Report of the British Rife Group. Presented to the International Rife Technology Conference. Las Vegas March 2002.

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Cory Wells
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1 Report of the British Rife Group Presented to the International Rife Technology Conference. Las Vegas March 2002.

2 Introduction. I came away from the last Rife conference with a sense of excitement, tinged with sadness. Excitement, because I was convinced that we were rapidly approaching a major breakthrough in Rife technology and the development of devices that could finally replicate the success of Dr Rife`s medical experiments. But sadness? Well, some of you have technical and historical information that is not being shared. I think it is time to remind us all that we gather together in a sense of community with the intention of solving a major scientific mystery, and benefiting the health of others. Rife research is the collective product of shared knowledge. In the past vested interests, to include former members of the American Medical Association, have acted to suppress what could have been a fascinating and beneficial medical technique. Putting it bluntly, lives have been lost because commercial advantage was put before the needs of patients. A wise man once said that those who do not learn the lessons of the past are condemned to repeat them. Let us learn from this and share our knowledge freely. Remember, selfishness is not a virtue. The British Rife Group was formally established last year as a small team with professional expertise in electronic and biological sciences. We are bound together by a determination to provide scientifically proven answers to remaining questions in Rife research. This document is an account of some of our work in progress, and a series of conclusions from repeatable data. We humbly offer this to the Rife community in the hope that its application may lead to new and improved medical treatments. Stuart Andrews. RTEB Secretary, British Rife Group. 2

3 Contents. 1. The secrets of the 1939 production Beam-Ray Machine. 2. Rife tube fields & effects. 3. Rife Missing Link? The significance of Impedance in Rife Therapy. -a paper by Aubrey Scoon. 3

4 1) Secrets of the 1939 Production Bean Ray Machine. Through a set of unique circumstances, members of the British Rife Group recently had the opportunity to examine and test an original 1939 production Beam-Ray machine. History. This device was discovered walled up in the closet of a former Doctors surgery. It had lain there undisturbed for some fifty years. The name of the original Doctor who possessed it, and possibly used it, is unknown. The machine was in a poor state of repair and replacement of some power supply components were necessary before active electronic testing could be undertaken. With the machine was discovered a single page from an undated diary. This page contained pencil written dial settings and a corresponding list of diseases, presumably for which the machine was used to treat. Physical Description. Note: Beam Ray Corporation Logo on lid. The machine consists of a large metal cabinet approximately 24 inches high by 23 inches wide with operational controls on the front panel, test jacks on the rear panel and a bracket on the left hand side that we believe held a spring loaded arm on which was mounted the Rife plasma tube. A flip up lid was provided on the top of the cabinet in order to gain access to critical oscillator stages, for calibration purposes and for replacement of electron tubes. 4

5 A Beam Ray logo was in evidence on both the top lid and the main access panel on the back of the machine. Operational controls on the front of the machine were as follows: Far left: Four position band switch oscillator control. Centre: Continuously variable vernier oscillator control. Far right: Power output control. In addition to the there were various switches for electron tube heaters and an operate switch which activated the high voltage feed to the RF power oscillator. Block Diagram. 4 band osc. 16Hz- 200Khz RF Osc + vari reactance Plasma Tube PSU 1 PSU 2 As can be seen in the above block diagram, the machine consists of a four band oscillator, with an operational range of between 16 Hz to 200,000 Hz. 5

6 Each of the four ranges are continuously variable. This oscillator has a separate and relatively well smoothed power supply. This four band low frequency oscillator feeds a power triode which acts as a self oscillating radio frequency (RF) power oscillator. This is coupled to a Rife tube of Phanotron design via a variable reactance path. A separate high voltage power supply is provided for this RF oscillator, with a power supply rail exhibiting a high degree of ripple. Circuit Description. For the purpose of this document, I shall be using the British convention of describing electron tubes as valves ; this is to prevent confusion between description of tubes and Rife tubes. (Please don t protest to your Congressman on this one!) Please see Figure 1. (see Appendix for larger view) Fig. 1. This is the schematic of the Beam Ray low-frequency oscillator stages. The circuit consists of a standard Wien-bridge oscillator of the Hewlett Packard design; this being the most stable of all oscillator designs that were available pre World War II. Please note lamp F1 as part of the feedback path on the 6SJ7 valve. The use of a Wien-bridge oscillator in this machine gives us our first and most surprising conclusion: that beam ray machines used sine waves, and not square waves! 6

