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Influencia del secado en el factor de potencia del aislamiento de los
arrollamientos de transformadores de distribución
Influence of drying on the
insulation power factor of distribution transformer windings
Jorge Ramos1 *, Carlos García1
1 Facultad de
Ingeniería Eléctrica y Electrónica, Universidad Nacional de Ingeniería. Lim=
a,
Perú
=
Recibido (<=
span
class=3DSpellE>Received ): 10/09/2018=
Aceptado( Accepted ): 11/09/=
2018
=
=
=
RESUMEN
=
=
=
El presente
artículo expone el desarrollo de la investigación sobre el análisis y
determinación de la influencia del proceso de eliminación de la humedad,
absorbida por el aislamiento sólido de los arrollamientos, en el factor de
potencia del aislamiento de los transformadores de distribución. Considerán=
dose
al factor de potencia como =
un
parámetro característico que permite determinar qué tan seco está el aislamiento y
definir así su calidad desde el punto de vista eléctrico. Se demostró que existe una influencia significa=
tiva
sobre el factor de potencia.
=
=
Palabras clave -
Secado en vacío, factor de potencia del aislamiento, aislamiento de los
arrollamientos, capacitancia de los arrollamientos.
=
ABSTRACT =
=
The present article exposes the
development of the investigation on the analysis and determination of the
influence of the process of elimination of the humidity, absorbed by the so=
lid
isolation of the windings, in the power factor of the isolation of the dist=
ribution
transformers. Considering the power factor as a characteristic parameter th=
at
allows to determine how dry the insulation is and thus define its quality f=
rom
the electrical point of view. It was shown that there is a significant
influence on the power factor.
Keywords - Vacuum drying,
insulation power factor, insulation of windings, capaci=
tance
of windings.
&nb=
sp;
Los transformadores de distribución en =
baño
de aceite dieléctrico son máquinas eléctricas utilizadas para el suministro=
de
energía eléctrica en sistemas de distribución. Constructivamente están
conformados por el tanque, la parte activa y los accesorios normales, siend=
o un
componente adicional el aceite dieléctrico (que actúa como refrigerante y
aislante).
La parte activa es el componente más
importante del transformador y está constituida por el núcleo magnético, los
arrollamientos y los elementos de conexionado. Durante el proceso de
fabricación de los arrollamientos, y posterior montaje en el núcleo magnéti=
co, sus
aislamientos absorben humedad del medio ambiente.
_____________________________________
* Correspondenci=
a:
=
E-mail:
jorgeramo=
sc@uni.edu.pe
Este
exceso de agua en el material aislante, si no se elimina adecuadamente,
producirá el envejecimiento acelerado ante la presencia de altas temperatur=
as
de operación, poniendo en riesgo la vida útil e integridad del transformado=
r.
Por esta razón, la parte activa se some=
te a
un proceso de eliminación d=
e la
humedad (secado del aislamiento), que generalmente se realiza en un horno c=
on
circulación de aire caliente y a presión atmosférica por un tiempo determin=
ado.
En =
este
proceso, la medición del factor de potencia del aislamiento sólido de los
arrollamientos y su comparación con valores experimentales, y recomendacion=
es
de las normas técnicas, permiten determinar qué tan seco está el aislamient=
o y
definir así su calidad desde el punto de vista eléctrico.
Un proceso complementario de secado es el tratamie=
nto a
presión de vacío del transformador, antes de la impregnación en aceite
dieléctrico, con mediciones del factor de potencia del aislamiento sólido de
los arrollamientos. En dicho proceso es necesario, a partir de los resultad=
os
de las mediciones, analizar y determinar los efectos producidos en la calid=
ad
del secado del aislamiento. En este contexto se formulan el problema general ¿Cómo
interactúan el aislamiento seco de los arrollamientos y el tiempo del
tratamiento en vacío sobre el factor de potencia del aislamiento de los
transformadores de distribución? y los problemas específicos: ¿Qué efecto
produce el aislamiento seco de los arrollamientos en el factor de potencia =
del aislamiento
de los transformadores de distribución? ¿Qué efecto produce el tiempo del t=
ratamiento
en vacío en el factor de potencia del aislamiento de los transformadores de
distribución?
