MIME-Version: 1.0 Content-Type: multipart/related; boundary="----=_NextPart_01C3E850.34CE0310" This document is a Web archive file. If you are seeing this message, this means your browser or editor doesn't support Web archive files. For more information on the Web archive format, go to http://officeupdate.microsoft.com/office/webarchive.htm ------=_NextPart_01C3E850.34CE0310 Content-Location: file:///C:/A0E53DF2/Lok_energet_u-ki-N2.htm Content-Transfer-Encoding: quoted-printable Content-Type: text/html; charset="windows-1251" Министерство путей сообщения Российской Федерации

Министерство путей сообщения Российской Федерации
Дальневосточный государственный университет путей сообщения

Кафедра "Теплово= зы и тепловые двигатели"
   
З.Б. Погребинский
А.Ю. Коньков

ЛОКОМОТИВНЫЕ ЭНЕРГЕТИЧЕСКИЕ УСТАНОВКИ=

Методические указания
на выполнение лабораторных работ

Часть 2


Хабаровск
2001


Рецензент: Доцент кафедры "Тепловозы и тепловые двигатели" Дальневосточного государственного университета путей сообщения В.В. Литвинчук


Погребинский З.Б., Коньков А.Ю. Локомотивные энергетические установки: Методические указания на выполнение лабораторных работ. Часть 2. - Хабаровск:
Изд-во ДВГУПС, 2001. - 35 с.: ил.

    В методических указаниях приведены сведения, необходимые= для выполнения лабораторных работ по курсу "Локомотивные энергетические ус= тановки". Во вторую часть указаний включены работы, связанные с особенностями конструкции, регулировкой и эксплуатацией топливной аппаратуры тепловозных дизелей.
Методические указания предназначены для студентов специальности "Локомотивы" всех форм обучения.


Издательство Дальневосточного государственного университета путей сообщения= (ДВГУПС), 2001

СОДЕРЖАНИЕ


ВВЕДЕНИЕ
1. Лабораторная работа № 1 ТОПЛИВНАЯ АППАРАТУРА ТЕПЛОВОЗНЫХ ДИЗЕЛЕЙ 
1.1. Цель работы  
1.2. Топливные системы тепловозов
1.2.1. Принцип работы топливного насоса высокого давления
1.2.2. Конструкция ТНВД дизеля Д5= 0
1.2.3. Конструкция ТНВД дизеля 10= Д100 
1.2.4. Конструкция и принцип работы форсунок дизелей типа Д10= 0 и Д50 
1.2.5. Конструкция форсунки дизеля 10Д100
1.2.6. Конструкция форсунки дизеля Д50
2. Лабораторная работа № 2 ВНЕШНИЙ ТЕПЛОВОЙ БАЛАНС  ДВИГАТЕЛЯ ВНУТРЕННЕГО СГОРАНИЯ
2.1. Цель работы 
2.2. Внешний тепловой баланс двигателя внутреннего сгорания
2.3. Расчет внешнего теплового баланса
2.4. Порядок проведения лабораторной работы
2.5. Контрольные вопросы
3. Лабораторная работа № 3 ОПРЕДЕЛЕНИЕ УГЛА ОПЕ= РЕЖЕНИЯ ПОДАЧИ ТОПЛИВА
3.1. Цель работы
3.2. Принципы регулирования угла опережения подачи топлива
3.3. Методы определения УОПТ
3.4. Объект исследований и оборудование
3.5. Порядок выполнения работы
3.6. Контрольные вопросы 
4. Лабораторная работа № 4 ВЛИЯНИЕ УГЛА ОПЕРЕЖЕНИЯ ПОДАЧИ ТОПЛИВА НА ПОКАЗАТЕЛИ РАБОТЫ ДИЗЕЛЯ
4.1. Цель работы
4.2. Теоретические сведения
4.3. Объект исследований и оборудование
4.4. Порядок выполнения работы
4.5. Контрольные вопросы   
СПИСОК ЛИТЕРАТУРЫ  

ВВЕДЕНИЕ


   = ; В методических указаниях изложены вопросы конструкции, принципы действия, регулировки элементов топливной аппаратуры тепловозных дизелей: топливных насосов высокого давления, форсунок. Особое внимание уделяется методам опре= деления и регулирования углов опережения подачи топлива, производительности насосов= - важнейших эксплуатационных регулировок дизелей. Раскрыты механизмы влияния = этих характеристик на рабочий процесс двигателя внутр= еннего сгорания.
В методических указаниях на выполнение лабораторных работ по ЛЭУ дается необходимый теоретический материал, расшир= яющий представления студентов о соответствующих разделах учебной дисциплины. Прив= еден достаточный справочный материал и необходимый объем аналитических выражений= для обработки опытных данных и анализа результатов экспериментов.
    Выбранный перечень лабораторных работ и содержание методических указаний на их выполнение соответствуют учебной программе дисциплины ЛЭУ, одобренной в 1999 г. учебно-методическим советом по специальности 150700 "Локомотивы".=


1. Лабораторная работа № 1
ТОПЛИВНАЯ АППАРАТУРА ТЕПЛОВОЗНЫХ ДИЗЕЛЕЙ

1.1. ЦЕЛЬ РАБОТЫ
Изучение требований, предъявляемых к топливной системе дизелей, конструкций= и принципов работы основных устройств топливной аппаратуры и методов регулирования подачи топлива в цилиндр.

1.2= . ТОПЛИВНЫЕ СИСТЕМЫ ТЕПЛОВОЗОВ<= b>
    Топливная система тепловозов служит для подачи топли= ва к форсункам тепловозного дизеля. Она должна обеспечивать:
- запас топлива для пробега поездных тепловозов на расстояние
800-1300 км и маневровых для работы в течение 8-15 суток;
- хорошую фильтрацию топлива;
- подогрев топлива в холодное время года до t<= span style=3D'font-size:10.0pt;font-family:Arial'>т =3D 3= 5-55 °С;
- избыточное давление в топливной системе, которое достигается увеличенной производительностью топливоподкачивающего насоса (ТПН<= /span>) относительно потребностей дизеля (коэффициент циркуляции 2-3 ед.);
- аварийную работу дизеля в случае отказа ТПН, при которой обеспечивается примерно 50 % номинальной мощности дизеля;
- устойчивую работу дизеля при минимальной частоте вращения коленчатого вал= а;
- точную дозировку цикловых подач топлива в цилиндр;
- оптимальное давление впрыска топлива в цилиндр;
- впрыск цикловой подачи в нужный момент;
- оптимальный закон подачи для заданных условий смесеобразования, воспламен= ения и сгорания топлива.
Топливные системы дизелей типа Д100 и Д50 относятся к системам непосредственного впрыска с механическим приводом, широко используемым в отечественных и зарубежных дизелях.
Основными элементами топливной системы являются насосы высокого давления, форсунки, фильтры, нагнетательные трубопроводы, топливный бак, ТПН.

    1.2.1. Принцип работы топливного насоса высокого давления
    Рассмотрим принцип действия топливного насоса высокого давления (ТНВД), принципиальная схема которого представлена на рис. 1.1. Внутри неподвижной гильзы помещен подвиж= ный плунжер. Плунжер - это поршень, длина которого значительно превышает диамет= р. Вместе эти детали - гильза и плунжер - образуют плунжерную пару. Плунжер подобран к гильзе или притерт к его стенкам так плотно, что утечки топлива между ними почти не происходит. Зазор между плунжером и гильзой не превышает обычно 1,5-4 мкм. Трубопровод, подходящий к окну А гильзы, всегда заполнен топливом.
Когда плунжер находится в нижнем положении, топливо через окно А заполняет пространство над плунжером (рис. 1.1, а).= При вращении кулачкового вала привода топливного насоса кулач= ок набегает на ролик толкателя (рис. 1.1, б), плунжер начинает двигаться вверх= и верхней кромкой постепенно закрывает окно А. При этом нагнетательный клапан, прижатый к своему седлу пружиной, испытывает снизу давление топлива, вытесняемого плунжером, а сверху - усилие пружины и давление топлива, оставшегося в трубопроводе. Пока усилие на клапан, создаваемое давле= нием топлива, меньше усилия, создаваемого пружиной, клапан закрыт и часть топлив= а, не имея другого выхода, устремится из надплунжерного пространства обратно в окно А (рис. 1.1, б). Ког= да плунжер кромкой a полностью закроет окно А (рис. 1.1, в), вытекание топлива через него прекрат= ится. Примерно с этого момента при продолжающемся ходе плунжера вверх начнется нагнетание: давление топлива преодолеет усилие пружины нагнетательного клап= ана, он откроется, и топливо будет через трубопровод поступать в форсунку до тех пор, пока плунжер не достигнет своего крайнего положения (рис. 1.1, г). Когда плунжер начинает двигаться вниз, прекращается подача топлива. Нагнетательный клапан под действием пружины снова садится на свое седло. Сбегая с выступа кулачка, ролик вместе с толкателем и плунжером= возвращается в первоначальное положение (см. рис. 1.1, а).

