US3393385A - Quadrupole magnet with reduced field distortion - Google Patents

Quadrupole magnet with reduced field distortion Download PDF

Info

Publication number
US3393385A
US3393385A US574818A US57481866A US3393385A US 3393385 A US3393385 A US 3393385A US 574818 A US574818 A US 574818A US 57481866 A US57481866 A US 57481866A US 3393385 A US3393385 A US 3393385A
Authority
US
United States
Prior art keywords
magnet
pole
quadrupole
protrusions
quadrupole magnet
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Expired - Lifetime
Application number
US574818A
Inventor
Gordon T Danby
John W Jackson
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
US Atomic Energy Commission (AEC)
Original Assignee
Atomic Energy Commission Usa
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Atomic Energy Commission Usa filed Critical Atomic Energy Commission Usa
Priority to US574818A priority Critical patent/US3393385A/en
Application granted granted Critical
Publication of US3393385A publication Critical patent/US3393385A/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

Links

Images

Classifications

    • HELECTRICITY
    • H05ELECTRIC TECHNIQUES NOT OTHERWISE PROVIDED FOR
    • H05HPLASMA TECHNIQUE; PRODUCTION OF ACCELERATED ELECTRICALLY-CHARGED PARTICLES OR OF NEUTRONS; PRODUCTION OR ACCELERATION OF NEUTRAL MOLECULAR OR ATOMIC BEAMS
    • H05H13/00Magnetic resonance accelerators; Cyclotrons
    • H05H13/04Synchrotrons
    • HELECTRICITY
    • H05ELECTRIC TECHNIQUES NOT OTHERWISE PROVIDED FOR
    • H05HPLASMA TECHNIQUE; PRODUCTION OF ACCELERATED ELECTRICALLY-CHARGED PARTICLES OR OF NEUTRONS; PRODUCTION OR ACCELERATION OF NEUTRAL MOLECULAR OR ATOMIC BEAMS
    • H05H7/00Details of devices of the types covered by groups H05H9/00, H05H11/00, H05H13/00
    • H05H7/04Magnet systems, e.g. undulators, wigglers; Energisation thereof

