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1) ORIGINAL RIFE RAY TUBES AND WHAT THEY DID a) Tube construction b) Tube light output pattern relative to electrical
signal input and its ability to
c) Tube as direct ultrasound generator from activity
of violent ion movement
d) Tube as multipole field generator which affects
tube glass wall and charged
e) How ultrasound effects periodically spaced elastically
coupled and closed on
2) NEW TYPE OF "RIFE RAY TUBE" a) Tube construction b) Tube light output pattern relative to electrical signal input c) Tube as a multipole field generator d) Tube as a direct ultrasound generator e) Voltage wave forms to use with new / old Rife tubes f) Simple electrical circuits to use with new / old
Rife tubes
1a) Tube construction Apparently on a hunch, Dr. Royal Raymond
Rife came up with the idea of an audio to radio frequency modulated gas
discharge source for destroying microbes. He called this device a
frequency instrument. The original Rife tubes used in Rife's frequency
instruments were old time X - ray tubes that had been back filled to a
low pressure with helium and/or argon gas. The X - ray tube had a
hot tungsten filament and a flat metal plate surface, a few inches away
from the filament, for tube electrodes. The tube envelope was spherical
and made of fussed quartz (see Figure 1).
The tubes were apparently driven by two oscillators. One oscillator a sine or square wave oscillator which supplied the driving voltage and current to the gas filled X - ray tube. The second oscillator was of a lower frequency and was probably a square wave oscillator used to turn on and off (modulate) the higher frequency being supplied to the X - ray tube. This X - ray tube had a hot tungsten cathode which gave the tube some diode characteristics. That is a preference for current flow in only one direction. However, do to the high operating voltages used ( ~ 900 volts RMS ) at low gas pressure, along with the ample electron generation from ultraviolet light emissions from the metastable states of the inert gases used, the tube was electrically conductive in both directions. Figure 1 shows a qualitative diagram of the frequency instrument. Figure 2 &
3 shows a amplitude modulated sine wave voltage being chosen for the
driving voltage for the tube. Figure 3 shows the magnitude of electron
current flow through the "diode"
Rife discovered that when he would observe
a microbe (be it a bacteria, rickettsia, virus, and or protozoa) under
his microscope while exposing that particular microbe to a particular discharge
pulse rate (light flashing rate) from the frequency instrument the microbe
would be deactivated. He found that all microbes had their own specific
discharge pulse rate (frequency) which deactivated them. Rife called
these their mortal oscillation rate (MOR). Note that there are two
light pulses per single complete voltage oscillation cycle. In other
words there is a frequency doubling effect here. Rife suspected that
some sort of mechanical resonance phenomena in the microbe's structure
was at work in this deactivation process. However, he apparently
did not have any specifics about what the process was. Depending
on the output light intensity and the direct tube wall ultrasound output
of the frequency instrument when operated at the MOR for a particular microbe,
the microbe's reaction could vary from just loosing its characteristic
luminescent and or florescent color (as seen in the field of view of the
Rife microscope) to the microbe violently exploding.
1c) Tube as direct ultrasound generator from activity
of violent ion movement
Figure 5 illustrates
the typical conditions occurring in a steady state direct current discharge
in a gas at low pressure, called a glow discharge. Note how the charged
ions separate themselves out into steady state patterns. Now imagine
that the polarity on the tube electrodes was abruptly reversed. The
glow discharge would immediately reorganize itself into the mirror image
of what is shown in Figure 5. This abrupt reorganization will cause
the generation of a violent shock wave inside the tube, if the time interval
for polarity reversal is significantly less than the time it takes a normal
sound pressure wave to cover the distance between the electrodes.
This shock wave generation is do to the rapid group collision between the
ions and neutral atoms / molecules during reorganization. These shock
waves will react with the tube wall deforming it and causing pressure waves
to be sent into the room air. Continuous abrupt polarity reversals
on the tube electrodes will cause the continuous production of pressure
waves into the room with a main frequency component equal to the polarity
reversal rate. We should also expect the tube to act as a resonance
chamber for specific frequencies of ultrasound generated by the shock waves.
