instituto tecnologico
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1. INSTITUTO TECNOLOGICO CARLOS CISNEROSINSTALACIONES ELECTRICAS POR: EDWIN MARIOESCUELA DE : ELECTROMECANICASECCION: TECNOLOGICAPARALELO: A 2011-2012Instalciones electricas 2. CONDUCTORES 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 elctrico de cobre.Un conductor elctrico es un material que ofrece poca resistencia al movimientode carga elctrica.DescripcinSon materiales cuya resistencia al paso de la electricidad es muy baja. Los mejoresconductores elctricos son metales, como el cobre, el oro, el hierro y el aluminio, y sus 28. aleaciones, aunque existen otros materiales no metlicos que tambin poseen lapropiedad de conducir la electricidad, como el grafito o las disoluciones y solucionessalinas (por ejemplo, el agua de mar) o cualquier material enestado de plasma.Para el transporte de energa elctrica, as como para cualquier instalacin de usodomstico o industrial, el mejor conductor es laplata, pero debido a su elevado precio,los materiales empleados habitualmente son el cobre (en forma de cables de uno ovarios hilos), o el aluminio; metal que si bien tiene una conductividad elctrica delorden del 60% de la del cobre, es sin embargo un material tres veces ms ligero, por loque su empleo est ms indicado en lneas areas de transmisin de energa elctricaen las redes de alta tensin.1 A diferencia de lo que mucha gente cree, el oro eslevemente peor conductor que el cobre, sin embargo, se utiliza en bornes de bateras yconectores elctricos debido a su durabilidad y resistencia a la corrosin.USOSAplicaciones de los conductores: Conducir la electricidad de un punto a otro (pasar electrones a travs delconductor; los electrones fluyen debido a la diferencia de potencial). Establecer una diferencia de potencial entre un punto A y B. Crear campos electromagnticos (como en las bobinas y electroimanes). Modificar el voltaje (con el uso de transformadores). Crear resistencias (con el uso de conductores no muy conductivos).De alta conductividad:Plata: este es el material con menor resistencia al paso de la electricidad pero al sermuy costoso, su uso es limitado. La plata se halla en la naturaleza en forma decloruros, sulfuros o plata nativa. Este material se caracteriza por ser muy dctil,maleable y no muy duro y fcil de soldar. Es utilizado en fusibles para cortocircuitoselctricos porque es muy preciso en la fusin, es inoxidable y posee una conductividadsumamente alta. Tambin se lo usa en contactos de relevadores o interruptores parabajas intensidades por su elevada conductividad trmica y elctrica.De alta resistividad:Aleaciones de cobre y nquel: estas presentan una resistencia al paso de corriente 29. elctrica relativamente baja y una fuerza electromotriz elevada en relacin al cobre. Elnquel representa el 40% y el cobre el 60% restante y es una aleacin que no resultatil para instrumentos de medida de precisin, a pesar de que su coeficiente detemperatura es bajo. Sin embargo, este se puede incrementar aadindole zinc.Aleacin de cromo y nquel: estas se caracterizan por presentar coeficientes bajos detemperatura, un coeficiente de resistividad mayor y una fuerza electromotriz pequeas conrespecto al cobre. MOTORES MONOFASICOPrincipio de funcionamientoLos motores de corriente alterna y los de corriente continua se basan en el mismoprincipio de funcionamiento, el cual establece que si un conductor por el que circulauna corriente elctrica se encuentra dentro de la accin de un campo magntico, stetiende a desplazarse perpendicularmente a las lneas de accin del campo magntico.El conductor tiende a funcionar como un electroimn debido a la corrienteelctrica que circula por el mismo adquiriendo de esta manera propiedadesmagnticas, que provocan, debido a la interaccin con los polos ubicados en el esttor,el movimiento circular que se observa en el rotor del motor. Aprovechando el estator yrotor ambos de acero laminado al silicio se produce un campo magntico uniforme enel motor.Partiendo del hecho de que cuando pasa corriente por un conductor produceun campo magntico, adems si lo ponemos dentro de la accin de un campomagntico potente, el producto de la interaccin de ambos campos magnticos haceque el conductor tienda a desplazarse produciendo as la energa mecnica.Dicha energa es comunicada al exterior mediante un dispositivo llamado flecha. 