THE FOUR VERTEX THEOREM AND ITS CONVERSE in honor of Björn Dahlberg

Size: px
Start display at page:

Download "THE FOUR VERTEX THEOREM AND ITS CONVERSE in honor of Björn Dahlberg"

Transcription

1 Writhe - Four Vertex Theorem.14 June, 2006 THE FOUR VERTEX THEOREM AND ITS CONVERSE in honor of Björn Dahlberg The Four Vertex Theorem says that a simple closed curve in the plane, other than a circle, must have at least four "vertices", that is, at least four points where the curvature has a local maximum or local minimum. There must be at least two local maxima, separated by two local minima. 1

2 The Converse to the Four Vertex Theorem says that any continuous real-valued function on the circle which has at least two local maxima and two local minima is the curvature function of a simple closed curve in the plane. Preassign curvature... then find the curve That is, given such a function κ defined on the circle S 1, there is an embedding α: S 1 R 2 whose image has curvature κ(t) at the point α(t) for all t S 1. 2

3 History. In 1909, the Indian mathematician S. Mukhopadhyaya proved the Four Vertex Theorem for strictly convex curves in the plane. Syamadas Mukhopadhyaya ( ) 3

4 In 1912, the German mathematician Adolf Kneser proved it for all simple closed curves in the plane, not just the strictly convex ones. Adolf Kneser ( ) In 1971, we proved the converse for strictly positive preassigned curvature, as a special case of a general result about the existence of embeddings of S n into R n+1 with strictly positive preassigned Gaussian curvature. 4

5 In 1997, the Swedish mathematician Björn Dahlberg proved the full converse to the Four Vertex Theorem without the restriction that the curvature be strictly positive. Björn E. J. Dahlberg ( ) Publication was delayed by Dahlberg's death in January 1998, but his paper was edited afterwards by his student Vilhelm Adolfsson in collaboration with Peter Kumlin, and appeared in 2005 in the Proceedings of the AMS. The work of Dahlberg completes the almost hundred year long thread of ideas begun by Mukhopadhyaya. 5

6 I. Why is the Four Vertex Theorem true? A counter-example would have a nonconstant curvature function with one max and one min, and be weakly monotonic on the two arcs between them. Let's try to build such a counter-example from a few arcs of circles. Start with the largest circle at the bottom, giving the minimum curvature there. Then go part way up to the right, switch to a smaller circle as shown, go up a little more and switch to a yet smaller circle, and go to its top. As we increase curvature by switching to smaller circles, their vertical diameters move to the right. Hence the top point lies to the right of the vertical diameter of the original circle. 6

7 When we try the same construction, but this time move up to the left from the bottom of the original circle, the top of the third circular arc will lie to the left of the vertical diameter of the original circle. Thus the convex curve that we are trying to build does not close up at the top...and so does not exist. 7

8 If we permit one self-intersection, then monotonicity of curvature is easy to realize. r = 1 2 sin θ 8

9 Recommended reading. Robert Osserman "The Four-or-More Vertex Theorem" American Mathematical Monthly Vol. 92, No. 5 (May 1985),

10 II. The Converse to the Four Vertex Theorem for strictly positive curvature. The Generalized Minkowski Problem. Does there exist an embedding of the n-sphere S n into Euclidean space R n+1 whose curvature has been preassigned as a strictly positive continuous function? In the early 1970's, we proved the following result. GENERALIZED MINKOWSKI THEOREM. Let K: S n R, for n 2, be a continuous, strictly positive function. Then there exists an embedding α: S n R n+1 onto a closed convex hypersurface whose Gaussian curvature at the point α(p) is K(p) for all p S n. When n = 1, the Four Vertex Theorem places a constraint on the curvature, so the above theorem says that by contrast, there are no constraints for n 2. The proof of this theorem was by a degree argument in the diffeomorphism group of the n-sphere S n. 10

11 The Converse to the Four Vertex Theorem. The proof of the Generalized Minkowski Theorem, when rewritten for n = 1, shows that the required embedding α exists if and only if the curvature is either a nonzero constant or else has at least two local maxima and two local minima. This gives us the converse to the Four Vertex Theorem in the case of strictly positive curvature. The spirit of the argument is shown in the following picture. A snake searches unsuccessfully for its tail 11

12 What story does this picture tell? Each of the eight little figures shows a map of an interval into the plane, which begins at the origin, moves off in the positive x-direction, ends up pointing the same way, and is positively curved throughout. We imagine that the snake is following a concealed loop of instructions, from which the above pictures are samples. The error vector in each picture extends from the snake's tail to its head, and the pictures are arranged so that the one at location θ on the circle has an error vector pointing in the direction θ. The resulting loop of error vectors circles once around the origin. If the loop of instructions is contractible in the space of all instructions, then some instruction in that space will have a corresponding error vector which is zero, and hence will tell the snake how to close up. 12

13 A specific example of the snake dance. The most elementary curvature function which can illustrate these ideas is a step-function, and the simplest case among these leads to curves built from four circular arcs, two cut from a circle of one size, alternating with two cut from a circle of another size, as shown below. Bicircle Since our curvatures are strictly positive, we can express the preassigned curvature as a function of the angle of inclination ϕ of the outward pointing normal vector. This has the advantage of making total curvature 2π automatic. Given a curvature function κ(ϕ), there will then be a unique map of the interval [0, 2π] into the plane which realizes this curvature function, subject to the initial condition that it begin at the origin, and start moving in the positive x-direction. 13

14 The figures on the left report the curvature κ as a step function of the angle ϕ with the heavier markings indicating the larger circle. The figures on the right show the resulting curve in the plane, built from arcs of these two circles. Preassign κ 0 (ϕ) Get this bicircle Preassign κ(ϕ) Get this curve 14

15 A two-curvature-snake searches unsuccessfully for its tail 15

16 Explanation of this picture. The inner group of eight circles reports the preassigned curvature step-functions κ(ϕ), while the outer group shows the corrresponding curves. Each curvature step function κ(ϕ) is a distortion, via a diffeomorphism of the circle, of the step function κ 0 (ϕ) which corresponds to the bicircle. The eight diffeomorphisms are a sample from a loop of diffeomorphisms, which is easily seen to be contractible in the space of all diffeomorphisms of the circle. Each error vector is parallel to the position of the curve in the group of eight, and therefore the error vectors turn once around the origin as we go once around the loop of diffeomorphisms. It follows that there is some diffeomorphism whose corresponding error vector is zero, and so the corresponding curve closes up. Of course we knew this, since a bicircle closes up. But this argument is robust, and so will apply to curvature functions which are close to κ 0 (ϕ). 16

