ТОМ 72, №5
Теплопроводность азота при высоких температурах и атмосферном давлении: уточнение обобщенных данных
Проанализированы возможные причины расхождения литературных
обобщенных данных о коэффициенте теплопроводности азота при Р = 0.1 МПа
и Т >>= 300 К. Их уточнение осуществлено с помощью степеннoй
зависимости от температуры в области 300-2500 К.
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Автор:
О. А. Коленчиц
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815-824
Новые интегральные представления аналитических решений краевых задач нестационарного переноса в областях с движущимися границами
Дано развитие метода функций Грина при решении краевых
задач нестационарного переноса в области с движущейся границей. Для
равномерного закона перемещения границы предложена модификация метода
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Автор:
Э. М. Карташов
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равномерного закона перемещения границы предложена модификация метода
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равномерного закона перемещения границы предложена модификация метода
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равномерного закона перемещения границы предложена модификация метода
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Стр:
825-836
Метод канонических элементов для моделирования переносных процессов в многосвязных областях произвольной формы
Излагается уточненный метод канонических элементов для
расчета процессов тепломассопереноса и деформирования в многосвязных
телах сложной конфигурации с криволинейными границами. Представлены
результаты сопоставления данных численных экспериментов с точными
аналитическими решениями.
Array
(
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расчета процессов тепломассопереноса и деформирования в многосвязных
телах сложной конфигурации с криволинейными границами. Представлены
результаты сопоставления данных численных экспериментов с точными
аналитическими решениями.
[~DETAIL_TEXT] => Излагается уточненный метод канонических элементов для
расчета процессов тепломассопереноса и деформирования в многосвязных
телах сложной конфигурации с криволинейными границами. Представлены
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аналитическими решениями.
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Автор:
Н. И. Никитенко , Ю. Н. Кольчик
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[CODE] => YEAR
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[SEARCHABLE] => Y
[FILTRABLE] => Y
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[USER_TYPE] =>
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[~DESCRIPTION] =>
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[~DEFAULT_VALUE] =>
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[TIMESTAMP_X] => 2024-07-09 10:49:32
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[NAME] => Организация
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[CODE] => COMPANY
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[COL_COUNT] => 30
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[MULTIPLE] => Y
[XML_ID] =>
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[USER_TYPE] =>
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[VALUE] =>
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[TIMESTAMP_X] => 2024-07-09 10:49:32
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[SEARCHABLE] => N
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[USER_TYPE] =>
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[HINT] =>
[PROPERTY_VALUE_ID] =>
[VALUE] =>
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[TIMESTAMP_X] => 2021-05-05 12:29:14
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[SORT] => 500
[CODE] => AUTHOR
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[TMP_ID] =>
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[WITH_DESCRIPTION] => N
[SEARCHABLE] => Y
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[0] => 23914
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[VALUE] => Array
(
[0] => Н. И. Никитенко , Ю. Н. Кольчик
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[0] =>
)
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[NAME] => Стр
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[~DESCRIPTION] =>
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Стр:
837-843
Об уравнениях акустики движущихся сред
Методами рациональной механики выведено новое уравнение
акустики неоднородных нестационарно движущихся сред.
Продемонстрировано его преимущество перед традиционными
подходами.
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акустики неоднородных нестационарно движущихся сред.
Продемонстрировано его преимущество перед традиционными
подходами.
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акустики неоднородных нестационарно движущихся сред.
Продемонстрировано его преимущество перед традиционными
подходами.
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[~IBLOCK_EXTERNAL_ID] => 23
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акустики неоднородных нестационарно движущихся сред.
Продемонстрировано его преимущество перед традиционными
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[~NAME] => Ключевые слова
[~DEFAULT_VALUE] =>
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(
[ID] => 100
[TIMESTAMP_X] => 2024-07-09 10:49:32
[IBLOCK_ID] => 23
[NAME] => Стр
[ACTIVE] => Y
[SORT] => 500
[CODE] => PAGE
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[COL_COUNT] => 50
[LIST_TYPE] => L
[MULTIPLE] => N
[XML_ID] => 100
[FILE_TYPE] =>
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[WITH_DESCRIPTION] => N
[SEARCHABLE] => N
[FILTRABLE] => Y
[IS_REQUIRED] => N
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[USER_TYPE] =>
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[HINT] =>
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[VALUE] => 844-850
[DESCRIPTION] =>
[VALUE_ENUM] =>
[VALUE_XML_ID] =>
[VALUE_SORT] =>
[~VALUE] => 844-850
[~DESCRIPTION] =>
[~NAME] => Стр
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(
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[TIMESTAMP_X] => 2016-10-18 16:42:53
[IBLOCK_ID] => 23
[NAME] => Номера
[ACTIVE] => Y
[SORT] => 500
[CODE] => NUMBER_JEPTER
[DEFAULT_VALUE] =>
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[COL_COUNT] => 30
[LIST_TYPE] => L
[MULTIPLE] => N
[XML_ID] => 107
[FILE_TYPE] =>
[MULTIPLE_CNT] => 5
[TMP_ID] =>
[LINK_IBLOCK_ID] => 0
[WITH_DESCRIPTION] => N
[SEARCHABLE] => N
[FILTRABLE] => Y
[IS_REQUIRED] => N
[VERSION] => 1
[USER_TYPE] =>
[USER_TYPE_SETTINGS] =>
[HINT] =>
[PROPERTY_VALUE_ID] =>
[VALUE] =>
[DESCRIPTION] =>
[VALUE_ENUM] =>
[VALUE_XML_ID] =>
[VALUE_SORT] =>
[~VALUE] =>
[~DESCRIPTION] =>
[~NAME] => Номера
[~DEFAULT_VALUE] =>
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[IFZ_FILE] => Array
(
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[TIMESTAMP_X] => 2016-10-13 13:20:50
[IBLOCK_ID] => 23
[NAME] => Файл
[ACTIVE] => Y
[SORT] => 500
[CODE] => IFZ_FILE
[DEFAULT_VALUE] =>
[PROPERTY_TYPE] => F
[ROW_COUNT] => 1
[COL_COUNT] => 30
[LIST_TYPE] => L
[MULTIPLE] => N
[XML_ID] => 304
[FILE_TYPE] =>
[MULTIPLE_CNT] => 5
[TMP_ID] =>
[LINK_IBLOCK_ID] => 0
[WITH_DESCRIPTION] => N
[SEARCHABLE] => N
[FILTRABLE] => N
[IS_REQUIRED] => N
[VERSION] => 1
[USER_TYPE] =>
[USER_TYPE_SETTINGS] =>
[HINT] =>
[PROPERTY_VALUE_ID] =>
[VALUE] =>
[DESCRIPTION] =>
[VALUE_ENUM] =>
[VALUE_XML_ID] =>
[VALUE_SORT] =>
[~VALUE] =>
[~DESCRIPTION] =>
[~NAME] => Файл
[~DEFAULT_VALUE] =>
)
[IFZ_YEAR] => Array
(
[ID] => 366
[TIMESTAMP_X] => 2021-05-06 15:18:10
[IBLOCK_ID] => 23
[NAME] => Год
[ACTIVE] => Y
[SORT] => 500
[CODE] => IFZ_YEAR
[DEFAULT_VALUE] =>
[PROPERTY_TYPE] => L
[ROW_COUNT] => 1
[COL_COUNT] => 30
[LIST_TYPE] => L
[MULTIPLE] => N
[XML_ID] =>
[FILE_TYPE] =>
[MULTIPLE_CNT] => 5
[TMP_ID] =>
[LINK_IBLOCK_ID] => 0
[WITH_DESCRIPTION] => N
[SEARCHABLE] => Y
[FILTRABLE] => Y
[IS_REQUIRED] => N
[VERSION] => 1
[USER_TYPE] =>
[USER_TYPE_SETTINGS] =>
[HINT] =>
[PROPERTY_VALUE_ID] =>
[VALUE] =>
[DESCRIPTION] =>
[VALUE_ENUM] =>
[VALUE_XML_ID] =>
[VALUE_SORT] =>
[VALUE_ENUM_ID] =>
[~VALUE] =>
[~DESCRIPTION] =>
[~NAME] => Год
[~DEFAULT_VALUE] =>
)
[YEAR] => Array
(
[ID] => 390
[TIMESTAMP_X] => 2021-05-04 12:31:09
[IBLOCK_ID] => 23
[NAME] => Год
[ACTIVE] => Y
[SORT] => 500
[CODE] => YEAR
[DEFAULT_VALUE] =>
[PROPERTY_TYPE] => S
[ROW_COUNT] => 1
[COL_COUNT] => 30
[LIST_TYPE] => L
[MULTIPLE] => N
[XML_ID] =>
[FILE_TYPE] =>
[MULTIPLE_CNT] => 5
[TMP_ID] =>
[LINK_IBLOCK_ID] => 0
[WITH_DESCRIPTION] => Y
[SEARCHABLE] => Y
[FILTRABLE] => Y
[IS_REQUIRED] => N
[VERSION] => 1
[USER_TYPE] =>
[USER_TYPE_SETTINGS] =>
[HINT] =>
[PROPERTY_VALUE_ID] =>
[VALUE] =>
[DESCRIPTION] =>
[VALUE_ENUM] =>
[VALUE_XML_ID] =>
[VALUE_SORT] =>
[~VALUE] =>
[~DESCRIPTION] =>
[~NAME] => Год
[~DEFAULT_VALUE] =>
)
[AUTHOR2] => Array
(
[ID] => 391
[TIMESTAMP_X] => 2021-10-20 13:14:23
[IBLOCK_ID] => 23
[NAME] => Автор2
[ACTIVE] => Y
[SORT] => 500
[CODE] => AUTHOR2
[DEFAULT_VALUE] =>
[PROPERTY_TYPE] => S
[ROW_COUNT] => 1
[COL_COUNT] => 30
[LIST_TYPE] => L
[MULTIPLE] => N
[XML_ID] =>
[FILE_TYPE] =>
[MULTIPLE_CNT] => 5
[TMP_ID] =>
[LINK_IBLOCK_ID] => 0
[WITH_DESCRIPTION] => N
[SEARCHABLE] => N
[FILTRABLE] => N
[IS_REQUIRED] => N
[VERSION] => 1
[USER_TYPE] =>
[USER_TYPE_SETTINGS] =>
[HINT] =>
[PROPERTY_VALUE_ID] =>
[VALUE] =>
[DESCRIPTION] =>
[VALUE_ENUM] =>
[VALUE_XML_ID] =>
[VALUE_SORT] =>
[~VALUE] =>
[~DESCRIPTION] =>
[~NAME] => Автор2
[~DEFAULT_VALUE] =>
)
[COMPANY] => Array
(
[ID] => 392
[TIMESTAMP_X] => 2024-07-09 10:49:32
[IBLOCK_ID] => 23
[NAME] => Организация
[ACTIVE] => Y
[SORT] => 500
[CODE] => COMPANY
[DEFAULT_VALUE] =>
[PROPERTY_TYPE] => L
[ROW_COUNT] => 1
[COL_COUNT] => 30
[LIST_TYPE] => L
[MULTIPLE] => Y
[XML_ID] =>
[FILE_TYPE] =>
[MULTIPLE_CNT] => 5
[TMP_ID] =>
[LINK_IBLOCK_ID] => 0
[WITH_DESCRIPTION] => N
[SEARCHABLE] => N
[FILTRABLE] => N
[IS_REQUIRED] => N
[VERSION] => 1
[USER_TYPE] =>
[USER_TYPE_SETTINGS] =>
[HINT] =>
[PROPERTY_VALUE_ID] =>
[VALUE] =>
[DESCRIPTION] =>
[VALUE_ENUM] =>
[VALUE_XML_ID] =>
[VALUE_SORT] =>
[VALUE_ENUM_ID] =>
[~VALUE] =>
[~DESCRIPTION] =>
[~NAME] => Организация
[~DEFAULT_VALUE] =>
)
[UDK] => Array
(
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[TIMESTAMP_X] => 2024-07-09 10:49:32
[IBLOCK_ID] => 23
[NAME] => УДК
[ACTIVE] => Y
[SORT] => 500
[CODE] => UDK
[DEFAULT_VALUE] =>
[PROPERTY_TYPE] => L
[ROW_COUNT] => 1
[COL_COUNT] => 30
[LIST_TYPE] => L
[MULTIPLE] => Y
[XML_ID] =>
[FILE_TYPE] =>
[MULTIPLE_CNT] => 5
[TMP_ID] =>
[LINK_IBLOCK_ID] => 0
[WITH_DESCRIPTION] => N
[SEARCHABLE] => N
[FILTRABLE] => N
[IS_REQUIRED] => N
[VERSION] => 1
[USER_TYPE] =>
[USER_TYPE_SETTINGS] =>
[HINT] =>
[PROPERTY_VALUE_ID] =>
[VALUE] =>
[DESCRIPTION] =>
[VALUE_ENUM] =>
[VALUE_XML_ID] =>
[VALUE_SORT] =>
[VALUE_ENUM_ID] =>
[~VALUE] =>
[~DESCRIPTION] =>
[~NAME] => УДК
[~DEFAULT_VALUE] =>
)
)
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(
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[TIMESTAMP_X] => 2021-05-05 12:29:14
[IBLOCK_ID] => 23
[NAME] => Автор
[ACTIVE] => Y
[SORT] => 500
[CODE] => AUTHOR
[DEFAULT_VALUE] => Автор
[PROPERTY_TYPE] => S
[ROW_COUNT] => 1
[COL_COUNT] => 50
[LIST_TYPE] => L
[MULTIPLE] => Y
[XML_ID] => 98
[FILE_TYPE] =>
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[LINK_IBLOCK_ID] => 0
[WITH_DESCRIPTION] => N
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[USER_TYPE] =>
[USER_TYPE_SETTINGS] =>
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[0] => 23916
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[VALUE] => Array
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[0] => А. И. Шнип
)
[DESCRIPTION] => Array
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[0] =>
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[VALUE_XML_ID] =>
[VALUE_SORT] =>
[~VALUE] => Array
(
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)
[~DESCRIPTION] => Array
(
[0] =>
)
[~NAME] => Автор
[~DEFAULT_VALUE] => Автор
[DISPLAY_VALUE] => А. И. Шнип
)
[PAGE] => Array
(
[ID] => 100
[TIMESTAMP_X] => 2024-07-09 10:49:32
[IBLOCK_ID] => 23
[NAME] => Стр
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[SORT] => 500
[CODE] => PAGE
[DEFAULT_VALUE] =>
[PROPERTY_TYPE] => N
[ROW_COUNT] => 1
[COL_COUNT] => 50
[LIST_TYPE] => L
[MULTIPLE] => N
[XML_ID] => 100
[FILE_TYPE] =>
[MULTIPLE_CNT] => 5
[TMP_ID] =>
[LINK_IBLOCK_ID] => 0
[WITH_DESCRIPTION] => N
[SEARCHABLE] => N
[FILTRABLE] => Y
[IS_REQUIRED] => N
[VERSION] => 1
[USER_TYPE] =>
[USER_TYPE_SETTINGS] =>
[HINT] =>
[PROPERTY_VALUE_ID] => 23917
[VALUE] => 844-850
[DESCRIPTION] =>
[VALUE_ENUM] =>
[VALUE_XML_ID] =>
[VALUE_SORT] =>
[~VALUE] => 844-850
[~DESCRIPTION] =>
[~NAME] => Стр
[~DEFAULT_VALUE] =>
[DISPLAY_VALUE] => 844-850
)
)
)
Автор:
А. И. Шнип
Array
(
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акустики неоднородных нестационарно движущихся сред.
