Macroscopic Fields in Accelerators

Similar documents
[5 points] (c) Find the charge enclosed by the cylindrical surface of radius ρ 0 = 9 mm and length L = 1 m. [2

Semiconductors materials

SULIT 3472/2. Rumus-rumus berikut boleh membantu anda menjawab soalan. Simbol-simbol yang diberi adalah yang biasa digunakan.

BINOMIAL THEOREM SOLUTION. 1. (D) n. = (C 0 + C 1 x +C 2 x C n x n ) (1+ x+ x 2 +.)

UNIT V: Z-TRANSFORMS AND DIFFERENCE EQUATIONS. Dr. V. Valliammal Department of Applied Mathematics Sri Venkateswara College of Engineering

Parametric Methods. Autoregressive (AR) Moving Average (MA) Autoregressive - Moving Average (ARMA) LO-2.5, P-13.3 to 13.4 (skip

PhysicsAndMathsTutor.com

Chapter 28 Sources of Magnetic Field

Micro-bunching: Longitudinal Bunch Profile Measurements at TTF

Summary: Binomial Expansion...! r. where

Advanced Higher Maths: Formulae

Advanced Higher Maths: Formulae

PhysicsAndMathsTutor.com

PROGRESSION AND SERIES

PhysicsAndMathsTutor.com

Electric Potential. and Equipotentials

PhysicsAndMathsTutor.com

PhysicsAndMathsTutor.com

We show that every analytic function can be expanded into a power series, called the Taylor series of the function.

Physics 11b Lecture #11

3.1 Magnetic Fields. Oersted and Ampere

Important Facts You Need To Know/Review:

Unit 10 Electro-magnetic forces and stresses in superconducting accelerator magnets

Lecture 38 (Trapped Particles) Physics Spring 2018 Douglas Fields

General Physics II. number of field lines/area. for whole surface: for continuous surface is a whole surface

Pearson Edexcel Level 3 Advanced Subsidiary and Advanced GCE Mathematics and Further Mathematics

ELECTROSTATICS. 4πε0. E dr. The electric field is along the direction where the potential decreases at the maximum rate. 5. Electric Potential Energy:

Pearson Edexcel Level 3 Advanced Subsidiary and Advanced GCE Mathematics and Further Mathematics

2012 GCE A Level H2 Maths Solution Paper Let x,

Multi-Electron Atoms-Helium

4.2 Boussinesq s Theory. Contents

Review. I will give you these formulas: Sphere: V=frr Circle: A = rr2 Cone: V = I 2rr2h Cube: V = side3

Mathematical Statistics

x a y n + b = 1 0<b a, n > 0 (1.1) x 1 - a y = b 0<b a, n > 0 (1.1') b n sin 2 + cos 2 = 1 x n = = cos 2 6 Superellipse (Lamé curve)

Mathematics: Lecture 1 Differential Equations:

Physics 235 Final Examination December 4, 2006 Solutions

Mapping Radius of Regular Function and Center of Convex Region. Duan Wenxi

For this purpose, we need the following result:

A GENERAL METHOD FOR SOLVING ORDINARY DIFFERENTIAL EQUATIONS: THE FROBENIUS (OR SERIES) METHOD

CHAPTER 5 : SERIES. 5.2 The Sum of a Series Sum of Power of n Positive Integers Sum of Series of Partial Fraction Difference Method

Mathematical Notation Math Calculus & Analytic Geometry I

( ) ( ) ( ) ( ) ( ) # B x ( ˆ i ) ( ) # B y ( ˆ j ) ( ) # B y ("ˆ ( ) ( ) ( (( ) # ("ˆ ( ) ( ) ( ) # B ˆ z ( k )

Expansion by Laguerre Function for Wave Diffraction around an Infinite Cylinder

Chapter 8 Complex Numbers

Week 13 Notes: 1) Riemann Sum. Aim: Compute Area Under a Graph. Suppose we want to find out the area of a graph, like the one on the right:

Repeated Root and Common Root

DRAFT. Formulae and Statistical Tables for A-level Mathematics SPECIMEN MATERIAL. First Issued September 2017

Plane Kinetics of Rigid Bodies 동역학 및 응용

Force and Motion. Force

Physics 604 Problem Set 1 Due Sept 16, 2010

Answers to test yourself questions

1 Using Integration to Find Arc Lengths and Surface Areas

BINOMIAL THEOREM An expression consisting of two terms, connected by + or sign is called a

FI 2201 Electromagnetism

BINOMIAL THEOREM OBJECTIVE PROBLEMS in the expansion of ( 3 +kx ) are equal. Then k =

Pearson Edexcel Level 3 Advanced Subsidiary and Advanced GCE Mathematics and Further Mathematics

ME 501A Seminar in Engineering Analysis Page 1

BINOMIAL THEOREM NCERT An expression consisting of two terms, connected by + or sign is called a

UNIVERSITY OF CALICUT SCHOOL OF DISTANCE EDUCATION

MATHEMATICS IV 2 MARKS. 5 2 = e 3, 4

This immediately suggests an inverse-square law for a "piece" of current along the line.

