MIME-Version: 1.0 Content-Type: multipart/related; boundary="----=_NextPart_01C3EE4C.51C201E0" 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_01C3EE4C.51C201E0 Content-Location: file:///C:/EB73C5D3/SUEP-3.htm Content-Transfer-Encoding: quoted-printable Content-Type: text/html; charset="windows-1251" При работе в линейном режиме DUВХ =3D UВХ(–) – UВХ(+) »0

При работе в линейном = режиме DUвх =3D Uвх(–) – Uвх(+) »0. При напряжении питания ±15В напряжение насыщения Uнас =3D ±13В (см. рисунок 3.52)= .

                      =     

Рисунок 3.51                                                      Рисунок 3.52

 

.

Пример – пусть К<= span style=3D'text-transform:uppercase'>оу =3D 26000 (10000 = £ Коу = £ 100000)

1мВ – перевод ОУ с одного уровня на другой.

а)                                                                         б)=

Ри= сунок 3.53

 

1.= 1.1      =   Основные схемы включения ОУ<= /span>

 

Правила для анализа схем ОУ:

- DUвх »0  (т.к. Коу= ® = ¥);

- по входу ОУ не потре= бляет ток Iвх =3D 0  (т.к. большое входное сопротивление Rвх ® ¥).

 

Инвертирующее включени= е

 

а) В соответствии с  рисунком 3.53а, напряжение на выходе ОУ=

,

Рисунок 3.54

где  –  на инвертирующем входе.

U<= /span>вых =3D –Ioc = ×Roc  (т.к. DUвх =3D 0),

где Ioc =3D I1  (т.к. Rвх оу =3D ¥);  (т.к. DUвх =3D 0).

Тогда  .

б) Инвертирующий сумма= тор (рисунок 3.53б)

Во входной цепи два независимых контура и I1 не влияет на I2 (см. рисунок 3.54). Выходной сигнал Uвых находится методом суперпозиции.

 

,

где ; .

Коэффициент передачи по каждому входу разный К1, К2 и К1 =3D К2 только при равенстве входных сопротивлений

К<= sub>1 =3D К2, если R1 =3D R2.<= /p>

Инвертирующее включение применяется:

- для масштабного преобразования и инверсии сигнала;

- для суммирования сиг= налов с инверсией.

 

Неинвертирующее включе= ние

 

а) Изолирующий повтори= тель (рисунок 3.55а)

Uвых =3D Е1 (DUвх =3D 0)

б) Неинвертирующий уси= литель (рисунок 3.55б)

Uвых =3D Ioc= ×Roc + I= 1×R= 1,

где Ioc =3D I1  (т= .к. Rвх =3D ¥); I1 =3D E1/R1  (= DUвх =3D 0).<= /p>

 Uвых= =3D E1/R1= ×(Roc + R1) =3D E1×= (Roc/R1= + 1) =3D K(+)×= E1,

где К(+) – коэффициент усиления.

; .

в) неинвертирующий сум= матор (рисунок 3.55в)

Uвых =3D Uвх= ×(Roc/R + 1) =3D {Roc =3D R} =3D 2<= /span>×Uвх (+).

Uвх (+) =3D ?

Контур К (см. рисунок 3.55в):  E1= – E2 =3D I×(R1 + R2);

;

 при R1=3DR2;

.

Если R =3D R1 =3D R2 =3D Roc , то  Uвых =3D Е1 + Е2.

В данном случае источн= ики входных сигналов Е1, Е2 действуют друг на друга, чего нет в системах с инвертирующим включением.

б)

а)

Применяются для масштабного преобразования и суммирования сигнала без инверсии.

в)

Рисунок 3.55

 

 

1.= 1.2      =   Схемы включения ОУ с огранич= ением входного сигнала

Ограничение выходного сигнала используется для ограничения величины задающего входного сигнала на внутреннем контуре регулирования в системах с подчиненным регулированием па= раметров.

 

1)      Схемы включения с нерегулируемым ограничением входного сигнала

 

В соответствии с рисун= ком 3.56, ограничение осуществляется за счет введения нелинейных элементов в це= пь обратной связи ОУ.

=             

= а)

                               

б)

                                

в)

Рисунок 3.56

  ;

–(UCT VD2 += DUVD1) £ U= вых £ UCT VD1 + = DUVD2,

где Uст – напряжение стабилизаци= и;

DUVD – падение напряжения на ди= оде (DUVD = »1В).=

 

2)      Схема включения с регулируемым ограничением выходного сигнала

 

Принцип классического ограничения состоит в том, что для ограничения выходного сигнала на заданном уровне на вход ОУ следует подавать сигнал в противофазе с задающим.

