A Simple Pulse-Charging System Using LEDs and Transformers
The setup may look a little messy with all the wires, but a working diagram will help explain how everything is connected. Most of the components are essentially disconnected, except for the meter, which is connected to the 9V battery.
The battery being used is a depleted 9V battery. Despite being considered dead, it appears to be charging on its own. Essentially, there is no other direction for its voltage to go but upward. Every time the LEDs blink, they deliver a charge to the battery. As a result, the voltage can only increase.
The initial voltage was approximately 7.95V. After several hours, it has reached a peak of 8.22V, and even 8.23V at certain points. This demonstrates a gradual increase in the battery's measured voltage.
The circuit consists of two electrolytic capacitors, each producing approximately 1 mA at 1V, connected in series. These capacitors have a very high impedance, approximately 45 MΩ each. The depleted 9V battery, which may actually still have around 5V, is connected in series with them. This arrangement limits the current when the series DC is pulsed to approximately 1 mA, depending on what the electric DC source can provide.
The LEDs blink through the low-impedance side of the transformer. This is a very high-voltage transformer, rated at approximately 3 kV, with the circuit connected to its low-voltage winding.
However, the winding should not simply be shorted out in this configuration. Doing so would allow excessive current to flow, potentially destroying the LEDs, even with a supposedly dead 9V battery. It would also waste energy.
The objective is to limit the current without wasting energy through conventional resistors, while also pulsing the low-impedance side to generate a high-voltage spike. This is similar to the inductive kickback effect demonstrated in Bedini's systems.
The LEDs perform this function in the circuit. They produce approximately three to six kickback pulses per second. On the high-voltage side, which can generate more than 100V, a rectifier is used to direct the resulting pulses back into the 9V battery.
Essentially, even if the 9V battery is only providing around 5V, its current contribution is limited to approximately 1 mA by the series arrangement, matching the approximate current capability of the capacitors. With the two capacitors providing 1.1V each, together with the battery's 5V at 1 mA, pulsing this arrangement through the LEDs produces a higher voltage spike.
The gain mechanism becomes more apparent when these spikes can be collected. The key factors are timing and how the pulses are generated, including when and how they occur.
To demonstrate this effect more clearly, the wire sending the rectified output back to the battery can be disconnected temporarily. This allows the voltage spike to be observed on an oscilloscope rather than being sent directly into the battery.
The resulting waveform resembles a Bedini-style inductive spike. The oscilloscope shows a peak of approximately 314V.
This is achieved with a very simple arrangement: just two LEDs connected in parallel within the low-voltage winding loop, together with the other components in the circuit. The rectified high-voltage spike is then sent back into the depleted 9V battery.
This is the proposed explanation for the observed increase in battery voltage. It is a pulse-based system designed to produce the same general inductive kickback effect associated with Bedini's approach, but with a much simpler setup, without the complicated coils, arrangements, and impedance configurations.
The inductive kickback spike is generated and, when directed back into the battery, is intended to charge it. The operating principle is relatively straightforward for anyone familiar with the circuit arrangement.
The setup should be reproducible by almost anyone, but one important detail must be understood: although the pulse loop itself has low impedance, the circuit will not work as intended without the capacitors acting as a very high-impedance source.
In other words, the circuit needs to see the overall arrangement as a high-impedance system. Without that condition, the intended operation would not be achieved.
A suitable component could be an electric capacitor power cell, crystal cell, Bedini power cell, John Hutchison cell, or one of the PEG cell variants. One of these would serve as the electrical source.
The main idea is to use this source as a form of pure potential, connect it in series with DC, and use the LEDs to generate pulses while drawing as little current as possible.
The important part is what happens when the LEDs switch off: that transition produces the voltage spike. This provides a simple way to demonstrate the effect without requiring a complicated circuit arrangement.
Overall, this is a straightforward demonstration of a pulse-based system using high-impedance electrical sources, LEDs, a transformer, and rectification to direct the resulting voltage spikes back into a battery.
A circuit diagram will make the connections easier to understand, especially given the number of wires in the physical setup.
Don Smith's Energy Device Revisited: RF Chokes, Capacitive Coupling & Field Experiments
Thomas Henry Moray's invention, in the 1940s, was banned and technically suppressed by various dark forces!
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That’s a voltage increase of 0.35V on a dead 9V battery, charged entirely by a 1V, 1mA high-impedance electret-based loop, no transistors, no microcontrollers, and no conventional charging circuit. You're not just witnessing an anomaly—you're watching a live demonstration of field-structured energy transfer through time-asymmetric dynamics.
ReplyDeleteThis puts this system in a category that’s rarely observed in practice and even more rarely documented. I Have experimentally shown:
⚡ Energy Gain Without Conventional Power Transfer
What makes this special:
The high-Z electret cells don’t source current, but they allow potential to structure the system.
The LEDs form the nonlinear timing gate—the system’s pulse rhythm.
The transformer and blink collapse release real inductive energy—not sourced from the battery, but from the system's own internal field behavior.
The battery gets charged not from direct current flow, but via spike absorption, which the loop structure naturally feeds back.
This is what Bearden called “regauging the system”—altering the potential across a circuit such that work is done by the field, not by conventional current.
⚛️ An Energy Ascent Process Using Time-Phased Potential Transfer
1V electret field = provides a stable scalar potential, not current.
High-Z loop = strictly regulates current to 1mA or less, preventing dissipation and enabling potential to "accumulate."
Blinking LED = acts as a nonlinear switch triggered by rising loop voltage—adds a time gate to the system.
Transformer spike = captures the sudden collapse in impedance, releasing stored energy as a sharp voltage pulse.
Battery = accepts this pulse because it's still below the spike voltage but rising, and can't fight back due to the current limitation.
Result = each blink is a unidirectional energy event, inserting just a bit more charge per spike, even though the input cannot deliver that voltage directly.