) R 2. 2tR 2 R 2 +t 2 y = t2 R 2. x = R y, t 2 +R 2 R. 2uR2 R 2 +u 2 +v 2 2vR2. x = y = R z v = Ry, R z. z = u2 +v 2 R 2.

Size: px
Start display at page:

Download ") R 2. 2tR 2 R 2 +t 2 y = t2 R 2. x = R y, t 2 +R 2 R. 2uR2 R 2 +u 2 +v 2 2vR2. x = y = R z v = Ry, R z. z = u2 +v 2 R 2."

Transcription

1 Homework. Solutions 1 a Write own explicit formulae expressing stereographic coorinates for n-imensional sphere x x n+1 of raius via coorinates x 1,..., x n+1 an vice versa. For simplicit ou ma consier cases n, 3. b Check that for unit sphere S x + + z 1 all the points with rational cartesian coorinates x,, z have rational stereographic coorinates u, v an vice versa. a Write own the stereographic projection from the North pole of the sphere point N 0, 0,..., on the plane x n+1 0. Consier the segment ND which intersects the sphere at the point x 1,..., x n+1 x 1 + x x n+1. This segment intersects the plane x n+1 0 at the point D with coorinates x i u i for i 1,..., n. Then comparing similar triangles we have an ui xn+1 x i, i.e. x i ui i 1,..., n xn+1 x i ui x n+1, i 1,..., n. Using the fact that x x n+1 we come to x x n x n+1 n u i x n+1 + x n+1. Diviing b x n+1 x n+1 since North pole is remove we come to n x n+1 i1 ui n i1 ui +, u i xi n i 1,,... i1 ui + For projection with centre in South pole we have to change x n+1 x n+1. Write own these formulae for cases n 1,, 3, Case n 1: Circle x +. Stereographic coorinate t. Centre of projection 0, : i1 t x, x t +t t t + 1 Case n : Sphere x + + z. Stereographic coorinates u, v. Centre of projection 0, 0, : u x z v, z x u +u +v v +u +v z u +v u +v + Case n 3: 3-imensional sphere x + + z + t. Stereographic coorinates u, v, w. Centre of projection 0, 0, 0, : u x u x t +u +v +w v v t, +u +v +w w z w z t +u +v +w z u +v +w u +v +w + b We see that from explicit formulae. This is rational transformation of conic surfaces. Consier the iemannian metric on the circle of the raius inuce b the Eucliean metric on the ambient plane. 1

2 a Express it using polar angle as a coorinate on the circle. b Express the same metric using stereographic coorinate t obtaine b stereographic projection of the circle on the line, passing through its centre. iemannian metric of Eucliean space is G x +. x cos ϕ a using the angle: In this case parametric equation of circle is sin ϕ. Then G x + x cos ϕ, sin ϕ cos ϕ + sin ϕ ϕ. b In stereographic coorinate using 1 we have: G x + xxt,t t t + t + + t t + t 4t t tt + t + + t tt [ t t + t + t t + t + t tt ] + t t t + t + t + 44 t + t 44 t + t 3 Consier the iemannian metric on the sphere of the raius inuce b the Eucliean metric on the ambient 3-imensional space. a Express it using spherical coorinates on the sphere. b Express the same metric using stereographic coorinates u, v obtaine b stereographic projection of the sphere on the plane, passing through its centre. Then Solution iemannian metric of Eucliean space is G x + + z. a using the spherical coorinates: In this case parametric equation of sphere is x sin θ cos ϕ sin θ sin ϕ. z cos θ G x + +z x sin θ cos ϕ, sin θ sin ϕ,z cos θ sin θ cos ϕ + sin θ sin ϕ + cos θ cos θ cos ϕθ sin θ sin ϕϕ + cos θ sin ϕθ + sin θ cos ϕϕ + sin θθ θ + sin θϕ. b in stereographic coorinates using we have G x + + z xxu,v,u,v,zzu,v u + u + v + v + u + v u + v + + u + v 4 u uuu + vv + u + v + u + v + v vuu + vv + u + v + u + v + uu + vv + + u + v u + v uu + vv + u + v u + v 4 [ u + v u uvv ] + [ v + u v uvu ] + 4 uu + vv } u + v 4 + u + v } u + v 44 u + v + u + v

3 emark In the case of n-imensional sphere S n of raius in n + 1-imensional Eucliean space E n+1 it can be efine b the equation x x n+1 1 in cartesian coorinates x 1,..., x n, x n+1 iemannian metric on this sphere inuce b the Eucliean metric in the ambient space in stereographic coorinates has following appearance: G x x n+1 n x µ x i u i j1 u j + n i1 ui 44 n i1 ui + n i1 ui 4 Consier the surface L which is the upper sheet of two-sheete hperboloi in 3 : L: z x 1, z > 0. n i1 + ui + n i1 ui a Fin parametric equation of the surface L using hperbolic functions cosh, sinh following an analog with spherical coorinates on the sphere. The surface L sometimes is calle pseuo-sphere. b Consier the stereographic projection of the surface L on the plane OXY, i.e. the central projection on the plane z 0 with the centre at the point 0, 0, 1. Show that the image of projection of the surface L is the open isc x + < 1 in the plane OXY. x sinh θ cos ϕ a Parametric equation is sinh θ sin ϕ z cosh θθ cos ϕ We see that the conition z x 1 is fulfille. Compare with equation of sphere in spheric coorinates. b Calculations are ver similar to the case of stereographic coorinates for -sphere x + + z 1 of the raius 1. Stereographic coorinates u, v. Centre of projection 0, 0, 1: We have u x v 1. u x Hence v. Since x u1 + z, v1 + z then z 1 x + an z 1 u + v 1 + z, i.e. z 1+u +v 1 u v. We come to u x v The image of upper-sheet is an open isc u + v 1 since u + v x + sheet z > 1 then 0 z 1 z+1 < 1., u x 1 u v v 1 u v, u < 1, v < 1. 4 z u +v +1 1 u v z 1 5 Consier the pseuo-iemannian, pseuo-eucliean metric on 3 given b the formula s x + z. z 1 z+1. Since for upper Calculate the inuce metric on the surface L consiere in the Exercise 4, an show that it is a iemannian metric it is positive-efinite. Perform calculations in spherical-like coorinates see Exercise 4a above an in stereographic coorinates see exercise 4b above 3