7 Later electronic testing showed a pure sine wave at the output (across C5) of the cathode follower buffer amplifier 6K6A. 1 Another surprise followed when we set the Wien bridge oscillator to the dial settings for BX (band 4, dial 10) given on the hand-written pencil notes. We obtained a frequency of Hz or Khz. We then set the machine to the other dial setting in the notes, and found that in all cases the active frequencies produced by this 1939 machine were 10 x that of the standard Crane-Stafford frequencies of the 1950s. This reminded us of a very strange letter written by Dr. Millbank-Johnson on November 4 th Johnson stated that while working in the laboratory, they had found a new wave band of frequencies. Johnson goes on to mention that this new band broke glass in the laboratory. Frequencies of Hz etc. are supersonic in that they cannot be heard by the human ear. But when generated at a sufficiently high amplitude, they have the capability to cause resonant destruction of glass and other fragile materials. Our conclusion then, is that this explains the effect that Johnson observed in The use of 10 x Crane frequencies may be of great significance to the actual operational uses of modern Rife technology. We urge researchers to try this out. It is noted in the bottom right hand of the schematic that a 6SN7 valve ( double triode) remains unconnected and performs no electronic function. It is speculated that this may have been intended as part of a multivibrator (flipflop) circuit to provide gating or, to act as another stage of buffer amplification. We simply don t know at this time. The Wien-bridge oscillator stages of this machine produce a highly stable sine wave output variable from 0 to 50 volts, peak to peak. 1 A quick note of explanation: at no time since the recovery of this machine have any of the pre-set oscillator controls been adjusted in any way. We left things exactly as we found them. In other words, just as they had been set in 1939 or in the 1940s. 7

8 We now move on to the main RF stage. See Figure 2. (See Appendix for larger version) Fig. 2 This consists of a medium MU 812A power triode coupled in a tuned anode self-oscillating configuration. A full wave power supply is provided by two 866A diode valves feeding a simple LC smoothing circuit (L1-C2). RF choke L2 prevents radio frequencies from being reflected back into the power supply. It is noted that the main smoothing capacitor C2 is only 2 uf (2 Microfarads) resulting in a high ripple current on the main power supply rail. This high voltage rail operates at approximately 990 V while the oscillator is running. A Jack socket is provided at J2 to inject an external frequency source or, alternatively (and more likely) to monitor the output of the Wien-bridge during calibration. Jack socket J3 forms the main cathode feed to the 812A triode and would be a convenient monitoring point to measure combined grid and anode current. The 812A triode produces an output in the region of 40 Watts RF, and Rife researchers will appreciate that this is a far lower power than we have been led to believe was used in Main carrier frequency was measured at 4.6 Mhz with harmonics being noted at 2.15 Mhz and 9.09 Mhz. This is to be expected as there is no harmonic suppression in this circuit. There are a number of features in this circuit that are both unique and ingenious. 8

