22.615, MDH Theory of Fusion Systems Prof. Final Exam Solution. ψ ψ. 1a. Solution: 1+κ κ

Size: px
Start display at page:

Download "22.615, MDH Theory of Fusion Systems Prof. Final Exam Solution. ψ ψ. 1a. Solution: 1+κ κ"

Transcription

1 .65, MDH Theor of Fusion Sstems Prof. Finl Em Solution. ψ ψ + +μ R J ψ ( S S: + Solution: ψ A + A + ψ A + R J μ A μ R J + μr J ψ , MDH Theor of Fusion Sstems Finl Em Solution Prof. Pge of

2 ψ ψ + ( + μ R J ψ, μ J ψ + R ψ ψ b. Bp ψ ez e R R R e B ψ ψ R R B ψ ψ R R. B ξ B B ξξ B B ξξ e B ξ p B p B B B e e J ξ + μ z μ J B δ F dr J B p ( p ξ + γ ξ + ξ ξ μ B δ F dr J B ξ μ B B B ξ 4ψξ μr μ μ B B ξ J B ξe ( Jzez ξ e ξ e ξ B Jz ξj B + ξ 4 + μ μ ψ ψ ψξ 4 4 R R R (.65, MDH Theor of Fusion Sstems Finl Em Solution Prof. Pge of

3 4ψξ ψξ F R μr μr δ dr π π 4πψξ F μr δ 4π ψξ μr 3. B A e B z B A e e A A e e A + A e A 3b. δ B μ dr z z B A e A e A z z z z z A A δ ( A dr + dr μ μ 3c. (See ttched sheet for summr of coordinte trnsformtion A n B n A ez n ez A n ez A t A ρθ A n B S b θ ρ b A b, θ Boundr Conditions n B n A e Sp z B n B n ξ ξ C B coshu cos B + sinhu sin C ψ ψ ξ coshu cos + sinhu sin R R.65, MDH Theor of Fusion Sstems Finl Em Solution Prof. Pge 3 of

4 C ψ R ξ ( coshu cos ψξ cos R C ψξ n B R C cos n A e n e A n e A t A ( C A z z z A ψξ cos R u A u, ψ ξ sin R Vcuum Vector Potentil A A + ψξ A u, A( u, sin R ( u ( ψξ sinh u A K sinh ( u u sin sin R sinh u u A ψξ cosh ( u u u R sinh( u u sin Vcuum Energ δ B dr ( A dr ( A A A A dr μ μ μ μ n AAdS p δ An A μ ds p.65, MDH Theor of Fusion Sstems Finl Em Solution Prof. Pge 4 of

5 A An AdSp A πr C d C Then A R π A d π A δ πr A μ u d u Complete δ πr 4 μ π ψξ cosh u sin R sinh u 4πψξ cosh u μr δ + πψξ R ( u ( u u 4 δ + coth μ Mrginl Stbilit ( u coth u ( u u sin d coshu u coshu coshu sinhu sinhu sinhu u sinhu coshu coshu sinhu coth u ( u tnhu tnhu tnhu tnhu Therefore +.65, MDH Theor of Fusion Sstems Finl Em Solution Prof. Pge 5 of

6 + Equte Epression for ( ( + ( ( + 4 ( , MDH Theor of Fusion Sstems Finl Em Solution Prof. Pge 6 of

7 Elliptic Coordintor Bsic Prmeters,, b Epress C,u,u,b, in terms of these prmeters C nd u Csinhucos C coshu sin Csinhu Ccoshu tnhu u,b, C.65, MDH Theor of Fusion Sstems Finl Em Solution Prof. Pge 7 of

8 Csinhu Ccoshu b C b b ( ( b ( ( + b + ( + b + tnhu Derition + Csinhucos Ccoshusin d C coshu cos du c sinhu sin d coshu cos sinhu sin d C sinhu sin du + c cosh cos d sinhu sin + coshu cos C cosh u cos + sinh u sin du coshu cos d + sinhu sin d.65, MDH Theor of Fusion Sstems Finl Em Solution Prof. Pge 8 of

9 C cosh u cos + sinh u sin d sinhu sin d + coshu cos d cos h u cos + sinh u sin cos h u cos + cos h u sin sin du d coshu cos d + sinhu sin d ( sin u C cosh u sinhu sin d + coshu cos d ( sin C cosh u cos h u sin u coshu cos sinhu sin u C cosh u sin C cosh u sin ( ( sinhu sin coshu cos C cosh u sin C cosh u sin ( ( u + u + coshu cos sinhu sin C cosh u ( sin sinhu sin + coshu cos C cosh u ( sin C ( cosh u sin + u u u + + u coshucos u sinhusin + coshucos sinhusin u + u + + u sinhusin + u coshucos.65, MDH Theor of Fusion Sstems Finl Em Solution Prof. Pge 9 of

10 + sinhusin + coshu cos Use u u u u + u + u u coshucos + u sinhusin u { ( + u coshucos u sinhusin + ( u sinhusin u coshu cos + u coshu cos + u sinh usin u cosh u cos + sinh u sin + + C cosh usin n, t n u u e + u e coshu cos sinhu sin e + e C n coshucose sinhusine C n coshucos sinhusin + C coshucos coshucos sinhusin + sinhu sin sinhu sin + coshu cos.65, MDH Theor of Fusion Sstems Finl Em Solution Prof. Pge of

11 n ( C C t ez n coshucose sinhusine C t coshu cos sinhu sin C coshu cos sinhu sin coshu cos + sinhu sin coshu cos sinhu sin t ( C Plsm Are u u du d d d ( u u d d cosh u cos sinh u sin d d + d d C d d C du d Surfce Are ds π R dl π R + d π R C sinh u sin + C cos h u cos d p ds πr C d.65, MDH Theor of Fusion Sstems Finl Em Solution Prof. Pge of

Total Score Maximum

Total Score Maximum Lst Nme: Mth 8: Honours Clculus II Dr. J. Bowmn 9: : April 5, 7 Finl Em First Nme: Student ID: Question 4 5 6 7 Totl Score Mimum 6 4 8 9 4 No clcultors or formul sheets. Check tht you hve 6 pges.. Find

More information

Integration Exercises - Part 3 (Sol'ns) (Hyperbolic Functions) (12 pages; 6/2/18) (The constant of integration has been omitted throughout.