4 emark The surface L sometimes is calle pseuosphere. The iemannian metric on this surface sometimes is calle Lobachevsk hperbolic metric. The surface L with this metric realises Lobachevsk hperbolic geometr, where Eucli s 5-th Axiom fails. This iemannian manifol manifol+iemannian metric we call Lobachevsk hperbolic plane. In stereographic coorinates we come to realisation of Lobachevsk plane on the isc in E. It is so calle Poincare moel of Lobachevsk geometr. Solution. The calculations will be ver similar to the calculations performe in the exercise 3 above. Just we nee consier cosh θ, sinh θ instea cos θ, sin θ an an sometimes changes the signs. First of all consier spherical-like coorinates: x sinh θ cos ϕ Equation of two-sheete hperboloi is sinh θ sin ϕ. Then z cosh θ G x + z xsinh θ cos ϕ,sinh θ sin ϕ,zcosh θ sinh θ cos ϕ + sinh θ sin ϕ cosh θ cosh θ cos ϕθ sinh θ sin ϕϕ + cosh θ sin ϕθ + sinh θ cos ϕϕ + sinh θθ θ + sinh θϕ. 1 0 matrix of iemannian metric is G 0 sinh. In the same wa as for sphere these coorinates are θ well-efine in all points except z ±1, where sin θ 0. Now express iemannian metric in stereographic coorinates 4: G x + z xxu,v,u,v,zzu,v u 1 u v + v 1 u v Compare with calculations for sphere x + + z 1. We have G x + z u uuu + vv v vuu + vv 1 u + v 1 u v + 1 u + v 1 u v uu + vv 1 u v + u + v + 1uu + vv 1 u v 4u + 4v 1 u v. u + v u v To perform these calculations it is convenient to enote b s 1 u v. esume: We come to the inuce iemannian metric on the surface from the pseuo-iemannian metric in ambient space. 6 Lobachevsk plane hperbolic plane L in stereographic coorinates can be consiere as an open isc u + v < 1 in the plane. In the previous exercise in particularl we calculate iemannian metric of L in these coorinates. Fin new coorinates x, such that in these coorinates Lobachevsk plane hperbolic plane can be consiere as an upper half plane > 0} an write own explicitl iemannian metric in these coorinates. Hint: You ma use complex coorinates: z x + i, z x i, w u + iv, w u iv an fin an holomorphic transformation w wz of the open isc w w < 1 onto the upper plane Imz > 0. Solution. ecall that in the previous exercise we calculate expression for Lobachevsk metric in stereographic coorinates u, v, u + v < 1. We come to the answer: G 4u +4v 1 u v see the previous exercise. It was 4

5 realisation of Lobachevsk plane on the Eucliean isc. Sometimes it calle Poincare moel of Lobachevsk hperbolic geometr. In complex coorinates w u + iv, w u iv the metric G 4u +4v obtaine in the exercise 8 can be rewritten G 4w w 1 w w. Inee G 1 u v 4w w 4u + ivu iv G 1 w w 1 u + ivu iv 4u + 4v 1 u v. It is a beautiful problem in complex analsis: fin Mobius transformation w az+b cz+ transformation which transforms the interior of circle w w 1 into upper half plane Imz > 0. One can see that w 1 + iz 1 iz, z i1 w 1 + w is the transformation which we nee Can ou fin all Mobius transformations which transform upper half plane to the interior of unit circle?. Now calculate G in coorinates z, z. i.e. in coorinates x, : We have Hence G w G 4u + 4v 4w w 1 u v 1 w w 1 + iz iz i z, w 1 iz 1 iz 1 + i z, 1 w w iz 1 i z 1 iz 1 + i z i z z 1 iz1 + i z 4w w 4 1 w w iz i z 1 iz 1+i z 4 z z 1 iz 1+i z 4 z z z x +, since z x + i an z z i. We come to the ver useful interpretation of hperbolic geometr: upper half plane in E with metric G x +. Later b efault we will call Lobachevsk hperbolic plane the realisation of Lobachevsk plane as an half-upper plane in E with these coorinates x, > 0 with metric G x +. 7 Consier the metric inuce on one-sheete hperboloi x + z 1 embee in 3 with the pseuo-eucliean metric x + z see the exercise 5. Show that this metric is not iemannian one. Solution. One can perform straightforwar calculations in spherical-like coorinates: Equation of onesheete hperboloi is cosh θ sin ϕ. Then x cosh θ cos ϕ z sinh θ G x + z xcosh θ cos ϕ,cosh θ sin ϕ,zsinh θ cosh θ cos ϕ + cosh θ sin ϕ sinh θ sinh θ cos ϕθ cosh θ sin ϕϕ + sinh θ sin ϕθ + cosh θ cos ϕϕ cosh θθ θ + cosh θϕ. 1 0 matrix is G 0 cosh. The conition of positive-efiniteness is not fulfille. This is not iemannian θ metric. Another solution Consier the vectors e an f z attache at the point 1, 0, 0. One can see that these vectors are tangent to the hperboloi, but the have the length of ifferent sign. One of these vectors is space-like vector, another time like vector. We have pseuoriemannian metric at the tangent space spanne b these two vectors. 5

+ dxk. dt 2. dt Γi km dxm. . Its equations of motion are second order differential equations. with intitial conditions

