Charles Coulomb came very close to discovering the electromagnetic (strong) charge:

I wished to use the same method to determine the attractive force between two balls charged with a different nature of electricity but by using this same balance to measure the attractive force, I found an experimental difficulty that did not occur when measuring the repulsive force.  The experimental difficulty arises when the two balls are drawn near to each other.  The attractive force which increases, as we have clearly seen, according to the inverse square law of distances, frequently increases at a greater rate than the torsional force, which increases only directly as the angle of twist…[1]

Had Coulomb considered that there are two different types of charge, he would have noticed that the second charge is electromagnetic in nature (as opposed to the electrostatic charge).  In addition, he would have been able to express the force law for this other type of charge in terms of a modified inverse square law of distances (as done in the Aether Physics Model).

As it is, modern physics recognizes only one type of charge, and consequently the strong force poorly describes in terms of particles called gluons[2].

Before quantifying strong charge, we note that the conductance of the Aether derives from Coulomb’s constant and its relationship to the other known constants of the “vacuum”:

$$Cd = \frac{{{k_C} \cdot {\varepsilon _0}}}{{c \cdot {\mu _0}}}$$

$$Cd = 2.112 \times {10^{ - 4}}\frac{{se{c^2} \cdot cou{l^2}}}{{kg \cdot {m^2}}}$$

Scant literature exists describing the conductance of Aether (vacuum, free space, quantum foam) in modern physics.  Conductance is the “measure of a material's ability to conduct electric charge.”[3] Electrons do “conduct” through the Aether, as observed when electrons travel in the space between the Sun and Earth.  Electrons also pass through Aether in a vacuum tube.  The conductance constant is a specific measure of the Aether’s ability to conduct strong charge.

Planck’s constant is equal to[4]:

$$h = 6.626 \times {10^{ - 34}}\frac{{kg \cdot {m^2}}}{{sec}}$$

Planck’s constant generally defines in modern physics as “The constant of proportionality relating the energy of a photon to the frequency of that photon.”[5] The Standard Model has missed the fact that Planck’s constant is actually the quantification of the electron.

Strong charge then calculates as:

$$h \cdot Cd = {e_{emax}}^2$$

$${e_{emax}}^2 = 1.400 \times {10^{ - 37}}cou{l^2}$$

where e_emax² is the strong charge.  The strong charge, like the electrostatic charge, is distributed.

Unlike electrostatic charge, each onn has a strong charge value proportional to its mass.  This is because the strong charge is dependent on the angular momentum of the onn, and the Aether length and frequency dimensions are quantum measurements.  Strong charge notates as e_emax² for the electron, e_pmax² for the proton, and e_nmax² for the neutron.

[1] Coulomb, Charles Augustin Institut de France, Mémoires de l’ Académie des Sciences (1785) 569ff, 578ff [as published in Shamos, Morris H. Great Experiments in Physics; Firsthand Accounts from Galileo to Einstein (New York, Dover Publications, Inc., 1987) 65]

[2] Gluon, an elementary particle that mediates, or carries, the strong, or nuclear, force. In quantum chromodynamics (QCD), the quantum field theory of strong interactions, the interaction of quarks (to form protons, neutrons, and other elementary particles) is described in terms of gluons—so called because they “glue” the quarks together. Gluons are massless, travel at the speed of light, and possess a property called color. The Columbia Electronic Encyclopedia, Sixth Edition Copyright © 2003

[3] The American Heritage® Dictionary of the English Language, Fourth Edition Copyright © 2003 by Houghton Mifflin Company.

[4] The NIST Reference on Constants, Units, and Uncertainty http://physics.nist.gov/cgi-bin/cuu/Value?h|search_for=planck+constant

[5] The American Heritage® Stedman's Medical Dictionary Copyright © 2002, 2001, 1995 by Houghton Mifflin Company.