   &nb= sp;            =    


     &nbs= p;            &= nbsp;         Рис. 1.1. Схема действия топливного насоса высокого давления

    Ес= ли бы дизель всегда работал только на постоянной мощности, то рассмотренный нами топливный насос вполне удовлетворял бы требованиям работы на дизеле, так ка= к за один ход плунжера он подает одно и то же количество топлива, необходимое для получения нужной мощности. Количество топлива, подаваемого таким насосом, постоянно потому, что высота кулачка, а следоват= ельно, и ход плунжера являются величинами постоянными, а начало и конец нагнетания топлива, определяемые ходом плунжера в процессе работы, как мы видим, при т= акой конструкции не могут быть изменены.
    Однако условия работы тепловоза требуют, чтобы мощность дизеля могла изменяться. Дизель должен быть приспособлен к переменному режи= му работы локомотива. Мощность дизеля зависит от количества впрыскиваемого в цилиндры топлива. Чем больше топлива поступит в цилиндр во время рабочего х= ода, тем большую мощность будет развивать дизель. Поэтому нужно, чтобы топливный насос при необходимости позволял изменять количество топлива, подаваемого в течение одного хода плунжера в каждый из цилиндров дизеля соответственно его нагрузке.
При номинальной мощности 2200 кВт и номинальной частоте вращения коленчатого вала 850 мин дизель 10Д100 расходует в среднем = за час 495 кг топлива. Очевидно, что за один оборот вала (дизель двухтактный) расх= од топлива в каждый из цилиндров дизеля составит 0,97 г.
    Подача топлива в цилиндр одним насосом за один оборот ва= ла будет вдвое меньше ( на каждый цилиндр установле= ны два топливных насоса), т.е. 0,485 г. При работе дизеля в режиме холостого вала и минимальной частоте вращения коленчатого вала n= =3D 400 мин-1, подача топлива одним насосом может сократится до 0,055 г за цикл, т.е. почти в девять раз меньше, чем на режиме номинальн= ой мощности.

   &nb= sp; Рис. 1.2. Форма головки плунжер= а

   Каким же образом можно регулировать количество подаваемого топлива, не усложняя слиш= ком конструкцию топливного насоса? Наиболее просто изменение подачи топлива в т= аком диапазоне решается путем изменения активного хода плунжера. Для этого в вер= хней части плунжера выполним поперечную кольцевую выточку (рис. 1.2, а), вертикальный сквозной паз и специальный косой срез со спиральной кромкой О. В результате головка плунжера примет вид, изображенны= й на рис. 1.2, в.
    Развертка рабочей поверхности головки плунжера (рис. 1.3) представляет собой прямоугольник, один угол которого срезан. Срез соответст= вует спиральной кромке О и является прямой линией cd.

    Рис. 1.3. Развертка головки плунжера

    Спиральная кромка О плунжера имеет большое значе= ние, так как она является регулирующей. С ее помощью можно изменять количество топлива, подаваемого плунжером. Количество подаваемого топлива зависит от положения, которое занимает регулирующая кромка О относительно окна А (рис. 1.4) гильзы плунжера. Топливо начнет подаваться в= тот момент, когда верхний торец плунжера перекроет окно А, а прекращение подачи соответствует моменту, когда плунжер, продолжая двигат= ься вверх, своей спиральной кромкой откроет это окно. Для того чтобы изменить величину подачи топлива насосом, нужно заставить плунжер повернуться на некоторый угол так, чтобы против окна оказался другой участок регулирующей кромки, т.е заставить плунжер участвовать одновр= еменно в двух разных движениях: поступательном и вращательном (рис. 1.4).



Рис. 1.4. Схемы различных положений плунжера в гильзе:
а) нулевая подача; б) неполная подача; в) полная подача


    Поступательное движение плунжеру насоса сообщает кулачек (см. рис. 1.1). Поворот же его осуществляется с помощью специального механи= зма через выступ (поводок) плунжера. На рис. 1.4 показаны различные положения плунжера, соответствующие нулевой, частичной и полной подаче топлива плунже= ром.
Вертикальный паз соединяет надплунжерное простр= анство с кольцевой выточкой, при этом топливо заполняет не только надплунжерное пространтво, но и вертикальный паз и кольцевую выточку. Если повернуть плунжер так, чтобы вертикальный паз расположился прямо против окна А в гильзе, то при движении плунжера вверх топливо будет перепускаться через окно А и не попад= ет в нагнетательный трубопровод.
Для осуществления частичной подачи топлива плунжер поворачивают вокруг оси = по часовой стрелке так, чтобы окно А было изолирова= но от вертикального паза (рис. 1.4, б). Топливо из надплунже= рного устройства будет поступать в нагнетательный топливопро= вод только до момента, когда кромка О не откроет окн= о А. Плунжер при этом поднимается на величину h1, об= ъем вытесненного в цилиндр топлива будет равен площади поперечного сечения плунжера, умноженной на расстояние h1. Дальнейш= ее движение плунжера вверх происходит вхолостую, так как вытесняемое топливо перепускается через окно А.
    Если плунжер повернуть на больший угол (рис. 1.4, в), то полезный ход его увеличится и станет равным h2. Соответственно увеличится и объем топлива, вытесненного плунжером и поданного через форсунку в цилиндр. Таким образом, каждому значению мощности дизеля соответствует определенное положение спиральной кромки О плунжера относительно окна г= ильзы. При увеличении мощности дизеля плунжер будет поворачиваться по часовой стре= лке до нужной величины. Уменьшение нагрузки будет сопровождаться поворотом плун= жера в обратном направлении. Чем больше угол, на который повернется плунжер по часовой стрелке, тем позднее спиральная кромка откроет = окно А. Тем больше топлива будет подано плунжером за один ход и тем меньше топлива уйдет обратно через окно А.
    Итак, изменение величины подачи топлива производится поворотом плунжера. Практически для изменения подачи топлива от нуля до максиму-ма плунжер достато= чно повернуть на 1/4 оборота.

1.2.2. Конструкция ТНВД = дизеля Д50
    На рис. 1.5 представлен разрез секции ТНВД дизеля Д50. Главными деталями каждой секции, обслуживающей отдельную форсунку, являются знакомая= нам плунжерная пара - плунжер и его гильза, а также нагнетательный клапан с пружиной и седлом.
    Пружина прижимает клапан к седлу. Гильза плунжера укрепл= ена в корпусе секции неподвижно, причем седло нагнетательного клапана опирается= на верхний торец гильзы. Соприкасающиеся поверхности седла клапана и гильзы плунжера притираются, поэтому в этом месте создается надежное уплотнение и пропуск топлива при работе исключается.
    Изменение подачи топлива секцией насоса достигается поворотом плунжера. Конструктивно это выполнено так. На гильзу плунжера сни= зу надевается поворотная гильза с зубчатым венцом, которая находится в зацепле= нии с зубчатой рейкой, соединенной механизмом (состоящим из рычагов и тяг) с регулятором частоты вращения коленчатого вала. При перемещении рейки ее зуб= ья заставляют поворачиваться поворотную гильзу.
   

    = На рис. 1.5 видно, что плунжер насоса снабжен в нижней части выступом - поводком. В свою очередь поворотная гильза имеет здесь прямоугольные пазы= , в которые входит выступ-поводок плунжера. Поворачиваясь, гильза упирается в поводок плунжера, заставляя и его поворачиваться.

