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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="ru"><front><journal-meta><journal-id journal-id-type="publisher-id">izmertech</journal-id><journal-title-group><journal-title xml:lang="ru">Измерительная техника</journal-title><trans-title-group xml:lang="en"><trans-title>Izmeritel`naya Tekhnika</trans-title></trans-title-group></journal-title-group><issn pub-type="ppub">0368-1025</issn><issn pub-type="epub">2949-5237</issn><publisher><publisher-name>ФГУП "ВНИИФТРИ"</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.32446/0368-1025it.2023-8-67-72</article-id><article-id custom-type="elpub" pub-id-type="custom">izmertech-1986</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>ТЕПЛОФИЗИЧЕСКИЕ ИЗМЕРЕНИЯ</subject></subj-group><subj-group subj-group-type="section-heading" xml:lang="en"><subject>THERMOPHYSIC MEASUREMENTS</subject></subj-group></article-categories><title-group><article-title>Устройство для измерения коэффициента Зеебека термоэлектрических материалов в диапазоне температур 300–800 К</article-title><trans-title-group xml:lang="en"><trans-title>Device for measuring the Seebeck coeffi cient of thermoelectric materials in the temperature range 300–800 K</trans-title></trans-title-group></title-group><contrib-group><contrib contrib-type="author" corresp="yes"><contrib-id contrib-id-type="orcid">https://orcid.org/0000-0002-6576-4613</contrib-id><name-alternatives><name name-style="eastern" xml:lang="ru"><surname>Карпов</surname><given-names>А. В.</given-names></name><name name-style="western" xml:lang="en"><surname>Karpov</surname><given-names>A. V.</given-names></name></name-alternatives><bio xml:lang="ru"><p>Андрей Владиславович Карпов</p><p>г. Черноголовка, Московская область</p></bio><bio xml:lang="en"><p>Andrey V. Karpov</p><p>Chernogolovka, Moscow Region</p></bio><email xlink:type="simple">kavan@ism.ac.ru</email><xref ref-type="aff" rid="aff-1"/></contrib><contrib contrib-type="author" corresp="yes"><contrib-id contrib-id-type="orcid">https://orcid.org/0000-0002-6774-2071</contrib-id><name-alternatives><name name-style="eastern" xml:lang="ru"><surname>Сычев</surname><given-names>А. Е.</given-names></name><name name-style="western" xml:lang="en"><surname>Sytschev</surname><given-names>A. E.</given-names></name></name-alternatives><bio xml:lang="ru"><p>Александр Евгеньевич Сычев</p><p>г. Черноголовка, Московская область</p></bio><bio xml:lang="en"><p>Alexander E. Sytschev</p><p>Chernogolovka, Moscow Region</p></bio><email xlink:type="simple">sytschev@ism.ac.ru</email><xref ref-type="aff" rid="aff-1"/></contrib><contrib contrib-type="author" corresp="yes"><contrib-id contrib-id-type="orcid">https://orcid.org/0009-0000-7292-5887</contrib-id><name-alternatives><name name-style="eastern" xml:lang="ru"><surname>Сивакова</surname><given-names>А. О.</given-names></name><name name-style="western" xml:lang="en"><surname>Sivakova</surname><given-names>A. O.</given-names></name></name-alternatives><bio xml:lang="ru"><p>Алина Олеговна Сивакова</p><p>г. Черноголовка, Московская область</p></bio><bio xml:lang="en"><p>Alina O. Sivakova</p><p>Chernogolovka, Moscow Region</p></bio><email xlink:type="simple">sivakova@ism.ac.ru</email><xref ref-type="aff" rid="aff-1"/></contrib></contrib-group><aff-alternatives id="aff-1"><aff xml:lang="ru"><institution>Институт структурной макрокинетики и проблем материаловедения им. А. Г. Мержанова Российской академии наук</institution><country>Россия</country></aff><aff xml:lang="en"><institution>Merzhanov Institute of Structural Macrokinetics and Materials Science Russian Academy of Sciences</institution><country>Russian Federation</country></aff></aff-alternatives><pub-date pub-type="collection"><year>2023</year></pub-date><pub-date pub-type="epub"><day>21</day><month>09</month><year>2023</year></pub-date><volume>0</volume><issue>8</issue><fpage>67</fpage><lpage>72</lpage><permissions><copyright-statement>Copyright &amp;#x00A9; ФГУП "ВНИИФТРИ", 2023</copyright-statement><copyright-year>2023</copyright-year><copyright-holder xml:lang="ru">ФГУП "ВНИИФТРИ"</copyright-holder><copyright-holder xml:lang="en">ФГУП "ВНИИФТРИ"</copyright-holder><license xlink:href="https://www.izmt.ru/jour/about/submissions#copyrightNotice" xlink:type="simple"><license-p>https://www.izmt.ru/jour/about/submissions#copyrightNotice</license-p></license></permissions><self-uri