“Energy for Free” in Resonance Electrical Circuits
In this work, we introduce a resonance electrical circuit producing effectively a power, [Formula: see text], much greater than the PSU power, [Formula: see text], that operates it; the additional energy is attributed to the entropic effect of the spins of electrons in the circuit wires, that is reg...
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| Format: | Article |
| Language: | English |
| Published: |
World Scientific Publishing
2024-01-01
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| Series: | Reports in Advances of Physical Sciences |
| Subjects: | |
| Online Access: | https://www.worldscientific.com/doi/10.1142/S2424942424500129 |
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| Summary: | In this work, we introduce a resonance electrical circuit producing effectively a power, [Formula: see text], much greater than the PSU power, [Formula: see text], that operates it; the additional energy is attributed to the entropic effect of the spins of electrons in the circuit wires, that is regenerated during the resonance and the PSU cycles. (The PSU is the commercial neon sign driver operating at 30[Formula: see text]kHz.) The application (for example, a train of LED bulbs) is placed in between the two ends of the electrical resonance part of the circuit; the circuit can power many more light bulbs than just the PSU can. The reason that the coefficient of performance (COP), COP [Formula: see text]/[Formula: see text], is larger than 1 is that the electrical signal is in a resonance that does not decay at all at the PSU frequency f of 30[Formula: see text]kHz. This behavior is a function of [Formula: see text] and [Formula: see text]; it complements and is independent of the spark gap grounding circuits. A 40-W PSU can power through the circuit 30 LED bulbs in a series, each of 12[Formula: see text]W, and so COP ≤ 9. The circuit can power a controller module, and a step-down transformer. The performance scales with [Formula: see text], is weak for the 25-W PSU and improves with the increase in [Formula: see text]. Yet, also, increasing [Formula: see text] effectively increases both A and V (V for volts and A for amperage) and keeping A low masks the full power of the effect. We derive the formula for the additional energy [Formula: see text], [Formula: see text], with coefficients that might also depend on [Formula: see text] and V, introducing nonlinear effects. |
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| ISSN: | 2424-9424 2529-752X |