NCE PS

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Circuladoras electrónicas de agua caliente sanitaria de bajo consumo energético

CAUDAL

0.2 / 2.6

mc / h

H MAX

0.4 / 6

m

POTENCIA

0.01 / 0.045

kW

Ejecución

Bombas de circulación de agua caliente sanitaria de alta eficiencia energética con motor síncrono con imán permanente de rotor húmedo controlado por variador de frecuencia. Cuerpo bomba bronce.

Aplicaciones

Sistemas de circulación de agua caliente sanitaria.

Límites de uso

Temperatura del líquido de +5 °C a +65 °C
– Temperatura ambiente de 0 °C a +40 °C
Presión máxima: 3 bar
Almacenaje: -10 °C/+50 °C Humedad Relativa 95% a 40%
– Marcado: conforme a los requisitos de marca CE
Nivel sonoro ≤ 45 dB (A).
– Presión mínima de aspiración: – 0,05 bar at 75 °C, 0,28 bar a 90 °C.
EMC segùn: EN 55014-1, EN 55014-2, EN 61000-3-2, EN 61000-3-3.
Bocas roscadas según ISO 228: G 1.

Motor

Motor sincrónico con imán permanente.
Número de vueltas del motor: variable
– Tensión de alimentación: monofásica 230 V (-10%; +6%)
Frecuencia: 50 Hz
– Protección: IP 44
Clase de aislamiento: F
– Aparato clase II
– Protección de la sobrecarga (integrado)
– Cableado: cable con fase y neutro.
Ejecución según EN 60335-1, EN 60335-2-51.

Catálogo 50HZ
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Catálogo 50HZ
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Catalog IT 50HZ

Catalog EN 50HZ

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NCE PS

NCE PS

Circuladoras electrónicas de agua caliente sanitaria de bajo consumo energético

CAUDAL

0.2 / 2.6

mc / h

H MAX

0.4 / 6

m

POTENCIA

0.01 / 0.045

kW

Ejecución

Aplicaciones

Límites de uso

﻿Motor

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0.1 / 4.2

mc / h

H MAX

0.2 / 6.8

m

POTENCIA

0.003 / 0.056

kW

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CAUDAL

0.1 / 4.2

mc / h

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0.2 / 6.8

m

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0.003 / 0.056

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mc / h

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0.2 / 3.8

m

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0.0045 / 0.044

kW

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CAUDAL

0.1 / 10.5

mc / h

H MAX

0.1 / 12

m

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kW

NCE HQ F

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1 / 48

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Motor