Lecture 21: Chapter 11 - Torque and Rotational Motion - Prof. Wolfgang Losert, Study notes of Physics

A part of the lecture notes for phys141, covering chapter 11 on torque and rotational motion. Topics include the definition of torque, the torque vector equation, net torque, torque and angular acceleration, work in rotational motion, power in rotational motion, and angular momentum. Important concepts such as the right-hand rule, the order of vector multiplication, and the relationship between torque and angular momentum are discussed.

Typology: Study notes

Pre 2010

Uploaded on 02/13/2009

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Phys141 – Fri 10/21 – Lecture 21
Today: Chapter 11
MON: Chapter 12 – Static equilibrium
Administrative:
Reading for Mon: Chapter 12
Midterm 2: Wed Nov 9
Office hours Mon Nov 7 NOT Wed Nov 9
Final exam Saturday 8am-10am December 17
Torque: tendency of a force to generate
rotation an object about some axis
Torque vector τ= rx F
(vector product)
Direction: perpendicular to
the plane formed by the
position vector and the
force vector (right-hand
rule)
Magnitude: r F sin(θ)
Depends on the choice of point O
Properties of the Vector Product
The order in which the vectors are multiplied is important
Ax B= - Bx A
If Ais parallel to B(θ= 0oor 180o), then Ax B= 0
For example, Ax A= 0
()
dd d
dt dt dt
×= ×+×
AB
AB BA
A x (B + C) = A x B + A x C
Torque Vector Example
Example 1: I x j
Example 2: Given the force
τ= ?
m
N
)
ˆ
00.5
ˆ
00.4(
)
ˆ
00.3
ˆ
00.2(
jir
jiF
+=
+=
ˆˆ ˆˆ
[(4.00 5.00 )N] [(2.00 3.00 )m]
ˆˆ ˆˆ
[(4.00)(2.00) (4.00)(3.00)
ˆˆ ˆˆ
(5.00)(2.00) (5.00)(3.00)
ˆ
2.0 N m
τ
=×= + × +
+×
+ ×
=⋅
rF i j i j
ii ij
ji ij
k
pf3
pf4

Partial preview of the text

Download Lecture 21: Chapter 11 - Torque and Rotational Motion - Prof. Wolfgang Losert and more Study notes Physics in PDF only on Docsity!

Phys141 – Fri 10/21 – Lecture 21

  • Today: Chapter 11
  • MON: Chapter 12 – Static equilibrium
  • Administrative:

Reading for Mon: Chapter 12

Midterm 2: Wed Nov 9

Office hours Mon Nov 7 NOT Wed Nov 9

Final exam Saturday 8am-10am December 17

Torque: tendency of a force to generate

rotation an object about some axis

Torque vector τ = r x F

(vector product)

Direction: perpendicular to

the plane formed by the

position vector and the

force vector (right-hand

rule)

Magnitude: r F sin(θ)

Depends on the choice of point O

Properties of the Vector Product

The order in which the vectors are multiplied is important A x B = - B x A

If A is parallel to B (θ = 0 o^ or 180 o), then A x B = 0

  • For example, A x A = 0

d d d dt dt dt

× = × + ×

A B

A B B A

A x (B + C) = A x B + A x C

Torque Vector Example

• Example 1: I x j

• Example 2: Given the force

m

N

r i j

F i j

= +

[(4.00^ ˆ 5.00 )N]ˆ^ [(2.00ˆ 3.00 )m]ˆ [(4.00)(2.00)ˆ ˆ^ (4.00)(3.00)ˆ^ ˆ (5.00)(2.00)ˆ ˆ^ (5.00)(3.00)ˆ^ ˆ 2.0 ˆN m

τ = × = + × + = × + ×

  • × + × = ⋅

r F i j i j i i i j j i i j k

Torque: tendency of a force to rotate an

object about some axis

Magnitude:

Two ways to understand torque equation:

(1) τ = F d

d: perpendicular distance from the axis of rotation to a line drawn along the direction of the force d = r sin Φ

(2) τ = Ft r F (^) t: tangential part of force F (^) t = F sin Φ

τ = r F sin φ

Net Torque

F 1 would cause counter- clockwise rotation about O F 2 would cause clockwise rotation about O

Total (net) torque = sum of torques

Στ =τ 1 +τ 2 = F 1 d 1 – F 2 d 2

Torque and Angular Acceleration

  • Rotating mass m (along circle of radius r) tangential force F t

-> tangential acceleration:

Ft = mat

Rotational motion description:

In general: Στ =Ια

2 t t t

a

F r ma r mr I

r

τ = I α

Work in Rotational Motion

Work done by F on the object as it rotates through an infinitesimal distance ds = r d θ dW = F.^ d s = ( F sin φ) r d θ

dW = τ d θ

IF the center O is fixed, the radial

component of F does no work

because it is perpendicular to

the displacement

Note: Both work and torque have

units of Nm – but remember:

torque is not an energy!!

Conservation Law Summary

• For an isolated system -

(1) Conservation of Energy:

  • Ei = Ef

(2) Conservation of Linear Momentum:

  • p i = p f

(3) Conservation of Angular Momentum:

  • L i = L f