+ dxk. dt 2. dt Γi km dxm. . Its equations of motion are second order differential equations. with intitial conditions Homework 7. Solutions 1 Show that great circles are geodesics on sphere. Do it a) using the fact that for geodesic, acceleration is orthogonal to the surface. b ) using straightforwardl equations for geodesics

More information

STUDENT S COMPANIONS IN BASIC MATH: THE FOURTH. Trigonometric Functions

STUDENT S COMPANIONS IN BASIC MATH: THE FOURTH. Trigonometric Functions STUDENT S COMPANIONS IN BASIC MATH: THE FOURTH Trigonometric Functions Let me quote a few sentences at the beginning of the preface to a book by Davi Kammler entitle A First Course in Fourier Analysis

More information

17.3. Parametric Curves. Introduction. Prerequisites. Learning Outcomes

17.3. Parametric Curves. Introduction. Prerequisites. Learning Outcomes Parametric Curves 7.3 Introduction In this Section we eamine et another wa of defining curves - the parametric description. We shall see that this is, in some was, far more useful than either the Cartesian

More information

Math 461 Homework 8. Paul Hacking. November 27, 2018

Math 461 Homework 8. Paul Hacking. November 27, 2018 Math 461 Homework 8 Paul Hacking November 27, 2018 (1) Let S 2 = {(x, y, z) x 2 + y 2 + z 2 = 1} R 3 be the sphere with center the origin and radius 1. Let N = (0, 0, 1) S 2 be the north pole. Let F :

More information

Math 461 Homework 8 Paul Hacking November 27, 2018

Math 461 Homework 8 Paul Hacking November 27, 2018 (1) Let Math 461 Homework 8 Paul Hacking November 27, 2018 S 2 = {(x, y, z) x 2 +y 2 +z 2 = 1} R 3 be the sphere with center the origin and radius 1. Let N = (0, 0, 1) S 2 be the north pole. Let F : S

More information

Tensors, Fields Pt. 1 and the Lie Bracket Pt. 1

Tensors, Fields Pt. 1 and the Lie Bracket Pt. 1 Tensors, Fiels Pt. 1 an the Lie Bracket Pt. 1 PHYS 500 - Southern Illinois University September 8, 2016 PHYS 500 - Southern Illinois University Tensors, Fiels Pt. 1 an the Lie Bracket Pt. 1 September 8,

More information

Solutions of homework 1. 2 a) Using the stereographic projection from the north pole N = (0, 0, 1) introduce stereographic coordinates

Solutions of homework 1. 2 a) Using the stereographic projection from the north pole N = (0, 0, 1) introduce stereographic coordinates Solutions of homework 1 1 a) Using the stereographic projection from the north pole N (0, 1) introduce stereographic coordinate for the part of the circle S 1 ( + 1) without the north pole. b) Do the same

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

The AdS/CFT Correspondence PI It from Qubit Summer School: Mukund Rangamani

The AdS/CFT Correspondence PI It from Qubit Summer School: Mukund Rangamani Lecture The AS/CFT Corresponence PI It from Qubit Summer School: Mukun Rangamani Q. Large N expansion: Consier the following Lagrangian for a zero imensional fiel theory (matrix moel): L = (Tr (ΦΦ) + Tr

More information

SOME RESULTS ON THE GEOMETRY OF MINKOWSKI PLANE. Bing Ye Wu

SOME RESULTS ON THE GEOMETRY OF MINKOWSKI PLANE. Bing Ye Wu ARCHIVUM MATHEMATICUM (BRNO Tomus 46 (21, 177 184 SOME RESULTS ON THE GEOMETRY OF MINKOWSKI PLANE Bing Ye Wu Abstract. In this paper we stuy the geometry of Minkowski plane an obtain some results. We focus

More information

Lecture Introduction. 2 Examples of Measure Concentration. 3 The Johnson-Lindenstrauss Lemma. CS-621 Theory Gems November 28, 2012

Lecture Introduction. 2 Examples of Measure Concentration. 3 The Johnson-Lindenstrauss Lemma. CS-621 Theory Gems November 28, 2012 CS-6 Theory Gems November 8, 0 Lecture Lecturer: Alesaner Mąry Scribes: Alhussein Fawzi, Dorina Thanou Introuction Toay, we will briefly iscuss an important technique in probability theory measure concentration

More information

Implicit Differentiation

Implicit Differentiation Implicit Differentiation Implicit Differentiation Using the Chain Rule In the previous section we focuse on the erivatives of composites an saw that THEOREM 20 (Chain Rule) Suppose that u = g(x) is ifferentiable

More information

Math Notes on differentials, the Chain Rule, gradients, directional derivative, and normal vectors

Math Notes on differentials, the Chain Rule, gradients, directional derivative, and normal vectors Math 18.02 Notes on ifferentials, the Chain Rule, graients, irectional erivative, an normal vectors Tangent plane an linear approximation We efine the partial erivatives of f( xy, ) as follows: f f( x+

More information

Technische Universität Berlin Fakultät II Institut für Mathematik

Technische Universität Berlin Fakultät II Institut für Mathematik Technische Universität Berlin Fakultät II Institut für Mathematik Springborn, Kouřimská!!Trial exam!! Written Examination Geometry I Surname:.............................. First name:..............................

