CS Tutorial 5 - Differential Geometry I - Surfaces

Size: px
Start display at page:

Download "CS Tutorial 5 - Differential Geometry I - Surfaces"

Transcription

1 Numerical Geometry of Images Tutorial 5 Differential Geometry II Surfaces c 2009

2 Parameterized surfaces A parameterized surface X : U R 2 R 3 a differentiable map 1 X from an open set U R 2 to R 3. Explicitly, X (U) is written as X (u, v) = (x(u, v), y(u, v), z(u, v)). X (U) R 3 is called the trace of X. 1 X (u, v) is called differentiable if x(u, v), y(u, v) and z(u, v) are differentiable functions w.r.t. the parameters u, v.

3 Parameterizations of a sphere - examples 2 (a) (b) (c) Figure: (a) Sphere in R 3. (b) Six overlapping parameterization of a kind X (x, y) = (x, y, ) 1 x 2 y 2. (c) X (θ, φ) = (sin θ cos φ, sin θ sin φ, cos θ). 2 Differential geometry of curves and surfaces, by Manfredo P. do Carmo

4 Differential of X Let X : U R n R m be a differential map. For each p U we will define the differential of X at p by dx p : U R n R m Let w R n and let α : ( ɛ, ɛ) U be a differential curve such that α(0) = p, α (0) = w. An image of α in R m s given by Then: β = X α( ɛ, ɛ) R m dx p (w) = β (0)

5 Differential of X : illustration ε v w X( p) z ( ) dx w p ε 0 α p u X X α = β y x

6 Calculation of the differential in R 3 Let X : U R 2 R 3 be a differential map. α(t) = (u(t), v(t)) β(t) = X α(t) = (x (u(t), v(t)), y (u(t), v(t)), z (u(t), v(t))) β (0) = x u y u z u x v y v z v ( du dt dv dt ) = dx p (w) Note: dx p (w) depends only on w, and not on the choice of α(t).

7 Exercise: df p calculation Calculate df p for F (u, v) = ( u 2 v 2, 2uv ), (u, v) R 2. Solution: df p = x = u 2 v 2, y = 2uv ( x u y u x v y v df (1,1) (2, 3) = df p ( 1 1 ) ( ) 2x 2y = 2y 2x ) = ( 2, 10)

8 Regular parameterization, Tangent space, Normal We will say that a differential parameterization X (U) is regular if X u (u, v) and X v (u, v) are linearly independent for all (u, v) U. Tangent plane (space) at p: a plane T p containing all the tangents to curves passing through the point p S. The tangent plane is spanned by the vectors X u (u, v), X v (u, v). Surface normal: a unit vector orthogonal to the tangent plane at the point p, defined by N(p) = X u X v X u X v (p)

9 Surfaces in R 3 - examples

10 Exercise: tangent space, normal Calculate the equation of the tangent plane of a surface which is a graph of a differentiable function z = f (x, y), at the point (x 0, y 0 ). Solution: X (x, y) = (x, y, f (x, y)) X x (x, y) = (1, 0, f x (x, y)) X y (x, y) = (0, 1, f y (x, y)) N = X u X v X u X v = ( f x, f y, 1) fx 2 + fy Equation of a plane passing through (x 0, y 0 ) and perpendicular to N(x 0, y 0 ) is: f x (x 0, y 0 )(x x 0 ) + f y (x 0, y 0 )(y y 0 ) (z f (x 0, y 0 )) = 0

11 The first fundamental form In order to measure local distances on the regular surface S, we assign an inner product on the tangent plane T p of S at every point p. The first fundamental form: a quadratic form I p : T p (S) T p (S) R, given by I p (w 1, w 2 ) = w 1, w 2 p. <, > p is a standard inner product of R 3 ; p stands for the tangent plane T p of the surface S at the point p. The form I p (w 1, w 2 ) is bilinear, symmetric and positive-definite.

12 The first fundamental form in terms of X u, X v Let α 1 (t) = X (u 1 (t), v 1 (t)) and α 2 (t) = X (u 2 (t), v 2 (t)) be two differential curves such that α 1 (0) = α 2 (0) = p, α 1(0) = w 1, α 2(0) = w 2. The first fundamental form is given by: I p (w 1, w 2 ) = α 1(0), α 2(0) = X u u 1 + X v v 1, X u u 2 + X v v 2 ( ) u T ( ) ( ) = 1 Xu, X u X u, X v u 2 v 1 X v, X u X v, X v v 2 ( ) u T ( ) ( ) = 1 E F u 2 v 1 F G v 2

13 The first fundamental form - alternative notation ( E F F G ) ( g11 g = 12 g 21 g 22 ) = ( Xu, X u X u, X v X v, X u X v, X v ) In coordinate notation: I p (w 1, w 2 ) = 2 2 g ij w 1 i w j 2 = g ij w 1 i w j 2 i=1 j=1 where we use the Einstein summation convention, according to which identical sub- and super-scripts are summed up; w k = (u k, v k ), k = 1, 2.

