Can one hear the shape of Information? Copyright 2014 by Evans M. Harrell II. Evans Harrell Georgia Tech www.math.gatech.edu/~harrell November, 2014.

Slides:



Advertisements
Similar presentations
Introduction to Sequences. The Real Number System/Sequences of Real Numbers/Introduction to Sequences by Mika Seppälä Sequences Definition A sequence.
Advertisements

Lecture 7: Basis Functions & Fourier Series
 Making Sound Waves:  A sound wave begins with a vibration.  How Sound Travels:  Like other mechanical waves, sound waves carry energy through a medium.
Chapter 13 Partial differential equations
Characterizing Non- Gaussianities or How to tell a Dog from an Elephant Jesús Pando DePaul University.
Lecture 8 Fourier Series applied to pulses Remember homework 1 for submission 31/10/08 Remember Phils Problems.
Fourier Series Eng. Ahmed H. Abo absa. Slide number 2 Fourier Series & The Fourier Transform Fourier Series & The Fourier Transform What is the Fourier.
Fourier Transform – Chapter 13. Image space Cameras (regardless of wave lengths) create images in the spatial domain Pixels represent features (intensity,
Synthesis. What is synthesis? Broad definition: the combining of separate elements or substances to form a coherent whole. (
Harmonic Series and Spectrograms 220 Hz (A3) Why do they sound different? Instrument 1 Instrument 2Sine Wave.
The frequency spectrum
Boyce/DiPrima 10th ed, Ch 10.1: Two-Point Boundary Value Problems Elementary Differential Equations and Boundary Value Problems, 10th edition, by William.
Quantum One: Lecture 3. Implications of Schrödinger's Wave Mechanics for Conservative Systems.
7/5/20141FCI. Prof. Nabila M. Hassan Faculty of Computer and Information Fayoum University 2013/2014 7/5/20142FCI.
Boyce/DiPrima 9th ed, Ch 11.2: Sturm-Liouville Boundary Value Problems Elementary Differential Equations and Boundary Value Problems, 9th edition, by.
Ch 9 pages ; Lecture 21 – Schrodinger’s equation.
Differential Equations Brannan Copyright © 2010 by John Wiley & Sons, Inc. All rights reserved. Chapter 10: Boundary Value Problems and Sturm– Liouville.
Differential Equations
Preview of Calculus.
Principal Component Analysis Adapted by Paul Anderson from Tutorial by Doug Raiford.
Wei Wang Xi’an Jiaotong University Generalized Spectral Characterization of Graphs: Revisited Shanghai Conference on Algebraic Combinatorics (SCAC), Shanghai,
UNIVERSAL FUNCTIONS A Construction Using Fourier Approximations.
Harmonic Series and Spectrograms
The extreme sport of eigenvalue hunting. Evans Harrell Georgia Tech Research Horizons Georgia Tech 1 March 2006.
FOURIER SERIES §Jean-Baptiste Fourier (France, ) proved that almost any period function can be represented as the sum of sinusoids with integrally.
The Discrete Fourier Transform. The Fourier Transform “The Fourier transform is a mathematical operation with many applications in physics and engineering.
The Story of Wavelets.
Lecture 2 Signals and Systems (I)
Harmonics November 1, 2010 What’s next? We’re halfway through grading the mid-terms. For the next two weeks: more acoustics It’s going to get worse before.
Lecture 16 Solving the Laplace equation in 2-D Remember Phils Problems and your notes = everything Only 6 lectures.
Lecture 9 Fourier Transforms Remember homework 1 for submission 31/10/08 Remember Phils Problems and your notes.
Quantum One: Lecture Representation Independent Properties of Linear Operators 3.
Fourier Series. Introduction Decompose a periodic input signal into primitive periodic components. A periodic sequence T2T3T t f(t)f(t)
Lecture 20 Spherical Harmonics – not examined
Fourier series: Eigenfunction Approach
CIS 350 – 4 The FREQUENCY Domain Dr. Rolf Lakaemper.
MODULE 1 In classical mechanics we define a STATE as “The specification of the position and velocity of all the particles present, at some time, and the.
Periodic driving forces
Part 4 Chapter 16 Fourier Analysis PowerPoints organized by Prof. Steve Chapra, University All images copyright © The McGraw-Hill Companies, Inc. Permission.
Hearing: Physiology and Psychoacoustics 9. The Function of Hearing The basics Nature of sound Anatomy and physiology of the auditory system How we perceive.
Loudness level (phon) An equal-loudness contour is a measure of sound pressure (dB SPL), over the frequency spectrum, for which a listener perceives a.
Harmonic Series and Spectrograms BY JORDAN KEARNS (W&L ‘14) & JON ERICKSON (STILL HERE )
The Mathematics of Sound. Professor Cross’s laser and video displays came out of a desire to visualize sound. Sound, while itself a phenomenon experienced.
Can one hear the shape of Information? Copyright 2014, 2015 by Evans M. Harrell II. Evans Harrell Georgia Tech October, 2015.
Copyright © Cengage Learning. All rights reserved.
The Amazing Fourier Transorm! Joseph Fourier
Boundary-Value Problems in Rectangular Coordinates
Recording Arts…Audio Sound Waves Fall What does this all mean to you in this class? You are always working with sound waves – it is important to.
3.3 Waves and Stuff Science of Music 2007 Last Time  Dr. Koons talked about consonance and beats.  Let’s take a quick look & listen at what this means.
Frequency domain analysis and Fourier Transform
Professor Brendan Morris, SEB 3216, EE360: Signals and System I Fourier Series Motivation.
The inference and accuracy We learned how to estimate the probability that the percentage of some subjects in the sample would be in a given interval by.
The Frequency Domain Digital Image Processing – Chapter 8.
Intro to Fourier Series BY JORDAN KEARNS (W&L ‘14) & JON ERICKSON (STILL HERE )
Ch. 12 Partial Differential Equations
Introduction and motivation Full range Fourier series Completeness and convergence theorems Fourier series of odd and even functions Arbitrary range Fourier.
Musical Instruments. Notes  Different musical notes correspond to different frequencies  The equally tempered scaled is set up off of 440 A  meaning.
Fourier Analysis Patrice Koehl Department of Biological Sciences National University of Singapore
Loudness level (phon) An equal-loudness contour is a measure of sound pressure (dB SPL), over the frequency spectrum, for which a listener perceives a.
FOURIER THEORY: KEY CONCEPTS IN 2D & 3D
Loudness level (phon) An equal-loudness contour is a measure of sound pressure (dB SPL), over the frequency spectrum, for which a listener perceives a.
How Many Ways Can 945 Be Written as the Difference of Squares?
Loudness level (phon) An equal-loudness contour is a measure of sound pressure (dB SPL), over the frequency spectrum, for which a listener perceives a.
UNIT II Analysis of Continuous Time signal
EE360: Signals and System I
Intro to Fourier Series
C-15 Sound Physics 1.
Quantum One.
Sound Waves and Beats with Vernier Sensors
Copyright © 2017, 2013, 2009 Pearson Education, Inc.
Presentation transcript:

