RIFE FREQUENCIES: FINDING THE ACTUAL ULTRASOUND FREQUENCIES
TO KILL A MICROBE
GIVEN BY GARY WADE ON
(This lecture has been slightly modified and lengthened for the internet presentation (11/1/99).See links below for contact information)
FREQUENCIES TO KILL VARIOUS PATHOGENS
UNDER A MICROSCOPE
1) Microbe / parasite targets which are rampant in the environment.
2) Mechanism and method of microbe destruction.
3) Needed Equipment to accomplish task.
4) Experimental techniques
5) Suggested lethal ultrasound frequencies
Microbe / parasite targets which are rampant in the environment
The parasitic microbes / parasites listed in 1a) and 1b) are fairly common throughout much of the world. Humans are quite susceptible to all of these microbes / parasites and regularly contract infections of one or more of them. In general you can think of multiples of tens of millions of people and or animals currently infected with each listing of 1a) and 1b). Rife type technology can dispose of these microbes / parasites easily and quickly. Let us move quickly to end this needless suffering. Pick several microbes you would like to find the lethal ultrasound frequencies for.
Lists 1a and 1b
1a) Water Supply Microbes / Parasites
Hookworm, Whipworm ( Trichuris Trichiura )
Protoza - Cryptosporidium, Giardia, Ameba (Entamoeba Histalytica)
Flukes - Fasciala, Paragoniums, Heterophyes, Schistosoma,
Metagonemus, Alaria, Opisthorchis, Dicracoelium
1b) Pet and Live Stock Microbes / Parasites
Hookworm (Ancylostoma Canibum), Roundworm (Toxocara Canis,
Toxo cara Cati), Pinworm (Enterobius Vermicularis), Dog Heartworm
Trichinosis (Trichinella Sprirais)
Protoza - Toxoplasma gondii, Isospora, Pneumocystis, Dientamoeba,
Chilomastix, Sarcocystis, Balantidium, Cryptosparidium,
Babesia, Retortamonas, Neopora caninum, Trichomanas
vaginalis, Giardia, Aegieria, Acanthamoeba, Entamoeba
gingivalis, Entamoeba histolytica
Tapeworms - Taenia saginata, Cyticercosis, Taenia solium, Diphyllo-
bothrium latum, Dipyiidium caninum, Hymenolepsis
nana, Hymenolepsis diminuta
Flukes - Fasciola, Paragonimus, Heterophyes, Schistosoma,
Metogonemus, Alaria, Opisthorchis, Dicrocoelium
Spirochetes - Spirochaeta, Saprospira, Cristispira, Treponema,
Mechanism and method of microbe destruction
About half the viruses that infect plants and animals have a outer coat (capsid) which has an intrinsic geometry as illustrated in Figures 1A and 1B. In animals the outer coat (capsid) of the virus is also covered with a bi-lipid layer obtained from the infected host cell from which the virus budded off of. Other virus types that will not be talked about here have analogous or similar symmetries and periodisities which make them also susceptible to easy disruption and distruction from specific frequencies of ultrasound.
In Figure 2A the black dots represent spheroid shaped large single protein molecules. Usually two or more types of protein spheroids make up the virus capsid coat. These large protein molecules are deformable and are elastic in nature. Figures 2B and 2C illustrate the periodically spaced, elastically coupled, closed on themselves protein clump structures that are formed when Figure 2 is folded into an icosahedral of Figure 1B.
When real viruses of the structural type as illustrated in Figure 1B 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 coat forms a simi- permeable membrane an 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. Figures 3A through F illustrate this situation.
The bonds between adjacent protein molecules in the virus capsid coat are generally hydrogen bonds and these are relatively weak chemical bonds. To a first approximation we can treat each protein clump (molecule) in the capsid coat as a simple harmonic oscillator as illustrated in Figure 4C. Imagine in Figure 4C that the center of mass is a steel ball. Imagine that that steel ball has two elastic cords attached to it and that the cords are attached to the ceiling and floor respectfully. And furthermore, the elastic cords are under some tension. Now imagine that the ball is pulled back and let go. The ball will oscillate back and forth at some constant frequency. If the tension is now increased in the cords and the ball is again pulled back and let go, the ball will again oscillate back and forth at a constant frequency, but now at a higher frequency. In fact the frequency of oscillation will vary approximately proportional to the square root of the tension in the cords for small displacements from equilibrium of the ball. If the ball is exposed to some small rythmic driving force of the same frequency of oscillation that is natural for the mass of the ball and the tension in the cords present, then the amplitude (displacement from equilibrium) of oscillation will increase until the energy release into the surrounding environment by the motion of the ball and cords per oscillation cycle equals the energy being supplied per cycle by the rhythmic force. 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 4A, the "floor " and "ceiling" connections are weak hydrogen bonds between adjacent protein clumps of the virus capsid. Figure 4E illustrates the most stressful standing wave oscillation mode on a ten member protein clump ring. In this oscillation mode adjacent protein clumps are oscillating 180 degrees out of phase, that is as one protein clump is moving upward from its equilibrium position the adjacent clumps are moving down ward and visa versa. This type of oscillation mode puts maximum tension / stress on the weak hydrogen bonds holding the protein clumps to each other. At some relatively small displacement amplitude the hydrogen bonds will fail and the ring / capsid coat will disintegrate. Rife observed viruses exploding like little hand grenades when they were exposed to their mortal oscillation rate (MOR).
