The Annals of Frontier and Exploratory Science

3P Water, Heavy Water Molecules, Deuterium, Tritium Collective Interaction-1

Vladi S. Travkin, $^{1,\ast }$

$^{1}$ Hierarchical Scaled Physics and Technologies (HSPT), Rheinbach, Germany, Denver, CO, USA

INTRODUCTION

Single Pair and Collective 3P Interaction of Protium and Deuterium Atoms in a Volume. No COH Physics can be Applied. Physics 2

It is not only of academic interests to study the direct interaction of $^{1}$H, $^{2}$H, and $^{3}$H in a 3D volume. The matter is that the 3-scale 3D interaction of different Hydrogen isotopes is of interest and fundamental interest for areas related to the formation of hydrogen gas and of What kind of hydrogen gas exists at all?

Whether is the mixture of $^{1}$H, $^{2}$H, and $^{3}$H in pairs and as manifolds of atoms will interact to each other and in which way ?

It is already known that the hydrogen gas is not just amount of H2 molecules, but much more rich compound. "Available" Conventional One-scale Homogeneous Physics (COHP) tools and methods for condensed media all is developed for a bulk Homogenized substance (truly) and this have not allowed to treat correctly a singular Up- and Down interaction or/and dynamics of atoms and molecules in a volume to connect the some features of atomic, sub-atomic knowledge base and wonderful sometimes properties of different kind of water [1-3,10,12-21,24-28,29-30].

Application of Homogeneous one scale MD is not correct [20,21], does not help or resolve the schemes of momentum and EM dynamics in between the atoms, molecules [1-2,22-24].

One of the great issues in this simulation is the interaction of not only the polyphase matter of interest, but more important are the issues of polyscale interaction Up- and Down the scales - which the homogeneous one scale MD cannot even formulate correctly [19-21,22-24].

MATH

Hydrogen atom $^{2}$H, at moderate temperature and pressure. No free photons and the aether dynamics interaction with the proton and neutron is not shown. Structure features of the electron, proton, and neutron are simplified. The mean distance scale between the electron and nucleus is incorrect (pretty short) only due to graphical apprehension convenience.

  • "Single Pair and Collective 3P Interaction of Protium and Deuterium Atoms in a Volume. No COH Physics can be Applied. Physics 2" **

    Single Pair and Collective 3P Interaction of Protium and Tritium Atoms in a Volume. Physics 2

    It seems at first that because the atoms of tritium $^{3}$H are pretty rare in the earth environment (approximately can be accounted that every atom of tritium is surrounded by at least ~ 10^(7) atoms of normal one proton hydrogen H) and because tritium is decaying due to beta-decay mechanisms that the available atoms of tritium in a volume with protium H or/and D can disappear quickly?

    Still, we need to take into account some more mechanisms of collective and polyphase - including the aether, of course, interaction in this mixture. Because the atoms of tritium are not disappearing at all! Can we do this in COHP?

    That is just one of the questions. Much more interesting are the interaction of Protium and Tritium atoms in a volume tasks.

    MATH

    Tritium atom $^{2}$H (one of Isomers) at moderate temperature and pressure. No free photons and the aether dynamics interaction with the proton and neutrons is not shown. Structure features of the electron, proton, and neutrons are simplified. The mean distance scale between the electron and nucleus is incorrect (pretty short) only due to graphical apprehension convenience.

  • "Single Pair and Collective 3P Interaction of Protium and Tritium Atoms in a Volume. Physics 2" **

    Single Pairs and Collective 3P Interaction of Protium, Deuterium and Oxygen Atoms $^{16}$O, $^{17}$O, and $^{18}$O in a Volume. Physics 2

    The problem of collective reaction-interaction of H2, H, and O atoms in a volume also cannot be stated, even just via a simple hypothetical volumetric collective co-existence statement within COHP.

    MATH

    The Upper scale regular H2O water properties Heterogeneous Hierarchical simulation in HS physics should treat this and similar 3D structural morphologies of water's physical systems for mathematical and physical estimation of bulk physically measured and modeled water properties at continuum scales. Never done up to the present time. Consider this is the kind of Manhattan project.