Продемонстрировано его преимущество перед традиционными
подходами.
[~DETAIL_TEXT] => Методами рациональной механики выведено новое уравнение
акустики неоднородных нестационарно движущихся сред.
Продемонстрировано его преимущество перед традиционными
подходами.
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акустики неоднородных нестационарно движущихся сред.
Продемонстрировано его преимущество перед традиционными
подходами.
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[VALUE] =>
[DESCRIPTION] =>
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[~DESCRIPTION] =>
[~NAME] => Год
[~DEFAULT_VALUE] =>
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[XML_ID] =>
[FILE_TYPE] =>
[MULTIPLE_CNT] => 5
[TMP_ID] =>
[LINK_IBLOCK_ID] => 0
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[~DEFAULT_VALUE] =>
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(
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[TIMESTAMP_X] => 2024-07-09 10:49:32
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[NAME] => Организация
[ACTIVE] => Y
[SORT] => 500
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[XML_ID] =>
[FILE_TYPE] =>
[MULTIPLE_CNT] => 5
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[LINK_IBLOCK_ID] => 0
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[USER_TYPE] =>
[USER_TYPE_SETTINGS] =>
[HINT] =>
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[VALUE] =>
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[VALUE_ENUM] =>
[VALUE_XML_ID] =>
[VALUE_SORT] =>
[VALUE_ENUM_ID] =>
[~VALUE] =>
[~DESCRIPTION] =>
[~NAME] => Организация
[~DEFAULT_VALUE] =>
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(
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[TIMESTAMP_X] => 2024-07-09 10:49:32
[IBLOCK_ID] => 23
[NAME] => УДК
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[SORT] => 500
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[IS_REQUIRED] => N
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[USER_TYPE] =>
[USER_TYPE_SETTINGS] =>
[HINT] =>
[PROPERTY_VALUE_ID] =>
[VALUE] =>
[DESCRIPTION] =>
[VALUE_ENUM] =>
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[VALUE_SORT] =>
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Стр:
844-850
Кривая восстановления уровня в релаксационной теории фильтраци
Рассмотрена задача о кривой восстановления уровня в релаксационной
теории фильтрации, когда имеется непрерывный спектр внутренних времен
релаксации. Найдена асимптотика при больших временах как функционал
релаксационного ядра. Для степенного спектра внутренних релаксационных
процессов в системе порода-насыщающая жидкость вычислено явное
выражение с двумя дополнительными параметрами, характеризующими
релаксационное ядро.
Array
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теории фильтрации, когда имеется непрерывный спектр внутренних времен
релаксации. Найдена асимптотика при больших временах как функционал
релаксационного ядра. Для степенного спектра внутренних релаксационных
процессов в системе порода-насыщающая жидкость вычислено явное
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релаксации. Найдена асимптотика при больших временах как функционал
релаксационного ядра. Для степенного спектра внутренних релаксационных
процессов в системе порода-насыщающая жидкость вычислено явное
выражение с двумя дополнительными параметрами, характеризующими
релаксационное ядро.
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релаксации. Найдена асимптотика при больших временах как функционал
релаксационного ядра. Для степенного спектра внутренних релаксационных
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[VALUE_XML_ID] =>
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[~VALUE] =>
[~DESCRIPTION] =>
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Автор:
О. Ю. Динариев
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процессов в системе порода-насыщающая жидкость вычислено явное
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Стр:
850-854
Предельная форма уравнения анизотропной теплопроводности в слое
Рассматривается задача асимптотического сведения трехмерного
по координатам уравнения, описывающего процесс распространения
тепла в анизотропном материале к двумерному уравнению. Область
теплопередачи - тонкий по одной из координат слой. Предполагается,
что матрица коэффициентов температуропроводности зависит от
пространственных координат. В построенном эквивалентном уравнении
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Автор:
А. И. Мошинский
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тепла в анизотропном материале к двумерному уравнению. Область
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что матрица коэффициентов температуропроводности зависит от
пространственных координат. В построенном эквивалентном уравнении
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[PREVIEW_TEXT] =>
[~PREVIEW_TEXT] =>
[PREVIEW_TEXT_TYPE] => text
[~PREVIEW_TEXT_TYPE] => text
[PREVIEW_PICTURE] =>
[~PREVIEW_PICTURE] =>
[LANG_DIR] => /
[~LANG_DIR] => /
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[~PROPERTY_PAGE_VALUE] => 855-861
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[~PROPERTY_PAGE_VALUE_ID] => 23921
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[~SORT] => 500
[CODE] =>
[~CODE] =>
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[~EXTERNAL_ID] => 6907
[IBLOCK_TYPE_ID] => aspro_corporation_content
[~IBLOCK_TYPE_ID] => aspro_corporation_content
[IBLOCK_CODE] => IFZ
[~IBLOCK_CODE] => IFZ
[IBLOCK_EXTERNAL_ID] => 23
[~IBLOCK_EXTERNAL_ID] => 23
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[EDIT_LINK] =>
[DELETE_LINK] =>
[DISPLAY_ACTIVE_FROM] =>
[IPROPERTY_VALUES] => Array
(
)
[FIELDS] => Array
(
[DETAIL_TEXT] => Рассматривается задача асимптотического сведения трехмерного
по координатам уравнения, описывающего процесс распространения
тепла в анизотропном материале к двумерному уравнению. Область
теплопередачи - тонкий по одной из координат слой. Предполагается,
что матрица коэффициентов температуропроводности зависит от
пространственных координат. В построенном эквивалентном уравнении
теплопроводности представлена эффективная матрица
температуропроводности.
)
[PROPERTIES] => Array
(
[AUTHOR] => Array
(
[ID] => 98
[TIMESTAMP_X] => 2021-05-05 12:29:14
[IBLOCK_ID] => 23
[NAME] => Автор
[ACTIVE] => Y
[SORT] => 500
[CODE] => AUTHOR
[DEFAULT_VALUE] => Автор
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[ROW_COUNT] => 1
[COL_COUNT] => 50
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[LINK_IBLOCK_ID] => 0
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[IS_REQUIRED] => N
[VERSION] => 1
[USER_TYPE] =>
[USER_TYPE_SETTINGS] =>
[HINT] =>
[PROPERTY_VALUE_ID] => Array
(
[0] => 23920
)
[VALUE] => Array
(
[0] => А. И. Мошинский
)
[DESCRIPTION] => Array
(
[0] =>
)
[VALUE_ENUM] =>
[VALUE_XML_ID] =>
[VALUE_SORT] =>
[~VALUE] => Array
(
[0] => А. И. Мошинский
)
[~DESCRIPTION] => Array
(
[0] =>
)
[~NAME] => Автор
[~DEFAULT_VALUE] => Автор
)
[KEYWORDS] => Array
(
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[TIMESTAMP_X] => 2021-03-15 13:13:26
[IBLOCK_ID] => 23
[NAME] => Ключевые слова
[ACTIVE] => Y
[SORT] => 500
[CODE] => KEYWORDS
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[ROW_COUNT] => 1
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[XML_ID] => 99
[FILE_TYPE] =>
[MULTIPLE_CNT] => 5
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[LINK_IBLOCK_ID] => 0
[WITH_DESCRIPTION] => N
[SEARCHABLE] => Y
[FILTRABLE] => Y
[IS_REQUIRED] => N
[VERSION] => 1
[USER_TYPE] =>
[USER_TYPE_SETTINGS] =>
[HINT] =>
[PROPERTY_VALUE_ID] =>
[VALUE] =>
[DESCRIPTION] =>
[VALUE_ENUM] =>
[VALUE_XML_ID] =>
[VALUE_SORT] =>
[~VALUE] =>
[~DESCRIPTION] =>
[~NAME] => Ключевые слова
[~DEFAULT_VALUE] =>
)
[PAGE] => Array
(
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[TIMESTAMP_X] => 2024-07-09 10:49:32
[IBLOCK_ID] => 23
[NAME] => Стр
[ACTIVE] => Y
[SORT] => 500
[CODE] => PAGE
[DEFAULT_VALUE] =>
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[XML_ID] => 100
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[SEARCHABLE] => N
[FILTRABLE] => Y
[IS_REQUIRED] => N
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[USER_TYPE] =>
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[HINT] =>
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[VALUE] => 855-861
[DESCRIPTION] =>
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[VALUE_SORT] =>
[~VALUE] => 855-861
[~DESCRIPTION] =>
[~NAME] => Стр
[~DEFAULT_VALUE] =>
)
[NUMBER_JEPTER] => Array
(
[ID] => 107
[TIMESTAMP_X] => 2016-10-18 16:42:53
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[NAME] => Номера
[ACTIVE] => Y
[SORT] => 500
[CODE] => NUMBER_JEPTER
[DEFAULT_VALUE] =>
[PROPERTY_TYPE] => G
[ROW_COUNT] => 1
[COL_COUNT] => 30
[LIST_TYPE] => L
[MULTIPLE] => N
[XML_ID] => 107
[FILE_TYPE] =>
[MULTIPLE_CNT] => 5
[TMP_ID] =>
[LINK_IBLOCK_ID] => 0
[WITH_DESCRIPTION] => N
[SEARCHABLE] => N
[FILTRABLE] => Y
[IS_REQUIRED] => N
[VERSION] => 1
[USER_TYPE] =>
[USER_TYPE_SETTINGS] =>
[HINT] =>
[PROPERTY_VALUE_ID] =>
[VALUE] =>
[DESCRIPTION] =>
[VALUE_ENUM] =>
[VALUE_XML_ID] =>
[VALUE_SORT] =>
[~VALUE] =>
[~DESCRIPTION] =>
[~NAME] => Номера
[~DEFAULT_VALUE] =>
)
[IFZ_FILE] => Array
(
[ID] => 304
[TIMESTAMP_X] => 2016-10-13 13:20:50
[IBLOCK_ID] => 23
[NAME] => Файл
[ACTIVE] => Y
[SORT] => 500
[CODE] => IFZ_FILE
[DEFAULT_VALUE] =>
[PROPERTY_TYPE] => F
[ROW_COUNT] => 1
[COL_COUNT] => 30
[LIST_TYPE] => L
[MULTIPLE] => N
[XML_ID] => 304
[FILE_TYPE] =>
[MULTIPLE_CNT] => 5
[TMP_ID] =>
[LINK_IBLOCK_ID] => 0
[WITH_DESCRIPTION] => N
[SEARCHABLE] => N
[FILTRABLE] => N
[IS_REQUIRED] => N
[VERSION] => 1
[USER_TYPE] =>
[USER_TYPE_SETTINGS] =>
[HINT] =>
[PROPERTY_VALUE_ID] =>
[VALUE] =>
[DESCRIPTION] =>
[VALUE_ENUM] =>
[VALUE_XML_ID] =>
[VALUE_SORT] =>
[~VALUE] =>
[~DESCRIPTION] =>
[~NAME] => Файл
[~DEFAULT_VALUE] =>
)
[IFZ_YEAR] => Array
(
[ID] => 366
[TIMESTAMP_X] => 2021-05-06 15:18:10
[IBLOCK_ID] => 23
[NAME] => Год
[ACTIVE] => Y
[SORT] => 500
[CODE] => IFZ_YEAR
[DEFAULT_VALUE] =>
[PROPERTY_TYPE] => L
[ROW_COUNT] => 1
[COL_COUNT] => 30
[LIST_TYPE] => L
[MULTIPLE] => N
[XML_ID] =>
[FILE_TYPE] =>
[MULTIPLE_CNT] => 5
[TMP_ID] =>
[LINK_IBLOCK_ID] => 0
[WITH_DESCRIPTION] => N
[SEARCHABLE] => Y
[FILTRABLE] => Y
[IS_REQUIRED] => N
[VERSION] => 1
[USER_TYPE] =>
[USER_TYPE_SETTINGS] =>
[HINT] =>
[PROPERTY_VALUE_ID] =>
[VALUE] =>
[DESCRIPTION] =>
[VALUE_ENUM] =>
[VALUE_XML_ID] =>
[VALUE_SORT] =>
[VALUE_ENUM_ID] =>
[~VALUE] =>
[~DESCRIPTION] =>
[~NAME] => Год
[~DEFAULT_VALUE] =>
)
[YEAR] => Array
(
[ID] => 390
[TIMESTAMP_X] => 2021-05-04 12:31:09
[IBLOCK_ID] => 23
[NAME] => Год
[ACTIVE] => Y
[SORT] => 500
[CODE] => YEAR
[DEFAULT_VALUE] =>
[PROPERTY_TYPE] => S
[ROW_COUNT] => 1
[COL_COUNT] => 30
[LIST_TYPE] => L
[MULTIPLE] => N
[XML_ID] =>
[FILE_TYPE] =>
[MULTIPLE_CNT] => 5
[TMP_ID] =>
[LINK_IBLOCK_ID] => 0
[WITH_DESCRIPTION] => Y
[SEARCHABLE] => Y
[FILTRABLE] => Y
[IS_REQUIRED] => N
[VERSION] => 1
[USER_TYPE] =>
[USER_TYPE_SETTINGS] =>
[HINT] =>
[PROPERTY_VALUE_ID] =>
[VALUE] =>
[DESCRIPTION] =>
[VALUE_ENUM] =>
[VALUE_XML_ID] =>
[VALUE_SORT] =>
[~VALUE] =>
[~DESCRIPTION] =>
[~NAME] => Год
[~DEFAULT_VALUE] =>
)
[AUTHOR2] => Array
(
[ID] => 391
[TIMESTAMP_X] => 2021-10-20 13:14:23
[IBLOCK_ID] => 23
[NAME] => Автор2
[ACTIVE] => Y
[SORT] => 500
[CODE] => AUTHOR2
[DEFAULT_VALUE] =>
[PROPERTY_TYPE] => S
[ROW_COUNT] => 1
[COL_COUNT] => 30
[LIST_TYPE] => L
[MULTIPLE] => N
[XML_ID] =>