 

а)

 

 

 

При любом сигнале на в= ыходе за счет подачи напряжения смещения с потенциометров R2, R3<= /sub> на выходе компараторов А2 и А3 будут действовать напряжения обратные для диодов VD2, VD3 (см. рисунок 3.57а). Следовательно,= они закрыты и на вход ничего не подается. Как только сигнал Uвых стал превышать уровень = ограничения на выходе А2 и А3 будут действовать напряжения по проводимости диода VD2 или VD3, благодаря чему на вход ОУ (А1) будет подано напряжение в противофазе с входным.

На рисунке 3.57б приме= нены операционные усилители типа К553УД2А, К153УД2А.

               

б)

в)

 

Ограничение Uвых за счет придания схеме с ОУ мягких внешних характеристик и это достигается путем введения в цепь R2 (см. рисунок 3.57в). На нем гасится тот излишек напряжения, на который выходной сигнал ОУ превышает заданный уровень выходного.

 

В соответствии с рисун= ком 3.57г, в исходном состоянии, пока схема не достигла исходного ограничения, = на выходе А2 действует  Å= U, превышающее по уров= ню выходной сигнал, следовательно VD3 закрыт. Когда выходной сигнал приблизитс= я к уровню ограничения, установленному на R3, диод VD3 включается и = фиксирует уровень выходного сигнала на уровне сигнала ограничения.<= /p>

 

 

 

г)

В схеме (см. рисунок 3= .57д) ОУ в режиме ограничения выходит в насыщение, а с помощью R2 устанавливается желаемый уровень выходного напряжения, который представляет= ся частью этого напряжения насыщения.

             

д)

 

Рисунок 3.57


I<= /span>вых ОУ = =3D (3¸5)мА.

При R2 >= > Roc  ,

где .

.

 

1.= 1.3      =   Схемы включения ОУ с частотно-зависимым преобразованием сигнала

&nbs= p;

П-регулятор

 

В соответствии с рисун= ком 3.58а, передаточная функция П-регулятора

  .

При анализе частотных свойств и синтезе схемы в 1-ю очередь нас интересует передаточная функция регулятора по каналу датчика обратной связи (ДОС) W(р), и только во 2-ю – по каналу задания Wрег= (р).

На рисунке 3.58а приведены обозначения: UДОС – напряжение датчика ОС; UЗ – напряжение задания.

Zoc =3D Roc ,   Zвх =3D R1  (R2);

W(p) =3D – k1   (k2),

где k1 =3D Roc/R1 ,   k2 =3D Roc/R2.

Частотная характеристи= ка и временные зависимости входного и выходного напряжений представлены на рисун= ке 3.58б, в, соответственно.

При k =3D 10    20= ×lg k =3D 20.

а)

           

б)                                              =                  в)

Рисунок 3.58

 

И-регулятор

В соответствии с рисунком 3.59а, передаточная функция И-р= егулятора

,

где ,  Z1 = =3D R1.

  ,

где Ти =3D CocR1, wCp =3D 1/Ти.

Частотная характеристи= ка и временные зависимости входного и выходного напряжений представлены на рисун= ке 3.59б, в, соответственно.

Физический смысл постоянной времени Ти состоит в том, что она численно равна времени, за которое выходной сигнал достигает уровня входного при нулевых начальных условиях.=

И-= регулятор и любой другой, имеющ= ий интегрирующую часть, обладает свойством памяти (т.е. при нулевом входном сигнале выходной сохраняет накопленное к этому моменту значение).

 

а)

                      =   

б)                                                   =                     в)

Рисунок 3.59

 

ПИ-регулятор

 

В соответствии с рисунком 3.60= а, передаточ= ная функция ПИ-регулятора

;

Zoc =3D Roc + 1/Coc p,  Zвх =3D R1.

В зависимости от соеди= нения ПИ-регулятор можно представить как параллельное (рисунок 3.60б), так и последовательное (рисунок 3.60в) соединение П- и= И- звеньев.

Так, параллельное соед= инение удобно для временных зависимостей.

.

Последовательное соеди= нение удобно для анализа частотных свойств, т.к.=     lg xy =3D lg x + lg y.

,

где Тиз =3D Roc×Coc – из= одромная постоянная времени;

Частотная характеристи= ка и временные зависимости входного и выходного напряжений представлены на рисун= ке 3.60г, д, соответственно.

