Kinetic Theory of Aether Particles

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Chapter 2 Kinetic Theory of Aether Particles 2.1 Basic Concepts and Assumptions This chapter will derive energy density and pressure from particles collision on a surface based on kinetic theory. Kinetic theory considers only collision motion of aether particles. The root-mean-square of collision speed v c will be shown to be almost constant in the universe and is proportional to the speed of light c. Fig.2.1 Mechanics of Aether Particles The basic concepts and assumptions are summarized as follows: 1. In a mechanical aether model, an aether particle has two basic microscopic motions that: (1) moving in straight line and (2) spin about its center. The straight line movement will hit or collide with another particle. 53

54 CHAPTER 2. KINETIC THEORY OF AETHER PARTICLES 2. Both colliding and spin motions are represented by vectors to show the directions and the magnitudes of the motions. 3. The directions and the magnitudes of both colliding and spin motions will change after each collision. 4. The directions of both colliding and spin motions point to random directions in space. The magnitudes of the velocities of both colliding and spin motions are Maxwell s distributed. Fig.2.2 Translational Motions of Aether Particles Fig.2.3 Rotational Motions of Aether Particles

2.2. ENERGY DENSITY OF A SINGLE AETHER PARTICLE 55 2.2 Energy Density of a Single Aether Particle In classical mechanics, any moving particle with mass and which occupies a volume in space has mass density and energy density. When this moving particle collides into a surface, this collision produces a pressure on the surface. This section discusses the mass density, energy density, and collision pressure of a single perfect elastic aether particle. Kinetic energy of one particle moving at a constant speed is shown below. where K a 1 2 m av 2 ca (2.1) K a is kinetic energy of one particle, m a is mass of one particle, v ca is collision speed of one particle. Note that, the subscript c in v ca represents collision and a in v ca represents one particle. Fig.2.4 One Particle inside a Sphere Assume this particle is moving inside a spherical ball with a radius R a as shown in Fig.2.4. Aether energy density is calculated from dividing kinetic energy by the volume occupied by this particle. where E K a = 1 m a vca 2 = 1 V a 2 V a 2 ρv2 ca (2.2) V a is volume occupied by a particle, ρ is mass density, E is energy density of particles with constant collision speed.

56 CHAPTER 2. KINETIC THEORY OF AETHER PARTICLES 2.3 Pressure due to a Single Aether Particle We assume this single particle always passes through the center of the ball and collides into the wall of the ball without energy loss. Since it is elastic collision, the momentum change of collision is two times that of its momentum, 2m a v ca. The reaction force on the wall can be determined by the conservation of momentum as shown below. F a = (m av ca ) t = 2m av ca 2R a v ca = m av2 ca R a (2.3) The average aether pressure of particles can be calculated from dividing collision force by the total surface area as p = F a 4πR 2 a = m a v 2 ca R a 4πR 2 a = m av 2 ca 4πR 3 a (2.4) where p is pressure from collision of particles, F a is collision force on the wall, t is the duration between two adjacent collisions, R a is radius of the spherical ball occupied by one particle. Fig.2.5 Pressure Due to a Single Particle

2.4. ROOT-MEAN-SQUARE OF COLLISION SPEED 57 get Replace mass with mass density in Eq.(2.4) and note that V a = 4πR3 a 3 to 2.4 Root-Mean-Square of Collision Speed p = m av 2 ca 3V a = 1 3 ρv2 ca (2.5) Based on constant mass m a and constant collision speed v ca, energy density E and pressure p are calculated for a single aether particle in the previous section. Since both energy density E and collision pressure p are proportional to the square of collision speed v 2 c when mass density ρ is constant, average energy density E avg and average collision pressure p are proportional to the square of root-mean-square of speed as Where E avg = 1 n [ n i=1 ] [ 1 2 ρv2 ci = 12 ρ 1 n n i=1 v 2 ci ] = 1 2 ρv2 c rms (2.6) E avg : Average energy density, n : Number of particles, ρ : Mass density, v ci : Collision speed of particle i, v c rms : Root-mean-square of collision speed. v c rms = 1 n n vci 2 (2.7) i=1 The same arguments hold for collision pressure. [ n ] [ ] p avg = 1 1 n 3 ρv2 ci = 13 ρ 1 n vci 2 = 1 n 3 ρv2 c rms (2.8) i=1 i=1 2.5 Maxwell s Distribution of Collision Speed Assume every aether particle has the same mass and moves randomly in all directions. Furthermore, assume that the collision speed of aether particles

