3.4. Radius of force reach of particles, calculation of velocities, frequencies, and mass of particles, "mass defect" notion |
The electron radius can be determined provided the whole electron mass me has electromagnetic nature, i.e. potential energy Wp is determined by charge e distributed on the surface of a ball of the radius of re, see [7]. In contemporary physics for the electric potential energy on the surface of the ball the following equation is valid (see [8])
Fig. 3.10. The dependence of Tkin on Wcurr
Fig. 3.11. The dependence of Tkin on , W on and Tc on
(3.23) |
(3.24) |
(3.25) |
Analogically for proton
(3.26) |
Similarly for quark, prequark, or - particle we get
(3.27) |
Table 6 of the dependence of or respectively d on
and
gives possible radii and diameters of subparticles, and particles, calculated according to the equation (3.27)
for speeds from the interval 10-11c trough c and the value .
Table 6.
v/c | dp [fm] | ||
10-11 10-10 10-9 10-8 10-7 10-6 10-4 10-3 |
3.06.1019 3.06.1017 3.06.1015 3.06.1013 3.06.1011 3.06.109 6.12.105 6.12.103 | ||
0.03 0.04 0.06 0.07 |
3.0719 1.66934 0.6917 0.49045 |
3.75224 2.1798 1.0324 0.78267 |
6.824 3.8491 1.7241 1.27312 |
0.1 | 0.6361 | ||
0.11 0.19 |
0.1716 0.0421 |
0.35832 0.1516 |
0.5299 0.1937 |
0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1 |
0.17719 0.09223 0.06261 0.04895 0.04165 0.0373 0.03458 0.0328 0.03168 |
(3.28) |
Fig. 3.12. The diameter of the particle di
Fig. 3.13 gives the dependence of di on while the "comb" ...is shown for one of the possible values of the relation of the particle and subparticle diameters:
Fig. 3.13. The dependence of di on
p | k | pk | ||
d | 4.1262 fm | 1.5103 fm | 0.552 fm | 0.2023 fm |
v | 0.04c | 0.065c | 0.11c | 0.19c |
dcircle | 7.149 fm | 2.6168 fm | 0.958 fm | 0.35 fm |
Vedge | 5.34.1020 Hz | 2.37.1021 Hz | 1.1.1022 Hz | 4.91.1022 Hz |
7360me | 1840me | 460me | 115me |
For the sake of simplicity we shall assume the closest possible arrangement of particles with less mass in the ones with more mass i.e. - particle is formed by four nucleons forming the disfenoid, a proton (nucleon) is formed by four quarks forming the disfenoid, a quark is formed by four prequarks forming the disfenoid. Table 7 gives the mass, frequency, diameter estimations of force reach according to 3.27, speed estimations of relevant particles existing one in the other, i.e. of prequarks in quarks, quarks in proton (nucleon), nucleons in - particle. More coherent and detailed evaluations and computations will be given in some future article.
The notion of "mass defect" (energetic defect) loses its sense, if we consider that the particles in the nucleus are compressed under high pressure into almost ball-like formations. That is the case of revolvement of subparticles around approximatelly circular path (the edges of the series), and vice versa. Free particles are characterized by low pressure, i.e. by the ellipticallity of the particles paths (ever more of spectral lines including the series heads).
From Table 6 we can find such speeds of circulation of subparticles which enable
that 4 subparticles (forming the disfenoid) to be situated in the particle at the same time, i.e. they are
smaller than the particles:
4 nucleons in - particle
4 quarks in a proton
4 prequarks in a quark
Naturally, the subparticles must have higher speeds of circulation (i.e. and energy). The energy of a particle is smaller than the sum of energies of the corresponding subparticles:
a) the energy of the - particle is smaller than the sum total of the energies of 4 nucleons forming the - particle
b) the proton energy is smaller than the sum of energies of four quarks forming the proton
c) the quark energy is smaller than the sum of the energies of four prequarks forming the quark.
According to (3.11) and Table 7 for - particle:
for 4 protons:
for 4 x 4 quarks:
for 4 x 4 x 4 prequarks:
see tab.8.
p | k | pk | |
v=0.04c | v=0.065c | v=0.11c | v=0.19c |
[]ad=0.0007 | < 0.0019 | < 0.0053 | < 0.014 |
[]id=0.0008 | < 0.0023 | < 0.0071 | < 0.024 |
< 0.0042 | < 0.0124 | < 0.038 |
, ,