НЧ: если Тиз= ×w<1, то = w< 1/Тиз;

ВЧ: если Тиз= ×w>1, то = w>1/Тиз.

 

а)

б)                                               в)

                  

= г)                            =                                        д)<= /span>

Рисунок 3.60

А-регулятор

В соответствии с рисунком 3.6= 1а, передаточ= ная функция А-регулятора

;

Z<= /span>ВХ (р) =3D R1;=

,

где Тф = =3D RocCoc.

Частотная характеристи= ка и временные зависимости входного и выходного напряжений представлены на рисун= ке 3.61б, в, соответственно.

НЧ:  Тф= ×w<1.

 

а)=

                 

б)                                              =                        в)

Рисунок 3.61

Д-регулятор

В соответствии с рисунком 3.62= а, передаточ= ная функция Д-регулятора

Zoc =3D Roc; Zвх =3D 1/C1p;

.

Частотная характеристи= ка и временные зависимости входного и выходного напряжений представлены на рисун= ке 3.62б, в, соответственно.

а)

                      =   

б)                                              =                           в)

Рисунок 3.62

 

 

1.2&= nbsp;      Датчики

Датчики относятся к информационной части = ЭП. От точности датчиков зависит точность замкнутых систем.

Требования, предъявляе= мые к датчикам:

- не должны вносить искажения в измеряемую цепь;

- определяемая точност= ь;

- должны осуществлять преобразования измеряемого сигнала в электрическую форму (U,= I)= .

 

1.= 2.1      =   Датчики постоянного тока

&nbs= p;

1.= 2.1.1      = Шунт

Шунт – самый распространенный датчик постоянного тока (комбинированное термостабилизированное сопротивление). Графическое изображение шунта представлено на рисунке 3.63а, где RS – его условное обозначение.

В соответствии с рисунком 3.63б, передато= чная функция шунта

.

Вольт-амперная характеристика (ВАХ) шунта представлена на рисунке 3.63= в.

UШН =3D 75мВ; IШН – от 1А  до 7,5кА.

Частотная характеристи= ка (ЛАЧХ) представлена на рисунке 3.63г.

Достоинства данного ви= да датчика тока:

- простота;=

- точность.=

Недостатки:=

- низкий уровень выход= ного сигнала;

                                  

 а)                                              =    б)

                      =   

в)                                              =     г)

Р= исунок 3.63

- гальваническая связь= с силовой схемой.

 

 

 

 

1.= 2.1.2      = Датчик тока на базе шунта с усилителями постоянного тока

Датчик тока = на базе шунта с усилителями постоянного тока представлен на рисунке 3.64а, где прин= ято обозначение – УПТ – усилитель постоянного тока.

Усилитель постоянного = тока включает в себя:

- усилитель (разделите= льный трансформатор), выполняющий роль гальванической развязки;

-      =    модулятор, преобразующий постоянный входной сигнал в переменный;

-      =    демодулятор, работая симфазно с модулятором, выпрямляет усиленный сигнал и придает ему соответствующий знак (преобразование на частоте 1кГц <= /span>¸50 кГц).

                                

а)                                                          =    б)

                                        

в)                                              =                г)

Рису= нок 3.64

Передаточная функция датчика тока

,

где  КШ – коэффициент шунта;

Кудт – коэффициент усиления датчика тока;

Кдт – коэффициент датчика тока;

ВАХ и ЛАЧХ датчика тока представлены на рисунках 3.64б, в, соответственн= о. Насыщение  ВАХ происходит либо за с= чет усилителя, либо от трансформатора.

Коэффициент усиления д= атчика тока

;

,

где Uдт max =3D 10В, Imax =3D (2¸2,5) Iн.

,  при  Iшн =3D Iдн   ;

.

Шунт используется для подключения к амперметру (см. рисунок 3.64г). Все ампермет= р – это милливольтметр со шкалой 75мВ, но проградуирован в токе.

 

1.= 2.1.3      = Датчик, построенные на базе трансформатора переменного тока

Этот датчик применяетс= я в схемах с ТП (см. рисунок 3.65а).

а)=


Id =3D 1,22= ×Iф (g =3D 0).

Передаточная функция д= атчика тока

;

.

Временные зависимости выходных напряжений и ЛАЧХ датчика тока представлены на рисунках 3.65б, в, соответственно.

                          

б)                                              =                         в)

Рисунок 3.65

Такой датчик применяет= ся в станочном приводе типа БПУ, ЭПУ.