      В зависимости от направления хода зубчатой рейки поворотная гильза поворачивается в одну и= ли другую сторону. Нижний конец плунжера, как это видно = из рис. 1.5, оканчивается пуговкой, на которую сверху опирается шайба. Пугов= ка упирается в дно стакана - детали, напоминающей обычный стакан. Пружина прижимает плунжер ко дну стакана. Перемещение стакана ограничивается стопорным кольцом. Подвод топлива в надплунжерное пространство осуществляется через оба окна А в гильзе плунжерной пары, а перепуск при отсечке подачи топлива через одно отверстие, которое перекрывается стороной плунжера, на которой расположена спиральная кромка.

<= v:shape id=3D"_x0000_i1029" type=3D"#_x0000_t75" alt=3D"" style=3D'width:264pt;h= eight:507.75pt'>

<= span style=3D'font-family:Arial'>Рис. 1.5. Секция ТНВД дизеля Д50

Основные технические данные ТНВД дизеля Д50 представлены в табл. 1.1.



Таблица 1.1
Техническая характеристика ТНВД дизеля Д50

   &nb= sp;           

    Направление вращения вала насоса      против часовой стрелки, если смотреть с противоположной стороны регуля= тора

    Общий вид ТНВД дизеля Д50 представлен на рис. 1.6. Все шесть секций установлены на одном картере, в котором смонтирован кулачковый вал. Привод кулачкового вала от коленчатого вала дизеля осуществляется с помощью цилиндрических зубчатых колес. От общего топливного коллектора топливо поступает в каждую секцию, которая обеспечивает подачу заданной порции топл= ива под давлением в нужный момент в соответствующий цилиндр дизеля. На корпусе = ТНВД установлен регулятор, обеспечивающий нужный режим работы дизеля, электропневматический серводвигатель, который позволяет перемещать рейку секции ТНВД и соответственно устанавливать цикловую подачу топлива. Стопор секции позволяет отключать ра= боту отдельных секций ТНВД.

   &nb= sp;           


     &nbs= p;            &= nbsp;           &nbs= p;         Рис. 1.6. Общий вид топливного насоса дизеля Д50

    Как видно из продольного разреза ТНВ= Д (рис. 1.7), картер 8 представляет собой чугунную литую коробку и служит для монтажа всех деталей и крепления насоса к блоку цилиндров. В нижней части он имеет полость, в которой помещается кулачковый вал, в средней части располо= жены шесть толкателей, а на верхней обработанной плоскости картера установлены ш= есть секций насоса. Между верхней плоскостью и полостью кулачкового вала картера имеется перегородка, в которой соосно с гнездами под секции расточено шесть гнезд для толкателей.

    Рис. 1.7. Топливный насос дизеля Д50, продо= льный разрез: 1 - пружина выклю-чающего устройства;      2 - направляющий стакан; 3 - манж= ета; 4 - болт толкателя; 5 - рукоятка выключающего устройства;              6 - пружина; 7 - тяга; 8 - корпус насоса; 9 - кулачковый вал; 10 - стакан; 11 - корпус толкателя; 12 - ролик толкателя; 13 - палец толкателя; 14 - рычаг пр= едельного регулятора; 15 - корпус предельного регулятора; 16 - рычаг; 17 - гру= з; 18 - сердечник; 19 - ограничитель хода; 20 - конический штифт;             &nb= sp; 21 - шестерня регулятора; 22 - крышка; 23 - болт; 24 - пружина; 25 - регулирующая гайка; 26 - корпус привода регулятора

    Кулачковый вал предназначен для периодического перемещен= ия плунжеров насоса из нижнего положения в верхнее.= Он имеет шесть кулачков, расположенных под углом 60° друг к другу в порядке 1 - 3 - 5 - 6 - 4 - 2. Фланцы кулачкового вала обработаны и служат для присоединения: левый - регулятора числа оборотов цилиндрической шестерней, а правый - вала привода топливного насоса. Внутри кулачковый вал имеет осевое отверстие, служащие каналом для подвода масла к опорным подшипникам и регулятору. Толкатели приводят в движение плунжеры насоса. Корпус 11 толкателя стальной, цементированный с цилиндрической нару= жной поверхностью и хвостовиком, с внутренней резьбой для болта 4, предназначенн= ого для регулировки моментов начала подачи топлива плунжерами (угла опережения подачи топлива). Он снабжен шестигранником под ключ и цилиндрической головк= ой с шаровой поверхностью, на которую опирается стакан пружины плунжера. Положен= ие болта фиксируется стаканом толкателя. В нижней части корпуса имеется поперечное сквозное отверстие для бронзового пальца 13= и ролика 12. Секции топливного насоса выполнены съемными<= /span>, что позволяет их менять в процессе эксплуатации.


    1.= 2.3. Конструкция ТНВД дизеля 10= Д100      

 

 

= Рис. 1.8. Топливный насос дизеля 10Д1= 00: 1 – регулировочный болт;             &= nbsp;           &nbs= p;     2 – регулировочная рейка; 3 – болт;       &= nbsp;    4 – стрелка; 5 – прокладка; 6 – фланец;     7 – пружи= на клапана; 8 – нажимной штуцер; 9 – прокладка клапана;             &= nbsp;    10 – седло клапана; 11 – нагнетательный клапан; 12 – гильза плунжера;
13 – плунжер; 14 – шестерня плунжера;   15 – корпус насоса; 16 – кольцо пружины; 17 – пружина плунжера; 18 – тарелка пружины; 19 – стопорное кольцо;             &= nbsp; 20 – уплотнительное кольцо;             &= nbsp;         21 – стопорный винт; 22 – прокладка

       
  &= nbsp; На рис. 1.8 представлен топливный насос высокого давления дизеля 10Д100. В расточке корпуса 15 насоса установлена прецизионная пара, состоящая из плунжера 13 и гильзы 12, фиксируемой в определенном положении стопорным винтом 21. На шлицы плунжера надета шестер= ня 14, которая находится в зацеплении с регулирующей рейкой. В верхней части расположено кольцо 16, ограничивающее шестерню от осевого перемещения. Нагн= етательный клапан 11 установлен в нижней части насоса и служит для разобщения нагнетательного топливного топливопровода от подплунжерной полости. Клапан прижимается к седлу пру= жиной 7. Плунжер 13 получает поступательное движение от толкателя, к корпусу кото= рого прикреплен топливный насос. При ходе вниз плунжер перекрывает нижней кромкой окно в гильзе, сообщающее полость низкого давления А с подплунжерной полостью. С этого момента происхо= дит повышение давления топлива под плунжером и, когда сила давления топлива достигает величины, превышающей силу затяжки пружины нагнетательного клапан= а и давления под ним, клапан открывается и топливо проходит по нагнетательному трубопроводу в форсунку. Нагнетание топлива продолжается до тех пор, пока винтовая кромка плунжера откроет окно в гильзе А.
   

      При дальнейшем движении плунжера вниз топливо из подплунжерной полости по вертикальному пазу плунжера и отверстию в гильзе будет перетек= ать в полость низкого давления.
    При этом давление под плунжером резко упадет, а нагнетательный клапан под действием пружины и разности давлений топлива в трубопроводе и под плунжером опустится на седло. При ходе плунжера вверх топливо поступает из полости низкого давления в подп= лунжерную полость.  Количество топлива, подаваемого плунжером, зависит от положения винтовой кромки плунжера относительно окна в гильзе и изменяется поворотом плунжера вокруг его оси при помощи шестерни 14 и регулирующей р= ейки 2.
В дизелях Д50 используются ТНВД блочного типа. В дизелях 10Д100 установлено 2= 0 индивидуальных ТНВД, конструкция которых уже рассмотрена, по= два насоса на каждый цилиндр. Привод 10 ТНВД кажд= ого ряда осуществляется кулачковым валом. Между кулачковым валом и каждым нас= осом устанавливается толкатель, который обеспечивает перемещение плунжера ТНВД (рис. 1.9).

