Introduction to particle theory: the measurement of the magnetic field of relativistic electrons and its implications in relation to general relativity

In an attempt to bridge the gap between quantum mechanics and general relativity, Particle Theory is a theory that may try to address this problem. The theory states that indivisible particles of non-zero mass, are instead divided into even smaller particles called EM (electromagnetic) particles. These EM particles collide and are held within a center potential, the speed of light being the limit to their velocities. Some particles that escape from this potential, through 'shedding', are responsible for the static and magnetic fields we observe. This also creates a 'screening' effect that, for an atomic particle at rest, blocks a good portion (half) of what this theory claims is the true gravitational potential, which is just twice the Newtonian value. When such a system of particles starts moving in one direction, the act of shedding begins to decrease as the EM particles orient themselves in the direction of the velocity, which reduces the electromagnetic field emitted as well as the screening effect in which we would start to observe the relativistic effects of Special and General Relativity. To test this, an experiment was conducted by measuring the magnetic field of an increasing velocity of relativistic electrons recorded at fixed intervals up to a maximum average velocity of up to sixteen percent the speed of light. The results showed the magnetic field of the beam of electrons diverging negatively from a linear pattern with an average second derivative of the plot being −0.02±0.002 microteslas per volts, compared to that of the magnetic field plot of the wire (non-relativistic) being 0.002±0.002 microteslas per volts. As a result, a possible application that this theory uniquely infers is the possibility of increasing the screening effect through emissions of high energy photons consequently reducing the gravitational pull of an object emitting such a field. (author)