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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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Заключен= ;ие. &#= 1056;абота над новым языком механики велась боле= 077; тридцати лет. Я являюсь учеником академиков Л.Ландау и <= span style=3D'position:absolute;top:16.0%;left:4.3%;width:99.81%;height:5.25%'>= П.К = 72;пицы. В силу обстоятель = 89;тв был лишен во&#= 1079;можности работать на переднем уровне наук= 080; и потому пришлось заняться ее основами, фундаменто = 84;.
Эти материалы в обсуждалис = 00; или рассказ= 099;вались Таргу, Седову, Ишлинскому, Раушенбаху, Легостаеву, Токарю, Алl= 0;фанову, Журавлеву, Караску,  Гребk= 7;никову, Сереброву, Трk= 7;щеву, докладывал = 72;сь на IV Съезде механиков в Киеве, в ГАh= 8;Ше, МАИ, ИМ МГУ, а Краснодарс = 82;ом университе = 90;е, на кафедрах механики  МФТИ, МГУ и пр..
телефон <= span style=3D'font-family:"Times New Roman";font-size:133%'>8-926-314-9817, e-mail= : vlad@yur.= ru, web<= /span>: www.yur.ru <= /b>
Благодар= ;ю за внимание и терпение.
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sld.filters.revealtrans ) setTimeout( "document.body.start()", sld.filters.revealtrans.duration * = 1000 ); else document.body.start(); } } function MakeSldVis()=20 { var fTrans=3Dg_showAnimation && SldHasTrans() if( fTrans )=09 { if( g_bgSound ) { idx=3Dg_bgSound.indexOf(","); pptSound.src=3Dg_bgSound.substr( 0, idx ); pptSound.loop=3D -(parseInt(g_bgSound.substr(idx+1))); } SlideObj.filters.revealtrans.Apply()=09 } SlideObj.style.visibility=3D"visible" if( fTrans ) SlideObj.filters.revealtrans.Play() } function MakeNotesVis()=20 { if( !IsNts() ) return false=20 SlideObj.style.display=3D"none" nObj =3D document.all.item("NotesObj") parent.SetHasNts(0) if( nObj ) {=20 nObj.style.display=3D"" parent.SetHasNts(1) } return 1 } function ChkAutoAdv() { if(SldHasTrans()) SlideObj.onfilterchange=3DAutoAdv else AutoAdv() } function AutoAdv() { if(!IsWin("PPTSld") || !gUseSldTimings )return var sld=3DGetCurSld() if( (sld.mAdvDelay>0) && !parent.IsFramesMode() ) setTimeout("parent.GoToNextSld()",sld.mAdvDelay) } function GetObj(id) { if(g_supportsPPTHTML) return document.all(id); else return document.getElementById(id); } function SldHasTrans() { return SlideObj.style.filter !=3D ""; } function GetSldId() { return sId=3Dlocation.href.substring(location.href.la= stIndexOf('/')+1) } function HideMenu() { if( frames["PPTSld"] && PPTSld.document.all.item("ctx= tmenu") && PPTSld.ctxtmenu.style.display!=3D"none" ) { PPTSld.ctxtmenu.styl= e.display=3D'none'; return true } return false } function IsWin( name ) { return window.name =3D=3D name } function IsNts() { return IsWin("PPTNts") } function IsSldOrNts() { return( IsWin("PPTSld")||IsWin("PPTNts") ) } function SupportsPPTAnimation() { return( navigator.platform =3D=3D "Win32"= && navigator.appVersion.indexOf("Windows")>0 ) } function SupportsPPTHTML() { var appVer=3Dnavigator.appVersion, msie=3DappVer.indexOf("MSIE "), ver=3D0 if( msie >=3D 0 ) ver=3DparseFloat( appVer.substring( msie+5, appVer.indexOf(";",msie) ) ) else ver=3DparseInt(appVer) return( ver >=3D 4 && msie >=3D 0 ) } function _RSW() { if( !g_supportsPPTHTML || IsNts() || ( !g_scaleInFrame && (!IsWin("PPTSld") || !parent.IsFullScrMode()) ) ) return var padding=3D0; if( IsWin("PPTSld") && parent.IsFramesMode() ) padding=3D6 