Intensity of Ultra Sound Generated the Rife Frequency Instrument

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The Intensity Of Ultra Sound Generated In The Upper Surface Of The Skin ByThe Rife Frequency Instrument by Gary Wade

[This is a REVISED and CORRECTED version of the Appendix B, which was originally released Jan12, 1993. This version was updated specifically for release on the internet. Gary Wade, May 6, 2000]

There are now four types of Rife frequency instruments:

1) The original type used an X- ray tube that had been back filled with helium and/or argon gas at lowpressure. This ray tube was used to emit high frequency light pulses. The tube also produced directultrasound in the room air from the vibration of the tube walls due to plasma shock waves generatedinside the tube. Furthermore, this tube produced multiple oscillating electric fields which caused ions inthe patients body to oscillate back and forth generating low intensity ultrasound.

2) The second type uses electrode contact with the skin to induce a sonic transducer action in thedead skin layer, induce charge density waves in the body's electrolytic solution, and produce very lowintensity pressure square waves due to constant drift velocity collisions of the body's salt ions underthe influence of the square wave voltage used. The charge density waves couple with the dipole layerof charge on the cell membranes to produce broad band ultrasound. Also, the electric fields

associated with charge density waves can denature delicate proteins on virus surfaces making thevirus unable to infect target cells. This second type of Rife frequency instrument was popularized byJohn Crane and will be discussed in APPENDIX C.

3) The third type uses gas filled tubes at low pressure as contact electrodes to the body. These gasdischarge tubes are supplied withoscillating high voltages, which producestrong charge density waves in the bodysalt solution, high intensity sonic pings inboth the tube wall and the dead skin layer,and low intensity pressure waves in bodyfluids do to ion current flow collisions withother molecules. All of these effects causethe generation of low intensity broad bandultrasound among other things.

4) The fourth type uses a piezoelectrictransducer element which convertsvoltage wave forms applied to thetransducer into mechanical oscillationswhich, like the other types of Rifefrequency instruments, destroys the


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microbe when the produced mechanical oscillation frequency matches the microbe's lethal mechanicaloscillation frequency.

Apparently on a hunch, Dr. Royal Raymond Rife came up with the idea of an audio to radio frequencyintensity modulated gas discharge source for destroying microbes. He called this device a frequencyinstrument. It apparently consisted of two oscillators. One was a sine or square wave oscillator which

supplied the driving voltage and current to a gas filled tube. The tube was a X-ray tube which hadbeen back filled with helium and or argon gas to a low pressure. The second oscillator was of a lowerfrequency and was probably a square wave oscillator used to turn on and off (modulate) the higherfrequency being supplied to the X-ray tube. This X-ray tube had a hot tungsten cathode which gavethe tube some diode characteristics (a preference for current to flow in only one direction). However,due to the high operating voltages used at low gas pressure along with substantial electron generationat the X - ray tube "anode" from ultraviolet light emissions from the metastable inert gases used, thetube gas was quite electrically conductive in both directions.

Figure 1 shows a qualitative diagram of the frequency instrument while Figure 2 shows a amplitudemodulated sine wave voltage being chosen for the driving voltage for the tube. Figure 3 shows themagnitude of electron current flow through the "diode" generated by the voltage signal from theoscillator. The current flows in both directions, but there is a preferred direction do to the ability of the

hot cathode to easily supply electrons when it is negatively charged relative to the plate (anode). Notethat the current flow is not proportional to the voltage. This happens for two reasons: First, the electronemission from the hot cathode is not a linear function of plate-cathode potential difference ( voltage ).Figure 4 illustrates how electron emission current depends on plate voltage and filament temperature.Secondly, the electrons gain kinetic energy on the way to the anode and if the tube driving voltage ishigh enough (and it is), the electrons gain enough energy to be able to ionize one or more helium /argon atoms during collisions with them while transiting the ray tube. These freed electrons join in thecurrent flow across the tube and also make collisions, thus freeing yet more electrons. The lightemission rate from the tube which determines the light intensity is proportional to electron collision ratewith helium / argon atoms. The electron collision rate with helium / argon atoms at a constant tubevoltage is approximately proportional to the electron current. Therefore we should expect the lightoutput intensity of the ray tube to have approximately the same shape as the electron currentmagnitude ofFigure 3. Just replace the electron current magnitude label on Figure 3with a tube light

intensity output label. Also, note that the X-ray tube wall was built from fussed quartz and thereforepassed ultraviolet, visible, and upper end IR "light".

