NCE EL

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Circolatori elettronici per impianti solari a basso consumo energetico

PORTATA

0.1 / 4.2

mc / h

PREVALENZA

0.2 / 6.8

m

POTENZA

0.003 / 0.056

kW

Esecuzione

Circolatore ad alta efficienza energetica a velocità variabile pilotato da motore sincrono a magneti permanenti controllato da inverter.

Applicazioni

Impianti termici solari.

Limiti impiego

Temperatura liquido da +2 °C a +110 °C
Temperatura ambiente da 0 °C a +40 °C
Massima pressione: 10 bar
Stoccaggio: -20°C/+70°C UR 95% a 40 °C
Marchi: conformi ai requisiti del marchio CE
Pressione sonora ? 43 dB (A).
Pressione minima in aspirazione: 0,3 bar a 50 °C, 1,0 bar a 95 °C, 1,5 bar a 110 °C
Max. quantità di glicole: 40%
EMC secondo: EN 55014-1, EN 61000-3-2, EN 55014-2
Bocche filettate secondo ISO 228: G 1, G 1 1/2, G 2
Potenza minima: 3 W.

Motore

Motore sincrono a magneti permanenti.
Numero di giri del motore: variabile.
Tensione di alimentazione: monofase 230 V (-10%;+6%).
Frequenza: 50 Hz.
Protezione: IP 44.
Classe di isolamento: H.
Apparecchio classe II.
Protezione contro sovraccarichi (rotore bloccato):
1) protezione automatica con funzione di sblocco elettronico del rotore.
2) protezione con termoprotettore.
Cablaggio: cavo con fase e neutro.
Esecuzione secondo EN 60335-1, EN 60335-2-51.

Catalogo 50HZ
Italiano

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Catalogo 50HZ
Inglese

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Istruzioni
Multilingua

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Catalogo IT 50 Hz

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Catalogo EN 50 Hz

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Istruzioni e sezioni

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Case History

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Prodotti Correlati

NCE EI Circolatori elettronici a basso consumo energetico PORTATA 0.1 / 4.2 mc / h PREVALENZA 0.2 / 6.8 m POTENZA 0.003 / 0.056 kW Scopri di più	NCE ES Circolatori elettronici per acqua calda sanitaria ad alta efficienza energetica PORTATA 0.1 / 3.3 mc / h PREVALENZA 0.2 / 3.8 m POTENZA 0.0045 / 0.044 kW Scopri di più	NCE H Circolatori elettronici a basso consumo energetico con inverter PORTATA 0.1 / 10.5 mc / h PREVALENZA 0.1 / 12 m POTENZA 0.01 / 0.20 kW Scopri di più
NCE HQ F Circolatori elettronici a basso consumo energetico con bocche flangiate PORTATA 1 / 48 mc / h PREVALENZA 0.1 / 17 m POTENZA 0.015 / 1.26 kW Scopri di più	NCE PS Circolatori elettronici per acqua calda sanitaria ad alta efficienza energetica PORTATA 0.2 / 2.6 mc / h PREVALENZA 0.4 / 6 m POTENZA 0.01 / 0.045 kW Scopri di più	NCS3 Circolatori per acqua calda sanitaria PORTATA 0.5 / 4 mc / h PREVALENZA 0.25 / 6.5 m POTENZA 0.04 / 0.122 kW Scopri di più
NR Pompe in-line 2 e 4 poli PORTATA 2 / 140 mc / h PREVALENZA 2 / 85 m POTENZA 0.25 / 22 kW Scopri di più

NCE EL

NCE EL

Circolatori elettronici per impianti solari a basso consumo energetico

PORTATA

0.1 / 4.2

mc / h

PREVALENZA

0.2 / 6.8

m

POTENZA

0.003 / 0.056

kW

Esecuzione

Applicazioni

Limiti impiego

Motore

Prodotti Correlati

NCE EI

PORTATA

0.1 / 4.2

mc / h

PREVALENZA

0.2 / 6.8

m

POTENZA

0.003 / 0.056

kW

NCE ES

PORTATA

0.1 / 3.3

mc / h

PREVALENZA

0.2 / 3.8

m

POTENZA

0.0045 / 0.044

kW

NCE H

PORTATA

0.1 / 10.5

mc / h

PREVALENZA

0.1 / 12

m

POTENZA

0.01 / 0.20

kW

NCE HQ F

PORTATA

1 / 48

mc / h

PREVALENZA

0.1 / 17

m

POTENZA

0.015 / 1.26

kW

NCE PS

PORTATA

0.2 / 2.6

mc / h

PREVALENZA

0.4 / 6

m

POTENZA

0.01 / 0.045

kW

NCS3

PORTATA

0.5 / 4

mc / h

PREVALENZA

0.25 / 6.5

m

POTENZA

0.04 / 0.122

kW

NR

PORTATA

2 / 140