    Should be depicted and visible the great deal of photons exchange while the aether dynamics interaction with particles and molecules is not shown. Structure features of molecules, electrons, particles are simplified with scaling.

    The mean distance scales between electrons, nuclei, molecules are incorrect (pretty short) only due to graphical apprehension convenience. It is obvious the need for scaling and Hierarchical modeling and simulation of these physical systems that cannot be done within COH physics - because the foundations of COH physics don't allow this physical model and picture (the Bounding Surface of assessing volume in COHP should not intersect the both, or more, phases! ) - the only one that nature makes for us, to be in theory, pictures and seems in reality.

    What a disclosure for students !

    This great endeavor is not of only academic field, but a principle one for determination of structure of water molecules, their types, overall or bulk water properties, for clustering (replication) of water molecules and imprinting (materialization) of various transducted molecules into the water effect named as the Homeopathic one. The latter feature just brings us closer to Spinning ("Torsion") Physics phenomenal experiments [19-21,24,29-30].

  • "Single Pairs and Collective 3P Interaction of Protium, Deuterium and Oxygen Atoms $^{16}$O, $^{17}$O, and $^{18}$O in a Volume. Physics 2" **

    Single Pairs and Collective 3P Interaction of H2$^{16}$O, H2$^{17}$O, H2$^{18}$O ; D2$^{16}$O, D2$^{17}$O, D2$^{18}$O ; and T2$^{16}$O, T2$^{17}$O, T2$^{18}$O Molecules in a Volume. Physics 2

    This chapter is probably the first attempt of this kind when the structural properties of various - those are a lot of, water molecule kinds and mass' are brought under umbrella of unified methodology approach of HSP to study, select, determine some bulk and species interaction properties for a volume that couldn't be achieved before (MD is not applicable), just because this methodology and direction in physics had not existed before the some recent years.

    Well, in spite that thousands studies and publications exist on the topics of water and heavy water properties, but nothing existed so far until our works on physics of 3D behavior of atoms and molecules and their parts in a filled volume.

    Homogeneous MD is not applicable to this challenge, more on that - it is wrong in some physics, and mathematical parts of this challenge simulation [3,19-21].

    For this task the physically correctly described molecules, atoms and their sub-atomic particles should be studied in a collective momentum and electromagnetic interaction.

    This even task and the mathematical formulations are not possible for performance within this COHP.

    Unfortunately this is true, and nothing of "real" or as "ab-initio" methods of COHP are able to tackle the modeling and simulations on the few scales 2P interaction as is demonstrated in our numerous studies and publications [1-2,10,12-13,14,24, 26-27,29-30,31-39].

  • "Single Pairs and Collective 3P Interaction of H2$^{16}$O, H2$^{17}$O, H2$^{18}$O ; D2$^{16}$O, D2$^{17}$O, D2$^{18}$O ; and T2$^{16}$O, T2$^{17}$O, T2$^{18}$O Molecules in a Volume. Physics 2" **

    Single Molecules of H2$^{16}$O, H2$^{17}$O, H2$^{18}$O ; D2$^{16}$O, D2$^{17}$O, D2$^{18}$O and Their Collective Interaction with Substances within a Blood (Normal) and Mammalian Cells. Preliminary Investigation (Analysis). Physics 2

    Well, this is the field that has been never studied correctly as well, because of a few mishaps of old COHP that control the fundamental biology studies:

    1) Because in Conventional One-scale Homogeneous Biology and biophysics (COHB) there is no the aether as well. Students should realize how large is the gap in the studies when interacting media of aether exists and doesn't exist!

    2) The electron - the main player in biology at the sub-atomic scales is of funny determination childish actor. It is just imaginable point-mass-charge object. COHB does not need the spin in an electron.

    3) Going Up the scales to an atomic one we should be aware of different mechanisms of atoms bonding into molecules and clusters. Because clusters formation mechanisms in COHP apparently are an imaginable and incorrect process and structures - because first of all of the 3D structure and magnetic properties of particles in structured water molecule types.

