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The integrals determining orientational order in liquid crystals by x-ray diffraction revisited
The orientational distribution function f([beta]) relative to the average orientation direction or director of liquid crystals and related materials can be obtained from the angular variation of the diffracted x-ray intensity distribution I(θ) of the wide-angle or equatorial arcs. The two quantities...
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Published in: | Liquid crystals 2018-04, Vol.45 (5), p.680-686 |
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description | The orientational distribution function f([beta]) relative to the average orientation direction or director of liquid crystals and related materials can be obtained from the angular variation of the diffracted x-ray intensity distribution I(θ) of the wide-angle or equatorial arcs. The two quantities f([beta]) and I(θ) are related by an integral equation. Two different integral equations, one by Kratky and the other by Leadbetter and Norris describing the same phenomena, are the basis of the analyses. There has been discussion of which of the equations is correct; however, the form first derived by Kratky is correct. In this paper, solutions to the Kratky form of the equation are presented. Analytical, closed-form expressions for [Formula omitted.] for n = 0, 1, 2 and 3 are presented. These allow calculation of the first three non-zero orientational order parameters. Experimental data are analysed using solutions to the Kratky kernel and the often used Leadbetter-Norris kernel as a series and in integral form, and the method of Lovell and Mitchell, based on symmetry considerations. The results show that the five approaches obtain indistinguishable values for the second- and fourth-order parameters in the range commonly encountered in liquid crystal studies. |
doi_str_mv | 10.1080/02678292.2017.1372526 |
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The two quantities f([beta]) and I(θ) are related by an integral equation. Two different integral equations, one by Kratky and the other by Leadbetter and Norris describing the same phenomena, are the basis of the analyses. There has been discussion of which of the equations is correct; however, the form first derived by Kratky is correct. In this paper, solutions to the Kratky form of the equation are presented. Analytical, closed-form expressions for [Formula omitted.] for n = 0, 1, 2 and 3 are presented. These allow calculation of the first three non-zero orientational order parameters. Experimental data are analysed using solutions to the Kratky kernel and the often used Leadbetter-Norris kernel as a series and in integral form, and the method of Lovell and Mitchell, based on symmetry considerations. 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The two quantities f([beta]) and I(θ) are related by an integral equation. Two different integral equations, one by Kratky and the other by Leadbetter and Norris describing the same phenomena, are the basis of the analyses. There has been discussion of which of the equations is correct; however, the form first derived by Kratky is correct. In this paper, solutions to the Kratky form of the equation are presented. Analytical, closed-form expressions for [Formula omitted.] for n = 0, 1, 2 and 3 are presented. These allow calculation of the first three non-zero orientational order parameters. Experimental data are analysed using solutions to the Kratky kernel and the often used Leadbetter-Norris kernel as a series and in integral form, and the method of Lovell and Mitchell, based on symmetry considerations. The results show that the five approaches obtain indistinguishable values for the second- and fourth-order parameters in the range commonly encountered in liquid crystal studies.</description><subject>Beta rays</subject><subject>Chemistry</subject><subject>Crystallography</subject><subject>Crystals</subject><subject>Distribution functions</subject><subject>Integral equations</subject><subject>Liquid crystals</subject><subject>Materials Science</subject><subject>Mathematical analysis</subject><subject>Order parameters</subject><subject>X-ray diffraction</subject><issn>0267-8292</issn><issn>1366-5855</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2018</creationdate><recordtype>article</recordtype><recordid>eNo10MtqAyEUgGEpLTS9PEJB2vWkR42jsyyhNwh0k67F8ZIYkplETem8fR2SrkT4zhF_hB4ITAlIeAZaC0kbOqVAxJQwQTmtL9CEsLquuOT8Ek1GU43oGt2ktAEAIaWYILVcOxy67FZRbxO2Lru4C13oVriPwXVZ59B3eltu1sUi8TYcjsFiE4eUx5F2wL9V1AO2wfuozehxdD8hhezsHbryRbn783mLvt9el_OPavH1_jl_WVSGgcyV5dQ5kE3jmRdN29SOtppaRjxYoiWHdtZaKpg2RgvtSSOgFUZ72lJJas7ZLXo87e1TDiqZ8rZZm77rnMmK8BkwKgt6OqF97A9Hl7La9MdYfpdUSdeIurSCovhJmdinFJ1X-xh2Og6KgBqDq__g45RQ5-DsDxtHdH0</recordid><startdate>20180409</startdate><enddate>20180409</enddate><creator>Agra-Kooijman, Deña M.