Česky / English

Homepage > Servomotors > Linear servomotors

Linear servomotors

Series motors are frameless permanent magnet, three phase brushless servomotors. Fundamentally, a linear motor is a rotary motor that is rolled out flat.The two primary components of permanent magnet brushless rotary
motors are the stator (primary coils) and the rotor (secondary or rotating magnets). In brushless linear motors the rotor is rolled out flat to become the magnet track (also called the magnet way). The primary coils of the rotary motor are rolled out flat to become the coil assembly (also sometimes called the slider). In most brushless linear motor applications it is typical for the magnet way to be stationary and the coil assembly to be in motion, because of the relative masses of the two components. But it is also perfectly acceptable and sometimes advantageous to reverse this arrangement. The basic electromagnetic operating principles are the same in either case and are identicalto those of a rotary motor.

Two types of linear motors are available, Ironcore and Ironless. Each one provides characteristics and features that are optimal depending upon the application. Ironcore motors have coils wound on
silicon steel laminations, to maximize the generated force, with a single sided magnet way. Using a patented electromagnetic design, linear motors have the highest rated force per size, a high Km motor constant (equals low thermal losses), and low cogging forces without the need for skewing of the magnets. The high thrust forces possible with these motors make them ideal for accelerating and moving high masses, and maintaining stiffness during machining or process forces. Ironless motors have no iron, or slots for the coils to be wound on. Therefore, these motors have zero cogging, a very light mass, and absolutely no attractive forces between the coil assembly and the magnet way. These characteristics are ideal for applications requiring very low bearing friction, high acceleration of lighter loads, and for maximizing constant velocity, even at ultra low speeds. The modular magnet ways consists of a double row of magnets to maximize the generated thrust force and to provide a flux return path for the magnetic circuit.


Data symb. unit ICD05-
050
ICD10-
050
ICD10-
100
IC11-
030
IC11-
050
IC22-
030
IC22-
050
IC22-
100
IC33-
150
IC44-
150
Max. power Fmax N 280 560 1130 375 625 750 1250 2500 5625 7500
Max. current Imax A 8,5 15,8 15,8 11,3 11,3 11,0 11,0 22,0 33,1 44,1
Constant power
(with 130°C)
FN N 87 171 615 151 276 298 548 1198 2718 3617
Constant current
(with 130°C)
IN A 2,0 3,8 3,5 4,0 4,4 3,9 4,4 9,5 14,4 19,2
Current meziobv. UDC V 330 560
Mot. constant
(with 130°C)
KM N/W 14,5 20,5 31,3 18,9 26,9 26,4 37,7 58,5 90,7 105
Current. constant
(with 25°C)
KE V/m/s 36,3 36,4 72,8 30,9 51,4 61,7 103 103 154 154
Power constant (with 25°C) KF N/A 44,5 44,6 89,2 37,8 62,9 75,6 126 162 189 189
Max. . loss PC W 36 69 101 64 106 128 212 420 897 1193
Resit two stage (with 25°C) R2Ph ohmů 4,5 2,2 3,9 1,9 2,6 3,9 5,3 2,2 2,1 1,5
Ind. two stage with distance air
L2Ph mH 14,4 7,3 13,9 16,7 26,7 33,4 53,4 26,0 25,8 19,3
Air distance less case   mm 0,8 (+/- 0,2)
Air distance with case   mm 0,6 (+/-0,2)
Temp. resist coil upon condenser
Rth °C/W 2,9 1,52 1,04 1,64 0,99 0,82 0,50 0,25 0,12 0,088
Gravity power
Fa kN 0,9 1,8 3,6 1,1 1,9 2,3 3,9 7,8 17,7 23,5
Teoretic max. acceleration amax g 30,2 30,7 33,7 15,3 17,7 15,9 18,5 20,4 21,0 21,0
Case
    IP 55
Category cover
    F(DIN 57530)
Tepl. sepnutí termost. °C 120+/-5
Termistors   ohmy/120°C     1650
Second parts (k=lenght) symb. unit
MC-
050-k
MC-
050-k
MC-
100-k
MC-
030-k
MC-
050-k
MC-
030-k
MC-
050-k
MC-
100-k
MC-
150-k
MC-
150-k
Efektiv width magnets b mm 50 50 100 30 50 30 50 100 150 150
Lenght sec. part k mm 64, 128, 256
Lenght prim. part   mm 135,5 183,5 183,5 200,2 200,2 376,2 376,2 376,2 552,2 728,2
Weight prim. part +/-15% mp kg 1 2 3,5 2,5 3,5 5 7 12,5 27 36
Weight  sec. part
+/-15%
ms kg/m 4 4 7 5,5 7,5 5,5 7,5 13 21 21
 
 Site map | About web | Print page
 | created by Omega Design