Feed: Dr. Myron Evans
Posted on: Friday, May 20, 2011 2:45 AM
Author: metric345
Subject: 183(2): Details of Resonant Dissociation
| These are details of resonant dissociation by circularly polarized light when a molecule contains a permanent electric dipole moment. This type of torque is animated in the award winning Evans / Pelkie animation of the early nineties on this site. The animation was produced from computer simulation code and shows the spinning effect very clearly. The extra ingredient in UFT 183 is Euler Bernoulli resonance defined by condition (27), when an angular frequency of the light is tuned to a characteristic angular frequency of a catalyst in a nanometre mould. In hydrocarbons the permanent electric and magnetic dipole moments are usually small, but there is a B(3) mechanism of resonance which will be developed in the next note. The B(3) mechanism induces a magnetic dipole moment in the inverse Faraday effect, and there is a torque between the induced magnetic dipole moment and the B(1) = B(2)* magnetic field of the circularly polarized light. I computer simulated this type of torque at the University of Zurich in the early nineties on the ETH IBM 3090 supercomputer (see Omnia Opera). Light contains many frequencies, so there are many resonance frequencies. More generally there will be a Langevin friction term (and a continued fraction of memory functions) and stochastic torque, giving a planar itinerant oscillator theory and barrier crossing theory. However this simple frictionless theory without stochastic torque is enough to show clearly how light can dissociate waste oil hydrocarbon structures in the Kurata / B(3) mechanism. The dissociated fragments are then recombined using controlling catalysts to give useful products such as clean burning diesel. In hydrocarbons the whole process is controlled by B(3), the spin carrier.
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