14 Exercise: calculation of I p Calculate the first fundamental form of a unit sphere parameterized by X (θ, φ) = (sin θ cos φ, sin θ sin φ, cos θ) Solution: X θ = (cos θ cos φ, cos θ sin φ, sin θ) X φ = (sin θ sin φ, sin θ cos φ, 0) E = X θ, X θ = cos 2 θ cos 2 φ + cos 2 θ sin 2 φ + sin 2 θ = 1 F = X θ, X φ = cos θ cos φ sin θ sin φ + cos θ sin φ sin θ cos φ = 0 G = X φ, X φ = sin 2 θ sin 2 φ + sin 2 θ cos 2 φ = sin 2 θ

15 Length calculation The length of a parameterized curve β : [0, T ] S is given by s(t) = t 0 β ( t) d t = t 0 I p (β, β )d t Given that α(t) = (u(t), v(t)), β(t) = X α(t), s(t) = t 0 E(u ) 2 + 2Fu v + G(v ) 2 d t Also, local element of the arclength is given by ds 2 = Edu 2 + 2Fdudv + Gdv 2

16 Area calculation Area of a bounded region R of a regular surface S = X (U) is given by A(R) = X u X v dudv, Q = X 1 (R) Q From the equality X u X v 2 + X u, X v 2 = X u 2 X v 2 it follows that X u X v = EG F 2 Note that EG F 2 > 0, by definition (prove).

17 Exercise: arclength and area measured on a sphere Calculate ds 2 and da = X u X v dθdφ of a unit sphere parameterized by X (θ, φ) = (sin θ cos φ, sin θ sin φ, cos θ) Solution: the first fundamental form of a sphere is given by ( ) ( ) E F 1 0 = F G 0 sin 2 θ Therefore: ds 2 = Edθ 2 + 2Fdθdφ + Gdφ 2 = dθ 2 + sin 2 θdφ 2 da = EG F 2 dθdφ = sin 2 θdθdφ

18 Orientation of surfaces We saw that a surface normal at point p S is defined by N(p) = X u X v X u X v (p) We will say that a regular surface S is orientable if and only if there exist a differentiable field of unit normal vectors N : S R 3 on S. Orientable surfaces: sphere, paper roll. Non-orientable surface: Möbius strip.

Chapter 4. The First Fundamental Form (Induced Metric)

Chapter 4. The First Fundamental Form (Induced Metric) Chapter 4. The First Fundamental Form (Induced Metric) We begin with some definitions from linear algebra. Def. Let V be a vector space (over IR). A bilinear form on V is a map of the form B : V V IR which

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

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

The First Fundamental Form

The First Fundamental Form The First Fundamental Form Outline 1. Bilinear Forms Let V be a vector space. A bilinear form on V is a function V V R that is linear in each variable separately. That is,, is bilinear if αu + β v, w αu,

More information

Surface x(u, v) and curve α(t) on it given by u(t) & v(t). Math 4140/5530: Differential Geometry

Surface x(u, v) and curve α(t) on it given by u(t) & v(t). Math 4140/5530: Differential Geometry Surface x(u, v) and curve α(t) on it given by u(t) & v(t). α du dv (t) x u dt + x v dt Surface x(u, v) and curve α(t) on it given by u(t) & v(t). α du dv (t) x u dt + x v dt ( ds dt )2 Surface x(u, v)

More information

Practice Final Solutions

Practice Final Solutions Practice Final Solutions Math 1, Fall 17 Problem 1. Find a parameterization for the given curve, including bounds on the parameter t. Part a) The ellipse in R whose major axis has endpoints, ) and 6, )

More information

Dierential Geometry Curves and surfaces Local properties Geometric foundations (critical for visual modeling and computing) Quantitative analysis Algo

Dierential Geometry Curves and surfaces Local properties Geometric foundations (critical for visual modeling and computing) Quantitative analysis Algo Dierential Geometry Curves and surfaces Local properties Geometric foundations (critical for visual modeling and computing) Quantitative analysis Algorithm development Shape control and interrogation Curves

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

7.1 Tangent Planes; Differentials of Maps Between

7.1 Tangent Planes; Differentials of Maps Between Chapter 7 Tangent Planes Reading: Do Carmo sections 2.4 and 3.2 Today I am discussing 1. Differentials of maps between surfaces 2. Geometry of Gauss map 7.1 Tangent Planes; Differentials of Maps Between

More information

Introduction to Algebraic and Geometric Topology Week 14

Introduction to Algebraic and Geometric Topology Week 14 Introduction to Algebraic and Geometric Topology Week 14 Domingo Toledo University of Utah Fall 2016 Computations in coordinates I Recall smooth surface S = {f (x, y, z) =0} R 3, I rf 6= 0 on S, I Chart

More information

9.1 Mean and Gaussian Curvatures of Surfaces

9.1 Mean and Gaussian Curvatures of Surfaces Chapter 9 Gauss Map II 9.1 Mean and Gaussian Curvatures of Surfaces in R 3 We ll assume that the curves are in R 3 unless otherwise noted. We start off by quoting the following useful theorem about self

More information

Summary for Vector Calculus and Complex Calculus (Math 321) By Lei Li

Summary for Vector Calculus and Complex Calculus (Math 321) By Lei Li Summary for Vector alculus and omplex alculus (Math 321) By Lei Li 1 Vector alculus 1.1 Parametrization urves, surfaces, or volumes can be parametrized. Below, I ll talk about 3D case. Suppose we use e

More information

Figure 25:Differentials of surface.

