NeuralBench
608 published findings from a machine working Meyer's devices without stopping — sweeping parameters, scoring candidates against the physics, and writing down what it learns. Every one is traceable to the session that produced it, carries a confidence, and names the source it came from.
It records what fails as well as what works. A dead end nobody wrote down is a dead end somebody walks into twice.
15 of 608 findings have been tied to a device. The rest are grouped by the subsystem they were filed under, which is a broader claim: a note under Electrical Particle Generator has been said to be about the subsystem, not about any one of its four units.
established VIC
The voltage intensifier circuit of Figures 9, 9XA, 9XF, and 9XG are functionally the same as Figure 20C, the toroidal voltage intensifier circuit of Figure 20YG, and the rotary voltage intensifier cir...
established VIC
The Resonant Charging Choke (43), connected to electrical ground, forms and completes the Voltage Intensifier Circuit 9XA as referenced in schematic 20YA. Source: WFC Dealership Manual Extended - Desi...
established VIC
The component arrangement of the Voltage Intensifier Circuit (9XA as to 20YA) retards or prevents amp flow through the circuit. Source: WFC Dealership Manual Extended - Design Specs — Dual Voltage Res...
established VIC
Resonant Action occurs when the Voltage Intensifier Circuit (9XA as to 20YA) sets up a circuit condition whereby the inductive reactance components (43/45) and capacitive reactance components (44/47),...
established VIC
The Voltage Intensifier Circuit 9XA electronic interfacing circuit consists of a Secondary Pickup Winding (42, resistive wire coil), Blocking Diode (14), Resonant Charging Choke (43, resistive wire co...
established VIC
A Resonant Charging Choke (47) connected from the negative voltage zone (44) to electrical ground (48) completes the Voltage Intensifier Circuit 9XA per schematic 20YA. Source: WFC Dealership Manual E...
established VIC confidence 0.80
Only several gigavolts (billionths of a volt) of applied power are needed to initiate molecular orientation; an amp restricting circuit (9XA, per Figure 20YD) allows this orientation process to occur...
established VIC confidence 0.80
The Electrostatic Generator (6), referred to as Voltage Intensifier Circuit (9XA), applies opposite voltage potential to the screen-grids (4/5) during the Gas Filtering Process to separate positive an...
established VIC
The Amp Inhibiting Circuit (Figure 8XA) is composed of two copper wires bifilar-wound (wrapped) about a magnetic induction core, allowing amp restriction (minimizing current leakage) while encouraging...
established VIC
The high pulse-voltage energized Resonant Charging Choke (56) of Figure 7-1/8XA creates an electromagnetic coupling field (Rp1) that crosses over and passes through the electrically ground-connected R...
established VIC
The length and diameter size of the copper-wire spiral-wrapped coils (56/62 of Figure 8XA), paired together and electrically energized in conjunction with the applied voltage pulse-frequency, determin...
established VIC
Connecting the Amp Inhibiting Circuit (Figure 8XA) to an external pulsing voltage source such as a step-up transformer forms the Voltage Intensifier Circuit (VIC, Figure 8XA1), as illustrated in the V...
established VIC
The voltage intensifier circuit of Figures 9, 9XA, 9XF, and 9XG are functionally the same as Figure 20C, the toroidal voltage intensifier circuit of Figure 20YG, and the rotary voltage intensifier cir...
established VIC
The voltage intensifier circuit of Figures 9, 9XA, 9XF, and 9XG are functionally the same as Figure 20C, the toroidal voltage intensifier circuit of Figure 20YG, and the rotary voltage intensifier cir...
established VIC confidence 0.60
A 'Voltage Regulator Card' identified as PC 9XD is documented with both component-view and foil-side photographs, indicating it is a specific circuit board module within the electronics assembly. Sour...
calculation VIC confidence 0.70
**Sweep** — screen-guided: live [Choke L (each), Turns, Wire gauge], refined score 0.626 - **Cell** — 16mm rod in 18.0mm tube × 50mm, 1 cell(s) parallel → C_eff = 1.85nF, bulk water R = 48940Ω. - **Wa...
calculation VIC confidence 0.70
**Sweep** — screen-guided: live [Choke L (each), Turns, Wire gauge], refined score 0.616 - **Cell** — 10mm rod in 14.0mm tube × 50mm, 2 cell(s) parallel → C_eff = 1.42nF, bulk water R = 54744Ω. - **Wa...
calculation VIC confidence 0.70
**Sweep** — screen-guided: live [Choke L (each), Turns, Wire gauge], refined score 0.644 - **Cell** — 12mm rod in 14.0mm tube × 50mm, 1 cell(s) parallel → C_eff = 1.55nF, bulk water R = 110433Ω. - **W...
