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where
= “shift” in the bond energy (change in the bond energy),
d
= inter nuclear
distances, Ʉ = constant characterizing the element (approximately equal to the elec-
trostatic interaction between the skeleton and valence electrons in a free atom),
Δ
W
q
=
effective transferred charge. As applicable to the binary bond, we have:
2
%%
Wd
P
1
K q
(8)
ii
Equation (8) is similar to Equation (6), but the calculations in it are made for initial
(primary) Ɋ-parameters
q
2
and
Wd
.
Considering the electric charge transfer as the electric current generating the mag-
netic ¿ eld under vacuum with magnetic constant
μ
, we can assume by analogy with
Equation (8), that it is more an elementary processes:
0
2
2
1
L
q
k
N
0
then
2
e
P N
,
where k = proportionality coefficient.
The calculations revealed that in these cases the simple correlation for the mag-
netic constant is ful¿ lled:
0
1
l l
(9)
2
2
2
2
2
(2
QN
)
3
Pc
4
Q N
3
Pc
k
N
P
2
c
0
e
0
e
0
e
2
π
where
k
, number 3 is apparently determined by the number of electrons interact-
ing with three quarks or three protons. Transfer coefficient from MeVfm
into Jm:
6
=
3
¸ ¸ ¸ ¸
Jm.
Then:
19
15
28
10
1.602 10
10
1.602 10
28
¸
Jm.
28
P
1.43995 1.602 10
¸ ¸
2.3068 10
Gn
m
μ
Calculation of
by Equation (9) gives
The relative error in
6
N
¸
1.2554 10
.
0
0
μ
comparison with the actual value of
is below 0.1%. Value
k
gets the dimension-
ality Jm
3
/
Gn
2
, where the numerator characterizes the volume values of Ɋ-parameter.
As
P
e
~ e
2
, then the dimensionality [
P
e
1/2
c
] gives the physical sense of magnetic
constant as the current element for the elementary charge: [Ⱥm].
The known correlation between three fundamental constants of electromagnetic
interactions can be represented as follows:
0
N
ñ
1/
F
c
0
0
ε
where
= electric constant.
Using this dependence together with Equation (9), and after the relevant calcula-
tions we can obtain the equation Ɋ-parameter bond with constants of electromagnetic
interactions:
0
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