30. VentajasEn diversas circunstancias presenta muchas ventajas respecto a los motores decombustin: A igual potencia, su tamao y peso son ms reducidos. Se pueden construir de cualquier tamao. Tiene un par de giro elevado y, segn el tipo de motor, prcticamente constante. Su rendimiento es muy elevado (tpicamente en torno al 75%, aumentando el mismo a medida que se incrementa la potencia de la mquina). Este tipo de motores no emite contaminantes, aunque en la generacin de energa elctrica de la mayora de las redes deQu es una bobina? La bobina es un elemento muy interesante. A diferencia delcondensador, la bobina por su forma (espiras de alambre arrollados) almacena energaen forma de campo magntico. Todo cable por el que circula una corriente tiene a sualrededor un campo magntico generado por la mencionada corriente, siendo elsentido de flujo del campo magntico el que establece la ley de la mano derecha. Alestar la bobina hecha de espiras de cable, el campo magntico circula por el centro dela bobinay cierra su camino por su parteexterior.Una caracterstica interesante de las bobinas es que se oponen a los cambios bruscosde la corriente que circula por ellas. Esto significa que a la hora de modificar lacorriente que circula por ellas (ejemplo: ser conectada y desconectada a una fuente depoder), estatratardemantenersu condicin anterior.Las bobinas se miden en Henrios (H.), pudiendo encontrarse bobinas que se miden enMiliHenrios (mH). El valor que tiene una bobina depende de:El nmero de espiras que tenga la bobina (a ms vueltas mayor inductancia, o seamayorvalor enHenrios).El dimetro de las espiras (a mayor dimetro, mayor inductancia, o sea mayor valor enHenrios).Lalongitud del cable de que est hecha labobina.El tipo de material de que esta hecho el ncleo si es que lo tiene.Quaplicaciones tiene unabobina?Una de la aplicaciones ms comunes de las bobinas y que forma parte de nuestra vidadiaria es la bobina que se encuentra en nuestros autos y forma parte del sistema deignicin. 31. En los sistemas de iluminacin con tubos fluorescentes existe un elemento adicionalque acompaa al tubo y que comnmente se llama balastroEn las fuentes de alimentacin tambin se usan bobinas para filtrar componentes decorriente alterna y solo obtener corriente continua en la salidaLa operacin de las bobinas se basa en un principio de la teora electromagntica,segn el cual, cuando circula una corriente a travs de un alambre, este produce a sualrededor un campo magntico.Las lneas de fuerza que representan el campo magntico son perpendiculares a ladireccin del flujo de la corriente. Si doblamos en algn punto el alambre para formarun bucle o espira, el campo magntico en esa parte del alambre se concentra dentrode la espira puesto que todas las lneas de fuerza apuntan en la misma direccin yconvergenhaciael centro.Por lo tanto, si continuamos agregando espiras, formando una bobina propiamentedicha, los campos magnticos creados por cada una se reforzaran mutuamente,configurando as un campo de mayor intensidad en el interior del sistema, El conjuntose comporta entonces como un electroimn.Condensadores elctricos.Un condensador elctrico es un dispositivo de dos terminales que consiste en doscuerpos conductores separados por un material no conductor. Tal material noconductor se conoce como aislante o dielctrico. A causa del dielctrico, las cargas nopueden moverse de un cuerpo conductor al otro dentro del dispositivo. Por tanto,stas pueden transportarse entre los cuerpos conductores va sistema de circuitosexternos conectados a las terminales del capacitor. Un tipo muy sencillo llamadocapacitor de placas paralelas se muestra en la siguiente figura. Los cuerposconductores son cuerpos planos y rectangulares que estn separados por un materialdielctrico.Se define la capacidad de