{"title":"High-Energy X-Rays: A tool for Advanced Bulk Investigations in Materials Science and Physics","authors":"K. Liss, A. Bartels, A. Schreyer, H. Clemens","doi":"10.1080/07303300310001634952","DOIUrl":"https://doi.org/10.1080/07303300310001634952","url":null,"abstract":"The combination of these techniques is a strong issue for the construction and development of future \u0000instruments.","PeriodicalId":129427,"journal":{"name":"Textures and Microstructures","volume":"169 1","pages":"0"},"PeriodicalIF":0.0,"publicationDate":"2003-09-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"115794050","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
{"title":"Partial Texture Analysis","authors":"H. Bunge","doi":"10.1155/TSM.12.47","DOIUrl":"https://doi.org/10.1155/TSM.12.47","url":null,"abstract":"The texture is the orientation distribution function of the crystallites of a polycrystalline sample. Being a continuous function of three variables, it requires a large number of values for its complete description. The texture can be expressed in terms of a series expansion. It then requires a large number of coefficients for its complete description. When all functional values or all coefficients are determined from experimental measurements we speak of complete texture analysis. The most important methods for complete texture analysis are individual orientation measurements of a large number of crystals and pole figure measurement followed by pole figure inversion. If only a limited number of values of the texture function or a few of its coefficients are being determined we speak of \"partial texture analysis\". The most important methods of partial texture analysis are the fixed angle texture analyzer and the measurement of the anisotropy of physical properties such as Young’s modulus magnetic properties, thermal expansion and others.","PeriodicalId":129427,"journal":{"name":"Textures and Microstructures","volume":"61 1","pages":"0"},"PeriodicalIF":0.0,"publicationDate":"1900-01-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"123162426","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Y. Perlovich, H. Bunge, M. Isaenkova, V. Fesenko, R. Rustamov
{"title":"X-RAY STUDY OF ROLLED SINGLE CRYSTALS OF TI-48%NI-2%FE ALLOY. PART I : TEXTURE DEVELOPMENT AND MECHANISMS OF PLASTIC DEFORMATION","authors":"Y. Perlovich, H. Bunge, M. Isaenkova, V. Fesenko, R. Rustamov","doi":"10.1155/TSM.31.53","DOIUrl":"https://doi.org/10.1155/TSM.31.53","url":null,"abstract":"Rolled single crystals of the alloy Ti–48%Ni–2%Fe were studied by methods of X-ray diffractometry using a PSD-technique. Single crystals, consisting of the phase B2, were rolled in 11 initial orientations at 350°C with deformation degrees up to ~80%. Texture development in single crystals under rolling was analyzed to determine the acting mechanisms of plastic deformation. Three stable orientations of single crystals were found: {011}〈011〉 ,{111}〈011〉 and {111}〈112〉. It was shown on the basis of texture data, that Ti–Ni single crystals deform by means of combined action of slip in the systems {011}〈001〉 and twinning. For the first time, along with twinning in the known systems {114}〈221〉 , twinning in the systems {118}〈441〉 was revealed. A number of concrete cases was considered to refine the contributions of slip and twinning into reorientation of single crystals depending on their initial orientations as well as to ascertain the interrelation of different mechanisms.","PeriodicalId":129427,"journal":{"name":"Textures and Microstructures","volume":"26 1","pages":"0"},"PeriodicalIF":0.0,"publicationDate":"1900-01-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"116960702","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
{"title":"Texture Analysis of a Zinc Layer on a Steel Substrate Using Neutron Diffraction","authors":"H. Brokmeier","doi":"10.1155/TSM.21.71","DOIUrl":"https://doi.org/10.1155/TSM.21.71","url":null,"abstract":"This paper describes the application of neutron diffraction to investigate the texture of a zinc layer \u00008 μm in thickness. In a nondestructive way both the texture of the zinc layer as well as the texture of \u0000the steel substrate were studied. Therefore, pole figures of iron ( ( 110 ) , ( 200 ) and ( 211 ) ) and of zinc \u0000( ( 0002 ) , ( 10 1 ¯ 0 ) , ( 10 1 ¯ 1 ) ; and ( 10 1 ¯ 3 ) / ( 11 2 ¯ 0 ) ) were measured; additionally the orientation distribution \u0000function of iron and zinc were calculated.","PeriodicalId":129427,"journal":{"name":"Textures and Microstructures","volume":"69 1","pages":"0"},"PeriodicalIF":0.0,"publicationDate":"1900-01-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"127076943","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