Figure 25:Differentials of surface. 2.5. Change of variables and Jacobians In the previous example we saw that, once we have identified the type of coordinates which is best to use for solving a particular problem, the next step is to do

More information

Math 212-Lecture 8. The chain rule with one independent variable

Math 212-Lecture 8. The chain rule with one independent variable Math 212-Lecture 8 137: The multivariable chain rule The chain rule with one independent variable w = f(x, y) If the particle is moving along a curve x = x(t), y = y(t), then the values that the particle

More information

Change of Variables, Parametrizations, Surface Integrals

Change of Variables, Parametrizations, Surface Integrals Chapter 8 Change of Variables, Parametrizations, Surface Integrals 8. he transformation formula In evaluating any integral, if the integral depends on an auxiliary function of the variables involved, it

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

Chapter 14. Basics of The Differential Geometry of Surfaces. Introduction. Parameterized Surfaces. The First... Home Page. Title Page.

Chapter 14. Basics of The Differential Geometry of Surfaces. Introduction. Parameterized Surfaces. The First... Home Page. Title Page. Chapter 14 Basics of The Differential Geometry of Surfaces Page 649 of 681 14.1. Almost all of the material presented in this chapter is based on lectures given by Eugenio Calabi in an upper undergraduate

More information

Topic 5.6: Surfaces and Surface Elements

Topic 5.6: Surfaces and Surface Elements Math 275 Notes Topic 5.6: Surfaces and Surface Elements Textbook Section: 16.6 From the Toolbox (what you need from previous classes): Using vector valued functions to parametrize curves. Derivatives of

More information

Lecture 13 The Fundamental Forms of a Surface

Lecture 13 The Fundamental Forms of a Surface Lecture 13 The Fundamental Forms of a Surface In the following we denote by F : O R 3 a parametric surface in R 3, F(u, v) = (x(u, v), y(u, v), z(u, v)). We denote partial derivatives with respect to the

More information

Gradient, Divergence and Curl in Curvilinear Coordinates

Gradient, Divergence and Curl in Curvilinear Coordinates Gradient, Divergence and Curl in Curvilinear Coordinates Although cartesian orthogonal coordinates are very intuitive and easy to use, it is often found more convenient to work with other coordinate systems.

More information

Name: SOLUTIONS Date: 11/9/2017. M20550 Calculus III Tutorial Worksheet 8

Name: SOLUTIONS Date: 11/9/2017. M20550 Calculus III Tutorial Worksheet 8 Name: SOLUTIONS Date: /9/7 M55 alculus III Tutorial Worksheet 8. ompute R da where R is the region bounded by x + xy + y 8 using the change of variables given by x u + v and y v. Solution: We know R is

More information

HOMEWORK 2 - SOLUTIONS

HOMEWORK 2 - SOLUTIONS HOMEWORK 2 - SOLUTIONS - 2012 ANDRÉ NEVES Exercise 15 of Chapter 2.3 of Do Carmo s book: Okay, I have no idea why I set this one because it is similar to another one from the previous homework. I might

More information

f(p i )Area(T i ) F ( r(u, w) ) (r u r w ) da

f(p i )Area(T i ) F ( r(u, w) ) (r u r w ) da MAH 55 Flux integrals Fall 16 1. Review 1.1. Surface integrals. Let be a surface in R. Let f : R be a function defined on. efine f ds = f(p i Area( i lim mesh(p as a limit of Riemann sums over sampled-partitions.

More information

Vector Calculus handout

Vector Calculus handout Vector Calculus handout The Fundamental Theorem of Line Integrals Theorem 1 (The Fundamental Theorem of Line Integrals). Let C be a smooth curve given by a vector function r(t), where a t b, and let f

More information

Chapter 5. The Second Fundamental Form

Chapter 5. The Second Fundamental Form Chapter 5. The Second Fundamental Form Directional Derivatives in IR 3. Let f : U IR 3 IR be a smooth function defined on an open subset of IR 3. Fix p U and X T p IR 3. The directional derivative of f

More information

1 The Differential Geometry of Surfaces

1 The Differential Geometry of Surfaces 1 The Differential Geometry of Surfaces Three-dimensional objects are bounded by surfaces. This section reviews some of the basic definitions and concepts relating to the geometry of smooth surfaces. 1.1

More information

51. General Surface Integrals

51. General Surface Integrals 51. General urface Integrals The area of a surface in defined parametrically by r(u, v) = x(u, v), y(u, v), z(u, v) over a region of integration in the input-variable plane is given by d = r u r v da.

More information

Sec. 1.1: Basics of Vectors

Sec. 1.1: Basics of Vectors Sec. 1.1: Basics of Vectors Notation for Euclidean space R n : all points (x 1, x 2,..., x n ) in n-dimensional space. Examples: 1. R 1 : all points on the real number line. 2. R 2 : all points (x 1, x

More information

Totally quasi-umbilic timelike surfaces in R 1,2

Totally quasi-umbilic timelike surfaces in R 1,2 Totally quasi-umbilic timelike surfaces in R 1,2 Jeanne N. Clelland, University of Colorado AMS Central Section Meeting Macalester College April 11, 2010 Definition: Three-dimensional Minkowski space R

More information

Multiple Integrals and Vector Calculus: Synopsis

Multiple Integrals and Vector Calculus: Synopsis Multiple Integrals and Vector Calculus: Synopsis Hilary Term 28: 14 lectures. Steve Rawlings. 1. Vectors - recap of basic principles. Things which are (and are not) vectors. Differentiation and integration

More information

Department of Aerospace Engineering AE602 Mathematics for Aerospace Engineers Assignment No. 6

Department of Aerospace Engineering AE602 Mathematics for Aerospace Engineers Assignment No. 6 Department of Aerospace Engineering AE Mathematics for Aerospace Engineers Assignment No.. Find the best least squares solution x to x, x 5. What error E is minimized? heck that the error vector ( x, 5

More information

Figure 21:The polar and Cartesian coordinate systems.