Integration Exercises - Part 3 (Sol'ns) (Hyperbolic Functions) (12 pages; 6/2/18) (The constant of integration has been omitted throughout. Integration Eercises - Part (Sol'ns) (Hyperbolic Functions) ( pages; 6//8) (The constant of integration has been omitted throughout.) () cosech Given that d tanh = sech, we could investigate d coth = d

More information

22.615, MHD Theory of Fusion Systems Prof. Freidberg Lecture 7: The First Order Grad Shafranov Equation. dp 1 dp

22.615, MHD Theory of Fusion Systems Prof. Freidberg Lecture 7: The First Order Grad Shafranov Equation. dp 1 dp First Order Eqution.65, MHD Theory of Fusion Systems Prof. Freiderg Lecture 7: The First Order Grd Shfrnov Eqution The first order Grd Shfrnov eqution is given y d p d dp d + μr + R B B = μr r cos + cos

More information

Physics 712 Electricity and Magnetism Solutions to Final Exam, Spring 2016

Physics 712 Electricity and Magnetism Solutions to Final Exam, Spring 2016 Physics 7 Electricity nd Mgnetism Solutions to Finl Em, Spring 6 Plese note tht some possibly helpful formuls pper on the second pge The number of points on ech problem nd prt is mrked in squre brckets

More information

Reference. Vector Analysis Chapter 2

Reference. Vector Analysis Chapter 2 Reference Vector nlsis Chpter Sttic Electric Fields (3 Weeks) Chpter 3.3 Coulomb s Lw Chpter 3.4 Guss s Lw nd pplictions Chpter 3.5 Electric Potentil Chpter 3.6 Mteril Medi in Sttic Electric Field Chpter

More information

arxiv:acc-phys/ v1 23 Sep 1996

arxiv:acc-phys/ v1 23 Sep 1996 Coupling Impedances of Azimuthally Symmetric Obstacles of Semi-Elliptical Shape in a Beam Pipe Robert L. Gluckstern Sergey S. Kurennoy Physics Department, University of Maryl, College Park, MD 074 arxiv:acc-phys/9609005v

More information

( 2) ( ) Hyperbolic Functions 6E. cosh d (cosh sech ) d sinh tanh. cosh. x x x x x x C. x 1 x. 2 a. x x x = + = + cosh dx sinh C 3sinh C.

( 2) ( ) Hyperbolic Functions 6E. cosh d (cosh sech ) d sinh tanh. cosh. x x x x x x C. x 1 x. 2 a. x x x = + = + cosh dx sinh C 3sinh C. Hyperolic Functions 6E a (sinh+ cosh ) cosh+ sinh+ + cosh cosh (cosh sech ) sinh tanh sinh sinh sechtanh sech+ cosh cosh cosh c a a sinh cosh+ cosh sinh sinh + + ( ) + + ( ) ( ) ( ) ( ) arcosh + ( ) +

More information

Phys 4321 Final Exam December 14, 2009

Phys 4321 Final Exam December 14, 2009 Phys 4321 Finl Exm December 14, 2009 You my NOT use the text book or notes to complete this exm. You nd my not receive ny id from nyone other tht the instructor. You will hve 3 hours to finish. DO YOUR

More information

UNSTEADY LOW REYNOLDS NUMBER FLOW PAST TWO ROTATING CIRCULAR CYLINDERS BY A VORTEX METHOD

UNSTEADY LOW REYNOLDS NUMBER FLOW PAST TWO ROTATING CIRCULAR CYLINDERS BY A VORTEX METHOD Proceedings of the 3rd ASME/JSME Joint Fluids Engineering Conference Jul 8-23, 999, San Francisco, California FEDSM99-8 UNSTEADY LOW REYNOLDS NUMBER FLOW PAST TWO ROTATING CIRCULAR CYLINDERS BY A VORTEX

More information

MATH 1220 Midterm 1 Thurs., Sept. 20, 2007

MATH 1220 Midterm 1 Thurs., Sept. 20, 2007 MATH 220 Midterm Thurs., Sept. 20, 2007 Write your name and ID number at the top of this page. Show all your work. You may refer to one double-sided sheet of notes during the eam and nothing else. Calculators

More information

Vacuum Polarization in the Presence of Magnetic Flux at Finite Temperature in the Cosmic String Background

Vacuum Polarization in the Presence of Magnetic Flux at Finite Temperature in the Cosmic String Background Vacuum Polarization in the Presence of Magnetic Flux at Finite Temperature in the Cosmic String Background Univ. Estadual da Paraíba (UEPB), Brazil E-mail: jeanspinelly@ig.com.br E. R. Bezerra de Mello

More information

Appendix: Orthogonal Curvilinear Coordinates. We define the infinitesimal spatial displacement vector dx in a given orthogonal coordinate system with

Appendix: Orthogonal Curvilinear Coordinates. We define the infinitesimal spatial displacement vector dx in a given orthogonal coordinate system with Appendix: Orthogonal Curvilinear Coordinates Notes: Most of the material presented in this chapter is taken from Anupam G (Classical Electromagnetism in a Nutshell 2012 (Princeton: New Jersey)) Chap 2

