physics 218, lecture xx1 physics 218 lecture 20 dr. david toback
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Physics 218, Lecture XX 1
Physics 218Lecture 20 Dr. David Toback
Physics 218, Lecture XX 2
Angular Quantities
• Position Angle • Velocity Angular Velocity • Acceleration Angular Acceleration • Force Torque Today we’ll finish:
– Mass
– Momentum
– Energy
Physics 218, Lecture XX 3
Physics 218, Lecture XX 4
Angular Quantities
• Position Angle • Velocity Angular Velocity • Acceleration Angular Acceleration • Force Torque Today we’ll finish:
– Mass
– Momentum
– Energy
Physics 218, Lecture XX 5
Calculating Moments of Inertia
dmR I
mR I
2
2
Physics 218, Lecture XX 6
Calculate the Moment of Inertia
A pulley has mass M, uniform density, radius R, and rotates around its fixed axis
Calculate its moment of inertia
R
Physics 218, Lecture XX 7
Angular Quantities
• Position Angle • Velocity Angular Velocity • Acceleration Angular Acceleration • Force Torque Today we’ll finish:
– Mass Moment of Inertia – Momentum
– Energy
Physics 218, Lecture XX 8
Angular Momentum
Define the Angular Momentum L
L = I
Is this a vector?
dt
dLI
dt
dL
dt
Ld
dt
Id
dt
dII
)()(
Physics 218, Lecture XX 9
Newton’s Laws
• Momentum vs. Angular Momentum
p=mv L=I
• Newton’s Laws
F=dp/dt = dL/dt
Physics 218, Lecture XX 10
Conservation of Angular Momentum
Const L 0 if
dt
dL
By Newton’s laws, the angular momentum of a body can change, but the angular momentum for a system cannot
change Conservation of Angular Momentum
Physics 218, Lecture XX 11
Ice Skater
• This one you’ve seen on TV
• Try this at home in a chair that rotates
• Get yourself spinning with your arms and legs stretched out, then pull them in
Physics 218, Lecture XX 12
Clutch Design
Model a car clutch as two plates, each with radius R, and masses MA and MB
Assume IPlate = ½MR2
Plate A spins with speed 1 and Plate B is at rest.
We close them and they spin together
Find the final angular velocity of the system
Physics 218, Lecture XX 13
Angular Quantities
• Position Angle • Velocity Angular Velocity • Acceleration Angular Acceleration • Force Torque Today we’ll finish:
– Mass Moment of Inertia – Momentum Angular Momentum L
– Energy
Physics 218, Lecture XX 14
Rotational Kinetic Energy
KE = ½I2
Conservation of Energy must take into account
rotational kinetic energy
Physics 218, Lecture XX 15
Rotating Rod
A rod of mass uniform density, mass m and length l pivots at a hinge. It starts at rest at a right angle and is let go
What is when it reaches the bottom?
What is the velocity of the tip at the bottom?
Physics 218, Lecture XX 16
Rotation and Translation• Objects can both Rotate
and Translate
• Both have energy separately
KE = ½ mv2 + ½I2
• Always true when you have rolling without slipping
Physics 218, Lecture XX 17
Rolling Down an Incline
A solid ball of mass m and radius R rolls without slipping down a plane with height h.
What will be the final speed of the ball?
What would be the speed if the ball didn’t roll? Note:
Isphere = 2/5MR2
Physics 218, Lecture XX 18
Person on a Disk
A person with mass m stands on the edge of a disk with radius R and moment ½MR2. Neither is moving.
The person then starts moving on the disk with speed V.
Find the angular velocity of the disk
Physics 218, Lecture XX 19
Same Problem: Forces
Same problem but with Forces
Physics 218, Lecture XX 20
Next Time
• Chapter 11– It’s a review of Chapter 10, but more
sophisticated
– Math, Torque, Angular Momentum, Energy
• The material will not be on the 3rd exam, but will help with the exam. It will all be on the final.
• Exam 3 is Tuesday November 26th
Physics 218, Lecture XX 21
Physics 218, Lecture XX 22
Hollow Cylinder
Consider a hollow cylinder with uniform density, inner radius R1, outer radius R2 and total Mass M.
Find the moment of Inertia
Physics 218, Lecture XX 23
Parallel-Axis Theorem
• Quick Trick for calculating Moments
• I = Icm + Mh2
• Example