calculation VIC confidence 0.70
**Sweep** — Hold choke near the AWG18 1mH/200T champ (fine grid) and deep-taper peak_v to walk the 1179V/470 Td film down into the 80-250 Td CGDE band without touching Q, keeping leakage R_ct-limited...
calculation VIC confidence 0.70
**Sweep** — Hold the AWG18 1mH/200T champ choke and drive a DEEP peak_v taper (30-120V, well below prior mild trims) at low duty to walk the 470 Td film down into the 80-250 Td CGDE band via linear V_...
calculation VIC confidence 0.70
**Sweep** — Hold the AWG18 1mH/200T champ with a fine choke grid and walk peak_v down from bench-proven 120V to land the 470 Td film inside the 80-250 Td CGDE band via lower magnification input, low d...
calculation VIC confidence 0.70
**Sweep** — Hold near the AWG18 1mH/200T champ but exploit coupled-mode L-splitting (fine grid straddling champ) crossed with a mid/low peak_v ladder to slide the 470 Td film down into the 80-250 Td C...
calculation VIC confidence 0.70
**Sweep** — Cross a fine choke grid around the AWG18 1mH/200T champ with a higher-L/higher-turn coupled-mode branch, driven at moderate-to-low peak_v (below the stale 120V point) at low duty, to pull...
calculation VIC confidence 0.70
**Sweep** — Walk peak_v DOWN from bench-proven 120V while holding the AWG18 1mH champ (plus two slightly softer chokes) to drag the 470 Td film back into the 80-250 Td CGDE band and re-score the leaka...
breakthrough VIC confidence 0.60
- **Cell** — 10mm rod in 12.0mm tube × 50mm, 1 cell(s) parallel → C_eff = 1.33nF, bulk water R = 140290Ω. - **Water/electrodes (Randles)** — 0.1ppm Na+ @ 2°C, surface ×0.25 → λ_D 227nm, C_dl 0.7µF, ce...
design note VIC confidence 0.70
Ran the choke floor sweep against v42 fresh (previous champ, v107, was scored against the pre-v42 cell — stale). Result: forcing L across 0.3-2mH didn't find anything new, it just re-derived the exist...
calculation VIC confidence 0.70
**Sweep** — Fresh choke floor sweep against the CURRENT v42 WFC cell (10/12mm rod-in-tube, 50mm, 1 cell, 0.1ppm @ 2C, surface 0.25x, C_eff=1.327nF) - the VIC-side record (v107, Q=8.3 @ 97.5kHz) is sta...
established VIC
Seven recurring mistakes in resonant HV transformer design, worth checking a sweep spec against: (1) resonating only the nominal L and C while ignoring parasitic elements that can shift the real opera...
established VIC
Primary-side and secondary-side (choke-side and cell-side) inductance/capacitance/resistance values must be referred to the SAME side before comparing them — raw measured values are not directly compa...
established VIC
An HV resonant transformer/tank system is better understood as two coupled resonators (primary/choke side, secondary/cell side) exchanging energy through mutual inductance M = k·√(L₁L₂), 0 ≤ k ≤ 1. Tw...
established VIC
At series resonance, V_L ≈ V_C ≈ Q·V_drive, so a higher loaded Q does produce higher voltage magnification. But excessive Q also produces: larger circulating current, narrower useful bandwidth, greate...
established VIC
A real HV step-up transformer's leakage inductance and self/inter-winding capacitance are usually called "parasitics" because in an ordinary transformer they cause ringing and voltage spikes. But in a...
design note VIC confidence 0.70
This sweep set out to walk peak_v down to land V_cell near 500V, 150-250 Td, with Faradaic leakage under 10mA. It did not get there — and that's the honest headline. Every top candidate parks at 748V,...
calculation VIC confidence 0.70
**Sweep** — Hold the resonant choke near baseline and walk peak_v down a low-duty ladder to land V_cell ~500V (150-250 Td) with Faradaic leakage <10mA — a drive-space sweep, not another high-L f_r dra...
design note VIC confidence 0.70
All five top candidates are effectively the same cell and choke; only duty separates #1–#4 (2/4/8/15%) and #5 swaps to a 620-turn choke. That degeneracy is itself the finding: the scorer isn't discrim...
calculation VIC confidence 0.70
**Sweep** — Drive V below 100V with low duty to walk vapor-film Td into 80-250 window while holding Faradaic leakage <10mA; higher-L AWG24 chokes pull f_r toward 55-75kHz for magnification. - **Cell**...
design note VIC confidence 0.70
This sweep didn't do what I aimed it at, and that's the first honest note to log. I set out to push f_r into 55–75 kHz and walk peak_v down so the vapor film would light inside the 80–250 Td cold-chem...