=
Desde el
punto de vista aplicativo y académico, el estudio es importante porque anal=
iza
el proceso de secado en vacío y su influencia en el factor de potencia del
aislamiento de los arrollamientos de transformadores de distribución utiliz=
ando
la metodología de la investigación científica y la aplicación del análisis
estadístico; contribuyendo así con el desarrollo de los conocimientos técnicos con base teórica. =
C entra el análisis en el proceso de secado de la parte activa de cuat=
ro
transformadores trifásicos de distribución, con núcleo magnético tipo colum=
nas
y de 500 Kilovoltioamperios (KVA) de potencia, =
de
fabricación nacional.
&nb=
sp;
Se establece como objetivo general, d eterminar el efecto que pro=
duce
la interacción del aislamiento seco de los arrollamientos y el tiempo del
tratamiento en vacío sobre el factor de potencia del aislamiento de los
transformadores de distribución. Y como objetivos específicos, determinar el
efecto que produce el aislamiento seco de los arrollamientos en el factor de
potencia del aislamiento de los transformadores de distribución, y determin=
ar
el efecto que produce el tiempo del tratamiento en vacío en el factor de
potencia del aislamiento de los transformadores de distribución.
Para dar
respuesta a las preguntas de investigación se formulan la hipótesis general=
: El aislamiento seco de los arrollamientos y el tiempo del
tratamiento en vacío interactúan sobre el factor de potencia del aislamient=
o de
los transformadores de distribución; y las hipótesis específicas : El aislamiento seco de los arrollamientos produce efecto
significativo sobre el factor de potencia del aislamiento de los
transformadores de distribución; y : E l tiempo del tratamiento en
vacío produce efecto significativo sobre el factor de potencia del aislamie=
nto
de los transformadores de distribución. Definiéndose como variables
independientes el aislamiento seco de los arrollamientos, que son los
diferentes aislamientos sólidos de los arrollamientos de la parte activa del
transformador de distribución; y el tiempo del tratamiento en vacío, que es=
la
duración en horas del proceso en vació, a un milibar de presión, al que es
sometida la parte activa dentro de su tanque.
Y como variable dependiente el factor de potencia del aislamiento, q=
ue viene
a ser el valor que determina el grado de secado del aislamiento sólido de l=
os
arrollamientos de la parte activa del transformador de distribución en el
proceso de tratamiento en vacío.
2.
BASE TEÓRICA
2.1 Factor de Potencia del Aislamien=
to
El factor de potencia e=
s un
parámetro del material dieléctrico que constituye el sistema de aislamiento=
de
las máquinas eléctricas, y en particular de los transformadores de
distribución, el cual representa las pérdidas eléctricas totales en el volu=
men
de este material, y que son el resultado de los diferentes fenómenos que se
presentan en la estructura del sistema de aislación. Con el fin de tener una
mejor comprensión del concepto de factor de potencia se plantea un modelo d=
el
sistema de aislación basado en parámetros eléctricos concentrados. Este mod=
elo
representa todos aquellos procesos físicos que determinan el comportamiento
eléctrico macroscópico del aislamiento.
Para realizar el modelo=
se
deberá tener en cuenta que al aplicar una excitación de tensión alterna al
sistema de aislación, circulará por éste una corriente total que explica los siguientes p rocesos físicos [1]:
· Capacitancia geométrica del sistema de aislamiento: Los
dieléctricos dependiendo de su forma constructiva presentan efectos capacit=
ivos
entre sus componentes. En una condición ideal pueden modelarse como un
capacitor [1].
· Polarización del dieléctrico: El modelo físico para estos
procesos estará constituido por resistores y capacitores. Estos parámetros
concentrados involucran los procesos físicos de pérdidas, magnitud de la
polarización y tiempo de relajación [1].
· Conducción superficial y volumétrica: Se debe al movimie=
nto
continuo de los portadores de carga a través del sistema de aislación. Depe=
nde
de la temperatura, humedad, contaminación, nivel de la tensión aplicada,
calidad y estado del aislamiento. Se modela este comportamiento mediante un
resistor [1].
·
Ionización: Comprende el proceso fí=
sico
de las descargas parciales, superficiales o internas, que consumen energía =
y que
a su vez producen el aumento de la capacitancia del sistema de aislación. El
modelo de este proceso estará constituido por un resistor y un capacitor [1=
].
<=
/span> Por lo expuesto, el sistema de aislamiento de los
transformadores puede mod=
elarse
como un capacitor con pérdidas, que se representa mediante un circuito
eléctrico de parámetros concentrados conformado por un capacitor ideal en paralelo con un
resistor , ver Figura 1.
Figura 1. Modelo del aislamiento.
