lecture set 07 october 4, 2004 the physics of sounds from strings

35
Lecture Set 07 Lecture Set 07 October 4, 2004 October 4, 2004 The physics of sounds from The physics of sounds from strings. strings.

Upload: dominic-bates

Post on 04-Jan-2016

214 views

Category:

Documents


2 download

TRANSCRIPT

Page 1: Lecture Set 07 October 4, 2004 The physics of sounds from strings

Lecture Set 07Lecture Set 07

October 4, 2004October 4, 2004

The physics of sounds from strings.The physics of sounds from strings.

Page 2: Lecture Set 07 October 4, 2004 The physics of sounds from strings

Things to NoteThings to Note

• All lectures are currently posted on the website.– The solution to the exam is also posted on the

website.

• Some of the files are rather long.– I cut some of the lectures into two or three

parts to keel them small but some are still pretty big because of the photographs.

– Today, we continue with sounds from strings.

Page 3: Lecture Set 07 October 4, 2004 The physics of sounds from strings

Last timeLast time• We listened to the sound generated by a

single stretched string.

• We noted:– The longer the string, the “lower” the tone.– The shorter the string, the “higher” the tone.– The more tension on the string, the “higher”

the tone.

Page 4: Lecture Set 07 October 4, 2004 The physics of sounds from strings

An Interesting observationAn Interesting observation• When the string is reduced to half, it

produces a tone related to the original tone.

• The new tone is said to be an OCTAVE higher than the original.– The textbook calls this interval a “diapason”

which in Greek means “through all”.– I am stubborn and will call it an octave

anyway.

Page 5: Lecture Set 07 October 4, 2004 The physics of sounds from strings

What are we doing?

Open string

Half length

D

D’

PLAY THEM TOGETHER AND THEY SOUND REALLY GOOD.PLAY THEM TOGETHER AND THEY SOUND REALLY GOOD.

Page 6: Lecture Set 07 October 4, 2004 The physics of sounds from strings

What do we have so far??

D D D D D DL/4 L/2 L L/2 L/4 L/8

‘’D ‘D D D’ D’’ D’’’

Page 7: Lecture Set 07 October 4, 2004 The physics of sounds from strings

So, they looked at another “simple” numerical division

DDL/3

NEW INTERVAL – THE FIFTH Length = 2/3 L

Also a fifthLength = 1/3

OCTAVE

A A

Page 8: Lecture Set 07 October 4, 2004 The physics of sounds from strings

Observation

The FIFTH sounds good when played with the original tone.

Bass and tenors singing together will tend to sing a fifth apart.

Recall that men and women, singing the “same tone” together, tend to sing an OCTAVE apart.

Our scale now has “two” notes. A little shabby!

Page 9: Lecture Set 07 October 4, 2004 The physics of sounds from strings

Differences/Intervals

The octave and the fifth represent an interval, or a “difference” between two reasonable consonant tones. Interval is D E F G A B C D E F G A ….= FIFTH

New IntervalThe FOURTH

Page 10: Lecture Set 07 October 4, 2004 The physics of sounds from strings

The fourth

A D A

fourth

octive

3

4

(1/2)L

(2/3)L RatiosLength

2

1

L/2

L RatiosLength

Page 11: Lecture Set 07 October 4, 2004 The physics of sounds from strings

These “Special” Ratios

All of these intervals sounded good to the ear.

The lengths corresponding to intervals that sounded good were found to have ratios expressible as small integers.

How perfect! God-like! MUST be true. The process can be continued to define

additional intervals.

Page 12: Lecture Set 07 October 4, 2004 The physics of sounds from strings

The Pythagorean Musical Scale .. Developed by rules

The Pythagoreans believed that the laws of physics could be revealed NOT by observation but by pure thought.

So they thought about the results that we just mentioned and came up with the “rule” to form the various intervals of the scale.

Page 13: Lecture Set 07 October 4, 2004 The physics of sounds from strings

The “RULE”

Take an existing ratio (lengths) and multiply or divide it by 3/2.