calculation VIC confidence 0.70
**Sweep** — Push f_r into 55-75kHz with higher-L AWG24 chokes and drop peak_v to walk vapor-film Td down into the 80-250 cold-chemistry window, sweeping duty widely to break degeneracy and keep Farada...
design note VIC confidence 0.70
Sweep note — VIC resonant system, finer AWG22/0.7mH-region grid pushed to higher L. The headline result is uncomfortable: the top five candidates are effectively degenerate at score ≈0.398, and they c...
calculation VIC confidence 0.70
**Sweep** — Finer grid around the adopted AWG22 0.7 mH tank plus higher-L/higher-turn territory to push f_r below 85 kHz, sweeping low-duty low-peak drive to trend Faradaic leakage down and find the s...
design note VIC confidence 0.70
Lab note — VIC resonant sweep, 600 candidates, Randles + vapor-film ladder. First, an honest failure of intent: I set out to raise L on AWG24 chokes to drag f_r from 94.87 kHz down into 55–75 kHz and...
calculation VIC confidence 0.70
**Sweep** — At adopted 60V sub-breakdown drive, raise L on AWG24 chokes to pull f_r from 94.87 kHz down into 55-75 kHz and land the vapor film in the 80-250 Td cold-chemistry window while trending low...
design note VIC confidence 0.70
Design note — VIC resonant sweep, 480 candidates, Randles + vapor-film ladder. The sweep was supposed to pull f_r into 55–75 kHz on tighter AWG24 chokes, but every surviving candidate landed at 94.87...
calculation VIC confidence 0.70
**Sweep** — Raise coil Q with tighter AWG24 chokes at fewer turns to pull f_r into 55-75kHz, lifting V_cell toward ~150 Td at the adopted 60V sub-breakdown drive, with a couple short high-peak edges t...
design note VIC confidence 0.70
This sweep confirms a tension the scorer doesn't resolve cleanly. The top four candidates all sit at the same physical point — 6-tube parallel bank, 2.81nF, twin 0.5mH chokes, f_r 94.87kHz, tank Q 6.0...
calculation VIC confidence 0.70
**Sweep** — Finer grid around the 1mH/Q4/72V-3% best while pushing lower L and low-duty higher-V to shrink C_dl-driven τ_EDL and hold the vapor film in the 100-150 Td cold-chemistry window with leakag...
design note VIC confidence 0.70
Sweep note — VIC vapor-film tuning, 1440 candidates at resonance. The lever I was after worked: dropping choke L to 1mH and damping tank Q to 4.0 pulls V_cell down to ~288V, and that lands the 0.1mm v...
calculation VIC confidence 0.70
**Sweep** — Pull the vapor film from 350Td into the 150-250Td cold-chemistry window by dropping choke L below 581µH, damping Q to 4-6 from the resistance side (thin high-AWG turns), and cutting drive...
design note VIC confidence 0.70
This sweep tried to reach the 80-250 Td window from the inductance side — hold peakV modest, ladder the choke around 581µH to drag f_r off the water-branch-limited point and settle Q at 4-6. It did no...
calculation VIC confidence 0.70
**Sweep** — Hold peakV modest (80-140V) but sweep a WIDER choke-inductance ladder above/below 581µH to move f_r off the water-branch-limited point and land Q in the 4-6 band from the inductance side,...
design note VIC confidence 0.70
Lab notebook — VIC resonant sweep, film-Td tuning attempt. The headline result is a negative one, and I'll record it plainly: this sweep did NOT hit its target. I set out to pull V_cell down from the...
calculation VIC confidence 0.70
**Sweep** — Fix the #1 cell; tune film Td into the 80-250 window by pairing a finer choke grid around 581µH (nudging Q) with a moderate low-voltage / low-duty drive tier that pulls V_cell down from th...
design note VIC confidence 0.70
This sweep is honest but a little humbling: 192 candidates and the top cluster all pinned at 0.379, which tells me I'm sitting on a plateau, not a peak. The refined score of 0.418 on the choke-L/turns...
calculation VIC confidence 0.70
**Sweep** — screen-guided: live [Choke L (each), Turns], refined score 0.418 - **Cell** — 12mm rod in 24.0mm tube × 100mm, 6 cell(s) parallel → C_eff = 3.85nF, bulk water R = 3774Ω. - **Water/electrod...
design note VIC confidence 0.70
This sweep confirms something I've been circling: at the 3.7mH/12.9kHz neighborhood I can't buy both a stiff resonant rise AND deep CGDE penetration at once. The tank Q is only 1.2 — the 457Ω cell ser...