Cuando un voltaje , de u=
na
fuente de tensión, se aplica a través del aislante, la corriente fasorial <=
/span> que ci=
rcula
tendrá dos componentes denominados (a tra=
vés
del capacitor ) e (a tr=
avés
del resistor ). Un aislante ideal tendría , lo c=
ual significaría
que la corriente que entrega la fuente estaría adelantada 90° a la tensión
aplicada. Un buen aislamiento eléctrico tendrá un ángulo de desfasaje muy
cercano a 90°. Cualquier deterioro en el aislamiento producirá un aumento d=
e la
desviación angular , ver Figura 1.
Definiéndose entonces el factor de potencia y la tange=
nte
delta como:
=
=
(1)=
=
(2)=
=
En general se
deberá tener presente que el factor de potencia y la tangente delta tienen
valores similares cuando el ángulo es, aproximadamente, mayor a 8=
0°, siendo
diferentes cuando es menor a este valor [2].
=
Según
recomendaciones de la norma internacional [3], los transformadores nuevos en
baño de aceite dieléctrico deben tener valores de factor de potencia menor =
al
0,5 %, medidos a una temperatura de 20 °C. Para el aislamiento seco de los
arrollamientos, sin impregnación de aceite dieléctrico, las normas no
prescriben un valor de referencia, por tanto en base a la experiencia se pu=
ede
considerar como un valor aceptable el que refiere la norma mencionada [3].<=
span
style=3D'mso-spacerun:yes'> Si la temperatura de medición difiere d=
e 20°C
es necesario corregir por temperatura los valores medidos del factor de
potencia, según prescribe la norma para transformadores inmersos en aceite =
dieléctrico
[4]. En el caso del aislamiento seco de los arrollamientos, sin impregnació=
n en
aceite dieléctrico, la norma no prescribe un valor de corrección por
temperatura.
=
En
la realización de las mediciones del factor de potencia del aislamiento y d=
e la
capacitancia de los arrollamientos se utilizan los siguientes modos de prue=
ba:
a) Modo de Prueba de Espécimen a Tierra (GST): La prueba de espécimen a tierra, se conoce como=
la
medición de una muestra de aislamiento que tiene uno de sus terminales
conectado a tierra [2]. Para la medición en transformadores=
de
dos arrollamientos, este modo de prueba se caracteriza por que la forma de
conexión entre el instrumento de medición y el transformador bajo ensayo lo=
gra
medir las corrientes y las pérdidas a tierra de los arrollamientos, por tan=
to,
se miden el factor de potencia y la capacitancia de los arrollamientos de a=
lta
tensión a tierra , Figura 2, y de los arrollamientos de baja tensión a tierra, Figur=
a 3.
Figura 2. Modo de prueba GST para medic=
iones
en el arrollamiento de alta tensi=
ón.
Figura 3. Modo de prueba GST para mediciones en el arrollamiento de baja tensión.
=
b) Modo de Prueba de Espécimen no Aterrado (UST): La prueba de espécimen sin conexión a tierra se
conoce como la medición de una muestra de aislamiento que no está conectada=
a
tierra [2]. Para la medición en transformadores=
de
dos arrollamientos, este modo de prueba se caracteriza por que la forma de
conexión entre el instrumento de medición y el transformador bajo ensayo lo=
gra
medir las corrientes y las pérdidas entre los arrollamientos, por tanto, se
miden el factor de potencia y la capacitancia entre los arrollamientos de a=
lta
tensión y los arrollamientos de baja tensión. No mide las corrientes y pérd=
idas
a tierra, ver Figura 4.
=
=
Figura 4. Modo de prueba UST para medic=
iones
entre arrollamientos de alta y baja tensión.
En las figuras, y son las capacit=
ancias
de los arrollamientos de alta tensión a tierra y de baja tensión a tierra,
y la capacitancia=
entre
arrollamientos.
2.2 Eliminación de la Humedad d=
e la
Parte Activa
Los aislamientos sólidos de los arr=
ollamientos
de transformadores de distribución, están compuestos principalmente por
material celulósico y madera, los cuales llegan a representar el 95% de los
aislamientos. Estos materiales son altamente higroscópicos conteniendo de 8=
% a
10 % de su peso en humedad, en malas condiciones de operación. Dentro de el=
los
el papel aislante seco absorbe agua más rápidamente que el papel impregnado=
de
aceite dieléctrico (el cual tiene un rango más bajo de absorción de humedad=
). Esta
humedad en el papel aislante afecta su rigidez dieléctrica, el factor de
potencia y la resistencia mecánica [5], originando el envejecimiento premat=
uro
del material.