1. The 0.1 kg particle has a speed v = 10 m/s as it passes the 30 position shown. The coefficient of kinetic friction between the particle and the

Vectors. Vectors in Plane ( 2

2.Decision Theory of Dependence

Force and Motion. Force. Classifying Forces. Physics 11- Summer /21/01. Chapter 4 material 1. Forces are vector quantities!

Section IV.6: The Master Method and Applications

U>, and is negative. Electric Potential Energy

ANSWER KEY PHYSICS. Workdone X

GRAPHING LINEAR EQUATIONS. Linear Equations. x l ( 3,1 ) _x-axis. Origin ( 0, 0 ) Slope = change in y change in x. Equation for l 1.

MATH Midterm Solutions

EGN 3353C Fluid Mechanics

Solutions to Midterm Physics 201

Lecture 24: Observability and Constructibility

Technical Report: Bessel Filter Analysis

EXERCISE - 01 CHECK YOUR GRASP

ELECTRO - MAGNETIC INDUCTION

Electron states in a periodic potential. Assume the electrons do not interact with each other. Solve the single electron Schrodinger equation: KJ =

Chapter 2: Electric Field

ANSWERS, HINTS & SOLUTIONS HALF COURSE TEST VII (Main)

Winter 2004 OSU Sources of Magnetic Fields 1 Chapter 32

(A) 6.32 (B) 9.49 (C) (D) (E) 18.97

BINOMIAL THEOREM & ITS SIMPLE APPLICATION

Limit of a function:

Chapter Linear Regression

n 2 + 3n + 1 4n = n2 + 3n + 1 n n 2 = n + 1

Optimization. x = 22 corresponds to local maximum by second derivative test

The limit comparison test

Graphing Review Part 3: Polynomials

FOURIER SERIES PART I: DEFINITIONS AND EXAMPLES. To a 2π-periodic function f(x) we will associate a trigonometric series. a n cos(nx) + b n sin(nx),

0 otherwise. sin( nx)sin( kx) 0 otherwise. cos( nx) sin( kx) dx 0 for all integers n, k.

Remarks: (a) The Dirac delta is the function zero on the domain R {0}.

General properties of definite integrals

S(x)along the bar (shear force diagram) by cutting the bar at x and imposing force_y equilibrium.

Numerical integration

Chapter 7 Infinite Series

Finite q-identities related to well-known theorems of Euler and Gauss. Johann Cigler

MA 1201 Engineering Mathematics MO/2017 Tutorial Sheet No. 2

MAGNETIC FIELD INTRODUCTION

Step-index silica fiber


Transcription:

48 E hs simil effect s v. d q E v Fo eltivistic ticles T hs simil effect s dt E c 3 8 V/m such Electic field is beod techicl limits. Electic fields e ol used fo ve lo eegies o Fo setig to coute ottig bems ith diffeet chge. Mcoscoic Fields i Acceletos E Electosttic setos t CESR Geog.Hoffstette@Coell.edu USPAS Advced Acceleto Phsics -3 Jue 6

Geog.Hoffstette@Coell.edu USPAS Advced Acceleto Phsics -3 Jue 6 49 Sttic mgetic fileds: Chge fee sce: is the bem s desig cuve ; E t j E j t ε Fo fiite fields o the desig cuve c be oe eded i d : m m m b Mgetic Fields i Acceletos

5 H llelout H llelout A X A X d s Sufces of Equl Potetil out i A X d s d s X llel llel A d s i i d s A d s d s X Fo lge emebilit Hout is eedicul to the sufce. X d s A d s A Fo highl emeble mteils like io sufces hve costt otetil. Geog.Hoffstette@Coell.edu USPAS Advced Acceleto Phsics -3 Jue 6 X

Geog.Hoffstette@Coell.edu USPAS Advced Acceleto Phsics -3 Jue 6 5 Koledge of the field d the scl mgetic otetil o closed sufce iside mget detemies the mgetic field fo the comlete volume hich is eclosed. G δ [ ] [ ] [ ] [ ] 3 3 3 d G G d G G d G G d G G d V V V V V δ Gee fuctio: Gee s Theoem