  • "Single Molecules of H2$^{16}$O, H2$^{17}$O, H2$^{18}$O ; D2$^{16}$O, D2$^{17}$O, D2$^{18}$O and Their Collective Interaction with Substances within a Blood (Normal) and Mammalian Cells. Preliminary Investigation (Analysis). Physics 2" **

    3P Dynamics and Two-scale Local-Nonlocal Hierarchical EM Modeling Characteristics of H2$^{16}$O, and D2$^{16}$O, D2$^{17}$O, D2$^{18}$O Molecules in a Volume. Physics 2

    The HSP (Hierarchical Scaled Physics) theory of governing equations for manifolds of various types water molecules in an outlined volume is created while demonstrating the incredible complexity of 3P modeling and simulation sets.

    Meanwhile, it is no sense to provide for modeling and simulation of an array of molecules images those are the spatial smeared cloudy structures with "circling" or "flying" electrons around of nuclei in COHP proclaimed and with nonsensical bonding of atoms within molecules as it is performed in COHP.

    Thus should be performed a great number of simulating tasks, we developed some of them, for understanding and revealing the paths, ways in which molecules of D2O reacting from within a community of other water molecules with the substances, macro- and just molecules of human cells (first of all we need to research these interactions), other cells as of plant environment, etc.

  • "3P Dynamics and Two-scale Local-Nonlocal EM Modeling Characteristics of H2$^{16}$O and D2$^{16}$O, D2$^{17}$O, D2$^{18}$O Molecules in a Volume. Physics 2" **

    3P Dynamics and Two-scale Local-Nonlocal Hierarchical EM and Radioactive Modeling Characteristics of H2$^{16}$O and T2$^{16}$O, HT$^{16}$O, T2$^{17}$O, T2$^{18}$O Molecules in a Volume. Physics 2

    The next chapter in water science should be devoted to a new language of 3P modeling and simulation of the real 3D structured arrays dynamics of molecules H2$^{16}$O, T2$^{16}$O, HT$^{16}$O, T2$^{17}$O, T2$^{18}$O in a volume.

    The boundary conditions (BC) for a volume of modeling and simulation are defined via a special Polyphase, Polyscale, Polyphysics (3P) method that reflects submission and exchange with the external 3P fields. There is no isolated BC in this and for other polyscale polyphase tasks because the universal medium that penetrates everything in material world is the aether and for the phases of aether (there are more than one of them) also should be no restriction so far for presence in a volume and over the Bounding Imaginable Mathematical Surface in the problem account that is accepted for finally defining the problem's mathematical statement that makes sets of simulating dependencies, equations.

    One of other important reasons is the one that is unusual for contemporary physics and is designed for justification of actions of materialization - dematerialization and the loss (and gain) of mass of some sub-atomic particles including the beta decay particles. That is the particle that changes its mass in a dynamic process.

    Then we should mention with regard of T atoms the phenomenon of the decaying process dynamics and the presence of the 3 scale objects physics within the volume of interest.

  • "3P Dynamics and Two-scale Local-Nonlocal EM and Radioactive Modeling Characteristics of T2$^{16}$O, HT$^{16}$O, T2$^{17}$O, T2$^{18}$O Molecules in a Volume. Physics 2" **

    The 4th Phase of Water. Physics 2

  • "The 4th Phase of Water. Physics 2" **

    Phase Transitions in Water Types. Physics 2

  • "Phase Transitions in Water Types. Physics 2" **

    REFERENCES:

    1. Travkin, V.S., "What Classical Mechanics of XVIII Provided in XX Has Done Wrong to the Base of Mechanical Science Including the Classical Mechanics of Continuum Particles and Conventional Orthodox Homogeneous Particle Physics", http://travkin-hspt.com/rottors/classmechwrong/classmechwrong.htm, (2014)

    2. Travkin, V.S.,"The Major Forces Have Been Missing From Governing Equations for Dynamics of Sub-atomic and Continuum Particles, Bodies in XVIII - XX ", http://travkin-hspt.com/rottors/forcemissing/forcemissing.htm, (2014)

