Номер 17.3, страница 105 - гдз по физике 8-11 класс учебник, задачник Гельфгат, Генденштейн

Физика, 8-11 класс Учебник, задачник, авторы: Гельфгат Илья Маркович, Генденштейн Лев Элевич, Кирик Леонид Анатольевич, издательство Илекса, Москва, 2005

Авторы: Гельфгат И. М., Генденштейн Л. Э., Кирик Л. А.

Тип: Учебник, задачник

Издательство: Илекса

Год издания: 2005 - 2026

Цвет обложки: синий мужчина в красном, летит на черном шаре

ISBN: 978-5-89237-332-6

Задачи. Электричество и магнетизм. 17. Электромагнитные колебания и волны. Переменный ток - номер 17.3, страница 105.

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            "field_navigation_title" => null
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            "field_metatags_description" => null
            "field_h1" => null
            "field_description_top" => null
            "field_description_bottom" => null
            "field_branch_cover" => []
            "field_branch_covers" => []
            "book" => Illuminate\Database\Eloquent\Collection {#1075}
            "branch_parent" => Illuminate\Database\Eloquent\Collection {#1111}
          ]
          #changes: []
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          #classCastCache: []
          #attributeCastCache: []
          #dateFormat: null
          #appends: []
          #dispatchesEvents: []
          #observables: []
          #relations: []
          #touches: []
          +timestamps: true
          +usesUniqueIds: false
          #hidden: []
          #visible: []
          #fillable: []
          #guarded: array:1 [
            0 => "*"
          ]
        }
        1 => App\Models\Branch {#1112
          #connection: "mysql"
          #table: "branches"
          #primaryKey: "id"
          #keyType: "int"
          +incrementing: true
          #with: []
          #withCount: []
          +preventsLazyLoading: false
          #perPage: 15
          +exists: true
          +wasRecentlyCreated: false
          #escapeWhenCastingToString: false
          #attributes: array:24 [
            "id" => 1287880
            "created_at" => "2026-04-10 13:58:26"
            "updated_at" => null
            "field_display_title" => "Электричество и магнетизм"
            "field_branch_order" => null
            "field_url" => null
            "field_branch_type" => Illuminate\Database\Eloquent\Collection {#1113
              #items: []
              #escapeWhenCastingToString: false
            }
            "field_page_start" => "68"
            "field_branch_display" => "0"
            "field_branch_expanded" => "0"
            "field_display_branch_in_title" => "1"
            "field_display_task_interval" => "0"
            "field_display_branch_page" => "1"
            "field_branch_title_in_content" => "0"
            "field_navigation_title" => null
            "field_metatags_title" => null
            "field_metatags_description" => null
            "field_h1" => null
            "field_description_top" => null
            "field_description_bottom" => null
            "field_branch_cover" => []
            "field_branch_covers" => []
            "book" => Illuminate\Database\Eloquent\Collection {#1114
              #items: array:1 [
                0 => App\Models\Book {#1115
                  #connection: "mysql"
                  #table: "books"
                  #primaryKey: "id"
                  #keyType: "int"
                  +incrementing: false
                  #with: []
                  #withCount: []
                  +preventsLazyLoading: false
                  #perPage: 15
                  +exists: true
                  +wasRecentlyCreated: false
                  #escapeWhenCastingToString: false
                  #attributes: array:50 [
                    "id" => 5401
                    "created_at" => "2026-04-10 13:58:26"
                    "updated_at" => null
                    "field_tree_default_status" => "tasks"
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                    "field_subject" => Illuminate\Database\Eloquent\Collection {#1116 …2}
                    "field_class" => Illuminate\Database\Eloquent\Collection {#1118 …2}
                    "field_publisher" => Illuminate\Database\Eloquent\Collection {#1123 …2}
                    "field_author" => Illuminate\Database\Eloquent\Collection {#1125 …2}
                    "field_author_foreign" => Illuminate\Database\Eloquent\Collection {#1129 …2}
                    "field_book_type" => Illuminate\Database\Eloquent\Collection {#1130 …2}
                    "field_country" => Illuminate\Database\Eloquent\Collection {#1132 …2}
                    "field_city" => Illuminate\Database\Eloquent\Collection {#1134 …2}
                    "field_series" => Illuminate\Database\Eloquent\Collection {#1136 …2}
                    "field_umk" => Illuminate\Database\Eloquent\Collection {#1137 …2}
                    "field_level_of_education" => Illuminate\Database\Eloquent\Collection {#1138 …2}
                    "field_standart_of_education" => Illuminate\Database\Eloquent\Collection {#1139 …2}
                    "field_publication_number" => "6"
                    "field_publication_type" => Illuminate\Database\Eloquent\Collection {#1140 …2}
