Download presentation
Presentation is loading. Please wait.
Published byDarion Sidell Modified over 9 years ago
1
Chapter 8 Rotational Motion © 2014 Pearson Education, Inc.
2
In a rotating object… The angle θ in radians is defined: where l is the arc length. © 2014 Pearson Education, Inc.
3
For one full revolution… l = 2r = So… 2r r Then… = 2 rad
4
Conversions 1 rev = 360 o = 2π rad
5
A particular bird’s eye can just distinguish objects that subtend an angle no smaller than about 3x10 -4 rad. How small an object can the bird just distinguish when flying at a height of 100m? © 2014 Pearson Education, Inc.
6
x = (theta) v = (omega) a = (alpha) © 2014 Pearson Education, Inc. New variables…
7
Fill in the blank… A ____________ causes acceleration. A ____________ causes rotation. force torque
8
Let’s pretend... You need to loosen a stuck bolt with a wrench... You aren’t strong enough...what do you do?
9
When opening a door... Is it easier to open if you push close to or far away from the hinges?
10
Torque Produces rotation = Fr Long arm, less force More force, shorter arm Ex. wrench, screwdriver, doorknob
11
Because most things can rotate clockwise or counterclockwise we need + and – for direction. + is counterclockwise - is clockwise
12
End of Chapter Problems 24, 25, 26, 29
13
If…F = ma Then… = I I = moment of inertia
14
Rotational Inertia Resistance to change in rotational motion Greater distance from center of mass to rotation point = greater inertia
15
Why do baseball players “choke up” on the bat? “ Choking up” on a baseball bat will increase speed of swing
16
Why do giraffes have a slower gait than Chihuahuas?
17
Why do longer pendulums swing more slowly than shorter ones?
18
8-5 Rotational Dynamics; Torque and Rotational Inertia I for various objects… © 2014 Pearson Education, Inc.
19
End Day 2 © 2014 Pearson Education, Inc.
20
If…F = ma Then… = I I = moment of inertia
21
8-5 Rotational Dynamics; Torque and Rotational Inertia I for various objects… © 2014 Pearson Education, Inc.
22
End of Chapter Problems 31, 37, 38, 40, 42
23
Rotational Kinetic Energy ½ mv 2 Becomes ½ I 2
24
Rotational Kinetic Energy K = translational + rotational K = ½ mv 2 + ½ I 2
25
Problem Solving Strategy E = E U g = K t + K r mg y = 1/2mv 2 + 1/2I 2 Note – friction must be present No friction = no rolling (object will just slide)
26
This will help… Linear velocity Radius = rotational velocity V = r
27
End of chapter problems 50, 51, 52, 55
28
End Day 3
29
Angular Momentum If the net torque on an object is zero, the total angular momentum is conserved: Iω = Iω p = mv
30
To change an object’s momentum… FΔt =Δp F = Δp/Δt = ΔL/Δt
31
© 2014 Pearson Education, Inc.
Similar presentations
© 2024 SlidePlayer.com. Inc.
All rights reserved.