17 Analogy with standard topological proof of the Fundamental Theorem of Algebra. This is analogous to proving that the polynomial p 0 (z) = a n z n has a zero by noting that it takes any circle in the complex plane to a curve which winds n times around the origin, even though we already know that p 0 (z) has a zero at the origin. Again the point is that this argument is robust, and will apply just as well to the polynomial p(z) = a n z n + a n 1 z n a 1 z + a 0, once we pay attention to a suitably large circle. 17

18 Proving the converse to the Four Vertex Theorem for strictly positive curvature. Given a preassigned strictly positive curvature funtion κ: S 1 R having at least two relative maxima and two relative minima, we first agree to parametrize our proposed curve by the inverse of the Gauss map. Then we find a diffeomorphism h: S 1 S 1 so that the curvature function κ h: S 1 R is ε-close in measure to the two-valued step function of some bicircle, meaning that the function κ h is within ε of this step function on almost all of S 1, and violates this only on a subset of measure less than ε. The robustness of the winding number argument for the two-valued step function then implies that, for sufficiently small ε > 0, there is another diffeomorphism h 1 of the circle so that the curve built with curvature function κ h h 1 closes up smoothly. Since the curvature is positive, this closed curve is convex, and since its normal vector rotates by just 2π as we go once around, the curve is simple. Reparametrizing this curve, it realizes the preassigned curvature function κ. 18

19 III. Dahlberg's proof of the Full Converse to the Four Vertex Theorem. When asked to draw a simple closed curve in the plane with strictly positive curvature, and another one with mixed positive and negative curvature, a typical response might be... 19

20 But in response to the second question, Dahlberg envisioned the following curve. Its four major subarcs are almost circular. They are connected by four small wiggly arcs, each of which has an almost constant tangent direction, but largely varying curvature, including negative curvature. This curve "marginalizes" its negative curvature and emphasizes its positive curvature, and from a distance looks like a bicircle. Dahlberg's Key Idea. You can construct such a curve with any preassigned curvature which has at least two local maxima and two local minima. You can use the winding number argument to get it to close up smoothly, and you can also make it C 1 close to a fixed convex curve, which will imply that it is simple. 20

21 Dahlberg's proof plan. (1) Choose as common domain the unit circle S 1, with arc length s as parameter. Since most of the curves will fail to close up, you can also think of the domain as the interval [0, 2π]. All the curves will have length 2π, and at the end can be scaled up or down to modify their curvature. (2) Given a preassigned curvature function κ: S 1 R which is not identically zero, evaluate 0 2π κ(s) ds. If this is zero, precede κ by a preliminary diffeomorphism of S 1 so as to make the integral nonzero. Then rescale κ by a constant c so that 0 2π c κ(s) ds = 2π. When we later modify this curvature by a diffeomorphism h: S 1 S 1, we will immediately rescale the new curvature κ h by a constant c h so that (*) 0 2π c h κ h(s) ds = 2π. 21

22 (3) Construct an arc-length parametrized curve α h : [0, 2π] R 2 with curvature c h κ h in the usual way, starting at the origin and heading to the right. In general, the curve α h will not close up, and the gap is measured by the error vector I(h) = α h (2π) α h (0). If the error vector is zero, then the curve closes up, and does so smoothly, because its total curvature is 2π. (4) Use the winding number argument to solve the equation I(h) = 0 for the unkown diffeomorphism h: S 1 S 1, with the search for h restricted to a certain 2-cell D (yet to be defined) within Diff(S 1 ). Finding h will give us a smooth closed curve with curvature function c h κ h, which we then rescale to realize the curvature function κ h, and then reparametrize to realize the curvature function κ. We can find such a curve arbitrarily C 1 -close to a bicircle, and conclude that it is simple, finishing the proof. 22

23 Configuration space. A central role in the proof is played by curvature stepfunctions with just two values, and these correspond to curves built from arcs of two different size circles. To deal with this kind of data, let CS denote the configuration space of ordered 4-tuples (p 1, p 2, p 3, p 4 ) of distinct points on the unit circle S 1, arranged in counterclockwise order, as shown below. The configuration space CS is homeomorphic to S 1 R 3. The diffeomorphism group Diff(S 1 ) acts on CS in the natural way: h(p 1, p 2, p 3, p 4 ) = (h(p 1 ), h(p 2 ), h(p 3 ), h(p 4 )). 23

24 The core of configuration space. If the ordered 4-tuple of points (p 1, p 2, p 3, p 4 ) guides the construction of a curve composed of arcs cut alternately from circles of two different sizes, then the curve will close up if and only if opposite arcs are equal in length, equivalently, if and only if p 1 and p 3 are antipodal, and also p 2 and p 4 are antipodal. These conditions are easily seen to be equivalent to the equation in the complex plane. p 1 p 2 + p 3 p 4 = 0 We will call the set of such points (p 1, p 2, p 3, p 4 ) the core of the configuration space CS. This core is homeomorphic to S 1 R 1. 24

25 Reduced configuration space. To aid in visualization, we can reduce the dimension of the configuration space from four to three, without losing any essential information. Define the reduced configuration space RCS CS to be the subset where p 1 = 1. Then RCS is homeomorphic to R 3 and we can use the group structure on S 1 to express the homeomorphism S 1 RCS CS by (e iθ, (1, p, q, r)) (e iθ, e iθ p, e iθ q, e iθ r). Notice that this homeomorphism preserves cores, that is, 1 p + q r = 0 iff e iθ e iθ p + e iθ q e iθ r = 0. Now change coordinates by writing p = e 2πix, q = e 2πiy and r = e 2πiz. Then RCS {(x, y, z) : 0 < x < y < z < 1}. 25

26 The reduced configuration space appears as an open solid tetrahedron 26

27 A point (1, p, q, r) in RCS is in the core if and only if 1 and q are antipodal, and also p and r are antipodal. In the x, y, z coordinates for RCS, this means that 0 < x < y = ½ < z = x + ½ < 1. In the open tetrahedron in xyz-space which represents RCS, the core corresponds to the open line segment connecting the point (0, ½, ½) to the point (½, ½, 1). The core of the reduced configuration space. 27

28 Special Möbius transformations. Dahlberg's choice of 2-cell D Diff(S 1 ) consists of the special Möbius transformations g β (z) = (z β) / (1 β z), where β < 1 and β is the complex conjugate of β. These special Möbius transformations are all isometries of the Poincaré disk model of the hyperbolic plane. The transformation g 0 is the identity, and if β 0, then g β is a hyperbolic translation of the line through 0 and β which takes β to 0 and 0 to β. The point β/ β and its antipode β/ β on S 1 (the circle at infinity) are the only fixed points of g β on the unit disk. 28