<= v:shape id=3D"_x0000_i1034" type=3D"#_x0000_t75" alt=3D"" style=3D'width:222pt;h= eight:394.5pt'>

<= span style=3D'font-family:Arial'>    Рис. 1.9. Толкатель и топл= ивный
насос дизелей 10Д100, 2Д= 100

   &nb= sp;    При набегании кулачка на ролик шток перемещает плунжер ТНВД вниз, что обеспечивает подачу топл= ива в цилиндр, а когда кулачек обращен к ролику тыльной стороной под действием возвратной пружины, шток поднимается и плунжер п= од действием своей пружины возвращается в исходное положение.

1.2.4. Конструкция и принцип работы форсунок дизелей= типа Д100 и Д50
    Цикловая подача топлива под большим давлением из ТНВД поступает в форсунку. Основное назначение форсун= ки - распыливание и распределение топлива по объему камеры сгорания.
    Преимущественное распространение на тепловозных дизелях получили форсунки закрытого типа, имеющие распылитель с запорной иглой. Они называются закрытыми потому, что запорная игла после впрыска топлива разобщ= ает цилиндр от объема топливного трубопровода высокого давления. По нагнетатель= ной трубке (рис. 1.10), выдерживающей большие давления, ТН= ВД подает топливо к форсунке. Однако сразу к распыливающи= м отверстиям топливо пройти не может, так как путь ему преграждает игла, конус которой плотно притерт к седлу корпуса распылителя форсунки.

       Для впрыска топлива необходимо приподнять иглу, прижатую пружиной. Это осуществляется= за счет высокого давления топлива. Впрыскивание происходит, когда давление топлива, действующее на кольцевой заплечик иг= лы, создает усилие, достаточное для сжатия пружины при подъеме иглы. При этом топливо со значительной скоростью устремляется в цилиндр дизеля через распыливающие отверстия, расположенные за иглой в н= ижней части корпуса распылителя (соплового наконечника). Начальное давление впрыска, необходимое для поднятия иглы и определяемое затяжкой пружины, составляет 20-30 МПа.

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<= span style=3D'font-family:Arial'>Рис. 1.10. Схема устройства
форсунки закрытого типа

Едва игла оторвется от своего седла, как действующее на нее усилие со стороны топлива возрастает. = Дело в том, что при закрытом положении иглы давление топлива действует не на всю поверхность конусной части. Когда игла начинает пропускать топливо к распыливающим отверстиям, общее усилие на нее возраст= ает за счет увеличения площади, на которую действуют давление топлива.
    После прекращения подачи топлива насосом давление падает= , и игла под воздействием пружины тотчас опускается. При быстром закрытии (отсе= чке) возможность подтекания, просачивания топлива из распылителя форсунки исключается. Этому способствует также следующая особенность работы топливного насоса.
    В момент отсечки (прекращение подачи топлива плунжером) = на какоето время нагнетательная полость топливного насос= а, нагнетательная трубка и полость форсунки соединяются через окно А (см. рис. 1.4) с полостью низкого давления. За счет= этого давление топлива перед иглой форсунки резко падает. Это положительно сказывается на четкой, без подтекания работе форсунки.

1.2.5. Конструкция форсунки дизеля 10Д100
    Для равномерного распределения топлива по кам= ере сгорания в форсунке имеется несколько распыливающих отверстий. Форсунка дизеля 10Д100 имеет три отв= ерстия диаметром 0,56 мм каждое.
На дизелях Д100 в каждом цилиндре имеются две форсунки, расположенные одна против другой. Для обеспечения плотности, чтоб= ы в местах их соединения с цилиндром не просачивались ни газы, ни охлаждающая цилиндры вода, форсунки крепятся с помощью промежуточной (переходной) детал= и, называемой адаптером.
Главной деталью форсунки (рис. 1.11) является распылите= ль, состоящий из корпуса распылителя и иглы, которая притирается к корпусу распылителя по цилиндрической и конической (запирающей) поверхностям. Этим достигается плотность этой пары и легкость перемещения иглы в распылит= еле. Игла прижимается к конусу корпуса распылителя усилием пружины, которое передается через тарелку, толкатель и ограничитель.
    Подъем иглы форсунки в момент впрыска обычно ограничивае= тся упором (ограничителем) и в тепловозных дизелях не превышает 0,7 мм. Форсунки тепловозных дизелей имеют, например, максимальный подъем иглы, равный 0,45 = мм (см. рис. 1.11). Несмотря на такую малую величину подъема, площадь проходно= го сечения под конусом иглы в несколько раз больше суммарной площади распыливающих отверстий.
    Топливо, поступающее от насоса, проходит щелевой фильтр, задерживающий случайно попавшие в топливо крупные частицы грязи, и направля= ется по пазам и каналам в полость, окружающую нижний конец иглы. Далее форсунка работает так, как описано выше.

&= nbsp;      Давление топлива, которое испытывают распылители, может превышать 100 МПа= , а промежутки времени, в течение которого происходит впрыск топлива под таким давлением, чрезвычайно малы: на впрыск отводятся тысячные доли секунды. В остальное время между конусом иглы и конусом корпуса распылителя топливо = не должно просочиться в цилиндр дизеля.
    Это требует высокоточного изготовления и подбора прецизионной пары: корпуса распылителя и иглы распылителя. В процессе эксплуатации распылители форсунок соприкасаются с горячими газами в цилин= дре. Это может вызвать перегрев. В результате могут измениться зазоры, возника= ет коробление, что нарушает нормальную работу форсунки. Большим недостатком топливной аппаратуры является ее ненадежная работа на режимах холостого х= ода и малых нагрузок двигателя из-за низких давлений, создаваемых в ТНВД, и некачественного распыливания цикловой подач= и.
     В результате большой работы исследователей по повышению топливной экономичности дизелей типа 10Д10= 0 конструкция форсунки претерпела изменения, которые коснулись в первую оче= редь распылителя.

<= v:shape id=3D"_x0000_i1036" type=3D"#_x0000_t75" alt=3D"" style=3D'width:267.75p= t;height:402pt'>

   Рис. 1.11. Разрез форсу= нки дизелей 10Д100, 2Д100

    На= рис. 1.12 видно, что сопловой наконечник укорочен и на нем установлена проставка 5. В проставке = есть центральное отверстие, закрытое клапаном 6 и пружиной 7. Второй канал в проставке связан с каналом Ж в сопловом наконечнике.

&= nbsp;

№ 2
ВНЕШНИЙ ТЕПЛОВОЙ БАЛАНС ДВИГАТЕЛЯ ВНУТРЕННЕГО СГОРАНИЯ


2.1= . ЦЕЛЬ РАБОТЫ
    Ознакомление с направлениями использования теплоты в двигателях внутреннего сгорания, принципами проведения теплобалансовых испытаний, численное определение значений уравнения теплового баланса двига= теля лабораторной установки.

2.2= . ВНЕШНИЙ ТЕПЛОВОЙ БАЛАНС ДВИГАТЕЛЯ ВНУТРЕННЕГО СГОРАНИЯ
    Современный двигатель является комбинированным тепло= вым двигателем, состоящим из поршневого двигателя внутреннего сгорания, газовой турбины, компрессора и целого ряда устройств для подвода и отвода теплоты, объединенных общим рабочим телом, совершающим еди= ный рабочий цикл.
    Рабочим телом единого рабочего цикла дизеля являются продукты сгорания, образующиеся в результате реакций окисления топлива.
Таким образом, дизель - это такой тепловой двигатель, в цилиндре которого происходят процессы сгорания топлива с выделением теплоты и преобразования тепловой энергии в механическую.
Основными отличиями дизеля являются:
- высокая степень сжатия;
- работа на тяжелом жидком топливе;
- внутреннее смесеобразование, т.е. раздельное поступление в цилиндр топлив= а и воздуха;
- самовоспламенение топлива от сжатия.
Дизельные двигатели нашли наибольшее распространение на теплово-зах и в судовых тепловых установках.
Другой наиболее распространенный тип двигателя внутреннего сгорания - карбюраторный. Основные отличия этого теплового двигателя:
- низкая степень сжатия воздуха;
- работа на легком жидком топливе;
- внешнее смесеобразование, т.е. рабочая смесь паров топлива и воздуха образуется в карбюраторе, за пределами цилиндра;
- принудительное воспламенение рабочей смеси.
Карбюраторные двигатели преимущественно используются на автомобильном транс= порте.
Тепловая энергия, выделяющаяся при сгорании топлива в цилиндрах двигателя, = лишь частично используется для совершения эффективной работы. Значительная часть тепла теряется с выпускными газами, охлаждающей водой и смазочным маслом, вследствие неполноты сгорания и др.
Внешним тепловым балансом двигателя внутреннего сгорания называется распределение теплоты, выделяющейся при сгорании топлива в камере сгорания,= на отдельные составляющие, включающие как полезно используемую теплоту, так и потери теплоты.
    Тепловой баланс можно определять на различных режимах ра= боты двигателя. Это позволяет выяснить, как изменяются тепловые потери при измен= ении нагрузки и числа оборотов. Тем самым появляется возможность оценить характер изменения экономичности в зависимости от режима работы двигателя.
    Во всех случаях тепловой баланс определяется только на установившихся режимах работы двигателя, когда с течением времени не изменя= ются температуры охлаждающей воды, смазочного масла и выпускных газов, нагрузка и частота вращения коленчатого двигателя.
    Для проведения испытаний используется лабораторная установка, схема которой представлена на рис. 2.1.

