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PHYS16 – Lecture 32 Ch. 15 Oscillations

PHYS16 – Lecture 32

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PHYS16 – Lecture 32. Ch. 15 Oscillations . Oscillations pre-question. Is a bouncing ball an example of simple harmonic motion? Yes No. Oscillations pre-question. - PowerPoint PPT Presentation

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Page 1: PHYS16 – Lecture 32

PHYS16 – Lecture 32

Ch. 15 Oscillations

Page 2: PHYS16 – Lecture 32

Oscillations pre-question

• Is a bouncing ball an example of simple harmonic motion?

A) YesB) No

Page 3: PHYS16 – Lecture 32

Oscillations pre-question

• Two kids are swinging on two swings of the same height – one kid is a little chubbier than the other. Neglecting frictional forces, which kid completes a back and forth swing in the fastest time?

A) The chubby kidB) The skinny kidC) The kid who pushes off the ground the bestD) Both complete in the same time

Page 4: PHYS16 – Lecture 32

Outline for Oscillations

• Simple Harmonic Motion– Position, Velocity, Acceleration– Force– Energy

• Resonance and Damping

Page 5: PHYS16 – Lecture 32

Oscillations and Periodic Motion

http://img.tfd.com/ggse/c9/gsed_0001_0012_0_img2993.png

Simple Harmonic Motion

1) About Equil.2) Periodic3) Sinusoidal

Page 6: PHYS16 – Lecture 32

Discussion: Examples of SHM?

• Mass on a Spring• Pendulum

• Snowboarder in halfpipe• Bungee jumper• Child on swing• Bobble head doll?

Page 7: PHYS16 – Lecture 32

Simple Harmonic Motion:Position, Velocity, Acceleration

Page 8: PHYS16 – Lecture 32

Simple Harmonic Motion

T

tAx

2

)sin(

Equilibrium Point

http://www.gailruby.com/Picture4.png

Page 9: PHYS16 – Lecture 32

Discussion: Phase

• Your book says that displacement is in terms of cosine and I just said that it is in terms of sine? Who is right?

)cos()90sin()sin(

tAtAxtAx

There is also a phase term (φ) that let’s you set the initial condition.If the oscillation starts at A it is a sine with a φ=90 degrees or a cosinewith a φ=0 degrees.

Page 10: PHYS16 – Lecture 32

SHM Position, Velocity, Acceleration

http://www.tutornext.com/system/files/u89/Chapter%2011-3.gif

)sin(

)cos(

)sin(

2 tAa

tAv

tAx

Page 11: PHYS16 – Lecture 32

Discussion

• What is the max speed and when does it occur?

Equilibrium Point

/2at t 0 0at t max

v

Av

Page 12: PHYS16 – Lecture 32

Example Question

• An object undergoes simple harmonic motion. If the amplitude and period are doubled, the object’s max speed is:

A) QuadrupledB) DoubledC) UnchangedD) HalvedE) Quartered

Page 13: PHYS16 – Lecture 32

Simple Harmonic Motion:Restoring Force

Page 14: PHYS16 – Lecture 32

Restoring Force

• Force that always points back to the equilibrium position – Example = spring

k is just a constant – for a spring it is the spring constant

xkxF ˆ

http://www.cs.wright.edu/~jslater/SDTCOutreachWebsite/images/gif/spring_mass_dia.gif

Page 15: PHYS16 – Lecture 32

Restoring Force – Spring

mkf

mk

xmkx

tAmtAk

xkxF

21 ,

)sin()sin(dtdmma

2

2

2

2

Page 16: PHYS16 – Lecture 32

Discussion: Period

• A block on a spring has a period of T. What is the period if:

A) the mass is doubled?

B) k is quadrupled?

C) A is doubled?

T2

T21

T

Page 17: PHYS16 – Lecture 32

Restoring Force - Pendulum• What is the period of a pendulum?

http://upload.wikimedia.org/wikipedia/en/thumb/a/a8/Pendulum.png/300px-Pendulum.png

Lg

smallfor ,

)sin(

Lsmgks

mgksF

Page 18: PHYS16 – Lecture 32

Simple Harmonic Motion:Energy

Page 19: PHYS16 – Lecture 32

Energy in SHM

2

22222

22

21

)(cos21)(sin

21

21

21

kAE

tAktAmE

kxmvE

http://www.farraguttn.com/science/milligan/APPhys/SHMOver_files/image022.jpg

Page 20: PHYS16 – Lecture 32

Main Points - SHM

• Movement

• Restoring Force creates oscillation

• Energy is dependent on amplitude

)sin( tAx

2

2

dtxdmkxF

2

21 kAE