Figure 21:The polar and Cartesian coordinate systems. Figure 21:The polar and Cartesian coordinate systems. Coordinate systems in R There are three standard coordinate systems which are used to describe points in -dimensional space. These coordinate systems

More information

Metrics on Surfaces. Chapter The Intuitive Idea of Distance

Metrics on Surfaces. Chapter The Intuitive Idea of Distance Chapter 12 Metrics on Surfaces In this chapter, we begin the study of the geometry of surfaces from the point of view of distance and area. When mathematicians began to study surfaces at the end of the

More information

Green s Theorem. MATH 311, Calculus III. J. Robert Buchanan. Fall Department of Mathematics. J. Robert Buchanan Green s Theorem

Green s Theorem. MATH 311, Calculus III. J. Robert Buchanan. Fall Department of Mathematics. J. Robert Buchanan Green s Theorem Green s Theorem MATH 311, alculus III J. obert Buchanan Department of Mathematics Fall 2011 Main Idea Main idea: the line integral around a positively oriented, simple closed curve is related to a double

More information

MATH503 - HOMEWORK #2. v k. + v i. (fv i ) = f v i. + v k. ) + u j (ɛ ijk. ) u j (ɛ jik

MATH503 - HOMEWORK #2. v k. + v i. (fv i ) = f v i. + v k. ) + u j (ɛ ijk. ) u j (ɛ jik 1 KO UNIVERITY Mon April 18, ollege of Arts and ciences Handout # Department of Physics Instructor: Alkan Kabakço lu MATH - HOMEWORK # 1 ( f) = Using Einstein notation and expressing x, y, x as e 1, e,

More information

MATHEMATICS FOR ENGINEERING DIFFERENTIATION TUTORIAL 2 ADVANCED DIFFERENTIATION

MATHEMATICS FOR ENGINEERING DIFFERENTIATION TUTORIAL 2 ADVANCED DIFFERENTIATION MATHEMATICS FOR ENGINEERING DIFFERENTIATION TUTORIAL ADVANCED DIFFERENTIATION CONTENTS Function of a Function Differentiation of a Sum Differentiation of a Proct Differentiation of a Quotient Turning Points

More information

Notes on Cartan s Method of Moving Frames

Notes on Cartan s Method of Moving Frames Math 553 σιι June 4, 996 Notes on Cartan s Method of Moving Frames Andrejs Treibergs The method of moving frames is a very efficient way to carry out computations on surfaces Chern s Notes give an elementary

More information

HILBERT S THEOREM ON THE HYPERBOLIC PLANE

HILBERT S THEOREM ON THE HYPERBOLIC PLANE HILBET S THEOEM ON THE HYPEBOLIC PLANE MATTHEW D. BOWN Abstract. We recount a proof of Hilbert s result that a complete geometric surface of constant negative Gaussian curvature cannot be isometrically

More information

= π + sin π = π + 0 = π, so the object is moving at a speed of π feet per second after π seconds. (c) How far does it go in π seconds?

= π + sin π = π + 0 = π, so the object is moving at a speed of π feet per second after π seconds. (c) How far does it go in π seconds? Mathematics 115 Professor Alan H. Stein April 18, 005 SOLUTIONS 1. Define what is meant by an antiderivative or indefinite integral of a function f(x). Solution: An antiderivative or indefinite integral

More information

CURRENT MATERIAL: Vector Calculus.

CURRENT MATERIAL: Vector Calculus. Math 275, section 002 (Ultman) Fall 2011 FINAL EXAM REVIEW The final exam will be held on Wednesday 14 December from 10:30am 12:30pm in our regular classroom. You will be allowed both sides of an 8.5 11

More information

Multiple Integrals and Vector Calculus (Oxford Physics) Synopsis and Problem Sets; Hilary 2015

Multiple Integrals and Vector Calculus (Oxford Physics) Synopsis and Problem Sets; Hilary 2015 Multiple Integrals and Vector Calculus (Oxford Physics) Ramin Golestanian Synopsis and Problem Sets; Hilary 215 The outline of the material, which will be covered in 14 lectures, is as follows: 1. Introduction

More information

Map Projections. Jim Emery. Revision 7/21/ The Earth Ellipsoid 2. 2 The Fundamental Quadratic Forms of a Surface 6

Map Projections. Jim Emery. Revision 7/21/ The Earth Ellipsoid 2. 2 The Fundamental Quadratic Forms of a Surface 6 Map Projections Jim Emery Revision 7/21/2004 Contents 1 The Earth Ellipsoid 2 2 The Fundamental Quadratic Forms of a Surface 6 3 Principal Directions On A Surface 9 4 Principal Normal Curvatures on the

