Toroid Coils and Vector Potential
The following information is directed to those involved in
the ATG/Telos Quadra test series. The information content is of little value to
the general public or when when taken out of the context of the Quadra
tests.
The Quadra test power supply

*Note that V1 was increased from 40V
to 50V in series #2 testing and the total capacity was increased to
21.7Kuf.
The pulse power supply consists of 2 x 8200uf capacitors
charged to 50 volts, resulting in the pulse in Joules being equal to the
J
= ½ CV2 or ½
1.64E-2 * 502 = 2.04E1 W/sec
The strange oscillation seen in the Quadra test run, Series
#3B, run #4.
Movement of coils caused from Vector
Potential?
The coils visibly move upward against gravity when excited.
The movement can not be attributed to wire heating on the leads that suspend the
coils. The reason is that if the wire is heated, it would sag and the coils
would move downward rather than upward. In addition the majority of heat would
be generated in the largest resistance, which is the coils themselves. The
resistance of the 1cm
lead lengths is a small fraction of the total
resistance.
Ejecting the paper dot off the Quadra
configuration
The small paper dot cut from 20lb paper is ejected off of
the top of the coils when the coils are excited with a trigger
pulse.
Ejection of a small Fe wire from the center of the Quadra
coils, the loaded wire.

When the coils are pulsed, the wire is shot out like a
missile, a far different reaction than from a common coil where the wire would
attemp to center itself within the coil.
Notice that this is the same direction of force
indicated when the coils are placed horizontal and move upward against gravity.
Where in this test the Fe wire is pushed from the smaller to the larger coils,
indicating the same direction of the force, yet not indicating the magnetic
effect expected.
Can the Vector Potential Bend Laser
Light?
The following is a picture of the photo sensor (without
lens and light tube) that was used in the laser testing. The laser beam was
adjusted to a 0.5mm diameter before striking the lense over the photo detector.
Testing indicated that we could detect a shift of 0.25
degrees.

An increase in beam shift sensitivity was accomplished by construction of
an end cap over the end of the detector light tube. Four holes were placed in
the cap every 90' as shown in the following illustration. The beam was adjusted
so that it fell just out side of the holes. If the beam moved in any way
the photocell would detect light. The sensor was placed 15 meters from the coils
and the laser entered the coils from 20cm behind.
![]()