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