More information

HOMEWORK 3 MA1132: ADVANCED CALCULUS, HILARY 2017

HOMEWORK 3 MA1132: ADVANCED CALCULUS, HILARY 2017 HOMEWORK MA112: ADVANCED CALCULUS, HILARY 2017 (1) A particle moves along a curve in R with position function given by r(t) = (e t, t 2 + 1, t). Find the velocity v(t), the acceleration a(t), the speed

More information

e x3 dx dy. 0 y x 2, 0 x 1.

e x3 dx dy. 0 y x 2, 0 x 1. Problem 1. Evaluate by changing the order of integration y e x3 dx dy. Solution:We change the order of integration over the region y x 1. We find and x e x3 dy dx = y x, x 1. x e x3 dx = 1 x=1 3 ex3 x=

More information

Instructions: No books. No notes. Non-graphing calculators only. You are encouraged, although not required, to show your work.

Instructions: No books. No notes. Non-graphing calculators only. You are encouraged, although not required, to show your work. Exam 3 Math 850-007 Fall 04 Odenthal Name: Instructions: No books. No notes. Non-graphing calculators only. You are encouraged, although not required, to show your work.. Evaluate the iterated integral

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

PDF Created with deskpdf PDF Writer - Trial ::

PDF Created with deskpdf PDF Writer - Trial :: y 3 5 Graph of f ' x 76. The graph of f ', the derivative f, is shown above for x 5. n what intervals is f increasing? (A) [, ] only (B) [, 3] (C) [3, 5] only (D) [0,.5] and [3, 5] (E) [, ], [, ], and

More information

Math 234 Final Exam (with answers) Spring 2017

Math 234 Final Exam (with answers) Spring 2017 Math 234 Final Exam (with answers) pring 217 1. onsider the points A = (1, 2, 3), B = (1, 2, 2), and = (2, 1, 4). (a) [6 points] Find the area of the triangle formed by A, B, and. olution: One way to solve

More information

MA102: Multivariable Calculus

MA102: Multivariable Calculus MA102: Multivariable Calculus Rupam Barman and Shreemayee Bora Department of Mathematics IIT Guwahati Differentiability of f : U R n R m Definition: Let U R n be open. Then f : U R n R m is differentiable

More information

1. (a) (5 points) Find the unit tangent and unit normal vectors T and N to the curve. r (t) = 3 cos t, 0, 3 sin t, r ( 3π

1. (a) (5 points) Find the unit tangent and unit normal vectors T and N to the curve. r (t) = 3 cos t, 0, 3 sin t, r ( 3π 1. a) 5 points) Find the unit tangent and unit normal vectors T and N to the curve at the point P 3, 3π, r t) 3 cos t, 4t, 3 sin t 3 ). b) 5 points) Find curvature of the curve at the point P. olution:

More information

AN INTRODUCTION TO CURVILINEAR ORTHOGONAL COORDINATES

AN INTRODUCTION TO CURVILINEAR ORTHOGONAL COORDINATES AN INTRODUCTION TO CURVILINEAR ORTHOGONAL COORDINATES Overview Throughout the first few weeks of the semester, we have studied vector calculus using almost exclusively the familiar Cartesian x,y,z coordinate

More information

d F = (df E 3 ) E 3. (4.1)

d F = (df E 3 ) E 3. (4.1) 4. The Second Fundamental Form In the last section we developed the theory of intrinsic geometry of surfaces by considering the covariant differential d F, that is, the tangential component of df for a

More information

DO NOT BEGIN THIS TEST UNTIL INSTRUCTED TO START

DO NOT BEGIN THIS TEST UNTIL INSTRUCTED TO START Math 265 Student name: KEY Final Exam Fall 23 Instructor & Section: This test is closed book and closed notes. A (graphing) calculator is allowed for this test but cannot also be a communication device

More information

THEODORE VORONOV DIFFERENTIAL GEOMETRY. Spring 2009

THEODORE VORONOV DIFFERENTIAL GEOMETRY. Spring 2009 [under construction] 8 Parallel transport 8.1 Equation of parallel transport Consider a vector bundle E B. We would like to compare vectors belonging to fibers over different points. Recall that this was

More information

16.5 Surface Integrals of Vector Fields

16.5 Surface Integrals of Vector Fields 16.5 Surface Integrals of Vector Fields Lukas Geyer Montana State University M73, Fall 011 Lukas Geyer (MSU) 16.5 Surface Integrals of Vector Fields M73, Fall 011 1 / 19 Parametrized Surfaces Definition

More information

Sample Final Questions: Solutions Math 21B, Winter y ( y 1)(1 + y)) = A y + B

Sample Final Questions: Solutions Math 21B, Winter y ( y 1)(1 + y)) = A y + B Sample Final Questions: Solutions Math 2B, Winter 23. Evaluate the following integrals: tan a) y y dy; b) x dx; c) 3 x 2 + x dx. a) We use partial fractions: y y 3 = y y ) + y)) = A y + B y + C y +. Putting

More information

Definition of Derivative

Definition of Derivative Definition of Derivative The derivative of the function f with respect to the variable x is the function ( ) fʹ x whose value at xis ( x) fʹ = lim provided the limit exists. h 0 ( + ) ( ) f x h f x h Slide