Достоинства:

- сигнал гальванически развязан;

- высокий коэффициент усиления.

Недостаток: инерционно= сть.

 

1.= 2.1.4      = Датчик постоянного тока на базе магнитодиодов

Этот датчик измеряет т= ок косвенно по величине магнитного поля, которое создает протекающий по шине т= ок (см. рисунок 3.66).

RRM =3D f(Ф= ).

Сам магниторезистор включается в цепь измерительного моста.

 

1.= 2.1.5      =  Датчик постоянного тока = на основе элементов Холла

Датчик постоянного ток= а на основе элементов Холла представлен на рисунке 3.67.

ЕэХ =3D К×Iист= ×В » 250мВ при В до 0,7Тл.

У датчиков на базе магнитопроводов и элементов Холла отсутствует гальваническая связь с питающ= ей сетью, а передаточная функция может быть представлена безынерционным звеном= .

W<= /span>дт(p) =3D Кдт.

                       

Рисунок 3.66                                              =        Рисунок 3.67

Применяется в мощных двигателях.

 

1.= 2.2      =   Датчики постоянного напряжен= ия

1.2.2.1 .

Недостаток: гальваниче= ская связь с силовой схемой.

 

1.2.2.2                                    

Рисунок 3.68                                              =              Рисунок 3.69


 

1.= 2.3      =   Датчики скорости

1.= 2.3.1      = Датчик скорости на базе тахогенератора постоянного тока

 Рисунок 3.70<= /p>


Датчик скорости на базе тахогенератора постоянного тока представлен на рисунке 3.70.

Етг =3D См= ×Ф<= /span>×W =3D Uдс.

Если Ф =3D const, то Етг º W.

Для стабилизации потока двигателя Фдв осуществляют:<= /p>

а) магнитную систему ТГ делают насыщенной, т.е. рабочая точка лежит за коленом (см. рисунок 3.71);<= o:p>

Рисунок 3.71

б) питание цепи ОВ тахогенератора от источника стабилизированного тока (см. рисунок 3.72).

Рисунок 3.72

На рисунке 3.72 приняты обозначения: РТ – регулятор тока; ТП – тиристорный преобразователь.

в) применение ТГ с возбуждением от постоянных магнитов.

Передаточная функция датчика скорости в э= том случае

.

Для ЭП с глубоким диап= азоном регулирования 1:1000 и более ТГ должен иметь напряжение не менее 20В при 10= 00 об/мин.

 .

 

 

1.= 2.3.2      = Датчик скорости на базе тахогенератора переменного тока

Рисунок 3.73

Датчик скорости на базе тахогенератора переменного тока представлен на рисунке 3.73.

Применяется только в нереверсивном электроприводе.

 

1.2.3.3°, и по фазе определяют направление вращения. Тогда нужно иметь второй источник и соответственно приемник света (см. рисунок 3.75).

                   

 

Рисунок 3.74                                                Рисунок 3.75

 

1.= 2.4      =   Датчики ЭДС

Датчики ЭДС применяются в  системах ЭП для контроля скорости вращения с определенной точностью. Применяются в  системах ЭП с диапазоном регулирования = Д =3D 1¸40 только с однозонным регулированием скорости, т.к. при Фдв =3D const  Е º W.

 

1.= 2.4.1      = Датчик ЭДС на базе тахометрического моста

Датчик ЭДС на базе тахометрического моста представлен на рисунке 3.76а, где приняты обозначени= я: КО – компенсационная обмотка; ДП – дополнительные полю= са.

Если , то Uдэ º<= /span> е (см. рисунок 3.76б)= .

                  

а)                                              =                         б)

Рисунок 3.76

 

Достоинство: простота = схемы.

Недостатки:

- температурная нестабильность датчика, вызванная разной величиной тока, протекающего по силовой схеме и схеме делителя и разными условиями охлаждения (погрешность = 7¸10%);

- плохая точность датч= ика в переходных режимах, где проявляется влияние индуктивности силовой цепи двигателя.

Схема с учетом индукти= вности представлена на рисунке 3.77.

Рисуно= к 3.77

 

Чтобы Uдэ = º е, надо .

Таким образом, требуется чтобы .

Такое соотношение не в= сегда выполняется, поэтому включают дополнительные индуктивности L1 и = L2, тогда имеем баланс по активному и индуктивному сопротивлению.

.

Но это усложняет схему, поэтому выбирают простоту (т.е. без L1 и L2).