More information

June 2011 Further Pure Mathematics FP Mark Scheme

June 2011 Further Pure Mathematics FP Mark Scheme . June 0 Further Pure Mthemtics FP 6669 Mrk dy 6x dx = nd so surfce re = π x ( + (6 x ) dx B 4 = 4 π ( 6 x ) + 6 4 4π D 860.06 = 806 (to sf) 6 Use limits nd 0 to give [ ] B Both bits CAO but condone lck

More information

Lecture 3. Lecturer: Prof. Sergei Fedotov Calculus and Vectors. Exponential and logarithmic functions

Lecture 3. Lecturer: Prof. Sergei Fedotov Calculus and Vectors. Exponential and logarithmic functions Lecture 3 Lecturer: Prof. Sergei Fedotov 10131 - Calculus and Vectors Exponential and logarithmic functions Sergei Fedotov (University of Manchester) MATH10131 2011 1 / 7 Lecture 3 1 Inverse functions

More information

Integrals in cylindrical, spherical coordinates (Sect. 15.7)

Integrals in cylindrical, spherical coordinates (Sect. 15.7) Integrals in clindrical, spherical coordinates (Sect. 15.7 Integration in spherical coordinates. Review: Clindrical coordinates. Spherical coordinates in space. Triple integral in spherical coordinates.

More information

( ) = 1 t + t. ( ) = 1 cos x + x ( sin x). Evaluate y. MTH 111 Test 1 Spring Name Calculus I

( ) = 1 t + t. ( ) = 1 cos x + x ( sin x). Evaluate y. MTH 111 Test 1 Spring Name Calculus I MTH Test Spring 209 Name Calculus I Justify all answers by showing your work or by proviing a coherent eplanation. Please circle your answers.. 4 z z + 6 z 3 ez 2 = 4 z + 2 2 z2 2ez Rewrite as 4 z + 6

More information

Solution Midterm 2, Math 53, Summer (a) (10 points) Let f(x, y, z) be a differentiable function of three variables and define

Solution Midterm 2, Math 53, Summer (a) (10 points) Let f(x, y, z) be a differentiable function of three variables and define Solution Midterm, Math 5, Summer. (a) ( points) Let f(,, z) be a differentiable function of three variables and define F (s, t) = f(st, s + t, s t). Calculate the partial derivatives F s and F t in terms

More information

Dr. Back. Nov. 3, 2009

Dr. Back. Nov. 3, 2009 Dr. Back Nov. 3, 2009 Please Don t Rely on this File! In you re expected to work on these topics mostly without computer aid. But seeing a few better pictures can help understanding the concepts. A copy

More information

Taylor Series 6B. lim s x. 1 a We can evaluate the limit directly since there are no singularities: b Again, there are no singularities, so:

Taylor Series 6B. lim s x. 1 a We can evaluate the limit directly since there are no singularities: b Again, there are no singularities, so: Taylor Series 6B a We can evaluate the it directly since there are no singularities: 7+ 7+ 7 5 5 5 b Again, there are no singularities, so: + + c Here we should divide through by in the numerator and denominator

More information

MATH 6102 Spring 2009 A Bestiary of Calculus Special Functions

MATH 6102 Spring 2009 A Bestiary of Calculus Special Functions MATH 6102 Spring 2009 A Bestiary of Calculus Special Functions Transcendental Functions Last time we discussed eponential, logarithmic, and trigonometric functions. Theorem 1: If f : R R is a continuous

More information

Spherically Symmetric Logistic Distribution

Spherically Symmetric Logistic Distribution Journal of Multivariate Analysis 7, 2226 (999) Article ID jmva.999.826, available online at httpwww.idealibrary.com on Spherically Symmetric Logistic Distribution Nikolai A. Volodin The Australian Council

More information

Chapter 9. Arc Length and Surface Area

Chapter 9. Arc Length and Surface Area Chpter 9. Arc Length nd Surfce Are In which We ppl integrtion to stud the lengths of curves nd the re of surfces. 9. Arc Length (Tet 547 553) P n P 2 P P 2 n b P i ( i, f( i )) P i ( i, f( i )) distnce

More information

Lecture 04. Curl and Divergence

Lecture 04. Curl and Divergence Lecture 04 Curl and Divergence UCF Curl of Vector Field (1) F c d l F C Curl (or rotor) of a vector field a n curlf F d l lim c s s 0 F s a n C a n : normal direction of s follow right-hand rule UCF Curl

More information

Chapter 1 VECTOR ALGEBRA

Chapter 1 VECTOR ALGEBRA Chpter 1 VECTOR LGEBR INTRODUCTION: Electromgnetics (EM) m be regrded s the stud of the interctions between electric chrges t rest nd in motion. Electromgnetics is brnch of phsics or electricl engineering

More information

Problem Set 3 Solutions

Problem Set 3 Solutions Msschusetts Institute of Technology Deprtment of Physics Physics 8.07 Fll 2005 Problem Set 3 Solutions Problem 1: Cylindricl Cpcitor Griffiths Problems 2.39: Let the totl chrge per unit length on the inner

More information

ECE Spring Prof. David R. Jackson ECE Dept. Notes 37

ECE Spring Prof. David R. Jackson ECE Dept. Notes 37 ECE 6341 Spring 16 Prof. David R. Jacson ECE Dept. Notes 37 1 Line Source on a Grounded Slab y ε r E jω A z µ I 1 A 1 e e d y ( ) + TE j y j z 4 j +Γ y 1/ 1/ ( ) ( ) y y1 1 There are branch points only

More information

Trigonometric substitutions (8.3).