Para eliminar la humedad de los
aislamientos es necesario transformarla en vapor y expulsarla a la atmosfer=
a;
ello se puede lograr aplicando el Método con Presión de Vacío. Este método
consiste en un proceso de disminución de la temperatura de ebullición del a=
gua
por medio del alto vacío, o sea, bajar la presión interna en el tanque del
transformador, que contiene a la parte activa, a niveles en los cuales el a=
gua
se vaporice y pueda ser extraída en forma de gas [5]. Al convertirse el agu=
a en
vapor [6], este puede ser evacuado rápidamente por medio de la bomba de vac=
ío.
3.&n=
bsp;
METODOLOGÍA DE LA INVESTIGA=
CIÓN
=
<=
/span> La unidad de análisis de la investigación fue e=
l grado de secado del aislamiento sólid=
o de
los arrollamientos del transformador de distribución . El tamaño de la muestra consistió de cuatro partes activas de transformadores trifásicos de distribución=
,
de fabricación nacional, cuyas características técnicas generales se presen=
tan
en la Tabla 1.
Tabla 1. =
Características
técnicas de los transformadores
N°
Potencia Nominal
(KVA)
Tensión Nominal
Tensión Máxima de Servicio
Peso Parte Activa
(Kg)
Alta Tensión
(kV )
Baja Tensión (kV )
Alta Tensión
(kV )
Baja Tensión (kV )
1
500
22,90
0,46
36
3,6
783
2
500
22,90
0,40
36
3,6
777
3
500
22,90
0,46
36
3,6
714
4
500
22,90
0,40
36
3,6
760
N°: Número del transformador de dis=
tribución.
KVA: Kilovoltioamperios . k=
V :
Kilovoltios. Kg: Kilogramos. =
Con la
finalidad de determinar y analizar los factores que influyeron
significativamente en el valor del factor de potencia del aislamiento de los
arrollamientos, durante el tratamiento en vacío, se consideraron dos factores de influencia. El primer factor, fue el Aislamiento seco de los arrollamientos=
que comprendió tres niveles: a)
Aislamiento seco del arrollamiento de baja tensión (Nivel de tensión máxima=
de
servicio de 3,6 kV ), b) Aislamiento seco entre
arrollamientos de alta y baja tensión, c) Aislamiento seco del arrollamient=
o de
alta tensión (Nivel de tensión máxima de servicio de 36 kV ).
El segundo factor, fue el Tiempo de=
l tratamiento
en vacío que comprendió cinco niveles, que fueron los intervalos de med=
ición
de media hora. El Factor de potencia del aislamiento, expresad=
o en %,
fue la respuesta observada. De las pruebas se=
obtuvieron
los siguientes datos: a) Las temperaturas del núcleo magnético de la parte
activa de uno de los transformadores, medidos durante el secado en el horno=
; b)
Los valores de la capacitancia de los arrollamientos de cada uno de los cua=
tro
transformadores, medidos durante el tratamiento en vacío; c) Los valores del
factor de potencia del aislamiento de los arrollamientos de cada uno de los
cuatro transformadores, medidos durante el tratamiento en vacío.
=
=
En el análisis de los resultados se aplicó el
diseño factorial utilizando un software de análisis estadístico [7], que permitió contrastar las hipótesis de investigación y
determinar la interacción entre factores y el efecto de los factores en la
respuesta. Para ello se aplicó un análisis=
de
varianza (ANOVA) de dos factores [8], el que contrasta, para cada uno de los
factores, la hipótesis nula de que los resultados de la variable dependient=
e no
dependen del factor.
4.&n=
bsp;
EXPERIMENTACIÓN<=
/o:p>
Las cuatro partes activas de los
transformadores seleccionados como muestras, fueron sometidas a un proceso =
de
tratamiento térmico de secado en el horno – durante 72 horas y a presión
atmosférica – con la finalidad de extraer la humedad de los aislamientos; h=
abiéndose
monitoreado la temperatura del núcleo magnético de uno de ellos, inicialmen=
te en
periodos de una hora, obteniéndose la curva de calentamiento que se present=
a en
la Figura 5. Se realizó el montaje de cada parte activa en su respectivo ta=
nque
(transformador completo), y luego de ello, el transformador se colocó dentr=
o de
un tanque diseñado para soportar presiones en vacío sellándose herméticamen=
te
contra el exterior. =
Se inició al tratamiento en va=
cío
con una presión de un milibar, man=
teniéndose
constante durante todo el proceso que tuvo una duración de dos horas. En
intervalos de media hora se midió el valor de las capacitancias de los
arrollamientos y el factor de potencia del aislamiento, utilizando un instrumento para prueba de baja tensión en sistemas de
aislamientos .