    Рис. 2.1. Схема лабораторной установки: 1 - впускной коллектор; 2 - термометр воздуха, поступающего в дизель; 3 - подводы охлаждающей воды; 4 - термометр охлаждающей воды на в= ходе в дизель; 5 - бачок для определения расхода топлива; 6 - дизель; 7 - выпускной коллектор; 8 - термометр выпускных газов; 9 - отвод ох-лаждающей воды; 10 - термометр охлаждающей воды = на выходе из дизеля; 11 - амперметр генератора; 12 - вольтметр генератора; 13 - бачок охлаждающей воды; 14 - весы для замера расхода охлаждающей воды; 15 - генератор постоянного тока

    Це= лью лабораторной работы является овладение методикой расчета составляющих внешн= его теплового баланса на основе проведения испытаний двигателя внутреннего сгорания, овладение навыками пользования измерительной аппаратурой и обрабо= тки опытных данных.

2.3= . РАСЧЕТ ВНЕШНЕГО ТЕПЛОВОГО БАЛАНСА
    Внешним тепловым балансом ДВС является распределение общего количества теплоты, внесенной в цилиндр на основные составляющие, на которые расходуется подводимая теплота. Обозначим общее количество теплоты, внесенной в цилиндр за час, , а сумму расходных составляющих   , тогда уравнение внешнего тепл= ового баланса будет иметь вид

           = ;            &n= bsp;            = ;            &n= bsp;            = ;            &n= bsp;            = ;            &n= bsp;            = ;         (2.1)

или ,             &nb= sp;            =             &nb= sp;            =             &nb= sp; (2.2)

где – общее количество располагаемой теплоты топлива; – количество физической теплоты, внесенной топливом в цилиндр; – количество физической теплоты, внесенной воздухом; – количество теплоты, преобразованной в эффективную мощность дизе= ля.

При проведении лабора= торной работы величинами и можно пренебречь ввиду их малости:

,             &nb= sp;            =             &nb= sp;            =             &nb= sp;            =             &nb= sp;            =             (2.3)

где В – часовой расход топлива, кг/ч; Н<= sub>и – теплота сгорания дизельного топлива, Ни =3D 42700 кДж/кг;

,             &nb= sp;            =             &nb= sp;            =             &nb= sp;            =             &nb= sp;            =             &nb= sp;   (2.4)

где – эффективная мощность дизеля, кВт.

Во время испытаний , кВт, определяется по выходным параметрам генератора, который приводится в действие дизелем:

,             &nb= sp;            =             &nb= sp;            =             &nb= sp;            =             &nb= sp;            =             &nb= sp;  (2.5)

где I – сила тока, А; V – напряжение, В; =3D 0,9 – КПД генератора.

– количество теплоты, которое уносится выпускными газами:

,             &nb= sp;            =             &nb= sp;            =             &nb= sp;            =             &nb= sp;            =             (2.6)

где – количество выпускных газов, кг/ч; – теплоемкость выпускных газов, кДж/кг= · ° С; – температура выпускных газов, ° С.

Для расчетов можно пр= инять @ 1,05–1,08 кДж/кг· ° С.

Количество выпускных = газов можно определить по уравнению

           = ;            &n= bsp;            = ;            &n= bsp;            = ;            &n= bsp;            = ;            &n= bsp;     (2.7)

или=

,             &nb= sp;            =             &nb= sp;            =             &nb= sp;            =             &nb= sp;        (2.8)<= /span>

    гд= е – количество воздуха, поступившего в цилиндр дизеля; – коэффициент избытка воздуха или воздушно-топливное отношение, <= v:shape id=3D"_x0000_i1066" type=3D"#_x0000_t75" alt=3D"" style=3D'width:16.5pt;he= ight:18pt'> =3D 1,7; – коэффициент продувки, =3D 1,05 – 1,15; – молекулярная масса выпускных газов воздуха, =3D 28,95 кг/кмоль; – теоретически необходимое количество воздуха для полного сгорани= я 1 кг топлива. Для дизельного топлива, имеющего следующий элементарный состав:= С =3D 0,87; Н2<= sub> =3D 0,126;
О =3D 0,004, величина =3D 0,5 кмоль/кг.

может быть определено экспериментально= с использованием расходомерного устройства.<= /o:p>

– количество теплоты, уносимое охлаждающей водой:

,             &nb= sp;            =             &nb= sp;            =             &nb= sp;             (2.9)

где – количество охлаждающей воды, кг; – теплоемкость охлаждающей воды, кДж/кг· ° С,= =3D 4,2 кДж/кг· ° С; , – температура охлаждающей воды соответственно на входе и выходе из дизеля.

– остаточный член управления типового баланса, включающий неучтен= ные в эксперименте потери теплоты:

.



2.4= . ПОРЯДОК ПРОВЕДЕНИЯ ЛАБОРАТОРНОЙ РАБОТЫ=
    Время проведения испытаний , устанавливается преподавателем. Для записи показателей измерительных прибор= ов и других операций составляют табл. 2.1.

аблица2.1

Результаты измерений

№ замера

, кг

 , кг

 , °= С

 , °= С

 I, А

V, В

, °= С

 , кВт=

, кг/ч

1

 

 

 

 

 

 

 

 

 

2

 

 

 

 

 

 

 

 

 

3

 

 

 

 

 

 

 

 

 

4

 

 

 

 

 

 

 

 

 

5

 

 

 

 

 

 

 

 

 

6

 

 

 

 

 

 

 

 

 

7

 

 

 

 

 

 

 

 

 

среднее значение

 

 

 

 

 

 

 

 

 

    Для подсчета часового расхода, кг/ч, используется выражение

,             &nb= sp;            =             &nb= sp;            =             &nb= sp;            =             &nb= sp;            =         (2.10)<= /span>

где – расход топлива за время в минутах.

Аналогично рассчитыва= ется .

    По= сле выполнения расчетов, указанных в п. 2.4, уравнение теплового баланса можно представить в таком виде:

,             &nb= sp;            =             &nb= sp;            =             &nb= sp;            =           (2.11)

 

,             &nb= sp;            =             &nb= sp;            =             &nb= sp;            =          (2.12)

 

,             &nb= sp;            =             &nb= sp;            =             &nb= sp;            =             &nb= sp;    (2.13)

    гд= е – относительная доля теплоты, перешедшая в эффективную мощность, = , т.е. это есть эффективный КПД; – относительная доля теплоты, унесенная выпускными газами; – относительная доля теплоты, перешедшая в охлаждающую воду; – относительная доля невязки баланса.

    На основе анализа полученных данных после выполнения лабораторной работы необходимо сравнить их с данными современных тепловозных дизелей.



2.5= . КОНТРОЛЬНЫЕ ВОПРОСЫ
1. Что называется внешним тепловым балансом?
2. Какие составные части теплового баланса вы знаете?
3. В каких пределах измеряется относительная доля теплоты, уносимая выпускн= ыми газами?
4. Чему равен эффективный КПД дизеля?
5. Чему равна относительная доля теплоты, уносимая охлаждающей водой?
6. Чему равна теплота сгорания дизельного топлива?
7. Какие величины измеряются при проведении лабораторной работы?
8. Как подсчитать количество теплоты, вносимой в цилиндр топливом?
9. Как определить мощность дизеля?
10. Как подсчитать количество теплоты, уносимой выпускными газами?
11. Как подсчитать теплоту, уносимую охлаждающей водой?