29 Mapping Dahlberg's 2-cell into configuration space. Start with Dahlberg's 2-cell D Diff(S 1 ), and map it into the configuration space CS by picking any point (p 1, p 2, p 3, p 4 ) in the core of CS, and sending g β (g β (p 1 ), g β (p 2 ), g β (p 3 ), g β (p 4 )). KEY PROPOSITION. The above map of D into CS is a smooth embedding which meets the core transversally at the point p, and nowhere else. We omit the proof, which makes good use of the fact that the transformations g β are isometries of the Poincaré disk model of the hyperbolic plane. 29

30 Finding the image of Dahlberg's disk in the reduced configuration space. Take the embedding of Dahlberg's disk D into the configuration space CS, and then project to the reduced configuration space RCS. Dahlberg's disk D mapped into the tetrahedron In this tetrahedral picture of the reduced configuration space RCS, the midpoint (1/4, 1/2, 3/4) of the core corresponds to the point (1, i, 1, i). Dahlberg's disk is mapped into RCS by g β (1, g β (1) 1 g β (i), g β (1) 1 g β ( 1), g β (1) 1 g β ( i)), and the answer is then converted to xyz-coordinates. 30

31 Completion of Dahlberg's proof. We start with a continuous, preassigned curvature function κ: S 1 R which has at least two local maxima and two local minima, and must find an embedding α: S 1 R 2 with curvature κ(t) at each point α(t). Changing the sign of κ if necessary, there are real numbers 0 < a < b and four points on S 1 in counterclockwise order where κ takes the values a, b, a, b in succession. The points 1, i, 1, i divide the circle S 1 into four equal arcs of length π/2. Let κ 0 by the step function which takes the values a, b, a, b on these arcs. The value of κ 0 at the four division points is irrelevant. Given any ε > 0, it is easy to find a diffeomorphism h: S 1 S 1 such that κ h is "ε-close in measure" to the step function κ 0. For notational simplicity, replace κ h by κ. 31

32 Since κ is bounded, we can choose ε sufficiently small that the total curvatures of κ and κ 0 are arbitrarily close. We then rescale both of these to achieve total curvature 2π, and they will again be ε-close in measure, for a new small ε. Suppose now that h = g β is one of the diffeomorphisms selected from Dahlberg's disk D, and consider the curvature functions κ h and κ 0 h. If β is close to 0, then h is close to the identity, so κ h and κ 0 h have total curvatures close to 2π. Hence they can be rescaled to have total curvatures exactly 2π : 0 2π c h κ h(σ) dσ = 2π = 0 2π c 0h κ 0 h(σ) dσ. Then in the usual way we construct curves α h and α 0h : [0, 2π] R 2, with these curvatures, and consider their error vectors I(h) = α h (2π) α h (0) and I 0 (h) = α 0h (2π) α 0h (0). 32

33 The finale. Let the diffeomorphism h = g β circle around the identity in Dahlberg's disk D, keeping β small and fixed. Since the image of the disk D is transverse to the core, the error vector I 0 (h) will circle once around the origin in the complex plane. 33

34 If the curvature function κ is sufficiently close in measure to the step function κ 0, and β is sufficiently small, then the error vector I(h) will also circle once around the origin in the complex plane. Hence there must be a diffeomorphism h close to the identity in the Dahlberg disk, for which the error vector I(h) = 0. This means that the corresponding curve α h closes up, and since the total curvature is 2π, it does so smoothly. For ε and β sufficiently small, this curve α h is C 1 - close to the bicircle corresponding to the original step function κ 0, and hence must itself be simple. The simple closed curve α h realizes the curvature function c h κ h, rescaling it realizes the curvature function κ h, and reparametrizing this realizes the curvature function κ. This completes Dahlberg's proof of the Converse to the Four Vertex Theorem. 34

An Investigation of the Four Vertex Theorem and its Converse

An Investigation of the Four Vertex Theorem and its Converse Union College Union Digital Works Honors Theses Student Work 6-2017 An Investigation of the Four Vertex Theorem and its Converse Rebeka Kelmar Union College - Schenectady, NY Follow this and additional

More information

THE CONVERSE OF THE FOUR VERTEX THEOREM

THE CONVERSE OF THE FOUR VERTEX THEOREM PROCEEDINGS OF THE AMERICAN MATHEMATICAL SOCIETY Volume 133, Number 7, Pages 2131 2135 S 2-9939(5)7788-9 Article electronically published on January 31, 25 THE CONVERSE OF THE FOUR VERTEX THEOREM BJÖRNE.J.DAHLBERG

More information

Part IB GEOMETRY (Lent 2016): Example Sheet 1

Part IB GEOMETRY (Lent 2016): Example Sheet 1 Part IB GEOMETRY (Lent 2016): Example Sheet 1 (a.g.kovalev@dpmms.cam.ac.uk) 1. Suppose that H is a hyperplane in Euclidean n-space R n defined by u x = c for some unit vector u and constant c. The reflection

More information

Hyperbolic Transformations

Hyperbolic Transformations C H A P T E R 17 Hyperbolic Transformations Though the text of your article on Crystal Symmetry and Its Generalizations is much too learned for a simple, selfmade pattern man like me, some of the text-illustrations

More information

612 CLASS LECTURE: HYPERBOLIC GEOMETRY

612 CLASS LECTURE: HYPERBOLIC GEOMETRY 612 CLASS LECTURE: HYPERBOLIC GEOMETRY JOSHUA P. BOWMAN 1. Conformal metrics As a vector space, C has a canonical norm, the same as the standard R 2 norm. Denote this dz one should think of dz as the identity

More information

Part IB Geometry. Theorems. Based on lectures by A. G. Kovalev Notes taken by Dexter Chua. Lent 2016

Part IB Geometry. Theorems. Based on lectures by A. G. Kovalev Notes taken by Dexter Chua. Lent 2016 Part IB Geometry Theorems Based on lectures by A. G. Kovalev Notes taken by Dexter Chua Lent 2016 These notes are not endorsed by the lecturers, and I have modified them (often significantly) after lectures.