Definitions

  • ABSTRACT OF THE DISCLOSURE A quadrupole magnet using pole pieces which are largely rectangular in configuration utilizing protrusions on the faces thereof to reduce down to acceptable values any n-on-linearities and undesirable harmonics which may occur.
  • AGS Alternating Gradient Synchrotron
  • a quadrupole magnet The purpose of a quadrupole magnet is to focus beams of charged particles.
  • a single quadrupole magnet focuses particles in one plane and defocuses them in a plane perpendicular to the focusing plane.
  • a pair of quadrupoles with their focusing planes alternated can be set up to focus in all planes.
  • Another important problem presented in the design of a quadrupole magnet is that of eliminating, or minimizing, harmonic effects and that of reducing to acceptable values non-linearities in the magnetic field.
  • this problem has largely been overcome by calculating with elaborate mathematic techniques a magnet profile of quite complex shape which requires a special die to punch the quadrupole magnets to the shape desired.
  • the cost of the die is spread over the large number of magnets prepared, but, when, as in the usual case a relatively small number of magnets is to be made, the cost attributed to make each magnet becomes very high.
  • the special profile tends to limit to a narrow range the use of the magnet whereas a quadrupole for more general use may be desirable so that it can be used under a greater variety of conditions.
  • the present invention overcomes the disadvantages associated with the use of the profiled magnet by producing a magnet which can be machined readily to obtain an approximation of the shape desired and incorporates specific features designed to reduce down to acceptable values any non-linearities and undesirable harmonics which may occur.
  • pole 3,393,385 Patented July 16, 1968 pieces which are largely rectangular in configuration and are provided with appropriate protrusions to reduce or eliminate the undesirable effects noted above.
  • FIG.1 is an elevation view of a conventional quadrupole magnet such as those used in the AGS;
  • FIG. 2 is a graph of magnetic field intensity versus distance from the center of the air space in a quadrupole magnet
  • FIG. 3 is an elevation view of a quadrupole magnet embodying the principles of this invention.
  • FIG. 3a is an isometric view of a magnetic pole shown in FIG. 3;
  • FIG. 4 is a detailed 'view of a magnet pole piece used in the magnet of F IG. 2;
  • G. 5 is a view showing the face of the pole piece of FIG. 4.
  • FIG. 1 there is illustrated a conventional quadrupole magnet assembly 1 having an air space 2 and curved pole faces 3, 4, 5 and 6 and coils 7 schematically illustrated.
  • the purpose of the curved pole faces is to reduce the harmonic content of magnet 1.
  • the curved faces of the magnet pole pieces 3, 4, 5 and 6 would come together tangentially.
  • room must be left for coils 7 passing between adjacent pieces.
  • RG. 2 What should be an ideal straight line curve R representing the intensity B of the magnetic field as a function of the distance d from center 0 of air space 2 within quadrupole 1, actually droops and forms a curve R as the pole faces are approached.
  • This droop can be considered from a mathematical point of view as being caused by harmonics so that by minimizing the harmonic terms in the equations for the magnetic field the drooping can be minimized to an acceptable level.
  • quadrupole magnet 10 shaped in accordance with this invention consists of pole pieces 12, 14, 16 and 18 assembled in the square array as shown to form an air gap 20 and pairs of copper windings 24, 26, ped around pole pieces 12, 14, 16 and 18 respectively.
  • Structural members 34, 36, 38 and 42 of iron material hold pole pieces 12,-18 together, while iron yokes 44 and 46 are assembled as shown to complete the necessary magnetic circuits as described in our previously mentioned patent application.
  • Pole pieces 12-18 have the shape shown for piece 16 illustrated in FIG. 3a.
  • Each of the pole pieces 12, 14, 16 and 18 is provided with a pole face 121:, 14a, 16a and 18a, respectively, which is a flat surface on which a plurality of bumps or protrusions 50 are formed.
  • pole piece 14 with pole face 14a on which a pair of stepped protrusions 52 and 54 are formed. It was found that the use of such bumps or protrusions on the pole faces can be used successfully to suppress harmonics and that it was unnecessary to go to the more elaborate curvatures of the faces themselves as has been thought to be the case up to now.
  • the protrusions extend the whole depth of each pole face and are symmetrical across the width of the pole face.
  • Protrusions 52 and 54 extend along the whole length of piece 14 as indicated for piece 16 in FIG. 3a.
  • steps or protrusions 52 and 54 tend to cancel the effect of having the spaces between adjoining pole pieces to accommodate the coils necessary to establish the magnetic fields; and by trying different size protrusions it is possible to bring curve R shownin FIG. 2 up to where it approaches R.
  • the size and number of steps or protrusions 52 and 54 may vary, it is necessary to locate them in the center of the pole faces, to make them symmetrical across the face, and have the faces parallel to that of the pole faces.
  • a quadrupole electro-magnet comprising:

Description

July 16, 1968 G. T. DANBY ETAL 3,393,385
QUADRUPOLE MAGNET WITH REDUCED FIELD DISTORTION iled Aug. 24, 1966 2 Sheets-Sheet l A o d F ig. 2
IO\ 24 I20 26 g9 32 I80 I60 50 2s iii F /'g. 3 INVENTOR.
QUADRUPOLE MAGNET WITH REDUCED FIELD DISTORTION Filed Aug. 24. 1966 2 Sheets-Sheet 2 Fig. 4
Fig. 5 INVENTOR.
GORDON T. DANBY JOHN W. JACKSON United States Patent 3,393,385 QUADRUPOLE MAGNET WITH REDUCED FIELD DISTORTION Gordon T. Danby, Wading River, and John W. Jackson,
Medford, N.Y., assignors to the United States of America as represented by the United States Atomic Energy Commission Filed Aug. 24, 1966, Ser. No. 574,818 2 Claims. (Cl. 335-410) ABSTRACT OF THE DISCLOSURE A quadrupole magnet using pole pieces which are largely rectangular in configuration utilizing protrusions on the faces thereof to reduce down to acceptable values any n-on-linearities and undesirable harmonics which may occur.
The invention described herein was made in the course of, or under a contract with the US. Atomic Energy Commission.
Background of the invention The Alternating Gradient Synchrotron (AGS) located at the Brookhaven National Laboratory utilizes a series of combined function quadrupole focusing and dipole bending magnets to keep the proton beam focused and bent around a circular path.
The purpose of a quadrupole magnet is to focus beams of charged particles. A single quadrupole magnet focuses particles in one plane and defocuses them in a plane perpendicular to the focusing plane. However, a pair of quadrupoles with their focusing planes alternated can be set up to focus in all planes.
In our US. Patent No. 3,284,744, issued Nov. 8, 1966, entitled Quadrupole Magnet with Reduced Lateral Dimension we presented an improved quadrupole magnet construction which makes it possible to utilize quadrupole magnets for the purpose of taking away from the primary proton beam path secondary particles at an angle which is smaller than was previously possible due to reduced lateral dimension of the magnet covered in the mentioned application.
Another important problem presented in the design of a quadrupole magnet is that of eliminating, or minimizing, harmonic effects and that of reducing to acceptable values non-linearities in the magnetic field. Heretofore, this problem has largely been overcome by calculating with elaborate mathematic techniques a magnet profile of quite complex shape which requires a special die to punch the quadrupole magnets to the shape desired. Where a large number of identical magnets are required for a specific situation the cost of the die is spread over the large number of magnets prepared, but, when, as in the usual case a relatively small number of magnets is to be made, the cost attributed to make each magnet becomes very high. In addition, the special profile tends to limit to a narrow range the use of the magnet whereas a quadrupole for more general use may be desirable so that it can be used under a greater variety of conditions.
Description of the invention The present invention overcomes the disadvantages associated with the use of the profiled magnet by producing a magnet which can be machined readily to obtain an approximation of the shape desired and incorporates specific features designed to reduce down to acceptable values any non-linearities and undesirable harmonics which may occur.
In this invention it is accomplished by using pole 3,393,385 Patented July 16, 1968 pieces which are largely rectangular in configuration and are provided with appropriate protrusions to reduce or eliminate the undesirable effects noted above.
It is thus a principal object of this invention to provide a quadrupole magnet of simple shape utilizing protrusions to reduce harmonics and non-linearities in the magnetic field.
Other objects and advantages of this invention will hereinafter become readily apparent from the following description of a preferred embodiment of this invention taken with respect to the accompanying drawings in which:
FIG.1 is an elevation view of a conventional quadrupole magnet such as those used in the AGS;
FIG. 2 is a graph of magnetic field intensity versus distance from the center of the air space in a quadrupole magnet;
FIG. 3 is an elevation view of a quadrupole magnet embodying the principles of this invention;
FIG. 3a is an isometric view of a magnetic pole shown in FIG. 3;
FIG. 4 is a detailed 'view of a magnet pole piece used in the magnet of F IG. 2; and
G. 5 is a view showing the face of the pole piece of FIG. 4.