3. Лабораторн= ая работа № 3
ОПРЕДЕЛЕНИЕ У= ГЛА ОПЕРЕЖЕНИЯ ПОДАЧИ ТОПЛИВА

3.1. ЦЕЛЬ РАБОТЫ<= b>
  &= nbsp; Изучение принципов регулирования угла опережения подачи топлива, методов определения этой характеристики в эксплуатации.

3.2. ПРИНЦИПЫ РЕГУЛИРОВАНИЯ УГЛА ОПЕРЕЖЕНИЯ ПОДАЧИ ТОПЛИВА

   Угол опережения подачи топлива (УОПТ) является одной из важнейших регулировочных характеристик дизеля. Своевременность подачи топлива в цилиндры двигателя= во многом определяет качественные и количественные параметры рабочего процес= са дизеля в целом. Для понимания принципов регулирования УОПТ рассмотрим упрощенно процесс топливоподачи насосом высокого давления (рис. 3.1). При работе секции насоса плунжер 4 вместе с толкателем 2 совершает возвратно-поступательное движение под действием вращающегося кулачка 1 и пружины 6. При движении плунжера вниз топливо через канал А во втулке заполняет надплунжерное пространств= о.     В начале движения плунжера вверх плунжер вытесняет час= ть топлива через впускное отверстие втулки в питательный канал.     Геометрический момент начала подачи топлива, соответствующий так называемому геометрическому УОПТ= , определяется моментом перекрытия впускного отверстия = А втулки верхней кромкой плунжера. С этого момента при дальнейшем движении плунжера вверх происходит сжатие топлива в надплунже= рной полости, а при достижении давления, при котором открывается нагнетательный клапан, также и в полостях трубопровода высокого давления, и в форсунке. В цилиндр топливо поступит только после подъема иглы форсунки. Этот момент называют действительной подачей топлива, а УОПТ соответственно действительным или фактическим УОПТ.

<= /span>

Ри= с. 3.1. Схема топливного насоса: А – питательный канал; 1 – кулачок;
2 – ролик толкателя;            3 – толкател= ь; 4 – плунжер;
5 – пружина нагнетательного клапана;   6 – возвратная пружина плунжера

Воздействовать на вел= ичину геометрического момента начала подачи топлива можно двумя основными направлениями. Во-первых, поворотом кулачкового вала топливного насоса относительно верхней мертвой точки (ВМТ) в цили= ндре. Как правило, такая возможность имеется у большинства типов дизелей за счет взаимного смещения полумуфт привода топливного насоса или изменением сцепле= ния зубчатых колес передачи от коленчатого вала к кулачково= му. Вращая полумуфты относительно друг друга, можно изменить УОПТ в значительных пределах. Такую регулировку выполняют обычно при установке топливного насоса на дизель после замены или ремонта, а в эксплуатации к такой регулировке прибегают редко. Во-вторых, изменить момент перекрытия плунжером отверстия А (см. рис. 3.1) можно, если конструктивно предусмотреть возможность изменения расстояния h, при этом обеспечивается большая точность и "плавность" изменения УОПТ= . Это достигается или установкой регулировочных прокладок между толкателем и плунжером (рис. 3.2, б), или наличием в конструкции толкателя регулировочно= го винта (рис. 3.2, а).

<= /span>

Ри= с. 3.2. Фрагмент конструкции топливного насоса:     а – с резьбовой регулировкой (дизель 11Д45);              = б – с регулировкой прокладками (Д70); 1 – кулачок;      2 – ролик толкателя; 3 – толкатель; 4 – регулиро= вочный винт; 5 – тарелка пружины; 6 – хвостовик плунжера; 7 – регулировочные прокладки

        Кроме тог= о, в малой степени на момент начала подачи топлива можно повлиять еще и измене= нием затяжки пружины нагнетательного клапана насоса или возвратной пружины форсунки. Однако назначение этих элементов топливной аппаратуры иное: нагнетательный клапан должен разобщать полости форсунки и насоса в промеж= утки между впрысками, а пружина форсунки предназначена для регулировки давления топлива в момент впрыска. От величины давления начала подачи топлива зави= сит качество распыления топлива и последующего смесеобразования в цилиндре.



3.3= . МЕТОДЫ ОПРЕДЕЛЕНИЯ УОПТ<= /span>

    Определение геометрического момента начала подачи топлива осуществляют с помощью простого устройства = - моментоскопа (рис. 3.3). Момен= тоскоп устанавливают на регулируемом насосе (секции насоса), проворачивают вал дизеля с помощью валоповоротного устройства до заполнения стеклянной трубки топливом, примерно на половину ее рабочей высоты. Далее медленно поворачивают коленчатый вал двигателя. В момент на= чала подачи топлива в этой трубке будет хорошо видно движение мениска топлива вверх. По градуированному диску определяют угол, при котором происходит начало подачи топлива. Определение момента начала подачи следует произвес= ти два-три раза. Опытный регулировщик может установить этот угол с точностью= до 1°.
    Описанный метод часто называют способом определения УОПТ "по мениску". Преимущества этого мет= ода - простота устройств, универсальность, наглядность. Недостатки - необходимо= сть частичной разборки топливной системы, трудоемкость, сравнительно невысокая точность.

=         Рис. 3.3. Моментоскоп:    = ;     1 – штуцер насоса; 2 – пружина нагнетательного клапана;
3 – наконечник; 4 – нажимное кольцо; 5 – стеклянная трубка;   6= – резиновая трубка


  &= nbsp; Среди методов определения фактического (действительного) УОПТ наибольшее распространение на железнодорожном транспорте получил метод, основанный на измерении начала перемещения иглы форсунки. Требуемое оборудование включает: специализированный компьютер, датчик угла поворота коленчатого вала, датчик перемещения иглы форсунки, блоки питания и сопряже= ния сигналов. В качестве датчика хода иглы форсунки применяют магнитоиндукционн= ый преобразователь, который закрепляют на форсунке таким образом, чтобы его подвижная часть (сердечник катушки) при работе форсунки двигалась вместе с иглой. Следует отметить, что среди тепловозных дизелей только топливная аппаратура дизеля 10Д100 позволяет применить по= добные датчики без переделки конструкции форсунки. Согласуя сигналы с датчика угла поворота коленчатого вала и магнитоиндукционного датчика, получают диаграмму вида, подобного диаграмме рис. 3.4.

           &n= bsp;            = ;   

                         &nbs= p;             Рис. 3.4. Диаграмма хода иглы форсунки

    По диаграмме легко определяются моменты начала подъема иг= лы форсунки (т. Ф) и посадки иглы в седло (т. К), продолжительность подачи топлива, ход иглы h и ряд других важных характе= ристик топливоподачи. Наряду с высокой дополнительной информативностью такого спос= оба определения УОПТ, к достоинствам последнего сле= дует отнести точность и достовер-ность<= /span> измерений, а к недостаткам - сложность оборудования, значительные затраты времени на оснащение дизеля датчиками, неуниверсальнос= ть.
    Существует способ определения действительного УОПТ, основанный на анализе кривой давления в нагнетательном топливопроводе (рис. 3.5). Получ= ить такую диаграмму можно, установив в трубке высокого давления (ближе к форсун= ке) датчик давления.