58 CHAPTER 2. KINETIC THEORY OF AETHER PARTICLES follows Maxwell s speed distribution as ψ(v) = 4v2 πˆv 3 c e v2 /ˆv 2 c (2.9) where ψ(v) is Maxwell s speed distribution, ˆv c is collision speed at maximum probability. The root-mean-square speed of a group of particles is shown below to be linearly related to the particle collision speed at its maximum probability ˆv c. Note that speed v c without hat represents root-mean-square (RMS) speed, and with hat represents the maximum probability speed of Maxwell s distribution. Therefore, the RMS speed of Maxwell s distributed collision speed can be written as v 2 c 0 v 2 ψ(v)dv = 3 2 ˆv2 c (2.10) Therefore, aether energy density is E = 1 2 ρv2 c = 3 4 ρˆv2 c (2.11) Similarly, aether pressure is p = 1 3 ρv2 c = 1 2 ρˆv2 c (2.12) Both aether energy density and pressure are linearly related to aether mass density and collision speed square at maximum probability as shown in Eq.(2.11) and Eq.(2.12), and aether pressure can be expressed in terms of aether energy as p = 2 3 E (2.13)

2.6. IDEAL GAS FORMULA 59 Fig.2.6 Maxwell s Distributed Collision Speed and Spin Speed 2.6 Ideal Gas Formula Fig.2.7 Pressure Due to Multiple Particles Ideal gas formula can be derived from Eq.(2.14), for n mole gas by replace mass density with mass and volume occupied by n mole gas as p = 1 m 3 V v2 c = 1 3 nn A m a vc 2 (2.14) V

60 CHAPTER 2. KINETIC THEORY OF AETHER PARTICLES where n is number of mole of gas, N A is Avogadro constant represent the number of particles (molecules) per mole, m is total mass of n mole gas(= nn A m a ), V is total volume occupied by n mole gas. Rewrite Eq.(2.12) to get pv = n( N Am a v 2 c 3 ) (2.15) N Am av 2 c 3 is proportional to total kinetic energy of gas. Also, temperature is proportional to the total kinetic energy. Therefore, Eq.(2.15) can be written as the ideal gas formula by transferring kinetic energy into temperature through gas constant R. R = N Am a v 2 c 3T (2.16) Substitute Eq.(2.16) into Eq.(2.15) to get pv = nrt (2.17) Even though Eq.(2.17) and Eq.(2.12) have the same meaning in physics, Eq.(2.17) relates pressure with temperature while Eq.(2.12) relates pressure with particle collision speed. 2.7 Mass Density and Root-Mean-Square Speed To consider the energy of the spin particles, assume that the spin energy is proportional to the colliding energy. The ratio of spin energy to colliding energy is (α 1), where α >= 1. And the total energy will be modified by an α factor. The energy density and collision pressure had been shown to be related to mass density ρ and root-mean-square speed v c as E = α 2 ρv2 c (2.18) p = 1 3 ρv2 c (2.19) p = 1 3α E (2.20)

2.7. MASS DENSITY AND ROOT-MEAN-SQUARE SPEED 61 Where v c is root-mean-square speed of randomly distributed collision speed of aether particles. Fig.2.8 Kinetic Energy of a Single Particle including Spin Energy Fig.2.9 Kinetic Energy of Multiple Particles including Spin Energy The root-mean-square speed v c and mass density ρ are functions of position and time as v c (x, y, z, t) (2.21) ρ(x, y, z, t) (2.22)

62 CHAPTER 2. KINETIC THEORY OF AETHER PARTICLES Therefore, energy density E and collision pressure p are also functions of position and time as E(x, y, z, t) (2.23) p(x, y, z, t) (2.24) Since all of energy density E, collision pressure p, root-mean-square speed v c and mass density ρ are functions of position and time, all of them can be called fields. Fig.2.10 Relationship between Pressure and Energy Density Fig.2.11 Relationship between Energy Density and Mass Density