Trigonometric substitutions (8.3). Review for Eam 2. 5 or 6 problems. No multiple choice questions. No notes, no books, no calculators. Problems similar to homeworks. Eam covers: 7.4, 7.6, 7.7, 8-IT, 8., 8.2. Solving differential equations

More information

Integrals along a curve in space. (Sect. 16.1)

Integrals along a curve in space. (Sect. 16.1) Integrals along a curve in space. (Sect. 6.) Line integrals in space. The addition of line integrals. ass and center of mass of wires. Line integrals in space Definition The line integral of a function

More information

Some Methods in the Calculus of Variations

Some Methods in the Calculus of Variations CHAPTER 6 Some Methods in the Clculus of Vritions 6-. If we use the vried function ( α, ) α sin( ) + () Then d α cos ( ) () d Thus, the totl length of the pth is d S + d d α cos ( ) + α cos ( ) d Setting

More information

STABILITY AND OSCILLATIONS OF A CATENOID SOAP FILM SURFACE

STABILITY AND OSCILLATIONS OF A CATENOID SOAP FILM SURFACE STABILITY AND OSCILLATIONS OF A CATENOID SOAP FILM SURFACE Interpretable quantities and equations of motion derived from Sturm-Liouville theory for a minimized surface Sweden, 015-016 Edited by ANDREAS

More information

Electromagnetics P5-1. 1) Physical quantities in EM could be scalar (charge, current, energy) or vector (EM fields).

Electromagnetics P5-1. 1) Physical quantities in EM could be scalar (charge, current, energy) or vector (EM fields). Electromgnetics 5- Lesson 5 Vector nlsis Introduction ) hsicl quntities in EM could be sclr (chrge current energ) or ector (EM fields) ) Specifing ector in -D spce requires three numbers depending on the

More information

Edexcel GCE A Level Maths. Further Maths 3 Coordinate Systems

Edexcel GCE A Level Maths. Further Maths 3 Coordinate Systems Edecel GCE A Level Maths Further Maths 3 Coordinate Sstems Edited b: K V Kumaran kumarmaths.weebl.com 1 kumarmaths.weebl.com kumarmaths.weebl.com 3 kumarmaths.weebl.com 4 kumarmaths.weebl.com 5 1. An ellipse

More information

Multiple Integrals. Review of Single Integrals. Planar Area. Volume of Solid of Revolution

Multiple Integrals. Review of Single Integrals. Planar Area. Volume of Solid of Revolution Multiple Integrls eview of Single Integrls eding Trim 7.1 eview Appliction of Integrls: Are 7. eview Appliction of Integrls: olumes 7.3 eview Appliction of Integrls: Lengths of Curves Assignment web pge

More information

Created by T. Madas SURFACE INTEGRALS. Created by T. Madas

Created by T. Madas SURFACE INTEGRALS. Created by T. Madas SURFACE INTEGRALS Question 1 Find the area of the plane with equation x + 3y + 6z = 60, 0 x 4, 0 y 6. 8 Question A surface has Cartesian equation y z x + + = 1. 4 5 Determine the area of the surface which

More information

MTH3101 Spring 2017 HW Assignment 4: Sec. 26: #6,7; Sec. 33: #5,7; Sec. 38: #8; Sec. 40: #2 The due date for this assignment is 2/23/17.

MTH3101 Spring 2017 HW Assignment 4: Sec. 26: #6,7; Sec. 33: #5,7; Sec. 38: #8; Sec. 40: #2 The due date for this assignment is 2/23/17. MTH0 Spring 07 HW Assignment : Sec. 6: #6,7; Sec. : #5,7; Sec. 8: #8; Sec. 0: # The due date for this assignment is //7. Sec. 6: #6. Use results in Sec. to verify that the function g z = ln r + iθ r >

More information

Theoretische Physik 2: Elektrodynamik (Prof. A.-S. Smith) Home assignment 4

Theoretische Physik 2: Elektrodynamik (Prof. A.-S. Smith) Home assignment 4 WiSe 1 8.1.1 Prof. Dr. A.-S. Smith Dipl.-Phys. Ellen Fischermeier Dipl.-Phys. Mtthis Sb m Lehrstuhl für Theoretische Physik I Deprtment für Physik Friedrich-Alexnder-Universität Erlngen-Nürnberg Theoretische

More information

Math 1B Final Exam, Solution. Prof. Mina Aganagic Lecture 2, Spring (6 points) Use substitution and integration by parts to find:

Math 1B Final Exam, Solution. Prof. Mina Aganagic Lecture 2, Spring (6 points) Use substitution and integration by parts to find: Math B Final Eam, Solution Prof. Mina Aganagic Lecture 2, Spring 20 The eam is closed book, apart from a sheet of notes 8. Calculators are not allowed. It is your responsibility to write your answers clearly..

More information

FUNCTIONS OF ONE VARIABLE FUNCTION DEFINITIONS

FUNCTIONS OF ONE VARIABLE FUNCTION DEFINITIONS Page of 6 FUNCTIONS OF ONE VARIABLE FUNCTION DEFINITIONS 6. HYPERBOLIC FUNCTIONS These functions which are defined in terms of e will be seen later to be related to the trigonometic functions via comple

More information

Exercises of Mathematical analysis II

Exercises of Mathematical analysis II Eercises of Mathematical analysis II In eercises. - 8. represent the domain of the function by the inequalities and make a sketch showing the domain in y-plane.. z = y.. z = arcsin y + + ln y. 3. z = sin

More information

Math 223, Fall 2010 Review Information for Final Exam

Math 223, Fall 2010 Review Information for Final Exam 1. Generl Informtion Mth 223, Fll 2010 Review Informtion for Finl Exm Time, dte nd plce of finl exm: Mondy, ecember 13, 10:30 AM 1:00 PM, Wescoe 4051 (the usul clssroom). Pln to rrive 15 minutes erly so