Figures 5B, 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 5B and D are very destructive where as that of 5C is only marginally destructive.
Figures 6A and B illustrate two more very simple virus capsid coats. By following the instructions and building the capsid coat models, you can see how many types of periodically spaced, closed on themselves protein clump structures you find and also how many overlapping and tangential closed protein clump structures you can find. RIFE MACHINE INFO
Needed Equipment to Accomplish Task
a) Microscope with TV camera
b) B and K 10 MHz sweep function generator
c) VCR with time readout on video tape capability
d) Sweep controller box (see Alteronics below)
e) Ultrasound transducer that mounts on microscope stage (see Alteronics )
f) TV monitor
g) 20 MHz oscilloscope (optional)
Alteronics - Equipment available from Alteronics (1-530-589-4926). And ask about their new combination sweep function generator and controller box unit built for just this type of experimental research.
A great deal of very useful work can be done at relatively low magnification (~400 power) when dealing with one cell animals and multicell parasites. However, when trying to find the lethal ultrasound frequencies for bacteria much higher power is needed (1,200 to 2,500 power) and some special light staining technique such as Rife used are very helpful and definitely needed for good research results (finding the lethal ultrasound frequencies).
Figure 7A is the conceptual flow chart for carrying out the experimental research.
The intensity (energy / area / time ) of ultrasound output of the piezoelectric transducer of Figure 7B is a very non-linear function of the peak to peak voltage of the driving voltage signal. The intensity goes as the fourth power of the peak to peak driving voltage. For example, if the peak to peak voltage of a sign wave driving voltage is doubled, the sign wave pressure wave output intensity is increased by a factor of
16 = (2)(2)(2)(2). It is only the sine and cosine voltage wave forms which are transformed into cosine and sine wave pressure waves respectfully (see Figure 8). All other voltage wave forms are transformed by the piezoelectric transducer into another type of wave form. For example, a voltage triangle wave form is transformed into a pressure square wave form by the piezoelectric transducer (see Figures 9A and B).
All commercially available piezoelectric transducers have an effective cut off frequency above which they can not produce significant and generally useful ultrasound output. The best commonly available PZT piezoelectric transducers that I use, start to quickly lose their ultrasound producing ability a little above 12 MHz. To get around this short coming there is a trick. That is to use a voltage triangle wave form at a frequency below the cut off frequency of the piezoelectric material being used and use the hidden higher frequency ultrasound components in the generated pressure square wave to kill the microorganism. Figure 9C, D, and E illustrate the first three hidden Fourier components in the pressure square wave of Figure 9B which was generated by the transducer being supplied with the voltage triangle wave form of Figure 9A.
Figures 10A and 10B show the power absorption / power radiated verses frequency curves for some mechanical resonators / oscillators. The curve of Figure 10B where b=bo is a more realistic looking shape for real viruses, which are in general the easiest structures to destroy do to their high symmetry. Everything stated in the caption of Figure 10A still holds true, only it is more obvious in Figure 10A.
Here are the technical details for implementing the experimental setup shown in the flow diagram of Figure 7A, to kill specific microbes.
Examples of scanning technique
1) The controller box going from 0 to +10 volts in time T and connected to VCG input on B and K sweep function generator set to 10 MHz.
For our purposes we need to know the relationship (the particular equation) between frequency (F) and time (t) in the experimental run when the controller box voltage starts at 0 volts and linearly progresses to +10 volts in time T. Refer to Figure 11.
F = M t + B
F = First variable, M = Slope of line, t = Second variable, B = F axis intercept
(Frequency) (Rise / Run) (time)
Run = t2 - t1, Rise = F2 - F1 , M = (F2 - F1) / (t2 - t1)
In Figure 11, F1 = 10 MHz, F2 = 2 MHz, t1 = 0, t2 = T. Using these values we obtain
M = (- 8 MHz / T). Substituting in initial values of frequency and time ( 10 MHz and 0) into our straight line equation above we obtain:
F = ( - 8 MHz / T ) t + 10 MHz
What this last equation tells us is that once you place the total time (T) for the scan into the equation you can find the frequency of the generator at any specific time t. So using the time (t) readout on the video camera / VCR you can determine the frequency at which the microbe came undone (dead).