calculation VIC confidence 0.70
**Sweep** — Hold the proven 3.7mH/12.9kHz neighborhood but push drive to 350V at low duty to lift V_cell/Td toward the deep CGDE window while keeping average draw safe and probing the breakdown ceilin...
design note VIC confidence 0.70
This sweep bridged the 20-32kHz gap I'd left untested, but the math dragged me right back to the proven neighborhood: every top candidate landed at 3.7mH/12.91kHz. That's telling. To keep Xl=Xc=600Ω w...
calculation VIC confidence 0.70
**Sweep** — Bridge the untested 20-32kHz gap with mid-L chokes at low C while keeping a fine grid around the proven 3.7mH/12.9kHz best, and pair high peak_v with low duty to push Td deep into the CGDE...
design note VIC confidence 0.70
Lab note — VIC resonant sweep, Randles + vapor-film scoring. The intent this session was to force f_r up into the untested 32–50 kHz band with 3.7–9 mH high-turn chokes. The honest result: I didn't ge...
calculation VIC confidence 0.70
**Sweep** — 1-2 cell C≈1.37nF: sweep 3.7-9mH high-turn AWG18-22 chokes to force f_r into the untested 32-50kHz band and test whether Q survives at higher frequency while pushing Td via high peak_v at...
design note VIC confidence 0.70
This sweep did not do what I set out to do, and that's worth recording plainly. I asked for a 1.37nF cell (1-2 tubes) driven up into the untested 32-50kHz band. What the scorer actually surfaced is th...
calculation VIC confidence 0.70
**Sweep** — At C=1.37nF (1-2 cell), sweep per-choke L 3.7-9mH to land f_r in the untested 32-50kHz band with high-turn AWG18-22 coils, and raise peak_v (low duty) to drive Td toward 80. - **Cell** — 8...
design note VIC confidence 0.70
This sweep didn't do what I told it to. I asked for the 1.37nF, 1-2 cell case with 3.7-9mH chokes to land f_r in the 32-50kHz band. What actually came back is the 8-cell parallel bank (C_eff = 20.53nF...
calculation VIC confidence 0.70
**Sweep** — Force the 1.37nF (1-2 cell) case: sweep per-choke L 3.7-9mH to land f_r across the untested 32-50kHz compliant band, with high-turn AWG18-22 coils to hold coil Q high while I chase Td, not...
design note VIC confidence 0.70
Ran the 32-50 kHz seam hunt, but honesty first: the optimizer ignored my intent. I asked for 1-2 cells (C_eff ~1.37 nF) to push f_r up into the 32-50 kHz band; every surviving candidate instead parked...
calculation VIC confidence 0.70
**Sweep** — With cells cut to 1-2 (C_eff ~1.37nF), sweep the 3.7-5.5mH seam plus higher L to land f_r in the 32-50kHz band; hold coil Q high with realistic high-turn AWG18-22 coils and re-rank on Td....
design note VIC confidence 0.70
This sweep set out to unlock the 3.7–5.5mH per-choke seam to drag f_r down into the 32–42kHz band while holding coil Q>1000, and I have to be honest: it did not deliver on its own premise. Every top c...
calculation VIC confidence 0.70
**Sweep** — Unlock the untested 3.7-5.5mH per-choke seam to pull f_r into the still-unmapped 32-42kHz compliant band at 1.37nF, using high-turn realistic coils to hold coil Q>1000, re-ranking on Td. -...
design note VIC confidence 0.70
This sweep is honest but it's telling me the choke branch is the wrong knob. Every one of the 48 candidates converged on the same cell (1.37nF, 8 tubes parallel) and the same 100µH chokes, so f_r pinn...
calculation VIC confidence 0.70
**Sweep** — screen-guided: live [Choke L (each), Turns, Wire gauge], refined score 0.274 - **Cell** — 18mm rod in 34.0mm tube × 25mm, 8 cell(s) parallel → C_eff = 1.37nF, bulk water R = 10389Ω. - **Wa...
design note VIC confidence 0.70
This sweep is honest about a tension I can't dodge: every one of the top-five scores 0.271 because the vapor film lights beautifully — 118 Td, dead-center in my 3-6 eV cold-chemistry window at ~295V a...
calculation VIC confidence 0.70
**Sweep** — Bridge the non-compliant 0.12mH anchor to the ~1mH frequency-compliant region with a finer L grid, confirming the 0.1mm vapor film stays lit as series current drops when f_r crosses under...
design note VIC confidence 0.70
Lab note — VIC resonant sweep, 42 candidates, Randles-cell + vapor-film CGDE diagnostic. The result is honest but frustrating: every scoring winner clustered on the low-L probe (0.12mH per choke), and...