[FILE_TYPE] =>
[MULTIPLE_CNT] => 5
[TMP_ID] =>
[LINK_IBLOCK_ID] => 0
[WITH_DESCRIPTION] => N
[SEARCHABLE] => N
[FILTRABLE] => N
[IS_REQUIRED] => N
[VERSION] => 1
[USER_TYPE] =>
[USER_TYPE_SETTINGS] =>
[HINT] =>
[PROPERTY_VALUE_ID] =>
[VALUE] =>
[DESCRIPTION] =>
[VALUE_ENUM] =>
[VALUE_XML_ID] =>
[VALUE_SORT] =>
[~VALUE] =>
[~DESCRIPTION] =>
[~NAME] => Автор2
[~DEFAULT_VALUE] =>
)
[COMPANY] => Array
(
[ID] => 392
[TIMESTAMP_X] => 2024-07-09 10:49:32
[IBLOCK_ID] => 23
[NAME] => Организация
[ACTIVE] => Y
[SORT] => 500
[CODE] => COMPANY
[DEFAULT_VALUE] =>
[PROPERTY_TYPE] => L
[ROW_COUNT] => 1
[COL_COUNT] => 30
[LIST_TYPE] => L
[MULTIPLE] => Y
[XML_ID] =>
[FILE_TYPE] =>
[MULTIPLE_CNT] => 5
[TMP_ID] =>
[LINK_IBLOCK_ID] => 0
[WITH_DESCRIPTION] => N
[SEARCHABLE] => N
[FILTRABLE] => N
[IS_REQUIRED] => N
[VERSION] => 1
[USER_TYPE] =>
[USER_TYPE_SETTINGS] =>
[HINT] =>
[PROPERTY_VALUE_ID] =>
[VALUE] =>
[DESCRIPTION] =>
[VALUE_ENUM] =>
[VALUE_XML_ID] =>
[VALUE_SORT] =>
[VALUE_ENUM_ID] =>
[~VALUE] =>
[~DESCRIPTION] =>
[~NAME] => Организация
[~DEFAULT_VALUE] =>
)
[UDK] => Array
(
[ID] => 393
[TIMESTAMP_X] => 2024-07-09 10:49:32
[IBLOCK_ID] => 23
[NAME] => УДК
[ACTIVE] => Y
[SORT] => 500
[CODE] => UDK
[DEFAULT_VALUE] =>
[PROPERTY_TYPE] => L
[ROW_COUNT] => 1
[COL_COUNT] => 30
[LIST_TYPE] => L
[MULTIPLE] => Y
[XML_ID] =>
[FILE_TYPE] =>
[MULTIPLE_CNT] => 5
[TMP_ID] =>
[LINK_IBLOCK_ID] => 0
[WITH_DESCRIPTION] => N
[SEARCHABLE] => N
[FILTRABLE] => N
[IS_REQUIRED] => N
[VERSION] => 1
[USER_TYPE] =>
[USER_TYPE_SETTINGS] =>
[HINT] =>
[PROPERTY_VALUE_ID] =>
[VALUE] =>
[DESCRIPTION] =>
[VALUE_ENUM] =>
[VALUE_XML_ID] =>
[VALUE_SORT] =>
[VALUE_ENUM_ID] =>
[~VALUE] =>
[~DESCRIPTION] =>
[~NAME] => УДК
[~DEFAULT_VALUE] =>
)
)
[DISPLAY_PROPERTIES] => Array
(
[AUTHOR] => Array
(
[ID] => 98
[TIMESTAMP_X] => 2021-05-05 12:29:14
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[NAME] => Автор
[ACTIVE] => Y
[SORT] => 500
[CODE] => AUTHOR
[DEFAULT_VALUE] => Автор
[PROPERTY_TYPE] => S
[ROW_COUNT] => 1
[COL_COUNT] => 50
[LIST_TYPE] => L
[MULTIPLE] => Y
[XML_ID] => 98
[FILE_TYPE] =>
[MULTIPLE_CNT] => 5
[TMP_ID] =>
[LINK_IBLOCK_ID] => 0
[WITH_DESCRIPTION] => N
[SEARCHABLE] => Y
[FILTRABLE] => Y
[IS_REQUIRED] => N
[VERSION] => 1
[USER_TYPE] =>
[USER_TYPE_SETTINGS] =>
[HINT] =>
[PROPERTY_VALUE_ID] => Array
(
[0] => 23920
)
[VALUE] => Array
(
[0] => А. И. Мошинский
)
[DESCRIPTION] => Array
(
[0] =>
)
[VALUE_ENUM] =>
[VALUE_XML_ID] =>
[VALUE_SORT] =>
[~VALUE] => Array
(
[0] => А. И. Мошинский
)
[~DESCRIPTION] => Array
(
[0] =>
)
[~NAME] => Автор
[~DEFAULT_VALUE] => Автор
[DISPLAY_VALUE] => А. И. Мошинский
)
[PAGE] => Array
(
[ID] => 100
[TIMESTAMP_X] => 2024-07-09 10:49:32
[IBLOCK_ID] => 23
[NAME] => Стр
[ACTIVE] => Y
[SORT] => 500
[CODE] => PAGE
[DEFAULT_VALUE] =>
[PROPERTY_TYPE] => N
[ROW_COUNT] => 1
[COL_COUNT] => 50
[LIST_TYPE] => L
[MULTIPLE] => N
[XML_ID] => 100
[FILE_TYPE] =>
[MULTIPLE_CNT] => 5
[TMP_ID] =>
[LINK_IBLOCK_ID] => 0
[WITH_DESCRIPTION] => N
[SEARCHABLE] => N
[FILTRABLE] => Y
[IS_REQUIRED] => N
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[USER_TYPE] =>
[USER_TYPE_SETTINGS] =>
[HINT] =>
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[VALUE] => 855-861
[DESCRIPTION] =>
[VALUE_ENUM] =>
[VALUE_XML_ID] =>
[VALUE_SORT] =>
[~VALUE] => 855-861
[~DESCRIPTION] =>
[~NAME] => Стр
[~DEFAULT_VALUE] =>
[DISPLAY_VALUE] => 855-861
)
)
)
Стр:
855-861
Решение задачи о распределении газовых молекул в слое с зеркальными граничными условиями
Исследуется распределение газовых молекул в слое, заполненном
разреженным газом. Для решения задачи применяется модельное
нестационарное уравнение Больцмана. Функция распределения найдена
в виде разложения по собственным обобщенным функциям
соответствующего характеристического уравнения.
Array
(
[DETAIL_TEXT] => Исследуется распределение газовых молекул в слое, заполненном
разреженным газом. Для решения задачи применяется модельное
нестационарное уравнение Больцмана. Функция распределения найдена
в виде разложения по собственным обобщенным функциям
соответствующего характеристического уравнения.
[~DETAIL_TEXT] => Исследуется распределение газовых молекул в слое, заполненном
разреженным газом. Для решения задачи применяется модельное
нестационарное уравнение Больцмана. Функция распределения найдена
в виде разложения по собственным обобщенным функциям
соответствующего характеристического уравнения.
[ID] => 6908
[~ID] => 6908
[IBLOCK_ID] => 23
[~IBLOCK_ID] => 23
[IBLOCK_SECTION_ID] => 350
[~IBLOCK_SECTION_ID] => 350
[NAME] => Решение задачи о распределении газовых молекул в слое с зеркальными граничными условиями
[~NAME] => Решение задачи о распределении газовых молекул в слое с зеркальными граничными условиями
[ACTIVE_FROM] =>
[~ACTIVE_FROM] =>
[TIMESTAMP_X] => 23.06.2021 14:33:32
[~TIMESTAMP_X] => 23.06.2021 14:33:32
[DETAIL_PAGE_URL] => /publications/jepter/bibl/?ELEMENT_ID=6908
[~DETAIL_PAGE_URL] => /publications/jepter/bibl/?ELEMENT_ID=6908
[LIST_PAGE_URL] => /publications/jepter/bibl/
[~LIST_PAGE_URL] => /publications/jepter/bibl/
[DETAIL_TEXT_TYPE] => html
[~DETAIL_TEXT_TYPE] => html
[PREVIEW_TEXT] =>
[~PREVIEW_TEXT] =>
[PREVIEW_TEXT_TYPE] => text
[~PREVIEW_TEXT_TYPE] => text
[PREVIEW_PICTURE] =>
[~PREVIEW_PICTURE] =>
[LANG_DIR] => /
[~LANG_DIR] => /
[PROPERTY_PAGE_VALUE] => 862-869
[~PROPERTY_PAGE_VALUE] => 862-869
[PROPERTY_PAGE_VALUE_ID] => 23923
[~PROPERTY_PAGE_VALUE_ID] => 23923
[SORT] => 500
[~SORT] => 500
[CODE] =>
[~CODE] =>
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[~EXTERNAL_ID] => 6908
[IBLOCK_TYPE_ID] => aspro_corporation_content
[~IBLOCK_TYPE_ID] => aspro_corporation_content
[IBLOCK_CODE] => IFZ
[~IBLOCK_CODE] => IFZ
[IBLOCK_EXTERNAL_ID] => 23
[~IBLOCK_EXTERNAL_ID] => 23
[LID] => s1
[~LID] => s1
[EDIT_LINK] =>
[DELETE_LINK] =>
[DISPLAY_ACTIVE_FROM] =>
[IPROPERTY_VALUES] => Array
(
)
[FIELDS] => Array
(
[DETAIL_TEXT] => Исследуется распределение газовых молекул в слое, заполненном
разреженным газом. Для решения задачи применяется модельное
нестационарное уравнение Больцмана. Функция распределения найдена
в виде разложения по собственным обобщенным функциям
соответствующего характеристического уравнения.
)
[PROPERTIES] => Array
(
[AUTHOR] => Array
(
[ID] => 98
[TIMESTAMP_X] => 2021-05-05 12:29:14
[IBLOCK_ID] => 23
[NAME] => Автор
[ACTIVE] => Y
[SORT] => 500
[CODE] => AUTHOR
[DEFAULT_VALUE] => Автор
[PROPERTY_TYPE] => S
[ROW_COUNT] => 1
[COL_COUNT] => 50
[LIST_TYPE] => L
[MULTIPLE] => Y
[XML_ID] => 98
[FILE_TYPE] =>
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[TMP_ID] =>
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[WITH_DESCRIPTION] => N
[SEARCHABLE] => Y
[FILTRABLE] => Y
[IS_REQUIRED] => N
[VERSION] => 1
[USER_TYPE] =>
[USER_TYPE_SETTINGS] =>
[HINT] =>
[PROPERTY_VALUE_ID] => Array
(
[0] => 23922
)
[VALUE] => Array
(
[0] => А. В. Латышев , Г. В. Слободской
)
[DESCRIPTION] => Array
(
[0] =>
)
[VALUE_ENUM] =>
[VALUE_XML_ID] =>
[VALUE_SORT] =>
[~VALUE] => Array
(
[0] => А. В. Латышев , Г. В. Слободской
)
[~DESCRIPTION] => Array
(
[0] =>
)
[~NAME] => Автор
[~DEFAULT_VALUE] => Автор
)
[KEYWORDS] => Array
(
[ID] => 99
[TIMESTAMP_X] => 2021-03-15 13:13:26
[IBLOCK_ID] => 23
[NAME] => Ключевые слова
[ACTIVE] => Y
[SORT] => 500
[CODE] => KEYWORDS
[DEFAULT_VALUE] =>
[PROPERTY_TYPE] => S
[ROW_COUNT] => 1
[COL_COUNT] => 50
[LIST_TYPE] => L
[MULTIPLE] => Y
[XML_ID] => 99
[FILE_TYPE] =>
[MULTIPLE_CNT] => 5
[TMP_ID] =>
[LINK_IBLOCK_ID] => 0
[WITH_DESCRIPTION] => N
[SEARCHABLE] => Y
[FILTRABLE] => Y
[IS_REQUIRED] => N
[VERSION] => 1
[USER_TYPE] =>
[USER_TYPE_SETTINGS] =>
[HINT] =>
[PROPERTY_VALUE_ID] =>
[VALUE] =>
[DESCRIPTION] =>
[VALUE_ENUM] =>
[VALUE_XML_ID] =>
[VALUE_SORT] =>
[~VALUE] =>
[~DESCRIPTION] =>
[~NAME] => Ключевые слова
[~DEFAULT_VALUE] =>
)
[PAGE] => Array
(
[ID] => 100
[TIMESTAMP_X] => 2024-07-09 10:49:32
[IBLOCK_ID] => 23
[NAME] => Стр
[ACTIVE] => Y
[SORT] => 500
[CODE] => PAGE
[DEFAULT_VALUE] =>
[PROPERTY_TYPE] => N
[ROW_COUNT] => 1
[COL_COUNT] => 50
[LIST_TYPE] => L
[MULTIPLE] => N
[XML_ID] => 100
[FILE_TYPE] =>
[MULTIPLE_CNT] => 5
[TMP_ID] =>
[LINK_IBLOCK_ID] => 0
[WITH_DESCRIPTION] => N
[SEARCHABLE] => N
[FILTRABLE] => Y
[IS_REQUIRED] => N
[VERSION] => 1
[USER_TYPE] =>
[USER_TYPE_SETTINGS] =>
[HINT] =>
[PROPERTY_VALUE_ID] => 23923
[VALUE] => 862-869
[DESCRIPTION] =>
[VALUE_ENUM] =>
[VALUE_XML_ID] =>
[VALUE_SORT] =>
[~VALUE] => 862-869
[~DESCRIPTION] =>
[~NAME] => Стр
[~DEFAULT_VALUE] =>
)
[NUMBER_JEPTER] => Array
(
[ID] => 107
[TIMESTAMP_X] => 2016-10-18 16:42:53
[IBLOCK_ID] => 23
[NAME] => Номера
[ACTIVE] => Y
[SORT] => 500
[CODE] => NUMBER_JEPTER
[DEFAULT_VALUE] =>
[PROPERTY_TYPE] => G
[ROW_COUNT] => 1
[COL_COUNT] => 30
[LIST_TYPE] => L
[MULTIPLE] => N
[XML_ID] => 107
[FILE_TYPE] =>
[MULTIPLE_CNT] => 5
[TMP_ID] =>
[LINK_IBLOCK_ID] => 0
[WITH_DESCRIPTION] => N
[SEARCHABLE] => N
[FILTRABLE] => Y
[IS_REQUIRED] => N
[VERSION] => 1
[USER_TYPE] =>
[USER_TYPE_SETTINGS] =>
[HINT] =>
[PROPERTY_VALUE_ID] =>
[VALUE] =>
[DESCRIPTION] =>
[VALUE_ENUM] =>
[VALUE_XML_ID] =>
[VALUE_SORT] =>
[~VALUE] =>
[~DESCRIPTION] =>
[~NAME] => Номера
[~DEFAULT_VALUE] =>
)
[IFZ_FILE] => Array
(
[ID] => 304
[TIMESTAMP_X] => 2016-10-13 13:20:50
[IBLOCK_ID] => 23
[NAME] => Файл
[ACTIVE] => Y
[SORT] => 500
[CODE] => IFZ_FILE
[DEFAULT_VALUE] =>
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Автор:
А. В. Латышев , Г. В. Слободской
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соответствующего характеристического уравнения.
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нестационарное уравнение Больцмана. Функция распределения найдена
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композитного материала, представляющего собой трехслойную
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слоя магнитореологической жидкости (МРЖ) между ними, способную
менять свои упругие свойства под воздействием внешнего
магнитного поля в реальном масштабе времени. Измеренные
характеристики: динамический модуль накопления G2 демпфирующего
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так и всей балки в целом находятся в диапазоне значений,
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В. И. Кордонский , С. А. Демчук , В. А. Кузьмин
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[DETAIL_TEXT] => Используется оригинальная методика измерения упругих свойств
композитного материала, представляющего собой трехслойную
вибрирующую балку, состоящую из двух металлических пластин и
слоя магнитореологической жидкости (МРЖ) между ними, способную
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так и всей балки в целом находятся в диапазоне значений,
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870-873
Динамические характеристики гидравлических тормозных устройств с магнитореологическим принципом управления
Рассматривается магнитореологический принцип управления работой
электрогидравлического тормозного устройства. Уровень диссипативных
потерь в канале управляющего элемента, определяющий силу торможения
в подобных системах, регулируется магнитным полем, настраивающим
магниточувствительную гидравлическую жидкость на заданную величину
эффективной вязкости. В эксперименте осуществлен контроль основных
параметров, характеризующих силовые и частотные характеристики
устройства. Обнаружено, что характерное время формирования силы
торможения составляет 10-3 с, а быстродействие системы лимитируется
главным образом частотными характеристиками индуктора магнитного
поля магнитореологического дросселя.
