Issue 17 - Free-Energy Devices

Fig. 7. Magnetic orbital engine with interrelated axial and
orbital rotation of inverted rotor magnet
1. Central fixed constant magnet
2. Mobile constant magnet of axial and orbital rotation
3. Rim- ring of magnet 2 rotation round the magnet 1
4. Axial rotation platform of magnet 2
МЭ – aclinic line
МСЛ – magnetic lines of force of magnet 1
Blue color – north pole of magnets
Red color - south pole of magnets
V1 – orbital velocity of magnet 2 rotation round the magnet 1
V2 – axial velocity of magnet 2
However, we noticed an inevitable effect:
having passed the fixed magnet 1 aclinic line,
the magnet automatically swivels in space on
the plane axis to be attracted to the closest pole
of the central CM with its antipole along the
trajectory of its orbital rotation with rim 3.
As a matter of fact, this is a simplified physical
model of a natural magnetic motor in the solar
system (interrelated spontaneous axial and
orbital rotation of constant magnet as to the
central constant magnet).
b) Orbital Magnetic Engine With a Central
Compound Magnet (Quasimonopole) and an
Orbital Mobile Magnet
This is the first device of a totally non-contact
ME with a compound magnet, quasimonopole
of the inverted stator. That is why the rotor
magnet 2 is rigidly oriented on rim 3 as a tangent
to it.
New Energy Technologies, Issue #3 (18) 2004
Fig. 8. Magnetic engine with a compound magnet- quasipole
in the centre
1. Compound magnetic quasipole (2 fixed constant
magnets1-1 and 1-2 are installed oppositely)
2. Mobile constant magnets
3. Rotor with rigidly fixed magnets 2
4. Magnetic shields
5. Magnetic lines of force of magnet 1
МE – aclinic line
VI – linear velocity of magnet 2 rotation around magnet 1
Having analyzed the interaction of magnetic
forces of the mobile magnet of the rotor 2 with
the total magnetic pole of the stator
quasimonopole 1 in such ME, we came to the
conclusion that there is a permanent
accelerating force of the magnet 2 on every part
of its orbit. Actually, the rotor magnet will
accelerate from the point 2-1 of the aclinic line
to the point of the magnetic pole of the
quasimonopole 1. In the point of the rotor
magnetic bar symmetrical installation, as Fig.
8 shows, above the pole of the central
quasimonopole, obliquely and symmetrically to
the polar axis of the quasimonopole, the force
of their magnetic attraction will equal to zero,
as both parts of the magnet 2 are set at one and
the same distance to this pole of the
quasimonopole.
It means, that the force interaction of the rotor
magnet poles is also equal, but is opposite in
sign. If the rotor magnet is mobile on the axis,
it will turn with its antipole to the pole of the
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