Rife discovered that when he would observe a microbe ( be it a bacteria, rickettsia, virus or protozoa )under his microscope while exposing that particular microbe to a particular discharge pulse rate fromthe frequency instrument, the microbe would be deactivated. He found that all microbes had their ownspecific discharge pulse rate ( frequency ) which deactivated them. Rife called these killingfrequencies their mortal oscillation rate (MOR). Remember, the tube is also producing directultrasound into the air that has the same main frequency as the flashing light rate. Note that there aretwo light pulses per single complete voltage oscillation cycle. Also, note that there are two positive ionshock waves generated per voltage oscillation cycle. In other words there is a frequency doublingeffect here.

Rife suspected that some sort of mechanical resonance phenomena in the microbe's structure was atwork in this deactivation process. However, he apparently did not have any specifics about what theprocess was. Depending on the output light intensity and the direct tube wall ultrasound output of thefrequency instrument when operated atthe MOR for a particular microbe, themicrobe's reaction could vary from justloosing its characteristic luminescentand or florescent color (as seen in thefield of view of the Rife microscope ) tothe microbe violently exploding. Rifefound that when test animals which wereinfected with a disease causing microbewere treated by the frequency

instrument operated at the MOR of thatmicrobe, the test animals were cured.

Under the auspices of the Special
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Medical Research Committee of the U.S.C. Medical School, clinical trails on sixteen terminally illcancer patients using the frequency instrument were conducted in 1934. Rife, in the mid 1920's , hadisolated from and associated with cancer tumor tissue, two types of motile virus particles. In 1932 Rifewas able to make these isolated virus particles carcinogenic by exposing them to 24 hours of UV lightfrom a high voltage argon gas discharge. These exposed viruses were 100 % carcinogenic wheninjected into test animals (see Appendix G). Rife found that these two forms ( labeled BX and BY )

caused at least 95 % of the cancers at that time. Sixteen out of sixteen terminally ill cancer patientswere cured of cancer in those trials. It should also be mentioned that while Rife treated them forcancer, he also cured many other disease conditions these patients had.

In Appendix D, the details of how and why specific frequencies of very low intensity ultrasound candestroy viruses and bacteria are derived and discussed using standard physics. Here we wish to knowthe approximate intensity of ultrasound necessary to kill the cancer virus and other microbes as wasdone by the Rife frequency instrument used in the U.S.C 1934, 1935, and 1937 clinical trials.

We should anticipate three significant physical processes being involved in generating ultrasound inthe patients:

One, pressure waves being generated in the patient from exposure to oscillating light intensity from

the X - ray tube.

Two, direct generation of ultrasound from the X - ray tube walls vibrating from their interaction withplasma shock waves generated by tube electric current flows and electric fields from oscillating chargedensity distributions.

Third, oscillating forces on the ions in the salt solution of the patient's body from the oscillating electricfields of the discharge tube ( X - ray tube ). These oscillating ions inside the patient produce pressurewaves (ultrasound).

The intensity ( Watts / Meter squared ) of an acoustic sinusoidal wave when expressed in terms ofpressure is frequency independent and is given by:I = ( P )2 / ( 2D V ) ; where I is intensity in watts / meter squared , P is the maximum pressure in

Newton / meter squared , D is the density of the medium in kilograms / meter cubed , and V is thevelocity of sound in meters / second in the medium. P will now be calculated approximately and alongwith approximate assumed values for D and V, I will be given to within two orders of magnitude. Withperhaps two orders of magnitude of slop, this may seem like a non useful result. However, we shallfind that the results have some profound implications. Figure 5A shows a frequency instrument beingused on a cancer patient. Assume the light leaves the ray tube uniformly in all directions.

Then the light intensity on the patient's abdomen directly below the tube as illustrated in Figure 5Bisequal to the total light out put in watts divided by the surface area of a sphere which has a radius equalto the shortest distance between the center of the ray tube and the patients skin surface. We willassume 40 % efficiency in conversion of electric power to light, this includes UV, visible, and IR in theray tube. The quartz wall of the X-ray tube passed UV, visible and upper IR band light through it.