</creator><creator>Fisch, Michael R.</creator><creator>Kumar, Satyendra</creator><general>Taylor & Francis Ltd</general><general>Taylor & Francis</general><scope>AAYXX</scope><scope>CITATION</scope><scope>7SP</scope><scope>7U5</scope><scope>8FD</scope><scope>L7M</scope><scope>OTOTI</scope></search><sort><creationdate>20180409</creationdate><title>The integrals determining orientational order in liquid crystals by x-ray diffraction revisited</title><author>Agra-Kooijman, Deña M. ; Fisch, Michael R. ; Kumar, Satyendra</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c308t-d52ee0899f3f79b96e2ba2d31f0d1a850b4bd273acca7af1970b7caf2b2816553</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2018</creationdate><topic>Beta rays</topic><topic>Chemistry</topic><topic>Crystallography</topic><topic>Crystals</topic><topic>Distribution functions</topic><topic>Integral equations</topic><topic>Liquid crystals</topic><topic>Materials Science</topic><topic>Mathematical analysis</topic><topic>Order parameters</topic><topic>X-ray diffraction</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Agra-Kooijman, Deña M.</creatorcontrib><creatorcontrib>Fisch, Michael R.</creatorcontrib><creatorcontrib>Kumar, Satyendra</creatorcontrib><creatorcontrib>Kent State Univ., Kent, OH (United States)</creatorcontrib><collection>CrossRef</collection><collection>Electronics & Communications Abstracts</collection><collection>Solid State and Superconductivity Abstracts</collection><collection>Technology Research Database</collection><collection>Advanced Technologies Database with Aerospace</collection><collection>OSTI.GOV</collection><jtitle>Liquid crystals</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Agra-Kooijman, Deña M.</au><au>Fisch, Michael R.</au><au>Kumar, Satyendra</au><aucorp>Kent State Univ., Kent, OH (United States)</aucorp><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>The integrals determining orientational order in liquid crystals by x-ray diffraction revisited</atitle><jtitle>Liquid crystals</jtitle><date>2018-04-09</date><risdate>2018</risdate><volume>45</volume><issue>5</issue><spage>680</spage><epage>686</epage><pages>680-686</pages><issn>0267-8292</issn><eissn>1366-5855</eissn><abstract>The orientational distribution function f([beta]) relative to the average orientation direction or director of liquid crystals and related materials can be obtained from the angular variation of the diffracted x-ray intensity distribution I(θ) of the wide-angle or equatorial arcs. The two quantities f([beta]) and I(θ) are related by an integral equation. Two different integral equations, one by Kratky and the other by Leadbetter and Norris describing the same phenomena, are the basis of the analyses. There has been discussion of which of the equations is correct; however, the form first derived by Kratky is correct. In this paper, solutions to the Kratky form of the equation are presented. Analytical, closed-form expressions for [Formula omitted.] for n = 0, 1, 2 and 3 are presented. These allow calculation of the first three non-zero orientational order parameters. Experimental data are analysed using solutions to the Kratky kernel and the often used Leadbetter-Norris kernel as a series and in integral form, and the method of Lovell and Mitchell, based on symmetry considerations. The results show that the five approaches obtain indistinguishable values for the second- and fourth-order parameters in the range commonly encountered in liquid crystal studies.</abstract><cop>Abingdon</cop><pub>Taylor & Francis Ltd</pub><doi>10.1080/02678292.2017.1372526</doi><tpages>7</tpages></addata></record> |
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subjects | Beta rays Chemistry Crystallography Crystals Distribution functions Integral equations Liquid crystals Materials Science Mathematical analysis Order parameters X-ray diffraction |
title | The integrals determining orientational order in liquid crystals by x-ray diffraction revisited |
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