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Rotational Motion

Angular Displacement, Velocity, Acceleration

Rotation w/constant angular acceleration

Linear vs. Angular Kinematics

Rotational Energy

Parallel Axis Thm.

Angular Displacement (πœƒ)β€’ Angular = Rotational

β€’ Measured in Radians

β€’ 1 complete rotation = 2πœ‹ radians

β€’ Easy to convert from angular to translational

β€’ 𝑑 = πœƒπ‘Ÿ

πœƒ

𝑑

Examples

A dog (r = 0.12m) make 3 complete rotations as it rolls own a hill.

β€’ What is the angular displacement of the dog?β€’ What is the linear displacement dog?

β€’ A cat runs 7m on wheel with a radius of 0.75 m. How many rotations does the wheel make?

Angular Velocity = (πœ”)

β€’ 𝑣 =𝑑

𝑑=

πœƒ

𝑑= Ξ€π‘Ÿπ‘Žπ‘‘

𝑠𝑒𝑐

β€’ rpm = rotations per minute

β€’ π‘Ÿπ‘π‘š βˆ—2πœ‹

60= πœ”

β€’ 𝑣 = πœ”π‘Ÿ

EXAMPLE

β€’ Convert 45rpm to rad/s

β€’ What is the translation Velocity on the outer edge of the record? (diameter = 30cm)

Angular Acceleration = (Ξ±)

β€’ 𝛼 =βˆ†πœ”

𝑑

Translational Acceleration

β€’ π‘Žπ‘‘ = π›Όπ‘Ÿ

Centripetal Acceleration

β€’ π‘Žπ‘ =𝑣2

π‘Ÿ= Ο‰2π‘Ÿ

π‘Žπ‘‘

π‘Žπ‘π›Ό

Example:

A Washing machine motor accelerates from 0 -200rpm in 5 seconds.

β€’ What is the angular acceleration of the motor in rad/s2?

β€’ A small pony is in the machine (r = 0.30m), what is the translational acceleration of the pony as the motor accelerates?

β€’ What is the centripetal acceleration of the pony?

Example:

πœ” = 90π‘Ÿπ‘π‘šπ‘Ÿ = 0.10π‘š

πœ” =? π‘Ÿπ‘π‘šπ‘Ÿ = 0.04π‘š

r = 0.35mV=

Motion with Constant Acceleration

𝑣 =𝑑

𝑑

πœ” =πœƒ

𝑑

d=vt +di

πœƒ = πœ”π‘‘ + πœƒπ‘–

π‘Ž =βˆ†π‘£

𝑑

𝛼 =βˆ†πœ”

𝑑

vf =at + vi

πœ” = 𝛼𝑑 + πœ”π‘–

𝑑 =1

2π‘Žπ‘‘2 + 𝑣𝑖𝑑 + 𝑑𝑖

πœƒ =1

2𝛼𝑑2+πœ”π‘–π‘‘ + πœƒπ‘–

𝑑 =1

2(𝑣1+ 𝑣2)𝑑

πœƒ =1

2(πœ”1+ πœ”2)𝑑

𝑣𝑓2 = 2π‘Žπ‘‘ + 𝑣𝑖2

πœ”π‘“2 = 2π›Όπœƒ + πœ”π‘–

2

Example:

A biker accelerates from rest to 8 m/s in 5 seconds.

The radius of the bicycle wheels is 0.25 m.β€’ What is the angular acceleration of the wheels?

β€’ How far does the biker travel?

β€’ How many rotations does the wheel make?

β€’ If he gets tired and comes to rest in 10m, what is the angular acceleration of the wheels?

Energy in Rotational MotionObjects in motion have Kinetic Energy

Rotating Objects have Kinetic Energy

Energy of single particle:

𝐾𝐸 =1

2π‘šπ‘£2 β†’ 𝑣 = πœ”π‘Ÿ β†’

1

2π‘š πœ”π‘Ÿ 2

𝐾𝐸 =1

2π‘šπ‘Ÿ2 πœ”2 β†’ π‘šπ‘Ÿ2 = 𝐼 = π‘šπ‘œπ‘šπ‘’π‘›π‘‘ π‘œπ‘“ πΌπ‘›π‘’π‘Ÿπ‘‘π‘–π‘Ž =

𝑖

π‘šπ‘–π‘Ÿπ‘–2

𝐾𝐸 =1

2πΌπœ”2

Moment of Inertia (rotational mass)

β€’ Resistance to changes in Rotational Motion

β€’ Depends in distribution of mass.

pg. 342:

Moment of Inertiadetermine the moment of Inertia around the center of the object below

Length=LMass = m

Length=LMass = m

Length=LMass = m

Length=LMass = m

Energy in Rotational Motion

A force of 10N acts for 2.0m on 40 kg Solid Disc with a radius of 0.15m. What is the final angular speed of the wheel as it spins on its axis?

F = 10Nd=2m

m=40kgr=0.15m

π‘Š = βˆ†πΎπΈ

𝐼 =1

2π‘šπ‘Ÿ2

+

Energy in Rotational Motion

m = 2.0kg

h = 1.5m

Solid spherem=1.5kgr=0.40m

πœ” =?

𝑣 =?

