Issue 17 - Free-Energy Devices

quasimonopole 1, but it is rigidly fixed on the rim, and it will pass
this pole of the magnet 1 mechanically (with the rim 3). But as
soon as the rotor passes the polar point of the quasimonopole, the
force of magnetic repulsion will act up to the point where it will
cross the aclinic line of the quasimonopole 1. Then, as soon as the
magnet 2 crosses the aclinic line (AL), the force of magnetic
attraction will exert on the rotor magnet pole and the antipole of
the magnetic monopole, due to the heterogeneous magnetic field
of the monopole and closeness of magnetic lines of force in the area
of its second magnetic field. That is, it will move to the antipole, to
the area of the lines closeness.
Thus, this ME alternates the magnetic forces of attraction and
repulsion. The attraction force of magnets 1,2 exerts from the point
2-1 up to the moment, where the rotor magnet 2 approaches the
antipole of the quasimonopole.
This is the force of magnetic attraction to the area of magnetic lines
closeness to the antipole of the quasimonopole. Moreover, the force
is nonlinear and increases as soon as the magnet approaches the
Fig. 9
1. Permanent magnet
2. Permanent magnet
3. Non-magnetic rotor
4. Solenoid-stator
5. Central permanent magnet
6. Commutator
7. Bearing mount assembly
8. Radii
9. Axis of rotation
10. Stand
11. Magnetic lines of force of the central magnet 5
12. Magnetic lines of force of the constant magnets 1, 2
pole of the quasimonopole
along the rim trajectory and
exerts in the area from the
aclinic line to the pole of the
quasimonopole. The force of
repulsion exerts as soon as
the rotor magnet crosses the
magnetic pole of the
quasimonopole.
This force of like poles
repulsion exerts in the area
from the pole up to aclinic
line in the second part of the
magnet 2 trajectory round
the quasimonopole 1- in
comparison with the initial
point 2-1, and it is also
nonlinear and reaches its
maximum right after the
magnetic pole of the magnet
1-1, then it decreases and
equals zero on the aclinic
line.
c) Orbital magnetic engine
with quick and cheap effect
magnetic reversal of the
fixed stator CM with a
rectangular loop of
hysteresis (effect of
magnetic trigger or
Barkgausen effect), Fig. 9.
If feedback is introduced,
the device can operate in
totally automatic regime of
motor-generator in a selflocked
inductive magnetic
system.
It is possible to add
generator inductive
windings on the stator
magnets in the ME
according to the drafts (Fig.
6- 8).
Thus, all the magnetomechanical
devices can
operate simultaneously in
mobile and generating
regimes.
56 New Energy Technologies, Issue #3(18) 2004