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Образ= ец заголовка
Образец текста
Второй уровень
Третий уровень
Четверты= 081; уровень
Пятый уровень
‹дата/вр= 077;мя›
‹ниж&= #1085;ий колонтитул̹= 0;
‹#›
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Неоптолем= еевская меm= 3;аника
=
механика эры космоса
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Языки механики
<= span class=3DBB style=3D'position:absolute;left:-4.43%'>•Н&#= 1100;ютоновский
<= span class=3DBB style=3D'position:absolute;left:-4.43%'>•Л&#= 1072;гранжев
<= span class=3DBB style=3D'position:absolute;left:-4.43%'>•П&#= 1091;анкаре
<= span class=3DBB style=3D'position:absolute;left:-4.43%'>•Г&#= 1072;мильтонов
•И другие язык= 080; аналитичес = 82;ой динамики
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Н&= #1086;вое время требует новой механики
•Век космонавти = 82;и требует перехода от нынешней коперникиа = 85;ской механики с выделенным = 80;, главными системами отсчета к неоптолеме = 77;вской, в которой любой наблюдател = 00; есть центр вселенной, любая система отсчета хороша, законы механики формулирую= 090;ся для любой, произвольн= 086;й системы отсчета
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Три принципа новой механики
<= span class=3DBB style=3D'position:absolute;left:-4.39%'>•Р&#= 1072;вноправие всех систем отсчета
•Г&#= 1088;авитация не взаимодейс = 90;вие (концепци= 103; Ньютона), а изменение свойств пространст = 74;а (концепция Эйнштейна) •Н&#= 1077; сила, а механическ = 86;е состояние (весомость) есть фундамента = 83;ьная механиче = 89;кая характерис = 90;ика
<= span style=3D'visibility:hidden'>•
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Принц&= #1080;п эквивалент = 85;ости
•В гравитацио = 85;ном пространст = 74;е движение = свободных тел отлично от равномk= 7;рного и прямолиней = 85;ого аналогич = 85;о движению свободных тел в неиl= 5;ерциальной системе отсчета. Гравитацио = 85;ные силы как и силы инерц&= #1080;и фиктивны. Третий зако= 085; Ньютона к гравитации не имеет отношения. Всемирный закон тяготения неверен.
<= span style=3D'visibility:hidden'>•
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Что есть гравитация
•<= /span>Гравитация есть област= 100; измененног = 86; пространст= 074;а вокруг тяготеющег = 86; тела, гра = 74;итационная аура, в котором другие своk= 3;одные тела движутся не равномерно и прямолиней = 85;о, а более слоk= 8;ным образом. Тела, гра = 74;итационные ауры которы= 093; пересека = 02;тся, находятся в гравитацио = 85;ном контакте, оставаясь = свободными. Гравитацио = 85;ные ауры аддит&= #1080;вны. Они неизменны при неизм&= #1077;нности тел.
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ЗАКОН&#= 1067; НЕОПТОЛЕ = 52;ЕЕВСКОЙ МЕХАНИКИ
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З= акон движения в негравитац = 80;онном прос&#= 1090;ранстве в инерциальн = 86;й системе отсчета<= /span>
&nb= sp;w − ускорение; <= /span>W − весомость, Н/кг.
    Закон механическ = 86;го состояния
Закон взаимодейс = 90;вия
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Систе&#= 1084;а отсчета
•<= span style=3D'font-size:114%'>Система отсчета использует = 89;я ньют&= #1086;новская на основе абсолютно твердог= о тела (АТТ). Общая ее характе= ристика − угловая скорость вращени= я Ώ. Микрохарак = 90;еристика есть весомость е= 077; элементов − тел l= 6;тсчета. Распределе = 85;ие весомости B(r) опис&= #1099;вает весомостно = 77; поле.
•
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Весомостно&#= 1077; поле H галилеева прос= 090;ранства в неинерциал = 00;ной сист= 077;ме отсчета
<= span class=3DHBB style=3D'position:absolute;left:-5.06%'>•i= 5;оле ускорений АТТ
<= span style=3D'visibility:hidden'>•
Задают = 89;я начальные (а не &#= 1075;раничные) условия. Принци = 87;иальное отличие от электр = 86;магнитного поля
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Весомостно = 77; поле V гравитацио= нного пространст = 74;а в
Начало системы отсчета связано со свободн= ым, невесомым объектом, т.е. с лю&= #1073;ым свободным телом в гравитацио = 85;ном поле<= /span>.