                    "field_under_the_edition" => Illuminate\Database\Eloquent\Collection {#1142 …2}
                    "field_under_the_edition_degree" => null
                    "field_cover_description" => "мужчина в красном, летит на черном шаре"
                    "field_publication_year" => "2005"
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                    "field_part" => ""
                    "field_part_writing" => ""
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                    "field_for_whom" => "Учебное издание"
                    "field_allowed" => null
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                    "field_tasks_count" => "1001"
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                    "field_default_folder" => "/fizika_08/gelfgat-u/"
                    "field_isbn" => "978-5-89237-332-6"
                    "field_cover" => array:1 [ …1]
                    "field_cover_alts" => array:1 [ …1]
                    "field_covers" => array:1 [ …1]
                    "field_popular_book" => "0"
                    "field_recommended_books" => Illuminate\Database\Eloquent\Collection {#1143 …2}
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                    "field_old_book" => Illuminate\Database\Eloquent\Collection {#1145 …2}
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                    "field_cover_color" => Illuminate\Database\Eloquent\Collection {#1146 …2}
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                    "breadcrumbs" => array:3 [ …3]
                  ]
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                    "id" => 5401
                    "created_at" => "2026-04-10 13:58:26"
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                    "field_subject" => Illuminate\Database\Eloquent\Collection {#1116 …2}
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                    "field_author_foreign" => Illuminate\Database\Eloquent\Collection {#1129 …2}
                    "field_book_type" => Illuminate\Database\Eloquent\Collection {#1130 …2}
                    "field_country" => Illuminate\Database\Eloquent\Collection {#1132 …2}
                    "field_city" => Illuminate\Database\Eloquent\Collection {#1134 …2}
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                    "field_level_of_education" => Illuminate\Database\Eloquent\Collection {#1138 …2}
                    "field_standart_of_education" => Illuminate\Database\Eloquent\Collection {#1139 …2}
                    "field_publication_number" => "6"
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                    "field_under_the_edition" => Illuminate\Database\Eloquent\Collection {#1142 …2}
                    "field_under_the_edition_degree" => null
                    "field_cover_description" => "мужчина в красном, летит на черном шаре"
                    "field_publication_year" => "2005"
                    "field_publication_year_until" => null
                    "field_part" => ""
                    "field_part_writing" => ""
                    "field_second_foreign_language" => null
                    "field_for_whom" => "Учебное издание"
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                    "field_default_folder" => "/fizika_08/gelfgat-u/"
                    "field_isbn" => "978-5-89237-332-6"
                    "field_cover" => array:1 [ …1]
                    "field_cover_alts" => array:1 [ …1]
                    "field_covers" => array:1 [ …1]
                    "field_popular_book" => "0"
                    "field_recommended_books" => Illuminate\Database\Eloquent\Collection {#1143 …2}
                    "field_new_book" => Illuminate\Database\Eloquent\Collection {#1144 …2}
                    "field_old_book" => Illuminate\Database\Eloquent\Collection {#1145 …2}
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                    "field_cover_color" => Illuminate\Database\Eloquent\Collection {#1146 …2}
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                    "field_metatags_description" => null
                    "field_h1" => null
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                    "breadcrumbs" => array:3 [ …3]
                  ]
                  #changes: []
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                  #touches: []
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                  #visible: []
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                    0 => "*"
                  ]
                }
              ]
              #escapeWhenCastingToString: false
            }
            "branch_parent" => Illuminate\Database\Eloquent\Collection {#1148
              #items: array:1 [
                0 => App\Models\Branch {#1149
                  #connection: "mysql"
                  #table: "branches"
                  #primaryKey: "id"
                  #keyType: "int"
                  +incrementing: true
                  #with: []
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                  #perPage: 15