{"title":"Texture of Cold-Rolled β-Titanium Alloys With Additions ofHydrogen","authors":"T. Sokolova, L. Anisimova, B. Sokolov","doi":"10.1155/TSM.32.101","DOIUrl":"https://doi.org/10.1155/TSM.32.101","url":null,"abstract":"This paper presents a study of texture investigations in a cold-rolled VT-35 titanium alloy \u0000with hydrogen concentration varied within 0.04–0.55 wt. %. It is shown that the character \u0000of the rolling texture depends on hydrogen contents and is caused by changes in the \u0000mechanism of plastic deformation of the alloy. The poorly deformable alloy may be \u0000plastified by introducing small additions of hydrogen (0.06–0.12wt.%.). The texture \u0000formed in this case has a relatively strong {112}–{100}〈111〉 component and a lowintense \u0000111 component.","PeriodicalId":129427,"journal":{"name":"Textures and Microstructures","volume":"14 1","pages":"0"},"PeriodicalIF":0.0,"publicationDate":"1900-01-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"125946955","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
{"title":"Texture Analysis by theMeasurement of IndividualGrain Orientations—Electron Microscopical Methods and Application on Dual-Phase Steel","authors":"R. Schwarzer, H. Weiland","doi":"10.1155/TSM.8-9.551","DOIUrl":"https://doi.org/10.1155/TSM.8-9.551","url":null,"abstract":"A short review is given on electron microscopical methods for the determination of \u0000local textures. Electron microscopy offers the unique facility of diffraction from well \u0000defined locations in the sample and high resolution imaging of the microstructure. \u0000Standard techniques of orientation determination are the evaluation of electron \u0000diffraction spot and—more recently—Kikuchi patterns, which are applicable to \u0000electron transparent fine-grain materials. Specimen areas smaller than 500 nm or \u000050 nm in diameter, respectively, can be selected. Bulk samples with crystallite sizes \u0000greater than approximately 1 μm or 5 μm, respectively, can be studied with the SEM \u0000using electron backscattering or channelling patterns. For routine work a program \u0000has been developed to do on-line determination of orientation of cubic, orthorhombic \u0000or hexagonal crystals from Kikuchi, channelling and backscattering patterns.Applications of this technique on dual-phase steel are given. The orientation \u0000distribution functions (ODF) of the ferrite and martensite phases from individual \u0000grain measurements are compared with X-ray and neutron pole-figure measurements. \u0000Misorientation distribution functions (MODF) are discussed for contiguous \u0000ferrite-martensite and martensite-martensite grains.","PeriodicalId":129427,"journal":{"name":"Textures and Microstructures","volume":"37 1","pages":"0"},"PeriodicalIF":0.0,"publicationDate":"1900-01-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"126128671","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
{"title":"Orientations of the Cubic Unit Cell and Tetrahedron","authors":"J. C. Casato, W. Fricke","doi":"10.1155/TSM.7.85","DOIUrl":"https://doi.org/10.1155/TSM.7.85","url":null,"abstract":"Charts are presented showing the cubic unit cell and tetrahedron for various simple orientations relative to the rolling plane and direction.","PeriodicalId":129427,"journal":{"name":"Textures and Microstructures","volume":"23 1","pages":"0"},"PeriodicalIF":0.0,"publicationDate":"1900-01-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"125289283","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
H. Bunge, H. Klein, L. Wcislak, U. Garbe, W. Weiss, J. Schneider
