Relaxation Time and Semiconductors

Relaxation Time: The time it takes for the free electrons in a conductor (or material) to reach
the skin of the wire after potential is applied, is, of course, called the relaxation time. During that
time, the free electrons in the gas are "trapped" insofar as producing current (dissipation of the
potential) is concerned. However, immediately after the relaxation time ends, current begins and
dissipation of the trapped energy begins.
In copper, the relaxation time is incredibly rapid. It's about 1.5 x 10-19 sec. However, in quartz it
is about 10 days! So as you can see, we need to get somewhere in between these two values,
and so we will have to "mix" or "dope" materials. We must get a sufficiently long relaxation time
so that we can switch and collect comfortably in cycle one, then switch into cycle two for
dispersion of the freely collected energy in the collector. However, the relaxation time we get
must also be short enough to allow quick discharge in the load, as soon as we switch the
primary source away from the collector. Actually, we need a degenerate semiconductor material
instead of plain copper.
Degenerate Semiconductor Material: A semiconductor material is intermediate between a
good conductor and an insulator. It's a nonlinear material, and doped. A degenerate
semiconductor material is one which has all its conduction bands filled with electrons, and so it
thinks it is a conductor. That is, a degenerate semiconductor is essentially a doped conductor,
so to speak. As you can see, we can increase the relaxation time in our "conductors" connected
to the source by making them of degenerate semiconductor material. What we're talking about
is "doping" the copper in the wire, and in the collector, so that we can have plenty of time to
collect, and switch, and discharge, and switch, and collect, etc.
Now in a doped conductor (degenerate semiconductor), we can tailor the relaxation time by
tailoring the doping. We must dope the copper before we make the wire. Why would we wish to
do that? We want to overcome the single problem that so far has defeated almost all the
"overunity" researchers and inventors.
WHEN YOU CONNECT TO A SOURCE, YOU CAN ONLY EXTRACT CURRENT-FREE
POTENTIAL -- FREE "TRAPPED EM ENERGY" -- DURING THE ELECTRON RELAXATION
TIME IN THE CONNECTING CONDUCTORS AND SUCCEEDING CIRCUIT COMPONENTS.
AFTER THAT, YOU'RE STEADILY EXTRACTING POWER, AND THE ENERGY EXTRACTED
FROM THE SOURCE IS BEING PARTIALLY DISSIPATED IN THE RESISTANCE/LOADING
OF THE CIRCUIT, AND PARTIALLY DISSIPATED IN THE INTERNAL RESISTANCE OF THE
SOURCE. IN THE LATTER DISSIPATION, YOU'RE ALSO DISSIPATING YOUR SOURCE BY
DOING WORK ON IT INTERNALLY TO KILL IT.
Good Copper Wire: Bane of Overunity Inventors: Many destitute inventors, tinkering and
fiddling with overunity devices, finally get something (a circuit or device) that does yield more
work out than they had to input. At that point, they usually conclude that it's simply the specific
circuit configuration and its conventional functioning that produces the overunity work. However,
usually as soon as this configuration is more carefully built with very good materials, boom! It
isn't overunity anymore. The inventors and their assistants then desperately bang and clang
away, getting more frustrated as the years pass. The investors get mad, sue for fraud, or get in
all sorts of squabbles. The scientists who tested it and found it wanting, pooh-pooh the whole
thing as a scam and a fraud, or just a seriously mistaken inventor. Scratch one more "overunity"
device.
Most of these inventors got their successful effect (and possibly erratically) when they were
struggling with inferior, usually old, usually corroded materials. Actually, the more inferior, the
better. The more contaminated/doped, the better!
The moment you wire up your circuit with good copper wire connected between the battery or
primary source and any kind of load including the distributed circuitry loading itself, you can
forget about overunity. You will lose it in the copper, after the first 1.5 x 10-19 second!
Think of a really good conductor such as copper as an essentially linear material. Linear means
energy conservative. Overunity can only be done with a highly nonlinear effect. So your
"conductors" have to be made of nonlinear materials. In fact, they have to be made of
degenerate semiconductor material. For the type of circuitry we are talking about, the copper
has to be doped and then made into "doped copper" wiring. You also have to utilize the primary
battery only to potentialize a collector (secondary battery/source), and then use this secondary
battery source to conventionally power the load while also killing itself.
The Wiring And the Collector Must Be of Degenerate Semiconductor (DSC) Material.26 A
good materials scientist/engineer, together with a decent electrodynamicist, can readily design
and tailor some doped copper wiring so that the material in the wiring is a degenerate
semiconductor material, with a target (desired) relaxation time. That's what you should use to
make the wiring to connect up your source to the collector with, and that type of material is also
what you use in your collector. You can use either a coil or a capacitor as the collector, but its
"conductive" material has to be degenerate semiconductor material -- in short, it must be doped
to have the proper relaxation time. From the collector to the load, however, obviously you want
to use a good conductor material. Ordinary copper will do nicely there.
Once you do that, you're in business. When making the DSC material, simply tailor the
relaxation time to something which is easily switched. For example, take one millisec. With a
relaxation time of that long, switching is easy. In fact, one could even use good mechanical
switching. Or easily use inexpensive ordinary solid state switching, without having to go all the
way to nanosecond switching.
Then, in the collector, you calculate the number of "trapped coulombs" you have. Take the
"trapped voltage" (current-free potential's energy density per coulomb) you extract from the
source during the electron relaxation time after the collector is connected. Multiply the number
of trapped coulombs in the collector by the trapped voltage during collection, and you have the
amount of energy in joules that you extract FOR FREE, without paying for it, from the source
during every collection cycle.