     &nbs= p;            &= nbsp;         Рис. 3.5. Диаграмма давления топлива перед форсункой

    Повышение давления на участке, предшествующему Н, соответствует началу подачи топлива насосом, а сам участок Н обычно связыва= ют с открытием нагнетательного клапана и началом формирования волны давления на участке "ТНВД - форсунка". Дальнейшее повышение давления топлива вызвано продолжающимся движением плунжера ТНВД вверх. Падение давления после т. Ф обусловлено начавшимся движением иглы форсунки вверх, а следовательно, расх= одом топлива через сопла форсунки. На последующих участках возможно некоторое повышение давления топлива (в данном случае оно значительно), что связано с продолжающейся со стороны = ТНВД подачей топлива. Как правило, такая картина наблюдается на режимах большой производительности насоса. Прекращение подачи топлива насосом (отсечка) характеризуется резким снижением давления. Минимум первой полуволны на этом участке (т. К) соответствует посадке иглы на место (завершение подачи топли= ва). Наряду с действительным УОПТ, по диаграмме давл= ения можно судить еще о целом ряде диагностических характеристик топливной аппаратуры: величине давления начала подачи топлива, плотности запорного ко= нуса форсунки, цикловой подаче и др. Существенным недостатком такого метода след= ует признать необходимость изменения длины и объема нагнетательного топливопровода, что может исказить процесс топливопод= ачи. Кроме того, установка датчика давления в топливопровод= требует значительных дополнительных затрат времени. Необходимо отметить, что существуют устройства для измерения давления жидкости "через стенки трубопровода". Хотя их применение и приведет к некоторому удорожанию оборудования, зато указанные выше недостатки могут быть устранены.
    Наиболее полно требованию удобства установки на двигатель измерительного оборудования отвечает способ измерения = УОПТ по виброграмме (рис. 3.6). Датчик (акселерометр) закрепляют на корпусе форс= унки или на нагнетательном трубопроводе c помощью магнитного крепления или пружинного зажима.

   &nb= sp;            =    

            =             &nb= sp;         Рис. 3.6. Виброграмма эталонной форсунки = дизеля 10Д100

    Реализация сигнала, показанная на рис. 3.6, содержит три характерных участка. Передний фронт первого импульса соответствует удару иг= лы об ограничитель (Ф), второго - удару иглы при посадке о седло (К). Эти импу= льсы отличаются высокой амплитудой и частотой сигнала. Участок между ними содерж= ит низкочастотные колебания, вызванные гидродинамическими явлениями, сопровождающими подачу топлива в цилиндр двигателя. В качестве недостатка применения данного метода для определения УОПТ следует указать наличие существенных виброакустических= помех, сопровождающих работу многоцилиндрового дизеля, что усложняет анализ реальных виброграмм. Однако применение компьютера для обработки вибросигнала может устранить указанный недостаток. Сл= едует отметить, что в точности этот метод несколько уступает методам, описанным в= ыше. Главным преимуществом можно считать универсальность: измерительное оборудов= ание одинаково хорошо работает с любыми форсунками закрытого типа.




3.4. ОБЪЕКТ ИССЛЕДОВАНИЙ И ОБОРУДОВАНИЕ
1. Дизель 1Ч8,5/11,5.
2. Моментоскоп.
3. Измерительный комплекс "Вектор".

3.5. ПОРЯДОК ВЫПОЛНЕНИЯ РАБОТЫ 1. Изучить способы регулировки и определения УОПТ<= /span>.
2. Определить величину геометрического УОПТ с помощью моментоско-па. Измерения выполнить не менее трех раз. Результаты занести в табл. 3.1.
3. С помощью компьютерного измерительного комплекса "Вектор" опре-делить диаграмму давл= ения топлива перед форсункой.
4. По распечатанной диаграмме давления топлива определить действи-тельный УОПТ. Результат занести в табл. 3.1.
5. В выводе работы сопоставить величины геометрического= и действи-тельного УОПТ, объяснить их расхождение.


Таблица 3.1


Результаты измерений УОПТ

№ опыта

Геометрический УОПТ

Действительный УОПТ

отметка на диске

УОПТ, о

среднее значение, о

УОПТ, о

среднее значение, о

1

 

 

 

 

 

2

 

 

 

3

 

 

 

<= span style=3D'font-family:Arial'>4

 

 

 

   &nb= sp;          

3.6. КОНТРОЛЬНЫЕ ВОПРОСЫ
1. В чем различие между действительным и геометрическим углом опережения подачи топлива?
2. Каким образом можно изменить величину УОПТ д= изеля?
3. Принцип определения УОПТ по "мениску&qu= ot;.
4. Принципы определения действительного УОПТ. 5. В чем заключаются основные недостатки и преимущества используемых в настоящей работе способов определения УОПТ?
6. Какой из рассмотренных способов определения УОПТ вам представляется наиболее подходящим для условий депо или завода?<= /p>

4. Лабораторн= ая работа № 4
ВЛИЯНИЕ УГЛА ОПЕРЕЖЕНИЯ ПОДАЧИ ТОПЛИВА НА ПОКАЗАТЕЛИ РАБОТЫ ДИЗЕЛЯ
4.1. ЦЕЛЬ РАБОТЫ<= span class=3DGramE>
Теоретически и экспериментально оценить влияние угла опережения подачи топлива на показатели работы дизеля.

4.2= . ТЕОРЕТИЧЕСКИЕ СВЕДЕНИЯ=

&= nbsp;       Для выявления механизмов влияния угла опережения пода= чи топлива на показатели работы дизеля выполним анализ процесса сгора= ния по индикаторной диаграмме. Традиционно различают четыре фазы сгорания топ= лива в цилиндре дизеля (рис. 4.1).

       Первая фаза I - задержка самовоспламенения топлива. Длительность фазы определяется от момента начала подъема иглы форсунки (т. 1) до начала сгорания (т. 2) и зависит от ряда условий. Решающее значение оказывают состояние рабочего т= ела в цилиндре в момент начала подачи топлива (прежде всего температура) и свойства топлива (цетановое число).

=           Рис. 4.1. Фазы сгорания: p – кривая давления в цилиндре; T – кривая температуры; jоп – УОПТ

Вторая фаза <= span class=3DSpellE>II - фаза быстрого сгорания. Границей этой фазы принято считать момент достижения максимального давления в цилиндре двигателя (т.3). В течение этой фазы сгорает большая часть топлива, накопившегося за период задержки самовоспламенения. Скорость повышения давления, определяющая жестк= ость сгорания, во многом зависит от количества топлива, поданного в цилиндр в пе= рвой фазе: чем больше это количество, тем выше скорость нарастания давления, выше жесткость работы дизеля. С другой стороны, на жесткость процесса сгорания оказывает влияние и момент начала сгорания топлива (абсцисса точки 2).
    Третья фаза III - основное сгорание. Начало треть= ей фазы определяется положением максимума давления (т. 3), а конец - положением максимума температуры газов в цилиндре (т. 4). При высоких температурах, достигаемых в третьей фазе, преобладающее влияние на сгорание оказывают продолжающиеся процессы смесеобразования, в частности диффузия (перемешиван= ие топлива с воздухом). Поэтому длительность третьего периода сгорания в основ= ном определяется степенью совершенства подвода воздуха к топливу и продуктам его частичного окисления.
    Четвертая фаза= IV - догорание топлива и продуктов его неполного окис-ления= . Начало этой фазы приходится на момент максимума температуры в цилиндре (т. 4), кон= ец (т. 5) - на момент максимума кривой тепловыделения (кривая не показана). Пе= риод характеризуется отсутствием подачи свежего топлива в цилиндр, увеличением скорости поршня. Количество неиспользованного воздуха в цилиндре к этому моменту невелико, поэтому догорание топлива происходит сравнительно медленн= о. Теплота, выделяющаяся в этот период, используется малоэффективно, так как степени расширения газа на этой части хода поршня малы.
Регулируя УОПТ, можно воздействовать на протека= ние рабочего процес-са в цилиндрах двигателя.

&n= bsp;        Рис. 4.2. Индикаторные диаграммы: 1 – нормальный УОП= Т (j<= sub>оп1);   2 – ранний впрыск (jоп2)

        Увеличение УОПТ - смещение т.1 (см. рис. 4.1) влево. Если условия в цилиндре (температура, количество воздуха и др.) остаются по-прежнему благоприятными, то при увеличении УОПТ существенного изменения продолжительности перв= ой фазы сгорания не наблюдается, поэтому видимое сгорание наступает раньше. Протекание фазы быстрого сгорания приходится на участок до ВМТ, поэтому сопровождается большей скоростью повыш= ения давления (увеличивается жесткость сгорания), ростом максимального давления сгорания (рис. 4.2).

