I MUST DO MY DUTY
(continue)
I.G. Goriachko, St. Petersburg, in February, 23.
Forms of neutral and changed body’s trajectories in Nature are very differently and depended on a pressure (p) and temperature (T) of surroundings. With reference to microcosm, the neutral bodies (photons, roentgen-rays, gamma-rays, free neutrons, and etc.) for lack of influence to them coulomb’s forces always moving merely by the parabolical trajectories. The changed orbital bodies (electrons, protons,
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-particles, and etc., being on the steady atom’s and nucleus’s orbits) always moving merely by
elliptical orbits. These
changed particles by their
crossing from the one to the next steady
elliptical orbit (and a free changed ones) always moving merely by
hyperbolical trajectories. As a result of these crossings eccentricities of trajectories suddenly changed from the range
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to the
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(and back). This signified that eccentricity (e) of the orbit is appeared as the
quantum parameter depended on (p, T). Into the atom and into its nucleus acted
only exactly balanced
coulomb’s and gravity forces of differently (
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) orientations. Therefore, so-called «nuclei ‘s forces» are not existing. The
circle or the
straight-line motions in Nature are
impossible in order to a really
curvature in space and time. But as natural
indicator of this curvature may be namely the
form of body’s trajectory.
3.The real body’s trajectories in Nature
The explanation 2. It was shown in the exp. 1 for the orbital body: W < 0,
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for the non-orbital body: W>0,
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Write down the conical equation (for the circle, ellipse, parabola, hyperbola) in the non-dimensional forms
- for the ellipse
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, where 0 <
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, (2)
- for the hyperbola
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, where 1
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. (3)
By means of (2), (3),(A) we obtain
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, where
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, (a)
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, where
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(b)
For the straight-line:
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Therefore,
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(c). For the circle:
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. Therefore,
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(d)
For the parabola:
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Therefore,
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(e). But for the
elliptical and
hyperbolical trajectories parameters
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are
periodical ones.
4.Some useful formulas
Cephler’s the Third law has the next modern form (where f – the gravity constant, M – mass of the Sun,
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- the orbit ‘s semi-axis,
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– period)
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But as w=
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(where m – the planet’s mass) we obtain from (1)
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From these equations we obtain the correlation (A), where
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. Also from the (1) we obtain: a)
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For the
circle (
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) motion
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- the
first cosmic velocity. For the
parabolic (
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) motion
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- the
second (or so-called - the «parabolic») cosmic velocity, and etc. b)
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(where M – the planet’s mass, r–the planet’s radius,
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the basis vector). Therefore, the body’s
weight (
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) on the planet depended on the
form its orbit. For the
circle (
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) motion, we obtain:
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- the
acceleration of gravity. From the (B’) for the
photon (
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) , we obtain :
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- the
full photon’s energy. And etc. You will be certained soon about the parameter
fundamental significance in thermomechanics of macro- and microcosm.
Thank you. To the next report in March, 08. G.I.G.