Thermoelectric Power Generation - Utilising Metals and their Carbide Alloys

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Benefits of Coherence and Decoherence of Metal

Coherent metal is

• Unstretched metal - i.e. non-malleated and non-ducted metal

• Slowly cooled metal - generally cooled in a higher temperature atmosphere, just above the molten metal temperature and very low pressure (partial vacuum - or under reverse air compressor influence). This is known as Warm-Forming.

• To achieve warm-forming efficiently, first apply as much reverse air pressure at higher temperature than the molten metal as possible. That will prevent a solid surface from forming too early while extracting bubbles of volatile gases and vapours - possibly including ablated solids.

• More thermoelectrically conductive than decoherent metal. That implies that the conductivity of heat and of electric flux are confluent.

• Lower in carbon alloy than decoherent metals. Once the chemical threshold of carbon lattice ratio has passed from 4+ valency to 4-, it shifts from behaving as a metal to behaving as a dielectric.

Decoherent metal is the alternatively describe metal configuration. That includes molten metal being deliberately , micro-partitioned, at the lattice level, by the inclusion of near-dielectric levels of carbon. Once dielectric levels are achieved, geometric lattice integrity lowers to amorphous lattice of a covalent compound.

A thermocouple is a pair of metals - one coherent and the other decoherent, and connected by a coherent conductor or standard or quantum induction. They form the basis of thermoelectric power generation when in the presence of heat. The entire circuit will always be at a heat differential to the exterior environment. It is the heat differential which generates electric flux. The charge carrier field will build in capacitance from higher electric field presence to the lower presence - from more decoherent (electric hole carrier rich) side to the electric charge carrier side when the exterior is at a higher temperature. The charge field rich area will reflect photons more easily than the hole field area which will accept photons and convert them to the electric field more than the alternative area. The reverse will occur for lower environmental temperature.

For greatest thermoelectric effect the decoherent metal must be as thinly distributed as possible - i.e with the highest surface area to volume or diameter ratio and a greater material length. The coherent portion must have the highest possible diameter to length ratio of the material.

Placing either side of the thermocouple in two independent sets of closed environments where each can open to the environmental temperature while leaving the other enclosed, and vice versa, for temperature differential switches or heat ratio inversions. Double opening and closing well insulated vents is the best methodology to achieve this. Powerful convection requires an upper and well separated lower vent for maximum, natural Bernoulli air flow. Rabbit warrens exist and thrive on that air flow dynamic. The coherent side would always be exposed to higher temperature environment, and vice versa. That indoor or outdoor exposure may alter given atmospheric changes outside.

One already very coherent metal and one already very decoherent metal gains the best advantage. One pairing which I would suggest respectively, is coherent Copper and decoherent Aluminium or Aluminium Carbide.

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