The Confirmed Validity of the Thermohydrogravidynamic Theory Concerning the Forthcoming Intensification of the Global Natural Processes from December 7, 2019 to April 18, 2020 AD

We present the confirmed validity of the prediction (made in unpublished article (Simonenko, 2019b) presented on December 9, 2019 to the journal Energy Research) of the thermohydrogravidynamic theory (Simonenko, 2014) concerning the evaluated probabilities of the forthcoming intensification of the global seismotectonic, volcanic, climatic and magnetic processes of the Earth during the evaluated beginning (from December 7, 2019 to April 18, 2020) of the established in 2012 AD (Simonenko, 2012a) and finally confirmed in 2019 AD (Simonenko, 2019a) “first forthcoming subrange 2020 ÷ 2026 AD of the increased intensification of the Earth” determined by the combined non-stationary cosmic energy gravitational influences on the Earth of the planets (Mercury, Venus, Mars and Jupiter) and the Sun (owing to the gravitational interaction of the Sun with Jupiter, Saturn, Uranus and Nep-tune). Thermohydrogravidynamic


Introduction
The problem of the long-term predictions of the strong earthquakes (Richter,  Zealand (2010), and Japan (2011) "have shown that, in present state, scientific researchers have achieved little or almost nothing in the implementation of short-and medium-term earthquake prediction, which would be useful for disaster mitigation measures".
In this article, following the global prediction thermohydrogravidynamic principle (11) used for the real planetary configurations of the Earth and the planets of the Solar System, the author presents the confirmed validity of the prediction (of the unpublished article (Simonenko, 2019b) presented on December 9, 2019 to the journal Energy Research) of the thermohydrogravidynamic theory concerning the evaluated probabilities of the strongest earthquakes during the established beginning (from December 7, 2019 to April 18, 2020) of the predicted (Simonenko, 2012a(Simonenko, , 2014 and confirmed (Simonenko, 2019a) "first forthcoming subrange 2020 ÷ 2026 AD of the increased intensification of the Earth" determined by the combined non-stationary cosmic energy gravitational influences on the Earth of the system Sun-Moon, Mercury, Venus, Mars, Jupiter and the Sun (owing to the gravitational interaction of the Sun with Jupiter, Saturn, Uranus and Neptune).
To do this, in Section 2.1 we present the established (Simonenko, 2006(Simonenko, , 2007a generalized differential formulation (7) of the first law of thermodynamics (for moving rotating deforming compressible heat-conducting stratified individual finite continuum region τ subjected to the non-stationary Newtonian gravitational field) extending the classical identical formulation (Gibbs, 1873;Landau & Lifshitz, 1976) by taking into account (along with the classical infinitesimal change of heat Q δ and the classical infinitesimal change of the internal energy τ dU ) the established (Simonenko, 2006(Simonenko, , 2007a differential (infinitesimal) energy gravitational influence dG (as the result of the Newtonian non-stationary cosmic and terrestrial gravitation) on the individual finite continuum region τ during the infinitesimal time interval dt . Based on the established (Simonenko, 2006(Simonenko, , 2007a (Simonenko, 2012a(Simonenko, , 2014 global prediction thermohydrogravidynamic principles (11) and (12) determining the maximal temporal intensifications of the global and regional natural (seismotectonic, volcanic, climatic and magnetic) processes of the Earth.