More information

( x )( x) dx. Year 12 Extension 2 Term Question 1 (15 Marks) (a) Sketch the curve (x + 1)(y 2) = 1 2

( x )( x) dx. Year 12 Extension 2 Term Question 1 (15 Marks) (a) Sketch the curve (x + 1)(y 2) = 1 2 Yer Etension Term 7 Question (5 Mrks) Mrks () Sketch the curve ( + )(y ) (b) Write the function in prt () in the form y f(). Hence, or otherwise, sketch the curve (i) y f( ) (ii) y f () (c) Evlute (i)

More information

Final: Solutions Math 118A, Fall 2013

Final: Solutions Math 118A, Fall 2013 Final: Solutions Math 118A, Fall 2013 1. [20 pts] For each of the following PDEs for u(x, y), give their order and say if they are nonlinear or linear. If they are linear, say if they are homogeneous or

More information

Velocity, Acceleration and Equations of Motion in the Elliptical Coordinate System

Velocity, Acceleration and Equations of Motion in the Elliptical Coordinate System Aailable online at www.scholarsresearchlibrary.com Archies of Physics Research, 018, 9 (): 10-16 (http://scholarsresearchlibrary.com/archie.html) ISSN 0976-0970 CODEN (USA): APRRC7 Velocity, Acceleration

More information

Lecture 18 April 5, 2010

Lecture 18 April 5, 2010 Lecture 18 April 5, 2010 Darwin Particle dynamics: x j (t) evolves by F k j ( x j (t), x k (t)), depends on where other particles are at the same instant. Violates relativity! If the forces are given by

More information

AXIALLY SLOTTED ANTENNA ON A CIRCULAR OR ELLIPTIC CYLINDER COATED WITH METAMATERIALS

AXIALLY SLOTTED ANTENNA ON A CIRCULAR OR ELLIPTIC CYLINDER COATED WITH METAMATERIALS Progress In Electromagnetics Research, PIER 1, 329 341, 2 AXIALLY SLOTTED ANTENNA ON A CIRCULAR OR ELLIPTIC CYLINDER COATED WITH METAMATERIALS A-K. Hamid Department of Electrical/Electronics and Computer

More information

Solution Sheet 1.4 Questions 26-31

Solution Sheet 1.4 Questions 26-31 Solution Sheet 1.4 Questions 26-31 26. Using the Limit Rules evaluate i) ii) iii) 3 2 +4+1 0 2 +4+3, 3 2 +4+1 2 +4+3, 3 2 +4+1 1 2 +4+3. Note When using a Limit Rule you must write down which Rule you

More information

Multiple Integrals. Review of Single Integrals. Planar Area. Volume of Solid of Revolution

Multiple Integrals. Review of Single Integrals. Planar Area. Volume of Solid of Revolution Multiple Integrls eview of Single Integrls eding Trim 7.1 eview Appliction of Integrls: Are 7. eview Appliction of Integrls: Volumes 7.3 eview Appliction of Integrls: Lengths of Curves Assignment web pge

More information

ME 501A Seminar in Engineering Analysis Page 1

ME 501A Seminar in Engineering Analysis Page 1 Phse-plne Anlsis of Ordinr November, 7 Phse-plne Anlsis of Ordinr Lrr Cretto Mechnicl Engineering 5A Seminr in Engineering Anlsis November, 7 Outline Mierm exm two weeks from tonight covering ODEs nd Lplce

More information

Hyperbolic Functions and the Twin Paradox

Hyperbolic Functions and the Twin Paradox Hyperbolic Functions and the Twin Paradox Basics of hyperbolic functions The basic hyperbolic functions are defined as cosh x 1 2 (ex + e x ), sinh 1 2 (ex e x ). The notation ch, sh is also used (especially

More information

Introduction Calculation in Gauge Theory Calculation in String Theory Another Saddle Point Summary and Future Works

Introduction Calculation in Gauge Theory Calculation in String Theory Another Saddle Point Summary and Future Works Introduction AdS/CFT correspondence N = 4 SYM type IIB superstring Wilson loop area of world-sheet Wilson loop + heavy local operator area of deformed world-sheet Zarembo s solution (1/2 BPS Wilson Loop)

More information

Spectrum of Holographic Wilson Loops

Spectrum of Holographic Wilson Loops Spectrum of Holographic Wilson Loops Leopoldo Pando Zayas University of Michigan Continuous Advances in QCD 2011 University of Minnesota Based on arxiv:1101.5145 Alberto Faraggi and LPZ Work in Progress,

More information

New Exact Solutions to NLS Equation and Coupled NLS Equations

New Exact Solutions to NLS Equation and Coupled NLS Equations Commun. Theor. Phys. (Beijing, China 4 (2004 pp. 89 94 c International Academic Publishers Vol. 4, No. 2, February 5, 2004 New Exact Solutions to NLS Euation Coupled NLS Euations FU Zun-Tao, LIU Shi-Da,

More information

Solutions to Math 152 Review Problems for Exam 1

Solutions to Math 152 Review Problems for Exam 1 Soltions to Math 5 Review Problems for Eam () If A() is the area of the rectangle formed when the solid is sliced at perpendiclar to the -ais, then A() = ( ), becase the height of the rectangle is and

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

Conic Sections in Polar Coordinates

Conic Sections in Polar Coordinates Conic Sections in Polar Coordinates MATH 211, Calculus II J. Robert Buchanan Department of Mathematics Spring 2018 Introduction We have develop the familiar formulas for the parabola, ellipse, and hyperbola