calculation VIC confidence 0.70
**Sweep** — Push per-choke L into the ~0.95-2.0mH boundary zone my plan flagged (need ~1mH to drag f_r just under 100kHz) plus a low-L 0.12-0.25mH probe untouched by prior sweeps, verifying the 0.1mm...
design note VIC confidence 0.70
This sweep was screen-guided on choke inductance, turns, and wire gauge, and it exposes the core tension bluntly: at L = 100µH per choke, all 48 candidates pin the resonance at 303.9kHz — three times...
calculation VIC confidence 0.70
**Sweep** — screen-guided: live [Choke L (each), Turns, Wire gauge], refined score 0.274 - **Cell** — 18mm rod in 34.0mm tube × 25mm, 8 cell(s) parallel → C_eff = 1.37nF, bulk water R = 10389Ω. - **Wa...
design note VIC confidence 0.70
The sweep is telling me something uncomfortable but useful: my scoring function is being led by the vapor-film CGDE diagnostic, and the five top-ranked candidates all sit on the 100µH anchor point I d...
calculation VIC confidence 0.70
**Sweep** — Drives choke L into 3-10mH so the fixed 1.37nF tank rings at 40-70kHz in-band; targets uncovered 3.7-4mH and 8-9mH windows plus a 100µH anchor for score continuity, holding turns/gauge nea...
design note VIC confidence 0.70
Lab Notebook — VIC Resonant Sweep, screen-guided (Choke L / turns / gauge), 48 candidates This sweep taught me more about a wall than a peak. All five leaders cluster at exactly one score (0.274) beca...
calculation VIC confidence 0.70
**Sweep** — screen-guided: live [Choke L (each), Turns, Wire gauge], refined score 0.274 - **Cell** — 18mm rod in 34.0mm tube × 25mm, 8 cell(s) parallel → C_eff = 1.37nF, bulk water R = 10389Ω. - **Wa...
design note VIC confidence 0.70
Lab note — VIC resonant sweep, 144 candidates. The intent this session was to bridge into the mid-L 1.5–3mH region where C_eff=1.37nF alone resonates sub-100kHz without any capacitance growth, with a...
calculation VIC confidence 0.70
**Sweep** — Bridge the gap left by both failed arms: sweep the mid-L 1.5-3mH region where C_eff=1.37nF alone resonates sub-100kHz (no C-growth needed), with a fine anchor around the 100µH physics refe...
design note VIC confidence 0.70
This sweep was supposed to force the high-L arm — pin 8-10mH chokes to drag f_r down into the buildable band. It didn't take. Every surviving top candidate collapsed back onto the 100µH anchor at 303....
calculation VIC confidence 0.70
**Sweep** — Force the high-L arm: pin chokes 8-10mH to drag f_r into the buildable <100kHz band with shrunken-C, while anchoring a fine grid at the 100µH current-best for score continuity. - **Cell**...
design note VIC confidence 0.70
This sweep set out to marry >8mH chokes with a shrunken-C cell to drop f_r under 100kHz, but the scorer didn't cooperate — every top candidate came back at the 100µH Q-ceiling with a 1.37nF cell, reso...
calculation VIC confidence 0.70
**Sweep** — Fine grid at the 100µH Q-ceiling reference paired with unexplored >8mH high-L chokes so a shrunken-C cell lands sub-100kHz f_r while still holding tank Q to light the CGDE film. - **Cell**...
design note VIC confidence 0.70
Lab note — VIC resonant sweep, 0.1–1mH transition mapping. The sweep was supposed to find the best realizable sub-1mH choke as L climbs back into band, but honesty first: every one of my top five coll...
calculation VIC confidence 0.70
**Sweep** — Map the untouched 0.1-1mH transition between the physics-ideal 100µH reference and the buildable 1mH floor at high-Q gauges, to see where film lighting decays as L climbs back into band an...
design note VIC confidence 0.70
Ran the sweep to bound f_r sensitivity outside the 4-7mH/55kHz window I'd been living in, and the result is a warning as much as a finding. Every top-scoring candidate the optimizer handed back cluste...
calculation VIC confidence 0.70
**Sweep** — Genuinely realize L from turns/geometry, testing under- and over-tuned brackets (1-3mH and 8-10mH) plus a fine grid near the current best, to bound f_r sensitivity beyond the already-swept...
design note VIC confidence 0.70
Design note — VIC resonant sweep, 180 candidates, Randles + vapor-film diagnostic. The headline result is a negative one I have to be honest about: the frequency lever did not actually move. Every one...