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потерь в канале управляющего элемента, определяющий силу торможения
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потерь в канале управляющего элемента, определяющий силу торможения
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потерь в канале управляющего элемента, определяющий силу торможения
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[NAME] => Организация
[ACTIVE] => Y
[SORT] => 500
[CODE] => COMPANY
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[XML_ID] =>
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[SORT] => 500
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[VALUE_XML_ID] =>
[VALUE_SORT] =>
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[~VALUE] =>
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[~NAME] => УДК
[~DEFAULT_VALUE] =>
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(
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)
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(
[0] =>
)
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(
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[NAME] => Стр
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Стр:
874-880
Численное моделирование заполнения осесимметричного канала нелинейно-вязкопластичной жидкостью с учетом П-эффекта
(Re 
1) течения нелинейно-вязкопластичной жидкости
с реологией Шульмана, реализующегося при заполнении вертикально
расположенных объемов в поле силы тяжести. Учитывается эффект
скольжения жидкости у твердой стенки (П-эффект). Проведены
численные исследования процесса заполнения осесимметричной области.
Показано влияние П-эффекта на характер гидродинамического процесса
заполнения
Array
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с реологией Шульмана, реализующегося при заполнении вертикально
расположенных объемов в поле силы тяжести. Учитывается эффект
скольжения жидкости у твердой стенки (П-эффект). Проведены
численные исследования процесса заполнения осесимметричной области.
Показано влияние П-эффекта на характер гидродинамического процесса
заполнения
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с реологией Шульмана, реализующегося при заполнении вертикально
расположенных объемов в поле силы тяжести. Учитывается эффект
скольжения жидкости у твердой стенки (П-эффект). Проведены
численные исследования процесса заполнения осесимметричной области.
Показано влияние П-эффекта на характер гидродинамического процесса
заполнения
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[~NAME] => Численное моделирование заполнения осесимметричного канала нелинейно-вязкопластичной жидкостью с учетом П-эффекта
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[~LIST_PAGE_URL] => /publications/jepter/bibl/
[DETAIL_TEXT_TYPE] => html
[~DETAIL_TEXT_TYPE] => html
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[~PREVIEW_TEXT] =>
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[~IBLOCK_TYPE_ID] => aspro_corporation_content
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[~IBLOCK_EXTERNAL_ID] => 23
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[~LID] => s1
[EDIT_LINK] =>
[DELETE_LINK] =>
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[IPROPERTY_VALUES] => Array
(
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с реологией Шульмана, реализующегося при заполнении вертикально
расположенных объемов в поле силы тяжести. Учитывается эффект
скольжения жидкости у твердой стенки (П-эффект). Проведены
численные исследования процесса заполнения осесимметричной области.
Показано влияние П-эффекта на характер гидродинамического процесса
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(
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[VALUE] =>
[DESCRIPTION] =>
[VALUE_ENUM] =>
[VALUE_XML_ID] =>
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[~VALUE] =>
[~DESCRIPTION] =>
[~NAME] => Ключевые слова
[~DEFAULT_VALUE] =>
)
[PAGE] => Array
(
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[TIMESTAMP_X] => 2024-07-09 10:49:32
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[NAME] => Стр
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[TIMESTAMP_X] => 2016-10-18 16:42:53
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[NAME] => Номера
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[CODE] => NUMBER_JEPTER
[DEFAULT_VALUE] =>
[PROPERTY_TYPE] => G
[ROW_COUNT] => 1
[COL_COUNT] => 30
[LIST_TYPE] => L
[MULTIPLE] => N
[XML_ID] => 107
[FILE_TYPE] =>
[MULTIPLE_CNT] => 5
[TMP_ID] =>
[LINK_IBLOCK_ID] => 0
[WITH_DESCRIPTION] => N
[SEARCHABLE] => N
[FILTRABLE] => Y
[IS_REQUIRED] => N
[VERSION] => 1
[USER_TYPE] =>
[USER_TYPE_SETTINGS] =>
[HINT] =>
[PROPERTY_VALUE_ID] =>
[VALUE] =>
[DESCRIPTION] =>
[VALUE_ENUM] =>
[VALUE_XML_ID] =>
[VALUE_SORT] =>
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[~NAME] => Номера
[~DEFAULT_VALUE] =>
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[TIMESTAMP_X] => 2016-10-13 13:20:50
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[NAME] => Файл
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[SORT] => 500
[CODE] => IFZ_FILE
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[PROPERTY_TYPE] => F
[ROW_COUNT] => 1
[COL_COUNT] => 30
[LIST_TYPE] => L
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[XML_ID] => 304
[FILE_TYPE] =>
[MULTIPLE_CNT] => 5
[TMP_ID] =>
[LINK_IBLOCK_ID] => 0
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[FILTRABLE] => N
[IS_REQUIRED] => N
[VERSION] => 1
[USER_TYPE] =>
[USER_TYPE_SETTINGS] =>
[HINT] =>
[PROPERTY_VALUE_ID] =>
[VALUE] =>
[DESCRIPTION] =>
[VALUE_ENUM] =>
[VALUE_XML_ID] =>
[VALUE_SORT] =>
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[~DESCRIPTION] =>
[~NAME] => Файл
[~DEFAULT_VALUE] =>
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(
[ID] => 366
[TIMESTAMP_X] => 2021-05-06 15:18:10
[IBLOCK_ID] => 23
[NAME] => Год
[ACTIVE] => Y
[SORT] => 500
[CODE] => IFZ_YEAR
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[PROPERTY_TYPE] => L
[ROW_COUNT] => 1
[COL_COUNT] => 30
[LIST_TYPE] => L
[MULTIPLE] => N
[XML_ID] =>
[FILE_TYPE] =>
[MULTIPLE_CNT] => 5
[TMP_ID] =>
[LINK_IBLOCK_ID] => 0
[WITH_DESCRIPTION] => N
[SEARCHABLE] => Y
[FILTRABLE] => Y
[IS_REQUIRED] => N
[VERSION] => 1
[USER_TYPE] =>
[USER_TYPE_SETTINGS] =>
[HINT] =>
[PROPERTY_VALUE_ID] =>
[VALUE] =>
[DESCRIPTION] =>
[VALUE_ENUM] =>
[VALUE_XML_ID] =>
[VALUE_SORT] =>
[VALUE_ENUM_ID] =>
[~VALUE] =>
[~DESCRIPTION] =>
[~NAME] => Год
[~DEFAULT_VALUE] =>
)
[YEAR] => Array
(
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[TIMESTAMP_X] => 2021-05-04 12:31:09
[IBLOCK_ID] => 23
[NAME] => Год
[ACTIVE] => Y
[SORT] => 500
[CODE] => YEAR
[DEFAULT_VALUE] =>
[PROPERTY_TYPE] => S
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[COL_COUNT] => 30
[LIST_TYPE] => L
[MULTIPLE] => N
[XML_ID] =>
[FILE_TYPE] =>
[MULTIPLE_CNT] => 5
[TMP_ID] =>
[LINK_IBLOCK_ID] => 0
[WITH_DESCRIPTION] => Y
[SEARCHABLE] => Y
[FILTRABLE] => Y
[IS_REQUIRED] => N
[VERSION] => 1
[USER_TYPE] =>
[USER_TYPE_SETTINGS] =>
[HINT] =>
[PROPERTY_VALUE_ID] =>
[VALUE] =>
[DESCRIPTION] =>
[VALUE_ENUM] =>
[VALUE_XML_ID] =>
[VALUE_SORT] =>
[~VALUE] =>
[~DESCRIPTION] =>
[~NAME] => Год
[~DEFAULT_VALUE] =>
)
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(
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[SORT] => 500
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[VERSION] => 1
[USER_TYPE] =>
[USER_TYPE_SETTINGS] =>
[HINT] =>
[PROPERTY_VALUE_ID] =>
[VALUE] =>
[DESCRIPTION] =>
[VALUE_ENUM] =>
[VALUE_XML_ID] =>
[VALUE_SORT] =>
[~VALUE] =>
[~DESCRIPTION] =>
[~NAME] => Автор2
[~DEFAULT_VALUE] =>
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[COMPANY] => Array
(
[ID] => 392
[TIMESTAMP_X] => 2024-07-09 10:49:32
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[NAME] => Организация
[ACTIVE] => Y
[SORT] => 500
[CODE] => COMPANY
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[LIST_TYPE] => L
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[XML_ID] =>
[FILE_TYPE] =>
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[LINK_IBLOCK_ID] => 0
[WITH_DESCRIPTION] => N
[SEARCHABLE] => N
[FILTRABLE] => N
[IS_REQUIRED] => N
[VERSION] => 1
[USER_TYPE] =>
[USER_TYPE_SETTINGS] =>
[HINT] =>
[PROPERTY_VALUE_ID] =>
[VALUE] =>
[DESCRIPTION] =>
[VALUE_ENUM] =>
[VALUE_XML_ID] =>
[VALUE_SORT] =>
[VALUE_ENUM_ID] =>
[~VALUE] =>
[~DESCRIPTION] =>
[~NAME] => Организация
[~DEFAULT_VALUE] =>
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(
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[FILE_TYPE] =>
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[TMP_ID] =>
[LINK_IBLOCK_ID] => 0
[WITH_DESCRIPTION] => N
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[FILTRABLE] => N
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[VERSION] => 1
[USER_TYPE] =>
[USER_TYPE_SETTINGS] =>
[HINT] =>
[PROPERTY_VALUE_ID] =>
[VALUE] =>
[DESCRIPTION] =>
[VALUE_ENUM] =>
[VALUE_XML_ID] =>
[VALUE_SORT] =>
[VALUE_ENUM_ID] =>
[~VALUE] =>
[~DESCRIPTION] =>
[~NAME] => УДК
[~DEFAULT_VALUE] =>
)
)
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(
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(
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[TIMESTAMP_X] => 2021-05-05 12:29:14
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К. А. Чехонин , П. А. Сухинин
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Моделирование уравнения для скорости диссипации напряжений Рейнольдса
Выполнено моделирование всех корреляций, входящих в уравнение
для скорости диссипации кинетической энергии турбулентности.
В качестве модельных соотношений использованы аппроксимации,
выведенные ранее. Моделирование выполнено путем прямого сравнения
аппроксимаций с величинами корреляций, полученными в результате
численного решения нестационарных уравнений Навье-Стокса.
Определен вид аппроксимаций и эмпирические коэффициенты. Получены
аппроксимации для корреляций, входящих в уравнение для тензорной
диссипативной функции. Предложено новое уравнение для скорости
диссипации энергии турбулентности. Результаты работы могут
быть использованы для определения напряжений Рейнольдса в моделях
турбулентности второго порядка.
Array
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В качестве модельных соотношений использованы аппроксимации,
выведенные ранее. Моделирование выполнено путем прямого сравнения
аппроксимаций с величинами корреляций, полученными в результате
численного решения нестационарных уравнений Навье-Стокса.
Определен вид аппроксимаций и эмпирические коэффициенты. Получены
аппроксимации для корреляций, входящих в уравнение для тензорной
диссипативной функции. Предложено новое уравнение для скорости
диссипации энергии турбулентности. Результаты работы могут
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В качестве модельных соотношений использованы аппроксимации,
выведенные ранее. Моделирование выполнено путем прямого сравнения
аппроксимаций с величинами корреляций, полученными в результате
численного решения нестационарных уравнений Навье-Стокса.
Определен вид аппроксимаций и эмпирические коэффициенты. Получены
аппроксимации для корреляций, входящих в уравнение для тензорной
диссипативной функции. Предложено новое уравнение для скорости
диссипации энергии турбулентности. Результаты работы могут
быть использованы для определения напряжений Рейнольдса в моделях
турбулентности второго порядка.
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В качестве модельных соотношений использованы аппроксимации,
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численного решения нестационарных уравнений Навье-Стокса.
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аппроксимации для корреляций, входящих в уравнение для тензорной
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Автор:
Е. П. Сухович
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В качестве модельных соотношений использованы аппроксимации,
выведенные ранее. Моделирование выполнено путем прямого сравнения
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численного решения нестационарных уравнений Навье-Стокса.
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аппроксимации для корреляций, входящих в уравнение для тензорной
диссипативной функции. Предложено новое уравнение для скорости
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турбулентности второго порядка.
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В качестве модельных соотношений использованы аппроксимации,
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аппроксимаций с величинами корреляций, полученными в результате
численного решения нестационарных уравнений Навье-Стокса.
Определен вид аппроксимаций и эмпирические коэффициенты. Получены
аппроксимации для корреляций, входящих в уравнение для тензорной
диссипативной функции. Предложено новое уравнение для скорости
диссипации энергии турбулентности. Результаты работы могут
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для скорости диссипации кинетической энергии турбулентности.
В качестве модельных соотношений использованы аппроксимации,
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аппроксимаций с величинами корреляций, полученными в результате
численного решения нестационарных уравнений Навье-Стокса.
Определен вид аппроксимаций и эмпирические коэффициенты. Получены
аппроксимации для корреляций, входящих в уравнение для тензорной
диссипативной функции. Предложено новое уравнение для скорости
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Динамические характеристики пульсирующего турбулентного потока сжимаемого газа в канале
Модель турбулентного переноса, учитывающая влияние пульсаций
расхода на турбулентное напряжение, использована для исследования
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Предложен алгоритм численного решения системы уравнений, описывающей
этот процесс, методом конечных разностей с применением неявной итерационной
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Автор:
Е. П. Валуева
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Предложен алгоритм численного решения системы уравнений, описывающей
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Предложен алгоритм численного решения системы уравнений, описывающей
этот процесс, методом конечных разностей с применением неявной итерационной
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[FILE_TYPE] =>
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[TMP_ID] =>
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Стр:
896-901
Аэродинамическое возбуждение однотипных узкополосных пульсаций в различных технических устройствах
В экспериментах на моделях воспроизведен характер пульсационных
процессов в потоке, возникающих в пусковых участках газокомпрессорных
станций при открытом обратном клапане. На основании анализа и сопоставлений
полагается, что в проточной части клапана формируются крупномасштабные
вихревые структуры, генерируются связанные узкополосные гидродинамические
и акустические колебания, подобные наблюдаемым в аэродинамических
трубах замкнутого типа с открытой рабочей частью и при обтекании крылового
профиля. Общность механизма возбуждения интенсивных возмущений в потоке
газа с различными неоднородностями обосновывается близостью соотношений
характеризующих его безразмерных параметров к единой зависимости.