                  +exists: true
                  +wasRecentlyCreated: false
                  #escapeWhenCastingToString: false
                  #attributes: array:24 [
                    "id" => 1287866
                    "created_at" => "2026-04-10 13:58:26"
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                    "field_branch_type" => Illuminate\Database\Eloquent\Collection {#1150 …2}
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                    "field_branch_covers" => []
                    "book" => Illuminate\Database\Eloquent\Collection {#1151 …2}
                    "branch_parent" => Illuminate\Database\Eloquent\Collection {#1152 …2}
                  ]
                  #original: array:24 [
                    "id" => 1287866
                    "created_at" => "2026-04-10 13:58:26"
                    "updated_at" => null
                    "field_display_title" => "Задачи"
                    "field_branch_order" => null
                    "field_url" => null
                    "field_branch_type" => Illuminate\Database\Eloquent\Collection {#1150 …2}
                    "field_page_start" => "5"
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                    "field_branch_covers" => []
                    "book" => Illuminate\Database\Eloquent\Collection {#1151 …2}
                    "branch_parent" => Illuminate\Database\Eloquent\Collection {#1152 …2}
                  ]
                  #changes: []
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                  #classCastCache: []
                  #attributeCastCache: []
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                  #touches: []
                  +timestamps: true
                  +usesUniqueIds: false
                  #hidden: []
                  #visible: []
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                  #guarded: array:1 [
                    0 => "*"
                  ]
                }
              ]
              #escapeWhenCastingToString: false
            }
          ]
          #original: array:24 [
            "id" => 1287880
            "created_at" => "2026-04-10 13:58:26"
            "updated_at" => null
            "field_display_title" => "Электричество и магнетизм"
            "field_branch_order" => null
            "field_url" => null
            "field_branch_type" => Illuminate\Database\Eloquent\Collection {#1113}
            "field_page_start" => "68"
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            "field_navigation_title" => null
            "field_metatags_title" => null
            "field_metatags_description" => null
            "field_h1" => null
            "field_description_top" => null
            "field_description_bottom" => null
            "field_branch_cover" => []
            "field_branch_covers" => []
            "book" => Illuminate\Database\Eloquent\Collection {#1114}
            "branch_parent" => Illuminate\Database\Eloquent\Collection {#1148}
          ]
          #changes: []
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          #classCastCache: []
          #attributeCastCache: []
          #dateFormat: null
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          #relations: []
          #touches: []
          +timestamps: true
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          #hidden: []
          #visible: []
          #fillable: []
          #guarded: array:1 [
            0 => "*"
          ]
        }
        2 => App\Models\Branch {#1153
          #connection: "mysql"
          #table: "branches"
          #primaryKey: "id"
          #keyType: "int"
          +incrementing: true
          #with: []
          #withCount: []
          +preventsLazyLoading: false
          #perPage: 15
          +exists: true
          +wasRecentlyCreated: false
          #escapeWhenCastingToString: false
          #attributes: array:24 [
            "id" => 1287886
            "created_at" => "2026-04-10 13:58:26"
            "updated_at" => null
            "field_display_title" => "17. Электромагнитные колебания и волны. Переменный ток"
            "field_branch_order" => null
            "field_url" => null
            "field_branch_type" => Illuminate\Database\Eloquent\Collection {#1154
              #items: []
              #escapeWhenCastingToString: false
            }
            "field_page_start" => "105"
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            "field_display_branch_in_title" => "1"
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            "field_h1" => null
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            "field_description_bottom" => null
            "field_branch_cover" => []
            "field_branch_covers" => []
            "book" => Illuminate\Database\Eloquent\Collection {#1155
              #items: array:1 [
                0 => App\Models\Book {#1156
                  #connection: "mysql"
                  #table: "books"
                  #primaryKey: "id"
                  #keyType: "int"
                  +incrementing: false
                  #with: []
                  #withCount: []
                  +preventsLazyLoading: false