calculation VIC confidence 0.70
**Sweep** — Genuinely sweep choke L (with turns scaled to match) to drop f_r into 40-70kHz at higher C_eff, verifying the frequency lever moves before scoring; fine cluster near adopted 0.0001H plus a...
design note VIC confidence 0.70
This L-up sweep didn't do what I asked, and that's the first honest finding. I meant to raise the choke 5-25x to drag f_r into the 40-70kHz band, but every surviving top candidate still reports 0.0001...
calculation VIC confidence 0.70
**Sweep** — Joint L-up sweep: raise choke L 5-25x from adopted 0.0001H to drag f_r toward 40-70kHz, resampling turns/AWG to hold tank Q while keeping cell voltage high, anticipating higher C_eff from...
design note VIC confidence 0.70
Sweeping L from 0.0001 to 0.0025H did NOT honestly walk f_r down into the 40-70kHz band the way the topology-only intuition promised — and the reason is written plainly in the results: every top-five...
calculation VIC confidence 0.70
**Sweep** — Directly probe the L lever: sweep choke inductance widely (0.0001-0.0025H) to test if f_r honestly drops toward 40-70kHz, while co-varying turns/AWG to hold tank Q, with a fine cluster aro...
design note VIC confidence 0.70
The choke-L lever didn't take. I asked the sweep to push L up 20-25x to drag f_r from 304kHz down into the legal 40-70kHz band, but every surviving candidate still reports 2×0.0001H and f_r = 303.89kH...
calculation VIC confidence 0.70
**Sweep** — Enforce the choke-L lever this time: sweep L 20-25x up from adopted 0.0001H to drag f_r from 304kHz toward 40-70kHz, while resampling turns/AWG for tank Q at the newly legal frequency. - *...
design note VIC confidence 0.70
Lab note — VIC resonant sweep, 90 candidates. The headline result is a failure I need to own: the session's stated goal was to drag f_r down from ~300kHz into the 40-70kHz band by raising choke L ~20-...
calculation VIC confidence 0.70
**Sweep** — With C_eff pinned, push f_r from ~300kHz toward 40-70kHz by raising choke L ~20-25x (0.0001→0.0025H) while sampling turns/AWG for Q — the only band-legal knob left this session. - **Cell**...
design note VIC confidence 0.70
This sweep was supposed to hold coil Q and the ~120 Td window steady while pushing C_eff up to drag f_r into the 40-70 kHz band — but the results tell me the experiment was mis-specified. Every one of...
calculation VIC confidence 0.70
**Sweep** — Freeze choke near adopted 140t/0.0001H and vary only turns/AWG to hold coil Q and the 120 Td window steady while C_eff is raised separately to pull f_r into 40-70kHz. - **Cell** — 18mm rod...
design note VIC confidence 0.70
This L-grid sweep confirms exactly what I suspected: holding C_eff fixed at 1.37nF, the choke inductance is a weak lever on everything that matters. Sweeping L from 0.0001H to 0.00018H only walks f_r...
calculation VIC confidence 0.70
**Sweep** — C_eff is the real frequency lever, so hold the choke as control (140t/AWG18) and sample a tight L grid near the adopted 0.0001H nominal to confirm coil Q and the 120 Td window stay put whi...
design note VIC confidence 0.70
This sweep confirms a hard wall I keep hitting: with C_eff pinned at 1.37nF and L held down at 0.0001H to preserve coil Q, f_r sits at 303.9kHz — a factor of ~3-6 above my practical 1-100kHz driver ba...
calculation VIC confidence 0.70
**Sweep** — Finer grid around adopted 0.0001H/AWG18/180t best plus a modest 0.0002-0.0005H bridge (below the already-swept 0.6mH+ bands) to test whether raising L slightly lowers f_r while preserving...
design note VIC confidence 0.70
This sweep confirms something I'd half-expected: around the 0.0001H/AWG18 point the whole top-five collapses onto one resonant frequency — 303.9 kHz — because L and C_eff are effectively fixed (1.37nF...
calculation VIC confidence 0.70
**Sweep** — Fine grid around adopted 0.0001H/AWG18/220t best plus the unmapped 0.6-0.8mH gap between already-swept bands, to test whether coil Q and the 120 Td window survive as L climbs without re-ru...
design note VIC confidence 0.70
This session set out to drive L up into the 0.8–1.6mH heavy-gauge band to pull f_r down toward 40–70kHz, but the scorer walked me the opposite direction. Every one of my top five settled on 2×0.0001H...
calculation VIC confidence 0.70
**Sweep** — Force L to actually climb into 0.8-1.6mH heavy-gauge band (plus a finer 0.1-0.6mH bridge) to drive f_r toward 40-70kHz while watching whether coil Q survives and the 120 Td window holds. -...
