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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