Array
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газа с различными неоднородностями обосновывается близостью соотношений
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вихревые структуры, генерируются связанные узкополосные гидродинамические
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Автор:
В. А. Вишняков , В. Г. Засецкий , Р. К. Каравосов , А. Г. Прозоров , Л. И. Соколинский
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профиля. Общность механизма возбуждения интенсивных возмущений в потоке
газа с различными неоднородностями обосновывается близостью соотношений
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902-906
Приближенный метод расчета турбулентного двухфазного течения в канале с проницаемыми стенками
На основе модели двухскоростной и двухтемпературной среды
построена система уравнений, описывающая плоское или осесимметричное
турбулентное течение газовзвеси в канале с проницаемыми стенками.
Система уравнений движения и теплопереноса сводится к системе обыкновенных
дифференциальных уравнений, интегрирование которой сопряжено со значительно
меньшими вычислительными трудностями по сравнению с решением исходной
системы. Получены распределения скорости и локальных характеристик
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Автор:
К. Н. Волков , В. Н. Емельянов
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Анализируется актуальность применения твердых сорбентов
для хранения природного газа на транспорте. Приводятся экспериментальные
данные по сорбции метана активированным угольным волокном в диапазоне
температур -40 - +40oС и давлений до 4 МПа. Используемый
баллон обеспечивает за счет применения сорбента понижение уровня рабочего
давления и увеличение объемной плотности хранения по сравнению с системами
сжатого природного газа.
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данные по сорбции метана активированным угольным волокном в диапазоне
температур -40 - +40oС и давлений до 4 МПа. Используемый
баллон обеспечивает за счет применения сорбента понижение уровня рабочего
давления и увеличение объемной плотности хранения по сравнению с системами
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температур -40 - +40oС и давлений до 4 МПа. Используемый
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Автор:
Л. Л. Васильев , Л. Е. Канончик , Д. А. Мишкинис
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для хранения природного газа на транспорте. Приводятся экспериментальные
данные по сорбции метана активированным угольным волокном в диапазоне
температур -40 - +40oС и давлений до 4 МПа. Используемый
баллон обеспечивает за счет применения сорбента понижение уровня рабочего
давления и увеличение объемной плотности хранения по сравнению с системами
сжатого природного газа.
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температур -40 - +40oС и давлений до 4 МПа. Используемый
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данные по сорбции метана активированным угольным волокном в диапазоне
температур -40 - +40oС и давлений до 4 МПа. Используемый
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Стр:
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Гелеобразование при ультрафильтрации в плоском канале с одной проницаемой поверхностью
Исследован нестационарный ламинарный процесс ультрафильтрации
в плоском канале с одной проницаемой поверхностью в стадии неподвижного
гелеобразования.
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Автор:
В. И. Байков , П. К. Зновец
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[USER_TYPE] =>
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[~DEFAULT_VALUE] =>
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[DEFAULT_VALUE] =>
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[COL_COUNT] => 30
[LIST_TYPE] => L
[MULTIPLE] => N
[XML_ID] =>
[FILE_TYPE] =>
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[TMP_ID] =>
[LINK_IBLOCK_ID] => 0
[WITH_DESCRIPTION] => N
[SEARCHABLE] => Y
[FILTRABLE] => Y
[IS_REQUIRED] => N
[VERSION] => 1
[USER_TYPE] =>
[USER_TYPE_SETTINGS] =>
[HINT] =>
[PROPERTY_VALUE_ID] =>
[VALUE] =>
[DESCRIPTION] =>
[VALUE_ENUM] =>
[VALUE_XML_ID] =>
[VALUE_SORT] =>
[VALUE_ENUM_ID] =>
[~VALUE] =>
[~DESCRIPTION] =>
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[~DEFAULT_VALUE] =>
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[YEAR] => Array
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[XML_ID] =>
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[VERSION] => 1
[USER_TYPE] =>
[USER_TYPE_SETTINGS] =>
[HINT] =>
[PROPERTY_VALUE_ID] =>
[VALUE] =>
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[VERSION] => 1
[USER_TYPE] =>
[USER_TYPE_SETTINGS] =>
[HINT] =>
[PROPERTY_VALUE_ID] =>
[VALUE] =>
[DESCRIPTION] =>
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[~VALUE] =>
[~DESCRIPTION] =>
[~NAME] => Автор2
[~DEFAULT_VALUE] =>
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[COMPANY] => Array
(
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[CODE] => COMPANY
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[XML_ID] =>
[FILE_TYPE] =>
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[TMP_ID] =>
[LINK_IBLOCK_ID] => 0
[WITH_DESCRIPTION] => N
[SEARCHABLE] => N
[FILTRABLE] => N
[IS_REQUIRED] => N
[VERSION] => 1
[USER_TYPE] =>
[USER_TYPE_SETTINGS] =>
[HINT] =>
[PROPERTY_VALUE_ID] =>
[VALUE] =>
[DESCRIPTION] =>
[VALUE_ENUM] =>
[VALUE_XML_ID] =>
[VALUE_SORT] =>
[VALUE_ENUM_ID] =>
[~VALUE] =>
[~DESCRIPTION] =>
[~NAME] => Организация
[~DEFAULT_VALUE] =>
)
[UDK] => Array
(
[ID] => 393
[TIMESTAMP_X] => 2024-07-09 10:49:32
[IBLOCK_ID] => 23
[NAME] => УДК
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[SORT] => 500
[CODE] => UDK
[DEFAULT_VALUE] =>
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[LIST_TYPE] => L
[MULTIPLE] => Y
[XML_ID] =>
[FILE_TYPE] =>
[MULTIPLE_CNT] => 5
[TMP_ID] =>
[LINK_IBLOCK_ID] => 0
[WITH_DESCRIPTION] => N
[SEARCHABLE] => N
[FILTRABLE] => N
[IS_REQUIRED] => N
[VERSION] => 1
[USER_TYPE] =>
[USER_TYPE_SETTINGS] =>
[HINT] =>
[PROPERTY_VALUE_ID] =>
[VALUE] =>
[DESCRIPTION] =>
[VALUE_ENUM] =>
[VALUE_XML_ID] =>
[VALUE_SORT] =>
[VALUE_ENUM_ID] =>
[~VALUE] =>
[~DESCRIPTION] =>
[~NAME] => УДК
[~DEFAULT_VALUE] =>
)
)
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Исследовано влияние радиального изменения температуры стенки
на теплообмен при центробежном турбулентном течении в зазоре
между параллельными вращающимися дисками. Рассмотрены случаи
положительного, приблизительно постоянного и отрицательного
радиального градиентов температуры диска. Результаты расчетов
с помощью интегрального метода хорошо согласуются с известными
экспериментами. Показано, что изменение температуры стенки
оказывает незначительное влияние в области источника и решающее
- в слоях экмановского типа, приводя в итоге к возникновению
зоны с обратным направлением теплового потока на периферии
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выходящего из плоского слоя селективной среды. Анализируются ошибки
расчета интенсивности излучения, возникающие при игнорировании этого
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931- 936
Radiative Transfer in nongray Gas Using a Narrow-Band Model and Monte Carlo Simulation
Radiation transfer is treated by the application of
a narrow-band statistical model (NBSM) that takes emission
and absorption gas spectral structures into account. A Monte
Carlo method (MCM) using a net exchange technique was developed
to integrate the radiative-transfer equation in nongray gas.
The proposed procedure is based on a net-exchange formulation
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fulfilling the reciprocity principle, which avoids some of the major
problems usually associated with the Monte Carlo Method;
the numerical efficiency becomes independent of the optical thickness,
highly nonuniform grid sizes can be used with no increase
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differences can be treated with very good accuracy. It is shown that
the radiative term is significant compared to the conductive term
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Теплофизические эффекты при фотодинамической терапии опухолей
Предложена математическая модель температурных режимов
при фотодинамической терапии опухолей мозга. Определены технологические
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клеток наряду с фотопроцессами дополнительно может сопровождаться
достижением гипертермических и термотерапевтических температур. Такие
реализованные возможности позволяют добиться большего объема разрушения
опухоли, особенно малоперфузионной, при сохранении близлежащих здоровых
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Автор:
В. Н. Бидненко , В. Л. Сигал
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Методами физического моделирования с помощью линейной
гребневой регрессии установлено, что в плазмотронах постоянного тока
со ступенчатыми электродами вольт-амперная характеристика дуги формируется
под воздействием теплообменных процессов, а газодинамические факторы
оказывают слабое влияние. Уточнены обобщенные ВАХ плазмотронов одностороннего
и двустороннего истечения при обдуве дуги воздухом и водородом.
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Автор:
А. Ф. Бублиевский , О. И. Ясько , Е. И. Юринок
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Увеличение температуры до 400 К стимулирует процесс скольжения в реализации
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Анализ высокоэффективных методов обработки при проектировании технологических комплексов .
На основании анализа самоорганизации поверхностных явлений
предложены критерии для управления устойчивостью процессов
высокоэффективной обработки. Рекомендовано создавать
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гибких производственных модулей.
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высокоэффективной обработки. Рекомендовано создавать
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высокоэффективной обработки. Рекомендовано создавать
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Автор:
Л. М. Акулович , Л. М. Кожуро , М. Л. Хейфец , Е. З. Зевелева
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[USER_TYPE] =>
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[HINT] =>
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[VALUE] =>
[DESCRIPTION] =>
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Стр:
980-982
Твердость покрытий из различных присадочных материалов при электродуговой металлизации
Экспериментально исследовано влияние материала электродов
на твердость покрытий при электродуговой металлизации.
Array
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на твердость покрытий при электродуговой металлизации.
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на твердость покрытий при электродуговой металлизации.
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[VERSION] => 1
[USER_TYPE] =>
[USER_TYPE_SETTINGS] =>
[HINT] =>
[PROPERTY_VALUE_ID] =>
[VALUE] =>
[DESCRIPTION] =>
[VALUE_ENUM] =>
[VALUE_XML_ID] =>
[VALUE_SORT] =>
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[~NAME] => Номера
[~DEFAULT_VALUE] =>
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[FILE_TYPE] =>
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[LINK_IBLOCK_ID] => 0
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[SEARCHABLE] => N
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[IS_REQUIRED] => N
[VERSION] => 1
[USER_TYPE] =>
[USER_TYPE_SETTINGS] =>
[HINT] =>
[PROPERTY_VALUE_ID] =>
[VALUE] =>
[DESCRIPTION] =>
[VALUE_ENUM] =>
[VALUE_XML_ID] =>
[VALUE_SORT] =>
[~VALUE] =>
[~DESCRIPTION] =>
[~NAME] => Файл
[~DEFAULT_VALUE] =>
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(
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[NAME] => Год
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[SORT] => 500
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[DEFAULT_VALUE] =>
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[ROW_COUNT] => 1
[COL_COUNT] => 30
[LIST_TYPE] => L
[MULTIPLE] => N
[XML_ID] =>
[FILE_TYPE] =>
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[TMP_ID] =>
[LINK_IBLOCK_ID] => 0
[WITH_DESCRIPTION] => N
[SEARCHABLE] => Y
[FILTRABLE] => Y
[IS_REQUIRED] => N
[VERSION] => 1
[USER_TYPE] =>
[USER_TYPE_SETTINGS] =>
[HINT] =>
[PROPERTY_VALUE_ID] =>
[VALUE] =>
[DESCRIPTION] =>
[VALUE_ENUM] =>
[VALUE_XML_ID] =>
[VALUE_SORT] =>
[VALUE_ENUM_ID] =>
[~VALUE] =>
[~DESCRIPTION] =>
[~NAME] => Год
[~DEFAULT_VALUE] =>
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[YEAR] => Array
(
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[TIMESTAMP_X] => 2021-05-04 12:31:09
[IBLOCK_ID] => 23
[NAME] => Год
[ACTIVE] => Y
[SORT] => 500
[CODE] => YEAR
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[PROPERTY_TYPE] => S
[ROW_COUNT] => 1
[COL_COUNT] => 30
[LIST_TYPE] => L
[MULTIPLE] => N
[XML_ID] =>
[FILE_TYPE] =>
[MULTIPLE_CNT] => 5
[TMP_ID] =>
[LINK_IBLOCK_ID] => 0
[WITH_DESCRIPTION] => Y
[SEARCHABLE] => Y
[FILTRABLE] => Y
[IS_REQUIRED] => N
[VERSION] => 1
[USER_TYPE] =>
[USER_TYPE_SETTINGS] =>
[HINT] =>
[PROPERTY_VALUE_ID] =>
[VALUE] =>
[DESCRIPTION] =>
[VALUE_ENUM] =>
[VALUE_XML_ID] =>
[VALUE_SORT] =>
[~VALUE] =>
[~DESCRIPTION] =>
[~NAME] => Год
[~DEFAULT_VALUE] =>
)
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(
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[IBLOCK_ID] => 23
[NAME] => Автор2
[ACTIVE] => Y
[SORT] => 500
[CODE] => AUTHOR2
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[PROPERTY_TYPE] => S
[ROW_COUNT] => 1
[COL_COUNT] => 30
[LIST_TYPE] => L
[MULTIPLE] => N
[XML_ID] =>
[FILE_TYPE] =>
[MULTIPLE_CNT] => 5
[TMP_ID] =>
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[VERSION] => 1
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[~DESCRIPTION] =>
[~NAME] => Автор2
[~DEFAULT_VALUE] =>
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[COMPANY] => Array
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[NAME] => Организация
[ACTIVE] => Y
[SORT] => 500
[CODE] => COMPANY
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[VERSION] => 1
[USER_TYPE] =>
[USER_TYPE_SETTINGS] =>
[HINT] =>
[PROPERTY_VALUE_ID] =>
[VALUE] =>
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[VALUE_SORT] =>
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[~VALUE] =>
[~DESCRIPTION] =>
[~NAME] => Организация
[~DEFAULT_VALUE] =>
)
[UDK] => Array
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[TIMESTAMP_X] => 2024-07-09 10:49:32
[IBLOCK_ID] => 23
[NAME] => УДК
[ACTIVE] => Y
[SORT] => 500
[CODE] => UDK
[DEFAULT_VALUE] =>
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[COL_COUNT] => 30
[LIST_TYPE] => L
[MULTIPLE] => Y
[XML_ID] =>
[FILE_TYPE] =>
[MULTIPLE_CNT] => 5
[TMP_ID] =>
[LINK_IBLOCK_ID] => 0
[WITH_DESCRIPTION] => N
[SEARCHABLE] => N
[FILTRABLE] => N
[IS_REQUIRED] => N
[VERSION] => 1
[USER_TYPE] =>
[USER_TYPE_SETTINGS] =>
[HINT] =>
[PROPERTY_VALUE_ID] =>
[VALUE] =>
[DESCRIPTION] =>
[VALUE_ENUM] =>
[VALUE_XML_ID] =>
[VALUE_SORT] =>
[VALUE_ENUM_ID] =>
[~VALUE] =>
[~DESCRIPTION] =>
[~NAME] => УДК
[~DEFAULT_VALUE] =>
)
)
[DISPLAY_PROPERTIES] => Array
(
[AUTHOR] => Array
(
[ID] => 98
[TIMESTAMP_X] => 2021-05-05 12:29:14
[IBLOCK_ID] => 23
[NAME] => Автор
[ACTIVE] => Y
[SORT] => 500
[CODE] => AUTHOR
[DEFAULT_VALUE] => Автор
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(
[0] => 23960
)
[VALUE] => Array
(
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)
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(
[0] =>
)
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[~VALUE] => Array
(
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)
[~DESCRIPTION] => Array
(
[0] =>
)
[~NAME] => Автор
[~DEFAULT_VALUE] => Автор
[DISPLAY_VALUE] => М. С. Третьяк , В. В. Чупрасов
)
[PAGE] => Array
(
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[USER_TYPE] =>
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[HINT] =>
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[VALUE] => 983-987
[DESCRIPTION] =>
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[VALUE_XML_ID] =>
[VALUE_SORT] =>
[~VALUE] => 983-987
[~DESCRIPTION] =>
[~NAME] => Стр
[~DEFAULT_VALUE] =>
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)
)
)
Автор:
М. С. Третьяк , В. В. Чупрасов
Array
(
[DETAIL_TEXT] => Экспериментально исследовано влияние материала электродов
на твердость покрытий при электродуговой металлизации.
