Optimal current shell approximation for solenoids of rectangular cross-section

The manipulation of magnetic objects using variable magnetic fields is a growing field of study with a variety of applications. Many magnetic manipulation systems use multiple electromagnets to generate magnetic fields. To control objects in real time, it is necessary to have a computationally effic...

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Main Authors: Paige L. Husa, Brandon D. Saunders, Brooke E. Suesser, Andrew J. Petruska
Format: Article
Language:English
Published: AIP Publishing LLC 2020-09-01
Series:AIP Advances
Online Access:http://dx.doi.org/10.1063/5.0011847
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spelling doaj-e5424ecaa72840c29c23cad5d52d89052020-11-25T03:58:29ZengAIP Publishing LLCAIP Advances2158-32262020-09-01109095126095126-910.1063/5.0011847Optimal current shell approximation for solenoids of rectangular cross-sectionPaige L. Husa0Brandon D. Saunders1Brooke E. Suesser2Andrew J. Petruska3Colorado School of Mines, 1610 Illinois St., Golden, Colorado 80401, USAColorado School of Mines, 1610 Illinois St., Golden, Colorado 80401, USAColorado School of Mines, 1610 Illinois St., Golden, Colorado 80401, USAColorado School of Mines, 1610 Illinois St., Golden, Colorado 80401, USAThe manipulation of magnetic objects using variable magnetic fields is a growing field of study with a variety of applications. Many magnetic manipulation systems use multiple electromagnets to generate magnetic fields. To control objects in real time, it is necessary to have a computationally efficient method of calculating the field produced by each solenoid anywhere in space. This paper presents a procedure to replace a real cylindrical solenoid of rectangular cross section with infinitely thin shells and rings that generate an equivalent magnetic field. The best approximation for a real solenoid is determined by its physical characteristics. The field produced by these idealized shapes can be calculated expediently using elliptic integrals as can the field gradient and higher-order derivatives. We find that for most real solenoids, the error in the magnetic field approximation is at most 2.5% at a 50% offset and in most cases is much less.http://dx.doi.org/10.1063/5.0011847
collection DOAJ
language English
format Article
sources DOAJ
author Paige L. Husa
Brandon D. Saunders
Brooke E. Suesser
Andrew J. Petruska
spellingShingle Paige L. Husa
Brandon D. Saunders
Brooke E. Suesser
Andrew J. Petruska
Optimal current shell approximation for solenoids of rectangular cross-section
AIP Advances
author_facet Paige L. Husa
Brandon D. Saunders
Brooke E. Suesser
Andrew J. Petruska
author_sort Paige L. Husa
title Optimal current shell approximation for solenoids of rectangular cross-section
title_short Optimal current shell approximation for solenoids of rectangular cross-section
title_full Optimal current shell approximation for solenoids of rectangular cross-section
title_fullStr Optimal current shell approximation for solenoids of rectangular cross-section
title_full_unstemmed Optimal current shell approximation for solenoids of rectangular cross-section
title_sort optimal current shell approximation for solenoids of rectangular cross-section
publisher AIP Publishing LLC
series AIP Advances
issn 2158-3226
publishDate 2020-09-01
description The manipulation of magnetic objects using variable magnetic fields is a growing field of study with a variety of applications. Many magnetic manipulation systems use multiple electromagnets to generate magnetic fields. To control objects in real time, it is necessary to have a computationally efficient method of calculating the field produced by each solenoid anywhere in space. This paper presents a procedure to replace a real cylindrical solenoid of rectangular cross section with infinitely thin shells and rings that generate an equivalent magnetic field. The best approximation for a real solenoid is determined by its physical characteristics. The field produced by these idealized shapes can be calculated expediently using elliptic integrals as can the field gradient and higher-order derivatives. We find that for most real solenoids, the error in the magnetic field approximation is at most 2.5% at a 50% offset and in most cases is much less.
url http://dx.doi.org/10.1063/5.0011847
work_keys_str_mv AT paigelhusa optimalcurrentshellapproximationforsolenoidsofrectangularcrosssection
AT brandondsaunders optimalcurrentshellapproximationforsolenoidsofrectangularcrosssection
AT brookeesuesser optimalcurrentshellapproximationforsolenoidsofrectangularcrosssection
AT andrewjpetruska optimalcurrentshellapproximationforsolenoidsofrectangularcrosssection
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