cltWidth=3Ddocument.body.clientWidth-padding cltHeight=3Ddocument.body.clientHeight-padding factor=3D(1.0*cltWidth)/g_origW if( cltHeight < g_origH*factor ) factor=3D(1.0*cltHeight)/g_origH newSize =3D g_origSz * factor if( newSize < 1 ) newSize=3D1 s=3DSlideObj.style s.fontSize=3DnewSize+"px" s.posWidth=3Dg_origW*factor s.posHeight=3Dg_origH*factor s.posLeft=3D(cltWidth-s.posWidth+padding)/2 s.posTop=3D(cltHeight-s.posHeight+padding)/2 if( g_scaleHyperlinks ) ScaleHyperlinks( factor ) } function _InitAnimations() { animRuntimeInstalled =3D ''+document.body.localTime !=3D 'undefined'; isFullScreen =3D (window.name =3D=3D "PPTSld") && !parent.IsFramesMode(); g_animUseRuntime =3D g_showAnimation && animRuntimeInstalled && !(isFullSc= reen && parent.IsSldVisited()); if( g_animUseRuntime ) { collSeq =3D document.all.tags("seq"); if( collSeq !=3D null ) { for(ii=3D0;ii numSlds ) gSldJumpIdx =3D numSlds; if ( gSldJumpIdx >=3D 0 ) { if ( gSldJumpIdx =3D=3D 0 ) gSldJumpIdx =3D 1; var jumpTo =3D parseInt(gSldJumpIdx); gSldJump =3D 0; gSldJumpIdx =3D ""; win.GoToSld( parent.GetSldList().mList[jumpTo-1].mSldHref ) } } } function _KDH() { if( event.keyCode =3D=3D 8 ) { event.returnValue =3D 0; parent.GoToPrevSld(); } } function DocumentOnClick() { if( IsNts() || parent.HideMenu() ) return; if( ( g_allowAdvOnClick && !parent.IsFramesMode() ) || (event && (event.keyCode=3D=3D32) ) ) parent.GoToNextSld(); } var g_supportsPPTHTML =3D SupportsPPTHTML(), g_scaleInFrame =3D 1, gId=3D""= , g_bgSound=3D"", g_scaleHyperlinks =3D false, g_allowAdvOnClick =3D 1, g_showInBrowser = =3D 0, gLoopCont =3D 0, gUseSldTimings =3D 1; var g_showAnimation =3D g_supportsPPTHTML && SupportsPPTAnimation() && ( (w= indow.name=3D=3D"PPTSld" && !parent.IsFramesMode()) || g_showInBrowser );va= r g_animManager =3D null; var g_animUseRuntime =3D false; var g_animItemsToHide, g_animInteractiveItems, g_animSlideTime; var g_animMainSequence =3D null; var ENDSHOW_MESG=3D"Конец поl= 2;аза слайдов. = Щелкните дл = 03; выхода.", SCREEN_MODE=3D"Frames", g= IsEndShow=3D0, NUM_VIS_SLDS=3D40, SCRIPT_HREF=3D"script.js", FULLSCR_HREF= =3D"fullscreen.htm"; var gCurSld =3D gPrevSld =3D 1, g_offset =3D 0, gNtsOpen =3D gHasNts =3D gO= tlTxtExp =3D 0, gHasNarration =3D 0, gOtlOpen =3D true window.gPPTHTML=3DSupportsPPTHTML() var gMainDoc=3Dnew Array(new hrefList("slide0001.htm",1,-1,1),new hrefList(= "slide0002.htm",1,-1,1),new hrefList("slide0003.htm",1,-1,1),new hrefList("= slide0004.htm",1,-1,1),new hrefList("slide0005.htm",1,-1,1),new hrefList("s= lide0013.htm",1,-1,1),new hrefList("slide0006.htm",1,-1,1),new hrefList("sl= ide0007.htm",1,-1,1),new hrefList("slide0008.htm",1,-1,1),new hrefList("sli= de0009.htm",1,-1,1),new hrefList("slide0010.htm",1,-1,1),new hrefList("slid= e0011.htm",1,-1,1),new hrefList("slide0012.htm",1,-1,1),new hrefList("slide= 0014.htm",1,-1,1),new hrefList("slide0018.htm",1,-1,1),new hrefList("slide0= 015.htm",1,-1,1),new hrefList("slide0022.htm",1,-1,1),new hrefList("slide00= 16.htm",1,-1,1),new hrefList("slide0042.htm",1,-1,1),new hrefList("slide004= 3.htm",1,-1,1),new hrefList("slide0017.htm",1,-1,1),new hrefList("slide0019= .htm",1,-1,1),new hrefList("slide0020.htm",1,-1,1),new hrefList("slide0021.