TRAVELING VEHICLE SYSTEM

• US 20110101792A1
• Filed: 06/19/2009
• Published: 05/05/2011
• Est. Priority Date: 07/04/2008
• Status: Active Grant

• Current Assignee: Murata Machinery Limited (Muratec)
• Original Assignee: Murata Machinery Limited (Muratec)
• Inventors: Koumoto, Homare
• Granted Patent: US 8,519,570 B2
• Time in Patent Office: Days
• US Class Current: 307/104
• CPC Class Codes: B60L 2200/26 Rail vehicles
• CPC Class Codes: B60L 5/005 without mechanical contact between the collector and the power supply line
• CPC Class Codes: H01L 21/67766 Mechanical parts of transfer devices robots in general in B25J
• CPC Class Codes: H02J 50/12 of the resonant type
• CPC Class Codes: H02J 50/70 involving the reduction of electric, magnetic or electromagnetic leakage fields

Abstract

A contactless power feed type traveling vehicle system prevents and minimizes leakage of the magnetic field from a power feed cable and includes an AC power source, a power feed cable, a power reception pickup, and a magnetic field reducing section. The power feed cable is connected to the AC power source. The power reception pickup is provided on a traveling vehicle and arranged to receive electric power through the power feed cable in a contactless fashion. The magnetic field reducing section includes a coil antenna and a capacitor. An induced electric current flows in the coil antenna due to a magnetic field generated by an electric current flowing in the power feed cable. A resonance relationship is established between the coil antenna and the capacitor such that the induced electric current in the coil antenna is out of phase or in opposite phase with the electric current flowing in the power feed cable.

Claims

1-4. -4. (canceled)

5. :

A contactless power feed system, comprising;

an AC power source;

a power feed cable connected to the AC power source;

a power reception pickup that is provided on a traveling vehicle and arranged to receive electric power through the power feed cable in a contactless fashion; and

a magnetic field reducing circuit including a coil antenna and a capacitor connected to the coil antenna, the coil antenna being arranged to carry an electric current induced therein by a magnetic field generated due to an electric current flowing in the power feed cable, a resonance relationship is established between the coil antenna and the capacitor such that the induced electric current in the coil antenna is out of phase with the electric current flowing in the power feed cable.

6. :

The contactless power feed system according to claim 5, wherein the capacitor is arranged to achieve the resonance relationship in which a magnetic field generated by the induced electric current in the coil antenna cancels out a magnetic field generated by the electric current flowing in the power feed cable.

7. :

A magnetic field reducing method for a contactless power feed system including an AC power source, a power feed cable connected to the AC power source, and a power reception pickup that is provided on a traveling vehicle and arranged to receive electric power through the power feed cable in a contactless fashion, the method includes the steps of;

preparing a coil antenna; and

preparing a capacitor by adjusting a resonance relationship with respect to the coil antenna such that a magnetic field generated by an induced electric current in the coil antenna cancels out a magnetic field generated by an electric current flowing in the power feed cable.

8. :

The magnetic field reducing method for a contactless power feed system according to claim 7, wherein the adjusting of the resonance relationship includes a step of adjusting a phase 8 of the induced current in the coil antenna and a magnetic field H generated at the coil antenna by the induced current using the following relationships;

impedance Z of a circuit including the coil antenna and the capacitor=ω

L−

1/ω

C;

induced voltage Vc generated across the coil antenna=−

N×

dΦ

/dt;

induced current I generated in the coil antenna=Vc/Z;

the magnetic field H generated at the coil antenna by the induced current=I/(4π

r)×

[J(J²+r²)<sup>−

1/2</sup>];

the phase θ

of the induced current=cos<sup>−

1</sup>(R/Z);

where L is an inductance of the coil antenna, C is a capacitance of the capacitor, N is the number of windings of the coil antenna, dΦ

/dt is a rate of change of a magnetic flux in the coil antenna, r is a distance from the coil antenna to a magnetic flux that is to be reduced, J is a length of the coil antenna, and R is a DC resistance of the coil antenna.