un condensador como la cantidad de electricidad, expresadaen culombios, que es necesario transportar de una lamina a otra para crear unadiferencia de potencial de un voltio entre ambas lminas. La cantidad de electricidadtransportada se denomina carga. Aunque pareciera natural expresar la cantidad enculombios por voltio, se expresa en realidad en faradios o microfaradios, siendo unfaradio la capacidad de un condensador en el cual una carga de un culombio produceuna diferencia de potencial de un voltio entre las dos lminas.Un microfaradio = a una millonsima de faradio.Un picofaradio = 10-12 faradios.Si despus de cargar el condensador, se desconecta el generador, abriendo los 32. interruptores, la carga volver gradualmente a la lmina inferior a travs delaislamiento, puesto que no existe ningn aislamiento perfecto; pero si el tiempo esseco, transcurrirn varios das antes que la carga desaparezca completamente. Elcondensador puede descargarse en pocas millonsimas de segundo conectando losextremos de un trozo corto de hilo a ambas lminas.La capacidad es inversamente proporcional a la distancia que los separa. La explicacina esto est en el hecho en el que los protones en exceso que hay sobre la barra inferiorejercen una fuerza de atraccin sobre los electrones que abandonan esta lminaoponindose as a los flujos de los mismos, mientras que los electrones en exceso en lalamina superior repelen a los de la inferior favoreciendo as el flujo. Puesto que loselectrones en exceso en la lamina superior estn a alguna distancia del lugar donde seproducen las separaciones, mientras que los protones en exceso estn justamente endicho sitio, las fuerzas repulsivas que favorecen el flujo de electrones son menores quelas fuerzas atractivas que se oponen a l, y el generador tiene que realizar un trabajoparar separar los electrones de la lamina inferior.La capacidad de un condensador varia tambin considerablemente con la naturalezade la sustancia aislante comprendida entre las laminas, denominada generalmentedielctrico, y la razn de la capacidad de un condensador dado con un dielctricodeterminado entre sus lminas, a la capacidad del mismo condensador cuando entrelas lminas hay aire o existe el vaco, se denomina constante dielctrica.SUSTANCIAConstante DielctricaAceite 2,2 - 4,7Agua 81Aire 1Ebonita2,0 - 3,5Goma Laca2,9 - 3,7Mica 2,5 - 6,6Papel Parafinado 2,0 - 2,6Vidrio 5,4 - 9,9La razn de por qu la capacidad cambia por el dielctrico es que los propiosdielctricos contienen un gran nmero de protones y electrones que, aunque nopuedan fluir, son capaces sin embargo, de moverse apreciablemente. Esto s, estnsujetos de modo elstico y no rgido. La deformacin de la estructura del dielctrico,producida al cargar el condensador, tiene un efecto fundamental sobre las fuerzas deatraccin y repulsin que ayudan o se oponen al paso de la carga, y por tanto, unefecto fundamental sobre la capacidad.Para describir la relacin carga - voltaje del dispositivo, transfiramos carga de una placa 33. a la otra. Supongamos, por ejemplo, que por medio de un circuito externo, tomamosuna carga pequea que segn la primera figura denominados q,de la placa inferior a laplaca superior. Esto, por supuesto, deposita una carga +q en la placa superior y dejauna carga -q en la inferior. Ya que mover estas cargas requiere la separacin de cargasde diferente signo (recurdense que cargas opuestas se atraen), se desarrolla unapequea cantidad de trabajo, y la placa superior se eleva a un potencial quedesignaremos v con respecto a la placa inferior.Cada elemento de carga q que transfiramos incrementa la diferencia de potencialentre las placas en una cantidad v . Por tanto, la diferencia de potencial entre lasplacas es proporcional a la carga transferida. Esto sugiere que un cambio en el voltajeentre terminales en una cantidad v origina un cambio correspondiente en la carga dela placa superior en una cantidad q. As, la carga es proporcional a la diferencia depotencial. Esto significa que si un voltaje entre terminalesv corresponde a unacarga q en el capacitor ha sido cargado al voltaje