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Physics of the Blues: Music, Fourier and the Wave-Particle Duality J. Murray Gibson Presented at Fermilab October 15 th 2003
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Physics of the Blues: Music, Fourier and the Wave- Particle Duality J. Murray Gibson Presented at Fermilab October 15 th 2003.

Dec 14, 2015

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Page 1: Physics of the Blues: Music, Fourier and the Wave- Particle Duality J. Murray Gibson Presented at Fermilab October 15 th 2003.

Physics of the Blues:Music, Fourier and the Wave-

Particle DualityJ. Murray Gibson

Presented at Fermilab

October 15th 2003

Page 2: Physics of the Blues: Music, Fourier and the Wave- Particle Duality J. Murray Gibson Presented at Fermilab October 15 th 2003.

The Advanced Photon Source

Page 3: Physics of the Blues: Music, Fourier and the Wave- Particle Duality J. Murray Gibson Presented at Fermilab October 15 th 2003.

Art and Science

• Art and science are intimately connected

• Art is a tool for communication between scientists and laypersons

Page 4: Physics of the Blues: Music, Fourier and the Wave- Particle Duality J. Murray Gibson Presented at Fermilab October 15 th 2003.

The Poetry of Mathematics

02

Page 5: Physics of the Blues: Music, Fourier and the Wave- Particle Duality J. Murray Gibson Presented at Fermilab October 15 th 2003.

Music is excellent example…

Page 6: Physics of the Blues: Music, Fourier and the Wave- Particle Duality J. Murray Gibson Presented at Fermilab October 15 th 2003.

Outline:

• What determines the frequency of notes on a musical scale?

• What is harmony and why would fourier care? • Where did the blues come from?

   (We' re talking the "physics of the blues", and not "the blues of physics"  - that's another colloquium).

• Rules (axioms) and ambiguity fuel creativity • Music can explain physical phenomena

– Is there a musical particle? (quantum mechanics)– The importance of phase in imaging?

Page 7: Physics of the Blues: Music, Fourier and the Wave- Particle Duality J. Murray Gibson Presented at Fermilab October 15 th 2003.

Overtones of a string

Fourier analysis – all shapes of a string are a sum of harmonics

)/cos()( Lnxcxfn

n

Harmonic content describes difference between instrumentse.g. organ pipes have only odd harmonics..

Page 8: Physics of the Blues: Music, Fourier and the Wave- Particle Duality J. Murray Gibson Presented at Fermilab October 15 th 2003.

Spatial Harmonics

• Crystals are spatially periodic structures which exhibit integral harmonics– X-ray diffraction reveals

amplitudes which gives structure inside unit cell

• Unit-cell contents?(or instrument timbre?)

T. A. Steitz, et al., Yale University50S Ribosomal Subunit

Structural Biology Center 19ID

A portion of a diffraction pattern obtained at the Structural Biology Center 19ID beamline fromcrystals of the 50S ribosomal subunit Ń orthorhombic space group C222 1, a = 212 , b = 301 ,c = 576 Ń showing the spatial resolution of the measurement.(Courtesy of Dr. T. Steitz, Yale University)

Page 9: Physics of the Blues: Music, Fourier and the Wave- Particle Duality J. Murray Gibson Presented at Fermilab October 15 th 2003.

Semiconductor Bandgaps…

• Standing waves in a periodic lattice (Bloch Waves) – the phase affects energy and leads to a bandgap

Page 10: Physics of the Blues: Music, Fourier and the Wave- Particle Duality J. Murray Gibson Presented at Fermilab October 15 th 2003.

Familiarity with the Keyboard

C D E GA FB

1 step = semitone2 steps = whole tone

C D E F G A

Page 11: Physics of the Blues: Music, Fourier and the Wave- Particle Duality J. Murray Gibson Presented at Fermilab October 15 th 2003.

How to make a scale using notes with overlapping harmonics

2 3 4 51 6 7 8

Pythagoras came up with this….

