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Industrial Servo Motor SGMRV-09ANA-YR11 Yaskawa Servo Motor For Motoman Robot

    Buy cheap Industrial Servo Motor SGMRV-09ANA-YR11 Yaskawa  Servo Motor For Motoman Robot from wholesalers
     
    Buy cheap Industrial Servo Motor SGMRV-09ANA-YR11 Yaskawa  Servo Motor For Motoman Robot from wholesalers
    • Buy cheap Industrial Servo Motor SGMRV-09ANA-YR11 Yaskawa  Servo Motor For Motoman Robot from wholesalers
    • Buy cheap Industrial Servo Motor SGMRV-09ANA-YR11 Yaskawa  Servo Motor For Motoman Robot from wholesalers

    Industrial Servo Motor SGMRV-09ANA-YR11 Yaskawa Servo Motor For Motoman Robot

    Ask Lasest Price
    Brand Name : Yaskawa
    Model Number : SGMRV-09ANA-YR11
    Price : negotiable
    Payment Terms : T/T, Western Union
    Supply Ability : 100
    Delivery Time : 2-3 work days
    • Product Details
    • Company Profile

    Industrial Servo Motor SGMRV-09ANA-YR11 Yaskawa Servo Motor For Motoman Robot

    Industrial Servo Motor SGMRV-09ANA-YR11 Yaskawa Servo Motor For Motoman Robot


    Quick Details

    Place of Origin:

    Japan, Japan

    Brand Name:

    Yaskawa

    Model Number:

    SGMRV-09ANA-YR11

    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-09ANA-YR11

    Power:

    0.85KW

    Voltage:

    200V

    Current:

    5.7A

    Options:

    With Brake

    Series:

    SGMRV




    OTHER SUPERIOR PRODUCTS

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    Contact person: Anna
    E-mail: wisdomlongkeji@163.com
    Cellphone: +0086-13534205279
    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

    In some cases, decreasing the current is the aim of the exercise. In power transmission lines, for example, the power lost in heating the wires due to their non-zero resistance is proportional to the square of the current. So it saves a lot of energy to transmit the electrical power from power station to city at very high voltages so that the currents are only modest.

    Finally, and again assuming that the transformer is ideal, let's ask what the resistor in the secondary circuit 'looks like' to the primary circuit. In the primary circuit:

    • Vp = Vs/r and Ip = Is.r so

      Vp/Ip = Vs/r2Is = R/r2.

    R/r2 is called the reflected resistance. Provided that the frequency is not too high, and provided that there is a load resistance (conditions usually met in practical transformers), the inductive reactance of the primary is much smaller than this reflected resistance, so the primary circuit behaves as though the source were driving a resistor of value R/r2.

    Efficiency of transformers

    In practice, real transformers are less than 100% efficient.
    • First, there are resistive losses in the coils (losing power I2.r). For a given material, the resistance of the coils can be reduced by making their cross section large. The resistivity can also be made low by using high purity copper. (See Drift velocity and Ohm's law.)
    • Second, there are some eddy current losses in the core. These can be reduced by laminating the core. Laminations reduce the area of circuits in the core, and so reduce the Faraday emf, and so the current flowing in the core, and so the energy thus lost.
    • Third, there are hysteresis losses in the core. The magentisation and demagnetisation curves for magnetic materials are often a little different (hysteresis or history depedence) and this means that the energy required to magnetise the core (while the current is increasing) is not entirely recovered during demagnetisation. The difference in energy is lost as heat in the core.
    • Finally, the geometric design as well as the material of the core may be optimised to ensure that the magnetic flux in each coil of the secondary is nearly the same as that in each coil of the primary.

    More about transformers: AC vs DC generators

    Transformers only work on AC, which is one of the great advantages of AC. Transformers allow 240V to be stepped down to convenient levels for digital electronics (only a few volts) or for other low power applications (typically 12V). Transformers step the voltage up for transmission, as mentioned above, and down for safe distribution. Without transformers, the waste of electric power in distribution networks, already high, would be enormous. It is possible to convert voltages in DC, but more complicated than with AC. Further, such conversions are often inefficient and/or expensive. AC has the further advantage that it can be used on AC motors, which are usually preferable to DC motors for high power applications.


    Product Tags:

    ac servo motor

      

    electric servo motor

      
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