Three-phase servomotor DS2 series
400 Vpermanent magnetIP54

Three-phase servomotor - DS2 series - Baumüller Nürnberg GmbH - 400 V / permanent magnet / IP54
Three-phase servomotor - DS2 series - Baumüller Nürnberg GmbH - 400 V / permanent magnet / IP54
Three-phase servomotor - DS2 series - Baumüller Nürnberg GmbH - 400 V / permanent magnet / IP54 - image - 2
Three-phase servomotor - DS2 series - Baumüller Nürnberg GmbH - 400 V / permanent magnet / IP54 - image - 3
Three-phase servomotor - DS2 series - Baumüller Nürnberg GmbH - 400 V / permanent magnet / IP54 - image - 4
Three-phase servomotor - DS2 series - Baumüller Nürnberg GmbH - 400 V / permanent magnet / IP54 - image - 5
Three-phase servomotor - DS2 series - Baumüller Nürnberg GmbH - 400 V / permanent magnet / IP54 - image - 6
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Characteristics

Type
three-phase
Voltage
400 V
Configuration
permanent magnet
Protection class
IP54, IP23, maintenance-free
Cooling mechanism
air-cooled, water-cooled
Applications
packaging machine, for the textile industry
Other characteristics
high-power, high-efficiency, low-noise
Power

Max.: 295 kW
(401.09 hp)

Min.: 5.3 kW
(7.21 hp)

Torque

Max.: 2,190 Nm
(1,615.261107 ft.lb)

Min.: 48 Nm
(35.402983 ft.lb)

Rotational speed

Max.: 4,500 rpm
(28,274.3339 rad.min-1)

Min.: 500 rpm
(3,141.5927 rad.min-1)

Diameter

100 mm, 132 mm, 160 mm, 200 mm
(3.94 in, 5.2 in, 6.3 in, 7.87 in)

Description

The motor name for synchronous motors at Baumüller is DS. "DS" refers to the German for three-phase current synchronous motor ("Drehstrom-Synchronmotor"). Functional principle of a three-phase current synchronous motor This is a permanently excited synchronous motor, as the magnets glued onto the rotor generate a permanent magnetic field (north and south poles). If current is applied to windings U, V, and W in the stand (also referred to as the housing), this current generates a magnetic field around the windings. This magnetic field and the permanent magnetic field on the rotor cause an immediate attraction between the north and south poles and a repulsion of like poles. This in turn causes the rotary motion of the motor. As a result of this motor structure, the rotating field frequency of the housing and the rotor always remains the same. This is therefore referred to as a synchronous rotating field frequency and the motor is therefore called a synchronous motor. In contrast, the frequency of the housing and the rotor of an asynchronous motor must never be identical. This is therefore referred to as an asynchronous rotating field frequency and the motor is therefore called an asynchronous motor. Animation of a synchronous motor The animation shows a 3-phase winding system. For better clarity, the sketch shows a simple permanent magnet instead of a rotor. As soon as current flows into the windings, a rotating magnetic field is generated in the motor housing as described above. This also flows through the permanent magnets of the rotor, thereby causing a torque. The rotor executes a rotary motion and follows the rotation of the magnetic field.

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