More information

Hyperbolic Geometry on Geometric Surfaces

Hyperbolic Geometry on Geometric Surfaces Mathematics Seminar, 15 September 2010 Outline Introduction Hyperbolic geometry Abstract surfaces The hemisphere model as a geometric surface The Poincaré disk model as a geometric surface Conclusion Introduction

More information

Unit Speed Curves. Recall that a curve Α is said to be a unit speed curve if

Unit Speed Curves. Recall that a curve Α is said to be a unit speed curve if Unit Speed Curves Recall that a curve Α is said to be a unit speed curve if The reason that we like unit speed curves that the parameter t is equal to arc length; i.e. the value of t tells us how far along

More information

THE POINCARE-HOPF THEOREM

THE POINCARE-HOPF THEOREM THE POINCARE-HOPF THEOREM ALEX WRIGHT AND KAEL DIXON Abstract. Mapping degree, intersection number, and the index of a zero of a vector field are defined. The Poincare-Hopf theorem, which states that under

More information

Tangent spaces, normals and extrema

Tangent spaces, normals and extrema Chapter 3 Tangent spaces, normals and extrema If S is a surface in 3-space, with a point a S where S looks smooth, i.e., without any fold or cusp or self-crossing, we can intuitively define the tangent

More information

274 Curves on Surfaces, Lecture 4

274 Curves on Surfaces, Lecture 4 274 Curves on Surfaces, Lecture 4 Dylan Thurston Notes by Qiaochu Yuan Fall 2012 4 Hyperbolic geometry Last time there was an exercise asking for braids giving the torsion elements in PSL 2 (Z). A 3-torsion

More information

William P. Thurston. The Geometry and Topology of Three-Manifolds

William P. Thurston. The Geometry and Topology of Three-Manifolds William P. Thurston The Geometry and Topology of Three-Manifolds Electronic version 1.1 - March 00 http://www.msri.org/publications/books/gt3m/ This is an electronic edition of the 1980 notes distributed

More information

AN OVERVIEW OF KNOT INVARIANTS

AN OVERVIEW OF KNOT INVARIANTS AN OVERVIEW OF KNOT INVARIANTS WILL ADKISSON ABSTRACT. The central question of knot theory is whether two knots are isotopic. This question has a simple answer in the Reidemeister moves, a set of three

More information

A PROOF OF THE GAUSS-BONNET THEOREM. Contents. 1. Introduction. 2. Regular Surfaces

A PROOF OF THE GAUSS-BONNET THEOREM. Contents. 1. Introduction. 2. Regular Surfaces A PROOF OF THE GAUSS-BONNET THEOREM AARON HALPER Abstract. In this paper I will provide a proof of the Gauss-Bonnet Theorem. I will start by briefly explaining regular surfaces and move on to the first

More information

8. THE FARY-MILNOR THEOREM

8. THE FARY-MILNOR THEOREM Math 501 - Differential Geometry Herman Gluck Tuesday April 17, 2012 8. THE FARY-MILNOR THEOREM The curvature of a smooth curve in 3-space is 0 by definition, and its integral w.r.t. arc length, (s) ds,

More information

Solutions for Math 348 Assignment #4 1

Solutions for Math 348 Assignment #4 1 Solutions for Math 348 Assignment #4 1 (1) Do the following: (a) Show that the intersection of two spheres S 1 = {(x, y, z) : (x x 1 ) 2 + (y y 1 ) 2 + (z z 1 ) 2 = r 2 1} S 2 = {(x, y, z) : (x x 2 ) 2

More information

arxiv: v1 [math.dg] 11 Nov 2007

arxiv: v1 [math.dg] 11 Nov 2007 Length of parallel curves arxiv:711.167v1 [math.dg] 11 Nov 27 E. Macías-Virgós Abstract We prove that the length difference between a closed periodic curve and its parallel curve at a sufficiently small

More information

Junior Seminar: Hyperbolic Geometry Lecture Notes

Junior Seminar: Hyperbolic Geometry Lecture Notes Junior Seminar: Hyperbolic Geometry Lecture Notes Tim Campion January 20, 2010 1 Motivation Our first construction is very similar in spirit to an analogous one in Euclidean space. The group of isometries

More information

Length of parallel curves and rotation index

Length of parallel curves and rotation index Length of parallel curves and rotation index E. Macías-Virgós 1 Institute of Mathematics. Department of Geometry and Topology. University of Santiago de Compostela. 15782- SPAIN Abstract We prove that

More information

Diffeomorphism Groups of Reducible 3-Manifolds. Allen Hatcher

Diffeomorphism Groups of Reducible 3-Manifolds. Allen Hatcher Diffeomorphism Groups of Reducible 3-Manifolds Allen Hatcher In a 1979 announcement by César de Sá and Rourke [CR] there is a sketch of an intuitively appealing approach to measuring the difference between

More information

Packing, Curvature, and Tangling

Packing, Curvature, and Tangling Packing, Curvature, and Tangling Osaka City University February 28, 2006 Gregory Buck and Jonathan Simon Department of Mathematics, St. Anselm College, Manchester, NH. Research supported by NSF Grant #DMS007747

More information

Math 147, Homework 6 Solutions Due: May 22, 2012

Math 147, Homework 6 Solutions Due: May 22, 2012 Math 147, Homework 6 Solutions Due: May 22, 2012 1. Let T = S 1 S 1 be the torus. Is it possible to find a finite set S = {P 1,..., P n } of points in T and an embedding of the complement T \ S into R

More information

B 1 = {B(x, r) x = (x 1, x 2 ) H, 0 < r < x 2 }. (a) Show that B = B 1 B 2 is a basis for a topology on X.

B 1 = {B(x, r) x = (x 1, x 2 ) H, 0 < r < x 2 }. (a) Show that B = B 1 B 2 is a basis for a topology on X. Math 6342/7350: Topology and Geometry Sample Preliminary Exam Questions 1. For each of the following topological spaces X i, determine whether X i and X i X i are homeomorphic. (a) X 1 = [0, 1] (b) X 2

More information

Solutions for the Practice Final - Math 23B, 2016

Solutions for the Practice Final - Math 23B, 2016 olutions for the Practice Final - Math B, 6 a. True. The area of a surface is given by the expression d, and since we have a parametrization φ x, y x, y, f x, y with φ, this expands as d T x T y da xy

More information

13 Spherical geometry

13 Spherical geometry 13 Spherical geometry Let ABC be a triangle in the Euclidean plane. From now on, we indicate the interior angles A = CAB, B = ABC, C = BCA at the vertices merely by A, B, C. The sides of length a = BC

More information

NOTES FOR MATH 5520, SPRING Outline

NOTES FOR MATH 5520, SPRING Outline NOTES FOR MATH 5520, SPRING 2011 DOMINGO TOLEDO 1. Outline This will be a course on the topology and geometry of surfaces. This is a continuation of Math 4510, and we will often refer to the notes for

More information

1 Hermitian symmetric spaces: examples and basic properties

1 Hermitian symmetric spaces: examples and basic properties Contents 1 Hermitian symmetric spaces: examples and basic properties 1 1.1 Almost complex manifolds............................................ 1 1.2 Hermitian manifolds................................................