                  #perPage: 15
                  +exists: true
                  +wasRecentlyCreated: false
                  #escapeWhenCastingToString: false
                  #attributes: array:50 [
                    "id" => 5401
                    "created_at" => "2026-04-10 13:58:26"
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                    "field_subject" => Illuminate\Database\Eloquent\Collection {#1157 …2}
                    "field_class" => Illuminate\Database\Eloquent\Collection {#1159 …2}
                    "field_publisher" => Illuminate\Database\Eloquent\Collection {#1164 …2}
                    "field_author" => Illuminate\Database\Eloquent\Collection {#1166 …2}
                    "field_author_foreign" => Illuminate\Database\Eloquent\Collection {#1170 …2}
                    "field_book_type" => Illuminate\Database\Eloquent\Collection {#1171 …2}
                    "field_country" => Illuminate\Database\Eloquent\Collection {#1173 …2}
                    "field_city" => Illuminate\Database\Eloquent\Collection {#1175 …2}
                    "field_series" => Illuminate\Database\Eloquent\Collection {#1177 …2}
                    "field_umk" => Illuminate\Database\Eloquent\Collection {#1178 …2}
                    "field_level_of_education" => Illuminate\Database\Eloquent\Collection {#1179 …2}
                    "field_standart_of_education" => Illuminate\Database\Eloquent\Collection {#1180 …2}
                    "field_publication_number" => "6"
                    "field_publication_type" => Illuminate\Database\Eloquent\Collection {#1181 …2}
                    "field_under_the_edition" => Illuminate\Database\Eloquent\Collection {#1183 …2}
                    "field_under_the_edition_degree" => null
                    "field_cover_description" => "мужчина в красном, летит на черном шаре"
                    "field_publication_year" => "2005"
                    "field_publication_year_until" => null
                    "field_part" => ""
                    "field_part_writing" => ""
                    "field_second_foreign_language" => null
                    "field_for_whom" => "Учебное издание"
                    "field_allowed" => null
                    "field_reserve_field" => null
                    "field_link_to_source" => null
                    "field_tasks_count" => "1001"
                    "field_priority" => null
                    "field_default_folder" => "/fizika_08/gelfgat-u/"
                    "field_isbn" => "978-5-89237-332-6"
                    "field_cover" => array:1 [ …1]
                    "field_cover_alts" => array:1 [ …1]
                    "field_covers" => array:1 [ …1]
                    "field_popular_book" => "0"
                    "field_recommended_books" => Illuminate\Database\Eloquent\Collection {#1184 …2}
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                    "field_old_book" => Illuminate\Database\Eloquent\Collection {#1186 …2}
                    "field_url" => "/8-klass/fizika/ileksa-gelfgat-uchebnik"
                    "field_cover_color" => Illuminate\Database\Eloquent\Collection {#1187 …2}
                    "field_metatags_title" => null
                    "field_metatags_description" => null
                    "field_h1" => null
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                    "breadcrumbs" => array:3 [ …3]
                  ]
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                    "field_author_foreign" => Illuminate\Database\Eloquent\Collection {#1170 …2}
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                    "field_default_folder" => "/fizika_08/gelfgat-u/"
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                    "field_cover" => array:1 [ …1]
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                    "field_cover_color" => Illuminate\Database\Eloquent\Collection {#1187 …2}
                    "field_metatags_title" => null
                    "field_metatags_description" => null
                    "field_h1" => null
                    "field_description_top" => null
                    "field_description_bottom" => null
                    "breadcrumbs" => array:3 [ …3]
                  ]
                  #changes: []
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                    0 => "*"
                  ]
                }
              ]
              #escapeWhenCastingToString: false
            }
            "branch_parent" => Illuminate\Database\Eloquent\Collection {#1189
              #items: array:1 [
                0 => App\Models\Branch {#1190
                  #connection: "mysql"
                  #table: "branches"
                  #primaryKey: "id"
                  #keyType: "int"
                  +incrementing: true
                  #with: []
                  #withCount: []
                  +preventsLazyLoading: false
                  #perPage: 15
                  +exists: true
                  +wasRecentlyCreated: false
                  #escapeWhenCastingToString: false
                  #attributes: array:24 [
                    "id" => 1287880
