Research
Synthesis of Thermodynamics and Continuum Mechanics
On the basis of a unified theory of the processes of transfer and transformation of any form of energy, called "energy dynamics" by the author, the possibility of synthesizing the methods of non equilibrium thermodynamics and continuum mechanics is shown. A unified substantiation of the main provisions of both the theory of irreversible processes and classical mechanics, free from postulates and hypotheses, is given. At the same time, a new method for studying real processes is proposed, which does not exclude from consideration any (reversible or irreversible) part of them. This made it possible to generalize all three Newton's principles, to find a short-range form of his law of gravity, and for the first time to substantiate the principle of least action, which mutually enriches both thermodynamics and mechanics.
New Applications of Non-Equilibrium Thermodynamics
We propose to extend the existing theory of irreversible processes (TIP) to include reversible real processes associated with the performance of useful work. This is achieved by the fact that the main quantities used by this theory, thermodynamic forces and fluxes, are derived not from the principle of increasing entropy, but rather from the law of the conservation of energy. This way of constructing TIP prevents the occurrence of thermodynamic inequalities and allows one to substantiate all its provisions without invoking the postulates and considerations of a molecular-kinetic and statistical-mechanical nature. This opens up the possibility of further reducing the number of empirical coefficients and expanding the scope of TIP applicability to nonlinear systems and states that are far from equilibrium, as well as to energy conversion processes which are primarily of interest to power engineers, technologists, biophysicists and astro-physicists. At the same time, the unity of the laws of transformation of all forms of energy and the difference between their equations, reciprocity relations and efficiency criteria from the generally accepted ones are proved. On this basis, a theory of similarity of power plants is proposed and their universal load characteristics are constructed, which make it possible to take the next step towards bringing the results of the thermodynamic analysis of their efficiency closer to reality.
Instruction Of Paralogistics Thermodynamics
ΓΒΓΒ° Γβ¬ΓΒΓΒ΄ΓΒ΅ ΓΒΊΓΒΎΓΒ½ΓΒΊΓβ¬ΓΒ΅ΓβΓΒ½ΓβΉΓβ¦ ΓΒΏΓβ¬ΓΒΈΓΒΌΓΒ΅Γβ¬ΓΒΎΓΒ² ΓΒΏΓΒΎΓΒΊΓΒ°ΓΒ·ΓΒ°ΓΒ½ΓΒΎ, Γβ‘ΓβΓΒΎ ΓΒΏΓΒΎΓΒ΄ΓΒΌΓΒ΅ΓΒ½ΓΒ° ΓΒΓΒ½ΓΒ΅Γβ¬ΓΒ³ΓΒΎΓΒ½ΓΒΎΓΒΓΒΈΓβΓΒ΅ΓΒ»ΓΒ ΓβΓΒ΅ΓΒΏΓΒ»ΓΒΎΓΒ²ΓΒΎΓΒΉ ΓβΓΒΎΓβ¬ΓΒΌΓβΉ ΓΒ΄ΓΒ²ΓΒΈΓΒΆΓΒ΅ΓΒ½ΓΒΈΓΒΓΒΓΒ½ΓβΓβ¬ΓΒΎΓΒΏΓΒΈΓΒ΅ΓΒΉ ΓΒΊΓΒ°ΓΒΊ ΓΒΊΓΒΎΓΒΎΓβ¬ΓΒ΄ΓΒΈΓΒ½ΓΒ°ΓβΓΒΎΓΒΉ ΓβΓΒ΅ΓΒΏΓΒ»ΓΒΎΓΒΎΓΒ±ΓΒΌΓΒ΅ΓΒ½ΓΒ° ΓΒΏΓβ¬ΓΒΈΓΒ²ΓΒΎΓΒ΄ΓΒΈΓβ ΓΒΊ Γβ¬ΓΒΓΒ΄ΓΖ ΓΒΏΓΒ°Γβ¬ΓΒ°ΓΒ»ΓΒΎΓΒ³ΓΒΈΓΒ·ΓΒΌΓΒΎΓΒ², Γβ‘ΓΒΈΓΒΓΒ»ΓΒΎ ΓΒΊΓΒΎΓβΓΒΎΓβ¬ΓβΉΓβ¦ Γβ¬ΓΒ°ΓΒΓβΓβΓβ ΓΒΏΓΒΎ ΓΒΌΓΒ΅Γβ¬ΓΒ΅ Γβ¬ΓΒ°ΓΒΓΛΓΒΈΓβ¬ΓΒ΅ΓΒ½ΓΒΈΓΒ ΓΒΓβΓΒ΅Γβ¬ΓβΉ ΓΒΏΓβ¬ΓΒΈΓΒ»ΓΒΎΓΒΆΓΒ΅ΓΒ½ΓΒΈΓΒ ΓβΓΒ΅Γβ¬ΓΒΌΓΒΎΓΒ΄ΓΒΈΓΒ½ΓΒ°ΓΒΌΓΒΈΓΒΊΓΒΈ. ΓβΓΒΓΒΊΓβ¬ΓβΉΓβΓβΉ ΓΒ³ΓΒ½ΓΒΎΓΒΓΒ΅ΓΒΎΓΒ»ΓΒΎΓΒ³ΓΒΈΓβ‘ΓΒ΅ΓΒΓΒΊΓΒΈΓΒ΅ ΓΒΊΓΒΎΓβ¬ΓΒ½ΓΒΈ ΓΒΓβΓΒΈΓβ¦ ΓΒΏΓΒ°Γβ¬ΓΒ°ΓΒ»ΓΒΎΓΒ³ΓΒΈΓΒ·ΓΒΌΓΒΎΓΒ² ΓΒΈ ΓΒΏΓβ¬ΓΒ΅ΓΒ΄ΓΒ»ΓΒΎΓΒΆΓΒ΅ΓΒ½ΓΒ°ΓΒ±ΓΒΎΓΒ»ΓΒ΅ΓΒ΅ ΓΒΎΓΒ±Γβ°ΓΒ°ΓΒ ΓΒΌΓΒ΅Γβ¬ΓΒ° ΓΒΊΓΒΎΓΒ»ΓΒΈΓβ‘ΓΒ΅ΓΒΓβΓΒ²ΓΒ° Γβ¦ΓΒ°ΓΒΎΓβΓΒΈΓβ‘ΓΒ΅ΓΒΓΒΊΓΒΎΓΒ³ΓΒΎ ΓΒ΄ΓΒ²ΓΒΈΓΒΆΓΒ΅ΓΒ½ΓΒΈΓΒ, ΓΒ½ΓΒ°ΓΒ·ΓΒ²ΓΒ°ΓΒ½ΓΒ½ΓΒ°ΓΒ ΓΒ΄ΓΒ»ΓΒ ΓΒΊΓβ¬ΓΒ°ΓβΓΒΊΓΒΎΓΒΓβΓΒΈ ΓβΓΒ΅Γβ¬ΓΒΌΓΒΎΓΒΈΓΒΌΓΒΏΓΖΓΒ»ΓΕΓΒΓΒΎΓΒΌ. ΓΕΈΓΒΎΓΒΊΓΒ°ΓΒ·ΓΒ°ΓΒ½ΓΒΎ, ΓΒΊΓΒ°ΓΒΊ ΓΒ΅ΓΒ³ΓΒΎ ΓΒΏΓβ¬ΓΒΈΓΒΌΓΒ΅ΓΒ½ΓΒ΅ΓΒ½ΓΒΈΓΒ΅ ΓΒ²ΓΒΌΓΒ΅ΓΒΓβΓΒΎ ΓΒΓΒ½ΓβΓβ¬ΓΒΎΓΒΏΓΒΈΓΒΈ ΓΖΓΒΓβΓβ¬ΓΒ°ΓΒ½ΓΒΓΒ΅ΓβΓΒΏΓβ¬ΓΒ°ΓΒΊΓβΓΒΈΓβ‘ΓΒ΅ΓΒΓΒΊΓΒΈ ΓΒ²ΓΒΓΒ΅ ΓΒΈΓΒ·ΓΒ²ΓΒ΅ΓΒΓβΓΒ½ΓβΉΓΒ΅ ΓΒΈ ΓΒΎΓΒ±ΓΒ½ΓΒ°Γβ¬ΓΖΓΒΆΓΒ΅ΓΒ½ΓΒ½ΓβΉΓΒ΅ ΓΒ°ΓΒ²ΓβΓΒΎΓβ¬ΓΒΎΓΒΌΓΒΏΓΒ°Γβ¬ΓΒ°ΓΒ»ΓΒΎΓΒ³ΓΒΈΓΒ·ΓΒΌΓβΉ, ΓΒ²ΓΒΊΓΒ»ΓΕ½Γβ‘ΓΒ°ΓΒ ΓΒΏΓβ¬ΓΒ΅ΓΒ΄ΓΒΓΒΊΓΒ°ΓΒ·ΓΒ°ΓΒ½ΓΒΈΓΒ΅ ΓβΓΒ΅ΓΒΏΓΒ»ΓΒΎΓΒ²ΓΒΎΓΒΉ ΓΒΓΒΌΓΒ΅Γβ¬ΓβΓΒΈ ΓβΓΒΓΒ΅ΓΒ»ΓΒ΅ΓΒ½ΓΒ½ΓΒΎΓΒΉ ΓΒΈΓΒ΄ΓΒ΅ΓΒ³Γβ¬ΓΒ°ΓΒ΄ΓΒ°Γβ ΓΒΈΓΒΈ ΓΒ±ΓΒΈΓΒΎΓΒ»ΓΒΎΓΒ³ΓΒΈΓβ‘ΓΒ΅ΓΒΓΒΊΓΒΈΓβ¦ ΓΒΓΒΈΓΒΓβΓΒ΅ΓΒΌ.ΓΒ‘ΓΒ΄ΓΒ΅ΓΒ»ΓΒ°ΓΒ½ ΓΒ²ΓβΉΓΒ²ΓΒΎΓΒ΄, Γβ‘ΓβΓΒΎ ΓΒ·ΓΒ°ΓΒΌΓΒ΅ΓΒ½ΓΒ° ΓΒΓΒ½ΓβΓβ¬ΓΒΎΓΒΏΓΒΈΓΒΈ ΓβΓΒ΅Γβ¬ΓΒΌΓΒΎ- ΓΒΈΓΒΌΓΒΏΓΖΓΒ»ΓΕΓΒΓΒΎΓΒΌΓΒΎΓβΓΒΊΓβ¬ΓβΉΓΒ²ΓΒ°ΓΒ΅ΓβΓΒΏΓΖΓβΓΕ ΓΒΊ Γβ¬ΓΒ°ΓΒΓΛΓΒΈΓβ¬ΓΒ΅ΓΒ½ΓΒΈΓΕ½ ΓΒ²ΓΒΎΓΒ·ΓΒΌΓΒΎΓΒΆΓΒ½ΓΒΎΓΒΓβΓΒ΅ΓΒΉ ΓβΓΒ΅Γβ¬ΓΒΌΓΒΎΓΒ΄ΓΒΈΓΒ½ΓΒ°ΓΒΌΓΒΈΓβ‘ΓΒ΅ΓΒΓΒΊΓΒΎΓΒ³ΓΒΎ ΓΒΌΓΒ΅ΓβΓΒΎΓΒ΄ΓΒ° ΓΒΏΓβ¬ΓΒΈ ΓΒΈΓΒΓΒΓΒ»ΓΒ΅ΓΒ΄ΓΒΎΓΒ²ΓΒ°ΓΒ½ΓΒΈΓΒΈ ΓΒ½ΓΒ΅Γβ¬ΓΒ°ΓΒ²ΓΒ½ΓΒΎΓΒ²ΓΒ΅ΓΒΓΒ½ΓβΉΓβ¦ ΓΒΓΒΈΓΒΓβΓΒ΅ΓΒΌ ΓΒΈ ΓΒ½ΓΒ΅ΓΒΓβΓΒ°ΓβΓΒΈΓβ‘ΓΒ΅ΓΒΓΒΊΓΒΈΓβ¦ ΓΒΏΓβ¬ΓΒΎΓβ ΓΒ΅ΓΒΓΒΓΒΎΓΒ², ΓΒΊ ΓΒΓΒΈΓΒ½ΓβΓΒ΅ΓΒ·ΓΖ ΓβΓΒ΅Γβ¬ΓΒΌΓΒΎΓΒ΄ΓΒΈΓΒ½ΓΒ°ΓΒΌΓΒΈΓΒΊΓΒΈ ΓΒ ΓΒ΄Γβ¬ΓΖΓΒ³ΓΒΈΓΒΌΓΒΈ ΓβΓΖΓΒ½ΓΒ΄ΓΒ°ΓΒΌΓΒ΅ΓΒ½ΓβΓΒ°ΓΒ»ΓΕΓΒ½ΓβΉΓΒΌΓΒΈ ΓΒ΄ΓΒΈΓΒΓβ ΓΒΈΓΒΏΓΒ»ΓΒΈΓΒ½ΓΒ°ΓΒΌΓΒΈ ΓΒΈ ΓΒΊ ΓΒ±ΓΒΎΓΒ»ΓΒ΅ΓΒ΅ ΓΒ³ΓΒ»ΓΖΓΒ±ΓΒΎΓΒΊΓΒΎΓΒΌΓΖ ΓΒΏΓΒΎΓΒ½ΓΒΈΓΒΌΓΒ°ΓΒ½ΓΒΈΓΕ½ ΓΒΌΓΒΈΓβ¬ΓΒΎΓΖΓΒΓβΓβ¬ΓΒΎΓΒΉΓΒΓβΓΒ²ΓΒ°.