1d) Tube as multipole field generator which effects
tube dielectric wall material
Also, it should be noted that the dielectric material
of the tube wall (fussed quartz) is polarized / deformed by the electric
fields associated with the net charge distributions occurring inside the
discharge tube. The rapid oscillating polarization / deformations
associated with the oscillating discharge current produces ultrasound in
the room air. Figure 6 illustrates
how a piston moving with a sinusoidal velocity creates a sinusoidal pressure
wave in air. The same kind of sinusoidal velocity movement of a tube
wall will produce a sinusoidal pressure wave to be sent into the room air.
1e) How ultrasound effects periodically spaced elastically
coupled and closed
About half the viruses that infect plants and
animals have a outer coat (capsid) which has an intrinsic geometry as illustrated
in When real viruses of the structural type as illustrated
in Figure 7B are in living tissue they are deformed into spheroids.
This is do to the interaction of the virus capsid with the environment.
The bi-lipid coat on the surface of the capsid has an affinity with water
and this tends to deform the capsid into a sphere and with tension on the
surface. The capsid and its outer bi-lipid coat form a simi-permeable
membrane and the phenomena of osmotic pressure causes the capsid to expand
and be under tension. There are other hydrophobic and hydrophilic
reactions that can cause and contribute to capsid deformation as was illustrated
in Figures 9D, E, and F.
However, the larger the amplitude (displacement
from equilibrium) of the oscillation, the larger the stress on where the
elastic cords are attached. If the cords are not well secured to
the ceiling or floor, the cords may decouple before the system goes into
equilibrium with the rhythmic driving force. In the case of the periodically
spaced, elastically coupled, and closed on themselves virus capsid sub-structures
of Figure 10C, the "floor" and "ceiling" connections are weak hydrogen
bonds between adjacent protein clumps of the virus capsid. Figures 11B, C, and D illustrate several standing
wave oscillation modes that a ten member protein clump ring can support.
Maximum stress / tension occurs at the location of standing wave nodes
and the weakest regions on the protein clump ring is where the clumps bond
together with mainly hydrogen bonds. That is approximately half way
between adjacent protein clump centers of mass. Therefore, we see
that the oscillation modes illustrated in Figures 11B and D are very destructive
where as that of 11C is only marginally destructive.
2a) Tube Construction The new type of "Rife ray tube" I am
proposing has two parallel wires going down the center of a relatively
narrow and thin wall glass / quartz cylinder which is closed off at the
ends and contains the standard Neon Sign gas mixture of neon - argon gas
at low pressure. Figure 12 illustrates
just such a "Rife ray tube". Figure 13
shows the various gas pressures used in the operation of various gas discharge
devices. The gas discharge phenomena which we wish to make use of
in our new "Rife type tube" is the corona discharge. The pressure
range of interest is from around 30 mm Hg to around 200 mm Hg. In Figure 12
the ratio of (2S/D) must be greater than 5.85 or the wanted
corona type discharge does not occur from parallel wires, but instead a
spark occurs. See Gaseous Conductors by James Dillon Cobine
for technical details ( pages 252 to 258 ).
2b) Tube light output pattern relative to electrical signal input The light output pattern for a square wave amplitude modulated sine wave voltage driven discharge, such as that used in Figure 2, should be qualitatively the same for the new type of Rife ray tube. There will be subtle and not so subtle differences depending upon the various gas pressure, voltage, and frequencies used. However, the same basic relationship between electron current and light intensity output will still hold. That is, they are approximately directly proportional to each other. So, the same sort of time varying surface force on the target from the time varying light intensity can be expected as before with the old type Rife tubes. 2c) Tube as a multipole field generator As before in the old type Rife tubes there will be rapidly changing back and forth net charge configuration inside the discharge tube driven by the supply voltage. This is clearly illustrated in Figure 14. And as before these oscillating net charge configurations have electromagnetic fields which extend outside the discharge tube and effect the ions in the target (patient) causing these ions to oscillate back and forth and generate pressure waves in the patient just as the old Rife tubes did. 2d) Tube as a direct ultrasound generator As before in the old Rife type tubes the rapid reversals of electrode polarity causes ion current flows / movements that generate shock waves in the discharge tube gas. These shock waves in turn deform the tube wall and cause both compression and rarefaction waves in the wall material, all of which generate pressure waves in the room air in contact with the tube wall surface. The main frequency components produced in the room air are the same as the tube's driving voltage, however do to other types of plasma oscillation that can occur in this type of plasma discharge we should not be surprised by other frequency components being present. It should also be noted that this new Rife Tube design can produce much stronger shock waves, which in turn can produce much stronger pressure waves in the room air. The reason for the stronger shock waves is the close proximity of the parallel wire electrodes, their occupation of the entire tube length, the electrodes being close to the tube wall, and the large voltage gradients near the surfaces of the parallel electrode wires. 