Concept of intervals – two notes sounded simultaneouslywhich sound good together

Left brain meets the right brain…

C

G3/2

E5/4

Bflat7/4

Page 12: Physics of the Blues: Music, Fourier and the Wave- Particle Duality J. Murray Gibson Presented at Fermilab October 15 th 2003.

The pentatonic scale

C D E G A

1 5/4 3/29/8 27/16

* * * * *

Common to many civilizations (independent experiments?)

Page 13: Physics of the Blues: Music, Fourier and the Wave- Particle Duality J. Murray Gibson Presented at Fermilab October 15 th 2003.

Intervals

• Unison (“first”)• Second• Third• Fourth• Fifth• Sixth• Seventh• Octave (“eighth”)

Major, minor, perfect, diminished..

Two notesplayed simultaneously

Not all intervals are HARMONIC(although as time goes by there are more..Harmony is a learned skill, as Beethovendiscovered when he was booed)

Page 14: Physics of the Blues: Music, Fourier and the Wave- Particle Duality J. Murray Gibson Presented at Fermilab October 15 th 2003.

Natural Scale Ratios

IntervalRatio to Fundamental

in Just ScaleFrequency of Upper Note

based on C (Hz)

(C-C) Unison 1.0000 261.63

Minor Second 25/24 = 1.0417 272.54

(C-D) Major Second 9/8 = 1.1250 294.33

Minor Third 6/5 = 1.2000 313.96

(C-E) Major Third 5/4 = 1.2500 327.04

(C-F) Fourth 4/3 = 1.3333 348.83

Diminished Fifth 45/32 = 1.4063 367.93

(C-G) Fifth 3/2 = 1.5000 392.45

Minor Sixth 8/5 = 1.6000 418.61

(C-A) Major Sixth 5/3 = 1.6667 436.06

Minor Seventh 9/5 = 1.8000 470.93

(C- B) Major Seventh 15/8 = 1.8750 490.56

(C-C’) Octave 2.0000 523.26

Page 15: Physics of the Blues: Music, Fourier and the Wave- Particle Duality J. Murray Gibson Presented at Fermilab October 15 th 2003.

Diatonic Scale

C D E G AF B C

Doh, Re, Mi, Fa, So, La, Ti, Doh….

“Tonic” is C here

Page 16: Physics of the Blues: Music, Fourier and the Wave- Particle Duality J. Murray Gibson Presented at Fermilab October 15 th 2003.

Simple harmony

• Intervals– “perfect” fifth– major third– minor third– the harmonic triads – basis of western music

until the romantic era• And the basis of the blues, folk music etc.

The chords are based on harmonic overlapminimum of three notes to a chord(to notes = ambiguity which is widely played e.g. by Bach)

Page 17: Physics of the Blues: Music, Fourier and the Wave- Particle Duality J. Murray Gibson Presented at Fermilab October 15 th 2003.

The triads in the key of CC E G M3 P5 C Major Triad

D F A m3 P5 D Minor Triad

E G B m3 P5 E Minor Triad

F A G M3 P5 F Major Triad

G B D M3 P5 G Major Triad

A C E m3 P5 A Minor Triad

B D F m3 d5 B Diminished Triad

Page 18: Physics of the Blues: Music, Fourier and the Wave- Particle Duality J. Murray Gibson Presented at Fermilab October 15 th 2003.

Three chords and you’re a hit!

• A lot of folk music, blues etc relies on chords C, F and G

Page 19: Physics of the Blues: Music, Fourier and the Wave- Particle Duality J. Murray Gibson Presented at Fermilab October 15 th 2003.

Baroque Music

Based only on diatonic chords in one key (D in this case)

Page 20: Physics of the Blues: Music, Fourier and the Wave- Particle Duality J. Murray Gibson Presented at Fermilab October 15 th 2003.