Geog.Hoffstette@Coell.edu USPAS Advced Acceleto Phsics -3 Jue 6 5 If field dt i le fo emle the midle of ccloto o of bem lie mget is ko the comlete filed is detemied: Dt of the mgetic field i the le is used to detemie b d b. b b b b [ ] b b b b b b Potetil Esio

53 Comle Potetils i i i i i 4 Im{ Im{ Im{ λ λ Itetio equtio: λ λ 4 λ } λ λ [4 λ λ λ λ λ λ λ ] } The fuctios log lie detemie the comlete field iside mget. λ λ λ 4 λ λ Geog.Hoffstette@Coell.edu USPAS Advced Acceleto Phsics -3 Jue 6 λ λ }

Geog.Hoffstette@Coell.edu USPAS Advced Acceleto Phsics -3 Jue 6 54 e clled the -deedet multiole coefficiets The ide descibes C Smmet oud the -is due to sig chge fte } Im{!!! } 4!!! Im{ ] [ ] [ ϕ λ λ λ λ λ λ λ λ λ λ ϕ λ λ i e π ϕ e 3 S S S N N N Multiole Coefficiets

55 Fige Fields d Mi Fields Mi field Fige field Ol the fige field egio hs tems ith λ d Mi fields i cceleto hsics: ϑ e i i fo fo λ i ϕ ϑ ϕ Im{ e } Geog.Hoffstette@Coell.edu USPAS Advced Acceleto Phsics -3 Jue 6

56 Mi Field Potetil Mi field otetil: si[ ϕ ϑ ] The isolted multiole: siϕ ϑ Whee the ottio of the coodite sstem is set to The otetils oduced b diffeet multiole comoets hve Diffeet ottio smmet C b Diffeet dil deedece Geog.Hoffstette@Coell.edu USPAS Advced Acceleto Phsics -3 Jue 6

Geog.Hoffstette@Coell.edu USPAS Advced Acceleto Phsics -3 Jue 6 57 4 ' '' '' '' ± j m q i m q i m q m q q m γ γ γ γ γ ' ' ' t g dt i e m q g γ g g g e g ig g i t g dt i Focusig i ottig coodite sstem Multioles i Acceletos : Soleoids

Geog.Hoffstette@Coell.edu USPAS Advced Acceleto Phsics -3 Jue 6 58 Soleoid focusig is ek comed to the deflectios ceted b tsvese mgetic field. Tsvese fields: Stog focusig m qv m q ρ γ γ 4 e e m qv q m γ γ q ρ If the soleoids field s eedicul to the ticle s motio its bedig dius ould be Wek focusig < Stog focusig b bout ρ Soleoid vs. Stog Focusig

59 Soleoid Focusig Soleoid mgets e used i detectos fo ticle idetifictio vi ϕ q mγ The soleoid s ottio of the bem is ofte comested b evesed soleoid clled comesto. ρ q Soleoid o Wek Focusig: Soleoids e lso used to focus lo γ bems: Wek focusig fom tul ig focusig: R ϕ R [ R cosϕ ϕ Lieitio i : ] Geog.Hoffstette@Coell.edu USPAS Advced Acceleto Phsics -3 Jue 6 q mγ v ϕ ρ [ R siϕ cosϕ siϕ ] R q mγ

6 Im{ i } C Smmet Multioles i Acceletos : Dioles - - i e SN i - Equiotetil cost. d dt q v Diole mgets e used fo steeig the bems diectio dϕ edig dius: d dt ρ ρ qv q d dϕ dl dϕ vdt d / ρ q Geog.Hoffstette@Coell.edu USPAS Advced Acceleto Phsics -3 Jue 6

6 Diffeet Dioles C-she mget: H-she mget: Wido fme mget: H I out i out H i I H d s H H l H Geog.Hoffstette@Coell.edu USPAS Advced Acceleto Phsics -3 Jue 6 Fe Diole stegth: Fe l Fe H H q ρ I

6 Diole Fields T: Ticl limit sice the field becomes domited b the coils ot the io. Limitig j fo Cu is bout A/mm <.5 T: Ticll used egio < T: Regio i hich I Shims educe the sce tht is oe to the bem but the lso educe the fige field egio. Geog.Hoffstette@Coell.edu USPAS Advced Acceleto Phsics -3 Jue 6

63 Whee is the veticl Diole? HERA Tuel Geog.Hoffstette@Coell.edu USPAS Advced Acceleto Phsics -3 Jue 6

64 Multioles i Acceletos : Quduoles Im{ i } - C Smmet - - - I quduole ticles e focused i oe le d defocused i the othe le. Othe modes of stog focusig e ot ossible. Geog.Hoffstette@Coell.edu USPAS Advced Acceleto Phsics -3 Jue 6

