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 <front>
  <journal-meta>
   <journal-id journal-id-type="publisher-id">Solnechno-Zemnaya Fizika</journal-id>
   <journal-title-group>
    <journal-title xml:lang="en">Solnechno-Zemnaya Fizika</journal-title>
    <trans-title-group xml:lang="ru">
     <trans-title>Солнечно-земная физика</trans-title>
    </trans-title-group>
   </journal-title-group>
   <issn publication-format="online">2712-9640</issn>
  </journal-meta>
  <article-meta>
   <article-id pub-id-type="publisher-id">38662</article-id>
   <article-id pub-id-type="doi">10.12737/szf-64202009</article-id>
   <article-categories>
    <subj-group subj-group-type="toc-heading" xml:lang="ru">
     <subject>Результаты  исследований</subject>
    </subj-group>
    <subj-group subj-group-type="toc-heading" xml:lang="en">
     <subject>Results of current research</subject>
    </subj-group>
    <subj-group>
     <subject>Результаты  исследований</subject>
    </subj-group>
   </article-categories>
   <title-group>
    <article-title xml:lang="en">Applying the method of maximum contributions to the magnetogram inversion technique</article-title>
    <trans-title-group xml:lang="ru">
     <trans-title>ПРИМЕНЕНИЕ МЕТОДА НАИБОЛЬШИХ ВКЛАДОВ В ТЕХНИКЕ ИНВЕРСИИ МАГНИТОГРАММ</trans-title>
    </trans-title-group>
   </title-group>
   <contrib-group content-type="authors">
    <contrib contrib-type="author">
     <name-alternatives>
      <name xml:lang="ru">
       <surname>Пенских</surname>
       <given-names>Юрий Владимирович</given-names>
      </name>
      <name xml:lang="en">
       <surname>Penskikh</surname>
       <given-names>Yury Vladimirovich</given-names>
      </name>
     </name-alternatives>
     <email>penskikh@iszf.irk.ru</email>
     <xref ref-type="aff" rid="aff-1"/>
    </contrib>
   </contrib-group>
   <aff-alternatives id="aff-1">
    <aff>
     <institution xml:lang="ru">Институт солнечно-земной физики СО РАН</institution>
     <city>Иркутск</city>
     <country>Россия</country>
    </aff>
    <aff>
     <institution xml:lang="en">Institute of Solar Terrestrial Physics SB RAS</institution>
     <city>Irkutsk</city>
     <country>Russian Federation</country>
    </aff>
   </aff-alternatives>
   <volume>6</volume>
   <issue>4</issue>
   <fpage>67</fpage>
   <lpage>76</lpage>
   <self-uri xlink:href="https://naukaru.ru/en/nauka/article/38662/view">https://naukaru.ru/en/nauka/article/38662/view</self-uri>
   <abstract xml:lang="ru">
    <p>Основы созданного Гауссом сферического гармонического анализа (СГА) геомагнитного поля приобрели классическую форму Чепмена—Шмидта в первой половине ХХ в. В отечественной геомагнитологии метод СГА активно развивался  в ИЗМИРАНе, а с началом космической эры — и  в ИСЗФ СО РАН, где со временем СГА стал основой комплексного метода ТИМ (техники инверсии магнитограмм). СГА решает обратную задачу теории потенциала, в которой рассчитываются источники поля геомагнитных вариаций (ПГВ) — внутренние и внешние электрические токи. В алгоритме СГА формируется система линейных алгебраических уравнений (СЛАУ), включающая 3K уравнений (три компоненты вариаций геомагнитного поля, K — число наземных магнитных станций). Малые изменения левой и/или правой частей такой СЛАУ могут привести к значительному изменению неизвестных переменных. Как следствие, два последовательных момента времени с практически одинаковыми значениями ПГВ аппроксимируются значительно отличающимися коэффициентами СГА, что противоречит и логике, и реальным наблюдениям геомагнитного поля. Неустранимая погрешность магнитометров, как и различные методики определения ПГВ на магнитных станциях мировой сети, приводят также к неустойчивости решения СЛАУ. Для оптимального решения этой задачи около полувека назад в ИСЗФ СО РАН был разработан метод наибольших вкладов (МНВ) (Method of maximum contribution, MMC). В данной работе изложены основы этого оригинального метода, а также предложен ряд его модификаций, повышающих точность и/или скорость решения СЛАУ. Показано преимущество МНВ перед другими популярными методами, особенно для Южного полушария Земли.</p>
   </abstract>
   <trans-abstract xml:lang="en">
    <p>Fundamentals of the spherical harmonic analysis (SHA) of the geomagnetic field were created by Gauss. They acquired the classical Chapman — Schmidt form in the first half of the XXth century. The SHA method was actively developed for domestic geomagnetology by IZMIRAN, and then, since the start of the space age, by ISTP SB RAS, where SHA became the basis for a comprehensive method of MIT (magnetogram inversion technique). SHA solves the inverse problem of potential theory and calculates sources of geomagnetic field variations (GFV) - internal and external electric currents. The SHA algorithm forms a system of linear equations (SLE), which consists of 3K equations (three components of the geomagnetic field, K is the number of ground magnetic stations). Small changes in the left and (or) right side of such SLE can lead to a significant change in unknown variables. As a result, two consecutive instants of time with almost identical GFV are approximated by significantly different SHA coefficients. This contradicts both logic and real observations of the geomagnetic field. The inherent error of magnetometers, as well as the method for determining GFV, also entails the instability of SLE solution. To solve such SLEs optimally, the method of maximum contribution (MMC) was developed at ISTP SB RAS half a century ago. This paper presents basics of the original method and proposes a number of its modifications that increase the accuracy and (or) speed of solving the SLEs. The advantage of MMC over other popular methods is shown, especially for the Southern Hemisphere of Earth.</p>
   </trans-abstract>
   <kwd-group xml:lang="ru">
    <kwd>эквивалентная токовая функция</kwd>
    <kwd>техника инверсии магнитограмм</kwd>
    <kwd>сферический гармонический анализ</kwd>
    <kwd>система линейных алгебраических уравнений</kwd>
   </kwd-group>
   <kwd-group xml:lang="en">
    <kwd>equivalent current function</kwd>
    <kwd>magnetogram inversion technique</kwd>
    <kwd>spherical harmonic analysis</kwd>
    <kwd>system of linear equation</kwd>
   </kwd-group>
  </article-meta>
 </front>
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  <p></p>
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