The strong force law is unknown to modern physics.  According to the Standard Model, the strong force is “In physics, the force that holds particles together in the atomic nucleus and the force that holds quarks together in elementary particles.”[1] There is no practical equation for calculating the strong force in the Standard Model because there is no practical strong force carrier.

However, the strong force carrier in the Aether Physics Model is the electromagnetic charge, or strong charge.  The strong charge quantifies as the angular momentum of the onn times the conductance of the Aether.  Thus, the strong charge of the proton is equal to:

$${e_{pmax}}^2 = {h_p} \cdot Cd$$

The strong force of the proton calculates using the strong force law, which is similar to that of the electrostatic force law and the gravitational law.  As in the case of the electrostatic law, the product of two strong charges calculates from a single dimension of each charge.  Since the binding force causes the protons and neutrons to have large “small radii” and small “large radii,” the onta appear spherical.  Thus, the Coulomb constant instead of the Aether unit constant is the force mediator.

$${k_C}\frac{{{e_{pmax}} \cdot {e_{pmax}}}}{{{L^2}}} = F$$

The strong force of the neutron is similarly calculated:

$${k_C}\frac{{{e_{nmax}} \cdot {e_{nmax}}}}{{{L^2}}} = F$$

The strong force law for free protons and free neutrons would probably integrate the Aether unit constant with the Coulomb constant.  This is because free protons and free neutrons are more toroidal in shape.  However, once they bind, their shape becomes spherical.

Since the Aether is always acting upon strong charge, whether or not there is another onn present, the strong force per onn is actually the strong force of a single onn.  In other words, the Aether is acting on onta to produce force even when there is no other onn around to interact with the force.  This must be so since the onta have no proximity system that can sense when another onn is nearby, and then react to it.

The total nuclear binding force is the sum of all force acting upon onta in an atomic nucleus.  The total force acting upon a single neutron at one quantum length, even though there are no other neutrons or protons nearby, is:

$${A_u}\frac{{{e_{nmax}}^2}}{{{\lambda _C}^2}} = 1.839 \times {10^3}forc$$

The total strong force for an atomic nucleus of deuterium, however, is:

$${k_C}\frac{{{e_{pmax}}^2}}{{{\lambda _C}^2}} + {k_C}\frac{{{e_{nmax}}^2}}{{{\lambda _C}^2}} = 3675forc = 124newton$$

Coulomb’s constant appears in the above equation due to the spherical structure of the resulting nucleus.  The nuclear strong force equation then expresses as:

$${k_C}\frac{{Z \cdot {e_{pmax}}^2 + N \cdot {e_{nmax}}^2}}{{{\lambda _C}^2}} = F$$

where Z is the number of protons and N is the number of neutrons in the nucleus.  The nuclear strong force equation quantifies nuclear binding force.  We can modify the above equation to produce a nuclear binding energy equation, which predicts the nuclear binding energy for all isotopes.  (page 236)

As shown in the section on particle radii, the free proton has a very small “small radius” and a very large “large radius.”  Thus, a single hydrogen atom is both very thin and very wide.  However, as soon as protons and neutrons bind, the strong charge causes the onta to contract.  The large radius becomes much smaller and the small radius becomes much larger.  This causes the geometry of the strong charge to change from toroidal to spherical in geometry.

The two onta adjoining each other tend to squash into a single sphere as in the graphic of the deuterium atom below.

Nuclear Highlights, Jefferson Labs[2]

As long as the total surface area of the onn remains exactly one quantum length squared, the onn can assume any shape without violating conservation of angular momentum, mass, energy or any other perceived conservation law.

When onta are relatively far apart, the Coulomb electrostatic constant mediates the spherical geometry charge.  When protons and neutrons are contacting, Coulomb’s constant still mediates spherical geometry charge.  The change of shape from toroidal to spherical does not appear to occur to bound electrons within atoms, which have a mass of about 1836 times less than a proton or neutron.

[1] The New Dictionary of Cultural Literacy, Third Edition Edited by E.D. Hirsch, Jr., Joseph F. Kett, and James Trefil. Copyright © 2002 by Houghton Mifflin Company.

[2] Intrinsic Shape of the Deuteron, Jefferson Labs (Nuclear Highlights) http://www.jlab.org/highlights/nuclear/Nuclear.html