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Yaskawa 0.75kW Servo Motor Single-phase 400W Industrial Servo Motor SGMAH

China Yaskawa 0.75kW Servo Motor Single-phase 400W Industrial Servo Motor SGMAH

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Yaskawa 0.75kW Servo Motor Single-phase 400W Industrial Servo Motor SGMAH

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Price： Negotiable
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Payment Terms	T/T, Western Union
Supply Ability	100
Delivery Time	2-3 work days
Packaging Details	New in original box
Brand	Yaskawa
Model	SGMAH-08AAF41
Type	Motors-AC Servo
Voltage	200V
Current	4.4A
Power	750W
InS	B
Brand Name	Yaskawa
Model Number	SGMAH-08AAF41
Place of Origin	Japam

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Product Specification


Payment Terms	T/T, Western Union	Supply Ability	100
Delivery Time	2-3 work days	Packaging Details	New in original box
Brand	Yaskawa	Model	SGMAH-08AAF41
Type	Motors-AC Servo	Voltage	200V
Current	4.4A	Power	750W
InS	B	Brand Name	Yaskawa
Model Number	SGMAH-08AAF41	Place of Origin	Japam
High Light	ac servo motor ，electric servo motor

Yaskawa 0.75kW Servo Motor Single-phase 400W Industrial Servo Motor SGMAH-08AAF41

QUICK DETAILS
Manufacturer: Yaskawa
Product number: SGMAH-08AAF41
Description: SGMAH-08AAF41 is an Motors-AC Servo manufactured by Yaskawa
Servomotor Type: SGMAH Sigma II
Rated Output: 750W (1.0HP)
Power Supply: 200V
Output speed:5000 rpm
Torque rating:7.1 Nm
Minimum operating temperature:0 °C
Maximum operating temperature:+40 °C
Weight:8 lb
Height:3.15 in
Width:7.28 in
Depth:3.15 in
Encoder Specifications: 13-bit (2048 x 4) Incremental Encoder; Standard
Revision Level: F
Shaft Specifications: Straight shaft with keyway (not available with revision level N)
Accessories: Standard; without brake
Option: None
Type: none

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Let's discuss why one might want to introduce an Integral factor into the gain (A) of the control. The Bode diagram shows A approaching infinity as the frequency approaches zero. Theoretically, it does go to infinity at DC because if one put a small error into an open loop drive/motor combination to cause it to move, it would continue to move forever (the position would get larger and larger). This is why a motor is classified as an integrator itself - it integrates the small position error. If one closes the loop, this has the effect of driving the error to zero since any error will eventually cause motion in the proper direction to bring F into coincidence with C. The system will only come to rest when the error is precisely zero! The theory sounds great, but in actual practice the error does not go to zero. In order to cause the motor to move, the error is amplified and generates a torque in the motor. When friction is present, that torque must be large enough to overcome that friction. The motor stops acting as an integrator at the point where the error is just below the point required to induce sufficient torque to break friction. The system will sit there with that error and torque, but will not move.

The excitation sequences for the above drive modes are summarized in Table 1.
In Microstepping Drive the currents in the windings are continuously varying to be able to break up one full step into many smaller discrete steps. More information on microstepping can be
found in the microstepping chapter. Torque vs, Angle Characteristics

The torque vs angle characteristics of a stepper motor are the relationship between the displacement of the rotor and the torque which applied to the rotor shaft when the stepper motor is energized at its rated voltage. An ideal stepper motor has a sinusoidal torque vs displacement characteristic as shown in figure 8.

Positions A and C represent stable equilibrium points when no external force or load is applied to the rotor
shaft. When you apply an external force Ta to the motor shaft you in essence create an angular displacement, Θa

. This angular displacement, Θa , is referred to as a lead or lag angle depending on wether the motor is actively accelerating or decelerating. When the rotor stops with an applied load it will come to rest at the position defined by this displacement angle. The motor develops a torque, Ta , in opposition to the applied external force in order to balance the load. As the load is increased the displacement angle also increases until it reaches the maximum holding torque, Th, of the motor. Once Th is exceeded the motor enters an unstable region. In this region a torque is the opposite direction is created and the rotor jumps over the unstable point to the next stable point.

MOTOR SLIP
The rotor in an induction motor can not turn at the synchronous speed. In order to
induce an EMF in the rotor, the rotor must move slower than the SS. If the rotor were to
somehow turn at SS, the EMF could not be induced in the rotor and therefore the rotor
would stop. However, if the rotor stopped or even if it slowed significantly, an EMF
would once again be induced in the rotor bars and it would begin rotating at a speed less
than the SS.
The relationship between the rotor speed and the SS is called the Slip. Typically, the
Slip is expressed as a percentage of the SS. The equation for the motor Slip is:
2 % S = (SS – RS) X100
SS
Where:
%S = Percent Slip
SS = Synchronous Speed (RPM)
RS = Rotor Speed (RPM)

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Shenzhen Wisdomlong Technology CO.,LTD Mainly engaged in automation parts, PLCS,DCS,sensors, relays, dirves,encoder, servo drive,soft starter,touch screen,instrument,process control,electric transmission and factory automation aspects of the project design,software programming,technical service and ... Shenzhen Wisdomlong Technology CO.,LTD Mainly engaged in automation parts, PLCS,DCS,sensors, relays, dirves,encoder, servo drive,soft starter,touch screen,instrument,process control,electric transmission and factory automation aspects of the project design,software programming,technical service and ...

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