 

Передаточная функция д= атчика эдс

Wдэ(р) =3D Кдэ.

Датчики этого типа при= меняют в роботах и манипуляторах.

 

 

 

1.2.4.2  Рисунок 3.78


Передаточная функция д= атчика напряжения

.

В соответствии со схем= ой замещения цепи, представленной на рисунке 3.79, можно записать уравнения

;

Рисунок 3.79

Необходимость включения фильтра на выходе ДН вызвана тем, чтобы исключить из выходного сигнала датчика составляющую пропорциональную падению напряжения на индуктивности Lя, в независимости от источ= ника. В этом случае для получения на выходе усилителя сигнала датчика ЭДС необход= имо из сигнала на выходе фильтра вычесть сигнал токовой компенсации Uтк º i×Rя.

 

;

,

где Тф =3D Тяц =3D Lяц / Rяц – п= остоянная времени того участка цепи, к которому подключен ДН.

 

 

1.= 2.5      =   Датчики положения

а) аналоговые ДП<= /o:p>

1) потенциометрические= ;

2) сельсинные (n-отсче= тные).

W<= /span>дп =3D Кдп.

б) импульсные, использующие перфорированный диск (применяются в цифровых АЭП, микропроцессорных системах).

 

1.= 2.6      =   Датчики потока

Применяются в двухзонн= ых ЭП.

 

1.= 2.6.1      = Датчик потока на базе элемента Холла

Обеспечивает прямое (непосредственное) изменение потока и устанавливается прямо в конструкции электрической машины.

Передаточная функция д= атчика потока

Wдп(р) =3D Кдп.

 

1.= 2.6.2      = Датчик потока с применением датчика тока возбуждения

 

1.3&= nbsp;      Задатчики регулируемых велич= ин

Задатчики регулируемых величин предназначены для вв= ода задающих сигналов.

При ручном вводе задан= ия используются:

а) потенциометрические задатчики;

б) сельсинные задатчик= и.

 

1.= 3.1      =   Потенциометрический задатчик= с плавным изменением задающего сигнала

Потенциометрический задатчик с = плавным изменением задающего сигнала в реверсивном и нереверсивном электроприводах представлен на рисунке 3.80.

Рисунок 3.80

 

 

1.3.2        Потенциометрический задатчик= с дискретным изменением задающего сигнала

&nbs= p;

Потенциометрический за= датчик с дискретным изменением задающего сигнала представлен на рисунке 3.81, где приняты обозначения: S – галетный переключат= ель; R1¸= Rn – запаянные сопротивления.

Источники питания зада= ющих устройств должны иметь хорошую стабилизацию.

Рисунок 3.81

В ЭП с небольшим диапа= зоном регулирования (Д 1:10, 1:20) применяют линейную шкалу задатчика, е= сли диапазон использован большой (Д 1= :1000 и больше), то шка= лу делают нелинейной.

В случае линейной шкал= ы все сопротивления одинаковы, для нелинейной шкалы справедливо соотношение:=

=3D 1,1¸= 1,3.=

Достоинство нелинейной= шкалы – изменение регулируемой величины на каждой ступени будет отличаться в одно= и тоже значение.

Таблица 3.1 Ступени нелинейной шкалы при диапазоне Д 1= :1000=

q<= /p>

1.1

1.3

1.5

1.3.2.1 N

74=

28=

= 18=

Примечание – N – колич= ество положений.

 

1.= 3.3      =   Сельсинный задатчик

Сельсины применяются в= ЭП с напряженным режимом работы.

Бывают два типа: СКАП – сельсинный командоаппарат педальный; СКАР – сельсинный командоаппарат ручно= й.

Принцип действия одина= ковый.

Сельсины в этих устрой= ствах работают в трансформаторном режиме (см. рисунок 3.82).

Рисунок 3.82

На рисунке приняты обозначения: Г – генератор; ФЧВ – фазочувствительный выпрямитель.

½q= ½< p/6 – линейная зависимость.

Такие сельсинные задатчики широко применяются в качестве задающих устройств ЭП, работающих в агрессивных средах.=


2          Замкнутые одноконтурные сист= емы АЭП постоянного тока

 

В замкнутых системах А= ЭП имеются каналы связи, по которым в систему поступает информация о фактическ= ом значении регулируемой величины, а также информация о возмущающем воздействи= и.

Все замкнутые системы = могут быть в 3-х принципах работы:

- по отклонению (имеют= ся каналы, по которым передается информация о фактическом значении регулируемой величины);

- по возмущению (положительная обратная связь, с помощью которой компенсируется возмущающее воздействие);

- комбинированные.