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В&= #1077;сомостное поле B
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Уравнение движения в неинерц&= #1080;альной системе отсчета в негравитац = 80;онном прос= 090;ранстве
–Из уравнение Кориолиса
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Уравнение движения = произво&= #1083;ьного тела в произвольн&#= 1086;м пространст = 74;е в прl= 6;извольной системе отсчета
В заданном пространст = 74;е в заданной системе отсчета движение зависит только от состоян= ия. Движение всех свободных тел а= ;втомодельн = 86; и определяет = 89;я исключител = 00;но нача&= #1083;ьными условиями.
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Весом&#= 1080;ка
•Новый раздел механики, изучающий механич&= #1077;ское состояние объектов. = Примене&= #1085;ие – в медицине, в космонавти = 82;е, при конструиро = 74;ании и эксплуатац = 80;и тран= 089;портных средств − самолетов, кораблей и т.д., разработка аттракцион = 86;в, расчеты на прочнос&= #1090;ь динамическ = 80;х конструкци = 81;, спорт и <= span style=3D'font-size:88%'>т.д. Аналог статики ньютоновск = 86;й механики. = •Констру&= #1080;рование весомометр = 86;в, весо= 084;оизмерител&= #1100;ные органы чувств живы= 093; суще= 089;тв и человека, использова = 85;ие в на = 74;игационных целях.
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Гравитацио&= #1085;ное поле нескольких = тел
Напряже= нность гравитацио = 85;ного поля в системе многих (n+1) с= ;вободных тел на самих телах в невращающе = 81;ся системе отсчета, связанной с одним из тел.<= /span>
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i= 8;очные решения задачи многих тел
•<= /span>Они могут быть легко найдены, если вторая = скобка обращается = 074; нуль. Это возможно:
•<= /span>В конфигурац = 80;ях с равными расстояния = 84;и межд= 091; телами при любых массах. Таких конфигурац&#= 1080;й три – линейная, треугольни = 82;, тетр= 072;эдр.
•<= /span>В симметричн = 99;х конфигурац = 80;ях при р= авенстве масс. Симметричн = 99;х конф= 080;гураций существует бесконечно = 77; число линейных, плоских и пространст = 74;енных. Полу= 095;аем огромное число точны= 093; решений с = любым количество = 84; тел как финитных, так и инфинитных.=   
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Метод динамическ = 80;х систем отсчета состоит в использова = 85;ия систем отсчета, характерис = 90;ики которых = являютс= я переменным = 80; задачи
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Ориента= ция систем отсчета в задачах 1, 2, 3 и 4-х= ; тел. Хара&= #1082;теристикам= ;и системы отсчета являются угловая скорост= ь вращения W= (t) и значе&= #1085;ие весом&= #1086;стного поля начала системы отсчета B0(t), равное весомости тела начала системы отсчета W0.
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ПРОСТ&#= 1045;ЙШИЕ ЗАДАЧИ
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Самая простая
•От= 085;осительное движение двух свободных тела в негравитац = 80;онном пространст = 74;е
Задача о
радиолока = 90;оре
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•<= span style=3D'font-size:86%'>Задача Кеплера дву= 093; гравитирую = 97;их тел. Одно тело выбираем в качестве начала системы отсчета. На <= /span>второе направляем ось Оx. Задача одномерная. Перемен&= #1085;ые: координата x1 и угловая скорость Ώ= ; k= 4;доль оси Oz. Уравнения
Решение есть плоско= 077; коническое сечение с парамет= ром равным сумм= 077; масс. Но есть и иное неизвестно= е решение в прецессиру = 02;щей плоскости.
Эксперимен= тальное подтвержде = 85;ие − прецессия плоскос= ти земной орбиты.
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Д= вухчастичнm= 9;й росциллято = 88;
•Дву= ;хчастичный осциллятор, могущий = свободно вращаться. Одну из частиц 0 св= 103;зываем с началом системы отсчета. = Переменные - расстояние и скорость вращения.
<= span style=3D'visibility:hidden'>•
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Антир&#= 1077;зонансы
•При= ; Ώ=3Dω0 росци= ;ллятор превращает = 89;я в твердую частицу, осцилляцио = 85;ные и вращатель = 85;ые степени свободы заl= 4;ораживаютс= 103;. Исчезает поглощение свk= 7;та. Антирезона = 85;сное состояние есть област = 00; прозрачнос = 90;и. Можно исслеk= 6;овать многочасти = 95;ные росциллято = 88;ы и их полосы прозрачнос = 90;и. Решение проблем теплоемкос = 90;и газов.
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Развернуто = 77; уравнение = движени&= #1103;
Уравнение по другим координата = 84; получается = цикличе= ской перестанов = 82;ой.
Получающее= ся уравнение н= 072; первый взля= 076; нево&#= 1086;бразимо сложнее ньютоновск = 86;го F=3Dmw. <= /div>
Но в конкретны= 093; приложения = 93; оно зачасту= 102; оказ&#= 1099;вается значительн = 86; эффективне = 81; ньютоно= вского.