2) Controller box voltage output going from +10 volts to 0 volts in time T. See Figure 12. Using the same procedure as before we obtain:
F = ( + 8 MHz / T ) + 2 MHz
Suggested Lethal Ultrasound Frequencies
Let us first deal
with cancer. If cancer is suspected it is important not to kill off a tumor too
quickly. If large amounts of tumor are killed off, you now have a bacterial
feeding ground which can lead to toxemia which can lead to kidney and liver
failure. So, if the suspected cancer you have is susceptible to specific frequencies
of ultrasound, as the great majority of cancers were in Dr. Royal Raymond
Rife's time, you should consider perhaps one treatment cycle every two or three
days giving the body adequate time to deal with the kill off. However, if you
live in California or some other states you must ignore this entire last
paragraph, despite my constitutional rights of free expression both verbally
and of the press. In California by law (AB 1707.1) "The sale, offering for
sale, holding for sale, delivering, giving away, prescribing or administering
of any drug, medicine, compound or device to be used in the diagnosis,
treatment, alleviation or cure of cancer is unlawful unless (1) an application
with respect thereto has been approved under Section 505 of the Federal Food, Drug
and Cosmetic Act or"... . In California, you are only allowed to treat
cancer with whole body poisoning which havily damages your immune system and is
often carcinogenic in nature, massive carcinogenic in nature radiation damage,
and disfiguring and disabling surgery. Your health and well being in
As a practical
matter, if you wish to experiment on yourself to see if you can kill off a
cancer tumor on yourself, you will need a piezoelectric transducer, possibly a
controller box, and a standard sweep function generator used by electronic
technicians. Get a sweep function generator that has a four digit LED readout
(a 10 MHz B and K unit will do). There are over a dozen ultrasound equipment
manufactures in the
(11,780,000 cycles per second) / 3 = 3,926,666 cycles per second. Similarly, the first Fourier hidden component is 23,560,000 cycles per second, if the triangle voltage wave form has a frequency of 7,853,333 cycles per second. So, by slowly scanning through these lower triangle voltage wave form frequencies, the hidden Fourier higher frequency pressure sine waves are generated.
The third experimental protocol is perhaps the most interesting. It has been found empirically by several independent researchers that a pressure square wave of 2127 cycles per second can quickly destroy many types of cancer tumors. However, as stated earlier, you do not want to kill off a tumor to quickly. A conservative treatment approach that has achieved successful results is as follows: Running the function generator at maximum output, place the transducer on or near the tumor for one and one half minutes. Then wait three days to see if the kill off was O.K. or too big ( very painful inflammation of tumor tissue). If O.K. continue treatment . If, not then wait until all this subsides before treating yourself again. When treating yourself again use one half the treatment time used before. Again, wait a couple of days to see how big the kill off was.
It is best to kill off the cancer in small amounts over two or three months. This will allow the liver and kidneys to do their jobs without making the body toxic. Large amounts ( 5 to 10 grams) of vitamin C can be taken daily with lots of water (minimum of 10 oz. per gram of vitamin C) to detox. A buffered vitamin C is probably best for most people.
The actual mechanism that kills the cancer cell when using the 2127 cycles per second pressure square wave is not known. However, my guess is that one or more of the Fourier pressure wave components closely matches the mechanical resonance frequency of one or more of the cell's specific ion gates. Cancer cells have very abnormal ion concentrations in them. If ion gates for specific ions are opened up by these Fourier components the ion concentrations can be changed drastically inside the cancer cell and the bi-lipid membrane potential difference can fall drastically. If this potential difference fall is to large the cell can not recover and dies.
Here are photo copies of actual Rife research note book pages. A set of approximately twenty 24 such pages was supplied to me by Jasson Ringas. Table 1 is a compilation of the key frequency data for the microbes listed in those 24 pages.
In table 2 are listed some of the standard disease treatment frequencies used by voltage square wave generators, such as those made by John Crane. When electrodes are used on the body, which have voltage square waves applied to them, these voltage square waves among other things produce discontinuous steady state ion transport in the body electrolytic fluids. This discontinuous steady state ion transport produces sets of pressure square waves that have the full spectrum of relative phase differences, but all centered about the same frequency. These pressure square waves have the same center frequency as the driving / applied voltage square wave. And just as indicated in Figure 9 there are many hidden Fourier higher frequency components in the pressure square wave. Using voltage square waves to produce pressure square waves in body fluids is very inefficient. However, by using a voltage triangle wave put into a piezoelectric transducer, much more powerful pressure square waves can be produced. Therefore, using voltage triangle waves of the same frequency as listed in Table 2, we can expect much quicker and dramatic results. By using the formula given with Figure 9, you can use a standard sweep function generator and using the sine wave output function to see which hidden Fourier frequency(ies) are actually responsible for the dramatic results often seen.