По характеру действия обратные связи (ОС) бывают:

а) жесткие;=

б) гибкие.<= /span>

Жесткие обратные связи действуют в статике и динамике, их сигнал пропорционален контролируемой величине.

U<= /span>дос =3D А.

Сигнал гибкой обратной= связи пропорционален производной контролируемой величины и действует только в переходных процессах.

.

По направлению действи= я:

а) положительные   Uз= ­  Uдос­;

б) отрицательные    Uз= ­  Uдос¯.

Все системы АЭП бывают одноконтурные или многоконтурные.

                =

2.1       Статические характеристики одноконтурной системы АЭП с отрицательной обратной связью по напряжению

&nbs= p;

Система АЭП с отрицате= льной обратной связью по напряжению представлена на рисунке 4.1, где приняты обозначения: РН – регулятор напряжения; П – преобразователь; кпр =3D1 – коэффициент потенциального разделителя.

Рисунок 4.1

кдн =3D кдел ×кпр =3D кдел.

Проанализируем статиче= ский режим замкнутой системы и получим выражение для скоростной характеристики. Далее сравним жесткость этой системы с жесткостью естественной скоростной характеристики и характеристики разомкнутой системы.

а) Естественная характеристика (ЕХ)

U<= /span>н =3D Е + I×Ra =3D ce×Фн= ×W + I= ×Ra;

E =3D ce×Фн= ×W;

.

б) Разомкнутая система= (РС)

U =3D E + I×(Ra + Rп),

где Rп – сопротивление преобразователя.

.

Uзн1ЗС =3D 7,73В, Uзн1РС =3D 0,37В,=   = DWЕХ £ D= WЗС £ D= WРС.

;  .

в) Замкнутая система (= ЗС) по напряжению

Uy =3D (Uзн – Uдн)×крн  (если Rзн =3D Rдн);

Еп =3D Uy<= span style=3D'font-size:12.0pt;mso-bidi-font-size:10.0pt;font-family:Symbol; mso-ascii-font-family:"Times New Roman";mso-hansi-font-family:"Times New Ro= man"; mso-char-type:symbol;mso-symbol-font-family:Symbol'>×кп =3D Е + I= ×(Ra + Rп),  Е =3D се×Фн= ×W;

U<= /span>дн =3D Uд= ×кдн,  (Uд =3D Еп – I×Rп =3D Е + I×= Ra).

Е =3D Uy×кп – I×(Ra + Rп) =3D (Uзн – Uд= ×кдн)×кп×= крн – I×(Ra + Rп);

Е(1+крн×кп×= кдн) =3D Uзн= ×кп×= крн – I×(Ra<= span style=3D'font-size:12.0pt;mso-bidi-font-size:10.0pt;font-family:Symbol; mso-ascii-font-family:"Times New Roman";mso-hansi-font-family:"Times New Ro= man"; mso-char-type:symbol;mso-symbol-font-family:Symbol'>×крн×= кп×= кдн + Ra + Rп).

;

;

W =3D = Woi + DWЗС.

Анализ D= WЗС:

1)      пусть крн×= кп×= кдн ® = ¥

D= WЗС =3D I×= Ra/се×Фн =3D DWЕХ;

2) при крн×= кп×= кдн =3D 0 (разорвали связ= ь, т.е. РС)

.

Физический смысл дейст= вия отрицательной обратной связи по напряжению состоит в том, что она компенсир= ует падение напряжения в преобразователе и в идеале (при к1×= к2×= к3 ® = ¥) обеспечивает питание двигателя как бы от источника с нулевым внутренним сопротивлением.

Статические характерис= тики системы АЭП с отрицательной обратной связью по напряжению представлены на рисунке 4.2.

Определим сигнал Uзн, который надо подать, чтобы получить сигнал на выходе.

;

Рисунок 4.2

 

;

.

Численный пр= имер расчета:

U<= /span>н =3D 220В;   Еd0 =3D 300В.

крн =3D 20;   кп =3D Еd0 /Uу max = =3D 300/10 =3D30;

кдн =3D Uдн /Uд =3D Uдн <= span lang=3DEN-US style=3D'font-size:12.0pt;mso-bidi-font-size:10.0pt;mso-ansi-l= anguage: EN-US'>max /Uд max =3D 10/300 =3D 1/30;

;

.

