{"title":"THE DETERMINATION OF ORIENTATION DISTRIBUTION FUNCTION FROM INCOMPLETE POLE FIGURES AN EXAMPLE OF A COMPUTER PROGRAM","authors":"J. Jura, J. Pośpiech","doi":"10.1155/TSM.3.1","DOIUrl":null,"url":null,"abstract":"The use of incomplete pole figure data for \ndefining the orientation distribution function (ODF) in \na polycrystalline material is of great practical importance, \nbecause it enables the use of experimental data \nfrom a simplified measurement. The present paper provides \nthe source text of a computer program for calculating \nthe coefficients of ODF series expansion, Clμυ. The data for computations are in the incomplete pole figures of rhombic symmetry as determined by the \nback reflection or transmission technique for crystalline \nsolids of the cubic system. Also described is the \nnumerical method of determining the coefficients Clμυ, \nand the results so obtained are discussed.","PeriodicalId":413822,"journal":{"name":"Texture, Stress, and Microstructure","volume":"191 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"1900-01-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"10","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Texture, Stress, and Microstructure","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1155/TSM.3.1","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 10
Abstract
The use of incomplete pole figure data for
defining the orientation distribution function (ODF) in
a polycrystalline material is of great practical importance,
because it enables the use of experimental data
from a simplified measurement. The present paper provides
the source text of a computer program for calculating
the coefficients of ODF series expansion, Clμυ. The data for computations are in the incomplete pole figures of rhombic symmetry as determined by the
back reflection or transmission technique for crystalline
solids of the cubic system. Also described is the
numerical method of determining the coefficients Clμυ,
and the results so obtained are discussed.