v el cual es proporcional a la carga.Por lo tanto:C viene siendo la constante de proporcionalidad, conocida como la capacitancia deldispositivo en faradios. Los condensadores que satisfacen dicha anterior formula sedenominan conTipos de Condensadores.Los tipos comunes de Condensadores incluyen a los de cermica (titanato de bario),Mylar, Tefln y poliestireno. Estos tipos estn disponibles en escalas de valores de lacapacitancia tpicos desde 100 pF hasta 1 F con tolerancias de 3, 10% y 20%. Losproductos resistencia - capacitancia de estos tipos estn en la escala de 103 -F(cermica) a 2 x 4 106 -F (Tefln)Otro tipo de capacitor, que ofrece valores mayores de C, es el capacitor electroltico.Este capacitor est fabricado con placas polarizadas de xido de aluminio u xido detantalio y tiene valores de 1 a 100.000 F. Los productos resistencia - capacitancia, sinembargo, estn en la escala de 10 a 103 -F, lo cual indica que los electrolticos sonms disparadoresque los tipos no electrolticos.Adems, puesto que los condensadores electrolticos estn polarizados, debenconectarse al circuito con la polaridad de voltaje apropiada. Si se usa la polaridadincorrecta, se reducir el xido y puede ocurrir una conduccin abundante entre lasplacas.Los condensadores electrolticos son los que tienen mayor capacidad nominal, por sumayor relacin capacidad/volumen. Ello los hace atractivos a simple vista para lasaplicaciones de filtrado tipo de paso bajo. No obstante, su ESR es elevada, del orden de0,1 W e incluso 1 W en los de aluminio, valor que aumenta con la frecuencia y aldisminuir la temperatura. Su corriente de fugas aumenta si permanecen largo tiempo 34. sin tensin aplicada. Debido a su gran tamao, la inductancia de los condensadores dealuminio es elevada, lo que limita su utilizacin a frecuencias inferiores a 25 KHz. Seemplean principalmente en filtrado, desacoplamiento y acoplamiento a bajafrecuencia. Ante la posible presencia de altas frecuencias, deben desacoplarse con uncondensador de tipo distinto dispuesto en paralelo, que tenga pequeo valor y bajainductancia.Condensadores en Serie.La capacitancia equivalente de las conexiones en serie y paralelo son una analogadirecta de la conductancia equivalente. Consideremos primero la conexin en serie deN capacitores como se muestra a continuacinSi aplicamos LVK, encontramos que:Por lo tanto:Y si tenemos en serie C1 + C2, CS se saca como si estuvieran en paralelo. Por lo tanto,la capacitancia equivalente es el producto sobre la suma de dos capacitanciasindividuales.La Botella de LeydenEs uno de los condensadores ms simples, descubierto alrededor de 1745, de formaindependiente, por el fsico holands Pieter van Musschenbroek de la Universidad deLeyden y el fsico alemn Ewald Georg von Kleist. La botella de Leyden original era unabotella de cristal llena de agua y cerrada, con un alambre o una aguja que traspasabael tapn y estaba en contacto con el agua. La botella se cargaba sujetndola con unamano y poniendo la parte saliente del alambre en contacto con un dispositivoelctrico. Cuando se interrumpa el contacto entre el alambre y la fuente elctrica y setocaba el alambre con la mano, se produca una descarga que se presentaba como unasacudida violenta. La botella de Leyden actual est recubierta por una capa de estaotanto por la parte interior como por la exterior. El contacto elctrico se realiza con unabarra de latn que atraviesa el tapn de la botella y que est en contacto con la capainterior de metal mediante una cadena. Se produce una descarga completa cuando seconectan las dos capas por medio de un conductor. La botella de Leyden se utilizatodava para demostraciones y experimentos en los laboratorios. Inductancia: La inductancia de un circuito es la relacin entre la fuerza electromotriz inducida en l por una corriente variable, y la velocidad de variacin de dicha corriente. Los componentes diseados de modo que presenten adrede un valor de inductancia elevado se denominan bobinas elctricas, inductancias o inductores. Consisten bsicamente en un conductor arrollado de forma que se incremente el