[~DETAIL_TEXT] => Экспериментально исследовано влияние материала электродов
на твердость покрытий при электродуговой металлизации.
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[NAME] => Твердость покрытий из различных присадочных материалов при электродуговой металлизации
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[TIMESTAMP_X] => 24.06.2021 11:22:25
[~TIMESTAMP_X] => 24.06.2021 11:22:25
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[~DETAIL_PAGE_URL] => /publications/jepter/bibl/?ELEMENT_ID=6927
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[~LIST_PAGE_URL] => /publications/jepter/bibl/
[DETAIL_TEXT_TYPE] => html
[~DETAIL_TEXT_TYPE] => html
[PREVIEW_TEXT] =>
[~PREVIEW_TEXT] =>
[PREVIEW_TEXT_TYPE] => text
[~PREVIEW_TEXT_TYPE] => text
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[CODE] =>
[~CODE] =>
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[~EXTERNAL_ID] => 6927
[IBLOCK_TYPE_ID] => aspro_corporation_content
[~IBLOCK_TYPE_ID] => aspro_corporation_content
[IBLOCK_CODE] => IFZ
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[~IBLOCK_EXTERNAL_ID] => 23
[LID] => s1
[~LID] => s1
[EDIT_LINK] =>
[DELETE_LINK] =>
[DISPLAY_ACTIVE_FROM] =>
[IPROPERTY_VALUES] => Array
(
)
[FIELDS] => Array
(
[DETAIL_TEXT] => Экспериментально исследовано влияние материала электродов
на твердость покрытий при электродуговой металлизации.
)
[PROPERTIES] => Array
(
[AUTHOR] => Array
(
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[TIMESTAMP_X] => 2021-05-05 12:29:14
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[NAME] => Автор
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[SORT] => 500
[CODE] => AUTHOR
[DEFAULT_VALUE] => Автор
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[TMP_ID] =>
[LINK_IBLOCK_ID] => 0
[WITH_DESCRIPTION] => N
[SEARCHABLE] => Y
[FILTRABLE] => Y
[IS_REQUIRED] => N
[VERSION] => 1
[USER_TYPE] =>
[USER_TYPE_SETTINGS] =>
[HINT] =>
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(
[0] => 23960
)
[VALUE] => Array
(
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)
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)
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(
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)
[~DESCRIPTION] => Array
(
[0] =>
)
[~NAME] => Автор
[~DEFAULT_VALUE] => Автор
)
[KEYWORDS] => Array
(
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[TIMESTAMP_X] => 2021-03-15 13:13:26
[IBLOCK_ID] => 23
[NAME] => Ключевые слова
[ACTIVE] => Y
[SORT] => 500
[CODE] => KEYWORDS
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[USER_TYPE] =>
[USER_TYPE_SETTINGS] =>
[HINT] =>
[PROPERTY_VALUE_ID] =>
[VALUE] =>
[DESCRIPTION] =>
[VALUE_ENUM] =>
[VALUE_XML_ID] =>
[VALUE_SORT] =>
[~VALUE] =>
[~DESCRIPTION] =>
[~NAME] => Ключевые слова
[~DEFAULT_VALUE] =>
)
[PAGE] => Array
(
[ID] => 100
[TIMESTAMP_X] => 2024-07-09 10:49:32
[IBLOCK_ID] => 23
[NAME] => Стр
[ACTIVE] => Y
[SORT] => 500
[CODE] => PAGE
[DEFAULT_VALUE] =>
[PROPERTY_TYPE] => N
[ROW_COUNT] => 1
[COL_COUNT] => 50
[LIST_TYPE] => L
[MULTIPLE] => N
[XML_ID] => 100
[FILE_TYPE] =>
[MULTIPLE_CNT] => 5
[TMP_ID] =>
[LINK_IBLOCK_ID] => 0
[WITH_DESCRIPTION] => N
[SEARCHABLE] => N
[FILTRABLE] => Y
[IS_REQUIRED] => N
[VERSION] => 1
[USER_TYPE] =>
[USER_TYPE_SETTINGS] =>
[HINT] =>
[PROPERTY_VALUE_ID] => 23961
[VALUE] => 983-987
[DESCRIPTION] =>
[VALUE_ENUM] =>
[VALUE_XML_ID] =>
[VALUE_SORT] =>
[~VALUE] => 983-987
[~DESCRIPTION] =>
[~NAME] => Стр
[~DEFAULT_VALUE] =>
)
[NUMBER_JEPTER] => Array
(
[ID] => 107
[TIMESTAMP_X] => 2016-10-18 16:42:53
[IBLOCK_ID] => 23
[NAME] => Номера
[ACTIVE] => Y
[SORT] => 500
[CODE] => NUMBER_JEPTER
[DEFAULT_VALUE] =>
[PROPERTY_TYPE] => G
[ROW_COUNT] => 1
[COL_COUNT] => 30
[LIST_TYPE] => L
[MULTIPLE] => N
[XML_ID] => 107
[FILE_TYPE] =>
[MULTIPLE_CNT] => 5
[TMP_ID] =>
[LINK_IBLOCK_ID] => 0
[WITH_DESCRIPTION] => N
[SEARCHABLE] => N
[FILTRABLE] => Y
[IS_REQUIRED] => N
[VERSION] => 1
[USER_TYPE] =>
[USER_TYPE_SETTINGS] =>
[HINT] =>
[PROPERTY_VALUE_ID] =>
[VALUE] =>
[DESCRIPTION] =>
[VALUE_ENUM] =>
[VALUE_XML_ID] =>
[VALUE_SORT] =>
[~VALUE] =>
[~DESCRIPTION] =>
[~NAME] => Номера
[~DEFAULT_VALUE] =>
)
[IFZ_FILE] => Array
(
[ID] => 304
[TIMESTAMP_X] => 2016-10-13 13:20:50
[IBLOCK_ID] => 23
[NAME] => Файл
[ACTIVE] => Y
[SORT] => 500
[CODE] => IFZ_FILE
[DEFAULT_VALUE] =>
[PROPERTY_TYPE] => F
[ROW_COUNT] => 1
[COL_COUNT] => 30
[LIST_TYPE] => L
[MULTIPLE] => N
[XML_ID] => 304
[FILE_TYPE] =>
[MULTIPLE_CNT] => 5
[TMP_ID] =>
[LINK_IBLOCK_ID] => 0
[WITH_DESCRIPTION] => N
[SEARCHABLE] => N
[FILTRABLE] => N
[IS_REQUIRED] => N
[VERSION] => 1
[USER_TYPE] =>
[USER_TYPE_SETTINGS] =>
[HINT] =>
[PROPERTY_VALUE_ID] =>
[VALUE] =>
[DESCRIPTION] =>
[VALUE_ENUM] =>
[VALUE_XML_ID] =>
[VALUE_SORT] =>
[~VALUE] =>
[~DESCRIPTION] =>
[~NAME] => Файл
[~DEFAULT_VALUE] =>
)
[IFZ_YEAR] => Array
(
[ID] => 366
[TIMESTAMP_X] => 2021-05-06 15:18:10
[IBLOCK_ID] => 23
[NAME] => Год
[ACTIVE] => Y
[SORT] => 500
[CODE] => IFZ_YEAR
[DEFAULT_VALUE] =>
[PROPERTY_TYPE] => L
[ROW_COUNT] => 1
[COL_COUNT] => 30
[LIST_TYPE] => L
[MULTIPLE] => N
[XML_ID] =>
[FILE_TYPE] =>
[MULTIPLE_CNT] => 5
[TMP_ID] =>
[LINK_IBLOCK_ID] => 0
[WITH_DESCRIPTION] => N
[SEARCHABLE] => Y
[FILTRABLE] => Y
[IS_REQUIRED] => N
[VERSION] => 1
[USER_TYPE] =>
[USER_TYPE_SETTINGS] =>
[HINT] =>
[PROPERTY_VALUE_ID] =>
[VALUE] =>
[DESCRIPTION] =>
[VALUE_ENUM] =>
[VALUE_XML_ID] =>
[VALUE_SORT] =>
[VALUE_ENUM_ID] =>
[~VALUE] =>
[~DESCRIPTION] =>
[~NAME] => Год
[~DEFAULT_VALUE] =>
)
[YEAR] => Array
(
[ID] => 390
[TIMESTAMP_X] => 2021-05-04 12:31:09
[IBLOCK_ID] => 23
[NAME] => Год
[ACTIVE] => Y
[SORT] => 500
[CODE] => YEAR
[DEFAULT_VALUE] =>
[PROPERTY_TYPE] => S
[ROW_COUNT] => 1
[COL_COUNT] => 30
[LIST_TYPE] => L
[MULTIPLE] => N
[XML_ID] =>
[FILE_TYPE] =>
[MULTIPLE_CNT] => 5
[TMP_ID] =>
[LINK_IBLOCK_ID] => 0
[WITH_DESCRIPTION] => Y
[SEARCHABLE] => Y
[FILTRABLE] => Y
[IS_REQUIRED] => N
[VERSION] => 1
[USER_TYPE] =>
[USER_TYPE_SETTINGS] =>
[HINT] =>
[PROPERTY_VALUE_ID] =>
[VALUE] =>
[DESCRIPTION] =>
[VALUE_ENUM] =>
[VALUE_XML_ID] =>
[VALUE_SORT] =>
[~VALUE] =>
[~DESCRIPTION] =>
[~NAME] => Год
[~DEFAULT_VALUE] =>
)
[AUTHOR2] => Array
(
[ID] => 391
[TIMESTAMP_X] => 2021-10-20 13:14:23
[IBLOCK_ID] => 23
[NAME] => Автор2
[ACTIVE] => Y
[SORT] => 500
[CODE] => AUTHOR2
[DEFAULT_VALUE] =>
[PROPERTY_TYPE] => S
[ROW_COUNT] => 1
[COL_COUNT] => 30
[LIST_TYPE] => L
[MULTIPLE] => N
[XML_ID] =>
[FILE_TYPE] =>
[MULTIPLE_CNT] => 5
[TMP_ID] =>
[LINK_IBLOCK_ID] => 0
[WITH_DESCRIPTION] => N
[SEARCHABLE] => N
[FILTRABLE] => N
[IS_REQUIRED] => N
[VERSION] => 1
[USER_TYPE] =>
[USER_TYPE_SETTINGS] =>
[HINT] =>
[PROPERTY_VALUE_ID] =>
[VALUE] =>
[DESCRIPTION] =>
[VALUE_ENUM] =>
[VALUE_XML_ID] =>
[VALUE_SORT] =>
[~VALUE] =>
[~DESCRIPTION] =>
[~NAME] => Автор2
[~DEFAULT_VALUE] =>
)
[COMPANY] => Array
(
[ID] => 392
[TIMESTAMP_X] => 2024-07-09 10:49:32
[IBLOCK_ID] => 23
[NAME] => Организация
[ACTIVE] => Y
[SORT] => 500
[CODE] => COMPANY
[DEFAULT_VALUE] =>
[PROPERTY_TYPE] => L
[ROW_COUNT] => 1
[COL_COUNT] => 30
[LIST_TYPE] => L
[MULTIPLE] => Y
[XML_ID] =>
[FILE_TYPE] =>
[MULTIPLE_CNT] => 5
[TMP_ID] =>
[LINK_IBLOCK_ID] => 0
[WITH_DESCRIPTION] => N
[SEARCHABLE] => N
[FILTRABLE] => N
[IS_REQUIRED] => N
[VERSION] => 1
[USER_TYPE] =>
[USER_TYPE_SETTINGS] =>
[HINT] =>
[PROPERTY_VALUE_ID] =>
[VALUE] =>
[DESCRIPTION] =>
[VALUE_ENUM] =>
[VALUE_XML_ID] =>
[VALUE_SORT] =>
[VALUE_ENUM_ID] =>
[~VALUE] =>
[~DESCRIPTION] =>
[~NAME] => Организация
[~DEFAULT_VALUE] =>
)
[UDK] => Array
(
[ID] => 393
[TIMESTAMP_X] => 2024-07-09 10:49:32
[IBLOCK_ID] => 23
[NAME] => УДК
[ACTIVE] => Y
[SORT] => 500
[CODE] => UDK
[DEFAULT_VALUE] =>
[PROPERTY_TYPE] => L
[ROW_COUNT] => 1
[COL_COUNT] => 30
[LIST_TYPE] => L
[MULTIPLE] => Y
[XML_ID] =>
[FILE_TYPE] =>
[MULTIPLE_CNT] => 5
[TMP_ID] =>
[LINK_IBLOCK_ID] => 0
[WITH_DESCRIPTION] => N
[SEARCHABLE] => N
[FILTRABLE] => N
[IS_REQUIRED] => N
[VERSION] => 1
[USER_TYPE] =>
[USER_TYPE_SETTINGS] =>
[HINT] =>
[PROPERTY_VALUE_ID] =>
[VALUE] =>
[DESCRIPTION] =>
[VALUE_ENUM] =>
[VALUE_XML_ID] =>
[VALUE_SORT] =>
[VALUE_ENUM_ID] =>
[~VALUE] =>
[~DESCRIPTION] =>
[~NAME] => УДК
[~DEFAULT_VALUE] =>
)
)
[DISPLAY_PROPERTIES] => Array
(
[AUTHOR] => Array
(
[ID] => 98
[TIMESTAMP_X] => 2021-05-05 12:29:14
[IBLOCK_ID] => 23
[NAME] => Автор
[ACTIVE] => Y
[SORT] => 500
[CODE] => AUTHOR
[DEFAULT_VALUE] => Автор
[PROPERTY_TYPE] => S
[ROW_COUNT] => 1
[COL_COUNT] => 50
[LIST_TYPE] => L
[MULTIPLE] => Y
[XML_ID] => 98
[FILE_TYPE] =>
[MULTIPLE_CNT] => 5
[TMP_ID] =>
[LINK_IBLOCK_ID] => 0
[WITH_DESCRIPTION] => N
[SEARCHABLE] => Y
[FILTRABLE] => Y
[IS_REQUIRED] => N
[VERSION] => 1
[USER_TYPE] =>
[USER_TYPE_SETTINGS] =>
[HINT] =>
[PROPERTY_VALUE_ID] => Array
(
[0] => 23960
)
[VALUE] => Array
(
[0] => М. С. Третьяк , В. В. Чупрасов
)
[DESCRIPTION] => Array
(
[0] =>
)
[VALUE_ENUM] =>
[VALUE_XML_ID] =>
[VALUE_SORT] =>
[~VALUE] => Array
(
[0] => М. С. Третьяк , В. В. Чупрасов
)
[~DESCRIPTION] => Array
(
[0] =>
)
[~NAME] => Автор
[~DEFAULT_VALUE] => Автор
[DISPLAY_VALUE] => М. С. Третьяк , В. В. Чупрасов
)
[PAGE] => Array
(
[ID] => 100
[TIMESTAMP_X] => 2024-07-09 10:49:32
[IBLOCK_ID] => 23
[NAME] => Стр
[ACTIVE] => Y
[SORT] => 500
[CODE] => PAGE
[DEFAULT_VALUE] =>
[PROPERTY_TYPE] => N
[ROW_COUNT] => 1
[COL_COUNT] => 50
[LIST_TYPE] => L
[MULTIPLE] => N
[XML_ID] => 100
[FILE_TYPE] =>
[MULTIPLE_CNT] => 5
[TMP_ID] =>
[LINK_IBLOCK_ID] => 0
[WITH_DESCRIPTION] => N
[SEARCHABLE] => N
[FILTRABLE] => Y
[IS_REQUIRED] => N
[VERSION] => 1
[USER_TYPE] =>
[USER_TYPE_SETTINGS] =>
[HINT] =>
[PROPERTY_VALUE_ID] => 23961
[VALUE] => 983-987
[DESCRIPTION] =>
[VALUE_ENUM] =>
[VALUE_XML_ID] =>
[VALUE_SORT] =>
[~VALUE] => 983-987
[~DESCRIPTION] =>
[~NAME] => Стр
[~DEFAULT_VALUE] =>
[DISPLAY_VALUE] => 983-987
)
)
)
Стр:
983-987
Оценка контактной температуры и износа композиционной фрикционной накладки при торможении
Предложена аналитическая модель определения контактной
температуры и износа рабочей поверхности элементов фрикционных тормозов.