Equal temperament scale

(Middle C) C4 261.63 0

C#4/D

b4 277.18 4.64

D4 293.66 -0.67

D#4/E

b4 311.13 -2.83

E4 329.63 2.59

F4 349.23 0.4

F#4/G

b4 369.99 2.06

G4 392.00 -0.45

G#4/A

b4 415.30 -3.31

(Concert A) A4 440.00 3.94

A#4/B

b4 466.16 -4.77

B4 493.88 3.32

C5 523.25 0

Frequency (Hz)

Step (semitone) = 2^1/12

Pianoforteneedsmultiplestrings to hidebeats!

Difference from Just Scale (Hz)Note

Page 21: Physics of the Blues: Music, Fourier and the Wave- Particle Duality J. Murray Gibson Presented at Fermilab October 15 th 2003.

The Well-Tempered Clavier

1 2 3

45 6

Page 22: Physics of the Blues: Music, Fourier and the Wave- Particle Duality J. Murray Gibson Presented at Fermilab October 15 th 2003.

Mostly Mozart

From his Sonata in A Major

Page 23: Physics of the Blues: Music, Fourier and the Wave- Particle Duality J. Murray Gibson Presented at Fermilab October 15 th 2003.

D dimc.f. D min

Page 24: Physics of the Blues: Music, Fourier and the Wave- Particle Duality J. Murray Gibson Presented at Fermilab October 15 th 2003.

Minor and Major

Page 25: Physics of the Blues: Music, Fourier and the Wave- Particle Duality J. Murray Gibson Presented at Fermilab October 15 th 2003.
Page 26: Physics of the Blues: Music, Fourier and the Wave- Particle Duality J. Murray Gibson Presented at Fermilab October 15 th 2003.

The “Dominant 7th”

• The major triad PLUS the minor 7th interval• E.g. B flat added to C-E-G (in the key of F)• B flat is very close to the harmonic 7/4

– Exact frequency 457.85 Hz,– B flat is 466.16 Hz– B is 493.88 Hz– Desperately wants to resolve to the tonic (F)

B flat is notin the diatonic scale for C, but it is for F Also heading for the “blues”

Page 27: Physics of the Blues: Music, Fourier and the Wave- Particle Duality J. Murray Gibson Presented at Fermilab October 15 th 2003.

Circle of Fifths

• Allows modulation and harmonic richness– Needs equal

temperament– “The Well Tempered

Clavier”– Allows harmonic

richness

Page 28: Physics of the Blues: Music, Fourier and the Wave- Particle Duality J. Murray Gibson Presented at Fermilab October 15 th 2003.
Page 29: Physics of the Blues: Music, Fourier and the Wave- Particle Duality J. Murray Gibson Presented at Fermilab October 15 th 2003.

Diminished Chords

• A sound which is unusual– All intervals the same i.e. minor 3rds, 3 semitones (just scale

ratio 6/5, equal temp -1%)– The diminished chord has no root

• Ambiguous and intriguing

• An ability of modulate into new keys not limited by circle of fifths– And add chromatic notes– The Romantic Period was lubricated by diminished chords

C diminished

Page 30: Physics of the Blues: Music, Fourier and the Wave- Particle Duality J. Murray Gibson Presented at Fermilab October 15 th 2003.

Romantic music..A flat diminished (c.f. B flat dominant 7th)

C diminished (Fdominant 7th)

1 2

3 4 5

Page 31: Physics of the Blues: Music, Fourier and the Wave- Particle Duality J. Murray Gibson Presented at Fermilab October 15 th 2003.

Beethoven’s “Moonlight” Sonata in C# Minor

F# dim

F# (or C) dim

1

5

9

13

Page 32: Physics of the Blues: Music, Fourier and the Wave- Particle Duality J. Murray Gibson Presented at Fermilab October 15 th 2003.

“Blue” notes

• Middle C = 261.83 Hz • E flat = 311.13Hz• Blue note = perfect harmony = 5/4 middle C =

327.29 Hz – slightly flatter than E• E = 329.63 Hz

• Can be played on wind instruments, or bent on a guitar or violin. “Crushed” on a piano

• 12 Bar Blues - C F7 C C F7 F7 C C G7 F7 C C

Page 33: Physics of the Blues: Music, Fourier and the Wave- Particle Duality J. Murray Gibson Presented at Fermilab October 15 th 2003.