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                    "field_branch_order" => null
                    "field_url" => null
                    "field_branch_type" => Illuminate\Database\Eloquent\Collection {#1191 …2}
                    "field_page_start" => "68"
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                    "field_display_branch_page" => "1"
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            "text" => "<p><strong>17.3.</strong> Найдите силу тока в колебательном контуре (см. задачу 17.2):</p><p><strong>а)</strong> через $t_1 = 0,31$ мкс после подключения батареи конденсаторов к катушке;</p><p><strong>б)</strong> в момент, когда напряжение на батарее конденсаторов $u = 100$ В.</p><p>Рассмотрите только случай параллельного соединения конденсаторов.</p>"
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            "text" => "<p><strong>Дано:</strong></p><p>Данные из задачи 17.2:</p><p>$L = 0,2$ мГн</p><p>$C_0 = 0,5$ мкФ (2 конденсатора)</p><p>$U_{max} = 200$ В</p><p>Данные из задачи 17.3:</p><p>Соединение конденсаторов – параллельное</p><p>$t_1 = 0,31$ мкс</p><p>$u = 100$ В</p><p><em>Перевод в систему СИ:</em></p><p>$L = 0,2 \times 10^{-3} \text{ Гн} = 2 \times 10^{-4}$ Гн</p><p>$C_0 = 0,5 \times 10^{-6}$ Ф</p><p>$t_1 = 0,31 \times 10^{-6}$ с</p><p><strong>Найти:</strong></p><p>а) $i_1$ - сила тока в момент времени $t_1$</p><p>б) $i_2$ - сила тока при напряжении $\text{u}$</p><p><strong>Решение:</strong></p><p>В идеальном колебательном контуре происходят гармонические колебания. Если в начальный момент времени ($t=0$) конденсатор полностью заряжен, то напряжение на нем и сила тока в катушке изменяются со временем по законам:</p><p>$u(t) = U_{max}\cos(\omega t)$</p><p>$i(t) = I_{max}\sin(\omega t)$</p><p>где $U_{max}$ – максимальное напряжение, $I_{max}$ – амплитудная сила тока, а $\omega$ – циклическая частота колебаний.</p><p>Сначала определим параметры контура для случая параллельного соединения конденсаторов.</p><p>Общая емкость $\text{C}$ батареи из двух параллельно соединенных конденсаторов равна сумме их емкостей:</p><p>$C = C_0 + C_0 = 2C_0 = 2 \times 0,5 \times 10^{-6} \text{ Ф} = 1 \times 10^{-6}$ Ф.</p><p>Циклическая частота колебаний $\omega$ в контуре определяется по формуле Томсона:</p><p>$\omega = \frac{1}{\sqrt{LC}} = \frac{1}{\sqrt{2 \times 10^{-4} \text{ Гн} \times 1 \times 10^{-6} \text{ Ф}}} = \frac{1}{\sqrt{2 \times 10^{-10} \text{ с}^2}} = \frac{10^5}{\sqrt{2}}$ рад/с.</p><p>Амплитудное значение силы тока $I_{max}$ найдем из закона сохранения энергии. Максимальная энергия электрического поля конденсатора переходит в максимальную энергию магнитного поля катушки:</p><p>$\frac{CU_{max}^2}{2} = \frac{LI_{max}^2}{2}$</p><p>$I_{max} = U_{max}\sqrt{\frac{C}{L}} = 200 \text{ В} \times \sqrt{\frac{1 \times 10^{-6} \text{ Ф}}{2 \times 10^{-4} \text{ Гн}}} = 200 \times \sqrt{0,5 \times 10^{-2}} = 200 \times \frac{1}{\sqrt{200}} = \frac{200}{10\sqrt{2}} = \frac{20}{\sqrt{2}} = 10\sqrt{2}$ А.</p><p><strong>а)</strong> Найдем силу тока в момент времени $t_1 = 0,31$ мкс.</p><p>Сила тока в этот момент времени $i_1$ равна:</p><p>$i_1 = i(t_1) = I_{max}\sin(\omega t_1)$.</p><p>Вычислим фазу колебаний $\phi = \omega t_1$:</p><p>$\phi = \omega t_1 = \frac{10^5}{\sqrt{2}} \text{ рад/с} \times 0,31 \times 10^{-6} \text{ с} = \frac{0,031}{\sqrt{2}} \approx 0,0219$ рад.</p><p>Так как фаза $\phi$ является малым углом ($\phi \ll 1$), можно использовать приближение $\sin(\phi) \approx \phi$.</p><p>$i_1 \approx I_{max} \cdot (\omega t_1) = (10\sqrt{2} \text{ А}) \times \left(\frac{0,031}{\sqrt{2}}\right) = 10 \times 0,031 \text{ А} = 0,31$ А.</p><p>Другой способ для малых $\text{t}$: в начальный момент времени напряжение на катушке равно $U_{max}$, и оно определяет скорость нарастания тока: $U_{max} = L\frac{di}{dt}$. Для малого промежутка времени $t_1$ можно считать, что ток нарастает линейно: $i_1 \approx \frac{di}{dt} \cdot t_1 = \frac{U_{max}}{L}t_1$.</p><p>$i_1 \approx \frac{200 \text{ В}}{2 \times 10^{-4} \text{ Гн}} \times 0,31 \times 10^{-6} \text{ с} = 10^6 \text{ А/с} \times 0,31 \times 10^{-6} \text{ с} = 0,31$ А.</p><p><strong>Ответ:</strong> $i_1 = 0,31$ А.</p><p><strong>б)</strong> Найдем силу тока $i_2$ в момент, когда напряжение на конденсаторах $u = 100$ В.</p><p>Воспользуемся законом сохранения энергии для колебательного контура. Полная энергия контура $\text{W}$ постоянна и равна сумме энергии электрического поля конденсатора $W_C$ и энергии магнитного поля катушки $W_L$.</p><p>$W = W_C + W_L = \frac{Cu^2}{2} + \frac{Li_2^2}{2}$</p><p>Полная энергия также равна максимальной энергии, запасенной в конденсаторе:</p><p>$W = \frac{CU_{max}^2}{2}$</p><p>Приравнивая эти выражения, получаем:</p><p>$\frac{CU_{max}^2}{2} = \frac{Cu^2}{2} + \frac{Li_2^2}{2}$</p><p>$CU_{max}^2 = Cu^2 + Li_2^2$</p><p>Выразим отсюда искомую силу тока $i_2$:</p><p>$Li_2^2 = C(U_{max}^2 - u^2)$</p><p>$i_2 = \sqrt{\frac{C}{L}(U_{max}^2 - u^2)}$</p><p>Подставим числовые значения:</p><p>$i_2 = \sqrt{\frac{1 \times 10^{-6} \text{ Ф}}{2 \times 10^{-4} \text{ Гн}} \times ((200 \text{ В})^2 - (100 \text{ В})^2)} = \sqrt{0,5 \times 10^{-2} \frac{\text{Ф}}{\text{Гн}} \times (40000 - 10000) \text{ В}^2}$</p><p>$i_2 = \sqrt{5 \times 10^{-3} \times 30000} \text{ А} = \sqrt{150} \text{ А} = \sqrt{25 \times 6} \text{ А} = 5\sqrt{6}$ А.</p><p>Вычислим приближенное значение:</p><p>$i_2 \approx 5 \times 2,449 \approx 12,25$ А.</p><p><strong>Ответ:</strong> $i_2 = 5\sqrt{6}$ А $\approx 12,25$ А.</p>"