More information

Note: Each problem is worth 14 points except numbers 5 and 6 which are 15 points. = 3 2

Note: Each problem is worth 14 points except numbers 5 and 6 which are 15 points. = 3 2 Math Prelim II Solutions Spring Note: Each problem is worth points except numbers 5 and 6 which are 5 points. x. Compute x da where is the region in the second quadrant between the + y circles x + y and

More information

DIFFERENTIAL GEOMETRY OF CURVES AND SURFACES 5. The Second Fundamental Form of a Surface

DIFFERENTIAL GEOMETRY OF CURVES AND SURFACES 5. The Second Fundamental Form of a Surface DIFFERENTIAL GEOMETRY OF CURVES AND SURFACES 5. The Second Fundamental Form of a Surface The main idea of this chapter is to try to measure to which extent a surface S is different from a plane, in other

More information

Arc Length and Surface Area in Parametric Equations

Arc Length and Surface Area in Parametric Equations Arc Length and Surface Area in Parametric Equations MATH 211, Calculus II J. Robert Buchanan Department of Mathematics Spring 2011 Background We have developed definite integral formulas for arc length

More information

Math 67. Rumbos Fall Solutions to Review Problems for Final Exam. (a) Use the triangle inequality to derive the inequality

Math 67. Rumbos Fall Solutions to Review Problems for Final Exam. (a) Use the triangle inequality to derive the inequality Math 67. umbos Fall 8 Solutions to eview Problems for Final Exam. In this problem, u and v denote vectors in n. (a) Use the triangle inequality to derive the inequality Solution: Write v u v u for all

More information

Math 10C - Fall Final Exam

Math 10C - Fall Final Exam Math 1C - Fall 217 - Final Exam Problem 1. Consider the function f(x, y) = 1 x 2 (y 1) 2. (i) Draw the level curve through the point P (1, 2). Find the gradient of f at the point P and draw the gradient

More information

Contents. MATH 32B-2 (18W) (L) G. Liu / (TA) A. Zhou Calculus of Several Variables. 1 Multiple Integrals 3. 2 Vector Fields 9

Contents. MATH 32B-2 (18W) (L) G. Liu / (TA) A. Zhou Calculus of Several Variables. 1 Multiple Integrals 3. 2 Vector Fields 9 MATH 32B-2 (8W) (L) G. Liu / (TA) A. Zhou Calculus of Several Variables Contents Multiple Integrals 3 2 Vector Fields 9 3 Line and Surface Integrals 5 4 The Classical Integral Theorems 9 MATH 32B-2 (8W)

More information

18.02 Multivariable Calculus Fall 2007

18.02 Multivariable Calculus Fall 2007 MIT OpenourseWare http://ocw.mit.edu 8.02 Multivariable alculus Fall 2007 For information about citing these materials or our Terms of Use, visit: http://ocw.mit.edu/terms. 8.02 Lecture 8. hange of variables.

More information

1 + f 2 x + f 2 y dy dx, where f(x, y) = 2 + 3x + 4y, is

1 + f 2 x + f 2 y dy dx, where f(x, y) = 2 + 3x + 4y, is 1. The value of the double integral (a) 15 26 (b) 15 8 (c) 75 (d) 105 26 5 4 0 1 1 + f 2 x + f 2 y dy dx, where f(x, y) = 2 + 3x + 4y, is 2. What is the value of the double integral interchange the order

More information

DIFFERENTIAL GEOMETRY HW 4. Show that a catenoid and helicoid are locally isometric.

DIFFERENTIAL GEOMETRY HW 4. Show that a catenoid and helicoid are locally isometric. DIFFERENTIAL GEOMETRY HW 4 CLAY SHONKWILER Show that a catenoid and helicoid are locally isometric. 3 Proof. Let X(u, v) = (a cosh v cos u, a cosh v sin u, av) be the parametrization of the catenoid and

More information

Math 115 ( ) Yum-Tong Siu 1. Euler-Lagrange Equations for Many Functions and Variables and High-Order Derivatives

Math 115 ( ) Yum-Tong Siu 1. Euler-Lagrange Equations for Many Functions and Variables and High-Order Derivatives Math 115 006-007 Yum-Tong Siu 1 Euler-Lagrange Equations for Many Functions and Variables and High-Order Derivatives The Case of High-Order Derivatives. The context is to find the extremal for the functional

More information

Summary of various integrals

Summary of various integrals ummary of various integrals Here s an arbitrary compilation of information about integrals Moisés made on a cold ecember night. 1 General things o not mix scalars and vectors! In particular ome integrals

More information

MATH 52 FINAL EXAM SOLUTIONS

MATH 52 FINAL EXAM SOLUTIONS MAH 5 FINAL EXAM OLUION. (a) ketch the region R of integration in the following double integral. x xe y5 dy dx R = {(x, y) x, x y }. (b) Express the region R as an x-simple region. R = {(x, y) y, x y }

More information

3. On the grid below, sketch and label graphs of the following functions: y = sin x, y = cos x, and y = sin(x π/2). π/2 π 3π/2 2π 5π/2

3. On the grid below, sketch and label graphs of the following functions: y = sin x, y = cos x, and y = sin(x π/2). π/2 π 3π/2 2π 5π/2 AP Physics C Calculus C.1 Name Trigonometric Functions 1. Consider the right triangle to the right. In terms of a, b, and c, write the expressions for the following: c a sin θ = cos θ = tan θ =. Using