Предполагается, что один из элементов пары трения представляет собой
двухпериодическую систему сопряженных разнородных слоев, а другой
- однородное полупространство. В процессе трения коэффициент износа
линейно зависит от контактной температуры. Изучено влияние эффективных
параметров композита, а также параметра, характеризующего изменение
нагрузки от нуля до номинального значения, на распределение контактной
температуры и износа при торможении.
Array
(
[DETAIL_TEXT] => Предложена аналитическая модель определения контактной
температуры и износа рабочей поверхности элементов фрикционных тормозов.
Предполагается, что один из элементов пары трения представляет собой
двухпериодическую систему сопряженных разнородных слоев, а другой
- однородное полупространство. В процессе трения коэффициент износа
линейно зависит от контактной температуры. Изучено влияние эффективных
параметров композита, а также параметра, характеризующего изменение
нагрузки от нуля до номинального значения, на распределение контактной
температуры и износа при торможении.
[~DETAIL_TEXT] => Предложена аналитическая модель определения контактной
температуры и износа рабочей поверхности элементов фрикционных тормозов.
Предполагается, что один из элементов пары трения представляет собой
двухпериодическую систему сопряженных разнородных слоев, а другой
- однородное полупространство. В процессе трения коэффициент износа
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Трение твердых тел с образованием слоя расплава
Показано, что применение двустороннего шаржирования с использованием
ультразвука на дисках, применяемых для распиловки природных
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Трение твердых тел с образованием слоя расплава .
Исследованы некоторые закономерности трения твердых тел
с образованием развитой прослойки расплава. В отличие от [1] изучен
случай, когда тело конечных размеров движется по твердой плавящейся
подложке (полуплоскости), причем необходимое для плавления тепло выделяется
вследствие фрикционного тепловыделения или потока тепла от тела. Для
определения оттока тепла из слоя расплава в полуплоскость и длины
зоны расплава впереди движущегося тела рассмотрены две плоские краевые
задачи уравнения теплопроводности.
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Автор:
А. А. Шугай
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Пьезоэлектрический эффект в композиционных имплантатах, предназначенных для замещения костной ткани
Разработаны полимерные композиционные имплантаты ИКВОБАН-У
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Влияние метеоусловий на мощность тепло- отвода системой аварийного охлаждения реактора
Проведен аналитический и численный анализ влияния размеров
щелей между заслонками шиберов и внешних метеоусловий на суммарные
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Автор:
Л. И. Колыхан , Ю. В. Клименков , Ю. А. Голубничий , П. П. Храмцов , В. С. Бурак , И. А. Ших
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Особенности тепломассообмена при горении жидкой горючей нагрузки в помещении с открытым проемом
Предложена интегральная математическая модель расчета
тепломассообмена при пожаре в помещении с открытыми проемами.
Представлены результаты численного исследования влияния основных
параметров задачи на среднеобъемные параметры газовой среды
помещения, температуры ограждающих конструкций и параметры
естественного газообмена с окружающей средой через открытый проем
в случае горения жидкой горючей нагрузки.
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помещения, температуры ограждающих конструкций и параметры
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Автор:
С. В. Пузач
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тепломассообмена при пожаре в помещении с открытыми проемами.
Представлены результаты численного исследования влияния основных
параметров задачи на среднеобъемные параметры газовой среды
помещения, температуры ограждающих конструкций и параметры
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тепломассообмена при пожаре в помещении с открытыми проемами.
Представлены результаты численного исследования влияния основных
параметров задачи на среднеобъемные параметры газовой среды
помещения, температуры ограждающих конструкций и параметры
естественного газообмена с окружающей средой через открытый проем
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[~TIMESTAMP_X] => 24.06.2021 11:31:41
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[PREVIEW_TEXT] =>
[~PREVIEW_TEXT] =>
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тепломассообмена при пожаре в помещении с открытыми проемами.
Представлены результаты численного исследования влияния основных
параметров задачи на среднеобъемные параметры газовой среды
помещения, температуры ограждающих конструкций и параметры
естественного газообмена с окружающей средой через открытый проем
в случае горения жидкой горючей нагрузки.
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[NAME] => Файл
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[CODE] => IFZ_FILE
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[MULTIPLE] => N
[XML_ID] => 304
[FILE_TYPE] =>
[MULTIPLE_CNT] => 5
[TMP_ID] =>
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[USER_TYPE] =>
[USER_TYPE_SETTINGS] =>
[HINT] =>
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[VALUE] =>
[DESCRIPTION] =>
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[VALUE_XML_ID] =>
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[~DEFAULT_VALUE] =>
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[VALUE_XML_ID] =>
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[~VALUE] =>
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[~DEFAULT_VALUE] =>
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[TMP_ID] =>
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[FILTRABLE] => Y
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[VERSION] => 1
[USER_TYPE] =>
[USER_TYPE_SETTINGS] =>
[HINT] =>
[PROPERTY_VALUE_ID] =>
[VALUE] =>
[DESCRIPTION] =>
[VALUE_ENUM] =>
[VALUE_XML_ID] =>
[VALUE_SORT] =>
[~VALUE] =>
[~DESCRIPTION] =>
[~NAME] => Год
[~DEFAULT_VALUE] =>
)
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[TIMESTAMP_X] => 2021-10-20 13:14:23
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[NAME] => Автор2
[ACTIVE] => Y
[SORT] => 500
[CODE] => AUTHOR2
[DEFAULT_VALUE] =>
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[ROW_COUNT] => 1
[COL_COUNT] => 30
[LIST_TYPE] => L
[MULTIPLE] => N
[XML_ID] =>
[FILE_TYPE] =>
[MULTIPLE_CNT] => 5
[TMP_ID] =>
[LINK_IBLOCK_ID] => 0
[WITH_DESCRIPTION] => N
[SEARCHABLE] => N
[FILTRABLE] => N
[IS_REQUIRED] => N
[VERSION] => 1
[USER_TYPE] =>
[USER_TYPE_SETTINGS] =>
[HINT] =>
[PROPERTY_VALUE_ID] =>
[VALUE] =>
[DESCRIPTION] =>
[VALUE_ENUM] =>
[VALUE_XML_ID] =>
[VALUE_SORT] =>
[~VALUE] =>
[~DESCRIPTION] =>
[~NAME] => Автор2
[~DEFAULT_VALUE] =>
)
[COMPANY] => Array
(
[ID] => 392
[TIMESTAMP_X] => 2024-07-09 10:49:32
[IBLOCK_ID] => 23
[NAME] => Организация
[ACTIVE] => Y
[SORT] => 500
[CODE] => COMPANY
[DEFAULT_VALUE] =>
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[ROW_COUNT] => 1
[COL_COUNT] => 30
[LIST_TYPE] => L
[MULTIPLE] => Y
[XML_ID] =>
[FILE_TYPE] =>
[MULTIPLE_CNT] => 5
[TMP_ID] =>
[LINK_IBLOCK_ID] => 0
[WITH_DESCRIPTION] => N
[SEARCHABLE] => N
[FILTRABLE] => N
[IS_REQUIRED] => N
[VERSION] => 1
[USER_TYPE] =>
[USER_TYPE_SETTINGS] =>
[HINT] =>
[PROPERTY_VALUE_ID] =>
[VALUE] =>
[DESCRIPTION] =>
[VALUE_ENUM] =>
[VALUE_XML_ID] =>
[VALUE_SORT] =>
[VALUE_ENUM_ID] =>
[~VALUE] =>
[~DESCRIPTION] =>
[~NAME] => Организация
[~DEFAULT_VALUE] =>
)
[UDK] => Array
(
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[TIMESTAMP_X] => 2024-07-09 10:49:32
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[NAME] => УДК
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[SORT] => 500
[CODE] => UDK
[DEFAULT_VALUE] =>
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[COL_COUNT] => 30
[LIST_TYPE] => L
[MULTIPLE] => Y
[XML_ID] =>
[FILE_TYPE] =>
[MULTIPLE_CNT] => 5
[TMP_ID] =>
[LINK_IBLOCK_ID] => 0
[WITH_DESCRIPTION] => N
[SEARCHABLE] => N
[FILTRABLE] => N
[IS_REQUIRED] => N
[VERSION] => 1
[USER_TYPE] =>
[USER_TYPE_SETTINGS] =>
[HINT] =>
[PROPERTY_VALUE_ID] =>
[VALUE] =>
[DESCRIPTION] =>
[VALUE_ENUM] =>
[VALUE_XML_ID] =>
[VALUE_SORT] =>
[VALUE_ENUM_ID] =>
[~VALUE] =>
[~DESCRIPTION] =>
[~NAME] => УДК
[~DEFAULT_VALUE] =>
)
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(
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(
[ID] => 98
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[NAME] => Автор
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[ROW_COUNT] => 1
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[LIST_TYPE] => L
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[XML_ID] => 98
[FILE_TYPE] =>
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[TMP_ID] =>
[LINK_IBLOCK_ID] => 0
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[SEARCHABLE] => Y
[FILTRABLE] => Y
[IS_REQUIRED] => N
[VERSION] => 1
[USER_TYPE] =>
[USER_TYPE_SETTINGS] =>
[HINT] =>
[PROPERTY_VALUE_ID] => Array
(
[0] => 23972
)
[VALUE] => Array
(
[0] => С. В. Пузач
)
[DESCRIPTION] => Array
(
[0] =>
)
[VALUE_ENUM] =>
[VALUE_XML_ID] =>
[VALUE_SORT] =>
[~VALUE] => Array
(
[0] => С. В. Пузач
)
[~DESCRIPTION] => Array
(
[0] =>
)
[~NAME] => Автор
[~DEFAULT_VALUE] => Автор
[DISPLAY_VALUE] => С. В. Пузач
)
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(
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[TIMESTAMP_X] => 2024-07-09 10:49:32
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[NAME] => Стр
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[CODE] => PAGE
[DEFAULT_VALUE] =>
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[ROW_COUNT] => 1
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[LIST_TYPE] => L
[MULTIPLE] => N
[XML_ID] => 100
[FILE_TYPE] =>
[MULTIPLE_CNT] => 5
[TMP_ID] =>
[LINK_IBLOCK_ID] => 0
[WITH_DESCRIPTION] => N
[SEARCHABLE] => N
[FILTRABLE] => Y
[IS_REQUIRED] => N
[VERSION] => 1
[USER_TYPE] =>
[USER_TYPE_SETTINGS] =>
[HINT] =>
[PROPERTY_VALUE_ID] => 23973
[VALUE] => 1025-1032
[DESCRIPTION] =>
[VALUE_ENUM] =>
[VALUE_XML_ID] =>
[VALUE_SORT] =>
[~VALUE] => 1025-1032
[~DESCRIPTION] =>
[~NAME] => Стр
[~DEFAULT_VALUE] =>
[DISPLAY_VALUE] => 1025-1032
)
)
)
Стр:
1025-1032
Об автоколебаниях при фронтальном горении топливной смеси в резонаторе с сосредоточенными параметрами
Рассмотрены условия возбуждения гармонических автоколебаний
при фронтальном горении топливной смеси в горле или в полости резонатора
Гельмгольца. Показано, что они зависят от свойств топливной смеси,
положения и ориентации фронта пламени и могут выполняться только при
наличии в зоне горения поверхности разрыва параметров, определяющих
скорость горения. Отмечается, что следствия анализа не входят в противоречие
с фактами и зависимостями, наблюдаемыми при сжигании топливных смесей
в туннельных горелках, поршневых карбюраторных и ракетных двигателях.