De la medición de la Capacitancia de los
Arrollamientos de la parte activa de cada transformador se obtuvieron los
resultados que se presentan en la Tabla 2. En ella se puede apreciar que los valore=
s de
las capacitancias se mantienen aproximadamente constantes, tanto para el
aislamiento de los arrollamientos de alta tensión y de baja tensión como pa=
ra
el aislamiento entre ambos arrollamientos. Esto en razón de que el tratamie=
nto
en vacío no afecta significativamente la geometría y dimensiones de los
arrollamientos de alta tensión y baja tensión de la parte activa del
transformador de distribución.
&nbs=
p;
Figura 5. Curva de calentamiento del núcleo magné=
tico
de la parte activa del transformador de distribución.
Tabla 2. Valores
medidos de la capacitancia de los arrollamientos
N°
Prueba General
Capacitancia de los Arrollamientos
(Picofaradios)
Modo
Energizado
Guarda
UST
Aislamiento del Arrollamiento
Tiempo de Medición
(Horas del Tratamiento en Vacío)
0,0
0,5
1,0
1,5
2,0
1
GST
Alta Tensión
Baja Tensión
=
: Alta Tensión
388,25
388,40
387,80
387,60
387,40
UST
Alta Tensión
Baja Tensión
: Alta y Baja
Tensión
1161,80
1161,20
1160,40
1159,60
1159,00
GST
Baja Tensión
Alta Tensión
=
: Baja Tensión
1322,20
1322,00
1321,60
1321,20
1320,80
2
GST
Alta Tensión
Baja Tensión
=
: Alta Tensión
393,20
391,45
391,45
391,80
394,55
UST
Alta Tensión
Baja Tensión
: Alta y Baja
Tensión
914,80
907,60
908,60
910,80
910,00
GST
Baja Tensión
Alta Tensión
=
: Baja Tensión
1353,00
1152,00
1152,80
1154,00
1153,40
3
GST
Alta Tensión
Baja Tensión
=
: Alta Tensión
340,90
332,70
332,50
332,30
332,20
UST
Alta Tensión
Baja Tensión
: Alta y Baja
Tensión
819,60
814,60
813,80
813,20
812,60
GST
Baja Tensión
Alta Tensión
=
: Baja Tensión
1362,00
1345,00
1344,40
1343,20
1342,20
4
GST
Alta Tensión
Baja Tensión
=
: Alta Tensión
427,40
419,50
416,70
415,70
415,00
UST
Alta Tensión
Baja Tensión
: Alta y Baja
Tensión
1262,00
1262,00
1261,00
1260,00
1259,40
GST
Baja Tensión
Alta Tensión
=
: Baja Tensión
1431,40
1428,40
1424,20
1422,40
1421,60
N°: Número del tran=
sformador
de distribución sometido a ensayo.
=
;
De =
la
medición del Factor de Potencia del Aislamiento de cada transformador, se
obtuvieron los resultados que muestran en la Tabla 3; en la que se puede
apreciar que los valo=
res
del factor de potencia (%) correspondientes al aislamiento seco de los
arrollamientos de alta tensión y de baja tensión, al inicio del tratamiento=
en
vacío, son superiores a los obtenidos al final del tratamiento en vacío. Lo=
que
demuestra la efectividad del proceso para eliminar la humedad remanente en =
los
aislamientos de los arrollamientos de la parte activa del transformador de
distribución. Así mismo se observa que el factor de potencia del aislamiento
entre arrollamientos de alta y baja tensión no tiene una variación
significativa durante el proceso.
