{"title":"An improvement in the approximation of basic curve μ=μ(h) using spline functions","authors":"C. Akyel, S. Babic","doi":"10.1109/ANTEM.1998.7861664","DOIUrl":null,"url":null,"abstract":"This paper deals with a very efficient method in building the magnetic permeability curve using the cubic spline function C(2). We first approximate the basic curve of magnetization B = B(H) using spline function [1] and [3]. From this function we can find the first derivatives analytically. It is also possible to determine the maximum value of magnetic permeability [2]. Having all necessary information about B = B(H) and μmax we can deduce the derivative curve namely B' = B'(H) and also obtain the first derivative at the beginning and at the end of the curve μ = μ(H).","PeriodicalId":334204,"journal":{"name":"1998 Symposium on Antenna Technology and Applied Electromagnetics","volume":"19 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"1998-08-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"1","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"1998 Symposium on Antenna Technology and Applied Electromagnetics","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1109/ANTEM.1998.7861664","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 1
Abstract
This paper deals with a very efficient method in building the magnetic permeability curve using the cubic spline function C(2). We first approximate the basic curve of magnetization B = B(H) using spline function [1] and [3]. From this function we can find the first derivatives analytically. It is also possible to determine the maximum value of magnetic permeability [2]. Having all necessary information about B = B(H) and μmax we can deduce the derivative curve namely B' = B'(H) and also obtain the first derivative at the beginning and at the end of the curve μ = μ(H).