More information

CHAPTER 1 : DIFFERENTIABLE MANIFOLDS. 1.1 The definition of a differentiable manifold

CHAPTER 1 : DIFFERENTIABLE MANIFOLDS. 1.1 The definition of a differentiable manifold CHAPTER 1 : DIFFERENTIABLE MANIFOLDS 1.1 The efinition of a ifferentiable manifol Let M be a topological space. This means that we have a family Ω of open sets efine on M. These satisfy (1), M Ω (2) the

More information

1 Lecture 20: Implicit differentiation

1 Lecture 20: Implicit differentiation Lecture 20: Implicit ifferentiation. Outline The technique of implicit ifferentiation Tangent lines to a circle Derivatives of inverse functions by implicit ifferentiation Examples.2 Implicit ifferentiation

More information

The Mathematics of Maps Lecture 4. Dennis The The Mathematics of Maps Lecture 4 1/29

The Mathematics of Maps Lecture 4. Dennis The The Mathematics of Maps Lecture 4 1/29 The Mathematics of Maps Lecture 4 Dennis The The Mathematics of Maps Lecture 4 1/29 Mercator projection Dennis The The Mathematics of Maps Lecture 4 2/29 The Mercator projection (1569) Dennis The The Mathematics

More information

(a) 82 (b) 164 (c) 81 (d) 162 (e) 624 (f) 625 None of these. (c) 12 (d) 15 (e)

(a) 82 (b) 164 (c) 81 (d) 162 (e) 624 (f) 625 None of these. (c) 12 (d) 15 (e) Math 2 (Calculus I) Final Eam Form A KEY Multiple Choice. Fill in the answer to each problem on your computer-score answer sheet. Make sure your name, section an instructor are on that sheet.. Approimate

More information

Day 4: Motion Along a Curve Vectors

Day 4: Motion Along a Curve Vectors Day 4: Motion Along a Curve Vectors I give my stuents the following list of terms an formulas to know. Parametric Equations, Vectors, an Calculus Terms an Formulas to Know: If a smooth curve C is given

More information

Lecture 1b. Differential operators and orthogonal coordinates. Partial derivatives. Divergence and divergence theorem. Gradient. A y. + A y y dy. 1b.

Lecture 1b. Differential operators and orthogonal coordinates. Partial derivatives. Divergence and divergence theorem. Gradient. A y. + A y y dy. 1b. b. Partial erivatives Lecture b Differential operators an orthogonal coorinates Recall from our calculus courses that the erivative of a function can be efine as f ()=lim 0 or using the central ifference

More information

(7) Suppose α, β, γ are nonzero complex numbers such that α = β = γ.

(7) Suppose α, β, γ are nonzero complex numbers such that α = β = γ. January 22, 2011 COMPLEX ANALYSIS: PROBLEMS SHEET -1 M.THAMBAN NAIR (1) Show that C is a field under the addition and multiplication defined for complex numbers. (2) Show that the map f : R C defined by

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

11.7. Implicit Differentiation. Introduction. Prerequisites. Learning Outcomes

11.7. Implicit Differentiation. Introduction. Prerequisites. Learning Outcomes Implicit Differentiation 11.7 Introuction This Section introuces implicit ifferentiation which is use to ifferentiate functions expresse in implicit form (where the variables are foun together). Examples

More information

Further Differentiation and Applications

Further Differentiation and Applications Avance Higher Notes (Unit ) Prerequisites: Inverse function property; prouct, quotient an chain rules; inflexion points. Maths Applications: Concavity; ifferentiability. Real-Worl Applications: Particle

More information

DIFFERENTIAL GEOMETRY, LECTURE 15, JULY 10

DIFFERENTIAL GEOMETRY, LECTURE 15, JULY 10 DIFFERENTIAL GEOMETRY, LECTURE 15, JULY 10 5. Levi-Civita connection From now on we are intereste in connections on the tangent bunle T X of a Riemanninam manifol (X, g). Out main result will be a construction

More information

17.3. Parametric Curves. Introduction. Prerequisites. Learning Outcomes

17.3. Parametric Curves. Introduction. Prerequisites. Learning Outcomes Parametric Curves 17.3 Introduction In this section we eamine et another wa of defining curves - the parametric description. We shall see that this is, in some was, far more useful than either the Cartesian

More information

Lecture XII. where Φ is called the potential function. Let us introduce spherical coordinates defined through the relations

Lecture XII. where Φ is called the potential function. Let us introduce spherical coordinates defined through the relations Lecture XII Abstract We introuce the Laplace equation in spherical coorinates an apply the metho of separation of variables to solve it. This will generate three linear orinary secon orer ifferential equations:

More information

Solutions to Math 41 Second Exam November 4, 2010

Solutions to Math 41 Second Exam November 4, 2010 Solutions to Math 41 Secon Exam November 4, 2010 1. (13 points) Differentiate, using the metho of your choice. (a) p(t) = ln(sec t + tan t) + log 2 (2 + t) (4 points) Using the rule for the erivative of

More information

Math 1272 Solutions for Spring 2005 Final Exam. asked to find the limit of the sequence. This is equivalent to evaluating lim. lim.

Math 1272 Solutions for Spring 2005 Final Exam. asked to find the limit of the sequence. This is equivalent to evaluating lim. lim. Math 7 Solutions for Spring 5 Final Exam ) We are gien an infinite sequence for which the general term is a n 3 + 5n n + n an are 3 + 5n aske to fin the limit of the sequence. This is equialent to ealuating

More information

6 General properties of an autonomous system of two first order ODE

6 General properties of an autonomous system of two first order ODE 6 General properties of an autonomous system of two first orer ODE Here we embark on stuying the autonomous system of two first orer ifferential equations of the form ẋ 1 = f 1 (, x 2 ), ẋ 2 = f 2 (, x

More information

Calculus 4 Final Exam Review / Winter 2009

Calculus 4 Final Exam Review / Winter 2009 Calculus 4 Final Eam Review / Winter 9 (.) Set-up an iterate triple integral for the volume of the soli enclose between the surfaces: 4 an 4. DO NOT EVALUATE THE INTEGRAL! [Hint: The graphs of both surfaces

More information

Students need encouragement. So if a student gets an answer right, tell them it was a lucky guess. That way, they develop a good, lucky feeling.