=
;
=
;
Tabla 3. Valores
medidos del factor de potencia del aislamiento
N°
Prueba General
Factor de Potencia del Aislamiento
(%)
Modo
Energizado
Guarda
UST
Aislamiento del Arrollamiento
Tiempo de Medición
(Horas del Tratamiento en Vacío)
0,0
0,5
1.0
1,5
2,0
1
GST
Alta Tensión
Baja Tensión
Alta Tensión
1,392
0,588
0,584
0,582
0,580
UST
Alta Tensión
Baja Tensión
Alta y Baja Tensión
0,232
0,221
0,217
0,215
0,213
GST
Baja Tensión
Alta Tensión
Baja Tensión
1,021
0,937
0,933
0,925
0,915
2
GST
Alta Tensión
Baja Tensión
Alta Tensión
1,180
0,839
0,829
0,826
0,825
UST
Alta Tensión
Baja Tensión
Alta y Baja Tensión
0,263
0,196
0,190
0,179
0,175
GST
Baja Tensión
Alta Tensión
Baja Tensión
1,050
0,985
0,976
0,970
0,950
3
GST
Alta Tensión
Baja Tensión
Alta Tensión
2,080
0,495
0,465
0,456
0,450
UST
Alta Tensión
Baja Tensión
Alta y Baja Tensión
0,120
0,100
0,082
0,080
0,079
GST
Baja Tensión
Alta Tensión
Baja Tensión
1,030
0,526
0,513
0,510
0,508
4
GST
Alta Tensión
Baja Tensión
Alta Tensión
1,840
0,720
0,603
0,541
0,507
UST
Alta Tensión
Baja Tensión
Alta y Baja Tensión
0,123
0,123
0,118
0,117
0,116
GST
Baja Tensión
Alta Tensión
Baja Tensión
0,638
0,556
0,535
0,528
0,524
N°: Número del transformador de distribución
sometido a ensayo.
5.&n=
bsp;
ANÁLISIS E INTERPRETA=
CIÓN
DE RESULTADOS
=
El
paso previo a la contrastación de las hipótesis de investigación es verific=
ar
la validez del diseño factorial utilizado, mediante la prueba de significan=
cia
del análisis de varianza [8][ 7], cuyos resultado=
s se presentan
en la Tabla 4.
Tabla 4. =
Resultados
del análisis de varianza
Fuente de Variac=
ión
Estadístico de
Prueba
Nivel de
Significancia
p
Factor Aislamiento Secos de los Arrollamientos
72,43
0,000*=
Factor Tiempo del Tratamiento en Vacío
10,83
0,000*=
Interacción entre Factores Aislamiento Seco de los
Arrollamientos y Tiempo del Tratamiento en Vacío
5,74
0,000*=
=3D 83,87 % (corregido) =3D =
78,86
% (*) 0,05
=
De este análisis se puede apreciar =
que
el valor de (denominado
coeficiente de determinación), indica que estadísticamente el 83,87 % de la
variabilidad de las mediciones del factor de potencia del aislamiento está
explicada y sustentada, tanto por el efecto de los factores Aislamiento sólido de los arrollamient=
os y Tiempo
del tratamiento en vacío , como por la Interacción
entre ambos factores . Por tanto el diseño factorial es adecuado para el
experimento.
=
Para la contrastación de las hipóte=
sis
con el análisis de varianza, se tiene que evaluar el nivel de significancia=
, que demuestra estadísticamente que =
se
acepta la hipótesis de investigación . Así, d e los r esultados
de la contrastación de las tres
hipótesis, que se presentan en la Tabla 4, se infiere lo siguiente:
=
=
Se
acepta la Hipótesis General y se puede afir=
mar
que, para la muestra de transformadores =
de
distribución, e l aislamiento seco de los arrollamientos de la parte act=
iva
y el tiempo de tratamiento en vacío interactúan =
sobre
el factor de potencia del aislamiento de los transformadores de distribució=
n (Estadístico 5,74; =
significancia de
0,000; ) .
Se
acepta la Hipótesis Específica y se puede afirmar que, para la muestra de transformadores=
de
distribución, e l aislamiento seco de los arrollamientos produce efecto
significativo sobre el factor de potencia del aislamiento de los
transformadores de distribución (Estadístico 72,43; 0,000;
) .
=
Se
acepta la Hipótesis Específica y se puede afirmar que, para la muestra de transformadores de
distribución, e l tiempo del tratamiento en vacío produce efecto
significativo sobre el factor de potencia del aislamiento de los
transformadores de distribución (Estadístico 10,83; 0,000; ) .
=
La aceptación de las hipótesis se
traduce en la interpretación práctica de los resultados, que se expone a
continuación.
=
=
=
=
=
=
=
=
=
=
=
=
=
=
=
Figura 6. Gráfica de interacción entre
factores. Medias
ajustadas.
