3. Shape and sizes of particles
The resulting expression
binds the radius of a particle and its radius of inertia. It allows us to understand the shape of charged elementary particles.
For example, for an electron
r =
ri·1.00115965, i.e. the radius of an electron is only
slightly more than its radius of inertia. Consequently, an electron is a ring (torus) having a very small cross section, i.e. is approximately the closed vortex filament. Namely
for this reason the researchers
cannot determine the size of an electron in experiments and mistakenly consider it as a point [
15]. But we can calculate its size.
If an electron to consider as a closed filament or a
material circumference (a ring, the cross section of which in thise conditions can be neglected), then we can assume that the electron charge moves with velocity
υr along the circular orbit of radius
r and creates the orbital magnetic moment μ
e , according to equation (4):
The orbital speed
cannot exceed the speed of light, i.e.
υr ≤
c. So
On the other hand, according to equation (9), the spin magnetic moment of an electron
where
υe is the linear speed of electron rotation.
Comparing equations (13) and (14) we obtain:
Hence, the linear speed of electron rotation cannot exceed half the speed of light, i.e. υe is less than or equal to c/2: υe ≤ c/2.
Therefore, the electron’s radius of inertia
ri cannot be less than the reduced Compton wavelength of an electron ƛ
е , i.e.
ri is greater than or equal to ƛ
е ,
ri ≥ ƛ
e , because
where
S =
ћ/2 is spin of an electron.
The reduced Compton wavelength ƛ is natural representation for mass on the quantum scale, and as such, it appears in many of the fundamental equations of quantum mechanics.
Thus, we conclude that an electron (
me = 0.9109×10
–30 kg) has the linear velocity of rotation equal to half the speed of light,
υe =
c/2, and its radius of inertia equal to the reduced Compton wavelength,
ri = ƛ
e = 3.86159×10
−13 m [
13].
Knowing the values of the radius of inertia and linear velocity, we find the integral time of rotation (revolution) of the electron
ti (the characteristic time of processes occurring due to electromagnetic forces):
Since the electron has a circular cross-section, the circumference of inertia of an electron passes exactly through its center of section. Therefore, an electron has:
internal radius rin = ri /ne = ri /1.00115965 = 3.8571×10−13 m,
radius of section rs = ri – rin = 0.00449×10−13 m = 4.49×10−16 m,
external radius r = ri ne = ri·1.00115965 = ri + rs = 3.86606×10−13 m.
Hence follows the relatively large magnetic moment of an electron (in the SI units):
Here we will touch upon the issue of different systems of measurement.
It must be recalled that the International System of Units (SI) and the cm–g–s system of units (CGS) are variants of the metric system of physical units.
The SI system is a composite system: it includes, in particular, the MKS system for measuring mechanical quantities and the MKSA system for measuring electromagnetic quantities. The latter subsystem differs from the former primarily in that, along with the existing three basic units (meter, kilogram, second), it has a fourth basic unit – the ampere (A).
It should also be recalled that in addition to the CGS system for measuring mechanical quantities, there are various systems for measuring electromagnetic quantities that use centimeter, gram, second as basic units: absolute electrostatic system (CGSE), absolute electromagnetic system (CGSM), Gaussian system of units ( type of unification of SGSE and CGSM).
In mechanics, the SI (MKS) system and the CGS system are built in an identical way, and the laws of mechanics do not depend on the choice of units of measurement. However, this is not the case in electrodynamics. This is because there is no one-to-one correspondence between the electromagnetic units in the SI (MKSA) and the same units in the CGSE, CGSM and Gaussian system, as is the case for mechanical units. Therefore, it is necessary to clearly separate the CGS system itself from the CGSE, CGSM and Gaussian systems.
In 2018, we showed that the electromagnetic units of the MKSA system (ampere, coulomb, ohm, volt, etc.) can be expressed using the base units of the MKS and CGS systems [
16].