The Thermohydrogravidynamic Technology of the Short-Range Prediction of the Global Intensifications of the Seismotectonic and Magnetic Processes of the Earth Subjected to Non-Stationary Cosmic Gravitation of the Solar System
Journal of Geoscience and Environment Protection with respect to a Cartesian coordinate system K centred at the origin O and determined by the axes 1 2 3 , , X X X (see Figure 1). The unit normal K-basis coordinate vectors triad 1 2 3 , , μ μ μ is taken in the directions of the axes 1 2 3 , , X X X , respectively. The K-basis vector triad is taken to be right-handed in the order 1 2 3 , , μ μ μ , see Figure 1.
( , t) = g g r is the local gravity acceleration considered as a vector function (Simonenko, 2007a(Simonenko, , 2012a of variables r and the time t.
The position-vector c r of the mass center C of the individual finite continuum region τ in the K-coordinate system is given by the following expression where τ m is the mass of the individual finite continuum region τ , dV is the mathematical differential of the physical volume of the individual finite continuum region τ , ρ ρ( ,t) ≡ r is the local macroscopic density of mass distribution, r is the position-vector of the continuum volume dV . The speed of the mass centre C of the individual finite continuum region τ is defined by the We shall use the differential formulation of the first law of thermodynamics (De Groot & Mazur, 1962) for the specific volume 1/ ρ ϑ = of the one-component deformed continuum with no chemical reactions: where u is the specific (per unit mass) internal thermal energy, p is the thermodynamic pressure, П is the viscous-stress tensor, v is the hydrodynamic Figure 1. Cartesian coordinate system K of a Galilean frame of reference and an individual finite continuum region τ subjected to the non-stationary combined (cosmic and terrestrial) Newtonian gravitation field and non-potential terrestrial stress forces.
velocity of the continuum macrodifferential element (De Groot & Mazur, 1962), denotes the total derivative (De Groot & Mazur, 1962;Batchelor, 1967;Gyarmati, 1970;Landau & Lifshitz, 1988) following the continuum substance, dq is the differential change of heat across the boundary of the continuum region (of unit mass) related with the thermal molecular conductivity described by the heat equation (De Groot & Mazur, 1962): where q J is the heat flux. The viscous-stress tensor П is taken from the de- Groot & Mazur, 1962), where δ is the Kronecker delta-tensor. The macroscopic local mass density ρ of mass distribution and the local hydrodynamic velocity v of the macroscopic velocity field is determined by the classical hydrodynamic continuity equation (De Groot & Mazur, 1962;Batchelor, 1967;Landau & Lifshitz, 1988): under the absence of distributed space-time sources of mass output.
Using the differential formulation (2) for the specific (per unit mass) internal thermal energy u of the one-component deformed continuum with no chemical reactions, the heat equation (3), the decomposition p = + Ρ δ Π of the pressure tensor P , the hydrodynamic continuity equation (4), the classical equation (Batchelor, 1967;Gyarmati, 1970) for each variable f (such as 2 / 2 v , u and ψ ): and the general equation of continuum movement (Gyarmati, 1970): for the deformed continuum characterized by the symmetric stress tensor = − Т P (Gyarmati, 1970) of a general form and taking into account the time variations of the potential ψ of the non-stationary gravitational field (characterized by the local gravity acceleration vector ψ = −∇ g ) inside of the individual finite continuum region τ , we derived (Simonenko, 2006(Simonenko, , 2007a the generalized differential formulation (for the Galilean frame of reference) of the first law of thermodynamics (for moving rotating deforming heat-conducting stratified individual finite one-component continuum region τ subjected to the nonstationary Newtonian gravitational field and to non-potential stress forces characterized by the symmetric stress tensor Т ): where np, τ δA ∂ is the established generalized (Simonenko, 2006(Simonenko, , 2007a (Gibbs, 1873;Landau and Lifshitz, 1976) differential change of heat of the individual finite continuum region τ related with the thermal molecular conductivity of heat across the boundary ∂τ of the individ- is the established (Simonenko, 2007a(Simonenko, , 2007b) differential (infinitesimal) energy gravitational influence (as the result of the Newtonian non-stationary gravitation) on the individual finite continuum region τ (during the infinitesimal time interval dt ); τ π is the established (Simonenko, 2006(Simonenko, , 2007a macroscopic potential energy (of the individual finite continuum region τ ) related with the non-stationary potential ψ of the gravitational field; τ U is the classical (Gibbs, 1873;Landau & Lifshitz, 1976) microscopic internal thermal energy of the individual finite continuum region τ ; τ K is the established (Simonenko, 2006(Simonenko, , 2007a instantaneous macroscopic kinetic energy of the individual finite continuum region τ .

The Global Prediction Thermohydrogravidynamic Principles Determining the Maximal Temporal Intensifications of the Global Seismotectonic, Volcanic, Climaticand Magnetic Processes of the Earth Subjected to Non-Stationary Cosmic Gravitation
Taking into account the general relation (8) for the infinitesimal energy gravitational influence dG on the individual finite continuum region τ , we obtained (Simonenko, 2014, 2019) the following relation for the combined differential cosmic non-stationary energy gravitational influence c,r dG(τ ) (during the infinitesimal time dt ) of the Solar System (the planets, the Moon and the Sun owing to the gravitational interaction of the Sun with Jupiter, Saturn, Uranus and Neptune) on the internal rigid core c,r τ of the Earth: where c,r ρ is the mass density of the internal rigid core c,r τ , in the internal rigid core c,r τ of the Earth) approximated as follows (Simonenko, 2014, 2019) (Simonenko, 2009(Simonenko, , 2012a(Simonenko, , 2013 of the gravitational potential 3i 3 ψ (C ,t) created by the planet i τ (of the Solar System) at the mass center 3 C of the Earth; is the partial derivative (Simonenko, 2009(Simonenko, , 2012a(Simonenko, , 2013 of the gravitational potential 3MOON 3 ψ (C ,t) created by the Moon at the mass center 3 C of the Earth.
Based on the generalization (7) of the first law of thermodynamics (used for the internal rigid core c,r τ of the Earth), we formulated (Simonenko, 2012a(Simonenko, , 2014) the global prediction thermohydrogravidynamic principles determining the maximal temporal intensifications of the established thermohygrogravidynamic processes (in the internal rigid core c,r τ and in the boundary region rf τ between the internal rigid core c,r τ and the fluid core c,f τ of the Earth considered as a whole) subjected to the combined cosmic energy gravitational influence of the planets of the Solar System, the Sun (owing to the gravitational interaction of the Sun with the outer large planets) and the Moon. We concluded (Simonenko, 2012a(Simonenko, , 2014) (based on the generalization (7) of the first law of thermodynamics used for the internal rigid core c,r τ of the Earth) that the maximal intensifications of the established thermohygrogravidynamic processes are related with the corresponding maximal intensifications of the global and regional natural (seismotectonic, volcanic, climatic and magnetic) processes of the Earth.