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= Заk= 6;ача трех тел. Одно движение одномерно, в&#= 1090;орое = – двухмерно. Размерност = 00; 6, ранг 9.
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Плоская ограниченн = 72;я задача = трех тел − теория Луны
•Если принять за нулевое тел= 086; Землю, за = первое − Солнце с заданным заранее характе&= #1088;ом движения Ώ= ;(t), то система = l= 9;водится к двум уравнения ранга 4. Эта l= 9;истема допускает дальнейшее упрощение = l= 7;ри учете, что r2<<r1. <= span style=3D'font-size:88%'> Все данные и перемен&= #1085;ые непосредст = 74;енно наблюдаемы = 77; = величин&= #1099;, и она может прямо численно рассчит&= #1099;ваться, ни в каких искусствен = 85;ых прео= 073;разованиях нужды нет. <= /div>
------=_NextPart_01C93BA5.211FE1F0 Content-Location: file:///C:/8D437683/file8707.files/slide0025.htm Content-Transfer-Encoding: quoted-printable Content-Type: text/html; charset="us-ascii" Неоптолемk= 7;евская механика −
Новое состояние вещества
•Взрыв распростра = 85;енное состояние = веществ&= #1072;. Но в ньютоновск = 86;й механике не= 090; инст= 088;ументов их исследован = 80;я, и взрывные = процесс&= #1099; лежат вне пределов механическ = 86;й теор= 080;и. Новая механика имеет такие = инструм&= #1077;нты и целый крупный раздел механик&= #1080; посвящен теории взрывных = процесс&= #1086;в. = •Теорети&= #1095;еский инструмент = 722; однородные нестаци&= #1086;нарные среды (ОНС).=
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ОНС
<= span class=3DHBB style=3D'position:absolute;left:-4.55%'>•Н&= #1086;вый принцип однороднос = 90;и среды:
•С&#= 1088;еда является однородной, если все = наблюдателl= 0;, связанные с ее элементами, видят ее одинаково.
•М&#= 1077;ханические условия однороднос = 90;и среды:
•1. Материальн = 72;я
•2. Кинематиче = 89;кая
•3. Динамическ = 72;я
•H называ = 77;тся хабблиан. Все характерис = 90;ики = ОНС заключены в зависимост = 03;х ρ(t) и H(t). А во вращающихс = 03; ОНС в Ώ(= t).
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Типы ОНС
•По типу ОНС делятся на негравитир = 91;ющие и гравитl= 0;рующие. •П&#= 1086; размерност = 80; одномерные прецессиру= 102;щие, двухмерные вращающиес = 03; и трехмерные = ;
<= span class=3DBB style=3D'position:absolute;left:-3.47%'>•П&#= 1086; симметрии изотропные = 080; неизотропн = 99;е
•О&#= 1076;номерные и двухмерны= 077; гравитирую = 97;ие ОНС могут иметь стационарн = 99;е и пульсиl= 8;ующие решения.
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Испол= ;ьзование моделей ОНС
•ОНС могут быть моделью различных природных феноменов и процессов •Н&#= 1077;гравитирую= щие трехмерные = 722; взрыва ВВ= 3;•Д&#= 1074;ухмерные − разрыва вращающего = 89;я маховика = ;= •О= 076;номерные − стрельбы из стволового оружия
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•Гра= ;витирующие трехмерные = 722; взрывов звезд и космологич = 77;ских процессов − модель Хаббла-Милн= 072;
<= span class=3DBB style=3D'position:absolute;left:-3.92%'>•Д&#= 1074;ухмерные стационарн = 99;е − галактик
<= span class=3DBB style=3D'position:absolute;left:-3.89%'>•П&#= 1091;льсирующие − пульсирующ = 80;х звезд
•О&#= 1076;номерные стационарн = 99;е − солнечl= 5;ых систем
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Негра&#= 1074;итационные ОНС
<= span class=3DHBB style=3D'position:absolute;left:-15.74%'>•У= равнение
= •
= •Р= ешение
= •
<= span class=3DHBB style=3D'position:absolute;left:-15.74%'>•У= равнения
= •
= •
= •Р= ешения
&= #1058;рехмерная <= /b>
Скорость фронта взрыва=
Двухме = 88;ная
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file:///C:/8D437683/file8707.files/slide0033.htm Content-Transfer-Encoding: quoted-printable Content-Type: text/html; charset="us-ascii" Неоптолемk= 7;евская механика −
i= 5;ланарная гравитацио = 85;ная ОНС
Стацион= арное решение
 
Это решение может явиться модель = 02; галактики=
Существуе = 90; осцилляцио = 85;ное решение вбл= 080;зи сm= 0;ационарног= 086; состояния. Данное решение мож= 077;т ст= ;ать моделью переменных звезд − цефеид.
