I MUST DO MY DUTY
(continue)
I.G. Goriacvhko, St. Petersburg, in March, 08.
Quantified body’s motions are
realized in Universe in varity thermodynamical conditions (p, T) and
accompanied by the variable also quantified electromagnetic and
gravity fields forming the general ether.
But these fields may be arisen only at the expense of changed their
charges
and masses.
The harmony of Nature needs in the unity of its mathematical
description as in
mechanicsas
in thermodynamics which
practicable by the full
differential‘s
mathematical method (which successfully is used in thermodynamics).
Because that the full system of the quantum mechanics laws must be
described as it shown at the left side of table 1. Laws (a), (b) is
obtained by means the next vectors equations: for the impulse ,
for the moment of impulse
From the right side for comparing is given the full system of
Newton's mechanics laws.
5. Quantum mechanics
Table 1 Quantum mechanics laws | Newton’s mechanics laws |
where |
where |
where |
where |
|
|
In Newton’s laws (a’),
(b’) parameteris
absent (i.e.
).
Because of that these laws are incorrectly
as of physical as
of mathematical standpoints. On the physical
point of view all
the parameters (
)
for the circle
(
)
body’s motion – are constancy.
Therefore,
(i.e. the doubt).
On the mathematical
point of view these laws (excepting
(N)) – are
not the full
differentials. But
all
the laws ( a),( b ),(c) –are the full
differentials.
The explanation 3. The impulse
Because of that must be describing
,
where
– the integrating
factor. Therefore,
The verification.
Let us takes up the planet’s motion around the Sun. By means of
(1) and Newton law (assume
that the Sun immovable) we obtain
Therefore,
on the one side
–
the centripetal
force. But on the other side
the centrifugal
force. Because this
From
(a), (b) for the two
bodies interaction may be received as all
the well known
mechanic’s laws:
,
as the unknownquantum
mechanic’s laws:
If
we obtain the Third Newton’s law
and
-(i.e. the well known equilibrium
conditions of a
body). And etc.
6. The quantum corpuscular-wave theory
It is considered that modern corpuscular-wave theory applicable to any types of particles (i.e., to the changed and neutral ones). By means of (1) and (B’) they may be obtained the adjusted (i.e. the quantum) laws of the corpuscular-wave theory (see the left side of the table 2. On the right side for comparing is given the ruling redaction of this theory).
Table 2 The quantum corpuscular- wave theory | The modern corpuscular- wave theory |
The kinetic energy | ----------------------------------------------------------------- |
The potential energy | ----------------------------------------------------------------- |
The equation | The equation |
The impulse | The impulse |
The full energy | The full energy ( !) |
Here
Plank’s constancy,
the
angular frequency,
the
wave date,
the
wavelength,
the
wave’s velocity,
the
particle’s mass,
the
unit vector. With regard to the parameter
in all of these laws see P. 3.
It must be especially notes that all the laws of the tables 1 and 2 are carried up at a time. But the role of the major law belongs to the quantum law of conservation the full energy.
Thank you. To the next report in April, 12. G.I.G.
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