Can one hear the shape of Information? Copyright 2014 by Evans M. Harrell II. Evans Harrell Georgia Tech November, 2014

What is the mathematics behind the ear's ability to pick information out of a sound signal? What sort of information do we pick out when we listen to music? "Sonification" is the name for a current method in data science that involves turning data into sound and using the human ear to detect patterns. As we'll see, patterns are extracted from a signal through Fourier series and the Fourier transform, which I'll introduce. In order to answer the question of what kind of information we pick out, I'll discuss how the shape of an object and the sounds it makes are connected, in terms of the wave equation and associated eigenvalues. Then I'll discuss some recent research where information is instead encoded in a graph (network) and we use eigenvalues to detect some of of its features. Can one hear the shape of Information?

An insight of Joseph Fourier

 Or, as usual, maybe of Leonhard Euler before him: “Any” sound is a superposition of pure frequencies.

An insight of Joseph Fourier  Or, as usual, maybe of Euler before him: “Any” sound is a superposition of pure frequencies.  Your inner ear turns out to be an instrument capable of breaking sounds into pure frequencies, multiples of cos(  t -  ) or exp(i(  t))

Fourier series and integrals  If a signal (function) is periodic, f(t) = f(t+p), it is a sum of sine functions:

Fourier series and integrals  An arbitrary signal (say, square- integrable) is still an integral:

Fourier series and integrals  Moreover, given the signal, the formula for the coefficients is remarkably simple:

A recent trend in “data mining”  Turn it into music and listen. You could hear about “sonification,” example in a BBC report. BBC report

A recent trend in “data mining”  Anyway, it is easy, because the graph of any function can equally well be interpreted visually on Cartesian axes or as a sound wave.

A recent trend in “data mining”  Anyway, it is easy, because the graph of any function can equally well be interpreted visually on Cartesian axes or as a sound wave.  In Mathematica, there are two parallel commands:

Examples of sonification  Cosmic microwave background Cosmic microwave background  Galaxy spectra Galaxy spectra  Higgs boson Higgs boson  Tohoku earthquake Tohoku earthquake  (compare to:Japanese drumming)Japanese drumming  Financial market data (more randomness) Financial market data

A recent trend in “data mining”  Turn it into music and listen.  First Life - Translating Scientific Data Into Music, a collaboration of Steve Everett, Professor of Music at Emory and Martha Grover, Chemical & Biomolecular Engineering at Georgia Tech. (Sept. 2013, at the Atlanta Botanical Garden.)  Molecular music. (March, 2014, Atlanta Science Festival.)  European Science Café Atlanta

A recent trend in “data mining”

How are sounds produced?  Until now we have touched on how to take a sound apart into its frequencies.  Another question is: How can we put a sound together? What kinds of sounds does an object make?

Shapes of musical instruments  Instruments that produce sustained sound (i.e., not percussion) are almost all roughly one-dimensional in some way. Either they use strings or they have one dimension that is much more extended than the others. Why?