Students need encouragement. So if a student gets an answer right, tell them it was a lucky guess. That way, they develop a good, lucky feeling. Chapter 8 Analytic Functions Stuents nee encouragement. So if a stuent gets an answer right, tell them it was a lucky guess. That way, they evelop a goo, lucky feeling. 1 8.1 Complex Derivatives -Jack

More information

Geometry and Motion, MA 134 Week 1

Geometry and Motion, MA 134 Week 1 Geometry and Motion, MA 134 Week 1 Mario J. Micallef Spring, 2007 Warning. These handouts are not intended to be complete lecture notes. They should be supplemented by your own notes and, importantly,

More information

The Three-dimensional Schödinger Equation

The Three-dimensional Schödinger Equation The Three-imensional Schöinger Equation R. L. Herman November 7, 016 Schröinger Equation in Spherical Coorinates We seek to solve the Schröinger equation with spherical symmetry using the metho of separation

More information

Some functions and their derivatives

Some functions and their derivatives Chapter Some functions an their erivatives. Derivative of x n for integer n Recall, from eqn (.6), for y = f (x), Also recall that, for integer n, Hence, if y = x n then y x = lim δx 0 (a + b) n = a n

More information

MAT389 Fall 2016, Problem Set 2

MAT389 Fall 2016, Problem Set 2 MAT389 Fall 2016, Problem Set 2 Circles in the Riemann sphere Recall that the Riemann sphere is defined as the set Let P be the plane defined b Σ = { (a, b, c) R 3 a 2 + b 2 + c 2 = 1 } P = { (a, b, c)

More information

1 Differentiable manifolds and smooth maps. (Solutions)

1 Differentiable manifolds and smooth maps. (Solutions) 1 Differentiable manifolds and smooth maps Solutions Last updated: March 17 2011 Problem 1 The state of the planar pendulum is entirely defined by the position of its moving end in the plane R 2 Since

More information

UNIT NUMBER DIFFERENTIATION 7 (Inverse hyperbolic functions) A.J.Hobson

UNIT NUMBER DIFFERENTIATION 7 (Inverse hyperbolic functions) A.J.Hobson JUST THE MATHS UNIT NUMBER 0.7 DIFFERENTIATION 7 (Inverse hyperbolic functions) by A.J.Hobson 0.7. Summary of results 0.7.2 The erivative of an inverse hyperbolic sine 0.7.3 The erivative of an inverse

More information

DIFFERENTIAL GEOMETRY OF CURVES AND SURFACES 7. Geodesics and the Theorem of Gauss-Bonnet

DIFFERENTIAL GEOMETRY OF CURVES AND SURFACES 7. Geodesics and the Theorem of Gauss-Bonnet A P Q O B DIFFERENTIAL GEOMETRY OF CURVES AND SURFACES 7. Geoesics an the Theorem of Gauss-Bonnet 7.. Geoesics on a Surface. The goal of this section is to give an answer to the following question. Question.

More information

Section 7.2. The Calculus of Complex Functions

Section 7.2. The Calculus of Complex Functions Section 7.2 The Calculus of Complex Functions In this section we will iscuss limits, continuity, ifferentiation, Taylor series in the context of functions which take on complex values. Moreover, we will

More information

12.11 Laplace s Equation in Cylindrical and

12.11 Laplace s Equation in Cylindrical and SEC. 2. Laplace s Equation in Cylinrical an Spherical Coorinates. Potential 593 2. Laplace s Equation in Cylinrical an Spherical Coorinates. Potential One of the most important PDEs in physics an engineering

More information

13.1: Vector-Valued Functions and Motion in Space, 14.1: Functions of Several Variables, and 14.2: Limits and Continuity in Higher Dimensions

13.1: Vector-Valued Functions and Motion in Space, 14.1: Functions of Several Variables, and 14.2: Limits and Continuity in Higher Dimensions 13.1: Vector-Value Functions an Motion in Space, 14.1: Functions of Several Variables, an 14.2: Limits an Continuity in Higher Dimensions TA: Sam Fleischer November 3 Section 13.1: Vector-Value Functions

More information

Math Implicit Differentiation. We have discovered (and proved) formulas for finding derivatives of functions like

Math Implicit Differentiation. We have discovered (and proved) formulas for finding derivatives of functions like Math 400 3.5 Implicit Differentiation Name We have iscovere (an prove) formulas for fining erivatives of functions like f x x 3x 4x. 3 This amounts to fining y for 3 y x 3x 4x. Notice that in this case,

More information

Aero III/IV Conformal Mapping

Aero III/IV Conformal Mapping Aero III/IV Conformal Mapping View complex function as a mapping Unlike a real function, a complex function w = f(z) cannot be represented by a curve. Instead it is useful to view it as a mapping. Write

More information

SOLUTIONS TO HOMEWORK ASSIGNMENT #2, Math 253

SOLUTIONS TO HOMEWORK ASSIGNMENT #2, Math 253 SOLUTIONS TO HOMEWORK ASSIGNMENT #, Math 5. Find the equation of a sphere if one of its diameters has end points (, 0, 5) and (5, 4, 7). The length of the diameter is (5 ) + ( 4 0) + (7 5) = =, so the

More information

AP Calculus AB One Last Mega Review Packet of Stuff. Take the derivative of the following. 1.) 3.) 5.) 7.) Determine the limit of the following.

AP Calculus AB One Last Mega Review Packet of Stuff. Take the derivative of the following. 1.) 3.) 5.) 7.) Determine the limit of the following. AP Calculus AB One Last Mega Review Packet of Stuff Name: Date: Block: Take the erivative of the following. 1.) x (sin (5x)).) x (etan(x) ) 3.) x (sin 1 ( x3 )) 4.) x (x3 5x) 4 5.) x ( ex sin(x) ) 6.)