2e) Voltage wave forms to use with new / old Rife tubes The important thing to understand and note is that by choosing a tube driving voltage similar in form (shape) to that of Figure 16A, we can expect to a first approximation pressure waves of the same form as in Figure 16A. If the ultrasound frequency which kills a particular microbe is known, a voltage sine wave of that frequency can be supplied to the tube to generate that ultrasound frequency. If that voltage sine wave is amplitude modulated as illustrated in Figure 16A for the pressure sine wave, then we can expect a ultrasound frequency spectra generated in the target similar to that illustrated in Figure 16B. Now, if the amplitude modulation frequency is much lower than the carrier frequency, say 1 / 1,000 the carrier frequency instead of the 1 / 19 the carrier frequency as illustrated in Figure 16A and B, then we would expect a Fourier spectra qualitatively similar to Figure 16B, but now with the Fourier frequency components of significant intensity being bunched up close to the carrier frequency. The significance of this ultrasound frequency bunching together is that it can compensate for calibration drift in the carrier frequency and shifts in the lethal frequency that kills the microbe because of changes in the microbes environment, i.e. different host growth medium constituent concentrations. In Rife's time calibration drift in the carrier frequency was a real problem. Rife could set his carrier frequency on his frequency instrument for let us say 1,000,000 cycles per second as determined from frequency calibration the week before, however now do to temperature changes, humidity changes, and mechanical vibrations with associated electrical component movement the carrier frequency might now be 1,008,000 cycles per second. By amplitude modulating the carrier with a square wave frequency of around 5,000 cycles per second we create a Fourier spectra which has strong components with frequencies within 2,000 to 3,000 cycles per second of the desired carrier frequency of 1,000,000 cycles per second. Now if a particular microbe has a lethal ultrasound frequency of 1,000,000 cycles per second plus or minus 4,000 cycles per second, this sort of carrier amplitude modulation is very useful and in Rife's time apparently essential for practical frequency instrument operation in the doctor's office setting. With the electronic equipment available today
we can easily slowly scan the carrier frequency through the entire frequency
range Rife used and we can do this at high power. This allows us
to use a shot gun like approach and destroy all microbes.
2f) Simple electrical circuits to use with new / old Rife tubes Figures 17 and
Figure 18 illustrate two simple electrical
circuits to be used to drive old / new type Rife tubes. The function
generators shown can be regular electronic tech sweep function generators
that have the sine wave, triangle wave, and square wave output voltage
waves. This circuits can be run in pulsed mode or continuous mode.
These circuits can be used to find the specific frequency(ies) of ultrasound
to kill particular microbes. They can also just be used in the shot
gun type approach mentioned in the last section. The use of these
circuits assumes a certain familiarity with electrical circuits and how
to calculate circuit component values. GOOD HUNTING.
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generated
by the voltage signal from the oscillator. The current flows in both
directions, but there is a prefered direction due to the ability of the
hot cathode to easily supply electrons when it is negatively charged relative
to the plate (anode). Note that the current flow is not proportional
to the voltage. This is for two reasons. First, the electron
emission from the hot cathode is not a linear function of plate - cathode
potential difference (voltage).
Examining
Figure 5e we see that there are regions of net positive and negative charge
created during the discharge process. These net charges have associated
electric fields which extend outside the tube discharge region well into
the room surrounding the tube. These electric fields interact with
the charged ions of the patient's body fluids. As the net charge
distributions oscillate back and forth in the tube, their associated electric
fields oscillate at the patient's location causing oscillations in the
force on charged particles (ions) in the patient. This causes oscillating
motion in the ions imbedded in the patient's body fluids. This intern
causes pressure waves (ultrasound) to be generated from collisions of ions
with mainly water molecules.
In
pressure,
hydrophilic, and hydrophobic interactions of the capsid coat with its environment,
for real viruses. 