En la gráfica de interacción entre =
factores,
de la Figura 6, se observa que al cruzarse las líneas de los niveles del
aislamiento seco - arrollamiento de alta tensión y arrollamiento de baja
tensión – aproximadamente a las 0,5 horas, se comprueba que existe interacc=
ión
entre los factores Tiempo del trata=
miento
en vacío y Aislamiento seco de =
los
arrollamientos ; por tanto, la relación que existe entre la respuesta fa=
ctor
de potencia del aislamiento y el tiempo del tratamiento en vacío depende de=
la
calidad del aislamiento seco de los arrollamientos.
En esta gráfica también se aprecia =
que,
al iniciarse el tratamiento en vacío (0,0 horas), el aislamiento seco del
arrollamiento de baja tensión tiene un valor promedio del factor de potenci=
a menor
al del arrollamiento de alta tensión; lo que significa que el aislamiento d=
el
arrollamiento de baja tensión por encontrarse cerca del núcleo magnético, q=
ue
es la parte más caliente, ver Figura 7, ha tenido un secado uniforme en su
aislamiento en comparación con el aislamiento del arrollamiento de alta
tensión. Ello también podría indicar que el arrollamiento de alta tensión, =
al
estar ubicado exteriormente con respecto al núcleo magnético, la exposición=
al
medio ambiente, durante el proceso de ajuste y montaje de la parte activa e=
n su
tanque, ha originado que absorba humedad afectando la calidad del secado. E=
n la
misma gráfica, luego de 0,5 horas de tratamiento en vacío, el aislamiento d=
el
arrollamiento de alta tensión alcanza un valor promedio de factor de potenc=
ia
que es menor al valor que tiene el arrollamiento de baja tensión; para luego
mantenerse con una tendencia decreciente hasta el final del tratamiento en
vacío.
Con relación a la línea correspondiente =
al
nivel del aislamiento seco entre arrollamientos de alta y baja tensión, se
observa que esta no se cruza con las otras líneas durante todo el tratamien=
to
en vacío - valor promedio de factor de potencia del aislamiento aproximadam=
ente
constante - lo que significa que para este tipo de aislamiento no existe
interacción entre los factores Tiem=
po del
tratamiento en vacío y Aislamie=
nto
seco de los arrollamientos ; ya que el tratamiento en vacío no afecta en
gran medida el secado de estos aislamientos. Esto se explica porque en la z=
ona
intermedia de los arrollamientos (entre alta y baja tensión) el volumen de =
masa
del aislamiento sólido es mínimo, puestos que, básicamente, son canales de
refrigeración constituidos por cilindros aislantes y d=
istanciadores
axiales, como se aprecia en la Figura 7, y por tanto la escasa humedad que =
hubieren
contenido ha sido eliminada rápidamente durante el secado de la parte activ=
a en
el horno. Este espacio posteriormente será ocupado por el aceite dieléctric=
o.
De la Figura 6 y Tabla 3 se determina, que el
aislamiento seco de los arrollamientos representa un efecto individual
importante sobre el factor de potencia del aislamiento. Ya que para los tres
niveles del aislamiento, el factor de potencia disminuye gradualmente como
consecuencia de la eliminación de la humedad. Lo que ha sido corroborado co=
n el
nivel de significancia ( ) obtenido en el análisis de varianza, Tabla 4, y por tanto es un efecto en el que se debe priorizar su
atención. Esto implica que el control del secado de la parte activa podría
centrarse en el arrollamiento de alta tensión, puesto que, al ser de un niv=
el
de tensión máxima de servicio de 36 kV y contar=
con
mayor número de espiras, tiene también mayor masa de aislamiento sólido, ver
Figura 8, en comparación con el arrollamiento de baja tensión, ver Figura 9=
.
=
Figura 7. Vista transversal de los arrollamientos de la parte activa
del transformador.
=
=
=
=
=
<=
/o:p>
<=
/o:p>
<=
/o:p>
<=
/o:p>
<=
/o:p>
<=
/o:p>
<=
/o:p>
<=
/o:p>
<=
/o:p>
<=
/o:p>
<=
/o:p>
=
=
Figura 8. Disposic=
ión
del aislamiento sólido en el a=
rrollamiento
de alta tensión (36 kV ).
=
=
=
<=
/o:p>
<=
/o:p>
<=
/o:p>
<=
/o:p>
<=
/o:p>
<=
/o:p>
<=
/o:p>
<=
/o:p>
<=
/o:p>
<=
/o:p>
<=
/o:p>
<=
/o:p>
<=
/o:p>
=
=
Figura 9. Disposic=
ión
del aislamiento sólido en el arrollamiento de baja tensión (3,6 kV ).