Значительное увеличение УОПТ. При слишком больших значения= х УОПТ (5-10о и более от оптимальной величины) наблюдается заметное увеличение периода задержки самовоспламенения (первая фаза сгорания). Это объясняется недостаточно высо= кой температурой воздуха в цилиндре. Поэтому к моменту воспламенения в цилиндре скапливается большая массовая порция топлива, что при сгорании вызывает рез= кое повышение скорости нарастания давления, максимального давления.
    Так как при ранней подаче топлива значительная доля рабо= ты, совершаемой газами, приходится на участок до ВМТ, то экономические показатели работы дизеля, как правило, ухудшаются. Кроме того, увеличение жесткости сгорания, рост давления в цилиндре приводит к повышению механической и термической напряженности дизеля.
    По субъективной оценке, работа дизеля с ранней подачей топлива со-провождается отчетливо слышимыми стуками.

    Уменьшени= е УОПТ в незначительных пределах (до 5о= ) мало влияет на длительность периода задержки самовоспламенения. Поэтому п= ри позднем впрыске топлива в цилиндр будет наблюдаться и более позднее начало сгорания (линия 2 на рис. 4.3). К этому моменту времени поршень уже движе= тся к НМТ, скорость поршня увеличивается, что при= водит к уменьшению максимального давления сгорания и не эффективному использова= нию теплоты в цилиндре. Завершение сгорания наступает заметно позже нормально= го, а иногда продолжается и вне цилиндра: в выпускном коллекторе, в проточной части турбины и т.п. Температура отработавших газов увеличивается. На слух двигатель работает мягко. Мощность двигателя уменьшается.

Рис. 4.3. Индикаторные диаграммы: 1 – нормальный УОПТ ( j= оп1); 2 – поздний впрыск (jоп2)

При значительном уменьшении УОПТ (при впрыске вблизи или за ВМТ) сгорание в теку= щем цикле может вообще не наступить, так как температура воздуха при начавшемся= в цилиндре расширении уменьшается и может оказаться недостаточной для воспламенения. Вследствие несовершенства очистки цилиндра, не сгоревшее топ= ливо частично остается в цилиндре и может самовоспламениться в следующих циклах.= При этом сгорание наступает как при ранней подаче топлива (см. рис. 4.2). Поско= льку количество топлива, оказавшееся в цилиндре к началу сгорания, зависит от мн= огих величин, в том числе и случайных, то и сам процесс сгорания непрогнозируем и неуправляем. Двигатель работает с перебоями и сильными стуками.
    Таким образом, существует некоторое оптимальное значение= УОПТ, обеспечивающее наиболее совершенное сгорание то= плива в цилиндре. Необходимо понимать, что это оптимальное значение не может оставаться неизменным на всех режимах работы двигателя. И в большей мере зд= есь сказывается скоростной режим: при больших частотах вращения вала дизеля вре= мя задержки воспламенения топлива потребует соответственно большего угла повор= ота коленчатого вала. Быстроходные дизели, работающие в широком скоростном диапазоне (от 700 до 4000 мин-1), имеют, как правило, устройства для автоматической корректировки УОПТ в зависимости= от частоты вращения коленчатого вала. Тепловозные дизели, эксплуатируемые в настоящее время на отечественных железных дорогах (табл. 4.1), таких устрой= ств не имеют.             &nb= sp;            =                        

&nb= sp;            =             &nb= sp;            =             &nb= sp;     Таблица 4.1

Геометрический УОПТ тепловозных дизелей             &nb= sp;            =             &nb= sp;         

Дизель

УОПТ

ПД1М, Д50М<= /span>

29

10Д100

10

14Д40

20

2Д70, 12Д70=

21

Д49 (модификации)

26–29


    Регулируя УОПТ, можно воздействовать на вид индикаторной диаграммы и на положение максимума давле= ния с тем, чтобы установить оптимальное по показателям мощности и экономичности значение угла. Для четырехтактных дизелей величину УОП= Т подбирают таким образом, чтобы сгорание начиналось ближе к ВМТ, а для двухтактных дизелей - несколько раньше ВМТ, чтобы максимум сгорания приходился на 6-8о посл= е ВМТ. Различие связано с тем, что у двухтактного двига= теля меньшая часть хода поршня на рабочем такте посвящена сгоранию - расширению (раньше открываются выпускные органы). Следовательно, рабочий процесс надо организовать таким образом, чтобы к моменту начала выпуска сгорание было закончено.
    Необходимо помнить, что одним изменением УОПТ нельзя полностью компенсировать изменение задержки самовоспламенения, вызва= нное неисправностями двигателя или прочими изменившимися условиями.

4.3= . ОБЪЕКТ ИССЛЕДОВАНИЙ И ОБОРУДОВАНИЕ
1. Дизель 1Ч8,5/11,5.
2. Компьютерный измерительный комплекс "Вектор".

4.4= . ПОРЯДОК ВЫПОЛНЕНИЯ РАБОТЫ<= br> 1. Дизель к началу измерений должен быть прогрет в течение не менее двух часов.
2. Анализом диаграммы давления топлива перед форсункой определить текущий у= гол опережения подачи топлива.
3. По осредненной не менее чем за 100 циклов индикаторной диаграмме определ= ить: максимальное давление сгорания pz; угол поворота коленчатого вала jpz ; угол, соответствующий началу видимого сгорания j1 ; среднее индикаторное давлени= е в цилиндре pi

4. Определить часовой расход топлива В, температуру отработавших газов= T, эффективную мощность дизеля P= e.
5. Изменить УОПТ на 2–3о , не изменяя цикловую подачу топлива. После изменения режима дать двигателю поработать не менее 10 мин, не производя измерений. Повторить пп. 2-4.
6. Повторить п. 5 для разных УОПТ. Результаты измерений занести в табл. 4.2.
7. Рассчитать удельный индикаторный bi и удельн= ый эффективный be расходы топлива. Результаты расч= ета свести в табл. 4.2.
8. Построить графики T, p<= sub>z, jpz, bi= , be =3D f= (jоп). Сделать вывод.

Таблица 4.2

Результаты опытов

Показатель

Измерение

1

2

3

4

УОПТ, jоп, о

 

 

 

 

Максимальное давле= ние сгорания pz, МПа

 

 

 

 

Угол максимума дав= ления jpz, о

 

 

 

 

Угол, соответствую= щий началу видимого сгорания j1, о

 

 

 

 

Среднее индикаторн= ое давление в цилиндре pi, Па

 

 

 

 

Часовой расход топ= лива В, кг/ч

 

 

 

 

Температура отрабо= тавших газов T, К<= /span>

 

 

 

 

Эффективная мощнос= ть Pe, кВт

 

 

 

 

Индикаторная мощно= сть Pi, кВт; Pi =3D (pi Vh = n)/(30 t),
где Vh – рабочий объем, м3; t =3D 4 – для четырехтактных двигателей, t = =3D 2 – для двухтактных

 

 

 

 

Удельный индикатор= ный расход топлива bi, кг/кВт· ч,
bi <= /i>=3D В / Pi

 

 

 

 

Удельный эффективн= ый расход топлива be, кг/кВт· ч,
be =3D В / Pe

 

 

 

 



4.5= . КОНТРОЛЬНЫЕ ВОПРОСЫ
1. От чего зависит продолжительность периода задержки самовоспламе-нения?
2. Как меняется температура отработавших газов при увеличении и уменьшении = УОПТ?
3. Влияет ли величина УОПТ на жесткость сгорани= я?
4. Меняется ли максимальное давление сгорания при регулировке УОПТ?
5. Как сказывается отклонение УОПТ от оптимальн= ого значения на ресурс двигателя?



СПИ= СОК ЛИТЕРАТУРЫ
1. Двигатели внутреннего сгорания (тепловозные дизели и газотурбинн= ые установки) / А.Э. Симсон, А.З. Хомич, А.А. Кури= ц и др. - М.: Транспорт, 1987. - 536 с.
2. Двигатели внутреннего сгорания. Устройство и работа поршневых и комбинированных двигателей / Под ред. А.С. Орлин= а и М.Г. Круглова. - М.: Машиностроение, 1990. - 288 с.
3. Федотов Г.Б., Левин Г.И. Топливные системы тепловозных дизелей. Ремонт, испытания, совершенствование. - М.: Транспорт, 1983. - 192 с.
4. Диагностика дизелей автотракторного типа / Н.С. Жда= новский, Б.А. Улитковский, В.А. Аллилуев и др. - Л.: Кол= ос, 1973. - 264 с.

 

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