Referring to FIG. 1 there is illustrated a conventional quadrupole magnet assembly 1 having an air space 2 and curved pole faces 3, 4, 5 and 6 and coils 7 schematically illustrated. The purpose of the curved pole faces is to reduce the harmonic content of magnet 1. In the ideal magnet the curved faces of the magnet pole pieces 3, 4, 5 and 6 would come together tangentially. However, as is illustrated, room must be left for coils 7 passing between adjacent pieces. Thus, as shown in RG. 2 What should be an ideal straight line curve R representing the intensity B of the magnetic field as a function of the distance d from center 0 of air space 2 within quadrupole 1, actually droops and forms a curve R as the pole faces are approached. This droop can be considered from a mathematical point of view as being caused by harmonics so that by minimizing the harmonic terms in the equations for the magnetic field the drooping can be minimized to an acceptable level.
In accordance with this invention it is possible to minimize this harmonic effect without resorting to elaborately designed magnetic pole pieces. Referring to FIG. 3, quadrupole magnet 10 shaped in accordance with this invention consists of pole pieces 12, 14, 16 and 18 assembled in the square array as shown to form an air gap 20 and pairs of copper windings 24, 26, ped around pole pieces 12, 14, 16 and 18 respectively. Structural members 34, 36, 38 and 42 of iron material hold pole pieces 12,-18 together, while iron yokes 44 and 46 are assembled as shown to complete the necessary magnetic circuits as described in our previously mentioned patent application. Pole pieces 12-18 have the shape shown for piece 16 illustrated in FIG. 3a.
Each of the pole pieces 12, 14, 16 and 18 is provided with a pole face 121:, 14a, 16a and 18a, respectively, which is a flat surface on which a plurality of bumps or protrusions 50 are formed.
Referring to FIGS. 4 and 5 for a more particular description of protrusions 50, there is illustrated pole piece 14 with pole face 14a on which a pair of stepped protrusions 52 and 54 are formed. It was found that the use of such bumps or protrusions on the pole faces can be used successfully to suppress harmonics and that it was unnecessary to go to the more elaborate curvatures of the faces themselves as has been thought to be the case up to now. The protrusions extend the whole depth of each pole face and are symmetrical across the width of the pole face.
28 and 32 wrap-- It was determined'that the shape of protrusions 52 and 54 was not critical but cross-sectional surface areas are, and also it was necessary to have the protrusion surfaces parallel to that of the pole faces. Hence, simple rectangular protrusions, readily machinable, may be used to obtain the improved magnet characteristics. Protrusions 52 and 54 extend along the whole length of piece 14 as indicated for piece 16 in FIG. 3a.
The use of steps or protrusions 52 and 54 tend to cancel the effect of having the spaces between adjoining pole pieces to accommodate the coils necessary to establish the magnetic fields; and by trying different size protrusions it is possible to bring curve R shownin FIG. 2 up to where it approaches R. Thus, it was found while the size and number of steps or protrusions 52 and 54 may vary, it is necessary to locate them in the center of the pole faces, to make them symmetrical across the face, and have the faces parallel to that of the pole faces. An incidental but important advantage resulting from this invention is that it makes it possible to accommodate for a given magnetic field, coil assemblies using bigger copper conductors with the result that losses can be reduced and greater magnet efficiency is obtained without sacrificing field linearity.
It is thus seen that there has been provided a unique and remarkably effective approach to the problem of eliminating unwanted distortions in the field of a quadrupole magnet. While only a preferred embodiment has been shown it is understood that many changes thereof may be made without departing from the principles of this invention which is limited only by the scope of the appended claims. t 1 n We claim:
1. A quadrupole electro-magnet comprising:
(a) four pole pieces assembled in spaced relationship to form the corners of arectangle and a central air 'gap, each of said pole pieceshavi'ng a flat pole. face bordering said air gap;
(b) coils wrapped around each of said pole-pieces to I carry'jelectric current to establish magnetic fields and fluxes in said'pole'pieces; and v (c) means consistingof protrusions mounted integrally on each of said pole faces to minimize distortion in the magnetic field extending through said air gap, said protrusions on each pole face being stepped and having surfaces facing said air gap parallel to the flat surface of the respective pole face.
2. The magnet of claim 1 in which the protrusions in each pole face extend the whole length of the latter and 20 are symmetrical across the width of the pole face.
References Cited UNITED STATES PATENTS 2,882,396 4/1959 Courant et al 328-235 2,943,265 6/1960 Kaiser 335-210 XR 3,355,586 11/1967 Brechna et a1. 335-210 XR GEORGE HARRIS, Primary Examiner.
US574818A 1966-08-24 1966-08-24 Quadrupole magnet with reduced field distortion Expired - Lifetime US3393385A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
US574818A US3393385A (en) 1966-08-24 1966-08-24 Quadrupole magnet with reduced field distortion