The tubes used in the clinical trials dissipated around 80 watts. Therefore, we assume approximately32 watts of radiant light energy is emitted. Now looking back at Figure 3 we see that the light is emittedin pulses which to a first approximation can be approximated as a square wave modulated sine wavepattern. The 32 watt light output power is the root mean square ( RMS ) value of the output power( W{RMS} ) in the form of light. For a sine wave, the relationship between the peak instantaneouspower output and the root mean square value is :

W ( peak value ) = ( 2) W ( RMS value ). However, since the duty cycle of the square wave modulationis 50 / 50 , we must multiply our W (peak value) by a factor of 2. Light carries momentum and whenlight is absorbed by the skin, that momentum must be conserved. It is conserved by being convertedinto the longitudinal wave momentum of the pressure pulse that travels into the body. The peakamplitude of that pressure pulse associated with each light pulse is:

P = ( Pointing's vector ) / ( speed of light ) = S / C ; where S is the magnitude of Pointing's vector andC is the speed of light.

S = the instantaneous energy per time crossing unit area.
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S = ( (4) W( RMS value ) ) / ( Surface area of sphere )

P ( peak value ) = { (4) (32 watts) / (4*)(.3 m)2 } / ( 3 x 108 m/sec. )

P ( peak value ) = 3.76 x 10 -7 Newton/meter squared

The outer surface of the skin is made up of a dead skin cell layer. These cells have approximately10% water content and the rest is essentially protein. I know of no density or speed of soundmeasurements for this dead skin material. I will now assume a density of .7x103 kilograms/metercubed ( 70% of that of water ) and a speed of sound of 50 meters / second ( similar to vulcanizedrubber ). Using these values for P ( peak value ), D ,and V we obtain:

I = ( 3.76 x 10-7 n/m )2 / ( (2)(.7x103 kg/m3 )( 50 m/s ) ) = .2 x 10 -17 w/m2

It should be noted that in this approximation calculation, the fact that significant radiant "light" passesthrough the dead skin layer and is absorbed in the living tissue is ignored. Proper consideration of thisfact does not significantly change the results for the value of I calculated.

Now, let us, consider the ultrasound intensity generated in the air by the mechanical oscillations of thewall of the X - ray tube. From the operation of current gas filled tubes which are similar to Rife's tube,with some what similar electrode design, gas mixtures, pressures and power dissipation, it isexperimentally known that such tubes when operated at auditory frequencies make an audible sound.This sound occurs whether the tube is ran at mega hertz frequencies with audio frequency amplitudemodulation or simply by a audio frequency sine wave voltage. This sound can be produced by threeactions:

One, the bulk flexing of the tube wall under the influence of the plasma shock waves.

Two, the propagation of compression and rarefaction waves through the tube wall, which weregenerated by the interaction of plasma shock waves with the wall interior.

Three, the deformation of the dielectric material of the tube wall from interaction with high electricfields from the discharge plasma.

The sound is not very loud, but is clearly audible as long as the back ground sound is not too loud.The average human ear can just detect (hear) a tone of ~ 1,000 cycles per second in a very quitebackground, at around an intensity level of 10 -12 W / m 2. I believe that it is safe to assumeultrasound emission intensities of around 10-10 to -9 W / m2 for these Rife type tubes. As statedabove, the intensity of an acoustic sinusoidal wave when expressed in terms of pressure is frequencyindependent and is given by:

I = ( P )2 / ( 2DV); solving for P we have: P = ( 2DVI )1/2 ; if we now place into this equation the valuesof I = 10-10 to -9 W/m2, V = 333 m/S (speed of sound in air), and D = 1.22 kg/m3 ( air density ), weobtain P = 2.9 x 10 -4 t0 -3 n/m2. This would be the approximate sinusoidal air pressure variation

range experienced on the skin surface by a patient located only a few inches from a Rife type tubemaking the auditory sound mentioned above. Now the important question to ask is:

What is the intensity of the sound that travels into the patient's body generated by the sinusoidal airpressure variation experienced on the skin?