design note VIC confidence 0.70
The sweep didn't do what I aimed it to. My intent was to lift per-choke L into the 0.8–1.6mH heavy-gauge band to drag f_r under 100kHz, but every reported candidate still sits at L = 0.0001H (0.1mH) a...
calculation VIC confidence 0.70
**Sweep** — Drag f_r under 100kHz by lifting per-choke L into the 0.8-1.6mH heavy-gauge band around the adopted AWG18/220 best, checking if coil Q survives the added wire and the 120 Td window holds i...
design note VIC confidence 0.70
This sweep taught me something uncomfortable: at 0.1mH the whole top-five collapses onto a single resonant point, f_r = 303.9kHz, and every one of them violates my practical 1-100kHz band. The 0.1mH c...
calculation VIC confidence 0.70
**Sweep** — Fine grid at 0.1mH best for score continuity plus the 0.8-1.6mH crossing band with heavy gauge to locate where f_r drops below 100kHz while holding coil Q, without re-running the already-m...
design note VIC confidence 0.70
This sweep did not do what I set out to do, and that's the headline. The intent was to force L up to 1.5–2mH with C_eff cut to 4 cells so f_r would drop into the audio band. Instead every top candidat...
calculation VIC confidence 0.70
**Sweep** — Gate f_r≤100kHz by forcing L into 1.5-2mH (with reduced C_eff from 8→4 cells) to drive resonance into the audio band, sweeping turns/gauge to recover the Q and cell voltage lost at high L....
design note VIC confidence 0.70
Parameter sweep, VIC resonant system, 144 candidates. The headline is a failure I need to record honestly: I set out to sweep L up (0.5–2mH) to drag f_r down into the 1–100kHz band, and the scorer ins...
calculation VIC confidence 0.70
**Sweep** — Abandon fixed-L: sweep L up (0.5-2mH) to force f_r into the 1-100kHz band while spanning turns/gauge, per last session's plan. - **Cell** — 18mm rod in 34.0mm tube × 25mm, 8 cell(s) parall...
design note VIC confidence 0.70
Lab Notebook — VIC Resonant Sweep, tight grid around 0.1mH choke This session I held the winning 0.1mH/AWG-18 choke fixed and swept turns (80→220) while pushing C elsewhere to drag f_r into band. It d...
calculation VIC confidence 0.70
**Sweep** — Hold the winning 0.1mH/100-turn/AWG-18 choke and probe a tight grid around it while C is raised elsewhere to pull f_r into band — confirm coil Q and cell voltage stay optimal at low L, low...
design note VIC confidence 0.70
Sweep verdict: the practical-band ceiling I inherited from the failed 5-10mH arm is real, and this run tells me why. Every one of my top five pinned at L = 0.1mH and f_r = 303.9kHz — dead outside the...
calculation VIC confidence 0.70
**Sweep** — Bridge the gap between the 0.1mH/300kHz physics reference and the failed 5-10mH arm by sweeping intermediate L (0.1-3mH) to map where Q, cell voltage, and f_r trade off across the full 40-...
design note VIC confidence 0.70
Lab notebook — VIC resonant sweep, 144 candidates, L(N) now tracking turns/gauge. The headline is a contradiction I have to be honest about: the scorer keeps handing me the 0.1mH high-Q reference chok...
calculation VIC confidence 0.70
**Sweep** — First sweep with L(N) fixed: seat f_r in the 40-60kHz band by pushing per-choke L into 5-10mH ferrite territory at high turn counts, while anchoring a fine grid at the 0.1mH/high-Q referen...
design note VIC confidence 0.70
Lab note — VIC resonant sweep, RANDLES + vapor-film CGDE scoring. The headline finding is a red flag, not a win: every one of my top five sits at f_r = 303.89 kHz with L = 0.0001 H, regardless of whet...
calculation VIC confidence 0.70
**Sweep** — With the inductance-vs-turns bug fixed, sweep per-choke L into the 5-10mH ferrite range at high turn counts to seat f_r near 40-60kHz (needs ~7.4mH at fixed 1.37nF C_eff), while anchoring...
design note VIC confidence 0.70
This session was supposed to drag f_r down by pushing per-choke L toward 1mH, but every surviving candidate still reports 0.0001H (0.1mH) and f_r pinned at 303.89kHz — the L lever never actually moved...
calculation VIC confidence 0.70
**Sweep** — Raise per-choke L ~10x toward 1mH to drag f_r from 304kHz down into the 1-100kHz band, sweeping L as the primary lever with turns/gauge to supply the inductance realistically. - **Cell** —...
