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[Keyword] transverse magnetic field(4hit)

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  • Arc Duration of Break Arcs Magnetically Blown-Out in a DC 450 V Resistive Circuit

    Hitoshi ONO  Junya SEKIKAWA  Takayoshi KUBONO  

     
    PAPER

      Vol:
    E95-C No:9
      Page(s):
    1515-1521

    Silver electrical contacts are separated at constant speed and break arcs are generated in a DC100 V–450 V/10 A resistive circuit. The transverse magnetic field of a permanent magnet is applied to the break arcs. Dependences of the arc duration, arc dwell time and arc lengthening time on the strength of the magnetic field and supply voltage are investigated. The characteristics of the re-ignition of the break arc are also discussed. Following results are shown. The arc duration D is increased due to the increase of the arc lengthening time tm when the supply voltage E is increased for each magnetic flux density Bx, because the arc dwell time ts is almost constant. The arc duration D is increased due to the increase of both of the arc lengthening time tm and the arc dwell time ts when the magnetic flux density Bx is decreased. The arc lengthening time tended to become long when the re-ignition of the break arc is occurred. The lengthening time tends to become longer when the duration tm1 from the start of the arc lengthening to the start of the re-ignition is increased. Re-ignitions occurred frequently when the magnetic flux density of the transverse magnetic field is increased and the supply voltage is increased.

  • The Effect of Transverse Magnetic Field on Making & Breaking Arc Durations of Electrical Contact

    Yun LIU  Guangda XU  Laijun ZHAO  Zhenbiao LI  Makoto HASEGAWA  

     
    PAPER

      Vol:
    E95-C No:9
      Page(s):
    1481-1486

    Application of transverse magnetic field (TMF) is one of the most important ways to improve electric life and breaking capacity of DC relays. For better understanding of dependence of arc durations on transverse magnetic field, a series of experiments were conducted under an external transverse magnetic field with 12 pairs of AgSnO2 contacts in a DC 28 V 60 A/30 A/5 A circuit, respectively. By using permanent magnets, the transverse magnetic field was obtained and the magnetic flux density at the gap center was varied from 13 to 94 mT. The results show that breaking arc duration is decreased monotonically with increases in the magnetic flux density, but making arc duration isn't decreased monotonically with increases in the magnetic flux density. In addition, both the magnetic flux density and the breaking arc duration have threshold values Bl and Tbmin, respectively, which means the breaking arc duration is almost stable with the value Tbmin even if the magnetic flux density is higher than Bl.

  • Effect of Axial and Transverse Magnetic Fields on the Arc Duration and Material Transfer

    Guofu ZHAI  Xinglei CUI  Xue ZHOU  

     
    PAPER-Electromechanical Devices and Components

      Vol:
    E95-C No:3
      Page(s):
    395-400

    Axial and transverse magnetic fields are widely used in many kinds of switches to decrease the arc erosion. In this paper, the influence of these two kinds of magnetic fields on the arc phase transition was studied particularly for AgSnO2 contacts breaking a 28 V/25 A circuit. The experiments were carried out under resistive and inductive loads in an atmospheric environment. The relationships between flux densities ranging from 0 to 200 mT and the arc duration were obtained. It was found that the transverse magnetic field was more efficient in balancing the arc phases and decreasing the arc erosion. The results can be used to guide the design of arc extinguishment systems in DC high power relays.

  • Study on the Retrograde Motion of Arc under Transverse Magnetic Field

    Guofu ZHAI  Xinglei CUI  Xue ZHOU  

     
    PAPER

      Vol:
    E93-C No:9
      Page(s):
    1431-1436

    The phenomena of retrograde motion of arc in the atmosphere under transverse magnetic field were studied. AgSnO2 contacts were set in DC resistive and inductive circuits, respectively. The break voltage was 28 V, the current ranged from 1 to 5 A, and the magnetic flux density changed from 0 to 100 mT. A high speed camera and an oscilloscope were used to record time variations of arc images, voltages and currents, simultaneously. Different from previous experiment results, the arc motion showed three stages which was more obvious under larger magnetic flux density in inductive circuit. It was also found that the arc movement was closely related with the arc voltage. Explanation to the retrograde motion under such conditions was given.