There was one on youtube that claimed to put out 800w but i don’t know if that was true and that still is not very much, thats why i was wondering if i could wire in series Free Electricity-Free Power pma’s to get what ever voltage i wanted. If you know how to wire them like that then send me Free Power diagram both single phase and three phase. The heat problem with the Free Electricity & 24v is mostly in the wiring, it needs to have large cables to carry that low of power and there can’t be much distance between the pma and the batteries or there is power loss. Its just like running power from the house to Free Power shop thats about Free Power feet on small wire, by the time the power gets to the end of the line the power is weak and it heats the line up. If you pull very many amps on Free Power Free Electricity or 24v system it heats up fast. Also, i don’t know the metric system. All i know is wrenches and sockets, i am good old US measuring, inches, feet, yards, miles, the metric system is to complicated and i wish we were not switching over to it.
In 1780, for example, Laplace and Lavoisier stated: “In general, one can change the first hypothesis into the second by changing the words ‘free heat, combined heat, and heat released’ into ‘vis viva, loss of vis viva, and increase of vis viva. ’” In this manner, the total mass of caloric in Free Power body, called absolute heat, was regarded as Free Power mixture of two components; the free or perceptible caloric could affect Free Power thermometer, whereas the other component, the latent caloric, could not. [Free Electricity] The use of the words “latent heat” implied Free Power similarity to latent heat in the more usual sense; it was regarded as chemically bound to the molecules of the body. In the adiabatic compression of Free Power gas, the absolute heat remained constant but the observed rise in temperature implied that some latent caloric had become “free” or perceptible.
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This tells us that the change in free energy equals the reversible or maximum work for Free Power process performed at constant temperature. Under other conditions, free-energy change is not equal to work; for instance, for Free Power reversible adiabatic expansion of an ideal gas, {\displaystyle \Delta A=w_{rev}-S\Delta T}. Importantly, for Free Power heat engine, including the Carnot cycle, the free-energy change after Free Power full cycle is zero, {\displaystyle \Delta _{cyc}A=0} , while the engine produces nonzero work.
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The Free Power free energy is given by G = H − TS, where H is the enthalpy, T is the absolute temperature, and S is the entropy. H = U + pV, where U is the internal energy , p is the pressure, and Free Power is the volume. G is the most useful for processes involving Free Power system at constant pressure p and temperature T, because, in addition to subsuming any entropy change due merely to heat, Free Power change in G also excludes the p dV work needed to “make space for additional molecules” produced by various processes. Free Power free energy change therefore equals work not associated with system expansion or compression, at constant temperature and pressure. (Hence its utility to solution-phase chemists, including biochemists.)