The Strong Nuclear Force

Given the notion that the electromagnetic field in all its forms comprise the totality of the universe, as described here we can find the strong nuclear interaction within that concept. To start, consider the construct of the elementary particles as phase-locked patterns of looping photons. The most simple of the particles is the electron. We can start with that and show how a strong force develops that is ten times stronger than that assumed for the electromagnetic force.

The static electric charge of an electron radiates outward from the surface of the closed pattern that comprises the electron. This pattern is formed by a lone photon trapped
Shell mass and sizes developed by the Square of the Shells rule. The strength of the electric charge in units of electron force is the same as the mass in units of electron mass.
in an electromagnetic cavity produced by its own bent path. The strength of the charge is greatest at the surface of the sphere and diminishes as the square of distance away from the surface.

Any photon in a resonant cavity radiates this static charge. The measure of the strength of the charge is a constant because the electromagnetic saturation amplitude of photons is a constant. The circumference of the electron is determined by the wavelength of the photon that comprises it. Since the charge amplitude diminishes as the square of distance, the charge amplitude is at its maximum value at the electron's surface.

Since the photon completes one turn around the circumference in one wave length, the same half cycle polarity is toward the outside of the turn all the way around. In
The same polarity of the electric field is toward the outside all the way around the circumference. This is because the field polarity reversal is governed by the same sine function that creates a circle.
the case of the electron it is the negative electric field that is toward the outside all the way around. The positive field is on the inside of the shell.

We can consider the static electric force at the electron's surface as one unit. We know that the strong nuclear force would then be about ten units. We will show how to find the strong nuclear force within the stronger forces that must occur at the surface of smaller diameter surfaces.

We can calculate the strength of the force at the proton's surface with a simple square-of-the-shells rule using the neutron's outer shell as a starting point. This charge strength is directly related to the massiveness of the shells because the more massive the shell, the smaller its radius and the smaller its radius the greater the surface charge.

Starting with the neutron's outer shell, it is 2.5499 electrons more massive than a proton. The proton's outer shell is 6.5 and the proton's next shell in is 42.2 all in units of electron surface charge. These three shells provide the strong nuclear force and the weak nuclear force.

Proton-Proton bond When two protons are forced together so that shells 2 and shells 3 of each merging proton touch those of the other there are four points where they touch. The square root of the sum of the forces of the touching shells is the strong nuclear force. It turns out to be just slightly less than ten. Neutron-Proton bond

To see how this develops consider the electrostatic forces of shells two and three. Proton Image In the proton-proton bond there are two places where the shells overlap and the positive charge of one shell is in contact with the negative shell of the other. One proton's outer shell 2 is in contact with the other proton's shell 3. So we have shell 2 plus shell 3 plus shell 2 plus shell 3 forces. This is 6.5 + 42.2 + 6.5 + 42.2. When we extend the decimal and sum this we have 97.558 electron forces. The square root of that comes to 9.88.

We have found the strong nuclear force but this is just an approximation. There are many dynamics involved that are not considered here. They would all come into play in the evolution of a final theory.