Multipole Magnets from Maxwell’s Equations...Maxwell’s equations and their physical significance...

Operated by JSA for the U.S. Department of Energy

Thomas Jefferson National Accelerator Facility

http://cas.web.cern.ch/cas/Belgium-2009/Lectures/PDFs/Wolski-1.pdf1

Multipole Magnets from

Maxwell’s Equations

USPAS, Hampton, VA, Jan. 17-28, 2011

Alex Bogacz ,Geoff Krafft and Hisham Sayed

Maxwell’s Equations for Magnets - Outline

Solutions to Maxwell’s equations for magnetostatic fields:

in two dimensions (multipole fields)

in three dimensions (fringe fields, end effects, insertion devices...)

How to construct multipole fields in two dimensions, using

electric currents and magnetic materials, considering

idealized situations.

A. Wolski, University of Liverpool and the Cockcroft Institute, CAS

Specialized Course on Magnets, 2009,

http://cas.web.cern.ch/cas/Belgium-2009/Lectures/PDFs/Wolski-1.pdf

Vector calculus in Cartesian and polar coordinate systems;

Stokes’ and Gauss’ theorems

Maxwell’s equations and their physical significance

Types of magnets commonly used in accelerators.

following notation used in: A. Chao and M. Tigner, “Handbook of

Accelerator Physics and Engineering,” World Scientific (1999).

http://cas.web.cern.ch/cas/Belgium-2009/Lectures/PDFs/Wolski-1.pdf4USPAS, Hampton, VA, Jan. 17-28, 2011

Maxwell’s equations

Physical interpretation of

Linearity and superposition

Multipole fields

Generating multipole fields from a current

distribution

Multipole fields from a current distribution

Superconducting quadrupole - collider final focus

Multipole fields in an iron-core magnet

Generating multipole fields in an iron-core magnet

Maxwell’s Equations for Magnets - Summary

Multipoles in Magnets - Outline

Deduce that the symmetry of a magnet imposes constraints

on the possible multipole field components, even if we relax

the constraints on the material properties and other

geometrical properties;

Consider different techniques for deriving the multipole field

components from measurements of the fields within a

magnet;

Discuss the solutions to Maxwell’s equations that may be

used for describing fields in three dimensions.

Previous lecture re-cap

Allowed and forbidden harmonics

Measuring multipoles

Measuring multipoles in Cartesian basis

Measuring multipoles in Polar basis

Advantages of mode decompositions

Three-dimensional fields

Symmetries in multipole magnets restrict the multipole components that can be

present in the field.

It is useful to be able to find the multipole components in a given field from

numerical field data: but this must be done carefully, if the results are to be

accurate.

Usually, it is advisable to calculate multipole components using field data on a

surface enclosing the region of interest: any errors or residuals will decrease

exponentially within that region, away from the boundary. Outside the

boundary, residuals will increase exponentially.

Techniques for finding multipole components in two dimensional fields can be

generalized to three dimensions, allowing analysis of fringe fields and insertion

devices.

In two or three dimensions, it is possible to use a Cartesian basis for the field

modes; but a polar basis is sometimes more convenient.

Summary – Part II

Appendix A - Field Error Tolerances

Focusing ‘point’ error perturbs the betatron motion leading to the Courant-Snyder invariant change:

Beam envelope and beta-function oscillate at double the betatron frequency

Single point mismatch as measured by the Courant-Snyder invariant change:

22 cos ,

sin , sin cos - sin

( ) 2 ( )

B dlx where k dl

here, m =1 quadrupole, m =2 sextupole, m=3 octupole, etc

Each source of field error (magnet) contributes the following Courant-Snyder variation

2 cos sin sin ,m m

multipole expansion coefficients of the azimuthal magnetic field, B - Fourier series

representation in polar coordinates at a given point along the trajectory):

, cos sin

rB r B m A m

multipole gradient and integrated geometric gradient:

m mmG kGauss cm

r( 1) nn

G dlcm

Cumulative mismatch along the lattice (N sources):

Standard deviation of the Courant-Snyder invariant is given by:

1 2 cos sin sin ,N m m

2 2 21 1

2 cos sin sinN m m

i i m i i m

Assuming weakly focusing lattice (uniform beta modulation) the following averaging

(over the betatron phase) can by applied:

1... ...

Some useful integrals …. :

will reduce the coherent contribution to the C-S variance as follows:

cos sin 0 ,m

Including the first five multipoles yields:

2 cos sin sinN m m

i i m i i m

22 2 2 2 4 2 6

1 2 1 3 3 1 5 2 4

sin 2 sin 2 2 sin ...N

0 m odd1

sin sin 1 !!m even

Beam radius at a given magnet is : 1

One can define a ‘good fileld radius’ for a given type of magnet as:

Assuming the same multipole content for all magnets in the class one gets:

2 2 2 2 4 2

1 2 1 3 3 1 5 2 4

1 3 52 2 2 ...

( ) ia Max a

The first factor purely depends on the beamline optics (focusing), while the second one

describes field tolerance (nonlinearities) of the magnets:

2 2 2 4 2

1 2 1 3 3 1 5 2 4

3 52 2 2 ...

2 2a a

A scalar potential description of the magnetic field has been very useful to

derive the shape for the pole face of a multipole magnet.

Appendix B - The vector potential

Multipole Magnets from Maxwell’s Equations...Maxwell’s equations and their physical significance...

Documents

Displacement Current & Maxwell’s Equations Displacement current Chapter 29: Maxwell’s Equations and Electromagnetic Waves

Lecture 6: Maxwell’s Equations

Chapter 32 Maxwell’s equations; Magnetism of Matter ...bingweb.binghamton.edu/~suzuki/GeneralPhysNote_PDF/LN32v4.pdf · Chapter 32 Maxwell’s equations; Magnetism of Matter Masatsugu

Chapter 4. Electromagnetism and Maxwell’s Equations

In free space Maxwell’s equations become . E = 0 In free space Maxwell’s equations become Gauss’s Law ∆

Maxwell’s Equations

Maxwell’s Equations(M.husnain & M.hassan)

Forward-Mode Differentiation of Maxwell’s Equations

Lecture 1 Introduction, Maxwell’s Equations

Maxwell’s Equations (so far…)

Foundations of Maxwell’s Equations€¦ · Foundations of Maxwell’s Equations LEARNING OBJECTIVES † Review selected chronological developments of electromagnetic concepts †

3 Maxwell’s Equations

Maxwell’s equations for magnets - Computing …pcawolski/Teaching/CAS/Bruges/Maxwells...Maxwell’s equations for magnets Andrzej Wolski University of Liverpool, and the Cockcroft

Chapter 19 Maxwell’s Equations

Chapter 32 Maxwell’s Equations Electromagnetic Waves

Maxwell’s Equations in Differential Form

Maxwell’s Equations with Vector Hysteresis - unitn.itvisintin/ARMA2005.pdf · Maxwell’s Equations with Vector Hysteresis A. Visintin - Trento (Italy) Abstract. Electromagnetic

Discrete Electromagnetics: Maxwell’s Equations Tailored · PDF fileDiscrete Electromagnetics: Maxwell’s Equations Tailored to Numerical Simulations Markus Clemens and Thomas Weiland

Maxwell’s Equations in Vacuum

Fabry-Perot resonator Screen Maxwell’s equations