singularity theory and its applications dr cathy hobbs 30/01/09

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Singularity Theory and its Applications Dr Cathy Hobbs 30/01/09

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Page 1: Singularity Theory and its Applications Dr Cathy Hobbs 30/01/09

Singularity Theory and its Applications

Dr Cathy Hobbs30/01/09

Page 2: Singularity Theory and its Applications Dr Cathy Hobbs 30/01/09

Introduction: What is Singularity Theory?

Singularity Theory

Differential

geometryTopology

Page 3: Singularity Theory and its Applications Dr Cathy Hobbs 30/01/09

Singularity Theory

The study of critical points on manifolds (or of mappings) – points where the “derivative” is zero.

Developed from ‘Catastrophe Theory’ (1970’s).

Rigorous body of mathematics which enables us to study phenomena which re-occur in many situations

Page 4: Singularity Theory and its Applications Dr Cathy Hobbs 30/01/09

Singularity Theory

provides framework to classify critical points up to certain types of ‘natural’ equivalence

gives precise local models to describe types of behaviour

studies stability – what happens if we change our point of view a little?

Page 5: Singularity Theory and its Applications Dr Cathy Hobbs 30/01/09

Analogous example: Quadratic forms

2 2,F x y ax bxy cy

Quadratic forms in 2 variables can be classified:

Ellipse Parabola Hyperbola

2 2

2 21

x y

a b

2 2

2 21

x y

a b 2y ax

General form:

Page 6: Singularity Theory and its Applications Dr Cathy Hobbs 30/01/09

Morse Theory of Functions

Consider a smooth function .

If all partial derivatives are zero for a particular value x0 we say that y has a critical point at x0.

If the second differential at this point is a nondegenerate quadratic form then we call the point a non-degenerate critical point.

n R R

Page 7: Singularity Theory and its Applications Dr Cathy Hobbs 30/01/09

Morse Lemma

In a neighbourhood of a non-degenerate critical point a function may be reduced to its quadratic part, for a suitable choice of local co-ordinate system whose origin is at the critical point.

i.e. the function can be written as 2 2 2 2 21 2 1... ...k k ny x x x x x

Page 8: Singularity Theory and its Applications Dr Cathy Hobbs 30/01/09

Morse Lemma

Local theory – only valid in a neighbourhood of the point.

Explains ubiquity of quadratic forms.

Non-degenerate critical points are stable – all nearby functions have non-deg critical points of same type.

Page 9: Singularity Theory and its Applications Dr Cathy Hobbs 30/01/09

Splitting Lemma

Let be a smooth function with a degenerate critical point at the origin, whose Hessian matrix of second derivatives has rank r.

Then f is equivalent, around 0, to a function of the form

:R Rnf

2 21 1... ,...,r r nx x f x x

Inessential variablesEssential variables

Page 10: Singularity Theory and its Applications Dr Cathy Hobbs 30/01/09

Thom’s Classification

FoldCuspSwallowtailButterflyElliptic umbilicHyperbolic umbilicParabolic umbilic

31 1 1x a x M

4 21 1 1 2 1x a x a x M

5 3 21 1 1 2 1 3 1x a x a x a x M

6 4 3 21 1 1 2 1 3 1 4 1x a x a x a x a x M

3 2 2 21 1 2 1 1 2 2 1 3 23x x x a x x a x a x N

3 21 2 1 1 2 2 1 3 2x x a x x a x a x N

2 4 2 21 2 2 1 1 2 2 3 1 4 2x x x a x a x a x a x N

Page 11: Singularity Theory and its Applications Dr Cathy Hobbs 30/01/09

Singularities of Mappings

In many applications it is mappings that interest us, rather than functions.

For example, projecting a surface to a

plane is a mapping from 3-d to 2-d.

Page 12: Singularity Theory and its Applications Dr Cathy Hobbs 30/01/09

Singularities of Mappings

Can classify mappings from n-dim space to p-dim space for many (n,p) pairs (eg. n+p < 6).

Appropriate equivalence relations used eg diffeomorphisms.

Can list stable phenomena. Can investigate how unstable

phenomena break up as we perturb parameters.

Page 13: Singularity Theory and its Applications Dr Cathy Hobbs 30/01/09

Example: Whitney classification

Whitney classified stable mappings R2 to R3 (1955).

Immersion Fold Cusp

Page 14: Singularity Theory and its Applications Dr Cathy Hobbs 30/01/09

Applications: Robotics

Robotic motions are smooth maps from n-parameter space to 2 or 3 dimensional space.

Stewart-Gough platform Robot arm

Page 15: Singularity Theory and its Applications Dr Cathy Hobbs 30/01/09

Questions we might tackle:

What kinds of points might we see on the curve/surface traced out by a robotic motion?

Which points are stable, which are unstable (so likely to degenerate under small perturbance of the design)?

Page 16: Singularity Theory and its Applications Dr Cathy Hobbs 30/01/09

Eg. 4-bar mechanism

Used in many engineering applications.

Generally planar.

Page 17: Singularity Theory and its Applications Dr Cathy Hobbs 30/01/09

One parameter generates the motion.

There is a 2-parameter choice of coupler point.

Singularities from R to R2 have been classified.

The 2-dim choice of coupler point gives a codimension restriction to < 3.