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            "text" => "<p><strong>Дано:</strong></p><p>Данные из задачи 17.2:</p><p>$L = 0,2$ мГн</p><p>$C_0 = 0,5$ мкФ (2 конденсатора)</p><p>$U_{max} = 200$ В</p><p>Данные из задачи 17.3:</p><p>Соединение конденсаторов – параллельное</p><p>$t_1 = 0,31$ мкс</p><p>$u = 100$ В</p><p><em>Перевод в систему СИ:</em></p><p>$L = 0,2 \times 10^{-3} \text{ Гн} = 2 \times 10^{-4}$ Гн</p><p>$C_0 = 0,5 \times 10^{-6}$ Ф</p><p>$t_1 = 0,31 \times 10^{-6}$ с</p><p><strong>Найти:</strong></p><p>а) $i_1$ - сила тока в момент времени $t_1$</p><p>б) $i_2$ - сила тока при напряжении $\text{u}$</p><p><strong>Решение:</strong></p><p>В идеальном колебательном контуре происходят гармонические колебания. Если в начальный момент времени ($t=0$) конденсатор полностью заряжен, то напряжение на нем и сила тока в катушке изменяются со временем по законам:</p><p>$u(t) = U_{max}\cos(\omega t)$</p><p>$i(t) = I_{max}\sin(\omega t)$</p><p>где $U_{max}$ – максимальное напряжение, $I_{max}$ – амплитудная сила тока, а $\omega$ – циклическая частота колебаний.</p><p>Сначала определим параметры контура для случая параллельного соединения конденсаторов.</p><p>Общая емкость $\text{C}$ батареи из двух параллельно соединенных конденсаторов равна сумме их емкостей:</p><p>$C = C_0 + C_0 = 2C_0 = 2 \times 0,5 \times 10^{-6} \text{ Ф} = 1 \times 10^{-6}$ Ф.</p><p>Циклическая частота колебаний $\omega$ в контуре определяется по формуле Томсона:</p><p>$\omega = \frac{1}{\sqrt{LC}} = \frac{1}{\sqrt{2 \times 10^{-4} \text{ Гн} \times 1 \times 10^{-6} \text{ Ф}}} = \frac{1}{\sqrt{2 \times 10^{-10} \text{ с}^2}} = \frac{10^5}{\sqrt{2}}$ рад/с.</p><p>Амплитудное значение силы тока $I_{max}$ найдем из закона сохранения энергии. Максимальная энергия электрического поля конденсатора переходит в максимальную энергию магнитного поля катушки:</p><p>$\frac{CU_{max}^2}{2} = \frac{LI_{max}^2}{2}$</p><p>$I_{max} = U_{max}\sqrt{\frac{C}{L}} = 200 \text{ В} \times \sqrt{\frac{1 \times 10^{-6} \text{ Ф}}{2 \times 10^{-4} \text{ Гн}}} = 200 \times \sqrt{0,5 \times 10^{-2}} = 200 \times \frac{1}{\sqrt{200}} = \frac{200}{10\sqrt{2}} = \frac{20}{\sqrt{2}} = 10\sqrt{2}$ А.</p><p><strong>а)</strong> Найдем силу тока в момент времени $t_1 = 0,31$ мкс.</p><p>Сила тока в этот момент времени $i_1$ равна:</p><p>$i_1 = i(t_1) = I_{max}\sin(\omega t_1)$.</p><p>Вычислим фазу колебаний $\phi = \omega t_1$:</p><p>$\phi = \omega t_1 = \frac{10^5}{\sqrt{2}} \text{ рад/с} \times 0,31 \times 10^{-6} \text{ с} = \frac{0,031}{\sqrt{2}} \approx 0,0219$ рад.</p><p>Так как фаза $\phi$ является малым углом ($\phi \ll 1$), можно использовать приближение $\sin(\phi) \approx \phi$.</p><p>$i_1 \approx I_{max} \cdot (\omega t_1) = (10\sqrt{2} \text{ А}) \times \left(\frac{0,031}{\sqrt{2}}\right) = 10 \times 0,031 \text{ А} = 0,31$ А.</p><p>Другой способ для малых $\text{t}$: в начальный момент времени напряжение на катушке равно $U_{max}$, и оно определяет скорость нарастания тока: $U_{max} = L\frac{di}{dt}$. Для малого промежутка времени $t_1$ можно считать, что ток нарастает линейно: $i_1 \approx \frac{di}{dt} \cdot t_1 = \frac{U_{max}}{L}t_1$.</p><p>$i_1 \approx \frac{200 \text{ В}}{2 \times 10^{-4} \text{ Гн}} \times 0,31 \times 10^{-6} \text{ с} = 10^6 \text{ А/с} \times 0,31 \times 10^{-6} \text{ с} = 0,31$ А.</p><p><strong>Ответ:</strong> $i_1 = 0,31$ А.</p><p><strong>б)</strong> Найдем силу тока $i_2$ в момент, когда напряжение на конденсаторах $u = 100$ В.</p><p>Воспользуемся законом сохранения энергии для колебательного контура. Полная энергия контура $\text{W}$ постоянна и равна сумме энергии электрического поля конденсатора $W_C$ и энергии магнитного поля катушки $W_L$.</p><p>$W = W_C + W_L = \frac{Cu^2}{2} + \frac{Li_2^2}{2}$</p><p>Полная энергия также равна максимальной энергии, запасенной в конденсаторе:</p><p>$W = \frac{CU_{max}^2}{2}$</p><p>Приравнивая эти выражения, получаем:</p><p>$\frac{CU_{max}^2}{2} = \frac{Cu^2}{2} + \frac{Li_2^2}{2}$</p><p>$CU_{max}^2 = Cu^2 + Li_2^2$</p><p>Выразим отсюда искомую силу тока $i_2$:</p><p>$Li_2^2 = C(U_{max}^2 - u^2)$</p><p>$i_2 = \sqrt{\frac{C}{L}(U_{max}^2 - u^2)}$</p><p>Подставим числовые значения:</p><p>$i_2 = \sqrt{\frac{1 \times 10^{-6} \text{ Ф}}{2 \times 10^{-4} \text{ Гн}} \times ((200 \text{ В})^2 - (100 \text{ В})^2)} = \sqrt{0,5 \times 10^{-2} \frac{\text{Ф}}{\text{Гн}} \times (40000 - 10000) \text{ В}^2}$</p><p>$i_2 = \sqrt{5 \times 10^{-3} \times 30000} \text{ А} = \sqrt{150} \text{ А} = \sqrt{25 \times 6} \text{ А} = 5\sqrt{6}$ А.</p><p>Вычислим приближенное значение:</p><p>$i_2 \approx 5 \times 2,449 \approx 12,25$ А.</p><p><strong>Ответ:</strong> $i_2 = 5\sqrt{6}$ А $\approx 12,25$ А.</p>"
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№17.3 (с. 105)
Условие. №17.3 (с. 105)
скриншот условия
Физика, 8-11 класс Учебник, задачник, авторы: Гельфгат Илья Маркович, Генденштейн Лев Элевич, Кирик Леонид Анатольевич, издательство Илекса, Москва, 2005, страница 105, номер 17.3, Условие

