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) 

 

 

 

 Figure (1-1) 

 

 

 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. 

 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) 

 

 

 

 Figure (1-4) 

 

 

 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) 

 

 Where: 

 

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

 

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