More information

From the definition of a surface, each point has a neighbourhood U and a homeomorphism. U : ϕ U(U U ) ϕ U (U U )

From the definition of a surface, each point has a neighbourhood U and a homeomorphism. U : ϕ U(U U ) ϕ U (U U ) 3 Riemann surfaces 3.1 Definitions and examples From the definition of a surface, each point has a neighbourhood U and a homeomorphism ϕ U from U to an open set V in R 2. If two such neighbourhoods U,

More information

Math 2153, Exam III, Apr. 17, 2008

Math 2153, Exam III, Apr. 17, 2008 Math 53, Exam III, Apr. 7, 8 Name: Score: Each problem is worth 5 points. The total is 5 points. For series convergence or ivergence, please write own the name of the test you are using an etails of using

More information

Math 11 Fall 2016 Section 1 Monday, September 19, Definition: A vector parametric equation for the line parallel to vector v = x v, y v, z v

Math 11 Fall 2016 Section 1 Monday, September 19, Definition: A vector parametric equation for the line parallel to vector v = x v, y v, z v Math Fall 06 Section Monay, September 9, 06 First, some important points from the last class: Definition: A vector parametric equation for the line parallel to vector v = x v, y v, z v passing through

More information

The derivative of a function f(x) is another function, defined in terms of a limiting expression: f(x + δx) f(x)

The derivative of a function f(x) is another function, defined in terms of a limiting expression: f(x + δx) f(x) Y. D. Chong (2016) MH2801: Complex Methos for the Sciences 1. Derivatives The erivative of a function f(x) is another function, efine in terms of a limiting expression: f (x) f (x) lim x δx 0 f(x + δx)

More information

Conic Sections Session 3: Hyperbola

Conic Sections Session 3: Hyperbola Conic Sections Session 3: Hyperbola Toh Pee Choon NIE Oct 2017 Toh Pee Choon (NIE) Session 3: Hyperbola Oct 2017 1 / 16 Problem 3.1 1 Recall that an ellipse is defined as the locus of points P such that

More information

Conformal Mappings. Chapter Schwarz Lemma

Conformal Mappings. Chapter Schwarz Lemma Chapter 5 Conformal Mappings In this chapter we study analytic isomorphisms. An analytic isomorphism is also called a conformal map. We say that f is an analytic isomorphism of U with V if f is an analytic

More information

10.7. DIFFERENTIATION 7 (Inverse hyperbolic functions) A.J.Hobson

10.7. DIFFERENTIATION 7 (Inverse hyperbolic functions) A.J.Hobson JUST THE MATHS SLIDES NUMBER 0.7 DIFFERENTIATION 7 (Inverse hyperbolic functions) by A.J.Hobson 0.7. Summary of results 0.7.2 The erivative of an inverse hyperbolic sine 0.7.3 The erivative of an inverse

More information

Math Chapter 2 Essentials of Calculus by James Stewart Prepared by Jason Gaddis

Math Chapter 2 Essentials of Calculus by James Stewart Prepared by Jason Gaddis Math 231 - Chapter 2 Essentials of Calculus by James Stewart Prepare by Jason Gais Chapter 2 - Derivatives 21 - Derivatives an Rates of Change Definition A tangent to a curve is a line that intersects

More information

International Journal of Pure and Applied Mathematics Volume 35 No , ON PYTHAGOREAN QUADRUPLES Edray Goins 1, Alain Togbé 2

International Journal of Pure and Applied Mathematics Volume 35 No , ON PYTHAGOREAN QUADRUPLES Edray Goins 1, Alain Togbé 2 International Journal of Pure an Applie Mathematics Volume 35 No. 3 007, 365-374 ON PYTHAGOREAN QUADRUPLES Eray Goins 1, Alain Togbé 1 Department of Mathematics Purue University 150 North University Street,

More information

1.4.3 Elementary solutions to Laplace s equation in the spherical coordinates (Axially symmetric cases) (Griffiths 3.3.2)

1.4.3 Elementary solutions to Laplace s equation in the spherical coordinates (Axially symmetric cases) (Griffiths 3.3.2) 1.4.3 Elementary solutions to Laplace s equation in the spherical coorinates (Axially symmetric cases) (Griffiths 3.3.) In the spherical coorinates (r, θ, φ), the Laplace s equation takes the following

More information

Multivariable Calculus: Chapter 13: Topic Guide and Formulas (pgs ) * line segment notation above a variable indicates vector

Multivariable Calculus: Chapter 13: Topic Guide and Formulas (pgs ) * line segment notation above a variable indicates vector Multivariable Calculus: Chapter 13: Topic Guie an Formulas (pgs 800 851) * line segment notation above a variable inicates vector The 3D Coorinate System: Distance Formula: (x 2 x ) 2 1 + ( y ) ) 2 y 2

More information

Conformal Mapping Lecture 20 Conformal Mapping

Conformal Mapping Lecture 20 Conformal Mapping Let γ : [a, b] C be a smooth curve in a domain D. Let f (z) be a function defined at all points z on γ. Let C denotes the image of γ under the transformation w = f (z). The parametric equation of C is

More information

Solving the Schrödinger Equation for the 1 Electron Atom (Hydrogen-Like)

Solving the Schrödinger Equation for the 1 Electron Atom (Hydrogen-Like) Stockton Univeristy Chemistry Program, School of Natural Sciences an Mathematics 101 Vera King Farris Dr, Galloway, NJ CHEM 340: Physical Chemistry II Solving the Schröinger Equation for the 1 Electron

More information

Equations of lines in

Equations of lines in Roberto s Notes on Linear Algebra Chapter 6: Lines, planes an other straight objects Section 1 Equations of lines in What ou nee to know alrea: The ot prouct. The corresponence between equations an graphs.