For example, in the MKS and CGS units, the ampere has the dimension of
force, namely,
Therefore, in units of the MKS and CGS systems the magnetic moment of an electron
A stated argumentation concerning the electron is fully applicable to a muon (its mass
mμ = 1.8835×10
−28 kg), because its spin
S =
ћ/2, and the coefficient
nμ = 1.00116592 [
13]. Therefore, like an electron, a muon is a thin ring (torus), that has the following parameters:
linear speed of rotation υμ = c/2,
radius of inertia
ri =
ћ/
mμc = ƛ
μ = 1.867594×10
−15 m [
13],
internal radius rin = ri /nμ = ri /1.0011659 = 1.8654×10−15 m,
radius of section rs = ri – rin = 0.002194×10−15 m = 2.194×10−18 m,
external radius r = ri nμ = ri·1.0011659 = ri + rs = 1.86977×10−15 m.
Integral time of rotation (revolution) of the muon
The mean lifetime of muon τ = 2.2×10
–6 s [
13], during this time it makes
The muon magnetic moment, in the MKSA units,
or, in the MKS and CGS units,
With regard to a proton, from the experience are known its mass
mp = 1.6726×10
−27 kg, spin
S = ћ/2, and spin magnetic moment μ
p = 1.4106×10
−26 A m
2. However, the radius of the proton remains a puzzle to this day. Measurements show that the root mean square charge radius of a proton
r is about 0.83÷0.87 fm (1 fm = 10
−15 m) [
13].
From equation (9) we find a linear speed of proton rotation
υp:
Thus, the linear speed of proton rotation is approximately about 3 times less then the speed of light. The proton radius of inertia
Obviously that the proton’s circumference of inertia is located closer to the axis, as ri < (r – ri) = 0.53÷0.57 fm. Therefore, unlike an electron and muon, the cross-section of a proton is not a circle, i.e. the proton has the shape of a toroid.
As we noted, modern theoretical physics considers the electron to be a point particle. This delusion leads to the problem of infinite values (divergences) obtained in the theory of elementary particles. A point-like electron at rest must have infinite self-energy and, consequently, infinite mass. The meaninglessness of this result clearly confirms that the electron is not a point particle; in fact, as we have shown, it has a well-defined size.
Scientists call the value Rg = Gm/c2 or Rg = GρV/c2 (where G is the gravitational constant, ρ is the density of the body, V is its volume) the "gravitational radius" of a physical body; this quantity is always many times smaller than the size R of the body, Rg<< R.
For example:
mass of the Earth m = 5.97×1024 kg, its radius R ≈ 6370 km, value Rg = 4.43 mm;
mass of the Moon m = 7.34×1022 kg, its radius R ≈ 1737 km, value Rg = 0.054 mm.
In 1935, the Soviet physicist M. Bronstein rightly noted that in the quantum theory of the gravitational field «
the gravitational radius of the test body used for the measurement (
GρV/c2)
cannot be larger than its actual linear dimensions (
V1/3)
…», however, he was mistaken in asserting that «
In electrodynamics there is no analogy to this fact…» [
17].
In fact, there is the value r0 = ke2/mc2 which scientists call the "classical radius" of a charged elementary particle; this quantity is always much smaller than the radius r of the particle, r0 < r.
For example, for an electron r0 = ke2/mec2 = 2.81×10−15 м, r = 3.866×10−13 м;
for a muon r0 = ke2/mμc2 = 1.36×10−17 м, r = 1.869×10−15 м;
for a proton r0 = ke2/mpc2 = 1.53×10−18 м, r = (0.83÷0.87)×10−15 м.
Thus, the sizes of the electron and muon are determined correctly.
Modern physics cannot explain why the electron’s magnetic moment is slightly larger than the
Bohr magneton μ
B =
eћ/2
me , and the proton’s magnetic moment is much larger than the
nuclear magneton μ
N =
eћ/2
mp:
This discrepancy between the experimentally observed and assumed (according to the Dirac equation) values of the magnetic moment is considered an anomaly.
However, it must be so, because spin
S = mυri , magnetic moment μ
= eυr =
eυri·
n, and
Thus, in reality, there is no anomaly in the magnetic moment of the electron, muon, proton and other particles.