Array
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В. Н. Гладышев
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)
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[TIMESTAMP_X] => 2016-10-18 16:42:53
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[~DEFAULT_VALUE] =>
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[NAME] => Файл
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[DEFAULT_VALUE] =>
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[COL_COUNT] => 30
[LIST_TYPE] => L
[MULTIPLE] => N
[XML_ID] => 304
[FILE_TYPE] =>
[MULTIPLE_CNT] => 5
[TMP_ID] =>
[LINK_IBLOCK_ID] => 0
[WITH_DESCRIPTION] => N
[SEARCHABLE] => N
[FILTRABLE] => N
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[VERSION] => 1
[USER_TYPE] =>
[USER_TYPE_SETTINGS] =>
[HINT] =>
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[DESCRIPTION] =>
[VALUE_ENUM] =>
[VALUE_XML_ID] =>
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[~VALUE] =>
[~DESCRIPTION] =>
[~NAME] => Файл
[~DEFAULT_VALUE] =>
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[IFZ_YEAR] => Array
(
[ID] => 366
[TIMESTAMP_X] => 2021-05-06 15:18:10
[IBLOCK_ID] => 23
[NAME] => Год
[ACTIVE] => Y
[SORT] => 500
[CODE] => IFZ_YEAR
[DEFAULT_VALUE] =>
[PROPERTY_TYPE] => L
[ROW_COUNT] => 1
[COL_COUNT] => 30
[LIST_TYPE] => L
[MULTIPLE] => N
[XML_ID] =>
[FILE_TYPE] =>
[MULTIPLE_CNT] => 5
[TMP_ID] =>
[LINK_IBLOCK_ID] => 0
[WITH_DESCRIPTION] => N
[SEARCHABLE] => Y
[FILTRABLE] => Y
[IS_REQUIRED] => N
[VERSION] => 1
[USER_TYPE] =>
[USER_TYPE_SETTINGS] =>
[HINT] =>
[PROPERTY_VALUE_ID] =>
[VALUE] =>
[DESCRIPTION] =>
[VALUE_ENUM] =>
[VALUE_XML_ID] =>
[VALUE_SORT] =>
[VALUE_ENUM_ID] =>
[~VALUE] =>
[~DESCRIPTION] =>
[~NAME] => Год
[~DEFAULT_VALUE] =>
)
[YEAR] => Array
(
[ID] => 390
[TIMESTAMP_X] => 2021-05-04 12:31:09
[IBLOCK_ID] => 23
[NAME] => Год
[ACTIVE] => Y
[SORT] => 500
[CODE] => YEAR
[DEFAULT_VALUE] =>
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[COL_COUNT] => 30
[LIST_TYPE] => L
[MULTIPLE] => N
[XML_ID] =>
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[TMP_ID] =>
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[WITH_DESCRIPTION] => Y
[SEARCHABLE] => Y
[FILTRABLE] => Y
[IS_REQUIRED] => N
[VERSION] => 1
[USER_TYPE] =>
[USER_TYPE_SETTINGS] =>
[HINT] =>
[PROPERTY_VALUE_ID] =>
[VALUE] =>
[DESCRIPTION] =>
[VALUE_ENUM] =>
[VALUE_XML_ID] =>
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[~DESCRIPTION] =>
[~NAME] => Год
[~DEFAULT_VALUE] =>
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[TIMESTAMP_X] => 2021-10-20 13:14:23
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[NAME] => Автор2
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[XML_ID] =>
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[MULTIPLE_CNT] => 5
[TMP_ID] =>
[LINK_IBLOCK_ID] => 0
[WITH_DESCRIPTION] => N
[SEARCHABLE] => N
[FILTRABLE] => N
[IS_REQUIRED] => N
[VERSION] => 1
[USER_TYPE] =>
[USER_TYPE_SETTINGS] =>
[HINT] =>
[PROPERTY_VALUE_ID] =>
[VALUE] =>
[DESCRIPTION] =>
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[TIMESTAMP_X] => 2024-07-09 10:49:32
[IBLOCK_ID] => 23
[NAME] => Организация
[ACTIVE] => Y
[SORT] => 500
[CODE] => COMPANY
[DEFAULT_VALUE] =>
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[COL_COUNT] => 30
[LIST_TYPE] => L
[MULTIPLE] => Y
[XML_ID] =>
[FILE_TYPE] =>
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[TMP_ID] =>
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[WITH_DESCRIPTION] => N
[SEARCHABLE] => N
[FILTRABLE] => N
[IS_REQUIRED] => N
[VERSION] => 1
[USER_TYPE] =>
[USER_TYPE_SETTINGS] =>
[HINT] =>
[PROPERTY_VALUE_ID] =>
[VALUE] =>
[DESCRIPTION] =>
[VALUE_ENUM] =>
[VALUE_XML_ID] =>
[VALUE_SORT] =>
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[~NAME] => Организация
[~DEFAULT_VALUE] =>
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[UDK] => Array
(
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[TIMESTAMP_X] => 2024-07-09 10:49:32
[IBLOCK_ID] => 23
[NAME] => УДК
[ACTIVE] => Y
[SORT] => 500
[CODE] => UDK
[DEFAULT_VALUE] =>
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[COL_COUNT] => 30
[LIST_TYPE] => L
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[XML_ID] =>
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[TMP_ID] =>
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[SEARCHABLE] => N
[FILTRABLE] => N
[IS_REQUIRED] => N
[VERSION] => 1
[USER_TYPE] =>
[USER_TYPE_SETTINGS] =>
[HINT] =>
[PROPERTY_VALUE_ID] =>
[VALUE] =>
[DESCRIPTION] =>
[VALUE_ENUM] =>
[VALUE_XML_ID] =>
[VALUE_SORT] =>
[VALUE_ENUM_ID] =>
[~VALUE] =>
[~DESCRIPTION] =>
[~NAME] => УДК
[~DEFAULT_VALUE] =>
)
)
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(
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(
[ID] => 98
[TIMESTAMP_X] => 2021-05-05 12:29:14
[IBLOCK_ID] => 23
[NAME] => Автор
[ACTIVE] => Y
[SORT] => 500
[CODE] => AUTHOR
[DEFAULT_VALUE] => Автор
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[XML_ID] => 98
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[TMP_ID] =>
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[SEARCHABLE] => Y
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[VERSION] => 1
[USER_TYPE] =>
[USER_TYPE_SETTINGS] =>
[HINT] =>
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(
[0] => 23974
)
[VALUE] => Array
(
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)
[DESCRIPTION] => Array
(
[0] =>
)
[VALUE_ENUM] =>
[VALUE_XML_ID] =>
[VALUE_SORT] =>
[~VALUE] => Array
(
[0] => В. Н. Гладышев
)
[~DESCRIPTION] => Array
(
[0] =>
)
[~NAME] => Автор
[~DEFAULT_VALUE] => Автор
[DISPLAY_VALUE] => В. Н. Гладышев
)
[PAGE] => Array
(
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[TIMESTAMP_X] => 2024-07-09 10:49:32
[IBLOCK_ID] => 23
[NAME] => Стр
[ACTIVE] => Y
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[CODE] => PAGE
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[ROW_COUNT] => 1
[COL_COUNT] => 50
[LIST_TYPE] => L
[MULTIPLE] => N
[XML_ID] => 100
[FILE_TYPE] =>
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[TMP_ID] =>
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[WITH_DESCRIPTION] => N
[SEARCHABLE] => N
[FILTRABLE] => Y
[IS_REQUIRED] => N
[VERSION] => 1
[USER_TYPE] =>
[USER_TYPE_SETTINGS] =>
[HINT] =>
[PROPERTY_VALUE_ID] => 23975
[VALUE] => 1033-1040
[DESCRIPTION] =>
[VALUE_ENUM] =>
[VALUE_XML_ID] =>
[VALUE_SORT] =>
[~VALUE] => 1033-1040
[~DESCRIPTION] =>
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Стр:
1033-1040
О гидродинамике циркулирующего кипящего слоя
В рамках теории подобия с использованием критериев
Frt и Js, являющихся обобщенными характеристиками
циркулирующего кипящего слоя, получены безразмерные зависимости,
описывающие имеющиеся опытные данные по пристеночным массовым
потокам частиц и касательному напряжению на стенках стояка.
Выяснено влияние на эти величины масштабного фактора, других
параметров системы. Разработана методика расчета массовых потоков
частиц в ядре слоя.
Array
(
[DETAIL_TEXT] => В рамках теории подобия с использованием критериев
Frt и Js, являющихся обобщенными характеристиками
циркулирующего кипящего слоя, получены безразмерные зависимости,
описывающие имеющиеся опытные данные по пристеночным массовым
потокам частиц и касательному напряжению на стенках стояка.
Выяснено влияние на эти величины масштабного фактора, других
параметров системы. Разработана методика расчета массовых потоков
частиц в ядре слоя.
[~DETAIL_TEXT] => В рамках теории подобия с использованием критериев
Frt и Js, являющихся обобщенными характеристиками
циркулирующего кипящего слоя, получены безразмерные зависимости,
описывающие имеющиеся опытные данные по пристеночным массовым
потокам частиц и касательному напряжению на стенках стояка.
Выяснено влияние на эти величины масштабного фактора, других
параметров системы. Разработана методика расчета массовых потоков
частиц в ядре слоя.
[ID] => 6935
[~ID] => 6935
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[~NAME] => О гидродинамике циркулирующего кипящего слоя
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[~TIMESTAMP_X] => 24.06.2021 11:35:08
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[~DETAIL_PAGE_URL] => /publications/jepter/bibl/?ELEMENT_ID=6935
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[~LIST_PAGE_URL] => /publications/jepter/bibl/
[DETAIL_TEXT_TYPE] => html
[~DETAIL_TEXT_TYPE] => html
[PREVIEW_TEXT] =>
[~PREVIEW_TEXT] =>
[PREVIEW_TEXT_TYPE] => text
[~PREVIEW_TEXT_TYPE] => text
[PREVIEW_PICTURE] =>
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[IBLOCK_TYPE_ID] => aspro_corporation_content
[~IBLOCK_TYPE_ID] => aspro_corporation_content
[IBLOCK_CODE] => IFZ
[~IBLOCK_CODE] => IFZ
[IBLOCK_EXTERNAL_ID] => 23
[~IBLOCK_EXTERNAL_ID] => 23
[LID] => s1
[~LID] => s1
[EDIT_LINK] =>
[DELETE_LINK] =>
[DISPLAY_ACTIVE_FROM] =>
[IPROPERTY_VALUES] => Array
(
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Frt и Js, являющихся обобщенными характеристиками
циркулирующего кипящего слоя, получены безразмерные зависимости,
описывающие имеющиеся опытные данные по пристеночным массовым
потокам частиц и касательному напряжению на стенках стояка.
Выяснено влияние на эти величины масштабного фактора, других
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частиц в ядре слоя.
)
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(
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)
[~DESCRIPTION] => Array
(
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)
[~NAME] => Автор
[~DEFAULT_VALUE] => Автор
)
[KEYWORDS] => Array
(
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[USER_TYPE] =>
[USER_TYPE_SETTINGS] =>
[HINT] =>
[PROPERTY_VALUE_ID] =>
[VALUE] =>
[DESCRIPTION] =>
[VALUE_ENUM] =>
[VALUE_XML_ID] =>
[VALUE_SORT] =>
[~VALUE] =>
[~DESCRIPTION] =>
[~NAME] => Ключевые слова
[~DEFAULT_VALUE] =>
)
[PAGE] => Array
(
[ID] => 100
[TIMESTAMP_X] => 2024-07-09 10:49:32
[IBLOCK_ID] => 23
[NAME] => Стр
[ACTIVE] => Y
[SORT] => 500
[CODE] => PAGE
[DEFAULT_VALUE] =>
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[COL_COUNT] => 50
[LIST_TYPE] => L
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[XML_ID] => 100
[FILE_TYPE] =>
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[USER_TYPE] =>
[USER_TYPE_SETTINGS] =>
[HINT] =>
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[VALUE] => 1041-1046
[DESCRIPTION] =>
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[VALUE_SORT] =>
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[~DESCRIPTION] =>
[~NAME] => Стр
[~DEFAULT_VALUE] =>
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(
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[TIMESTAMP_X] => 2016-10-18 16:42:53
[IBLOCK_ID] => 23
[NAME] => Номера
[ACTIVE] => Y
[SORT] => 500
[CODE] => NUMBER_JEPTER
[DEFAULT_VALUE] =>
[PROPERTY_TYPE] => G
[ROW_COUNT] => 1
[COL_COUNT] => 30
[LIST_TYPE] => L
[MULTIPLE] => N
[XML_ID] => 107
[FILE_TYPE] =>
[MULTIPLE_CNT] => 5
[TMP_ID] =>
[LINK_IBLOCK_ID] => 0
[WITH_DESCRIPTION] => N
[SEARCHABLE] => N
[FILTRABLE] => Y
[IS_REQUIRED] => N
[VERSION] => 1
[USER_TYPE] =>
[USER_TYPE_SETTINGS] =>
[HINT] =>
[PROPERTY_VALUE_ID] =>
[VALUE] =>
[DESCRIPTION] =>
[VALUE_ENUM] =>
[VALUE_XML_ID] =>
[VALUE_SORT] =>
[~VALUE] =>
[~DESCRIPTION] =>
[~NAME] => Номера
[~DEFAULT_VALUE] =>
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[IFZ_FILE] => Array
(
[ID] => 304
[TIMESTAMP_X] => 2016-10-13 13:20:50
[IBLOCK_ID] => 23
[NAME] => Файл
[ACTIVE] => Y
[SORT] => 500
[CODE] => IFZ_FILE
[DEFAULT_VALUE] =>
[PROPERTY_TYPE] => F
[ROW_COUNT] => 1
[COL_COUNT] => 30
[LIST_TYPE] => L
[MULTIPLE] => N
[XML_ID] => 304
[FILE_TYPE] =>
[MULTIPLE_CNT] => 5
[TMP_ID] =>
[LINK_IBLOCK_ID] => 0
[WITH_DESCRIPTION] => N
[SEARCHABLE] => N
[FILTRABLE] => N
[IS_REQUIRED] => N
[VERSION] => 1
[USER_TYPE] =>
[USER_TYPE_SETTINGS] =>
[HINT] =>
[PROPERTY_VALUE_ID] =>
[VALUE] =>
[DESCRIPTION] =>
[VALUE_ENUM] =>
[VALUE_XML_ID] =>
[VALUE_SORT] =>
[~VALUE] =>
[~DESCRIPTION] =>
[~NAME] => Файл
[~DEFAULT_VALUE] =>
)
[IFZ_YEAR] => Array
(
[ID] => 366
[TIMESTAMP_X] => 2021-05-06 15:18:10
[IBLOCK_ID] => 23
[NAME] => Год
[ACTIVE] => Y
[SORT] => 500
[CODE] => IFZ_YEAR
[DEFAULT_VALUE] =>
[PROPERTY_TYPE] => L
[ROW_COUNT] => 1
[COL_COUNT] => 30
[LIST_TYPE] => L
[MULTIPLE] => N
[XML_ID] =>
[FILE_TYPE] =>
[MULTIPLE_CNT] => 5
[TMP_ID] =>
[LINK_IBLOCK_ID] => 0
[WITH_DESCRIPTION] => N
[SEARCHABLE] => Y
[FILTRABLE] => Y
[IS_REQUIRED] => N
[VERSION] => 1
[USER_TYPE] =>
[USER_TYPE_SETTINGS] =>
[HINT] =>
[PROPERTY_VALUE_ID] =>
[VALUE] =>
[DESCRIPTION] =>
[VALUE_ENUM] =>
[VALUE_XML_ID] =>
[VALUE_SORT] =>
[VALUE_ENUM_ID] =>
[~VALUE] =>
[~DESCRIPTION] =>
[~NAME] => Год
[~DEFAULT_VALUE] =>
)
[YEAR] => Array
(
[ID] => 390
[TIMESTAMP_X] => 2021-05-04 12:31:09
[IBLOCK_ID] => 23
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Автор:
Ю. С. Теплицкий , В. И. Ковенский
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Выяснено влияние на эти величины масштабного фактора, других
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Выяснено влияние на эти величины масштабного фактора, других
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Выяснено влияние на эти величины масштабного фактора, других
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Автор:
Бровман М. Я.
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Стр:
1047-1048
О движении волны прорыва в нижнем бьефе в случае мокрого русла
В работе [1] было показано, что асимптотическое (при t
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Автором впервые был обнаружен режим постоянной прерывной волны.
В представленной работе дается развитие теории для трех случаев
открытого потока: склона и русел прямоугольного и треугольного
поперечного сечения.
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