Specifications
Brand Name :
Yaskawa
Model Number :
SGMRV-09ANA-YR11
Place of Origin :
Japan
MOQ :
1
Price :
negotiable
Payment Terms :
T/T, Western Union
Supply Ability :
100
Delivery Time :
2-3 work days
Packaging Details :
New in original box
Brand :
Yaskawa
Model :
SGMRV-09ANA-YR11
Type :
AC SERVO MOTOR
Power :
0.85KW
Volatge :
200V
Current :
5.7A
Ins :
F
Description

Electric Bicycle Industrial SERVO MOTOR 5.2A Yaskawa Servo Motor 400W SGMRV-05ANA-YR21

Quick Details

Place of Origin:

Japan, Japan

Brand Name:

Yaskawa

Model Number:

SGMRV-05ANA-YR21

Usage:

Electric Bicycle

Certification:

UL

Type:

Servo Motor, Servo Motor

Construction:

Permanent Magnet

Commutation:

Brush

Protect Feature:

Drip-proof

Speed(RPM):

1500RMP

Continuous Current(A):

5.2A

Efficiency:

IE 1

Brand:

WTL

Model:

SGMRV-05ANA-YR21

Power:

0.4KW

Voltage:

200V

Current:

5.2A

Options:

With Brake

Series:

SGMRV

SIMILAR PRODUCTS

SGMRV-05ANA-YR11

SGMRV-05ANA-YR21

SGMRV-09ANA-YR11

SGMRV-13ANA-YR1A

SGMRV-13ANA-YR21

SGMRV-13ANA-YR31

SGMRV-20ANA-YR11

SGMRV-30ANA-YR12

SGMRV-30ANA-YR21

SGMRV-37ANA-YR12

The sketch and circuit show a step-up transformer. To make a step-down transformer, one only has to put the source on the right and the load on the left. (Important safety note: for a real transformer, you could only 'plug it in backwards' only after verifying that the voltage rating were appropriate.) So, how does a transformer work?

The core (shaded) has high magnetic permeability, ie a material that forms a magnetic field much more easily than free space does, due to the orientation of atomic dipoles. (In the photograph, the core is laminated soft iron.) The result is that the field is concentrated inside the core, and almost no field lines leave the core. If follows that the magnetic fluxes φ through the primary and secondary are approximately equal, as shown. From Faraday's law, the emf in each turn, whether in the primary or secondary coil, is −dφ/dt. If we neglect resistance and other losses in the transformer, the terminal voltage equals the emf. For the Np turns of the primary, this gives

  • Vp = − Np.dφ/dt .
For the Ns turns of the secondary, this gives
  • Vs = − Ns.φ/dt
Dividing these equations gives the transformer equation
  • Vs/Vp = Ns/Np = r.
where r is the turns ratio. What about the current? If we neglect losses in the transformer (see the section below on efficiency), and if we assume that the voltage and current have similar phase relationships in the primary and secondary, then from conservation of energy we may write, in steady state:
  • Power in = power out, so

    VpIp = VsIs, whence

    Is/Ip = Np/Ns = 1/r.

So you don't get something for nothing: if you increase the voltage, you decrease the current by (at least) the same factor. Note that, in the photograph, the coil with more turns has thinner wire, because it is designed to carry less current than that with fewer turns.

Electric Bicycle Industrial  5.2A Yaskawa Servo Motor 400W SGMRV-05ANA-YR21 SERVO MOTOR

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Electric Bicycle Industrial 5.2A Yaskawa Servo Motor 400W SGMRV-05ANA-YR21 SERVO MOTOR

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Brand Name :
Yaskawa
Model Number :
SGMRV-09ANA-YR11
Place of Origin :
Japan
MOQ :
1
Price :
negotiable
Payment Terms :
T/T, Western Union
Contact Supplier
Electric Bicycle Industrial  5.2A Yaskawa Servo Motor 400W SGMRV-05ANA-YR21 SERVO MOTOR
Electric Bicycle Industrial  5.2A Yaskawa Servo Motor 400W SGMRV-05ANA-YR21 SERVO MOTOR

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