 

2.2       Статические характеристики одноконтурной системы АЭП с обратной связью по току

 

Рисунок 4.3

Регулирование по возму= щению (ПОС), либо по отклонению (ООС) может осуществля= ться регулированием по току (см. рисунок 4.3).

Uy =3D (Uзт ± Uдт)×крт,

где (+) – для ПОС;

 (–) – для ООС.

Еп =3D Uy = ×кп =3D Едв + I×(Ra + Rп);

Е = =3D се×Фн= ×W;=

Uдт <= /span>=3D I×= кдт =3D b×I= ×(= Ra + Rп).

Е = =3D Uy×кп – I×= (Ra + Rп) =3D [Uзт = ± = b= ×I×(= Ra + Rп)]×крт×= кп – I×= (Ra + Rп) =3D

=3D Uзт= ×крт×= кп – I×= (Ra + Rп)×(= 1 ± b= ×крт×= кп)

.

Положительная обратная= связь по току (ПОС)

.

;  .

а) b= ×крт×= кп =3D 0  = Þ ;

б) b= ×крт×= кп =3D 1  = Þ  = DW(+) ЗС =3D 0 – абсолютно жес= ткая характеристика;

в) b= ×крт×= кп <= /span>® = ¥  = Þ  = DW(+) ЗС ® –= ¥.

Положительная обратная= связь по току делает характеристики более жесткими, чем те же характеристики в разомкнутой системе (см. рисунок 4.4).

Отрицательная обратная= связь по току (ООС)

.

а) b= ×крт×= кп =3D 0  = Þ ;

б) b= ×крт×= кп = =3D ¥  = Þ  = DW(–) ЗС =3D ¥.

Отрицательная обратная= связь по току применяется для реализации мягких характеристик ЭП.

        

Рисунок 4.4                                               =        Рисунок 4.5

В одноконтурных систем= ах АЭП отрицательная обратная связь, как правило, применяется задержанная, т.е. вступает в работу при определенной токовой нагрузке. Для задержания ОС применяется стабилитрон.

 

 

Численный пример расче= та обратной связи.

.

Пусть в системе положительная обратная связь по току. Нужно найти b, при котором абсолютно жесткая характеристика.

1– b= ×крт×= кп =3D 0,

где крт =3D 20; кп =3D 30.

b =3D 1/ крт×= кп =3D 1/600=3D0,002.

кдт =3D?  кудт = =3D?

Uдт =3D I= ×кдт =3D b= ×I×(R= a + R= п);

кдт =3D b= ×(R= a + Rп);  кдт =3D кш = ×= кудт;  кш =3D Uшн /Iшн.

.

Пример – пусть Р<= span style=3D'text-transform:uppercase'>н =3D 1кВт, Uн =3D 220В ,  Iн =3D 5А ,  Rа =3D 4Ом ,  Rп =3D 4Ом.

кдт½DW=3D0 =3D b= ×(Ra + Rп) =3D 0,002×= (4 + 4) =3D 0,016=

.

 ®  .

Рисунок 4.6

U<= /span>дт =3D Iн= ×кдт =3D 5×0,016 =3D 0,08В.<= /o:p>

РС= 1:  Uзт1 =3D 0,37В;

РС= 2:  Uзт2 =3D 0,37 + 0,08 =3D 0,45В.

Рассчитанные статическ= ие характеристики замкнутой и разомкнутой систем представлены на рисунке 4.6.<= o:p>

 

2.3       Статические характеристики одноконтурной системы АЭП с отрицательной обратно= й связью по скорости

&nbs= p;

Система АЭП с отрицат= ельной обратной связью по скорости представлена на рисунке 4.7.

 

Uy =3D (Uзс – Uдс)×= крс (при Rзс =3D Rдс);

Еп =3D Uу = ×кп =3D = Е + I×= (Ra + Rп);=

Е =3D се×Фн= ×W;

 

Рисунок 4.7

U<= /span>дс =3D кдс×W,    .

(U= зс – кдс= ×W)= ×крс×= кп =3D се×Фн= ×W + I= ×(Ra + Rп);

U<= /span>зс×крс×= кп + кдс= ×W= ×крс×= кп =3D се×Фн= ×W + I= ×(Ra + Rп);

;

.

 а) кдс×= крс×= кп =3D 0  = ®  ;

 б) кдс×= крс×= кп =3D ¥  = ®  = DW =3D 0.

Статические характерис= тики системы АЭП с отрицательной обратной связью по скорости представлены на рис= унке 4.8.

