‘WO little/087255
`
`PC'i‘lKRZfill3/0GIGE4
`
`current value necessary for the RLC serial resonant circuit can he calculated,
`
`By designing the magnet coil 170 of the apparatus for creating pulse magnetic
`
`stimulation according to the present invention as the singlewlayer solenoid, centers of the
`
`respective circular coils are placed on a central axis of the magnet coil Nil hy Ampere’s
`
`5
`
`right—handed screw law. As seen from. the target point, the individual magnetie flux is
`
`spaced from the origin point by the same distance, and as a result, the magnetic flux is
`
`added, so that it is possible to effectively generate the magnetic flux. Furthermore: the
`
`magnet coil 170 may he constructed as a multilayer wiring solenoirh but since the
`
`resistance and inductance are increased due to the increase of the number of windings,
`
`-0
`
`the singielayer winding shape applies to the apparatus for creating pulse magnetic
`
`stimulation according to the present invention Furthermore, in a case of application of
`
`the single—layer winding shape}, there is an advantage that relatively low storage voltage
`
`can be used to obtain the induced voltage
`
`Fig. 4B is a View illustrating a prhiciple oi" focusing the magnetic flux.
`
`The magnet coil 170 formed in the single~layer solenoid type is surrounded
`
`with a protective member having a tennis racket shape and having an insulating feature
`
`"for protecting the magnet cell 170. The protective member for the magnet coil 170 has
`
`air holes as many as possible to cool the generated heat in an air cooling manner, and is
`
`a mobile type.
`
`When it is necessary to focus the magnetic flux on one point; a magnetic flux
`
`30
`
`it?!
`
`[\‘3
`
`Q
`
`

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