    3. Travkin, V.S., "Why is it Different from Homogeneous and other Theories and Methods of Heterogeneous Media Mechanics/(other Sciences) Description?" http://travkin-hspt.com/fundament/03.htm, (2002)

    4. Kanarev, Ph.M., "A Model for the Free Electron," Galilean Electrodynamics, Vol. 13, No. S1, pp. 15-18, (2002)

    5. Kanarev, Ph.M., Photon, http://www.micro-world.su/ Folder "Books"; retrieved 05/05/2013

    6. Kanarev, Ph.M., Nuclei of Atoms, http://www.micro-world.su/ Folder "Books"; retrieved 05/05/2013

    7. Kanarev, Ph.M., Answers to Microworld Questions, http://www.micro-world.su/ Folder "Answers"; retrieved 05/05/2013

    8. Kanarev, Ph.M., Introduction to New Electrodynamics, http://www.micro-world.su/ Folder "Books"; retrieved 05/05/2013

    9. Kanarev, Ph.M. , The Foundations of Physchemistry of Microworld. Monograph. The 15th edition, http://www.micro-world.su/index.php/2010-12-22-11-45-21/139--i; retrieved 05/05/2013

    10. Travkin, V.S. and Bolotina, N.N., "Hydrogen in HSP-VAT. Introduction," http://travkin-hspt.com/parphys2/abstracts/hydrogen-ab.htm, (2013)

    11. Travkin, V.S. and Bolotina, N.N., "Iron. Introduction," http://travkin-hspt.com/parphys2/abstracts/iron-ab.htm, (2013)

    12. Travkin, V.S., Particle Physics - Heterogeneous Polyscale Collectively Interactive, http://travkin-hspt.com/parphys/index.htm, (2011)

    13. Travkin, V.S.,"Torsion" or Spinning (Rotation) Physics Scaled (SPS), http://travkin-hspt.com/rottors/index.htm, (2014)

    14. Travkin, V.S. and Bolotina, N.N., "The Classical and Sub-Atomic Physics are the Same Physics," http://travkin-hspt.com/parphys/pdf/51_PrAtEd-QM-Ref-2HSPT.pdf, (2013)

    15. Travkin, V.S., Particle Physics (Particle Physics 2). Fundamentals, http://travkin-hspt.com/parphys2/index.htm, (2013)

    16. Travkin, V.S., Nuclear Physics Structured. Introduction, http://travkin-hspt.com/nuc/index.htm, (2006-2013)

    17. Travkin, V.S., Statistical Mechanics Homogeneous for Point Particles. What Objects it Articulates? http://travkin-hspt.com/statmech/index.htm, (2014)

    18. Travkin, V.S., Solid State Polyscale Physics. Fundamentals, http://travkin-hspt.com/solphys/index.htm, (2014)

    19. Travkin, V.S., "Pseudo-Averaging (Scaling, Hierarchy), Quasi-Averaging, Ad-hoc Averaging, and other "Averaging" (Scaling, Hierarchy) Type Claims" http://travkin-hspt.com/fundament/pseudo.htm. (2003)

    20. Travkin, V.S. and Bolotina, N.N., "Quantum Chemistry, Physical Chemistry, Molecular Dynamics Simulation, DFT (Density Functional Theory), and Coarse-Graining Techniques Applied in Structural, Cellular Biology, Polymer Science and Implication for Scaleportation," Journal of Alternative Energy and Ecology, No. 2, pp. 58-75, (2011a)

    "Quantum Chemistry, Physical Chemistry, Molecular Dynamics Simulation, DFT (Density Functional Theory), and Coarse-Graining Techniques Applied in Structural, Cellular Biology, Polymer Science and Implication for Scaleportation"(757K)

    21. Travkin, V.S. and Bolotina, N.N., "Pseudo-Scaled and Scaled Description and Scaleportation of Inorganic and Organic Polymer and Polymer Composites Properties," Journal of Alternative Energy and Ecology, No. 1, pp. 62-77, (2011b)

    "Pseudo-Scaled and Scaled Description and Scaleportation of Inorganic and Organic Polymer and Polymer Composites Properties"(818K)