How are sounds produced?  When an object vibrates, it satisfies the wave equation u tt = c 2  u along with any “boundary conditions.” Here  designates the Laplace operator.

How are sounds produced?  If the solution is a “normal mode” of the form cos(  t) u(x), then the spatial factor must be an eigenfunction of the Laplace operator: -  u = k 2 u and the (angular) frequencies are related to the “eigenvalues” by k =  /c

What do eigenvalues tell us about shapes?  Mark Kac, Can one hear the shape of a drum?, Amer. Math. Monthly, 1966.

What do eigenvalues tell us about shapes?  Mark Kac, Can one hear the shape of a drum?, Amer. Math. Monthly,  Already in 1946, G. Borg considered whether you could hear the density of a guitar string, but he failed to think of such a colorful title.

What do eigenvalues tell us about shapes?  Mark Kac, Can one hear the shape of a drum?, Amer. Math. Monthly,  Besides, the answer is now known to be “no.” However, there are some facts about the shape we can hear, because the statistical distribution of eigenvalues satisfies many conditions in which volume, surface area, and other properties appear.

So, can one hear the shape of a drum? Gordon, Webb, and Wolpert, 1991

Depending on your beliefs…  You could say that animals like you are either evolved or designed to pick out statistical relations among frequencies (eigenvalues), so that your hearing helps you make sense of your environment.

Depending on your beliefs…  You could say that animals like you are either evolved or designed to pick out statistical relations among frequencies (eigenvalues), so that your hearing helps you make sense of your environment.  The fact that the underlying mathematical formulae are simple made such abilities possible.

For instance,  One can hear the area of the drum from its high frequencies, by the Weyl asymptotics:  For large values of m, in dimension, k m ~ C (m/Vol(  )) 1/. (A mathematician ’ s drum can be - dimensional, and even be a curved manifold.)

For instance,  One can hear the area of the drum from its high frequencies, by the Weyl asymptotics:  For large values of m, in dimension, k m ~ C (m/Vol(  )) 1/. In 1 dimension, the ratios of these numbers are rational, but not in any other dimension.

Shapes of musical instruments  If the part of a musical instrumental that produces vibrations is basically one-dimensional, then it will tend to have harmonic overtones. (The three- dimensionality only kicks in for much higher frequencies than you can hear.)

Wave forms of a vibrating string

Shapes of musical instruments  Percussion instruments tend to have two and three-dimensional structures, but they are less used for sustained musical tones.

What about network data, as encoded in a combinatorial graph?

Let the graph vibrate, and listen to it! The discrete version of the Laplace operator is a certain n  n matrix, where n is the number of vertices. Its eigenvalues are the squares of the frequencies of normal modes.

Let the graph vibrate, and listen to it! There are actually different ways to set up the discrete Laplacian, but in any version, the frequencies do not always determine the graph. Example of Steve Butler, Iowa State, for the “normalized Laplacian” and adjacency matrix. Mouse and fish for the standard Laplacian.

One can “hear” the number of edges, the number of triangles, and some other facts about connectedness: Some special graphs (cycle, complete, etc.) have unique spectra (= sets of eigenvalues). One can also easily hear whether a graph is bipartite (= needs only 2 colors).

One can “hear” the number of edges, the number of triangles, and some other facts about connectedness:

Let the graph vibrate, and listen to it! Nobody completely understands what sets of frequencies are possible for graphs, but there are regularities. Yay! Open problems and conjectures!

Dimension and complexity  A two-dimensional image can be complicated, but, as Descartes emphasized, each point in the image can be located by asking only two questions.  In this way, dimension is a measure of complexity: How many questions do you need to ask to understand the data?  Is this something one can hear?

Is dimension (complexity) something that one can hear? (See Mathematica notebook)

Dimension and complexity  A two-dimensional image can be complicated, but, as Descartes emphasized, each point in the image can be located by asking only two questions.  In this way, dimension is a measure of complexity. As we saw, one can hear the dimension of a vibrating object.

Dimension and complexity  A two-dimensional image can be complicated, but as Descartes emphasized, each point in the image can be located by asking only two questions.  In this way, dimension is a measure of complexity. As we saw, one can hear the dimension of a vibrating object.  What about a graph?

Dimension and complexity This is a randomly generated “graph” showing 520 connections among 100 items. How many independent kinds of information (“dimensions”) are there?

Dimension and complexity Some graphs, like regular lattices, have an obvious dimensionality. Z can be said to have dimension..

Dimension and complexity Harrell-Stubbe, Linear Algebra and Applications, 2014.

More exactly… Harrell-Stubbe, Linear Algebra and Applications, 2014.

A deeper look at the statistics of spectra:

This is a randomly generated “graph” showing 520 connections among 100 items. How many independent kinds of information (“dimensions”) are there? According to our theorem: It is only three-dimensional! The story of this graph can be understood in terms of three questions. Dimension and complexity

THE END