Рисунок 4.8

В системе с отрицатель= ной обратной связью по скорости можно получить абсолютно жесткие характеристики= , но только при очень большом коэффициенте усиления. Такие же характеристики мож= но получить при интегральном регуляторе скорости.

 

2.4       Статические характеристики двухконтурной системы АЭП с отрицательной обратной связью по скорости и отсечкой по току

&nbs= p;

Система АЭП с отрицат= ельной обратной связью по скорости и отсечкой по току представлена на рисунке 4.9.=

Рисунок 4.9

а) I < Iотс, ½Uдт= ½< Uст VD.

В рабочем диапазоне то= ка справедливы выражения для предыдущего случая, т.к. работает только одна обратная связь по скорости (см. рисунок 4.10).

б) I > Iотс, ½Uдт= ½> Uст VD.

В этом диапазоне тока одновременно на входе регулятора скорости действуют два сигнала ОС:

- сигнал по скорости, который стремится сделать скоростную характеристику более жесткой;

- сигнал по току, кото= рый стремится сделать скоростную характеристику более мягкой.=

Для получения требуемой характеристики должна преобладать ОС по току.

Uy =3D (Uзс – Uдс – Uдт + Uст)×крс;

Еп = =3D Uу×= кп =3D = Е + I×= (Ra + Rп);=

Е =3D се×Фн= ×W;

U<= /span>дс =3D W= ×кдс;

U<= /span>дт =3D b= ×I×(Ra + Rп).

[U= зс – W×кдс – b= ×I×(Ra + Rп) + Uст]= ×крс×= кп =3D се×Фн= ×W + I= ×(Ra + Rп);

W =3D = W0 – D= W;

.

Статические характери= стики двухконтурной системы АЭП с отрицательной ОС по скорости и отсечкой по току представлены на рисунке 4.10.

 

                      =      

Рисунок 4.= 10

 

2.5       Статические характеристики д= вухконтурной системы АЭП с отрицательной обратной связью по напряжению и положительной обратной связью по току

&nbs= p;

Система АЭП с отрицательной обратной связ= ью по напряжению и положительной обратной связью по току представлена на рисун= ке 4.11.

Рисунок 4.11

Uy =3D (Uзс – Uдн + Uдт)×= крс;

Еп = =3D Uу×= кп =3D Е + I×= (Ra + Rп);=

Е = =3D се×Фн= ×W;=

кдн =3D Uд×кдн =3D (Еп = – I×R= п)×кдн =3D (Е + I×= Ra)×= кдн;

Uдн <= /span>=3D b×I= ×(= Ra + Rп).

[Uзс – (се×Фн= ×W = + I×R= a)×кдн + b×I= ×(= Ra + Rп)]×крс×кп =3D = се×Фн= ×W = + I×(= Ra + Rп);

;

W =3D = Wоi= – D= W.

Эта система дает возмо= жность получить жесткие характеристики.

 

 

2.6       Статические характеристики одноконтурной системы АЭП с отрицательной обратной связью по скорости и упреждающим токовым ограничением

&nbs= p;

В этой системе огранич= ение тока осуществляется без его непосредственного измерения за счет ограничения разности ЭДС преобразователя и двигателя на допустимом уровне при любой скорости.

½Еп – Ед½ £ Iдоп= ×Rяц å

                           

Рисунок 4.12

 

Если скорость <= span style=3D'font-size:12.0pt;mso-bidi-font-size:10.0pt;font-family:Symbol; mso-ascii-font-family:"Times New Roman";mso-hansi-font-family:"Times New Ro= man"; mso-char-type:symbol;mso-symbol-font-family:Symbol'>W =3D const любая, то ограничение называет= ся линейным (см. рисунок 4.12). Применяется в ЭП с двигателями обычного исполнения.

Если ограничение перем= енное с переменной скоростью, то это нелинейное токоограничение (см. рисунок 4.13= ). Применяется в ЭП с высокомоментными двигателями.

Рисунок 4.13

Поддержание требуемой разности между Ед и Еп осуществляе= тся за счет ограничения на соответствующем уровне (для данной скорости) сигнала уп= равления на входе преобразователя (см. рисунок 4.14).

Еп =3D кп×= U<= /span>упр.

На рисунке 4.14 принято обозначение: БО – блок ограничения (линейный).

Статические характерис= тики системы представлены на рисунке 4.15, где приняты обозначения: ДР, ТР – двигательный и тормозной режимы; ИР – инверто= рный режим.

 

Рисунок 4.14

 

Рисунок 4.15


 

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