More information

Name Date Partners. Lab 2 GAUSS LAW

Name Date Partners. Lab 2 GAUSS LAW L02-1 Name Date Partners Lab 2 GAUSS LAW On all questions, work together as a group. 1. The statement of Gauss Law: (a) in words: The electric flux through a closed surface is equal to the total charge

More information

IV. Conformal Maps. 1. Geometric interpretation of differentiability. 2. Automorphisms of the Riemann sphere: Möbius transformations

IV. Conformal Maps. 1. Geometric interpretation of differentiability. 2. Automorphisms of the Riemann sphere: Möbius transformations MTH6111 Complex Analysis 2009-10 Lecture Notes c Shaun Bullett 2009 IV. Conformal Maps 1. Geometric interpretation of differentiability We saw from the definition of complex differentiability that if f

More information

A FRANKS LEMMA FOR CONVEX PLANAR BILLIARDS

A FRANKS LEMMA FOR CONVEX PLANAR BILLIARDS A FRANKS LEMMA FOR CONVEX PLANAR BILLIARDS DANIEL VISSCHER Abstract Let γ be an orbit of the billiard flow on a convex planar billiard table; then the perpendicular part of the derivative of the billiard

More information

Introduction: Pythagorean Triplets

Introduction: Pythagorean Triplets Introduction: Pythagorean Triplets On this first day I want to give you an idea of what sorts of things we talk about in number theory. In number theory we want to study the natural numbers, and in particular

More information

On the Diffeomorphism Group of S 1 S 2. Allen Hatcher

On the Diffeomorphism Group of S 1 S 2. Allen Hatcher On the Diffeomorphism Group of S 1 S 2 Allen Hatcher This is a revision, written in December 2003, of a paper of the same title that appeared in the Proceedings of the AMS 83 (1981), 427-430. The main

More information

Gauss Law 1. Name Date Partners GAUSS' LAW. Work together as a group on all questions.

Gauss Law 1. Name Date Partners GAUSS' LAW. Work together as a group on all questions. Gauss Law 1 Name Date Partners 1. The statement of Gauss' Law: (a) in words: GAUSS' LAW Work together as a group on all questions. The electric flux through a closed surface is equal to the total charge

More information

Surfaces JWR. February 13, 2014

Surfaces JWR. February 13, 2014 Surfaces JWR February 13, 214 These notes summarize the key points in the second chapter of Differential Geometry of Curves and Surfaces by Manfredo P. do Carmo. I wrote them to assure that the terminology

More information

arxiv: v1 [math.dg] 19 Jun 2017

arxiv: v1 [math.dg] 19 Jun 2017 LIMITING BEHAVIOR OF SEQUENCES OF PROPERLY EMBEDDED MINIMAL DISKS arxiv:1706.06186v1 [math.dg] 19 Jun 2017 DAVID HOFFMAN AND BRIAN WHITE Abstract. We develop a theory of minimal θ-graphs and characterize

More information

DIFFERENTIAL GEOMETRY, LECTURE 16-17, JULY 14-17

DIFFERENTIAL GEOMETRY, LECTURE 16-17, JULY 14-17 DIFFERENTIAL GEOMETRY, LECTURE 16-17, JULY 14-17 6. Geodesics A parametrized line γ : [a, b] R n in R n is straight (and the parametrization is uniform) if the vector γ (t) does not depend on t. Thus,

More information

LECTURE Itineraries We start with a simple example of a dynamical system obtained by iterating the quadratic polynomial

LECTURE Itineraries We start with a simple example of a dynamical system obtained by iterating the quadratic polynomial LECTURE. Itineraries We start with a simple example of a dynamical system obtained by iterating the quadratic polynomial f λ : R R x λx( x), where λ [, 4). Starting with the critical point x 0 := /2, we

More information

The Fundamental Group and Covering Spaces

The Fundamental Group and Covering Spaces Chapter 8 The Fundamental Group and Covering Spaces In the first seven chapters we have dealt with point-set topology. This chapter provides an introduction to algebraic topology. Algebraic topology may

More information

GLOBAL PROPERTIES OF PLANE AND SPACE CURVES

GLOBAL PROPERTIES OF PLANE AND SPACE CURVES GLOBAL PROPERTIES OF PLANE AND SPACE CURVES KEVIN YAN Abstract. The purpose of this paper is purely expository. Its goal is to explain basic differential geometry to a general audience without assuming

More information

Highly complex: Möbius transformations, hyperbolic tessellations and pearl fractals

Highly complex: Möbius transformations, hyperbolic tessellations and pearl fractals Highly complex: Möbius transformations, hyperbolic tessellations and pearl fractals Department of mathematical sciences Aalborg University Cergy-Pontoise 26.5.2011 Möbius transformations Definition Möbius

More information

DIFFERENTIAL GEOMETRY HW 5

DIFFERENTIAL GEOMETRY HW 5 DIFFERENTIAL GEOMETRY HW 5 CLAY SHONKWILER 1 Check the calculations above that the Gaussian curvature of the upper half-plane and Poincaré disk models of the hyperbolic plane is 1. Proof. The calculations

More information

A crash course the geometry of hyperbolic surfaces

A crash course the geometry of hyperbolic surfaces Lecture 7 A crash course the geometry of hyperbolic surfaces 7.1 The hyperbolic plane Hyperbolic geometry originally developed in the early 19 th century to prove that the parallel postulate in Euclidean

More information

Chapter 19 Clifford and the Number of Holes

Chapter 19 Clifford and the Number of Holes Chapter 19 Clifford and the Number of Holes We saw that Riemann denoted the genus by p, a notation which is still frequently used today, in particular for the generalizations of this notion in higher dimensions.

More information

GEOMETRY Notes Easter 2002

GEOMETRY Notes Easter 2002 Department of Pure Mathematics and Mathematical Statistics University of Cambridge GEOMETRY Notes Easter 2002 T. K. Carne. t.k.carne@dpmms.cam.ac.uk c Copyright. Not for distribution outside Cambridge

More information

Mathematics 3210 Spring Semester, 2005 Homework notes, part 8 April 15, 2005

Mathematics 3210 Spring Semester, 2005 Homework notes, part 8 April 15, 2005 Mathematics 3210 Spring Semester, 2005 Homework notes, part 8 April 15, 2005 The underlying assumption for all problems is that all points, lines, etc., are taken within the Poincaré plane (or Poincaré

More information

PICARD S THEOREM STEFAN FRIEDL

PICARD S THEOREM STEFAN FRIEDL PICARD S THEOREM STEFAN FRIEDL Abstract. We give a summary for the proof of Picard s Theorem. The proof is for the most part an excerpt of [F]. 1. Introduction Definition. Let U C be an open subset. A