= htm",1,-1,1),new hrefList("slide0023.htm",1,-1,1),new hrefList("slide0024.h= tm",1,-1,1),new hrefList("slide0025.htm",1,-1,1),new hrefList("slide0026.ht= m",1,-1,1),new hrefList("slide0028.htm",1,-1,1),new hrefList("slide0029.htm= ",1,-1,1),new hrefList("slide0030.htm",1,-1,1),new hrefList("slide0031.htm"= ,1,-1,1),new hrefList("slide0032.htm",1,-1,1),new hrefList("slide0033.htm",= 1,-1,1),new hrefList("slide0034.htm",1,-1,1),new hrefList("slide0035.htm",1= ,-1,1),new hrefList("slide0038.htm",1,-1,1),new hrefList("slide0039.htm",1,= -1,1),new hrefList("slide0040.htm",1,-1,1),new hrefList("slide0041.htm",1,-= 1,1)); /********************************************* Frameset functions These functions control slide navigation and state of the frameset. **********************************************/ function FullScrInit() { g_allowAdvOnClick =3D GetCurSld().mAdvOnClk document.body.style.backgroundColor=3D"black" document.oncontextmenu=3Dparent._CM; document.onkeydown =3D _KDH; document.ondragstart=3DCancel document.onselectstart=3DCancel self.focus() } function Redirect( frmId ) {=09 var str=3Ddocument.location.hash,idx=3Dstr.indexOf('#'), sId=3DGetSldId() if(idx>=3D0) str=3Dstr.substr(1); if( window.name !=3D frmId && ( sId !=3D str) ) { obj =3D GetObj("Main-File") window.location.href=3Dobj.href+"#"+sId return 1 } return 0 } var MHTMLPrefix =3D CalculateMHTMLPrefix();=20 function CalculateMHTMLPrefix() { if ( document.location.protocol =3D=3D 'mhtml:') {=20 href=3Dnew String(document.location.href)=20 Start=3Dhref.indexOf('!')+1=20 End=3Dhref.lastIndexOf('/')+1=20 if (End < Start)=20 return href.substring(0, Start)=20 else=20 return href.substring(0, End)=20 } return ''; } function GetTags(base,tag) { if(g_supportsPPTHTML) return base.all.tags(tag); else return base.getElementsByTagName(tag); } function UpdNtsPane(){ if(frames["PPTNts"]) PPTNts.location.replace( MHTMLP= refix+GetHrefObj( gCurSld ).mNtsHref ) } function UpdNavPane( sldIndex ){ if(gNavLoaded) PPTNav.UpdNav() } function UpdOtNavPane(){ if(gOtlNavLoaded) PPTOtlNav.UpdOtlNav() } function UpdOtlPane(){ if(gOtlLoaded) PPTOtl.UpdOtl() } function SetHasNts( fVal ) { if( gHasNts !=3D fVal ) { gHasNts=3DfVal UpdNavPane() } } function ToggleOtlText() { gOtlTxtExp=3D!gOtlTxtExp UpdOtlPane() } function ClearMedia() { // Clear any sounds playing before launching another browser window. Other= wise, // in fullscreen mode, you'll continue to hear the sound in the frames mod= e. if (PPTSld.pptSound) PPTSld.pptSound.loop =3D 0; } function FullScreen() {=20 if ( PPTSld.g_animUseRuntime ) PPTSld.document.body.pause(); ClearMedia(); var href =3D ( document.location.protocol =3D=3D 'mhtml:') ? FULLSCR_HREF = : FULLSCR_HREF+"#"+GetHrefObj(gCurSld).mSldHref; if(PPTNav.event.ctrlKey) { var w =3D (window.screen.availWidth * 1.0) / 2.0 var h =3D w * (PPTSld.g_origH * 1.0) / PPTSld.g_origW win =3D window.open( MHTMLPrefix+href,null,"toolbar=3D0,resizable=3D1,top= =3D0,left=3D0," + "width=3D"+ w + ",height=3D" + h ); if( win.document.body && PPTSld.g_animUseRuntime ) win.document.body.PPTSldFrameset=3Dwindow; } else { win =3D window.open( MHTMLPrefix+href,null,"fullscreen=3Dyes" ); if( win.document.body && PPTSld.g_animUseRuntime ) win.document.body.PPTSldFrameset=3Dwindow; } } function ToggleVNarration() { rObj=3DPPTSld.document.all("NSPlay") if( rObj && !PPTSld.g_animUseRuntime ) { if( (rObj.playState =3D=3D 1)||(rObj.playState =3D=3D 0) ) rObj.Play() else if( rObj.playState =3D=3D 2 ) rObj.Pause() else return; } else if( PPTSld.g_animUseRuntime ) { narObj =3D