=
De la Fi=
gura
6 y Tabla 3 también se determina, que el tiempo del tratamiento en vacío
representa un efecto individual importante sobre el factor de potencia del
aislamiento. Ya que para los cinco niveles de tiempo, el factor de potencia=
disminuye
gradualmente conforme se acelera la evaporación del agua del aislamiento, F=
igura
10. Lo que ha sido corroborado con el nivel de significancia ( ) obtenido en el análisis de varianza, Tabla 4. Por tanto es
recomendable que el tiempo del tratamiento en va=
cío
sea como mínimo de dos horas, puesto que el efecto en el factor de potencia=
del
aislamiento es favorable, alcanzándose un valor próximo al 0,5 %.
Figura 10. Diagrama=
de
fases de la eliminación del agua contenida en el aislamiento. Adaptado de
Fundamentos de Termodinámica [6].
=
=
Esto
se explica porque al iniciarse el tratamiento en vacío, punto C de la Figura 10, se produce una
expansión del aire contenido dentro del tanque del transformador. Esta
expansión ayuda a la expulsión inicial de la humedad, punto D . Simultáneamente, al reducirse =
el
punto de ebullición del agua contenida en los aislamientos, la evaporación =
se
acelera hasta que se logra la presión de un milibar, punto E . Así, conforme se prolonga el tratamiento en vacío a presión
constante, se mejora permanentemente el secado del aislamiento de los
arrollamientos. =
CONCLUSIONES
=
=
El
principal aporte del estudio ha sido comprobar la influencia del tratamient=
o de
secado en vacío sobre el factor de potencia del aislamiento de los
arrollamientos de transformadores de distribución. Pr obándose estadísticamente, para la muestra en estudio, =
la
hipótesis general y las hipótesis específicas formuladas en la investigació=
n, demostrándose así la eficacia del proceso.
=
Se confirmó como efectos principales, sobre el fac=
tor
de potencia del aislamiento de los arrollamientos, el grado de calidad del
aislamiento seco de los arrollamientos y el tiempo de duración del tratamie=
nto
en vacío.
Se demostró, que el tiempo de duración del tratamiento en vacío produce=
un
efecto que contribuye con la aceleración de la eliminación de la humedad
remanente del aislamiento de los arrollamientos, traduciéndose en una
disminución del valor promedio del
factor de potencia del aislamiento.
Se demostró, =
que
la calidad del secado del aislamiento sólido de los arrollamientos de alta
tensión y baja tensión produce un =
efecto
que se refleja en el valor promedio del factor de potencia del aislamiento.=
=
=
Se
comprobó, que la capacitancia a tierra de los arrollamientos de alta tensió=
n y de
baja tensión no se ve influenciada por el tratamiento en vacío.
REFERENCIAS=
[1] Prueba de Tangente Delta y Capacidad Ingeniería de Máquinas Eléctricas (IME=
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http://ww=
w.ime.com.co/filedownload/downloadfile/fileid/48/src/@random558829acd336e
[2] I=
wanusiw
O W 2010 Insulation Power Factor Testing of Power Transformers Eltel Industries, Bangalore http://www.eltelindustries.com/wp-content/uploads=
/2013/10/ACTS125K-PLUS.pdf
[3] <=
span
lang=3DEN-US style=3D'font-size:8.0pt;font-family:"Candara","sans-serif";
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mso-ansi-language:EN-US;mso-fareast-language:ES'> IEEE Std Revision of IEEE Std 62-1978
[4] IEEE Std C57.12.1999 IEEE Stand=
ard Test
Code for Liquid-Inmersed Distribution, Power, a=
nd Regulating
Transformers Revision of IEEE Std
C57.12.90-1993
[5] P=
rocedimiento
para secado de transformadores de distribución Bombas de Vacío y Deshidratación S A
http:/=
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[6] Van Wylen G y Sonntang R 1975 Fundamentos
de Termodinámica (Primera Edición) México: Editorial Limusa
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[7] Manual Minitab 16 Meet Minitab 16 =
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[8] Montgomery D 2008 Diseño
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Wiley pp 170-200
Los artículos publicados por TECNIA <=
span
class=3DSpellE>pueden ser compartidos
a través de la licencia<=
/span>
Creative Commons: CC BY 4.0 Perú . Permisos lejos de este alcance pueden ser consultados
a través del correo revistas@uni.edu.p=
e
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doi :
https://doi.org/10.21754/tecnia.v28i2.349 Revist=
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TECNIA Vol. 28 Nº 1 Agosto – Diciembre 2018
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