17.3. Найдите силу тока в колебательном контуре (см. задачу 17.2):

а) через $t_1 = 0,31$ мкс после подключения батареи конденсаторов к катушке;

б) в момент, когда напряжение на батарее конденсаторов $u = 100$ В.

Рассмотрите только случай параллельного соединения конденсаторов.

Решение. №17.3 (с. 105)
Физика, 8-11 класс Учебник, задачник, авторы: Гельфгат Илья Маркович, Генденштейн Лев Элевич, Кирик Леонид Анатольевич, издательство Илекса, Москва, 2005, страница 105, номер 17.3, Решение
Решение 2. №17.3 (с. 105)

Дано:

Данные из задачи 17.2:

$L = 0,2$ мГн

$C_0 = 0,5$ мкФ (2 конденсатора)

$U_{max} = 200$ В

Данные из задачи 17.3:

Соединение конденсаторов – параллельное

$t_1 = 0,31$ мкс

$u = 100$ В

Перевод в систему СИ:

$L = 0,2 \times 10^{-3} \text{ Гн} = 2 \times 10^{-4}$ Гн

$C_0 = 0,5 \times 10^{-6}$ Ф

$t_1 = 0,31 \times 10^{-6}$ с

Найти:

а) $i_1$ - сила тока в момент времени $t_1$

б) $i_2$ - сила тока при напряжении $\text{u}$

Решение:

В идеальном колебательном контуре происходят гармонические колебания. Если в начальный момент времени ($t=0$) конденсатор полностью заряжен, то напряжение на нем и сила тока в катушке изменяются со временем по законам:

$u(t) = U_{max}\cos(\omega t)$

$i(t) = I_{max}\sin(\omega t)$

где $U_{max}$ – максимальное напряжение, $I_{max}$ – амплитудная сила тока, а $\omega$ – циклическая частота колебаний.

Сначала определим параметры контура для случая параллельного соединения конденсаторов.

Общая емкость $\text{C}$ батареи из двух параллельно соединенных конденсаторов равна сумме их емкостей:

$C = C_0 + C_0 = 2C_0 = 2 \times 0,5 \times 10^{-6} \text{ Ф} = 1 \times 10^{-6}$ Ф.

