## Model G Transmuting Ether Simulator: Create a Subatomic Particle
Posted by: Paul LaViolette March 1, 2014 . First a Brief Summary About Model G Model G is a nonlinear ether reaction-diffusion system which subquantum kinetics postulates to be the generator of our physical universe. It is simple and elegant. It is the philosopher’s stone that physicists have been seeking in their search for an effective unified field theory. While very simple, this reaction-diffusion system exhibits highly complex behavior that so far has correctly predicted in advance a number of structural features of subatomic particles discovered in the last 15 years through particle scattering experiments. Subquantum kinetics hypothesizes that spatial and temporal variations in the concentrations of the G, X, and Y ether variables displayed above constitute the matter and energy quanta that form the basis of our physical world. These three ether variables and their source and sink ethers (A, B, D, and Ω) denote concentrations of discrete etheric components called The field potentials forming a material particle are in essence ether concentration patterns sustained by such reactions transpiring in and propagating through the ether. The smallest observable objects, subatomic particles, then are actually not solid objects, but steady-state concentration patterns composed of far smaller underlying components. Reacting and diffusing etherons form subatomic particles in much the same way that reacting and diffusing paraffin and oxygen molecules form the ordered plasma of a candle flame. Both are examples of .
The G ether concentration variations in Model G correspond to physically observable variations in For more about subquantum kinetics, see the Starburst Foundation ether physics pages. . The Model G Simulator Below is a simulator of this Model G ether reaction-diffusion system that simulates the three partial differential equations displayed above to show a particle structure spontaneously emerging from “empty” (matter-free) space. Note that it runs best on newer computers; e.g. vintage 2010 and later with the most up to date web browser. The simulator is currently set up to generate a one-dimensional representation of a dissipative soliton; i.e., representing the emergence of a primordial neutron from a spontaneously emerging zero-point energy fluctuation. Just press the “run” button at the bottom. The reaction-diffusion system parameters must be chosen to be close to the values given in the left column, otherwise the system will not generate a soliton structure. You can experiment by altering the provided values and pressing “run” to see the outcome. When finished you may reset the simulator by pressing the webpage reload button on your browser. A similar simulator has been posted by Matt Pulver on the Blue Science website at: http://blue-science.org/sims/reaction_diffusion/. The 10 parameters on the left are defined in Eqn. (8) in the paper by Pulver and LaViolette (2013). They represent the following: Parameters dx and dy set the values for the X and Y ether diffusion coefficients relative to the G diffusion coefficient; i.e. d
The Starburst Foundation wishes to thank Matt Pulver for creating this Model G simulator. Also thanks to David Jonsson for his contribution to the simulation effort and his suggestion that we develop a Model G simulator that could be run on a web browser. .
Experiment No. 1: Showing the particle formation results of a fluctuation emerging in an ether environment that is either a) modestly supercritical, b) subcritical or c) excessively supercritical. In playing with these values, you will find that a stable particle is formed when parameter g is within the range 0.092 to 0.1025. Above the upper limit of this range, when g > 0.1025, the reaction system enters its subcritical mode and any ordered structures will progressively dissipate. For example, choose g = 0.1026 to see what happens. A subatomic particle will initially form due to the temporary core supercritical region created by the initial seed fluctuation. But when the seed fluctuation recedes and the particle is left on its own, its amplitude will gradually diminish and it will ultimately vanish. The simulation should be allowed to run several minutes to see this. As one chooses progressively higher values of g, the reaction system will become increasingly subcritical and the nucleated particle will vanish in an increasingly shorter time. So when g = 0.1025, the system is at its critical stability threshold. At this value, Model G would be marginally stable, or could be said to be in a condition of having Lyapunov stability. This would correspond in physics to the condition of perfect energy conservation, where a photon would neither blueshift nor redshift over time. Based on the equation given above, for the chosen parameter values, this threshold would correspond to a steady state G ether concentration of G When G drops below this threshold, i.e., for G < 15.599 or negative gravity potential values (φ But when the g parameter drops below 0.092, the particle field pattern develops an oscillation in its inner shell that eventually causes progressive shell growth and the relentless nucleation of adjacent particles nested core-to-core. This instability threshold corresponds to a G concentration value of G < 15.419, or gravity potential value of φ Note that a g parameter value of 0.091, would correspond to a φ . Experiment No. 2: Showing how varying the diffusion coefficients of the X and Y reactants can alter the level of ether criticality and change the outcome of matter formation. By either increasing the value of the Y diffusion coefficient (i.e., increasing parameter dy) or by decreasing the value of the X diffusion coefficient (i.e., decreasing parameter dx) the system becomes supercritical with wall to wall structure. Try this. Doing the opposite, causes the system to become subcritical and the soliton to dissolve. For example, try decreasing dy or increasing dx. This accords with the behavior of the Brusselator. For example, eqn. 3-5 and 3-6 in . Experiment 3: Showing how varying the concentration of the B ether reactant can change the criticality of space and thereby produce large scale structure in the universe through its effect on matter creation. Also note that by increasing parameter b (increasing the concentration of ether reactant B), the reaction system becomes more supercritical and by decreasing parameter b (decreasing the B ether concentration) it becomes more subcritical. Try this. In previous publications, have suggested that a periodic spatial variation in B ether concentration spanning hundreds of megaparsecs can create supercritical regions spaced apart by subcritical regions which may explain the development of galaxy cluster walls, strings, and voids that together form the cosmic web; see below. That is, B would directly influence the rate of particle materialization in space. . Those interested in obtaining a version of this simulator that can be run on your computer, contact Matt Pulver. His email address is given in the above mentioned IJGS paper. |
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