9 Firstly, the main RF tuning capacitor C1 is series fed to ground by the plasma tube (at Jack point J1). This means that the plasma tube itself forms part of a variable capacitor, and that it will be reactive when brought near any object or patient. This means that the main frequency tuning of the RF oscillator will change according to the individual capacitance of a patient. We believe this to be significant, particularly as contemporary accounts describe the tube being placed within 10 inches of the patient. Secondly, the ground wire output of the plasma tube is fed to ground via R4 rheostat ( or in modern terms, a variable resistance ) This was found to be set at 2.2 Kilo-ohms. Such a resistor at this point in the circuit will provide the means to precisely control the impedance match of one of the many characteristics of the plasma tube. It is worth remembering that the later Vern-Thompson machine incorporated a similar arrangement, but used switched resistors instead of a variable one. Thirdly, a combination of 120Hz ripple ( in the USA ) on the main high voltage power supply rail and a 60Hz ripple noted at pin 1 (cathode) of the 812A valve will result in a 60Hz gating, or additional modulation, of the signal passing through this valve. This is the reason, we suspect, why Philip Hoyland, the designer, did not use the 6SN7 as a gating device in the Wien-bridge oscillator. He found another way to achieve the gating effect with greater simplicity! Modulation from the Wien bridge is applied across the grid via L4. The circuit needs about 50 volts peak to peak, at this point, to drive the 812A to full (100%) modulation. It is noted that the Wien-bridge amplitude control R4 enables modulation depth to be varied. During our experiments we found that the best results were obtained at levels of 100% modulation. The effect of applying this sort of modulation to the grid of a self oscillating RF triode are two fold. Firstly; It places a changing amplitude audio voltage on the grid which modulates the 812A. This results in amplitude modulation, that is, the strength of the RF power oscillator changes. Secondly; the change of overall grid voltage caused by the applied modulation signal will move the 812A up & down its operating curve. This affects the reactance of the valve. Because the 812A is a free running RF oscillator, changing the reactance results in a change of frequency. In short, frequency modulation. What does this mean? It means that our 812A is generating a 4.6Mhz carrier that is both amplitude and frequency modulated. In conclusion. This 1939 circuit incorporates a variable reactance power oscillator, producing AM & FM components. The RF voltage swings up to 2 Kilo volts. This is different from modern Rife-Bare devices which produce a 9

10 low voltage, high current signal from a linear amplifier. The 1939 machine generates a high voltage, low current waveform that drives the plasma tube. Enough already! - lets see some wave-forms. 10

11 Wave Forms Above. Measured at RF oscillator output, modulation at 1430 Hz, 90% modulation depth. Above. Again 1430 Hz, oscilloscope time-base expanded to show components within gated burst of modulation. 11

12 Above. Current and voltage waveforms at 3930 Hz, 100% modulation. Above. Result of 120% over-modulation Hz. Note extensive harmonic components. 12

1939 machine gates at approximately 16 ms (milli-seconds).

13 Above Hz modulation at 35%. Note with a USA/Canadian mains frequency of 60 Hz, the output of the 1939 machine gates at approximately 16 ms (milli-seconds). With European mains frequency of 50 Hz, gating will occur at approximately 20 ms. Time base expanded version of above waveform. 13

14 Pictures of the Machine. Above. Wien bridge modulator oscillator with valves removed. Above. RF oscillator section. Rectifiers on the left, main tuning coil on right. 14

15 Above. RF section running at full power. 812A triode on the right. Above. Helium plasma tube at 25% modulation. As the RF section produces voltages of over 2 KV, the tube lights every time! 15

16 Appendixes Figure 1: Beam Ray LF Oscillator. Figure 2: RF power section and output. 16

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19 2) Rife tube fields & effects. During our experiments with a number of Rife type devices, we observed a specific and directional field output from the plasma tube. See Figure 1. Fig. 1 Electric field vector -15Ø from +ion axis Positive ion beam A narrow ( 5 degree wide ) electric field was detected, and this forms a plane around the plasma tube. See Figure 2. Fig 2. 5Ø ( Only half the field is shown in this picture ) The plane of the field wobbles around the tube centre axis, as M.O.R frequency is varied. 19

20 Low light observations and special photographic exposures seem to suggest evidence of differing electron cloud formations around the angled electrode. The density and position of these electron clouds is dependant on applied voltage, gas type and modulation excitation. It is our belief that the electron clouds form a crude lens which serve to separate and deflect plasma ions and give rise to a focusing of the electric field. The existence of such a narrow, directional, electric field may have treatment implications. We are reminded that Dr Rife was quoted as stating that he used a Heathkit field strength meter to locate some sort of directional energy emission from the plasma tube, and that this energy was aimed to the patient. 20

21 3) Impedance- the missing link in Rife Research? -a paper by Aubrey Scoon. 21

A Prototype Frequency Machine for Plasma Tube Research

A Prototype Frequency Machine for Plasma Tube Research This document describes a prototype Frequency Machine which I have built for the purposes of Rife experimentation and other plasma tube research.