concatenamiento del flujo magntico creado por la corriente 35. variable que circule por las espiras. La inductancia de una bobina depende de susdimensiones, del nmero de vueltas del hilo (espiras) y de la permeabilidad delncleo, m . De todos los componentes pasivos, es el que ms cambia con lafrecuencia.Los inductores se clasifican segn el tipo de ncleo sobre el que estn devanados. Losdos tipos ms generales son los de ncleo de aire y los de ncleo magntico (hierro oferrita). En cualquier caso, un inductor real presenta, adems de la inductancia, unaresistencia en serie y una capacidad distribuida en el bobinado. Esta capacidad serepresenta por un condensador en paralelo en un modelo de parmetrosconcentrados.Bobinas Elctricas.Justo como las cargas estticas ejercen fuerzas las unas sobre las otras, se encuentraque las cargas en movimiento o corrientes tambin influyen una a otra. La fuerza quese experimenta entre dos alambres conductores de corriente vecinos la determinexperimentalmente Ampere en los rboles del siglo diecinueve. Estas fuerzas puedencaracterizarse por la existencia de un campo magntico. Este a su vez puede explicarseen trminos de flujo magntico que forma trayectorias cerradas alrededor decorrientes elctricas. El origen del flujo, por supuesto es la corriente elctrica.Un inductor o bobina elctrica es un dispositivo de dos terminales que consiste en unalambre conductor embobinado. Una corriente que fluya a travs del dispositivoproduce un flujo magntico el cual forma trayectorias cerradas encerrando lasbobinas construidas en el inductor:Supnganse que la bobina contiene N vueltas y que el flujo pasa a travs de cadavuelta. En este caso, el flujo total concatenado por las N vueltas de la bobina es:Este flujo total se conoce por lo comn como flujo concatenado. La unidad de flujomagntico es weber (Wb) as llamado por el fsico alemn Wilhelm Weber (1804-1891).En un inductor lineal, el acoplamiento por flujo es directamente proporcional a lacorriente que fluye a travs del dispositivo. Por tanto podemos afirmar que:Donde L, la constante de proporcionalidad, es la inductancia en webers por amperes.La unidad de 1 Wb/A se conoce como henry (H). Denominada as por el fsiconorteamericano Joseph Henry (1797 - 1878).En la anterior formula vemos que un incremento en i produce un incrementocorrespondiente . Este incremento en produce un voltaje en la N-sima vuelta de labobina. El hecho de que los voltajes ocurren al cambiar el flujo magntico fuedescubierto en primer lugar por Henry.Sin embargo, Henry repiti el error de Cavendish con el resistor, al omitir lapublicacin de sus descubrimientos. Como resultado de lo anterior, se otorga aFaraday el crdito por el descubrimiento de la Ley de induccin electromagntica. EstaLey establece que el voltaje es igual a la razn del cambio del tiempo del flujo 36. magntico total. En forma matemtica, la ley es:Y si la unimos con la penltima formula, tenemos que:Es evidente que si i se incrementa, se establece un voltaje entre los terminales delinductor. Este voltaje se opone a un incremento de i pero si este no fuera el caso, estoes, si la polaridad se invirtiera, el voltaje inducido podra ayudar a la corriente. Estono puede ser verdadero fsicamente porque la corriente se incrementaraindefinidamente.El smbolo de circuitos y la convencin corriente - voltaje del inductor se muestran el lafigura al principio de las Bobinas Elctricas. Justo como en los casos del resistor y elcapacitor, si la direccin de corriente o asignacin de voltajes, pero no ambas, seinvierten; entonces debe emplearse un signo negativo en el miembro derecho.Almacenamiento de energa en inductoresUna corriente i al fluir a travs de un inductor, origina que se produzca un flujoconcatenado total que pasa a travs de las vueltas de la bobina, constituyendo as eldispositivo. Justo como se realiza el trabajo de mover cargas entre las placas de uncapacitor, es necesario un trabajo semejante para establecer el flujo en el inductor.Se dice que el trabajo o energa que se requiere en este caso se almacena en el campomagntico.El inductor