More information

MATH 312 Section 7.1: Definition of a Laplace Transform

MATH 312 Section 7.1: Definition of a Laplace Transform MATH 312 Section 7.1: Definition of a Laplace Transform Prof. Jonathan Duncan Walla Walla University Spring Quarter, 2008 Outline 1 The Laplace Transform 2 The Theory of Laplace Transforms 3 Conclusions

More information

Summary: Method of Separation of Variables

Summary: Method of Separation of Variables Physics 246 Electricity nd Mgnetism I, Fll 26, Lecture 22 1 Summry: Method of Seprtion of Vribles 1. Seprtion of Vribles in Crtesin Coordintes 2. Fourier Series Suggested Reding: Griffiths: Chpter 3, Section

More information

11.4. Differentiating ProductsandQuotients. Introduction. Prerequisites. Learning Outcomes

11.4. Differentiating ProductsandQuotients. Introduction. Prerequisites. Learning Outcomes Differentiating ProductsandQuotients 11.4 Introduction We have seen, in the first three Sections, how standard functions like n, e a, sin a, cos a, ln a may be differentiated. In this Section we see how

More information

Hyperbolic Functions: Exercises - Sol'ns (9 pages; 13/5/17)

Hyperbolic Functions: Exercises - Sol'ns (9 pages; 13/5/17) Hyperbolic Functions: Exercises - Sol'ns (9 pages; 3/5/7) () (i) Prove, using exponential functions, that (a) cosh x sinh x = (b) sinhx = sinhxcoshx (ii) By differentiating the result from (i)(b), obtain

More information

Holographic Entanglement and Interaction

Holographic Entanglement and Interaction Holographic Entanglement and Interaction Shigenori Seki RINS, Hanyang University and Institut des Hautes Études Scientifiques Intrication holographique et interaction à l IHES le 30 janvier 2014 1 Contents

More information

1 M3-4-5A16 Assessed Problems # 1: Do all three problems

1 M3-4-5A16 Assessed Problems # 1: Do all three problems D. D. Holm M3-4-5A34 Assessed Problems # 1 Due 1 Feb 2013 1 1 M3-4-5A16 Assessed Problems # 1: Do all three problems Exercise 1.1 (Quaternions in Cayley-Klein (CK) parameters). Express all of your answers

More information

Calculus II. George Voutsadakis 1. LSSU Math 152. Lake Superior State University. 1 Mathematics and Computer Science

Calculus II. George Voutsadakis 1. LSSU Math 152. Lake Superior State University. 1 Mathematics and Computer Science Calculus II George Voutsadakis Mathematics and Computer Science Lake Superior State University LSSU Math 52 George Voutsadakis (LSSU) Calculus II February 205 / 88 Outline Techniques of Integration Integration

More information

Supporting Information

Supporting Information Supporting Information A: Calculation of radial distribution functions To get an effective propagator in one dimension, we first transform 1) into spherical coordinates: x a = ρ sin θ cos φ, y = ρ sin

More information

ANALLAGMATIC SPIRALS PURSUIT CURVES HYPERBOLIC-TANGENTOID SPIRALS. Part - VII

ANALLAGMATIC SPIRALS PURSUIT CURVES HYPERBOLIC-TANGENTOID SPIRALS. Part - VII ANALLAGMATIC SPIRALS PURSUIT CURVES HYPERBOLIC-TANGENTOID SPIRALS β-curves Part - VII C. Masurel 21/10/2014 Abstract By analogy with sinusoidal spirals and Ribaucour curves defined with trigonometric functions

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

M344 - ADVANCED ENGINEERING MATHEMATICS

M344 - ADVANCED ENGINEERING MATHEMATICS M3 - ADVANCED ENGINEERING MATHEMATICS Lecture 18: Lplce s Eqution, Anltic nd Numericl Solution Our emple of n elliptic prtil differentil eqution is Lplce s eqution, lso clled the Diffusion Eqution. If

More information

2016 FAMAT Convention Mu Integration 1 = 80 0 = 80. dx 1 + x 2 = arctan x] k2

2016 FAMAT Convention Mu Integration 1 = 80 0 = 80. dx 1 + x 2 = arctan x] k2 6 FAMAT Convention Mu Integration. A. 3 3 7 6 6 3 ] 3 6 6 3. B. For quadratic functions, Simpson s Rule is eact. Thus, 3. D.. B. lim 5 3 + ) 3 + ] 5 8 8 cot θ) dθ csc θ ) dθ cot θ θ + C n k n + k n lim

More information

Created by T. Madas VECTOR OPERATORS. Created by T. Madas

Created by T. Madas VECTOR OPERATORS. Created by T. Madas VECTOR OPERATORS GRADIENT gradϕ ϕ Question 1 A surface S is given by the Cartesian equation x 2 2 + y = 25. a) Draw a sketch of S, and describe it geometrically. b) Determine an equation of the tangent

More information

Student Handbook for MATH 3300

Student Handbook for MATH 3300 Student Hndbook for MATH 3300 0.8 0.6 0.4 0.2 0 0.2 0.4 0.6 0.8 0.5 0 0.5 0.5 0 0.5 If people do not believe tht mthemtics is simple, it is only becuse they do not relize how complicted life is. John Louis

More information

Hyperbolic functions

Hyperbolic functions Roberto s Notes on Differential Calculus Chapter 5: Derivatives of transcendental functions Section Derivatives of Hyperbolic functions What you need to know already: Basic rules of differentiation, including

More information

(b) Let S 1 : f(x, y, z) = (x a) 2 + (y b) 2 + (z c) 2 = 1, this is a level set in 3D, hence

(b) Let S 1 : f(x, y, z) = (x a) 2 + (y b) 2 + (z c) 2 = 1, this is a level set in 3D, hence Problem ( points) Find the vector eqution of the line tht joins points on the two lines L : r ( + t) i t j ( + t) k L : r t i + (t ) j ( + t) k nd is perpendiculr to both those lines. Find the set of ll