PPTSld.document.all("narrationID") if( narObj ) narObj.togglePause() } } function GetCurSldNum() { =20 obj=3DGetHrefObj(gCurSld) if( obj.mOrigVis =3D=3D 1 ) return obj.mSldIdx else =20 return gCurSld } function GetNumSlds() { =20 if( GetHrefObj(gCurSld).mOrigVis =3D=3D 1 ) return GetSldList().mNumVisSlds; else return GetSldList().mList.length } function GetSldNum( href ) { for(ii=3D0; ii 1 ) PopSldList(); else if( !IsFramesMode() ) { if( gLoopCont ) GoToFirst() else EndShow() } } function GoToPrevSld() { ii=3DgCurSld-1 if( ii > 0 ) { obj=3DGetHrefObj(ii) while ( obj && ( obj.mVis =3D=3D 0 ) && ( ii>0 ) ) obj=3DGetHrefObj(--ii) if( ii =3D=3D 0 ) ii=3D1 GoToSldNum(ii) } } function GoToFirst(){ GoToSld( GetHrefObj(1).mSldHref ) } function GoToLast() { ii=3DGetSldList().mList.length if( ii !=3D gCurSld ) GoToSld( GetHrefObj(ii).mSldHref ) } function GoToSldNum( num ) { if( PPTSld.event ) PPTSld.event.cancelBubble=3Dtrue obj =3D GetHrefObj( num ) obj.mVis=3D1 gPrevSld=3DgCurSld gCurSld =3D num; PPTSld.location.replace(MHTMLPrefix+obj.mSldHref) if( IsFramesMode() ) { UpdNavPane(); UpdOtlPane(); UpdNtsPane() } } function GoToSld( href ) { if( PPTSld.event ) PPTSld.event.cancelBubble=3Dtrue GetHrefObj( GetSldNum(href) ).mVis=3D1 PPTSld.location.replace(MHTMLPrefix+href) } function SldUpdated( id ) { if( id =3D=3D GetHrefObj(gCurSld).mSldHref ) return gPrevSld=3DgCurSld gCurSld=3DGetSldNum(id) if( IsFramesMode() ) { UpdNavPane(); UpdOtlPane(); UpdNtsPane() } } function PrevSldViewed(){ GoToSld( GetHrefObj(gPrevSld).mSldHref ) } function HasPrevSld() { return ( gIsEndShow || ( gCurSld !=3D 1 && GetHrefO= bj( gCurSld-1 ).mVis =3D=3D 1 )||( GetCurSldNum() > 1 ) ) } function HasNextSld() { return (GetCurSldNum() !=3D GetNumSlds()) } function CloseWindow() { if( HideMenu() ) return; =09 var event =3D PPTSld.event; if( !IsFramesMode() && event && (event.keyCode=3D=3D27 || event.keyCode=3D= =3D32 || event.type=3D=3D"click" ) ) window.close( self ); CatchNumKeys( self, event ); } function Unload() { gIsEndShow=3D0; } function SetupEndShow() { gIsEndShow=3D1; PPTSld.document.body.scroll=3D"no"; PPTSld.document.onkeypress=3DCloseWindow; PPTSld.document.onclick=3DCloseWindow; PPTSld.document.oncontextmenu=3D_CM; } function EndShow() { if( IsFramesMode() ) return if( PPTSld.event ) PPTSld.event.cancelBubble=3Dtrue doc=3DPPTSld.document var dir =3D doc.body.dir if( dir !=3D "rtl" ) dir =3D "ltr"; doc.open() doc.writeln('


' + ENDSHOW_MESG + '

') doc.close() } function SetSldVisited(){ GetSldList().mList[gCurSld-1].mVisited=3Dtrue } function IsSldVisited(){ return GetSldList().mList[gCurSld-1].mVisited } function hrefList( sldHref, visible, advDelay, advClk ) { this.mSldHref=3D this.mNtsHref =3D sldHref this.mOrigVis=3D this.mVis =3D visible this.mVisited=3D false this.mAdvDelay=3D advDelay this.mAdvOnClk=3D advClk } function SldList(arr,curSld,fEnd) { this.mCurSld =3D curSld; this.mList =3D new Array(); var idx =3D 1; for(ii=3D0;ii 0) { PushSldList(sldList,fEnd); gCurSld =3D 1; } else if( PPTSld.event ) PPTSld.event.cancelBubble=3Dtrue } function PushSldList(arr,fEnd) { var ii =3D gSldStack.length; gSldStack[ii] =3D new SldList(arr,gCurSld,fEnd); GoToSld( gSldStack[ii].mList[0].mSldHref ); } function PopSldList() { if (gSldStack[gSldStack.length-1].fEndShow) EndShow() else { gCurSld =3D gSldStack[gSldStack.length-1].mCurSld; gSldStack[gSldStack.length-1] =3D