65 Quduole Fields Equiotetil: cost. I H d s H d k e Quduole stegth: q q I Geog.Hoffstette@Coell.edu USPAS Advced Acceleto Phsics -3 Jue 6

66 Rel Quduoles SLAC The coils sho tht this is uight quduole ot otted o ske quduole. PETRA Tuel Geog.Hoffstette@Coell.edu USPAS Advced Acceleto Phsics -3 Jue 6

67 3 3 3 Im{ i } 3 3 3 3 C 3 Smmet S 3 N S 3 S N N Multioles i Acceletos 3: Setuoles 3 3 i Setuole fields hdl ifluece the ticles close to the cete hee oe c lieie i d. ii iii 63 I lie oimtio b shifted setuole hs quduole field. Whe deeds o the eeg oe c build eeg deedet quduole. O Geog.Hoffstette@Coell.edu USPAS Advced Acceleto Phsics -3 Jue 6

68 3 3 Setuole Fields Equiotetil: cost. 3 3 3 I H d s H d 3 3 k Quduole stegth: q q 6I 3 Geog.Hoffstette@Coell.edu USPAS Advced Acceleto Phsics -3 Jue 6

69 Rel Setuoles ESRF Geog.Hoffstette@Coell.edu USPAS Advced Acceleto Phsics -3 Jue 6

7 The CESR Tuel Geog.Hoffstette@Coell.edu USPAS Advced Acceleto Phsics -3 Jue 6

7 Highe ode Multioles Highe ode multioles come fom Field eos i mgets Mgetied mteils Fom multiole mgets tht comeste such eoeous fields To comeste olie effects of othe mgets To stbilie the motio of m ticle sstems To stbilie the olie motio of idividul ticles Im{ i } i q q Multiole stegth: k! uits: m /q is lso clled ρ d used to descibe the eeg of multil chge ios Nmes: diole quduole setuole octuole decole duodecole Geog.Hoffstette@Coell.edu USPAS Advced Acceleto Phsics -3 Jue 6

Geog.Hoffstette@Coell.edu USPAS Advced Acceleto Phsics -3 Jue 6 7 The discussed multioles oduce midle smmetic motio. Whe the field is otted b π/ i.e oe seks of ske multiole. v v v v v v v v v v v v ϑ π F F dt d dt d { } { } { } [ ] Re Im Im Im i i i i e i e i e ϑ ϑ ϑ ϑ Midle Smmetic Motio

73 Suecoductig Mgets Above T the field fom the be coils domite ove the mgetitio of the io. ut Cu ies cot cete much filed ithout io oles: 5T t 5cm distce fom 3cm ie ould equie cuet desit of j I d d π Cu c ol suot bout A/mm. A 389 mm Suecoductig cbles outiel llo cuet desities of 5A/mm t 4.6 K d 6T. Mteils used e usull Nb los e.g. NbTi Nb 3 Ti o Nb 3 S. Suecoductig mgets e ot ol used fo stog fields but lso he thee is o sce fo io oles like iside ticle hsics detecto. Suecoductig.T mgets fo iside the HERA detectos. Geog.Hoffstette@Coell.edu USPAS Advced Acceleto Phsics -3 Jue 6

74 Suecoductig Mgets Poblems: Suecoductivit bkes do fo too lge fields Due to the Meisse-Ochsefeld effect suecoductivit cuet ol flos o thi sufce le. Remed: Suecoductig cble cosists of m ve thi filmets bout m. Geog.Hoffstette@Coell.edu USPAS Advced Acceleto Phsics -3 Jue 6

Geog.Hoffstette@Coell.edu USPAS Advced Acceleto Phsics -3 Jue 6 75 Stight ie t the oigi: I e I j π π ϕ Wie t : { } { } i I I I I I I I e i i i i ϕ π π π π π π π Im l Im l Im l I ] [ π This c be eeseted b comle multiole coefficiets i i Comle Potetil of Wie

76 Cetig multiole be ceted b gemet of ies: π π δ Ai-coil Multioles e i ϕ Iˆ di dϕ if dϕ I ϕ Iˆ cos ϕ ϕ dϕ Idel multiole Aoimte multiole Geog.Hoffstette@Coell.edu USPAS Advced Acceleto Phsics -3 Jue 6

77 Rel Ai-coil Multioles Quduole coecto RHIC Tuel LHC diole Geog.Hoffstette@Coell.edu USPAS Advced Acceleto Phsics -3 Jue 6

78 LHC double quduole Secil SC Ai-coil Mgets Accuc RHIC Sibei Ske diole Geog.Hoffstette@Coell.edu USPAS Advced Acceleto Phsics -3 Jue 6