More information

Green s, Divergence, Stokes: Statements and First Applications

Green s, Divergence, Stokes: Statements and First Applications Math 425 Notes 12: Green s, Divergence, tokes: tatements and First Applications The Theorems Theorem 1 (Divergence (planar version)). Let F be a vector field in the plane. Let be a nice region of the plane

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

Algebra II. Paulius Drungilas and Jonas Jankauskas

Algebra II. Paulius Drungilas and Jonas Jankauskas Algebra II Paulius Drungilas and Jonas Jankauskas Contents 1. Quadratic forms 3 What is quadratic form? 3 Change of variables. 3 Equivalence of quadratic forms. 4 Canonical form. 4 Normal form. 7 Positive

More information

MULTIVARIABLE CALCULUS

MULTIVARIABLE CALCULUS MULTIVARIABLE CALCULUS JOHN QUIGG Contents 13.1 Three-Dimensional Coordinate Systems 2 13.2 Vectors 3 13.3 The Dot Product 5 13.4 The Cross Product 6 13.5 Equations of Lines and Planes 7 13.6 Cylinders

More information

MATH2111 Higher Several Variable Calculus Integration

MATH2111 Higher Several Variable Calculus Integration MATH2 Higher Several Variable Calculus Integration Dr. Jonathan Kress School of Mathematics and Statistics University of New South Wales Semester, 26 [updated: April 3, 26] JM Kress (UNSW Maths & Stats)

More information

Introduction to Differentials

Introduction to Differentials Introduction to Differentials David G Radcliffe 13 March 2007 1 Increments Let y be a function of x, say y = f(x). The symbol x denotes a change or increment in the value of x. Note that a change in the

More information

Math 212-Lecture Integration in cylindrical and spherical coordinates

Math 212-Lecture Integration in cylindrical and spherical coordinates Math 22-Lecture 6 4.7 Integration in cylindrical and spherical coordinates Cylindrical he Jacobian is J = (x, y, z) (r, θ, z) = cos θ r sin θ sin θ r cos θ = r. Hence, d rdrdθdz. If we draw a picture,

More information

Topics. CS Advanced Computer Graphics. Differential Geometry Basics. James F. O Brien. Vector and Tensor Fields.

Topics. CS Advanced Computer Graphics. Differential Geometry Basics. James F. O Brien. Vector and Tensor Fields. CS 94-3 Advanced Computer Graphics Differential Geometry Basics James F. O Brien Associate Professor U.C. Berkeley Topics Vector and Tensor Fields Divergence, curl, etc. Parametric Curves Tangents, curvature,

More information

Math 234. What you should know on day one. August 28, You should be able to use general principles like. x = cos t, y = sin t, 0 t π.

Math 234. What you should know on day one. August 28, You should be able to use general principles like. x = cos t, y = sin t, 0 t π. Math 234 What you should know on day one August 28, 2001 1 You should be able to use general principles like Length = ds, Area = da, Volume = dv For example the length of the semi circle x = cos t, y =

More information

5.3 Surface Theory with Differential Forms

5.3 Surface Theory with Differential Forms 5.3 Surface Theory with Differential Forms 1 Differential forms on R n, Click here to see more details Differential forms provide an approach to multivariable calculus (Click here to see more detailes)

More information

x + ye z2 + ze y2, y + xe z2 + ze x2, z and where T is the

x + ye z2 + ze y2, y + xe z2 + ze x2, z and where T is the 1.(8pts) Find F ds where F = x + ye z + ze y, y + xe z + ze x, z and where T is the T surface in the pictures. (The two pictures are two views of the same surface.) The boundary of T is the unit circle

More information

Math 23b Practice Final Summer 2011

Math 23b Practice Final Summer 2011 Math 2b Practice Final Summer 211 1. (1 points) Sketch or describe the region of integration for 1 x y and interchange the order to dy dx dz. f(x, y, z) dz dy dx Solution. 1 1 x z z f(x, y, z) dy dx dz

More information

Math Vector Calculus II

Math Vector Calculus II Math 255 - Vector Calculus II Review Notes Vectors We assume the reader is familiar with all the basic concepts regarding vectors and vector arithmetic, such as addition/subtraction of vectors in R n,

More information

LINEAR ALGEBRA (PMTH213) Tutorial Questions

LINEAR ALGEBRA (PMTH213) Tutorial Questions Tutorial Questions The tutorial exercises range from revision and routine practice, through lling in details in the notes, to applications of the theory. While the tutorial problems are not compulsory,

More information

Practice Problems for Exam 3 (Solutions) 1. Let F(x, y) = xyi+(y 3x)j, and let C be the curve r(t) = ti+(3t t 2 )j for 0 t 2. Compute F dr.

Practice Problems for Exam 3 (Solutions) 1. Let F(x, y) = xyi+(y 3x)j, and let C be the curve r(t) = ti+(3t t 2 )j for 0 t 2. Compute F dr. 1. Let F(x, y) xyi+(y 3x)j, and let be the curve r(t) ti+(3t t 2 )j for t 2. ompute F dr. Solution. F dr b a 2 2 F(r(t)) r (t) dt t(3t t 2 ), 3t t 2 3t 1, 3 2t dt t 3 dt 1 2 4 t4 4. 2. Evaluate the line

More information

HOMEWORK 2 - RIEMANNIAN GEOMETRY. 1. Problems In what follows (M, g) will always denote a Riemannian manifold with a Levi-Civita connection.