More information

BROWN UNIVERSITY MATH 0350 MIDTERM 19 OCTOBER 2017 INSTRUCTOR: SAMUEL S. WATSON. a b. Name: Problem 1

BROWN UNIVERSITY MATH 0350 MIDTERM 19 OCTOBER 2017 INSTRUCTOR: SAMUEL S. WATSON. a b. Name: Problem 1 BROWN UNIVERSITY MATH 0350 MIDTERM 19 OCTOBER 2017 INSTRUCTOR: SAMUEL S. WATSON Name: Problem 1 In this problem, we will use vectors to show that an angle formed by connecting a point on a circle to two

More information

Math 215a Homework #1 Solutions. π 1 (X, x 1 ) β h

Math 215a Homework #1 Solutions. π 1 (X, x 1 ) β h Math 215a Homework #1 Solutions 1. (a) Let g and h be two paths from x 0 to x 1. Then the composition sends π 1 (X, x 0 ) β g π 1 (X, x 1 ) β h π 1 (X, x 0 ) [f] [h g f g h] = [h g][f][h g] 1. So β g =

More information

4-MANIFOLDS: CLASSIFICATION AND EXAMPLES. 1. Outline

4-MANIFOLDS: CLASSIFICATION AND EXAMPLES. 1. Outline 4-MANIFOLDS: CLASSIFICATION AND EXAMPLES 1. Outline Throughout, 4-manifold will be used to mean closed, oriented, simply-connected 4-manifold. Hopefully I will remember to append smooth wherever necessary.

More information

Example 2 (new version): the generators are. Example 4: the generators are

Example 2 (new version): the generators are. Example 4: the generators are First, let us quickly dismiss Example 3 (and Example 6): the second generator may be removed (being the square of the third or, respectively, the fourth one), and then the quotient is clearly the simplest

More information

CHAPTER 3. Gauss map. In this chapter we will study the Gauss map of surfaces in R 3.

CHAPTER 3. Gauss map. In this chapter we will study the Gauss map of surfaces in R 3. CHAPTER 3 Gauss map In this chapter we will study the Gauss map of surfaces in R 3. 3.1. Surfaces in R 3 Let S R 3 be a submanifold of dimension 2. Let {U i, ϕ i } be a DS on S. For any p U i we have a

More information

Appendix E : Note on regular curves in Euclidean spaces

Appendix E : Note on regular curves in Euclidean spaces Appendix E : Note on regular curves in Euclidean spaces In Section III.5 of the course notes we posed the following question: Suppose that U is a connected open subset of R n and x, y U. Is there a continuous

More information

MATH DIFFERENTIAL GEOMETRY. Contents

MATH DIFFERENTIAL GEOMETRY. Contents MATH 3968 - DIFFERENTIAL GEOMETRY ANDREW TULLOCH Contents 1. Curves in R N 2 2. General Analysis 2 3. Surfaces in R 3 3 3.1. The Gauss Bonnet Theorem 8 4. Abstract Manifolds 9 1 MATH 3968 - DIFFERENTIAL

More information

Analytic Geometry MAT 1035

Analytic Geometry MAT 1035 Analytic Geometry MAT 035 5.09.04 WEEKLY PROGRAM - The first week of the semester, we will introduce the course and given a brief outline. We continue with vectors in R n and some operations including

More information

ISOMETRIES OF R n KEITH CONRAD

ISOMETRIES OF R n KEITH CONRAD ISOMETRIES OF R n KEITH CONRAD 1. Introduction An isometry of R n is a function h: R n R n that preserves the distance between vectors: h(v) h(w) = v w for all v and w in R n, where (x 1,..., x n ) = x

More information

SELECTED SAMPLE FINAL EXAM SOLUTIONS - MATH 5378, SPRING 2013

SELECTED SAMPLE FINAL EXAM SOLUTIONS - MATH 5378, SPRING 2013 SELECTED SAMPLE FINAL EXAM SOLUTIONS - MATH 5378, SPRING 03 Problem (). This problem is perhaps too hard for an actual exam, but very instructional, and simpler problems using these ideas will be on the

More information

Good Problems. Math 641

Good Problems. Math 641 Math 641 Good Problems Questions get two ratings: A number which is relevance to the course material, a measure of how much I expect you to be prepared to do such a problem on the exam. 3 means of course

More information

Lecture 6 SPHERICAL GEOMETRY

Lecture 6 SPHERICAL GEOMETRY 1 Lecture 6 SPHERICAL GEOMETRY So far we have studied finite and discrete geometries, i.e., geometries in which the main transformation group is either finite or discrete. In this lecture, we begin our

More information

DIFFERENTIAL GEOMETRY HW 5. Show that the law of cosines in spherical geometry is. cos c = cos a cos b + sin a sin b cos θ.

DIFFERENTIAL GEOMETRY HW 5. Show that the law of cosines in spherical geometry is. cos c = cos a cos b + sin a sin b cos θ. DIFFEENTIAL GEOMETY HW 5 CLAY SHONKWILE Show that the law of cosines in spherical geometry is 5 cos c cos a cos b + sin a sin b cos θ. Proof. Consider the spherical triangle depicted below: Form radii

More information

Part IB. Geometry. Year

Part IB. Geometry. Year Part IB Year 2017 2016 2015 2014 2013 2012 2011 2010 2009 2008 2007 2006 2005 2004 2003 2002 2001 2017 17 Paper 1, Section I 3G Give the definition for the area of a hyperbolic triangle with interior angles

More information

What is a Space Curve?

What is a Space Curve? What is a Space Curve? A space curve is a smooth map γ : I R R 3. In our analysis of defining the curvature for space curves we will be able to take the inclusion (γ, 0) and have that the curvature of

More information

Spiral spline interpolation to a planar spiral

Spiral spline interpolation to a planar spiral Spiral spline interpolation to a planar spiral Zulfiqar Habib Department of Mathematics and Computer Science, Graduate School of Science and Engineering, Kagoshima University Manabu Sakai Department of

More information

Lecture 14 Conformal Mapping. 1 Conformality. 1.1 Preservation of angle. 1.2 Length and area. MATH-GA Complex Variables

Lecture 14 Conformal Mapping. 1 Conformality. 1.1 Preservation of angle. 1.2 Length and area. MATH-GA Complex Variables Lecture 14 Conformal Mapping MATH-GA 2451.001 Complex Variables 1 Conformality 1.1 Preservation of angle The open mapping theorem tells us that an analytic function such that f (z 0 ) 0 maps a small neighborhood

More information

9th Bay Area Mathematical Olympiad

9th Bay Area Mathematical Olympiad 9th Bay rea Mathematical Olympiad February 27, 2007 Problems with Solutions 1 15-inch-long stick has four marks on it, dividing it into five segments of length 1,2,3,4, and 5 inches (although not neccessarily