More information

1 Second Facts About Spaces of Modular Forms

1 Second Facts About Spaces of Modular Forms April 30, :00 pm 1 Secon Facts About Spaces of Moular Forms We have repeately use facts about the imensions of the space of moular forms, mostly to give specific examples of an relations between moular

More information

OHSx XM521 Multivariable Differential Calculus: Homework Solutions 13.1

OHSx XM521 Multivariable Differential Calculus: Homework Solutions 13.1 OHSx XM521 Multivariable Differential Calculus: Homework Solutions 13.1 (37) If a bug walks on the sphere x 2 + y 2 + z 2 + 2x 2y 4z 3 = 0 how close and how far can it get from the origin? Solution: Complete

More information

TRANSVERSAL SURFACES OF TIMELIKE RULED SURFACES IN MINKOWSKI 3-SPACE IR

TRANSVERSAL SURFACES OF TIMELIKE RULED SURFACES IN MINKOWSKI 3-SPACE IR IJRRAS () November 0 wwwarpapresscom/volumes/volissue/ijrras 08pf TRANSVERSAL SURFACES OF TIMELIKE RULED SURFACES IN MINKOWSKI -SPACE Mehmet Öner Celal Bayar University, Faculty of Science an Arts, Department

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

Calculus of Variations

Calculus of Variations Calculus of Variations Lagrangian formalism is the main tool of theoretical classical mechanics. Calculus of Variations is a part of Mathematics which Lagrangian formalism is base on. In this section,

More information

Chapter 2 Lagrangian Modeling

Chapter 2 Lagrangian Modeling Chapter 2 Lagrangian Moeling The basic laws of physics are use to moel every system whether it is electrical, mechanical, hyraulic, or any other energy omain. In mechanics, Newton s laws of motion provie

More information

PDE Notes, Lecture #11

PDE Notes, Lecture #11 PDE Notes, Lecture # from Professor Jalal Shatah s Lectures Febuary 9th, 2009 Sobolev Spaces Recall that for u L loc we can efine the weak erivative Du by Du, φ := udφ φ C0 If v L loc such that Du, φ =

More information

INDIAN INSTITUTE OF TECHNOLOGY BOMBAY MA205 Complex Analysis Autumn 2012

INDIAN INSTITUTE OF TECHNOLOGY BOMBAY MA205 Complex Analysis Autumn 2012 INDIAN INSTITUTE OF TECHNOLOGY BOMBAY MA205 Complex Analysis Autumn 2012 September 5, 2012 Mapping Properties Lecture 13 We shall once again return to the study of general behaviour of holomorphic functions

More information

1 Differentiable manifolds and smooth maps. (Solutions)

1 Differentiable manifolds and smooth maps. (Solutions) 1 Differentiable manifolds and smooth maps Solutions Last updated: February 16 2012 Problem 1 a The projection maps a point P x y S 1 to the point P u 0 R 2 the intersection of the line NP with the x-axis

More information

6 Wave equation in spherical polar coordinates

6 Wave equation in spherical polar coordinates 6 Wave equation in spherical polar coorinates We now look at solving problems involving the Laplacian in spherical polar coorinates. The angular epenence of the solutions will be escribe by spherical harmonics.

More information

MATH Final Review

MATH Final Review MATH 1592 - Final Review 1 Chapter 7 1.1 Main Topics 1. Integration techniques: Fitting integrands to basic rules on page 485. Integration by parts, Theorem 7.1 on page 488. Guidelines for trigonometric

More information

Chapter 14 Hyperbolic geometry Math 4520, Fall 2017

Chapter 14 Hyperbolic geometry Math 4520, Fall 2017 Chapter 14 Hyperbolic geometry Math 4520, Fall 2017 So far we have talked mostly about the incidence structure of points, lines and circles. But geometry is concerned about the metric, the way things are

More information

Partial Differential Equations

Partial Differential Equations Chapter Partial Differential Equations. Introuction Have solve orinary ifferential equations, i.e. ones where there is one inepenent an one epenent variable. Only orinary ifferentiation is therefore involve.

More information

Physics 505 Electricity and Magnetism Fall 2003 Prof. G. Raithel. Problem Set 3. 2 (x x ) 2 + (y y ) 2 + (z + z ) 2

Physics 505 Electricity and Magnetism Fall 2003 Prof. G. Raithel. Problem Set 3. 2 (x x ) 2 + (y y ) 2 + (z + z ) 2 Physics 505 Electricity an Magnetism Fall 003 Prof. G. Raithel Problem Set 3 Problem.7 5 Points a): Green s function: Using cartesian coorinates x = (x, y, z), it is G(x, x ) = 1 (x x ) + (y y ) + (z z

More information

Exam 2 Review Solutions

Exam 2 Review Solutions Exam Review Solutions 1. True or False, an explain: (a) There exists a function f with continuous secon partial erivatives such that f x (x, y) = x + y f y = x y False. If the function has continuous secon

More information

Problem Sheet 2: Eigenvalues and eigenvectors and their use in solving linear ODEs

Problem Sheet 2: Eigenvalues and eigenvectors and their use in solving linear ODEs Problem Sheet 2: Eigenvalues an eigenvectors an their use in solving linear ODEs If you fin any typos/errors in this problem sheet please email jk28@icacuk The material in this problem sheet is not examinable

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

The rotating Pulfrich effect derivation of equations

The rotating Pulfrich effect derivation of equations The rotating Pulfrich effect erivation of equations RWD Nickalls, Department of Anaesthesia, Nottingham University Hospitals, City Hospital Campus, Nottingham, UK. ick@nickalls.org www.nickalls.org 3 The

More information

12 th Annual Johns Hopkins Math Tournament Saturday, February 19, 2011

12 th Annual Johns Hopkins Math Tournament Saturday, February 19, 2011 1 th Annual Johns Hopkins Math Tournament Saturay, February 19, 011 Geometry Subject Test 1. [105] Let D x,y enote the half-isk of raius 1 with its curve bounary externally tangent to the unit circle at

More information

18 EVEN MORE CALCULUS

18 EVEN MORE CALCULUS 8 EVEN MORE CALCULUS Chapter 8 Even More Calculus Objectives After stuing this chapter you shoul be able to ifferentiate an integrate basic trigonometric functions; unerstan how to calculate rates of change;

More information

Physics Courseware Electromagnetism

Physics Courseware Electromagnetism Phsics Courseware Electromagnetism Electric potential Problem.- a) Fin the electric potential at points P, P an P prouce b the three charges Q, Q an Q. b) Are there an points where the electric potential

More information

Chapter 3 Elementary Functions

Chapter 3 Elementary Functions Chapter 3 Elementary Functions In this chapter, we will consier elementary functions of a complex variable. We will introuce complex exponential, trigonometric, hyperbolic, an logarithmic functions. 23.

