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<article article-type="research-article" dtd-version="1.3" xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink" xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance" xml:lang="en"><front><journal-meta><journal-id journal-id-type="publisher-id">mrisel</journal-id><journal-title-group><journal-title xml:lang="en">Magnetic Resonance in Solids</journal-title><trans-title-group xml:lang="ru"><trans-title>Magnetic Resonance in Solids</trans-title></trans-title-group></journal-title-group><issn pub-type="epub">2072-5981</issn><publisher><publisher-name>Kazan Federal University</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.26907/mrsej-19201</article-id><article-id custom-type="elpub" pub-id-type="custom">mrisel-45</article-id><article-categories><subj-group subj-group-type="heading"><subject>Research Article</subject></subj-group><subj-group subj-group-type="section-heading" xml:lang="ru"><subject>Статьи</subject></subj-group></article-categories><title-group><article-title>Size effect for asphaltene particles in the resin by NMR</article-title><trans-title-group xml:lang="ru"><trans-title></trans-title></trans-title-group></title-group><contrib-group><contrib contrib-type="author" corresp="yes"><name-alternatives><name name-style="western" xml:lang="en"><surname>Ivanov</surname><given-names>D. S.</given-names></name></name-alternatives><bio xml:lang="en"><p>Kremlevskaya 18, Kazan 420008</p></bio><email xlink:type="simple">f.ma.dima@mail.ru</email><xref ref-type="aff" rid="aff-1"/></contrib><contrib contrib-type="author" corresp="yes"><name-alternatives><name name-style="western" xml:lang="en"><surname>Barskaya</surname><given-names>E. E.</given-names></name></name-alternatives><bio xml:lang="en"><p>Kazan 420029</p></bio><xref ref-type="aff" rid="aff-2"/></contrib><contrib contrib-type="author" corresp="yes"><name-alternatives><name name-style="western" xml:lang="en"><surname>Skirda</surname><given-names>V. D.</given-names></name></name-alternatives><bio xml:lang="en"><p>Kremlevskaya 18, Kazan 420008</p></bio><xref ref-type="aff" rid="aff-1"/></contrib></contrib-group><aff xml:lang="en" id="aff-1"><institution>Kazan Federal University</institution><country>Russian Federation</country></aff><aff xml:lang="en" id="aff-2"><institution>Arbuzov Institute of Organic and Physical Chemistry</institution><country>Russian Federation</country></aff><pub-date pub-type="collection"><year>2019</year></pub-date><pub-date pub-type="epub"><day>08</day><month>04</month><year>2019</year></pub-date><volume>21</volume><issue>2</issue><elocation-id>19201 (10 pp.)</elocation-id><permissions><copyright-statement>Copyright &amp;#x00A9; Ivanov D.S., Barskaya E.E., Skirda V.D., 2024</copyright-statement><copyright-year>2024</copyright-year><copyright-holder xml:lang="ru">Ivanov D.S., Barskaya E.E., Skirda V.D.</copyright-holder><copyright-holder xml:lang="en">Ivanov D.S., Barskaya E.E., Skirda V.D.</copyright-holder><license xml:lang="ru" license-type="creative-commons-attribution" xlink:href="https://creativecommons.org/licenses/by/4.0/" xlink:type="simple"><license-p>Данная работа распространяется под лицензией Creative Commons Attribution 4.0.</license-p></license><license xml:lang="en" license-type="creative-commons-attribution" xlink:href="https://creativecommons.org/licenses/by/4.0/" xlink:type="simple"><license-p>This work is licensed under a Creative Commons Attribution 4.0 License.</license-p></license></permissions><self-uri xlink:href="https://www.mrsej.ru/jour/article/view/45">https://www.mrsej.ru/jour/article/view/45</self-uri><abstract><p>The resin-asphaltene model systems with different sizes of asphaltenes are studied by nuclear magnetic resonance (NMR) using the solid-echo sequence. For systems with particle sizes of asphaltenes greater than 50 Âµm, the form of relaxation attenuation consists of two components, one of which is characterized by a typical asphaltene relaxation time of about 20 Âµs. In this case, the Gaussian form describes the relaxation attenuation of this component, which is typical for the NMR signal in disordered solids. At the same time, it is found that the share of the solid component in the NMR signal decreases with decreasing particle size of asphaltenes. The signal drops to zero when the size of asphaltenes particles reaches 10 microns. Based on the estimates of the rotational motion correlation time for an asphaltene particle in a dispersion medium (resin) with a known viscosity value, the influence of two factors is discussed: the difference in the values of macro- and microviscosity of the resin, as well as the possibility of partial dissolution of asphaltenes particles in the resin. The results of repeated measurements for a long time indicate the existence of a reverse process in the system, leading to the aggregation of asphaltene particles.</p></abstract><kwd-group xml:lang="en"><kwd>NMR</kwd><kwd>solid-echo</kwd><kwd>spin-spin relaxation</kwd><kwd>correlation time</kwd><kwd>asphaltene</kwd><kwd>resin</kwd><kwd>aggregation</kwd></kwd-group></article-meta></front><back><ref-list><title>References</title><ref id="cit1"><label>1</label><citation-alternatives><mixed-citation xml:lang="ru">Unger F.G., Andreeva L.N., Krasnogorskaya N.N. Fundamental Aspects of Oil Chemistry, Nauka, Novosibirsk (1995) (in Russian)</mixed-citation><mixed-citation xml:lang="en">Unger F.G., Andreeva L.N., Krasnogorskaya N.N. Fundamental Aspects of Oil Chemistry, Nauka, Novosibirsk (1995) (in Russian)</mixed-citation></citation-alternatives></ref><ref id="cit2"><label>2</label><citation-alternatives><mixed-citation xml:lang="ru">Akbarzadeh K., Dhillon A., Svrcek W.Y., Yarranton H.W. 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