Ciao
In the old valve and loved the secret to capturing the radiant energy?
Seems so ... the potential barrier allows the drive unidirectional
absolute privilege for creating the event radiant.
Some characteristics of vacuum tubes and the plasma is created between the electrodes,
the path outlined by Tesla Moray Gray and access to the sea of energy.
http://www.nuenergy.org/alt/valve.htmmore ...
Tesla still confirmations ...
Paulo Correa & Alexandra: PAGD (Pulsed Abnormal Glow Discharges)
EMISSIONS FROM POWER AUTOELECTRONIC
Pulsatory Spontaneous activity of the space medium in cold cathode diodes.
Moray and Reich discovered spontaneous pulse activity in
valves catoto cold.
Sustainable producing pulses in a vacuum tube to catoto cold, the conversion system supports alone, the electricity produced is far beyond the input supply. Reported overall performance efficiency of 483%. The pulses occur at a frequency controlled without the need for an external pulse.
Labofex Press Release: "Canadian Breakthrough in Power Generation..."
Arthur Axelrad: "PAGD, Aether Motors, and Free Energy"
Paulo & Alexandra Correa: "Power from Autoelectronic Emissions"
P. & A. Correa:US Patent # 5,416,391 ~ "Electromechanical Transduction of Plasma Pulses"
P. & A. Correa:US Patent # 5,449,989 ~ "Energy Conversion System"
P. & A. Correa:US Patent # 5,502,354 ~ "Direct Current Energized Pulse Generator Utilizing Autogenous Cyclical Pulsed Abnormal Glow Discharges"
http://www.rexresearch.com/correa/correa.htm#5449989bstract of US5502354
A cold cathode vacuum discharge tube is used in a circuit for generating pulsed autoelectronic emissions which are particularly intense and frequent in the abnormal glow discharge region, and involve much lower current densities than predicted by the Fowler-Nordheim vacuum arc discharge region law. The discharge tube is characterized by a large electrode area at least of the cathode, and a large interelectrode gap. The electrodes are preferably spaced at least 2 cm apart in a parallel relationship. A probe may be introduced between the electrodes to reduce still further the field required to generate the emissions. In another configuration the probe forms the anode and two plates form cathodes. The circuit is driven from a direct current source of having an impedance sufficient to prevent establishment of a vacuum arc discharge.
These pulse generators have diverse industrial applications; directly, they may be used as stroboscopic light sources, for vacuum deposition of cathode materials or cathode coatings (eg. polymer deposition or aluminum mirroring of target surfaces), detection of ionizing radiation fields, or electrostatic and electromagnetic proximity fields, high power noise-signal generation, destructive component testing (transient response) or destructive testing of materials in vacua (eg. insulations), high frequency medium voltage power supply applications (switching supplies and inverters), as an oscillator or as part of a pulse forming network. Indirectly, they may be used for laser pulsing, flash tube pulsing or for research (eg. chemical reaction triggering) and industrial switching applications.
Two conclusions, independently from all other varying conditions, may be taken from the data of Table 14: the pulse energy released within the reactor varies from <3 to >50.times. the input energy per pulse (column A vs columns B and C); and, in general, the reactor energy varies inversely to the pulse frequency (columns B and C, vs column D). In other experiments, reactor energies per pulse have been observed to reach >500 J. Given that the reactor pulse voltage (Vp) is determined by the extinction voltage Vx (Vp=Vb-Vx) and thus cannot reach the amplitude of the breakdown voltage Vb, this involution of energy observed per pulse in the reactor and at its output indicates that it is a current amplification phenomenon. Indeed, with input currents of 1.2 to 1.7 A and input pulse energies of 1 to 30 J, peak pulse reactor currents have been observed to reach >150 A.
Typically, a H34 device can produce about 0.25 kWh per 10,000 pulses. The corresponding value for a PLT is thus a minimum of 1.0 MWh/Alzak cathode and of 20 MWh/H34 cathode. As the cathode for each combination is only 66.7% consumed, the vacuum pulse generator may continue to be used in a reverse configuration, by utilizing the other plate in turn as the cathode; thus, the minimal values become, respectively, 2.0 MWh/Alzak pulse generator and 40 MWh/H34 pulse generator. The same rationale applies if the configuration utilized was that of the double diode.
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Topic: Correa's pulsed abnormal glow discharge tube (Read 87130 times)