More information

Cauchy s Integral Formula for derivatives of functions (part 2)

Cauchy s Integral Formula for derivatives of functions (part 2) auchy s Integral Formula DEPARTMENT OF ELETRIAL AND OMPUTER ENGINEERING Engineering Math EEE 3640 1 auchy s Integral Formula DEPARTMENT OF ELETRIAL AND OMPUTER ENGINEERING Statement of the formula (without

More information

Errata for Instructor s Solutions Manual for Gravity, An Introduction to Einstein s General Relativity 1st printing

Errata for Instructor s Solutions Manual for Gravity, An Introduction to Einstein s General Relativity 1st printing Errata for Instructor s Solutions Manual for Gravity, An Introduction to Einstein s General Relativity st printing Updated 7/7/003 (hanks to Scott Fraser who provided almost all of these.) Statement of

More information

Physics 241 Exam 1 February 19, 2004

Physics 241 Exam 1 February 19, 2004 Phsics 241 Em 1 Februr 19, 24 One (both sides) 8 1/2 11 crib sheet is llowed. It must be of our own cretion. k = 1 = 9 1 9 N m2 4p 2 2 = 8.85 1-12 N m 2 e =1.62 1-19 c = 2.99792458 1 8 m/s (speed of light)

More information

Mathematics for Physicists and Astronomers

Mathematics for Physicists and Astronomers PHY472 Dt Provided: Formul sheet nd physicl constnts Dt Provided: A formul sheet nd tble of physicl constnts is ttched to this pper. DEPARTMENT OF PHYSICS & Autumn Semester 2009-2010 ASTRONOMY DEPARTMENT

More information

EUCLIDEAN CONFORMALLY FLAT SUBMANIFOLDS IN CODIMENSION TWO OBTAINED AS INTERSECTIONS

EUCLIDEAN CONFORMALLY FLAT SUBMANIFOLDS IN CODIMENSION TWO OBTAINED AS INTERSECTIONS PROCEEDINGS OF THE AMERICAN MATHEMATICAL SOCIETY Volume 127, Number 1, January 1999, Pages 265 269 S 2-9939(994486-X EUCLIDEAN CONFORMALLY FLAT SUBMANIFOLDS IN CODIMENSION TWO OBTAINED AS INTERSECTIONS

More information

Equidistant curve coordinate system. Morio Kikuchi

Equidistant curve coordinate system. Morio Kikuchi Equidistant curve coordinate system Morio Kiuchi Abstract: An isometry is realized between Poincaré dis of which radius is not limited to 1 and upper half-plane. Poincaré metrics are the same in both regions

More information

Notes 19 Gradient and Laplacian

Notes 19 Gradient and Laplacian ECE 3318 Applied Electricity and Magnetism Spring 218 Prof. David R. Jackson Dept. of ECE Notes 19 Gradient and Laplacian 1 Gradient Φ ( x, y, z) =scalar function Φ Φ Φ grad Φ xˆ + yˆ + zˆ x y z We can

More information

MAT187H1F Lec0101 Burbulla

MAT187H1F Lec0101 Burbulla Chpter 6 Lecture Notes Review nd Two New Sections Sprint 17 Net Distnce nd Totl Distnce Trvelled Suppose s is the position of prticle t time t for t [, b]. Then v dt = s (t) dt = s(b) s(). s(b) s() is

More information

Tutorial Exercises: Geometric Connections

Tutorial Exercises: Geometric Connections Tutorial Exercises: Geometric Connections 1. Geodesics in the Isotropic Mercator Projection When the surface of the globe is projected onto a flat map some aspects of the map are inevitably distorted.

More information

Useful Mathematics. 1. Multivariable Calculus. 1.1 Taylor s Theorem. Monday, 13 May 2013

Useful Mathematics. 1. Multivariable Calculus. 1.1 Taylor s Theorem. Monday, 13 May 2013 Useful Mathematics Monday, 13 May 013 Physics 111 In recent years I have observed a reticence among a subpopulation of students to dive into mathematics when the occasion arises in theoretical mechanics

More information

MAS113 CALCULUS II SPRING 2008, QUIZ 4 SOLUTIONS

MAS113 CALCULUS II SPRING 2008, QUIZ 4 SOLUTIONS MAS113 CALCULUS II SPRING 8, QUIZ 4 SOLUTIONS Quiz 4a Solutions 1 Find the area of the surface obtained by rotating the curve y = x 3 /6 + 1/x, 1/ x 1 about the x-axis. We have y = x / 1/x. Therefore,

More information

Vortex motion. Wasilij Barsukow, July 1, 2016

Vortex motion. Wasilij Barsukow, July 1, 2016 The concept of vorticity We call Vortex motion Wasilij Barsukow, mail@sturzhang.de July, 206 ω = v vorticity. It is a measure of the swirlyness of the flow, but is also present in shear flows where the

More information

HOMEWORK SOLUTIONS MATH 1910 Sections 7.9, 8.1 Fall 2016

HOMEWORK SOLUTIONS MATH 1910 Sections 7.9, 8.1 Fall 2016 HOMEWORK SOLUTIONS MATH 9 Sections 7.9, 8. Fll 6 Problem 7.9.33 Show tht for ny constnts M,, nd, the function yt) = )) t ) M + tnh stisfies the logistic eqution: y SOLUTION. Let Then nd Finlly, y = y M

More information

4.317 d 4 y. 4 dx d 2 y dy. 20. dt d 2 x. 21. y 3y 3y y y 6y 12y 8y y (4) y y y (4) 2y y 0. d 4 y 26.