Looking at Figure 6we see the propagation path of sound waves from a Rife ray tube as they go fromair through the dead skin layer and into the living body. For simplicity, I have chosen propagation atright angles to the body surface and I have considered the body to be composed of two homogeneouslayers. Note that there is internal reflection / echoing at the dead skin medium interfaces. However, forour purposes, we will ignore this phenomena. From the calculations done on Figure 6, we see that theintensity of sound (I2) passing into the dead skin layer is :

I2 = { ( T12 )2 ( D1 V1/ D2 V2 ) } I1 ,

and similarly the intensity of sound passing into the living flesh is:
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I3 = { (T23)2 ( D2 V2 / D3 V3 ) } I2

substituting in the appropriate values of constants into these equations we obtain:

I3 = 7.7 X 10 -14 to -15 W/m2

If the above calculated values of ultrasound intensity are responsible for the amount of the observedmicrobe kill off with a Rife frequency instrument, then there are two important points to be made andrealized at this time. First, our approximation calculation for ultrasound intensity ( I ) of mega hertzultrasound actually generated by the tube wall are probably off (too large) by two or more orders ofmagnitude, therefore it is clear that what is normally thought of as a totally harmless and insignificantultrasound intensity can have profound effects on microbes. We can make this statement becauseRife and medical doctors which used his frequency instrument cured thousands of patients ofmicrobe / virus caused diseases using power levels in the ray tube we used for calculation purposesabove.

The second point to be made is that the microbes and viruses have high Q - values when consideredas mechanical resonators. Where 2E / Q is the approximate total vibration energy released ordissipated by a vibrating system per complete oscillation cycle of the system. E is the total energy

stored in the oscillator (potential plus kinetic energy). This Q - value as used above is understood for asimple oscillating system, such as a mass attached to a spring while going back and forth (oscillating)on a frictional surface. However, in our virus system it becomes a little more tricky to use, becausethere are so many vibration modes that can be simultaneously in existence.

For example when you pick up one of the virus models you have constructed from the material youhave been supplied in APPENDIX D, keep your finger on one of the spherical protein clumps. Nowcount to see how many different closed "ring" of protein clumps this one protein clump belongs to.Note that for each separate closed ring this protein clump has three independent degrees of vibrationassociated with each resonant frequency mode for each closed ring. These three independentdegrees of vibration consist of two transverse vibrations at right angles to each other and onelongitudinal. The physical displacement of one transverse vibration occurs approximately in the localtangent plane to the surface in which the clump is located and at right angle to the ring's local

curvature.

The other transverse vibration has its displacement occur at right angles to the first and occurs in theapproximate direction of above and below the local tangent plane to the virus's surface. Thelongitudinal vibration displacement occurs back and forth along and parallel with the local direction ofthe closed ring of clumped proteins. Once you realize that all of these vibration modes are allowed tocoexist together on the outer coat of the virus, you see that the coat is a "sitting duck", just waiting toabsorb resonant vibration energy up to the point where it comes apart by rupture of the weak bondingbetween adjacent protein clumps.

What about the effects of oscillating electric fields from the tube generating ultrasound in the patient?Well from the positive results from the use of such devices as the Lakhovsky Multiple Wave Oscillator,it is clear that we can expect similar results from a Rife frequency instrument when in close proximity

to it.

Figure 7a shows a closed ring of protein clumps such as are found in the outer capsid coat of a virus.Figure 7b shows the mathematical abstraction ofFigure 7a. Each protein clump has a mass m, andthey have a distance a between their centers of mass. The elastic connecting force is provided by theself elasticity of the protein clumps, which are weakly bound together mainly with hydrogen bonds. Atension in the closed ring of protein clumps is maintained by osmotic pressure and, by hydrophilic andhydrophobic interactions between the outer virus coat and water and other chemical compounds in theenvironment. The magnitude of this tension in the ring and the spacing of the protein clumps inconjunction with the mass of the protein clump determines the fundamental natural mechanicaloscillation frequency for the ring, which are most destructive to the ring.

Document 1 is a copy of the actual lab note book used by Rife in his lab on 11/20/32 when he found

the MOR to kill the BX-cancer virus, which was the main cause of carcinoma-type cancer in Rife'stime. Another form of the BX virus which Rife named the BY cancer virus causes sarcoma- typecancer. Both BX and BY cancer viruses are possibly destroyed by the same MOR, but this must beverified experimentally.
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Note that:

1) The size and shape of the BX cancer virus is that of an ovoid 1/15 microns = 750 Angstroms inlength and 1/20 microns = 500 Angstroms in width.,

2) The virus is motile (it has a proton transport driven flagella the same as its bacterial parent uses),

3) The virus has a luminescent and/or fluorescent color of purple-red,

4) The MOR is 11,780,000 cycles per second.

