Thinking of buying a replica of the original Rife Beam Ray device, also known as Rife machine or Rife MOPA (Master Power Oscillator Amplifier)? For more information and pricing, please contact us through our website: Demonstrated here is a replica of the historical Rife Beam Ray device that was used by medical doctors during the 1930s with a reported high success rate in curing some of the infectious and other more severe diseases. The original concept and research were done by Dr Royal Raymond Rife during the 1920s and '30s during which he discovered so-called MOR (Mortal Oscillatory Rate) frequencies of some pathogens. Those MOR frequencies were then applied (radiated) from the plasma antenna and used to kill targeted pathogens without noticeably affecting the rest of the organism adversely. Beam Ray devices were a later design done by Philip Hoyland during the period of cooperation with Dr Rife from 1935 to 1938. In this design, harmonics are created on both sidebands.
Notes:
00:00:10 – The triode heated filament power supply is turned on.
00:00:16 – The power supply of triode filament heating is voltage-stabilised to provide ideal potential even in cases when electrical mains potential is fluctuating. The electronic circuit on the right side of the power supply is a high-frequency preamplifier for the modulation signal input. Both circuits share the same large heatsink, which in operation becomes slightly warm. The anode power supply, filament heating and preamplifier transformers, as well as the anode high-voltage DC power supply, soft start circuit and microcontroller-driven turn-on/turn-off control circuits, are all placed under the middle section of the enclosure.
00:00:30 – After the triode filament heating is turned on, control circuitry doesn't allow any user operation for 1 minute. In that way, the stress on the triode is reduced during turn on/turn off sequences.
00:00:36 – After 1 minute, the control circuitry allows for normal user operation, i.e. start/stop. Each time the device is started, the soft-start circuit reduces initial stress on the triode.
The operation of the device is visible by the appearances of the anode current on the front panel instrument, the carrier signal on the screen of the oscilloscope and the presence of plasma in the Phanotron tube.
00:00:46 - The carrier wave frequency is adjustable. In this case, the adjustment range is 2.6 - 3.45 MHz. The carrier wave adjustment range includes historical carrier wave frequency of 3.3 MHz, but it also goes as low as possible. The advantage of the lower carrier wave frequency is that it requires a lesser number of LSB harmonics to reach targetted MOR, i.e. more energy is transferred. The existence of the carrier wave frequency (it is not suppressed) and of the USB harmonics means that the higher harmonic frequencies of the targetted MOR shall also be produced. The existence of higher harmonics of the MOR frequencies may be beneficial if the true MORs are higher harmonics of Dr Rife's set of historical frequencies that he used.
00:01:00 – The close vicinity of the grounded object within 20-30 cm (in this case, the hand) affects carrier wave frequency through capacitive coupling. The same effect is present in all of the historical plasma antenna based devices of Dr Rife and Philip Hoyland. The same effect of capacitive coupling is used to detect the E-field around the plasma antenna (Phanotron tube) by connecting the oscilloscope probe to a conductive surface.
00:01:10 – The carrier wave frequency is set with no modulation applied.
00:01:20 – The modulation of the carrier wave is applied, and the signal is zoomed out to observe the effects of the modulation.
00:01:34 – Carrier wave is modulated to 100% with the sine wave of up to 30 kHz, in the same way as it was with the historical Rife Beam Ray devices. In that way, distinctive high-frequency signal bursts are produced, during which plasma is ionised. During the periods when no signal is present plasma partially deionises.
00:01:38 - The effects of the modulation on the carrier wave and consequently on the output signal are evident after the modulation is turned on.
00:01:57 – Depending on the modulation frequency, there are periods when the output signal is effectively not present, and no E-field is produced around the Phanotron tube (plasma antenna).
00:02:10 – The effects of the output impedance matching are observable on the amplitude of the output signal. Better impedance matching between the output of the device and the plasma antenna results in a decrease in power losses and increase in strength of the E-field (indicated by the higher detected amplitude).
00:02:20 – Although the historical devices used solely sinusoidal wave for the modulation, the square wave can also be used. The difference between modulation of the carrier wave with the sine and square wave is visible on the signal modulation envelope.
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