| Title Page | Table of Contents | Preface | <<<< | >>>> | Appendixes | References | To Order This Book | WritWord Homepage |
A single unit-conversion factor links the magnitudes of the quantum attributes of a particular elementary particle to those of another elementary particle. The direction of conversion depends upon the dimension, as follows:
| Dimension | Less to More Massive | More to Less Massive |
| Mass | Multiply | Divide |
| Temperature | Multiply | Divide |
| Charge | no conversion | no conversion |
| Length | Divide | Multiply |
| Time | Divide | Multiply |
Before we establish the quantum attributes of the masson, we study the relationships between the already-known attributes of two other elementary particles--the electron and the proton. To do so, we use the electron-to-proton quantum-attribute conversion factor, δ, which is equal to about 1836.
We convert the electronic attributes, me, ke, λe, and te, respectively, into the protonic attributes, mp, kp, λp, and tp, as follows:
mp = δ me = 1.7 × 10-27 kg (76
kp = δ ke = 1.1 × 1013 K (77
λp = δ-1 λe = 1.3 × 10-15 m (78
tp = δ-1 te = 4.4 × 10-24 s (79
Upon examining the above table, we see that the proton is 1,836 times more massive than the electron, yet it makes light-speed quantum jumps like the electron. However, because of the proton's greater mass, each quantum jump covers less distance by the same factor of 1,836 and takes less time doing so--again by that same factor of 1,836 (see Table VI in Appendix E).
By extrapolation from the above example, we convert the electronic attributes, me, ke, λe, and te, respectively, to the massonic attributes, mg, kg, λg, and tg, by using the electron-to-masson quantum-attribute conversion factor, (θ = 2.0 × 1021), (see Equation 74), as follows:
mg = θ me = 1.9 × 10-9 kg (80
kg = θ ke = 1.2 × 1031 K (81
λg = θ-1 λe = 1.2 × 10-33 m (82
tg = θ-1 te = 4.0 × 10-42 s (83
These SI values of the masson's quantum attributes are also the already-established Planck values, which are listed in other books, but they differ from the above values by the factors 2π and the square root of β (see Table VIII in Appendix E). This is because the gravitational constant, G, contains both of these factors and its entire empirical value was used to formulate the historical definitions of the Planck values. The correct magnitudes for the Planck values are the quantum attributes of the masson as established by the electromagnetic-to-gravitational force ratio, θ2.
We use the quantum attributes of the masson to establish a Système Gravitatif (SG) of unit measures, which, when used in the Bekenstein and Hawking equation for the entropy of a Black Hole, a gravitational phenomenon, its multitude of FUPCONs vanish (see Chapter 18).
The mass and threshold temperature of the masson are humongous (by a factor of 1021) when compared to those of the electron and even to those of the proton. Conversely, the length of and time for its light-speed quantum jumps are infinitesimal (by a factor of 10-21) in comparison to that of "low-mass" elementary particles. Thus, we see that, going from the electron, to the proton, and on to the masson, the magnitudes of these two pairs of attributes diverge by the same factor.
This seems to resemble a particle that accelerates toward lightspeed, where its mass increases, but time and distance are compressed. Fantastic as it might seem, an electron, proton, and masson appear to be the same particle at different, specific near-lightspeed velocities.
Can extrapolation of this proportionality rule of determining the attributes of other elementary particles be extended to those contained within atomic nuclei?
| Title Page | Table of Contents | Preface | <<<< | >>>> | Appendixes | References | To Order This Book | WritWord Homepage |