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
US574818A US3393385A (en) 1966-08-24 1966-08-24 Quadrupole magnet with reduced field distortion

Publications (1)

Publication Number Publication Date
US3393385A true US3393385A (en) 1968-07-16

Family

ID=24297772

Family Applications (1)

Application Number Title Priority Date Filing Date
US574818A Expired - Lifetime US3393385A (en) 1966-08-24 1966-08-24 Quadrupole magnet with reduced field distortion

Country Status (1)

Country Link
US (1) US3393385A (en)

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US3831121A (en) * 1973-07-10 1974-08-20 Magna Tek Syst Inc Focusing magnet
US3980916A (en) * 1975-07-22 1976-09-14 The United States Of America As Represented By The United States Energy Research And Development Administration Beam limiter for thermonuclear fusion devices
US5347254A (en) * 1993-03-08 1994-09-13 The United States Of America As Represented By The Secretary Of The Army Tubular structure having transverse magnetic field with gradient

Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US2882396A (en) * 1953-10-30 1959-04-14 Ernest D Courant High energy particle accelerator
US2943265A (en) * 1957-02-08 1960-06-28 Herman F Kaiser Electron cyclotron
US3355586A (en) * 1964-12-23 1967-11-28 Brechna Habib Modified magnetic momentum slit including a pair of c-type magnets

Patent Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US2882396A (en) * 1953-10-30 1959-04-14 Ernest D Courant High energy particle accelerator
US2943265A (en) * 1957-02-08 1960-06-28 Herman F Kaiser Electron cyclotron
US3355586A (en) * 1964-12-23 1967-11-28 Brechna Habib Modified magnetic momentum slit including a pair of c-type magnets

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US3831121A (en) * 1973-07-10 1974-08-20 Magna Tek Syst Inc Focusing magnet
US3980916A (en) * 1975-07-22 1976-09-14 The United States Of America As Represented By The United States Energy Research And Development Administration Beam limiter for thermonuclear fusion devices
US5347254A (en) * 1993-03-08 1994-09-13 The United States Of America As Represented By The Secretary Of The Army Tubular structure having transverse magnetic field with gradient

Similar Documents

Publication Publication Date Title
US5117212A (en) Electromagnet for charged-particle apparatus
EP0306966A2 (en) Bending magnet
JP2018063949A (en) Magnetic structure for isochronism superconducting compact cyclotron
RU2693565C1 (en) Compact deflecting magnet
US3596167A (en) Cascade transformer high voltage generator
US5596304A (en) Permanent magnet edge-field quadrupole
US3393385A (en) Quadrupole magnet with reduced field distortion
US3831121A (en) Focusing magnet
US4095201A (en) Device for the magnetic correction of the trajectories of a beam of accelerated particles emerging from a cyclotron
Herminghaus The polytron as a cw electron accelerator in the 10 GeV range
US3303426A (en) Strong focusing of high energy particles in a synchrotron storage ring
US3781732A (en) Coil arrangement for adjusting the focus and/or correcting the aberration of streams of charged particles by electromagnetic deflection, particularly for sector field lenses in mass spectrometers
US3284744A (en) Quadrupole magnet with reduced lateral dimension
US10062486B1 (en) High performance superconducting undulator
US3789335A (en) Magnetic focusing device for an isochronous cyclotron
US2824987A (en) Electron optical elements and systems equivalent to light optical prisms for charge carriers in discharge vessels
US3388359A (en) Particle beam focussing magnet with a septum wall
US3304523A (en) Magnetic field straightener
US3265925A (en) Field perturbing means for preventing beam scalloping in reversed field focusing system
Korchuganov et al. Optimization of parameters of a dedicated synchrotron radiation source for technology
US3355586A (en) Modified magnetic momentum slit including a pair of c-type magnets
US3404360A (en) Transformer core construction
US3310764A (en) Connection system for magnet excitation coils
Bassalat et al. High Field Hybrid Permanent Magnet Wiggler Optimized for Tunable Synchrotron Radiation Spectrum
Danby et al. Magnet design for a very high energy synchrotron employing a separated function magnet lattice