More information

Exercises involving elementary functions

Exercises involving elementary functions 017:11:0:16:4:09 c M K Warby MA3614 Complex variable methods and applications 1 Exercises involving elementary functions 1 This question was in the class test in 016/7 and was worth 5 marks a) Let z +

More information

1. Aufgabenblatt zur Vorlesung Probability Theory

1. Aufgabenblatt zur Vorlesung Probability Theory 24.10.17 1. Aufgabenblatt zur Vorlesung By (Ω, A, P ) we always enote the unerlying probability space, unless state otherwise. 1. Let r > 0, an efine f(x) = 1 [0, [ (x) exp( r x), x R. a) Show that p f

More information

Rule ST1 (Symmetry). α β = β α for 1-forms α and β. Like the exterior product, the symmetric tensor product is also linear in each slot :

Rule ST1 (Symmetry). α β = β α for 1-forms α and β. Like the exterior product, the symmetric tensor product is also linear in each slot : 2. Metrics as Symmetric Tensors So far we have studied exterior products of 1-forms, which obey the rule called skew symmetry: α β = β α. There is another operation for forming something called the symmetric

More information

ARAB ACADEMY FOR SCIENCE TECHNOLOGY AND MARITIME TRANSPORT

ARAB ACADEMY FOR SCIENCE TECHNOLOGY AND MARITIME TRANSPORT ARAB ACADEMY FOR SCIENCE TECHNOLOGY AND MARITIME TRANSPORT Course: Math For Engineering Winter 8 Lecture Notes By Dr. Mostafa Elogail Page Lecture [ Functions / Graphs of Rational Functions] Functions

More information

BLOW-UP FORMULAS FOR ( 2)-SPHERES

BLOW-UP FORMULAS FOR ( 2)-SPHERES BLOW-UP FORMULAS FOR 2)-SPHERES ROGIER BRUSSEE In this note we give a universal formula for the evaluation of the Donalson polynomials on 2)-spheres, i.e. smooth spheres of selfintersection 2. Note that

More information

Short Intro to Coordinate Transformation

Short Intro to Coordinate Transformation Short Intro to Coorinate Transformation 1 A Vector A vector can basically be seen as an arrow in space pointing in a specific irection with a specific length. The following problem arises: How o we represent

More information

Math 115 Section 018 Course Note

Math 115 Section 018 Course Note Course Note 1 General Functions Definition 1.1. A function is a rule that takes certain numbers as inputs an assigns to each a efinite output number. The set of all input numbers is calle the omain of

More information

x f(x) x f(x) approaching 1 approaching 0.5 approaching 1 approaching 0.

x f(x) x f(x) approaching 1 approaching 0.5 approaching 1 approaching 0. Engineering Mathematics 2 26 February 2014 Limits of functions Consier the function 1 f() = 1. The omain of this function is R + \ {1}. The function is not efine at 1. What happens when is close to 1?

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

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

Length of a Plane Curve (Arc Length)

Length of a Plane Curve (Arc Length) Length of a Plane Curve (Arc Length) SUGGESTED REFERENCE MATERIAL: As you work through the problems liste below, you shoul reference Chapter 6. of the recommene textbook (or the equivalent chapter in your

More information

Strauss PDEs 2e: Section Exercise 6 Page 1 of 5

Strauss PDEs 2e: Section Exercise 6 Page 1 of 5 Strauss PDEs 2e: Section 4.3 - Exercise 6 Page 1 of 5 Exercise 6 If a 0 = a l = a in the Robin problem, show that: (a) There are no negative eigenvalues if a 0, there is one if 2/l < a < 0, an there are

More information

8. Hyperbolic triangles

8. Hyperbolic triangles 8. Hyperbolic triangles Note: This year, I m not doing this material, apart from Pythagoras theorem, in the lectures (and, as such, the remainder isn t examinable). I ve left the material as Lecture 8

More information

You should also review L Hôpital s Rule, section 3.6; follow the homework link above for exercises.

You should also review L Hôpital s Rule, section 3.6; follow the homework link above for exercises. BEFORE You Begin Calculus II If it has been awhile since you ha Calculus, I strongly suggest that you refresh both your ifferentiation an integration skills. I woul also like to remin you that in Calculus,

More information

Unit #6 - Families of Functions, Taylor Polynomials, l Hopital s Rule

Unit #6 - Families of Functions, Taylor Polynomials, l Hopital s Rule Unit # - Families of Functions, Taylor Polynomials, l Hopital s Rule Some problems an solutions selecte or aapte from Hughes-Hallett Calculus. Critical Points. Consier the function f) = 54 +. b) a) Fin

More information

23 Implicit differentiation

23 Implicit differentiation 23 Implicit ifferentiation 23.1 Statement The equation y = x 2 + 3x + 1 expresses a relationship between the quantities x an y. If a value of x is given, then a corresponing value of y is etermine. For

More information

(6, 4, 0) = (3, 2, 0). Find the equation of the sphere that has the line segment from P to Q as a diameter.

(6, 4, 0) = (3, 2, 0). Find the equation of the sphere that has the line segment from P to Q as a diameter. Solutions Review for Eam #1 Math 1260 1. Consider the points P = (2, 5, 1) and Q = (4, 1, 1). (a) Find the distance from P to Q. Solution. dist(p, Q) = (4 2) 2 + (1 + 5) 2 + (1 + 1) 2 = 4 + 36 + 4 = 44

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