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Lecture 17 October 29, 2004

Lecture 17 October 29, 2004. On Wednesday - Thumping

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Page 1: Lecture 17 October 29, 2004. On Wednesday - Thumping

Lecture 17October 29, 2004

Page 2: Lecture 17 October 29, 2004. On Wednesday - Thumping

On Wednesday - Thumping

Page 3: Lecture 17 October 29, 2004. On Wednesday - Thumping

The Drum

Each of these modes are usually excited.The tension of the drum determines the frequency of each mode.The modes may NOT be harmonicEach mode dies out at a different rate.The player can change the basic “tone” of the drum by changing the tension of the drum head.

Page 4: Lecture 17 October 29, 2004. On Wednesday - Thumping

Kettle Drum INITIAL Spectrum

Page 5: Lecture 17 October 29, 2004. On Wednesday - Thumping

Drum Frequencies

Page 6: Lecture 17 October 29, 2004. On Wednesday - Thumping

The Sonogram

Page 7: Lecture 17 October 29, 2004. On Wednesday - Thumping

Modes

All modes are excited at first strike.These vibrations may excite others … resonance. Each mode decays in a different time. Amplitude

time

Page 8: Lecture 17 October 29, 2004. On Wednesday - Thumping

So … back to the tuning forks

Page 9: Lecture 17 October 29, 2004. On Wednesday - Thumping

Objects will resonate when

They are in contact with something that vibrates at its resonant frequency. Buzz in cars is a good example

Sound can cause resonance if it is at a frequency that is the resonant frequency of another object nearby. It must have enough energy.

Page 10: Lecture 17 October 29, 2004. On Wednesday - Thumping

Back to the trip from the instrument into our heads

Page 11: Lecture 17 October 29, 2004. On Wednesday - Thumping

The Trip

CREATIONOf Sound

TRAVELAND

ROOM ACOUSTICS

Page 12: Lecture 17 October 29, 2004. On Wednesday - Thumping

Sound Travels

ENERGY

Page 13: Lecture 17 October 29, 2004. On Wednesday - Thumping

Something is Missing

As time progresses, the amount of energy received by the ear increases.We need a measure of energy per unit time.

ENERGY

Page 14: Lecture 17 October 29, 2004. On Wednesday - Thumping

ENERGY PER UNIT TIME

sec

Joule1 watt 1

Second

JoulesPOWER

TimeUnit

Energy

Page 15: Lecture 17 October 29, 2004. On Wednesday - Thumping

Example = The Light Bulb

Consider a 60 Watt light bulb.It requires 60 Joules of energy each second.One Joule = 1 Newton Meter Joule=1( N-m)x (1 lb/4.45N) x

(3.28ft/m) Joule=0.738 ft-lbs

Page 16: Lecture 17 October 29, 2004. On Wednesday - Thumping

Thinking about light bulbs

60 Joules = 44.2 ft-lbsLift a ~4 pound weight 10 ft. or about one story of a building.Do this every second for 60 watts.

Joule=0.738 ft-lbs

A 100 lb woman would have to run up about 2 floorsof a building per second to generate this much power!

Page 17: Lecture 17 October 29, 2004. On Wednesday - Thumping

About Spheres ….

2

3

4

3

4

rAreaSurface

rVolume

r

Page 18: Lecture 17 October 29, 2004. On Wednesday - Thumping

Energy Spreads Out

These AREAS increase with r2.

Power per unit area therefore DECREASES with r2.

Page 19: Lecture 17 October 29, 2004. On Wednesday - Thumping

Let’s go to a concert.50 Meters

30 watts Ear Canal ~ 0.5 cm = 0.005 m

Area = (0.005)2=0.000025 m2

Page 20: Lecture 17 October 29, 2004. On Wednesday - Thumping

Houston we have another problem

Ear Area = (0.005)2=0.000025 m2

30 watts, 50 meters

Page 21: Lecture 17 October 29, 2004. On Wednesday - Thumping

To the ear ….

50m

30 watt

Area of Sphere =r2

=3.14 x 50 x 50 = 7850 m2

Ear Area = 0.000025 m2

Page 22: Lecture 17 October 29, 2004. On Wednesday - Thumping

In the ear…

wattsmm

watt

Ear

m

watt

m

watt

areaunit

power

000000095.0000025.00038.0

:

0038.07850

30

22

22

How do we deal with all of these zeros???

Page 23: Lecture 17 October 29, 2004. On Wednesday - Thumping

Answer: Scientific NotationChapter 1 in Bolemon, Appendix 2 in Johnston

0.000000095 watts = 9.5 x 10-8 watts

Page 24: Lecture 17 October 29, 2004. On Wednesday - Thumping

NOTE

10a/10b=10a-b

Example 1000/10=103/101=10(3-1)=102=100 10000/0.005=104/5 x 10-3=(1/5)x10(4-(-3))

=(1/5)x 107 =(10/5) x 106 = 2,000,000

You can actually get used to doing it this way! But you probably won’t!

Page 25: Lecture 17 October 29, 2004. On Wednesday - Thumping

Q:Can we hear 9.5 x 10-8 watts?

?

Page 26: Lecture 17 October 29, 2004. On Wednesday - Thumping

Acoustic Power (Watts)

INSTRUMENT Acoustic Power

Clarinet 0.05

Double Bass 0.16

Trumpet 0.31

Cymbals 9.5

Bass Drum 25

Entire Orchestra 67

Page 27: Lecture 17 October 29, 2004. On Wednesday - Thumping

Decibels - dB

The decibel (dB) is used to measure sound level, but it is also widely used in electronics, signals and communication.

Page 28: Lecture 17 October 29, 2004. On Wednesday - Thumping

Decibel continued (dB)Suppose we have two loudspeakers, the first playing a sound with power P1, and another playing a louder

version of the same sound with power P2, but

everything else (how far away, frequency) kept the same.

The difference in decibels between the two is defined to be

10 log (P2/P1) dB       

where the log is to base 10.

?

Page 29: Lecture 17 October 29, 2004. On Wednesday - Thumping

What the **#& is a logarithm?

Bindell’s definition:

Take a big number … like 23094800394

Round it to one digit: 20000000000Count the number of zeros … 10The log of this number is about equal to the number of zeros … 10.Actual answer is 10.3Good enough for us!

Page 30: Lecture 17 October 29, 2004. On Wednesday - Thumping

Back to the definition of dB:

The dB is proportional to the LOG10 of a ratio of intensities.Let’s take P1=Threshold Level of Hearing which is 10-12 watts/m2

Take P2=P=The power level we are interested in.

10 log (P2/P1)

Page 31: Lecture 17 October 29, 2004. On Wednesday - Thumping

An example:

The threshold of pain is 1 w/m2

1201210)10log(1010

1log 10

:PAIN of thresholdfor the rating dB

1212-

Page 32: Lecture 17 October 29, 2004. On Wednesday - Thumping

Take another look.

Page 33: Lecture 17 October 29, 2004. On Wednesday - Thumping
Page 34: Lecture 17 October 29, 2004. On Wednesday - Thumping

The sensitivity range for human hearing depends on the loudness and pitch. Noises along each black line would be heard with the same volume.

Page 35: Lecture 17 October 29, 2004. On Wednesday - Thumping