More information

Homework 4: Mayer-Vietoris Sequence and CW complexes

Homework 4: Mayer-Vietoris Sequence and CW complexes Homework 4: Mayer-Vietoris Sequence and CW complexes Due date: Friday, October 4th. 0. Goals and Prerequisites The goal of this homework assignment is to begin using the Mayer-Vietoris sequence and cellular

More information

Analytic Geometry MAT 1035

Analytic Geometry MAT 1035 Analytic Geometry MAT 035 5.09.04 WEEKLY PROGRAM - The first week of the semester, we will introduce the course and given a brief outline. We continue with vectors in R n and some operations including

More information

Practice Problems for the Final Exam

Practice Problems for the Final Exam Math 114 Spring 2017 Practice Problems for the Final Exam 1. The planes 3x + 2y + z = 6 and x + y = 2 intersect in a line l. Find the distance from the origin to l. (Answer: 24 3 ) 2. Find the area of

More information

The Geometrization Theorem

The Geometrization Theorem The Geometrization Theorem Matthew D. Brown Wednesday, December 19, 2012 In this paper, we discuss the Geometrization Theorem, formerly Thurston s Geometrization Conjecture, which is essentially the statement

More information

Manifolds, Lie Groups, Lie Algebras, with Applications. Kurt W.A.J.H.Y. Reillag (alias Jean Gallier) CIS610, Spring 2005

Manifolds, Lie Groups, Lie Algebras, with Applications. Kurt W.A.J.H.Y. Reillag (alias Jean Gallier) CIS610, Spring 2005 Manifolds, Lie Groups, Lie Algebras, with Applications Kurt W.A.J.H.Y. Reillag (alias Jean Gallier) CIS610, Spring 2005 1 Motivations and Goals 1. Motivations Observation: Often, the set of all objects

More information

Abstract & Applied Linear Algebra (Chapters 1-2) James A. Bernhard University of Puget Sound

Abstract & Applied Linear Algebra (Chapters 1-2) James A. Bernhard University of Puget Sound Abstract & Applied Linear Algebra (Chapters 1-2) James A. Bernhard University of Puget Sound Copyright 2018 by James A. Bernhard Contents 1 Vector spaces 3 1.1 Definitions and basic properties.................

More information

Name Date Partners. Lab 4 - GAUSS' LAW. On all questions, work together as a group.

Name Date Partners. Lab 4 - GAUSS' LAW. On all questions, work together as a group. 65 Name Date Partners 1. The statement of Gauss' Law: Lab 4 - GAUSS' LAW On all questions, work together as a group. (a) in words: The electric flux through a closed surface is equal to the total charge

More information

MATH8808: ALGEBRAIC TOPOLOGY

MATH8808: ALGEBRAIC TOPOLOGY MATH8808: ALGEBRAIC TOPOLOGY DAWEI CHEN Contents 1. Underlying Geometric Notions 2 1.1. Homotopy 2 1.2. Cell Complexes 3 1.3. Operations on Cell Complexes 3 1.4. Criteria for Homotopy Equivalence 4 1.5.

More information

The Hurewicz Theorem

The Hurewicz Theorem The Hurewicz Theorem April 5, 011 1 Introduction The fundamental group and homology groups both give extremely useful information, particularly about path-connected spaces. Both can be considered as functors,

More information

1 Differentiable manifolds and smooth maps

1 Differentiable manifolds and smooth maps 1 Differentiable manifolds and smooth maps Last updated: April 14, 2011. 1.1 Examples and definitions Roughly, manifolds are sets where one can introduce coordinates. An n-dimensional manifold is a set

More information

1 Euclidean geometry. 1.1 The metric on R n

1 Euclidean geometry. 1.1 The metric on R n 1 Euclidean geometry This chapter discusses the geometry of n-dimensional Euclidean space E n, together with its distance function. The distance gives rise to other notions such as angles and congruent

More information

Vassiliev Invariants, Chord Diagrams, and Jacobi Diagrams

Vassiliev Invariants, Chord Diagrams, and Jacobi Diagrams Vassiliev Invariants, Chord Diagrams, and Jacobi Diagrams By John Dougherty X Abstract: The goal of this paper is to understand the topological meaning of Jacobi diagrams in relation to knot theory and

More information

Möbius Transformation

Möbius Transformation Möbius Transformation 1 1 June 15th, 2010 Mathematics Science Center Tsinghua University Philosophy Rigidity Conformal mappings have rigidity. The diffeomorphism group is of infinite dimension in general.

More information

2. Gauss Law [1] Equipment: This is a theoretical lab so your equipment is pencil, paper, and textbook.

2. Gauss Law [1] Equipment: This is a theoretical lab so your equipment is pencil, paper, and textbook. Purpose: Theoretical study of Gauss law. 2. Gauss Law [1] Equipment: This is a theoretical lab so your equipment is pencil, paper, and textbook. When drawing field line pattern around charge distributions

More information

MATH 434 Fall 2016 Homework 1, due on Wednesday August 31

MATH 434 Fall 2016 Homework 1, due on Wednesday August 31 Homework 1, due on Wednesday August 31 Problem 1. Let z = 2 i and z = 3 + 4i. Write the product zz and the quotient z z in the form a + ib, with a, b R. Problem 2. Let z C be a complex number, and let

More information

Smooth Dynamics 2. Problem Set Nr. 1. Instructor: Submitted by: Prof. Wilkinson Clark Butler. University of Chicago Winter 2013

Smooth Dynamics 2. Problem Set Nr. 1. Instructor: Submitted by: Prof. Wilkinson Clark Butler. University of Chicago Winter 2013 Smooth Dynamics 2 Problem Set Nr. 1 University of Chicago Winter 2013 Instructor: Submitted by: Prof. Wilkinson Clark Butler Problem 1 Let M be a Riemannian manifold with metric, and Levi-Civita connection.

