2+U2-WNC

  • Physics 218, Lecture XII 20

    Next time…

    •More problems on Chapters 6 & 7

    •Recitation on Chapter 6 problems

  • Physics 218, Lecture XII 21