HOMEWORK 2 - RIEMANNIAN GEOMETRY. 1. Problems In what follows (M, g) will always denote a Riemannian manifold with a Levi-Civita connection. HOMEWORK 2 - RIEMANNIAN GEOMETRY ANDRÉ NEVES 1. Problems In what follows (M, g will always denote a Riemannian manifold with a Levi-Civita connection. 1 Let X, Y, Z be vector fields on M so that X(p Z(p

More information

( sin(t), cos(t), 1) dt =

( sin(t), cos(t), 1) dt = Differential Geometry MT451 Problems/Homework Recommended Reading: Morgan F. Riemannian geometry, a beginner s guide Klingenberg W. A Course in Differential Geometry do Carmo M.P. Differential geometry

More information

SOME PROBLEMS YOU SHOULD BE ABLE TO DO

SOME PROBLEMS YOU SHOULD BE ABLE TO DO OME PROBLEM YOU HOULD BE ABLE TO DO I ve attempted to make a list of the main calculations you should be ready for on the exam, and included a handful of the more important formulas. There are no examples

More information

WORKSHEET #13 MATH 1260 FALL 2014

WORKSHEET #13 MATH 1260 FALL 2014 WORKSHEET #3 MATH 26 FALL 24 NOT DUE. Short answer: (a) Find the equation of the tangent plane to z = x 2 + y 2 at the point,, 2. z x (, ) = 2x = 2, z y (, ) = 2y = 2. So then the tangent plane equation

More information

Volumes of Solids of Revolution Lecture #6 a

Volumes of Solids of Revolution Lecture #6 a Volumes of Solids of Revolution Lecture #6 a Sphereoid Parabaloid Hyperboloid Whateveroid Volumes Calculating 3-D Space an Object Occupies Take a cross-sectional slice. Compute the area of the slice. Multiply

More information

Final Exam Topic Outline

Final Exam Topic Outline Math 442 - Differential Geometry of Curves and Surfaces Final Exam Topic Outline 30th November 2010 David Dumas Note: There is no guarantee that this outline is exhaustive, though I have tried to include

More information

Calculus III. Math 233 Spring Final exam May 3rd. Suggested solutions

Calculus III. Math 233 Spring Final exam May 3rd. Suggested solutions alculus III Math 33 pring 7 Final exam May 3rd. uggested solutions This exam contains twenty problems numbered 1 through. All problems are multiple choice problems, and each counts 5% of your total score.

More information

MAC2313 Final A. (5 pts) 1. How many of the following are necessarily true? i. The vector field F = 2x + 3y, 3x 5y is conservative.

MAC2313 Final A. (5 pts) 1. How many of the following are necessarily true? i. The vector field F = 2x + 3y, 3x 5y is conservative. MAC2313 Final A (5 pts) 1. How many of the following are necessarily true? i. The vector field F = 2x + 3y, 3x 5y is conservative. ii. The vector field F = 5(x 2 + y 2 ) 3/2 x, y is radial. iii. All constant

More information

A FEW APPLICATIONS OF DIFFERENTIAL FORMS. Contents

A FEW APPLICATIONS OF DIFFERENTIAL FORMS. Contents A FEW APPLICATIONS OF DIFFERENTIAL FORMS MATTHEW CORREIA Abstract. This paper introduces the concept of differential forms by defining the tangent space of R n at point p with equivalence classes of curves

More information

GEOMETRY HW Consider the parametrized surface (Enneper s surface)

GEOMETRY HW Consider the parametrized surface (Enneper s surface) GEOMETRY HW 4 CLAY SHONKWILER 3.3.5 Consider the parametrized surface (Enneper s surface φ(u, v (x u3 3 + uv2, v v3 3 + vu2, u 2 v 2 show that (a The coefficients of the first fundamental form are E G

More information

The Geometry of Relativity

The Geometry of Relativity The Geometry of Relativity Tevian Dray Department of Mathematics Oregon State University http://www.math.oregonstate.edu/~tevian OSU 4/27/15 Tevian Dray The Geometry of Relativity 1/27 Books The Geometry

More information

MATH 271 Test #4T Solutions

MATH 271 Test #4T Solutions MATH 7 Test #4T Solutions You do not need to evaluate the integrals in problems () (5); just set them up. () ( points) Consider the curve which is represented b the parametric equations x = + t + t, =

More information

Calculus II Practice Test Problems for Chapter 7 Page 1 of 6

Calculus II Practice Test Problems for Chapter 7 Page 1 of 6 Calculus II Practice Test Problems for Chapter 7 Page of 6 This is a set of practice test problems for Chapter 7. This is in no way an inclusive set of problems there can be other types of problems on

More information

Final exam (practice 1) UCLA: Math 32B, Spring 2018

Final exam (practice 1) UCLA: Math 32B, Spring 2018 Instructor: Noah White Date: Final exam (practice 1) UCLA: Math 32B, Spring 218 This exam has 7 questions, for a total of 8 points. Please print your working and answers neatly. Write your solutions in

More information