{"title":"High-Resolution Imaging of Texture and Microstructure by the Moving Detector Method","authors":"H. Bunge, H. Klein, L. Wcislak, U. Garbe, W. Weiss, J. Schneider","doi":"10.1080/07303300310001642638","DOIUrl":"https://doi.org/10.1080/07303300310001642638","url":null,"abstract":"In order to describe texture and microstructure of a polycrystalline material completely, crystal orientation g = {ϕ1 Φ ϕ2} must be known in all points x = {x 1 x 2 x 3} of the material. This can be achieved by location-resolved diffraction of high-energy, i.e. short-wave, X-rays from synchrotron sources. Highest resolution in the orientation- as well as the location-coordinates can be achieved by three variants of a detector “sweeping” technique in which an area detector is continuously moved during exposure. This technique results in two-dimensionally continuous images which are sections and projections of the six-dimensional “orientation–location” space. Further evaluation of these images depends on whether individual grains are resolved in them or not. Because of the high penetration depth of high-energy synchrotron radiation in matter, this technique is also, and particularly, suitable for the investigation of the interior of big samples.","PeriodicalId":129427,"journal":{"name":"Textures and Microstructures","volume":"727 1","pages":"0"},"PeriodicalIF":0.0,"publicationDate":"1900-01-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"126865901","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
{"title":"CALCULATION OF TEXTURE VOLUME FRACTIONS BY INTEGRATION AND GAUSSIAN FITTING","authors":"M. Cortie","doi":"10.1155/TSM.29.155","DOIUrl":"https://doi.org/10.1155/TSM.29.155","url":null,"abstract":"The concept of texture volume fractions has proved useful in the assessment of the \u0000orientation distributions of polycrystalline samples. Unfortunately, there is more than \u0000one method of calculating volume fractions, and the different techniques may give rather \u0000different answers. The three most commonly used methods appear to be calculation \u0000from the coefficients of the harmonic function, integration over a selected portion of an \u0000orientation distribution function (ODF), or decomposition of an ODF into component \u0000Gaussian ideal textures by a least squares fitting. The integration and Gaussian fitting \u0000methods are examined further here. In particular, the nature of the errors or differences \u0000arising from the method of integration or fitting chosen, the differing interpretations of \u0000the shape and ‘spread’ of the ideal texture, and the effect of neglecting texture components \u0000lying outside of the H0 subspace are considered. Integration of a volume enclosed \u0000by one or more cylinders defined in Eulerian space seems the most robust technique. It is \u0000usually, but not always, acceptable to neglect the effect of texture components lying \u0000outside of H0. However, it is vital that the ‘spread’ of the ideal texture component be \u0000precisely defined, and the texture volume fraction is very sensitive to the magnitude of \u0000the spread as well as to the geometric shape assumed for it.","PeriodicalId":129427,"journal":{"name":"Textures and Microstructures","volume":"189 1","pages":"0"},"PeriodicalIF":0.0,"publicationDate":"1900-01-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"115183085","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
T. Rickert, S. Guldberg, T. Furu, E. Nes, K. Lücke
{"title":"The Effect of Particles on Texture Evolution in Commercial AlMn","authors":"T. Rickert, S. Guldberg, T. Furu, E. Nes, K. Lücke","doi":"10.1155/TSM.14-18.721","DOIUrl":"https://doi.org/10.1155/TSM.14-18.721","url":null,"abstract":"Two commercial Aluminium alloys with high Mn content were investigated in three \u0000different precipitation states. The rolling textures possess a portion of random orientations \u0000that is proportional to the volume fraction of larger particles. It is therefore identified with \u0000their deformation zones having about double the diameter of the particles. The recrystallization \u0000textures are weak for high annealing temperatures and show the more retained rolling \u0000texture the more the temperature is lowered. This is interpreted as a matter of nucleation site. \u0000But also growth mechanisms influence the texture evolution. Minor texture components are \u0000characteristic for the different conditions.","PeriodicalId":129427,"journal":{"name":"Textures and Microstructures","volume":"32 1","pages":"0"},"PeriodicalIF":0.0,"publicationDate":"1900-01-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"122349439","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}