More information

Convex Analysis and Economic Theory Winter 2018

Convex Analysis and Economic Theory Winter 2018 Division of the Humanities and Social Sciences Ec 181 KC Border Convex Analysis and Economic Theory Winter 2018 Topic 0: Vector spaces 0.1 Basic notation Here are some of the fundamental sets and spaces

More information

Convergence in shape of Steiner symmetrized line segments. Arthur Korneychuk

Convergence in shape of Steiner symmetrized line segments. Arthur Korneychuk Convergence in shape of Steiner symmetrized line segments by Arthur Korneychuk A thesis submitted in conformity with the requirements for the degree of Master of Science Graduate Department of Mathematics

More information

fy (X(g)) Y (f)x(g) gy (X(f)) Y (g)x(f)) = fx(y (g)) + gx(y (f)) fy (X(g)) gy (X(f))

fy (X(g)) Y (f)x(g) gy (X(f)) Y (g)x(f)) = fx(y (g)) + gx(y (f)) fy (X(g)) gy (X(f)) 1. Basic algebra of vector fields Let V be a finite dimensional vector space over R. Recall that V = {L : V R} is defined to be the set of all linear maps to R. V is isomorphic to V, but there is no canonical

More information

SPRING 2008: POLYNOMIAL IMAGES OF CIRCLES

SPRING 2008: POLYNOMIAL IMAGES OF CIRCLES 18.821 SPRING 28: POLYNOMIAL IMAGES OF CIRCLES JUSTIN CURRY, MICHAEL FORBES, MATTHEW GORDON Abstract. This paper considers the effect of complex polynomial maps on circles of various radii. Several phenomena

More information

Some notes on Coxeter groups

Some notes on Coxeter groups Some notes on Coxeter groups Brooks Roberts November 28, 2017 CONTENTS 1 Contents 1 Sources 2 2 Reflections 3 3 The orthogonal group 7 4 Finite subgroups in two dimensions 9 5 Finite subgroups in three

More information

1.2 Functions What is a Function? 1.2. FUNCTIONS 11

1.2 Functions What is a Function? 1.2. FUNCTIONS 11 1.2. FUNCTIONS 11 1.2 Functions 1.2.1 What is a Function? In this section, we only consider functions of one variable. Loosely speaking, a function is a special relation which exists between two variables.

More information

The Symmetric Space for SL n (R)

The Symmetric Space for SL n (R) The Symmetric Space for SL n (R) Rich Schwartz November 27, 2013 The purpose of these notes is to discuss the symmetric space X on which SL n (R) acts. Here, as usual, SL n (R) denotes the group of n n

More information

Math 426H (Differential Geometry) Final Exam April 24, 2006.

Math 426H (Differential Geometry) Final Exam April 24, 2006. Math 426H Differential Geometry Final Exam April 24, 6. 8 8 8 6 1. Let M be a surface and let : [0, 1] M be a smooth loop. Let φ be a 1-form on M. a Suppose φ is exact i.e. φ = df for some f : M R. Show

More information

Classical transcendental curves

Classical transcendental curves Classical transcendental curves Reinhard Schultz May, 2008 In his writings on coordinate geometry, Descartes emphasized that he was only willing to work with curves that could be defined by algebraic equations.

More information

Index. Bertrand mate, 89 bijection, 48 bitangent, 69 Bolyai, 339 Bonnet s Formula, 283 bounded, 48

Index. Bertrand mate, 89 bijection, 48 bitangent, 69 Bolyai, 339 Bonnet s Formula, 283 bounded, 48 Index acceleration, 14, 76, 355 centripetal, 27 tangential, 27 algebraic geometry, vii analytic, 44 angle at a corner, 21 on a regular surface, 170 angle excess, 337 angle of parallelism, 344 angular velocity,

More information

Lesson 26: Characterization of Parallel Lines

Lesson 26: Characterization of Parallel Lines Student Outcomes Students know that when a system of linear equations has no solution, i.e., no point of intersection of the lines, then the lines are parallel. Lesson Notes The discussion that begins

More information

Isometries. Chapter Transformations of the Plane

Isometries. Chapter Transformations of the Plane Chapter 1 Isometries The first three chapters of this book are dedicated to the study of isometries and their properties. Isometries, which are distance-preserving transformations from the plane to itself,

More information

Chapter 16. Manifolds and Geodesics Manifold Theory. Reading: Osserman [7] Pg , 55, 63-65, Do Carmo [2] Pg ,

Chapter 16. Manifolds and Geodesics Manifold Theory. Reading: Osserman [7] Pg , 55, 63-65, Do Carmo [2] Pg , Chapter 16 Manifolds and Geodesics Reading: Osserman [7] Pg. 43-52, 55, 63-65, Do Carmo [2] Pg. 238-247, 325-335. 16.1 Manifold Theory Let us recall the definition of differentiable manifolds Definition

More information

A BRIEF INTRODUCTION TO MATHEMATICAL RELATIVITY PART 1: SPECIAL RELATIVITY ARICK SHAO

A BRIEF INTRODUCTION TO MATHEMATICAL RELATIVITY PART 1: SPECIAL RELATIVITY ARICK SHAO A BRIEF INTRODUCTION TO MATHEMATICAL RELATIVITY PART 1: SPECIAL RELATIVITY ARICK SHAO These notes are the first of a pair of brief articles containing an informal introduction to the mathematics behind

More information

CHARACTERIZATIONS OF CIRCLE PATTERNS AND CONVEX POLYHEDRA IN HYPERBOLIC 3-SPACE

CHARACTERIZATIONS OF CIRCLE PATTERNS AND CONVEX POLYHEDRA IN HYPERBOLIC 3-SPACE CHARACTERIZATIONS OF CIRCLE PATTERNS AND CONVEX POLYHEDRA IN HYPERBOLIC 3-SPACE XIAOJUN HUANG AND JINSONG LIU ABSTRACT In this paper we consider the characterization problem of convex polyhedrons in the

More information

9th and 10th Grade Math Proficiency Objectives Strand One: Number Sense and Operations

9th and 10th Grade Math Proficiency Objectives Strand One: Number Sense and Operations Strand One: Number Sense and Operations Concept 1: Number Sense Understand and apply numbers, ways of representing numbers, the relationships among numbers, and different number systems. Justify with examples

More information

Definition We say that a topological manifold X is C p if there is an atlas such that the transition functions are C p.

Definition We say that a topological manifold X is C p if there is an atlas such that the transition functions are C p. 13. Riemann surfaces Definition 13.1. Let X be a topological space. We say that X is a topological manifold, if (1) X is Hausdorff, (2) X is 2nd countable (that is, there is a base for the topology which

More information

Polynomials in knot theory. Rama Mishra. January 10, 2012

Polynomials in knot theory. Rama Mishra. January 10, 2012 January 10, 2012 Knots in the real world The fact that you can tie your shoelaces in several ways has inspired mathematicians to develop a deep subject known as knot theory. mathematicians treat knots

More information

Qualifying Exams I, 2014 Spring

Qualifying Exams I, 2014 Spring Qualifying Exams I, 2014 Spring 1. (Algebra) Let k = F q be a finite field with q elements. Count the number of monic irreducible polynomials of degree 12 over k. 2. (Algebraic Geometry) (a) Show that

More information

Euler Characteristic of Two-Dimensional Manifolds

Euler Characteristic of Two-Dimensional Manifolds Euler Characteristic of Two-Dimensional Manifolds M. Hafiz Khusyairi August 2008 In this work we will discuss an important notion from topology, namely Euler Characteristic and we will discuss several

More information