Claims Analysis
Total Claims: 3
Claim 1
Independent Claim
295 words
A gyroscopically stabilized magnetic suspension system, comprising: (A) a base assembly comprising: (i) a directed source of electromagnetic energy disposed substantially at the radial center of said assembly; (ii) a first toroidal magnet surrounding said source of electromagnetic energy, said first toroidal magnet having an axis of polarity transverse to its toroidal plane; and (iii) first anti-spin magnets disposed beyond the outer toroidal radius of said first toroidal magnet, said anti-spin magnets having the same axis of polarity as said first toroidal magnet but having an opposite polarity thereto; and (B) a suspended assembly, comprising: (i) electromagnetic energy receiving and converting means; (ii) a motor disposed upon said energy receiving and converting means, having a drive shaft disposed along the axis defined by the axial center of said first toroidal magnet, said motor powered by the output of said energy receiving and converting means; (iii) a second toroidal magnet surrounding said motor and radially connected to the drive shaft of said motor, said second toroidal magnet disposed parallel to the plane of said first toroidal magnet, said second toroidal magnet having a polarity transverse to its toroidal plane, said polarity opposite to the polarity of the first toroidal magnet to thereby form a repulsion mode therebetween; and (iv) second anti-spin magnets disposed axially above said first anti-spin magnets, said second anti-spin magnets having the same polarity as said first anti-spin magnets to thereby form an attraction mode therebetween, whereby the rotation of the drive shaft of said motor will induce a rotation of said second toroidal magnet at a velocity defined by said energy receiving and converting means, and said anti-spin magnets radially beyond said second toroid will define a gyroscopic plane of reference within which said second toroidal magnet will function as a gyroscope.
Claim 2
Dependent Claim
295 words
A gyroscopically stabilized magnetic suspension system, comprising: (A) a base assembly comprising: (i) a directed source of electromagnetic energy disposed substantially at the radial center of said assembly; (ii) a first toroidal magnet surrounding said source of electromagnetic energy, said first toroidal magnet having an axis of polarity transverse to its toroidal plane; and (iii) first anti-spin magnets disposed beyond the outer toroidal radius of said first toroidal magnet, said anti-spin magnets having the same axis of polarity as said first toroidal magnet but having an opposite polarity thereto; and (B) a suspended assembly, comprising: (i) electromagnetic energy receiving and converting means; (ii) a motor disposed upon said energy receiving and converting means, having a drive shaft disposed along the axis defined by the axial center of said first toroidal magnet, said motor powered by the output of said energy receiving and converting means; (iii) a second toroidal magnet surrounding said motor and radially connected to the drive shaft of said motor, said second toroidal magnet disposed parallel to the plane of said first toroidal magnet, said second toroidal magnet having a polarity transverse to its toroidal plane, said polarity opposite to the polarity of the first toroidal magnet to thereby form a repulsion mode therebetween; and (iv) second anti-spin magnets disposed axially above said first anti-spin magnets, said second anti-spin magnets having the same polarity as said first anti-spin magnets to thereby form an attraction mode therebetween, whereby the rotation of the drive shaft of said motor will induce a rotation of said second toroidal magnet at a velocity defined by said energy receiving and converting means, and said anti-spin magnets radially beyond said second toroid will define a gyroscopic plane of reference within which said second toroidal magnet will function as a gyroscope.
Claim 3
Dependent Claim
82 words
The system as defined in claim 1 in which said base assembly further comprises: (iv) a stabilizing toroidal magnet annularly disposed beyond the radius of said first magnet, said stabilizing magnet having the same direction of polarity as said first toroidal magnet, whereby a toroidal field of repulsion, near the outer radius of the attractive field of the anti-spin magnets is formed thereby compressing and thus stabilizing both the attractive anti-spin field and the repulsive field between the first and second toroids.