Циклическая частота колебаний $\omega$ в контуре определяется по формуле Томсона:

$\omega = \frac{1}{\sqrt{LC}} = \frac{1}{\sqrt{2 \times 10^{-4} \text{ Гн} \times 1 \times 10^{-6} \text{ Ф}}} = \frac{1}{\sqrt{2 \times 10^{-10} \text{ с}^2}} = \frac{10^5}{\sqrt{2}}$ рад/с.

Амплитудное значение силы тока $I_{max}$ найдем из закона сохранения энергии. Максимальная энергия электрического поля конденсатора переходит в максимальную энергию магнитного поля катушки:

$\frac{CU_{max}^2}{2} = \frac{LI_{max}^2}{2}$

$I_{max} = U_{max}\sqrt{\frac{C}{L}} = 200 \text{ В} \times \sqrt{\frac{1 \times 10^{-6} \text{ Ф}}{2 \times 10^{-4} \text{ Гн}}} = 200 \times \sqrt{0,5 \times 10^{-2}} = 200 \times \frac{1}{\sqrt{200}} = \frac{200}{10\sqrt{2}} = \frac{20}{\sqrt{2}} = 10\sqrt{2}$ А.

а) Найдем силу тока в момент времени $t_1 = 0,31$ мкс.

Сила тока в этот момент времени $i_1$ равна:

$i_1 = i(t_1) = I_{max}\sin(\omega t_1)$.

Вычислим фазу колебаний $\phi = \omega t_1$:

$\phi = \omega t_1 = \frac{10^5}{\sqrt{2}} \text{ рад/с} \times 0,31 \times 10^{-6} \text{ с} = \frac{0,031}{\sqrt{2}} \approx 0,0219$ рад.

Так как фаза $\phi$ является малым углом ($\phi \ll 1$), можно использовать приближение $\sin(\phi) \approx \phi$.

$i_1 \approx I_{max} \cdot (\omega t_1) = (10\sqrt{2} \text{ А}) \times \left(\frac{0,031}{\sqrt{2}}\right) = 10 \times 0,031 \text{ А} = 0,31$ А.

Другой способ для малых $\text{t}$: в начальный момент времени напряжение на катушке равно $U_{max}$, и оно определяет скорость нарастания тока: $U_{max} = L\frac{di}{dt}$. Для малого промежутка времени $t_1$ можно считать, что ток нарастает линейно: $i_1 \approx \frac{di}{dt} \cdot t_1 = \frac{U_{max}}{L}t_1$.

$i_1 \approx \frac{200 \text{ В}}{2 \times 10^{-4} \text{ Гн}} \times 0,31 \times 10^{-6} \text{ с} = 10^6 \text{ А/с} \times 0,31 \times 10^{-6} \text{ с} = 0,31$ А.

Ответ: $i_1 = 0,31$ А.

б) Найдем силу тока $i_2$ в момент, когда напряжение на конденсаторах $u = 100$ В.

Воспользуемся законом сохранения энергии для колебательного контура. Полная энергия контура $\text{W}$ постоянна и равна сумме энергии электрического поля конденсатора $W_C$ и энергии магнитного поля катушки $W_L$.

$W = W_C + W_L = \frac{Cu^2}{2} + \frac{Li_2^2}{2}$

Полная энергия также равна максимальной энергии, запасенной в конденсаторе:

$W = \frac{CU_{max}^2}{2}$

Приравнивая эти выражения, получаем:

$\frac{CU_{max}^2}{2} = \frac{Cu^2}{2} + \frac{Li_2^2}{2}$

$CU_{max}^2 = Cu^2 + Li_2^2$

Выразим отсюда искомую силу тока $i_2$:

$Li_2^2 = C(U_{max}^2 - u^2)$

$i_2 = \sqrt{\frac{C}{L}(U_{max}^2 - u^2)}$

Подставим числовые значения:

$i_2 = \sqrt{\frac{1 \times 10^{-6} \text{ Ф}}{2 \times 10^{-4} \text{ Гн}} \times ((200 \text{ В})^2 - (100 \text{ В})^2)} = \sqrt{0,5 \times 10^{-2} \frac{\text{Ф}}{\text{Гн}} \times (40000 - 10000) \text{ В}^2}$

$i_2 = \sqrt{5 \times 10^{-3} \times 30000} \text{ А} = \sqrt{150} \text{ А} = \sqrt{25 \times 6} \text{ А} = 5\sqrt{6}$ А.

Вычислим приближенное значение:

$i_2 \approx 5 \times 2,449 \approx 12,25$ А.

Ответ: $i_2 = 5\sqrt{6}$ А $\approx 12,25$ А.

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