    22. Travkin, V.S., "Two-Scale Three-Phase Regular and Irregular Shape Charged Particles (Electrons, Photons) Movement in MHL Electromagnetic Fields in a Vacuum0 (Aether)," http://travkin-hspt.com/parphys2/abstracts/twoparticlesshort-ab.htm

    23. Travkin, V.S. and Bolotina, N.N., "Two-Scale Two-Phase Formation of Charged 3D Continuum Particles - Sphere and Cube From Electrons in a Vacuum0 (Aether). An Example of Scaleportation of Charge from the Sub-Atomic to Continuum Charged Particles, Conventional MD Cannot be Applied," http://travkin-hspt.com/parphys2/abstracts/subtocontin-ab.htm

    24. Travkin, V.S.,"Scaled Presentation of "Torsion" Mechanics in Polyphase Media", http://travkin-hspt.com/rottors/tormechpoly/tormechpoly.htm, (2014)

    25. Travkin, V.S., Fundamentals of Hierarchical Scaled Physics (HSP-VAT). Description of Transport and Phenomena in Heterogeneous and Scaled Media, http://travkin-hspt.com/fundament/index.htm, (2003)

    26. Travkin, V.S., What's Wrong with the Pseudo-Averaging Used in Textbooks on Atomic Physics and Electrodynamics for Maxwell-Heaviside-Lorentz Electromagnetism Equations, http://travkin-hspt.com/eldyn/maxdown/maxdown.htm, (2009)

    27. Travkin, V.S., Incompatibility of Maxwell-Lorentz Electrodynamics Equations at Atomic and Continuum Scales, http://travkin-hspt.com/eldyn/incompat/incompat.htm, (2009)

    28. Travkin, V.S., Electrodynamics 2 - Elements 3P (Polyphase-Polyscale-Polyphysics), http://travkin-hspt.com/eldyn2/index.htm, (2013)

    29. Travkin, V.S. and Bolotina, N.N., "Water Structured. Introduction," http://travkin-hspt.com/parphys2/abstracts/water-ab.htm, (2013)

    30. Travkin, V.S. and Bolotina, N.N., "Two scale Modeling of Water Molecule Atoms and Overall Water Mesoscale EM Galilean Fields ," http://travkin-hspt.com/parphys2/abstracts/water2scale-ab.htm, (2013)

    31. Travkin, V.S., Education, Courses, http://travkin-hspt.com/edu/index.htm, (2006)

    32. Travkin, V.S., Continuum Mechanics of Heterogeneous (Ht) Media; Elasticity, Plasticity, http://travkin-hspt.com/elastic/index.htm, (2005)

    33. Travkin, V.S., Nanotechnologies - General Concept for Pretty Large Amount of Pretty Small Gadgets Embedded Into Something and Consequences for Design and Manufacturing, http://travkin-hspt.com/nanotech/index.htm, (2006)

    34. Travkin, V.S., "Classical Problems in Fluid Mechanics," http://travkin-hspt.com/fluid/03.htm, (2003)

    35. Travkin, V.S., Fluid Mechanics, http://travkin-hspt.com/fluid/index.htm, (2003)

    36. Travkin, V.S., Fluid Mechanics 2 - Elements 3P, http://travkin-hspt.com/fluid2/index.htm, (2010)

    37. Travkin, V.S., Thermal Physics, http://travkin-hspt.com/thermph/index.htm, (2003)

    38. Travkin, V.S., "Heat Exchangers. It is the Hierarchical ^v Technology," http://travkin-hspt.com/thermph/07.htm, (2009)

    39. Travkin, V.S., Thermal Physics 2 - Elements 3P (Polyphase-Polyscale-Polyphysics), http://travkin-hspt.com/thermph2/index.htm, (2011)

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    These are not well known problems, because of decades COHP studies in the mode of Homogeneous fields they (these tasks) couldn't be stated in either correct form - still can not be resolved within the Homogeneous One-Scale General physics, Spinning physics, nuclear, particle and atomic physics, electromagnetism, Gravidynamics and astrophysics.

    UNDER CONTINUAL DEVELOPMENT