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    • Home
    • About Edwin Gray
    • Youtube Links
    • RDC Theory
    • Equations & Derivations
    • Prototype Builds
    • RDC Applications
  • Home
  • About Edwin Gray
  • Youtube Links
  • RDC Theory
  • Equations & Derivations
  • Prototype Builds
  • RDC Applications

Understanding Radiant Displacement Current (RDC)

 

RDC uses displacement current – a changing electric field – from quick high-voltage pulses in a conversion tube. This turns regular DC into "cold" electricity: efficient, low heat, no shock. Tube (tungsten rods, copper meshes) gets 3kV pulses (>500 V/ns rise, 3ns width), making displacement dominant (ratio 2.95e12). Efficiency: η = η_t / (1 - r η_t), r=0.27. Applications: Wireless transfer, cold plasma, fusion aid, propulsion. Differs from steady DC: transients vs. constant flow (cold/efficient vs. hot/lossy).


 

Edwin Gray's conversion tube: High-voltage (3kV) pulses applied to tungsten high anode, low-voltage pulses to low anode, with copper mesh grids capturing output. Rapid dV/dt (>500 V/ns, 3ns width) creates displacement current dominance, converting conduction to "cold" electricity for efficient load powering and recovery.

RDC Efficiency Formula

 

Efficiency formula η = η_t / (1 - r η_t), where η_t is tube efficiency, r=0.27 recovery ratio.

Derivation:

Let E_c = capacitor input energy.

Output to load = η_t E_c.

Recovered = r × output = r η_t E_c.

Net input E_net = E_c - recovered = E_c (1 - r η_t).

Overall η = output / E_net = (η_t E_c) / [E_c (1 - r η_t)] = η_t / (1 - r η_t).

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