ON THE ELECTRODYNAMICS
OF
SPONTANEOUS
NON-EXISTENCE
Zefferon
PART 2 – MATTER-ANTIMATTER REACTORS AND SPACE TRAVEL
A matter-antimatter reactor is a coincident-beam mixer. In M-A reactors, beams of particles and anti-particles which have been accelerated to relativistic speeds in the same direction are mixed together with coherent radiation and focused with magnetism to create a series of phased annihilations to form a “bubble” in space-time which is an ANNIHILATION-VACUOLE. It is the Annihilation-vacuole, or a-vacuole, which is the sustained relativistic phenomena inside the m-a reactor which the reactor controls the size and shape of to produce energy for utilities or to macroscopically distort space-time to produce artificial gravity or to cause spacecraft to move.
There are two main types of m-a reactors, the cyclotron-synchrotron and the canon reactor. Both types of reactors form a-vacuoles, the cyclotron-synchrotron forms a ring-shaped a-vacuole, and the canon reactor forms a linear, cylindrical a-vacuole. They require pumps for high vacuum when operated in an atmosphere, and little or no vacuum pumps when operated in open space. Either one works well for generating power. When used for space-time distortion, hereafter referred to as GRAVIMETRICS, the cyclotron-synchrotron is well suited for forming artificial gravity environments and low-power spacecraft movement (attitude control), whereas the canon reactor is especially useful for forming extremely concentrated a-vacuoles in a straight line for high-power tractor applications and primary spacecraft movement at high, even relativistic, speeds. Both types of reactors can use “fuel” sources of from elementary particles to atoms. The cyclotron-synchrotron is restricted in its use of heavier particles because of the problem of containing the particles as they circulate in a circle. The canon reactor, on the other hand, is well suited to continuous operation using heavy particles because it only has to keep them packed in a straight line. The canon reactor is typically used for much higher power output.
In each type of m-a reactor, the phasing of the a-vacuole is controlled to maximize output of energy or space-time distortion. When producing energy, the a-vacuole is kept just above its forming threshold to help focus the particle beams. When used for gravimetrics, the a-vacuole is maximized for space-time distortion with very little loss to radiation and waste particles (debris).
The most powerful of the m-a reactors is the heavy-nuclei canon reactor, which can continuosly mix heavy particles such as uranium and anti-uranium ions, for sustained power outputs well into the hundreds of terawatts. Heavy-nuclei canon reactors, when operated in hard vacuum (open space), can extend their a-vacuoles beyond the edges of the reactor itself, providing a tremendous gravimetric distortion for pulling a spacecraft to relativistic speeds.