# LC Circuit **Resonant Charging Choke** (C) in series with **Excitor-array** (E1/E2) forms an **inductor-capacitor circuit** (LC) since the **Excitor-Array** (ER) acts or performs as an capacitor during pulsing operations, as illustrated in Figure (1-2) as to Figure (1-1).
Figure (1-2) [![image-1703011673363.png](https://stanslegacy.com/uploads/images/gallery/2023-12/scaled-1680-/VzsK8hdVflGHQSyd-image-1703011673363.png)](https://stanslegacy.com/uploads/images/gallery/2023-12/VzsK8hdVflGHQSyd-image-1703011673363.png) Figure (1-1) [![image-1703011664617.png](https://stanslegacy.com/uploads/images/gallery/2023-12/scaled-1680-/qhtqz9LzDjg4722f-image-1703011664617.png)](https://stanslegacy.com/uploads/images/gallery/2023-12/qhtqz9LzDjg4722f-image-1703011664617.png)
The **Dielectric Properties** (*insulator to the flow of amps*) of natural water (*dielectric constant being 78.54 @ 25c*) between the **electrical plates** (E1/E2) forms the **capacitor** (ER). Water now becomes part of the **Voltage Intensifier Circuit** in the form of "**resistance**" between electrical ground and pulse- frequency positive-potential

... helping to prevent electron flow within the **pulsing circuit** (AA) of Figure 1-1.

[![image-1703011664617.png](https://stanslegacy.com/uploads/images/gallery/2023-12/scaled-1680-/qhtqz9LzDjg4722f-image-1703011664617.png)](https://stanslegacy.com/uploads/images/gallery/2023-12/qhtqz9LzDjg4722f-image-1703011664617.png) The **Inductor** (C) takes on or becomes an **Modulator Inductor** which steps up an oscillation of an given charging frequency with the effective capacitance of an pulse-forming network in order to charge the **voltage zones** (E1/E2) to an higher potential beyond applied voltage input. The **Inductance** (C) and **Capacitance** (ER) properties of the LC circuit is therefore "**tuned**" to resonance at a certain frequency.

The Resonant Frequency can be raised or lowered by changing the inductance and/or the capacitance values.

The established **resonant frequency** is, of course, independent of voltage amplitude, as illustrated in Figure (1-3) as to Figure (1-4).

Figure (1-3) [![image-1703011682305.png](https://stanslegacy.com/uploads/images/gallery/2023-12/scaled-1680-/KS1IdCNzwsPJRslu-image-1703011682305.png)](https://stanslegacy.com/uploads/images/gallery/2023-12/KS1IdCNzwsPJRslu-image-1703011682305.png) Figure (1-4) [![image-1703011690241.png](https://stanslegacy.com/uploads/images/gallery/2023-12/scaled-1680-/BVSJKDz1yh7YR7m9-image-1703011690241.png)](https://stanslegacy.com/uploads/images/gallery/2023-12/BVSJKDz1yh7YR7m9-image-1703011690241.png)
The value of the **Inductor** (C), the value of the **capacitor** (ER), and the pulse-frequency of the voltage being applied across the LC circuit determines the impedance of the LC circuit.

The impedance of an inductor and a capacitor in series, Z series is given by (Eq 1)

[![image-1703012652433.png](https://stanslegacy.com/uploads/images/gallery/2023-12/scaled-1680-/5kijCBV9DAnEaHJ7-image-1703012652433.png)](https://stanslegacy.com/uploads/images/gallery/2023-12/5kijCBV9DAnEaHJ7-image-1703012652433.png) Where: [![image-1703012669666.png](https://stanslegacy.com/uploads/images/gallery/2023-12/scaled-1680-/WGRmcuSIYoItCgHP-image-1703012669666.png)](https://stanslegacy.com/uploads/images/gallery/2023-12/WGRmcuSIYoItCgHP-image-1703012669666.png)

The Resonant Frequency (F) of an LC circuit in series is given by (Eq 4)

[![image-1703012692611.png](https://stanslegacy.com/uploads/images/gallery/2023-12/scaled-1680-/OG0MPPsrNVExMFqI-image-1703012692611.png)](https://stanslegacy.com/uploads/images/gallery/2023-12/OG0MPPsrNVExMFqI-image-1703012692611.png)

Ohm's Law for LC circuit in series is given by:

[![image-1703012708035.png](https://stanslegacy.com/uploads/images/gallery/2023-12/scaled-1680-/YlXMelnpzpt0EBZg-image-1703012708035.png)](https://stanslegacy.com/uploads/images/gallery/2023-12/YlXMelnpzpt0EBZg-image-1703012708035.png)