xlink:href="https://www.izmt.ru/jour/article/view/1986">https://www.izmt.ru/jour/article/view/1986</self-uri><abstract><p>Описано определение потенциальных характеристик электрических свойств новых термоэлектрических материалов по результатам измерений коэффициента Зеебека. Разработано устройство для измерения коэффициента Зеебека (термоэлектродвижущей силы) термоэлектрических материалов в диапазоне температур 300–800 К в среде аргона, воздуха или в вакууме. Подробно описана конструкция и технические характеристики созданного устройства. Для проверки работоспособности разработанного устройства дифференциальным методом измерен коэффициент Зеебека эталонных образцов никеля в диапазоне температур 300–800 К в среде аргона. Погрешность измерений коэффициента Зеебека составляет менее 5 %. Во всём исследуемом интервале температур получены отрицательные значения коэффициента Зеебека никелевого образца, что свидетельствует о преобладании электронов как основных носителей заряда в материале образца. При комнатной температуре измеренный коэффициент Зеебека составляет –19,05 мкВ/К и с повышением температуры до 515 К уменьшается до –25,71 мкВ/К. При дальнейшем повышении температуры до 640 К коэффициент Зеебека монотонно увеличивается до значения  –19,60 мкВ/К. При температурах выше 640 К коэффициент Зеебека непрерывно уменьшается и при 824 К достигает значения –24,12 мкВ/К. Точка Кюри составляет 644 К. Полученные значения коэффициента Зеебека никеля в диапазоне температур 300–800 К сопоставимы с данными, приведёнными в литературе. При расчёте значений коэффициента Зеебека на основании измеренных термоэлектрических напряжений использованы уравнения с известными литературными значениями данного коэффициента для положительной и отрицательных ветвей термопары, что позволяет не привлекать дополнительные измерительные зонды и контакты для измерения термоэлектрического напряжения образца. Установку также можно применять при измерениях электрического сопротивления стандартным четырёхконтактным методом.  </p></abstract><trans-abstract xml:lang="en"><p>The problem of identifying patterns that are associated with the features of the structure and phase composition of new thermoelectric materials obtained by self-propagating high-temperature synthesis is considered. A measuring device has been developed to determine the Seebeck coefficient (thermoelectric motive force) of thermoelectric materials in the temperature range of 300–800 K in argon, air or vacuum. The design of the measuring device is described in detail, the capabilities of the device and the measurement error (less than 5 %) are discussed. The thermoelectromotive force of reference nickel samples in the temperature range of 300–800 K in an argon medium was measured by a differential method. Negative values of the Seebeck coefficient of the nickel sample were obtained throughout the studied temperature range, which indicates the predominance of electrons as the main charge carriers in the sample material. At room temperature, the measured value of the Seebeck coefficient is –19.05 mkV/K and decreases to a value of –25.71 mkV/K with an increase in temperature to 515 K. With a further increase in temperature to 640 K, the Seebeck coefficient monotonically increases to a value of –19.60 mkV/K. At temperatures above 640 K, the Seebeck coefficient continuously decreases and at 824 K reaches a value of –24.12 mkV/K. The Curie point is 644 K. The obtained values of the Seebeck coefficient for nickel in the temperature range 300–800 K are comparable with the data given in the literature. When calculating the Seebeck coefficient of the material, equations are used using the Seebeck coefficient values for the positive and negative thermocouple paths, which eliminates the need for additional measuring probes and contacts to measure the thermoelectric voltage on the sample. The set-up can also be used to make electrical resistance measurements using the standard 4-point method.</p></trans-abstract><kwd-group xml:lang="ru"><kwd>коэффициент Зеебека</kwd><kwd>термоэлектрические материалы</kwd><kwd>термопара</kwd><kwd>зонд</kwd></kwd-group><kwd-group xml:lang="en"><kwd>Seebeck coeffi cient</kwd><kwd>thermoelectric materials</kwd><kwd>thermocouple</kwd><kwd>probe</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">Goldsmid H. J. Introduction to Thermoelectricity. 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