4.317 d 4 y. 4 dx d 2 y dy. 20. dt d 2 x. 21. y 3y 3y y y 6y 12y 8y y (4) y y y (4) 2y y 0. d 4 y 26. 38 CHAPTER 4 HIGHER-ORDER DIFFERENTIAL EQUATIONS sstems are also able, b means of their dsolve commands, to provide eplicit solutions of homogeneous linear constant-coefficient differential equations.

More information

Applied Mathematics Masters Examination Fall 2016, August 18, 1 4 pm.

Applied Mathematics Masters Examination Fall 2016, August 18, 1 4 pm. Applied Mathematics Masters Examination Fall 16, August 18, 1 4 pm. Each of the fifteen numbered questions is worth points. All questions will be graded, but your score for the examination will be the

More information

Worksheet : Class XII Matrices & Determinants

Worksheet : Class XII Matrices & Determinants Worksheet : Clss XII Mtries & Determinnts Prepred B:Mr. durhimn K Mth Teher l-hej Interntionl Shool, Jeddh (IGCSE). rhmnrk@gmil.om #00966007900# MTHEMTICS WKSHEET I Nme: Mrh 0. If 8 LGEBR (Mtries nd Determinnts)

More information

6.7 Hyperbolic Functions

6.7 Hyperbolic Functions 6.7 6.7 Hyperbolic Functions Even and Odd Parts of an Exponential Function We recall that a function f is called even if f( x) = f(x). f is called odd if f( x) = f(x). The sine function is odd while the

More information

FP3 past questions - conics

FP3 past questions - conics Hperolic functions cosh sinh = sinh = sinh cosh cosh = cosh + sinh rcosh = ln{ + } ( ) rsinh = ln{ + + } + rtnh = ln ( < ) FP3 pst questions - conics Conics Ellipse Prol Hperol Rectngulr Hperol Stndrd

More information

Electromagnetic Fields in Space

Electromagnetic Fields in Space Chapter 3 Electromagnetic Fields in Space Magnetic and electric field are fundamental properties in the entire universe. Massive magnetic fields eist in the vicinity of pulsars, in active galactic nuclei,

More information

arxiv:hep-th/ v3 16 May 1996

arxiv:hep-th/ v3 16 May 1996 BNL-63106 An Exact Solution for Quantum Tunneling in a Dissipative System arxiv:hep-th/9605081v3 16 May 1996 Li Hua Yu National Synchrotron Light Source, Brookhaven National Laboratory, N.Y.11973 Abstract

More information

Chapter 5 Equilibrium of a Rigid Body Objectives

Chapter 5 Equilibrium of a Rigid Body Objectives Chapter 5 Equilibrium of a Rigid Bod Objectives Develop the equations of equilibrium for a rigid bod Concept of the free-bod diagram for a rigid bod Solve rigid-bod equilibrium problems using the equations

More information

MATH 13 FINAL STUDY GUIDE, WINTER 2012

MATH 13 FINAL STUDY GUIDE, WINTER 2012 MATH 13 FINAL TUY GUI, WINTR 2012 This is ment to be quick reference guide for the topics you might wnt to know for the finl. It probbly isn t comprehensive, but should cover most of wht we studied in

More information

Bethe Ansatz solution of the open XX spin chain with nondiagonal boundary terms

Bethe Ansatz solution of the open XX spin chain with nondiagonal boundary terms UMTG 231 Bethe Ansatz solution of the open XX spin chain with nondiagonal boundary terms arxiv:hep-th/0110081v1 9 Oct 2001 Rafael I. Nepomechie Physics Department, P.O. Box 248046, University of Miami

More information

MULTIPLE CHOICE. Choose the one alternative that best completes the statement or answers the question. C) 2

MULTIPLE CHOICE. Choose the one alternative that best completes the statement or answers the question. C) 2 Cal II- Final Review Name MULTIPLE CHOICE. Choose the one alternative that best completes the statement or answers the question. Epress the following logarithm as specified. ) ln 4. in terms of ln and

More information

A Note on a Three-Dimensional Bäcklund Transformation

A Note on a Three-Dimensional Bäcklund Transformation Interntionl Journl of Applied Science nd Engineering 006., : 5-0 A ote on Three-Dimensionl Bäcklund Trnsformtion Xuncheng Hung * nd Edwrd H. C. Chng Yngzhou Poltechnic Universit-903 Ho Yue Yun, Moon PrkYngzhou,

More information

Polarization and Related Antenna Parameters

Polarization and Related Antenna Parameters ANTENTOP- 01-007, # 009 Polarization and Related Antenna Parameters Feel Yourself a Student! Dear friends, I would like to give to ou an interesting and reliable antenna theor. Hours searching in the web

More information

The Metric and The Dynamics

The Metric and The Dynamics The Metric and The Dynamics r τ c t a () t + r + Sin φ ( kr ) The RW metric tell us where in a 3 dimension space is an event and at which proper time. The coordinates of the event do not change as a function

More information

ECE Spring Prof. David R. Jackson ECE Dept. Notes 33

ECE Spring Prof. David R. Jackson ECE Dept. Notes 33 ECE 6341 Spring 16 Prof. David R. Jackson ECE Dept. Notes 33 1 Complex Integral: Steepest-Descent Method Ω g z I f z e dz Ω = C This is an extension of Laplace s method to treat integrals in the complex

More information

Final Exam Solutions, MAC 3474 Calculus 3 Honors, Fall 2018

Final Exam Solutions, MAC 3474 Calculus 3 Honors, Fall 2018 Finl xm olutions, MA 3474 lculus 3 Honors, Fll 28. Find the re of the prt of the sddle surfce z xy/ tht lies inside the cylinder x 2 + y 2 2 in the first positive) octnt; is positive constnt. olution:

More information