Note that due to the above stated frequency doubling effect, that the ultrasound frequency of23,560,000 cycles per second may be the true fundamental (MOR).

WARNING, ultra sound of 11,780,000 or 23,560,000 cycles per second should not be used to treatcancer patients unless the required relationship between ultrasound intensity and treatment time forsuccessful treatment is understood (see Appendix C for detailed calculations). From the aboveapproximate calculations Rife probably used ultra sound intensity of around (10 -15 to -17 w/m2) for

three minutes once every three days. Usually the patient would be free of all tumors in seventy toninety days. What Rife did was to kill off only the surface layer of the tumor and then allowed thebody's immune system to remove the dead tissue before killing the next layer.

All "normal" cancer cells in Rife's time were teeming with either the BX or BY cancer virus. Thesecancer viruses are highly absorptive of ultrasound at their resonance frequencies. Ultrasound at theresonance frequencies is highly absorbed and exponentially attenuated as it enters a tumor mass. Ascancer viruses in the outer regions ( surface ) absorb critical resonant vibratory energy, they ruptureand no longer effectively absorb resonant ultrasound. The ultrasound effectively penetrates deeperand deeper into the tumor mass. If the normal ultrasound intensity of around ( 2 X 104 w/m2) used forphysical therapy in sports injuries is used, all tumors will be mortally wounded within a few seconds.However, when large tumors are involved, unless serious medical intervention is taken, the patient willquite possibly die in seven to ten days from a combination of kidney failure, liver failure, and toxemia

from the abscesses formed from the dead tumor masses becoming a bacterial feeding ground.

It now seems that bacteria have locations on their cell membrane / cell wall where they have proteinclump-type structures similar to viruses in that they form closed, periodically spaced structures. Thereis enough of the virus coat type pattern so that there exists at least one closed ring of protein clumps.Of course, this ring can be ruptured by the same mechanisms as the virus forms. When the bacteria'svirus-like clumped protein structure is ruptured by exposure to the acoustic resonance frequency, theosmotic pressure of the bacteria is relieved by the contents of the bacteria exiting out the rupture sitewhich is enlarging as the elastic energy of the stretched bacteria cell wall is relieved. Also, the cellmembrane potential difference will collapse. Bottom line: the bacteria will die.

Members of the Special Medical Research Committee of the University of Southern Californiaincluded: Dr. Milbank Johnson, M.D., member of the board of directors of U.S.C. and committee

chairman, Dr. Rufus B. van Klein-Schmidt, president of U.S.C., Dr. Charles Fischer, M.D., of theChildren's Hospital in New York, Dr. Hayland Morrison, M.D., chief surgeon of the Santa Fe Railway,Dr. George Dock, M.D., of Pasadena, Dr. Karl F. Meyer of the George Williams Hooper Foundation inSan Francisco ( U.C. Berkeley ), Dr. Alvin G. Ford, M.D., president of the American Association ofPathologists of Pasadena California.

Other doctors observing and collaborating on the results of the 1934 U.S.C. Special Medical ResearchCommittee clinic were: Dr. Ray Lounsberry, M.D., Dr. James B. Couche, M.D., Dr. E.F.F. Copp, M.D.,Dr. Thomas Burger, M.D., all of the San Diego area. Dr. Arthur Isaac Kendall, Ph.D., of NorthwesternUniversity faculty, Dr. Joseph Heitger, M.D., of Louisville, Kentucky, Dr. O.C. Gruner, M.D., head ofthe Archibald Cancer Research Committee of McGill University of Montreal, Canada, Dr. E.C.Rosenow, head of the department of research and bacteriology of Mayo Clinic, Rochester, Minnesota.

Taken from: DR. RIFE AND THE DEATH OF THE CANCER INDUSTRY, a paper by physicist GaryWade Jan 12, 1993


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Intensity of Ultra Sound Generated the Rife Frequency Instrument