null; gSldStack.length--; var sldList =3D gSldStack[gSldStack.length-1]; GoToSld( sldList.mList[gCurSld - 1].mSldHref ); } } var custShowList=3Dnew Array(); /********************************************* Navigation button implementation There are 2 types of buttons: ImgBtn, TxtBtn implemented as function objects. They share a similiar interface so the event handlers can call SetActive, for example, on a button=20 object without needing to know exactly=20 what type of button it is. **********************************************/ //---------------------------------- function ImgBtn( oId,bId,w,action ) //---------------------------------- { var t=3Dthis t.Perform =3D _IBP t.SetActive =3D _IBSetA t.SetInactive=3D _IBSetI t.SetPressed =3D _IBSetP t.SetDisabled=3D _IBSetD t.Enabled =3D _IBSetE t.ChangeIcon =3D null t.UserAction =3D action t.ChgState =3D _IBUI t.mObjId =3D oId t.mBorderId=3D bId t.mWidth =3D w t.mIsOn =3D t.mCurState =3D 0 } function _IBSetA() { if( this.mIsOn ) { obj=3Dthis.ChgState( gHiliteClr,gShadowClr,2 ) obj.style.posTop=3D0 } } function _IBSetI() { if( this.mIsOn ) { obj=3Dthis.ChgState( gFaceClr,gFaceClr,1 ) obj.style.posTop=3D0=20 } } function _IBSetP() { if( this.mIsOn ) { obj=3Dthis.ChgState( gShadowClr,gHiliteClr,2 ) obj.style.posLeft+=3D1; obj.style.posTop+=3D1 } } function _IBSetD() { =20 obj=3Dthis.ChgState( gFaceClr,gFaceClr,0 ) obj.style.posTop=3D0=20 } function _IBSetE( state ) { var t=3Dthis GetObj( t.mBorderId ).style.visibility=3D"visible" if( state !=3D t.mIsOn ) { t.mIsOn=3Dstate if( state ) t.SetInactive() else t.SetDisabled() } } function _IBP() { var t=3Dthis if( t.mIsOn ) { if( t.UserAction !=3D null ) t.UserAction() if( t.ChangeIcon ) { obj=3DGetObj(t.mObjId) if( t.ChangeIcon() ) obj.style.posLeft=3Dobj.style.posLeft+(t.mCurState-4)*t.mWidth else obj.style.posLeft=3Dobj.style.posLeft+(t.mCurState-0)*t.mWidth } t.SetActive() } =20 } function _IBUI( clr1,clr2,nextState ) { var t=3Dthis SetBorder( GetObj( t.mBorderId ),clr1,clr2 ) obj=3DGetObj( t.mObjId ) obj.style.posLeft=3Dobj.style.posLeft+(t.mCurState-nextState)*t.mWidth-obj= .style.posTop t.mCurState=3DnextState return obj } //----------------------------------------- function TxtBtn( oId,oeId,action,chkState ) //----------------------------------------- { var t=3Dthis t.Perform =3D _TBP t.SetActive =3D _TBSetA t.SetInactive=3D _TBSetI t.SetPressed =3D _TBSetP t.SetDisabled=3D _TBSetD t.SetEnabled =3D _TBSetE t.GetState =3D chkState t.UserAction =3D action t.ChgState =3D _TBUI t.mObjId =3D oId t.m_elementsId=3D oeId t.mIsOn =3D 1 } function _TBSetA() { var t=3Dthis if( t.mIsOn && !t.GetState() ) t.ChgState( gHiliteClr,gShadowClr,0,0 ) } function _TBSetI() { var t=3Dthis if( t.mIsOn && !t.GetState() ) t.ChgState( gFaceClr,gFaceClr,0,0 ) } function _TBSetP() { if( this.mIsOn ) this.ChgState( gShadowClr,gHiliteClr,1,1 ) } function _TBSetD() { =20 this.ChgState( gFaceClr,gFaceClr,0,0 ) this.mIsOn =3D 0 } function _TBSetE() { var t=3Dthis if( !t.GetState() ) t.ChgState( gFaceClr,gFaceClr,0,0 ) else t.ChgState( gShadowClr,gHiliteClr,1,1 ) t.mIsOn =3D 1 } function _TBP() { var t=3Dthis if( t.mIsOn ) {=20 if( t.UserAction !