Струйная (одномерная) гравитирую = 97;ая ОНС в прецессир = 91;ющей системе отсчета также имеет стацио = 85;арное решение, которое может стать модель = 02; солнечной системы.
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Космическа= я меха&= #1085;ика (меха= ника космическо = 75;о поле&= #1090;а)
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Системы отсчета в космическо = 84; = полете<= /span>
•<= /span>В навигации космическо = 75;о полета = использ&= #1091;ется большое количество систем = отсчета − система стартового стола, систе&#= 1084;а Цент= 088;а Земли, система стыкуемого корабля, солнечн&= #1072;я система, система центра Луны, <= /span>система отсчета места посадки на Луне и т.д.
•<= /span>Все это создает сложности перехода из одной системы отсчета в другую.
•<= /span>В неоптолеме = 77;вской механике можно иметь единую универсаль = 85;ую систему отсчета − = систему отсчета космическо = 75;о корабля.
•
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1.Ме&#= 1093;аника запуска КА.
Рассмотрен = 99; задачи запуска. Предложены = 080; проанализи = 88;ованы некоторые схk= 7;мы, определяем = 99;е программам = 80; весомости W(t) и угла разворота j(t). Введено понятие интегральн = 86;й весомости P и к.п.д. K схемы запуска,
Рассмотр&#= 1077;на задача нахождения схемы вывед= 077;ния, минимизиру = 02;щей интегральн = 91;ю весомость, и нахождения орбиты, на которой достигаетс = 03; маl= 2;симум K. Показано, что такой орбитой является орбита с высотой около 650 км и максимальн = 99;й к.п.д. равен 0.725. Весомость р= 072;вна 3.2 G (земной), а угол разворота двигателя 133= °. Возможно она окажетс= 103; полезной в качестве к прl= 6;межуточной при запуске на высокие и далекие орбиты.
Рассмотр&#= 1077;на схема двухстадий = 85;ого запуска на круговую орбиту (с веl= 8;тикальным стартом): первая стадия – вых&#= 1086;д на орбиту, вторая – орk= 3;итальный разгон до космическо = 81; скорости.
Думается, что теоретичес = 82;ие предельные = 101;ффективнос&= #1090;и могут оказаться стl= 6;ль же полезным= 080; в космонавти = 82;е, как таковые же в термодинам = 80;ке и теплоэне&#= 1088;гетике.
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2. Орбитальна = 03; механика
В орбитальну = 02; механику входит:
А) Движение по малоэллипт = 80;чным орбитам. Упр&#= 1086;щенная теория. Орбиты опl= 0;сываются угловыми скоростями круговых орбит, касающихся апl= 9;идальных точек.
w1 = ;
w2=3D w1-L
 j=
B) Опl= 8;еделение параметров орk= 3;итального движения по авm= 0;ономным наблюдения = 84; с КК.
С) Маневриров = 72;ние на орбите с <= /span>поl= 4;ощью импульсных воздействи = 81; и двигател&#= 1077;й малой тяги. Стыковка.
D) Идентифи&#= 1082;ация орбит.
Е) Орбитальны = 77; возмущения ввиду несферич&#= 1085;ости гравитацио = 85;ного поля, остаточн&#= 1086;й атмосферы и др.
F) Изl= 4;ерения на орбите: массы тел и самого корабля, центра и моl= 4;ентов инерции и т.п.=
Орб= ;ита
Зем= ;ля
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Будущее космонавти = 82;и.
Освоение Солнечной системы с помощью вес= 086;мой космонавти = 82;и, т.е. при работе = двига= ;телей в течение всего полета.
В таблице указаны времена прямолиней = 85;ого полета на различные тела Солнечной систе= ;мы с переворото = 84; двигателей = 074; середине полета при различной весомости.
30 = 095;.
180
150
120
15
14
Время в сутках при <= /span>W=3D0.1 Гл
3 = 95;.
18
15
12
1.5
1.4
В= ремя в сутках при <= /span>W=3D10 Гл
300000 км
39
29
18
0.5
0.3
Р= асстояние в а.е.
Л= ;уна
П= лутон
Н= ептун
У= ран
М= арс
Венер<= span style=3D'font-size:57%'>а
Планеты
Сол= ;нце
Зем= ;ля
Неп= ;тун
Пло= ;скость эклиптики
Схе= ;ма внеэклипти = 95;еского циклоидаль = 85;ого полета
(дительно&#= 1089;ть на 20% превышает прямолиней = 85;ый)
Очk= 7;нь далекое будущее – освоение новых звезд= 085;ых систем и гаl= 3;актик. Средство перемещени = 03; – планеты ил&#= 1080; их спутники. <= /span>Длl= 0;тельность полетов – сотни и тысячи лет
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