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Ch 10. Harmonic Motion & Elasticity k = spring constant Units: N/m Ideal Spring & Simple Harmonic Motion Example 1 A Tire Pressure Gauge The spring constant is 320 N/m and the bar indicator extends 2.0 cm. What force does the air in the tire apply on the spring? N 4 . 6 m 020 . 0 m N 320 x k F Applied x E’S LAW: restoring force on an ideal spring x k F x 1

Ch 10. Harmonic Motion & Elasticity

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Example 1 A Tire Pressure Gauge The spring constant is 320 N/m and the bar indicator extends 2.0 cm. What force does the air in the tire apply on the spring?. Ideal Spring & Simple Harmonic Motion. Ch 10. Harmonic Motion & Elasticity. HOOKE’S LAW : - PowerPoint PPT Presentation

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Page 1: Ch 10. Harmonic  Motion  & Elasticity

1

Ch 10. Harmonic Motion & Elasticity

k = spring constant

Units: N/m

Ideal Spring & Simple Harmonic MotionExample 1 A Tire Pressure Gauge

The spring constant is 320 N/m and the bar indicator extends 2.0 cm. What force does the air in the tire apply on the spring?

N 4.6m 020.0mN320 xkF Applied

x

HOOKE’S LAW:

The restoring force on an ideal spring

xkFx

Page 2: Ch 10. Harmonic  Motion  & Elasticity

2

10.2 Simple Harmonic Motion and Reference Circle

tAAx coscos

period T: time to complete one cycle

frequency f: number of cycles per second (Hz)

Tf 1

T

f 22

amplitude A: maximum displacement

Page 3: Ch 10. Harmonic  Motion  & Elasticity

3

SHM & the Reference Circle

tAvvv

Tx sinsinmax

VELOCITYEx. 3 Maximum Speed of Loudspeaker Diaphragm

Frequency of motion is 1.0 KHz, amplitude is 0.20 mm. (a) What is the maximum speed of the diaphragm?(b) Where in the motion does this max speed occur?

tAvvv

Tx sinsinmax

(a)

sm3.1

Hz100.12m1020.02 33max

fAAv

(b) The maximum speed occurs midway between the ends of its motion.

Page 4: Ch 10. Harmonic  Motion  & Elasticity

4

Simple Harmonic Motion

ACCELERATION

tAaaa

cx coscosmax

2

FREQUENCY OF VIBRATION

mk

tAax cos2tAx cos

xmakxF 2mAkA

Page 5: Ch 10. Harmonic  Motion  & Elasticity

5

Simple Harmonic Motion Example 6 A Body Mass Measurement Device

The device below consists of a spring-mounted chair in which the astronaut sits. The spring has a spring constant of 606 N/m and the mass of the chair is 12.0 kg. The measured period is 2.41 s. Find the mass of the astronaut.

totalmk

2total km

Tf 22

astrochair2total 2mm

Tkm

kg 77.2kg 0.12

4s 41.2mN606

2

2

2

chair2astro

m

Tkm

Page 6: Ch 10. Harmonic  Motion  & Elasticity

6

10.3 Energy and Simple Harmonic Motion

A compressed spring can do work.

fofo xxkxkxsFW 0coscos 21

elastic

2212

21

elastic fo kxkxW

ELASTIC POTENTIAL ENERGY

The elastic potential energy is the energy that a spring has by virtue of being stretched or compressed. For an ideal spring, the elastic potential energy is

221

elasticPE kx

Units: joule (J)

Page 7: Ch 10. Harmonic  Motion  & Elasticity

7

Energy and Simple Harmonic Motion

Example 8 Changing the Mass of a Simple Harmonic Oscilator

A 0.20-kg ball is attached to a vertical spring. The spring constant is 28 N/m. When released from rest, how far does the ball fall before being brought to a momentary stop by the spring?

of EE 2

212

212

212

212

212

21

ooooffff kymghImvkymghImv

oo mghkh 221

m 14.0mN28

sm8.9kg 20.02

2

2

kmgho

Page 8: Ch 10. Harmonic  Motion  & Elasticity

8

10.4 The Pendulum

A simple pendulum consists of a particle attached to a frictionless pivot by a cable of negligible mass.

only) angles (small Lg

only) angles (small ImgL

Example 10 Keeping Time

Determine the length of a simple pendulum that will swing back and forth in simple harmonic motion with a period of 1.00 s.

22Lg

Tf

m 248.04

sm80.9s 00.14 2

22

2

2

gTL

2

2

4gTL

Page 9: Ch 10. Harmonic  Motion  & Elasticity

9

Damped Harmonic Motion

In simple harmonic motion, an object oscillated with a constant amplitude.

In reality, friction is always present and amplitude decreases with time.

This is damped harmonic motion.

1) simple harmonic motion2&3) underdamped4) critically damped5) overdamped

Page 10: Ch 10. Harmonic  Motion  & Elasticity

10

Driven Harmonic Motion & Resonance

When a force is applied to an oscillating system at all times, the result is driven harmonic motion.

Here, the driving force has the same frequency as the spring system and always points in the direction of the object’s velocity.

RESONANCE

Resonance is the condition in which a time-dependent force can transmitlarge amounts of energy to an oscillating object, leading to a large amplitude motion.

Resonance occurs when the frequency of the force matches a natural frequency at which the object will oscillate.

Page 11: Ch 10. Harmonic  Motion  & Elasticity

11

Elastic DeformationBecause of these atomic-level “springs”, a material tends to return to its initial shape once forces have been removed.

STRETCHING, COMPRESSION, &YOUNG’S MODULUS

ALLYFo

Young’s modulus has units of pressure: N/m2

Page 12: Ch 10. Harmonic  Motion  & Elasticity

12

Elastic DeformationExample 12 Bone Compression

In a circus act, a performer supports the combined weight (1080 N) of a number of colleagues. Each thighbone of this performer has a length of 0.55 m and an effective cross sectional area of 7.7×10-4 m2. Determine the amount that each thighbone compresses under the extra weight.

ALLYFo

YAFLL o

2429 m 107.7mN104.9

m 55.0N 540

m 101.4 5

Page 13: Ch 10. Harmonic  Motion  & Elasticity

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Elastic Deformation

SHEAR DEFORMATION & SHEAR MODULUS

ALxSFo

The shear modulus has the units of pressure: N/m2

Page 14: Ch 10. Harmonic  Motion  & Elasticity

14

Elastic Deformation

Example 14 J-E-L-L-O

You push tangentially across the topsurface with a force of 0.45 N. The top surface moves a distance of 6.0 mmrelative to the bottom surface. What isthe shear modulus of Jell-O?

ALxSFo

xAFLS o

232 mN460

m 100.6m 070.0m 030.0N 45.0

S

Page 15: Ch 10. Harmonic  Motion  & Elasticity

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Elastic Deformation

VOLUME DEFORMATION & BULK MODULUS

oVVBP

The Bulk modulus has the units of pressure: N/m2

Page 16: Ch 10. Harmonic  Motion  & Elasticity

16

10.8 Stress, Strain, and Hooke’s Law

HOOKE’S LAW FOR STRESS AND STRAIN

Stress is directly proportional to strain.

Strain is a unitless quantitiy.

SI Unit of Stress: N/m2

In general the quantity F/A is called the stress.

The change in the quantity divided by that quantity is called thestrain:

ooo LxLLVV