=3D null ) t.UserAction() if( !t.GetState ) return if( t.GetState() ) t.SetPressed() else t.SetActive() } =20 } function _TBUI( clr1,clr2,lOffset,tOffset ) { SetBorder( GetObj( this.mObjId ),clr1,clr2 ) Offset( GetObj( this.m_elementsId ),lOffset,tOffset ) } function Offset( obj, top, left ){ obj.style.top=3Dtop; obj.style.left=3Dle= ft } function SetBorder( obj, upperLeft, lowerRight ) { s=3Dobj.style; s.borderStyle =3D "solid" s.borderWidth =3D 1=20 s.borderLeftColor =3D s.borderTopColor =3D upperLeft s.borderBottomColor=3D s.borderRightColor =3D lowerRight } function GetBtnObj(){ return gBtnArr[window.event.srcElement.id] } function BtnOnOver(){ b=3DGetBtnObj(); if( b !=3D null ) b.SetActive() } function BtnOnDown(){ b=3DGetBtnObj(); if( b !=3D null ) b.SetPressed() } function BtnOnOut(){ b=3DGetBtnObj(); if( b !=3D null ) b.SetInactive() } function BtnOnUp() { b=3DGetBtnObj() if( b !=3D null ) b.Perform() else Upd() } function GetNtsState(){ return parent.gNtsOpen } function GetOtlState(){ return parent.gOtlOpen } function GetOtlTxtState(){ return parent.gOtlTxtExp } function NtsBtnSetFlag( fVal ) { s=3Ddocument.all.item( this.m_flagId ).style s.display=3D"none" if( fVal ) s.display=3D"" else s.display=3D"none" } function _BSetA_Border(){ b =3D gBtnArr[this.mObjId]; if( b !=3D null ) b.S= etActive() } function _BSetI_Border(){ b =3D gBtnArr[this.mObjId]; if( b !=3D null ) b.S= etInactive() } function _BSetP_Border(){ b =3D gBtnArr[this.mObjId]; if( b !=3D null ) b.S= etPressed() } function _BSetA_BorderImg() {=20 b =3D gBtnArr[this.mBorderId]=20 if( b !=3D null && this.mIsOn && !b.GetState() ) { obj=3Dthis.ChgState( gHiliteClr,gShadowClr,2 ) obj.style.posTop=3D0 } } function _BSetI_BorderImg() {=20 b =3D gBtnArr[this.mBorderId] if( b !=3D null && this.mIsOn && !b.GetState() ) { obj=3Dthis.ChgState( gFaceClr,gFaceClr,1 ) obj.style.posTop=3D0 } } var gHiliteClr=3D"THREEDHIGHLIGHT",gShadowClr=3D"THREEDSHADOW",gFaceClr=3D"= THREEDFACE" var gBtnArr =3D new Array() gBtnArr["nb_otl"] =3D new TxtBtn( "nb_otl","nb_otlElem",parent.ToggleOtlPan= e,GetOtlState ) gBtnArr["nb_otlElem"] =3D new TxtBtn( "nb_otl","nb_otlElem",parent.ToggleOt= lPane,GetOtlState ) gBtnArr["nb_nts"] =3D new ImgBtn( "nb_nts","nb_ntsBorder",10,parent.ToggleN= tsPane ) gBtnArr["nb_nts"].SetActive =3D _BSetA_BorderImg; gBtnArr["nb_nts"].SetInactive =3D _BSetI_BorderImg; gBtnArr["nb_ntsBorder"] =3D new TxtBtn( "nb_ntsBorder","nb_ntsElem",parent.= ToggleNtsPane,GetNtsState ) gBtnArr["nb_ntsElem"] =3D new TxtBtn( "nb_ntsBorder","nb_ntsElem",parent.To= ggleNtsPane,GetNtsState ) gBtnArr["nb_prevBorder"] =3D gBtnArr["nb_prev"]=3D new ImgBtn( "nb_prev","n= b_prevBorder",30,parent.GoToPrevSld ) gBtnArr["nb_nextBorder"] =3D gBtnArr["nb_next"]=3D new ImgBtn( "nb_next","n= b_nextBorder",30,parent.GoToNextSld ) gBtnArr["nb_sldshw"]=3D new ImgBtn( "nb_sldshw","nb_sldshwBorder",18,parent= .FullScreen ) gBtnArr["nb_sldshwBorder"] =3D new TxtBtn( "nb_sldshw","nb_sldshwBorder",pa= rent.FullScreen,null ) gBtnArr["nb_sldshwBorder"].SetActive =3D _BSetA_Border; gBtnArr["nb_sldshwBorder"].SetInactive =3D _BSetI_Border; gBtnArr["nb_sldshwText"] =3D new TxtBtn( "nb_sldshw","nb_sldshwText",parent= .FullScreen,null ) gBtnArr["nb_sldshwText"].SetActive =3D _BSetA_Border; gBtnArr["nb_sldshwText"].SetInactive =3D _BSetI_Border; gBtnArr["nb_voice"] =3D gBtnArr["nb_voiceBorder"] =3D new ImgBtn( "nb_voice= ","nb_voiceBorder",18,parent.ToggleVNarration ) gBtnArr["nb_otlTxtBorder"] =3D gBtnArr["nb_otlTxt"]=3D new ImgBtn( "nb_otlT= xt","nb_otlTxtBorder",23,parent.ToggleOtlText ) gBtnArr["nb_ntsBorder"].m_flagId=3D "nb_nts" gBtnArr["nb_ntsBorder"].SetFlag =3D NtsBtnSetFlag gBtnArr["nb_otlTxt"].ChangeIcon=3D GetOtlTxtState /********************************************* Context menu implementation _CM() is the function that's hooked up to the oncontextmenu event. Once we're asked to show the menu, we first build it by creating DIVs on-the-fly. Then we position it=20 within the screen area so it doesn't get clipped. Creating the DIVs using createElement() means we don't have to write out any extra HTML into the slide HTML files. **********************************************/ var sNext=3D"Далее",sPrev=3D"На&#= 1079;ад",sEnd=3D"Заверш = 80;ть показ",sFont=3D"Arial",sArr= ow=3D"Стрелка",sFreeform=3D"i= 5;олилиния",sRect=3D"П= ;рямоугольн = 80;к",sOval=3D"Овал" function ShowMenu() { BuildMenu(); var doc=3DPPTSld.document.body,x=3DPPTSld.event.clientX+doc.scrollLeft,y= =3DPPTSld.event.clientY+doc.scrollTop m =3D PPTSld.document.all.item("ctxtmenu") m.style.pixelLeft=3Dx if( (x+m.scrollWidth > doc.clientWidth)&&(x-m.scrollWidth > 0) ) m.style.pixelLeft=3Dx-m.scrollWidth m.style.pixelTop=3Dy if( (y+m.scrollHeight > doc.clientHeight)&&(y-m.scrollHeight > 0) ) m.style.pixelTop=3Dy-m.scrollHeight m.style.display=3D"" } function _CM() { if( !parent.IsFullScrMode() ) return; if(!PPTSld.event.ctrlKey) { ShowMenu() return false } else HideMenu() } function BuildMenu() { if( PPTSld.document.all.item("ctxtmenu") ) return var mObj=3DCreateItem( PPTSld.document.body ) mObj.id=3D"ctxtmenu" mObj.style.visibility=3D"hidden" var s=3DmObj.style s.position=3D"absolute" s.cursor=3D"default" s.width=3D"120px" SetCMBorder(mObj,"menu","black") var iObj=3DCreateItem( mObj ) SetCMBorder( iObj, "threedhighlight","threedshadow" ) iObj.style.padding=3D2 CreateMenuItem( iObj,sNext,M_GoNextSld,M_True ) CreateMenuItem( iObj,sPrev,M_GoPrevSld,M_HasPrevSld ) =09 CreateSeparator( iObj ) CreateMenuItem( iObj,sEnd,M_End,M_True ) mObj.style.visibility=3D"visible" } function Cancel() { window.event.cancelBubble=3Dtrue; window.event.returnVa= lue=3Dfalse } function Highlight() { ChangeClr("activecaption","threedhighlight") } function Deselect() { ChangeClr("threedface","menutext") } function Perform() { e=3DPPTSld.event.srcElement if( e.type=3D=3D"menuitem" && e.IsActive() ) e.Action() else PPTSld.event.cancelBubble=3Dtrue } function ChangeClr( bg,clr ) { e=3DPPTSld.event.srcElement if( e.type=3D=3D"menuitem" && e.IsActive() ) { e.style.backgroundColor=3Dbg e.style.color=3Dclr } } function M_HasPrevSld() { return( parent.HasPrevSld() ) } function M_GoNextSld() { if( gIsEndShow ) M_End(); else GoToNextSld() } function M_GoPrevSld() { if( gIsEndShow ) { gIsEndShow=3D0; history.back();= PPTSld.event.cancelBubble=3Dtrue; } else GoToPrevSld() } function M_True() { return true } function M_End() { window.close( self ) } function CreateMenuItem( node,text,action,eval ) { var e=3DCreateItem( node ) e.type=3D"menuitem" e.Action=3Daction e.IsActive=3Deval e.innerHTML=3Dtext if( !e.IsActive() ) e.style.color=3D"threedshadow" e.onclick=3DPerform e.onmouseover=3DHighlight e.onmouseout=3DDeselect s=3De.style; s.fontFamily=3DsFont s.fontSize=3D"9pt" s.paddingLeft=3D2 } function CreateSeparator( node ) { var sObj=3DCreateItem( node ) SetCMBorder(sObj,"menu","menu") var s=3DsObj.style s.borderTopColor=3D"threedshadow" s.borderBottomColor=3D"threedhighlight" s.height=3D1 s.fontSize=3D"0px" } function CreateItem( node ) { var elem=3DPPTSld.document.createElement("DIV") node.insertBefore( elem ) return elem } function SetCMBorder( o,ltClr,rbClr ) { var s=3Do.style s.backgroundColor=3D"menu" s.borderStyle=3D"solid" s.borderWidth=3D1 s.borderColor=3DltClr+" "+rbClr+" "+rbClr+" "+ltClr } ------=_NextPart_01C93BA5.211FE1F0 Content-Location: file:///C:/8D437683/file8707.files/fullscreen.htm Content-Transfer-Encoding: quoted-printable Content-Type: text/html; charset="us-ascii" ------=_NextPart_01C93BA5.211FE1F0 Content-Location: file:///C:/8D437683/file8707.files/buttons.gif Content-Transfer-Encoding: base64 Content-Type: image/gif R0lGODlhWAESAPf4AAAAAIAAAACAAICAAAAAgIAAgACAgICAgAQEBISEBASEBISEhAQEhMTExAQE /KTM9Pz8/ERERPz8BAT8/KSkpGRkhMTcxCRkxAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAA AAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAA AAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAA AAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAA AAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAA AAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAA AAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAA AAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAA AAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAA AAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAA AAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAA AAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAAA AAAAAAAAAAAAAAAAAAAAAMDAwP8AAAD/AP//AAAA//8A/wD//////yH5BAEAAPgALAAAAABYARIA QAj/APEJHEiwoMGDCBMqXMiwocOHECNKnEixosWLGCEiQKCRo8YDIEHig2DxAD4LKD1avDDhgUuV GUOGbHBR5QGYFBG4fHAB58EKECJEwCfUYAWPFGAygLCRKQIIUKM6WAohKUGgCikcFWh1INWoYKVS 7SrQ41GbIhGYLAuVQVOoC+IyXUuUAkG1HE3KFDhAwkgJc5/qDZmxsOHDiBMrXsy4sePDGyP7lChT 5MULmDPnlDw5YmW6FTNrfgi0aNGEZPEtbfo2bNTUpYeeRph69dPWrqvCNFuBIGG1A59CYPAVQtwF cw0OxWdTIOiBCQAjaAB17fOFII8voGmRc+eOkilm/z9OvTtnjN4hYk1YoT3H2rnBOphPAB9skgq3 2lcaX/5YnJVt9BloAar12UEIRGCZdQghMABI1Tn32IQUVthYexhmqGGGMBHAgIfEhSiiiATAtOGJ GnYI4ogsEldicAYOGNJGZaml3Y0L3NTZUBz1xlB0PUoUI0jlVWRSVN89xBKSGB1YU1TMoRfVBEle hR9HQs1GEHxQ3RZZbveZthxt/LEmXHyp5XWABSCpaRJwbM13gAACPHVccgJFgF+NEhqUAEkQSCfc ddhVhh5dVTaEAEsTUNlkZUWKN9BNGDE6QU8OrSdbllzpxyVTTrU21Uj3scfhp7nNpyoDaTIEJ3P9 If8J2kbLNYegg9JRBwGhFvbq66+ZUiDssMQWK2yHxiZLrInKNotss8l+B5yBrr5p2UIJvortANoC 6+234IbLla/elRtZjeamh5CC3Sb0YLvixivvYkDFGlZqBNh7r4n6goVvv6/ZlCicN+kL71ALTnpQ dCIZp7CihkLA3UQmoWRBogyxtBPGCTnZncVR1rSTo5nuydC/Eo8kUH+lOoTyyvjoCuZu+PjYIKLD rZybtrM1d10C0QXKEVz48GrQkEeWdFJKlbb0UmEeV0SzyC6RvNB646LWIVjUNeC1zAFb+RDKXksM 9r531bwmpQW9+hQDDsx5pqwDRWBXcFES2hc+gEn/wJGdEEWdE6LoWcoxQweaTNmkhydkKaYMYY2Q p1unbLl/pPKbn3v7EZRvrKvqlja2ONvrtoIw9tn2g32/tQBlhtYkU+MNikZ7QYlPDPuMldpOmuJX nVo5VF3HjI+q89mteX5IDd/fVFClma5kiE4f2XUJhlz09gj2NbTDRifkmu7zXjR++RVJ/lPznuvr QH2iD6S+UewP9Dnon6d2NLwN8n90BB6hC68cFMCHoe+ACASP9c4DowUyEF0OPFcDI0ij/VXPaAKC UfhS95AKGoQ7IBRICI1HwhGaUIQoLGEKT6jCFrLwhSuMoQtlCMMZ2rCGOKShDm+4wxzy8Ic+DGIP B4cIRCKGMCAAOy== ------=_NextPart_01C93BA5.211FE1F0 Content-Location: file:///C:/8D437683/file8707.files/frame.htm Content-Transfer-Encoding: quoted-printable Content-Type: text/html; charset="us-ascii" Неоптолемk= 7;евская механика − ------=_NextPart_01C93BA5.211FE1F0 Content-Location: file:///C:/8D437683/file8707.files/outline.htm Content-Transfer-Encoding: quoted-printable Content-Type: text/html; charset="us-ascii"
 &#= 1047;аметки
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