Eg. 4-bar mechanism

Page 18: Singularity Theory and its Applications Dr Cathy Hobbs 30/01/09

Stable

Codimension 1

Codimension 2

Local models of coupler curves

All can be realised by a four-bar mechanism.

Page 19: Singularity Theory and its Applications Dr Cathy Hobbs 30/01/09

Other types of mechanism

Two-parameter planar motions – eg 5 bar planar linkage.

One-parameter spatial motions- eg 4 bar spatial linkage.

Two-parameter spatial motions

After this, classification gets complicated.

Page 20: Singularity Theory and its Applications Dr Cathy Hobbs 30/01/09

Applications: Vision

Think of viewing an object as a smooth mapping from a 3-d object to 2-d viewing plane.

Concentrate only on the outline of the object –points on surface where light rays coming from the eye graze it.

Page 21: Singularity Theory and its Applications Dr Cathy Hobbs 30/01/09

Examples of singularities on outlines

© Henry Moore

© Barbara Hepworth

Page 22: Singularity Theory and its Applications Dr Cathy Hobbs 30/01/09

Questions we might tackle:

What do smooth 3-d objects ‘look like’? i.e. what do their outlines look like locally?

What about non-smooth 3-d objects, eg those with corners, edges?

What are the effects of lighting on views, eg shadows, specular highlights?

What happens when motion occurs?

Page 23: Singularity Theory and its Applications Dr Cathy Hobbs 30/01/09

Some maths!

Think of a surface as the inverse image of a regular value of some smooth function.

Any smooth surface can be so described, and we can approximate actual expression with nice, smooth polynomial functions.

Page 24: Singularity Theory and its Applications Dr Cathy Hobbs 30/01/09

Expressing surface algebraically

Consider a smooth surface given by taking the inverse image of the value 0.

Choose co-ordinates so that the orthogonal projection onto the 2-d viewing plane is given by

Then F is given by 1

1 0, , , , ... ,n nn nF t x y a x y t a x y t a x y

, , ,t x y x y

Page 25: Singularity Theory and its Applications Dr Cathy Hobbs 30/01/09

Conditions for outline

Surface M is given by Suppose M goes through the origin,

i.e. Origin yields a point on the outline

exactly when and

1 0F

0 00F

000F

t

0 00F

Page 26: Singularity Theory and its Applications Dr Cathy Hobbs 30/01/09

Conditions for singularities on outline

If but

then t = 0 is a p-fold root of

In a neighbourhood of the origin we are able to rewrite our surface as

for some smooth functions .

1 2

1 2

0 0... 0 00 0

0

p p

p p

F FF

t t

00

p

p

F

t

0F t

11 0... 0w wp p

pt b t b

jb

Page 27: Singularity Theory and its Applications Dr Cathy Hobbs 30/01/09

Simplified local expression

Simplify by applying the Tschirnhaus transformation

Geometrically consists of sliding the surface up/down vertically – no change to outline.

Now local expression is

1

1wpt t b

p

12 0... 0w wp p

pt c t c

Page 28: Singularity Theory and its Applications Dr Cathy Hobbs 30/01/09

How large is p for a general surface?

We have a point of Multiplicity 1 if

Multiplicity 2 if

Multiplicity 3 if

Multiplicity > 3 if

0, 0F

Ft

2

20, 0

F FF

t t

2 3

2 30, 0

F F FF

t t t

2 3

2 30

F F FF

t t t

Page 29: Singularity Theory and its Applications Dr Cathy Hobbs 30/01/09

What does this look like?

Multiplicity 1: Diffeomorphism

Page 30: Singularity Theory and its Applications Dr Cathy Hobbs 30/01/09

What does this look like?

Multiplicity 2: Fold.

Write surface locally as

Outline is given by solvingi.e. x = 0

2 0t x

2 2 0t x t

Page 31: Singularity Theory and its Applications Dr Cathy Hobbs 30/01/09

What does this look like?

Multiplicity 3: cuspCan write the surface locally as

Eliminating t fromgives

3 0t xt y 3 23 0t xt y t x

2 327 4 0y x

Page 32: Singularity Theory and its Applications Dr Cathy Hobbs 30/01/09

Double points Fourth possibility: outline could have a double point.

Stable (and generic) – arises from two separated

parts of the surface projecting to the same neighbourhood.

Can consider such multiple mappings. In this case, it is a mapping .

Only stable cases are overlapping sheets or transverse crossings.

Codimension 3 – will only occur at isolated points along the outline.

3 3 2R R R

Page 33: Singularity Theory and its Applications Dr Cathy Hobbs 30/01/09

Motion

Can allow for motion, either of the object or camera.

Introduces further parameters so projection becomes a mapping from 4 or 5 variables into 2.

This allows the codimension to be higher and so we observe more types of singular behaviour.

Page 34: Singularity Theory and its Applications Dr Cathy Hobbs 30/01/09

Conclusions

Singularity Theory provides some useful tools for the study of local geometry of curves and surfaces.

Page 35: Singularity Theory and its Applications Dr Cathy Hobbs 30/01/09

References

Catastrophe Theory and its applications, Poston & Stewart.

Solid Shape, Koenderink Visual Motion of Curves and

Surfaces, Cipolla & Giblin Seeing – the mathematical

viewpoint, Bruce, Mathematical Intelligencer 1984 6 (4), 18-25.