Crushed notes and the blues

Page 34: Physics of the Blues: Music, Fourier and the Wave- Particle Duality J. Murray Gibson Presented at Fermilab October 15 th 2003.

Not quite ready for the blues

Page 35: Physics of the Blues: Music, Fourier and the Wave- Particle Duality J. Murray Gibson Presented at Fermilab October 15 th 2003.

Four-tone chords

• Minimum for Jazz and Contemporary Music

And more: 9th, 11th s and 13th s (5,6 and 7note chords)

Page 36: Physics of the Blues: Music, Fourier and the Wave- Particle Duality J. Murray Gibson Presented at Fermilab October 15 th 2003.

Ambiguities and Axioms

• Sophisticated harmonic rules play on variation and ambiguity

• Once people learn them they enjoy the ambiguity and resolution

• Every now and then we need new rules to keep us excited (even though we resist!)

Page 37: Physics of the Blues: Music, Fourier and the Wave- Particle Duality J. Murray Gibson Presented at Fermilab October 15 th 2003.

Using Music to Explain Physics

• Quantum Mechanics– general teaching

• Imaging and Phase– phase retrieval is important in lensless

imaging, e.g. 4th generation x-ray lasers

Page 38: Physics of the Blues: Music, Fourier and the Wave- Particle Duality J. Murray Gibson Presented at Fermilab October 15 th 2003.

The Wave-particle Duality

• Can be expressed as fourier uncertainty relationship

f T ~ 2

Demonstrated by musical notes of varying duration (demonstrated with Mathematica or synthesizer)Wave-nature melodyParticle-nature percussive aspect

T

2/f

Page 39: Physics of the Blues: Music, Fourier and the Wave- Particle Duality J. Murray Gibson Presented at Fermilab October 15 th 2003.

Ants Pant!

QuickTime™ and aCinepak decompressor

are needed to see this picture.

Phase-enhanced imaging

Westneat, Lee et. al..

Page 40: Physics of the Blues: Music, Fourier and the Wave- Particle Duality J. Murray Gibson Presented at Fermilab October 15 th 2003.

Phase Contrast and Phase Retrieval

• Much interest in reconstructing objects from diffraction patterns– “lensless” microscopy ios being developed

with x-ray and electron scattering

• Warning, for non-periodic objects, phase, not amplitude, is most important…..

Page 41: Physics of the Blues: Music, Fourier and the Wave- Particle Duality J. Murray Gibson Presented at Fermilab October 15 th 2003.

Fun with phases…

Helen Gibson Margaret Gibson

Page 42: Physics of the Blues: Music, Fourier and the Wave- Particle Duality J. Murray Gibson Presented at Fermilab October 15 th 2003.

Fourier TransformsHelen Marge

Amp

Phase

Page 43: Physics of the Blues: Music, Fourier and the Wave- Particle Duality J. Murray Gibson Presented at Fermilab October 15 th 2003.

Swap phasesHelen with Marge’s phases Marge with Helen’s phases

Phases contain most of the information… (especially when no symmetry)

Page 44: Physics of the Blues: Music, Fourier and the Wave- Particle Duality J. Murray Gibson Presented at Fermilab October 15 th 2003.

Sound Examples

Clapton Beethoven

Clapton with Beethoven’s phases Beethoven with Clapton’s Phases

Page 45: Physics of the Blues: Music, Fourier and the Wave- Particle Duality J. Murray Gibson Presented at Fermilab October 15 th 2003.

Conclusion

• Music and physics and mathematics have much in common

• Not just acoustics– Musician’s palette based on physics– Consonance and dissonance

• Both involved in pleasure of music

• Right and left brain connected?– Is aesthetics based on quantitative analysis?

• Music is great for illustrating physical principles