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PHYS16 – Lecture 23 Ch. 10 & 11 Rotation
17

PHYS16 – Lecture 23 Ch. 10 & 11 Rotation. Angular Motion – Angular displacement, velocity, & acceleration – Constant acceleration problems Angular Inertia.

Dec 19, 2015

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Page 1: PHYS16 – Lecture 23 Ch. 10 & 11 Rotation. Angular Motion – Angular displacement, velocity, & acceleration – Constant acceleration problems Angular Inertia.

PHYS16 – Lecture 23

Ch. 10 & 11 Rotation

Page 2: PHYS16 – Lecture 23 Ch. 10 & 11 Rotation. Angular Motion – Angular displacement, velocity, & acceleration – Constant acceleration problems Angular Inertia.

• Angular Motion– Angular displacement, velocity, & acceleration– Constant acceleration problems

• Angular Inertia• Angular Energy– Rotational Kinetic Energy

• Angular Force & Torque• Angular Momentum & Collisions

Ch. 10 & 11 Rotation

Page 3: PHYS16 – Lecture 23 Ch. 10 & 11 Rotation. Angular Motion – Angular displacement, velocity, & acceleration – Constant acceleration problems Angular Inertia.

Rotation pre-question

• You are unwinding a large spool of cable. As you pull on the cable with a constant tension and at a constant radius, what happens to α and ω? A) Both increase as the spool unwindsB) Both decrease as the spool unwindsC) α increases and ω decreasesD) α decreases and ω increasesE) α stays constant and ω increases

Page 4: PHYS16 – Lecture 23 Ch. 10 & 11 Rotation. Angular Motion – Angular displacement, velocity, & acceleration – Constant acceleration problems Angular Inertia.

Rotation pre-question

• An ice skater spins with his arms extended and then pulls his arms in and spins faster. Which statement is correct?A) His kinetic energy of rotation does not change

because energy is conservedB) His kinetic energy of rotation increases because

angular velocity increasesC) His kinetic energy of rotation decreases because

rotational inertia is decreasing

Page 5: PHYS16 – Lecture 23 Ch. 10 & 11 Rotation. Angular Motion – Angular displacement, velocity, & acceleration – Constant acceleration problems Angular Inertia.

Aside on Cross Product

• Cross product or Vector product – a way to multiply two vectors to get a vector

• Right-hand Rule gives directionI like to use curling hand instead…

)sin(

) , ,(

),,(),,(

122131313232

321321

ABC

ABBAABBAABBAC

BBBAAABAC

wikipedia

Page 6: PHYS16 – Lecture 23 Ch. 10 & 11 Rotation. Angular Motion – Angular displacement, velocity, & acceleration – Constant acceleration problems Angular Inertia.

Angular Force and Torque

Page 7: PHYS16 – Lecture 23 Ch. 10 & 11 Rotation. Angular Motion – Angular displacement, velocity, & acceleration – Constant acceleration problems Angular Inertia.

Torque

• Torque (τ) – a force that acts at a distance causing rotation

• Units = Joules = Nm• Vector quantity, direction given by right hand

rule

)sin(

rF

Fr

wikipedia

Page 8: PHYS16 – Lecture 23 Ch. 10 & 11 Rotation. Angular Motion – Angular displacement, velocity, & acceleration – Constant acceleration problems Angular Inertia.

Torque and Angular Acceleration

• F=ma so the angular equivalent would be τ=Iα• Is this true?

I

rmrrmarF

rFFr

tt

)sin(

Page 9: PHYS16 – Lecture 23 Ch. 10 & 11 Rotation. Angular Motion – Angular displacement, velocity, & acceleration – Constant acceleration problems Angular Inertia.

Example: Jet turbine

• The turbine of a jet engine has a moment of inertia of 25 kg∙m2. If the turbine is accelerated uniformly from rest to an angular speed of 150 rad/s in a time of 25 s, what is the torque? If the turbine is 1.0 m long, what is the force required?

r to N 150)rsin(/F

J 15025/)150)(25(/)(

/)(

0

0

0

tII

t

t

Page 10: PHYS16 – Lecture 23 Ch. 10 & 11 Rotation. Angular Motion – Angular displacement, velocity, & acceleration – Constant acceleration problems Angular Inertia.

Demo: Unrolling a spool

• When you pull the cable to the left, which way does the spool go?

University of Maryland Physics Demonstration Facility

What happens to inertia of spool as unravel?What happens to ang. velocity?What happens to ang. acceleration?

Page 11: PHYS16 – Lecture 23 Ch. 10 & 11 Rotation. Angular Motion – Angular displacement, velocity, & acceleration – Constant acceleration problems Angular Inertia.

Demo: Riding a tricycle

• When you pull cable to the left, which way does the trike go?

University of Maryland Physics Demonstration Facility

Page 12: PHYS16 – Lecture 23 Ch. 10 & 11 Rotation. Angular Motion – Angular displacement, velocity, & acceleration – Constant acceleration problems Angular Inertia.

Angular Momentum and Collisions

Page 13: PHYS16 – Lecture 23 Ch. 10 & 11 Rotation. Angular Motion – Angular displacement, velocity, & acceleration – Constant acceleration problems Angular Inertia.

Angular Momentum

• Angular momentum (L) – momentum of a rotating object

• Cross product like the dot product is a way to multiply vectors, except cross product gives vector not scalar

• Direction of cross product is given by right hand rule

IrpL

prL

)sin(

Page 14: PHYS16 – Lecture 23 Ch. 10 & 11 Rotation. Angular Motion – Angular displacement, velocity, & acceleration – Constant acceleration problems Angular Inertia.

Angular Collisions

• Angular momentum is conserved if there are no external torques

• Example: Kid jumps onto spinning merry go round, Person on a spinning chair is handed a spinning bicycle wheel, ice skater in a spin…

0L

Page 15: PHYS16 – Lecture 23 Ch. 10 & 11 Rotation. Angular Motion – Angular displacement, velocity, & acceleration – Constant acceleration problems Angular Inertia.

Discussion Question: Ice Skating

• In a spin, why do ice skaters decrease their angular velocity when they hold their arms out?

http://www.corbisimages.com/images/67/7760610C-6DF3-4A39-ACD6-C3CDEFF73296/PN015983.jpg

Kristi Yamaguchi

L=IωHolding arms out increases I.If L stays the same, and I increases thenω decreases.

What about Kinetic Energy?

Page 16: PHYS16 – Lecture 23 Ch. 10 & 11 Rotation. Angular Motion – Angular displacement, velocity, & acceleration – Constant acceleration problems Angular Inertia.

Conclusions

• Parameters for circular motion/ rotation basically have linear equivalents– θ is related to x, ω is related to v, α is related to a– I is related to m– Krotational is related to K

– L is related to p, L=Iω=rpsin(θ)– τ is related to F, τ=Iα =rFsin(θ)

Page 17: PHYS16 – Lecture 23 Ch. 10 & 11 Rotation. Angular Motion – Angular displacement, velocity, & acceleration – Constant acceleration problems Angular Inertia.

Conclusions