- International Journal of Thermodynamics
- Volume:9 Issue:3
- Teaching the Quantal Exposition of the Unified Quantum Theory of Mechanics and Thermodynamics
Teaching the Quantal Exposition of the Unified Quantum Theory of Mechanics and Thermodynamics
Authors : Michael Von Spakovsky
Pages : 147-159
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Publication Date : 2006-09-01
Article Type : Research Paper
Abstract :The author presents his experience in teaching at a graduate level the quantal exposition of a new non-statistically based paradigm of physics and thermodynamics. This paradigm, called the Unified Quantum Theory of Mechanics and Thermodynamics, applies to all systems large or small insert ignore into journalissuearticles values(including one particle systems); either in a state of thermodynamic insert ignore into journalissuearticles values(i.e. stable); equilibrium or not in a state of thermodynamic equilibrium. It uses as its primitives inertial mass, force, and time and introduces the laws of thermodynamics in the most unambiguous and general formulations found in the literature. Starting with a precise definition of system and of state followed by statements and corollaries of the laws of thermodynamics, the thermodynamic formalism is developed without circularity and ambiguity. In this quantal exposition of the new paradigm, a brief review of the formalism of thermodynamics as a general science not limited to stable equilibrium and large insert ignore into journalissuearticles values(macroscopic); systems as well as a very brief summary of the three prevalent formalisms in classical physics are presented followed by a presentation and development of solutions for a number of elementary problems in quantum physics insert ignore into journalissuearticles values(e.g., a particle in a box, a harmonic oscillator, a rigid rotor, etc.);. These solutions and the maximum entropy principle are then used in a constrained optimization to develop the canonical and grand canonical distributions for Fermi-Dirac and Bose-Einstein types of particles, i.e. for fermions and bosons. This is done without the use of analogies between statistical and thermodynamic results and without additional hypotheses such as the ergodic hypothesis of statistical mechanics. These distributions are then employed under various assumptions insert ignore into journalissuearticles values(i.e. the Boltzmann, constant-potential, point-particle, and continuous eigenvalue-spectrum approximations); to derive the corresponding thermodynamic property expressions for perfect, semi-perfect insert ignore into journalissuearticles values(ideal);, and Sommerfeld gases as well as for mixtures of ionized and dissociated gases. In a similar fashion but with a change from a single- to a multi-particle partition function and with the addition of various inter-particle potentials for two-particle interactions insert ignore into journalissuearticles values(e.g., the Lennard-Jones potential, the square-well potential, etc.);, expressions for the thermodynamic properties of dense gases are developed and presented. An initial version of this paper was published in July of 2006 in the proceedings of ECOS’06, Aghia Pelagia, Crete, Greece.Keywords : quantum mechanics, thermodynamics, graduate level teaching, non statistical paradigm of physics and thermodynamics, unified quantum theory of mechanics and thermodynamics