If the number that you get is greater than 2, then halve it.

If the number is less than 1, double it.

EXAMPLE : 1 x 2/3 produces the fifth.

NEXT: 1 x 3/2 = 3/2 .. Divide by 2 … = 3/4 = fourth

Page 14: Lecture Set 07 October 4, 2004 The physics of sounds from strings

The rule basically raises or lowers a tone by a fifth

and then divides or multiplies by two to keep it in the

proper range.

Page 15: Lecture Set 07 October 4, 2004 The physics of sounds from strings

So …

Page 16: Lecture Set 07 October 4, 2004 The physics of sounds from strings

Then … The Pentatonic Scale

Page 17: Lecture Set 07 October 4, 2004 The physics of sounds from strings

The septatonic scaleseptatonic scale (Our Own but starting with Re instead of Do)

Page 18: Lecture Set 07 October 4, 2004 The physics of sounds from strings

By the way … we are cheating!

16th century

Page 19: Lecture Set 07 October 4, 2004 The physics of sounds from strings

A 2000 year problem

SAME RATIOS!!!

Page 20: Lecture Set 07 October 4, 2004 The physics of sounds from strings

The Music of the Spheres

Page 21: Lecture Set 07 October 4, 2004 The physics of sounds from strings

The Music of the Spheres

Page 22: Lecture Set 07 October 4, 2004 The physics of sounds from strings

KeplerLike Plato and Pythagoras, Kepler believed that the world was ruled by number. He tried hard to prove that the distances of the planets from the sun were given by an arrangement of Eucid's five regular solids; by doing so, he believed, he could demonstrate something of the order of the mind of God. But his faith in number went further: he believed that musical harmony, mathematically expressed, and the harmony of the spheres were one thing: 'I affirm and demonstrate that the movements (of the planets) are modulated according to harmonic proportions’.

Page 23: Lecture Set 07 October 4, 2004 The physics of sounds from strings

Let’s talk some physics here.

Page 24: Lecture Set 07 October 4, 2004 The physics of sounds from strings

What is observed

The string moves back and forth. It sets the air into some kind of motion. The air motion (we presume pressure) strikes

the ear and produces what we hear as sound. WE DO NOT YET KNOW THE DIFFERENCE

BETWEEN THE VARIOUS TONES OF THE SCALE IN TERMS OF WHAT IT IS THAT TRAVELS THROUGH THE AIR..

Page 25: Lecture Set 07 October 4, 2004 The physics of sounds from strings

Enter Helmholtz ~1885

Siren

Air Stream

Page 26: Lecture Set 07 October 4, 2004 The physics of sounds from strings

FREQUENCY f

second

events"" ofnumber f

Page 27: Lecture Set 07 October 4, 2004 The physics of sounds from strings

Example

Suppose something has a frequency of 60 cycles per second.

One cycle per second is defined as the Hertz. So we have 60 hertz. In one second there are 60 events. Therefore ONE event takes 1/60th of a

second. That is defined as the PERIOD = T

Page 28: Lecture Set 07 October 4, 2004 The physics of sounds from strings

Definition:

1

1

1

fT

fT

frequencyPeriod

Page 29: Lecture Set 07 October 4, 2004 The physics of sounds from strings

The Helmholtz Resonator

Page 30: Lecture Set 07 October 4, 2004 The physics of sounds from strings

A set of resonators

Page 31: Lecture Set 07 October 4, 2004 The physics of sounds from strings

The Epiphany

“RESONANCE” TAKES PLACE ONLYWITH THE CORRECT HELMHOLTZRESONATOR.

SOUND HAS A FREQUENCY!

BUT HOW DOES IT MOVE TO US??

Page 32: Lecture Set 07 October 4, 2004 The physics of sounds from strings

Waves

Page 33: Lecture Set 07 October 4, 2004 The physics of sounds from strings

But What’s Moving??

Page 34: Lecture Set 07 October 4, 2004 The physics of sounds from strings
Page 35: Lecture Set 07 October 4, 2004 The physics of sounds from strings