A 2kg block is tied to the outer edge of a 1.5kg sphere with a diameter of 0.80m. The block is allowed to fall 1.5m, causing the sphere to rotate.What is the final speed of the wheel and the block?

βˆ†πΊπ‘ƒπΈ = 𝐾𝐸1+ 𝐾𝐸2

Energy in Rotational Motion

𝑙 = 1.0π‘š

Velocity at end of Stick?

A meter stick standing on one end is allowed to fall, What is the speed of the end of the meter stick?

βˆ†πΊπ‘ƒπΈ = 𝐾𝐸

Determine Moment of InertiaEvaluate the moment of Inertia by modeling the object divideded into many small β€œvolume elements” of mass Ξ”m

𝑰 = 𝚺 π’Žπ’“πŸ ⇉ 𝑰 = π’“πŸ π’…π’Ž Challenge: What is dm ?

Ξ”m

For 3D objects:

dm expressed in Volume Density

𝜌 =π‘‘π‘š

π‘‘π‘‰βŸΆ π‘‘π‘š = 𝜌 βˆ— 𝑑𝑉

𝐼 = ΰΆ±πœŒπ‘Ÿ2 βˆ— 𝑑𝑉

For 2D objects:

dm expressed in Linear Density

π‘‘π‘š =𝑀

𝐿

𝐼 = π‘Ÿ2 βˆ— π‘‘π‘š π‘Ÿ2= βˆ—π‘€

𝐿

Determine Moment of Inertia

Uniform (solid) Cylinder

𝐼 = ΰΆ±π‘Ÿ2 βˆ— π‘‘π‘š

π‘‘π‘š = 𝜌 βˆ— 𝑑𝑉

𝑑𝑉 = 𝑑𝐴 βˆ— 𝐿

𝑑𝐴 = πœ‹π‘Ÿ2 π‘‘π‘Ÿ = 2πœ‹π‘Ÿ

π‘‘π‘š = 𝜌(2πœ‹π‘Ÿ)𝐿

𝜌 =𝑀

𝑉=

𝑀

𝐿 βˆ— πœ‹π‘Ÿ2

Calculation:

𝐼 = ΰΆ±π‘Ÿ2 βˆ— π‘‘π‘šΰΆ±π‘Ÿ2 βˆ— πœŒπ‘‘π‘‰

𝐼 = ΰΆ±π‘Ÿ2 βˆ— 𝜌(2πœ‹π‘Ÿ)𝐿

𝐼 = 𝜌2πœ‹πΏΰΆ±π‘Ÿ3

𝐼 = 𝜌2πœ‹πΏ βˆ—π‘Ÿ4

4

𝐼 =𝑀

𝐿 βˆ— πœ‹π‘Ÿ2βˆ— 2πœ‹πΏ βˆ—

π‘Ÿ4

4

Simplify

𝐼 =1

2π‘šπ‘Ÿ2

Determine Moment of Inertia

𝐼 = ΰΆ±π‘Ÿ2 βˆ— π‘‘π‘š

π‘‘π‘š =𝑀

𝐿

Uniform Rod through the center (2D object)

Calculation:

𝐼 = ࢱ

βˆ’πΏ/2

𝐿/2

π‘Ÿ2 βˆ— π‘‘π‘š

𝐼 = ࢱ

βˆ’πΏ/2

𝐿/2

π‘Ÿ2 βˆ—π‘€

𝐿=𝑀

πΏΰΆ±π‘Ÿ2

𝐼 =𝑀

𝐿

π‘Ÿ3

3

𝐼 =𝑀

3πΏπ‘Ÿ3βˆ’ π‘Ÿ3

Simplify:

-L/2

L/2

𝐼 =1

12𝑀𝐿2

Determine Moment of Inertia

𝐼 = ΰΆ±π‘Ÿ2 βˆ— π‘‘π‘š

π‘‘π‘š =𝑀

𝐿

Uniform Rod through one end (2D object) Calculation: (you do it)

𝐼 = ࢱ

0

𝐿

π‘Ÿ2 βˆ— π‘‘π‘š

Parallel Axis Thm.β€’ Determine the moment of Inertia for alternative axis of rotation.

𝐼𝑝 = πΌπ‘π‘š +𝑀𝑑2

πΌπ‘π‘š = π‘€π‘œπ‘šπ‘’π‘›π‘‘ π‘œπ‘“ πΌπ‘›π‘’π‘Ÿπ‘‘π‘–π‘Ž π‘Žπ‘Ÿπ‘œπ‘’π‘›π‘‘ πΆπ‘’π‘›π‘‘π‘’π‘Ÿ π‘œπ‘“ π‘šπ‘Žπ‘ π‘ π‘‘ = π‘‘π‘–π‘ π‘‘π‘Žπ‘›π‘π‘’ π‘“π‘Ÿπ‘œπ‘š π‘Žπ‘₯𝑖𝑠 π‘‘π‘œ π‘π‘’π‘›π‘‘π‘’π‘Ÿ π‘œπ‘“ π‘šπ‘Žπ‘ π‘ 

cm𝐿

4

LUsing the Parallel Axis Thm., determine the moment of Inertia around the two positions shown.

Parallel Axis Thm.

𝑅

2

Using the Parallel Axis Thm, determine the moment of Inertia around the axis shown through the Hollow sphere.

cm

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