Conclusions
We have presented in Section 2.1 the established (Simonenko, 2006(Simonenko, , 2007a(Simonenko, , 2009(Simonenko, , 2012a, 2013) generalized differential formulation (7) (given for the Galilean frame of reference) of the first law of thermodynamics deduced rigorously based on the postulates of the non-equilibrium thermodynamics (De Groot & Mazur, 1962;Gyarmati, 1970) and hydrodynamics (Batchelor, 1967;Landau & Lifshitz, 1988). The generalized differential formulation (7) is valid for moving rotating deforming heat-conducting stratified individual finite one-component continuum region τ (characterized by the symmetric stress tensor T ) subjected to the non-stationary gravitational field. The generalized differential formulation (7) of the first law of thermodynamics extends the classical (Gibbs, 1873;Landau & Lifshitz, 1976) identical formulation by taking into account (along with the classical infinitesimal change of heat δQ and the classical infinitesimal change of the internal energy τ dU ) the established (Simonenko, 2004(Simonenko, , 2006(Simonenko, , 2007a infinitesimal increment τ dK of the macroscopic kinetic energy τ K , the established (Simonenko, 2006(Simonenko, , 2007a infinitesimal increment τ dπ of the gravitational potential energy τ π , the established generalized (Simonenko, 2006(Simonenko, , 2007a infinitesimal work np, τ δA ∂ done on the individual finite continuum region τ by the surroundings of τ , and the established (Simonenko, 2007a) differential energy gravitational influence dG on the individual finite continuum region τ during the infinitesimal time interval dt due to the non-stationary gravitational field.
We have presented in Section 2.2 the established (Simonenko, 2012a(Simonenko, , 2014(Simonenko, , 2019a global prediction thermohydrogravidynamic principles (11) and (12)   Pr 1/ 7 = (given by (38) We have presented in Section 3.3 the calculated (on October 6, 2020, especially for the presentation on the 10 th International Conference on Geology and Geophysics) the mean date t(2019, 2020) (given by (41) of the probable most strongest earthquake of the Earth during the considered range December 7, 2019 ÷ April 18, 2020. We have obtained the reasonably small difference of 8 days between the calculated theoretical date t(2019, 2020) (given by (41)) and the real date January 28, 2020 AD (given by (42)) of the most strongest earthquake (characterized by the maximal 7.7-magnitude) of the Earth occurred 123 km NNW of Lucea, Jamaica during the established (Simonenko, 2019b) range from December 7, 2019 to April 18, 2020. We can conclude that the reasonably small difference of 8 days is based on the used simple approximation of the circular orbits (Simonenko, 2007b(Simonenko, , 2012a(Simonenko, , 2013 of the planets around the Sun and by disregarding the established partial derivative 3MOON 3 ψ (C ,t)/ t ∂ ∂ (Simonenko, 2009(Simonenko, , 2012a(Simonenko, , 2013 of the gravitational potential 3MOON 3 ψ (C ,t) created by the Moon at the mass center 3 C of the Earth.
Taking into account the prediction (Simonenko, 2012a(Simonenko, , 2014(Simonenko, , 2019a of the thermohydrogravidynamic theory (Simonenko, 2006(Simonenko, , 2007b(Simonenko, , 2009(Simonenko, , 2012a(Simonenko, , 2013(Simonenko, , 2014(Simonenko, , 2016(Simonenko, , 2019a concerning the first forthcoming subrange 2020 ÷ 2026 AD Jupiter) and the Sun (owing to the gravitational interaction of the Sun with Jupiter, Saturn, Uranus and Neptune), we have concluded (on October 6, 2020 as the main conclusion for the presentation on the 10 th International Conference on Geology and Geophysics) that it is very important to make in the near future the urgent identical calculations (of the probabilities of the possible strongest intensifications of the seismotectonic, volcanic, climatic and magnetic processes for the time range containing the calculated date 2021.1 AD) for Japan , Italy , Greece , China (Simonenko, 2018) and Chile , for which we have established  the confirmed cosmic energy gravitational genesis of the strongest earthquakes.