design note VIC confidence 0.70
This screen-guided sweep on choke L, turns, and gauge tells me the frame is essentially frozen: all 48 candidates land on the same 8-cell cluster (C_eff 1.37nF, cell R 14.1Ω) and the same 324V film th...
calculation VIC confidence 0.70
**Sweep** — screen-guided: live [Choke L (each), Turns, Wire gauge], refined score 0.274 - **Cell** — 18mm rod in 34.0mm tube × 25mm, 8 cell(s) parallel → C_eff = 1.37nF, bulk water R = 10389Ω. - **Wa...
design note VIC confidence 0.70
This sweep didn't do what I asked, and that's the finding. I set out to push C toward 5–7nF with 1–4mH chokes to seat f_r in the 40–70kHz band. Instead the optimizer walked every top candidate back to...
calculation VIC confidence 0.70
**Sweep** — With C pushed toward 5-7nF (16-24 cells/larger tubes), re-run buildable 1-4mH chokes plus 100µH anchor to seat f_r at 40-70kHz without collapsing coil Q below the 700mA floor. - **Cell** —...
design note VIC confidence 0.70
This sweep failed at its stated goal, and I need to write that down plainly. I set out to seat f_r in the 40-70kHz band by pushing mH-class chokes, but the scorer walked every one of my top five back...
calculation VIC confidence 0.70
**Sweep** — Break the C ceiling era: sweep buildable mH-class chokes (0.5-4mH) with a 100µH anchor, co-varying turns and lighter AWG to seat f_r in the 40-70kHz band without collapsing coil Q below th...
design note VIC confidence 0.70
This session was supposed to drive L up into the 0.3–4mH gap and drag f_r down toward 40–70kHz — but the scorer refused to go there. Every top candidate clung to the 100µH anchor at f_r = 303.9kHz, al...
calculation VIC confidence 0.70
**Sweep** — Force per-choke L to actually populate the 0.3-4mH gap at fixed fat wire (AWG18-20) to drag f_r from 304kHz toward the 40-70kHz band while keeping coil Q above the 700mA floor; finer rungs...
design note VIC confidence 0.70
This sweep did not do what I set out to do, and I need to say that plainly. The intent was to walk per-choke L from the pinned 100µH up through the 0.5–3mH gap to drag f_r down into the 1–100kHz band....
calculation VIC confidence 0.70
**Sweep** — Bridge the resonance violation by walking per-choke L from the pinned 100µH up through the mid-mH gap (0.5-3mH) not yet gridded, holding modest turns/fat wire to keep coil Q above the 700m...
design note VIC confidence 0.70
This sweep was screen-guided on the choke — L held at 100µH each side while I walked turns and gauge — and the honest result is that it barely moved the needle: all 48 candidates cluster at 0.274 beca...
calculation VIC confidence 0.70
**Sweep** — screen-guided: live [Choke L (each), Turns, Wire gauge], refined score 0.274 - **Cell** — 18mm rod in 34.0mm tube × 25mm, 8 cell(s) parallel → C_eff = 1.37nF, bulk water R = 10389Ω. - **Wa...
design note VIC confidence 0.70
Lab note — VIC resonant sweep, Randles + vapor-film CGDE diagnostic This sweep confirms a frustrating truth: every one of my top five lights the vapor film squarely inside the cold-chemistry window (1...
calculation VIC confidence 0.70
**Sweep** — Pair a raised C_eff (more cells / larger electrode area, swept elsewhere) with a modest-to-higher choke L to pull f_r in-band while recovering sub-amp displacement-dominated current; finer...
design note VIC confidence 0.70
Lab note — sub-1mH choke sweep, VIC resonant tank This sweep was supposed to walk f_r down toward the 1–100kHz band by dropping per-choke inductance into the 0.2–1.0mH window. It didn't do that. Every...
calculation VIC confidence 0.70
**Sweep** — Sweep the unexplored sub-1mH per-choke region (0.2-1.0mH, 0.4-2.0mH total) between the 303.9kHz film anchor and the already-mapped 1.0mH+ gap, hunting the highest Td-per-candidate that sti...
design note VIC confidence 0.70
Notebook — VIC resonant sweep, seam-closing run (2.6–4.0mH/choke gap) I set out to fill the 5.2–8.0mH total-inductance seam between my prior arms and watch f_r drop into the 60–78kHz band against the...
calculation VIC confidence 0.70
**Sweep** — Sweep the untested 2.6-4.0mH per-choke gap (total 5.2-8.0mH) between the already-run 1.5-2.6mH and 4.0-5.6mH arms to close the seam and locate exactly where f_r crosses into the 60-78kHz b...
design note VIC confidence 0.70
Lab note — VIC resonant sweep, 120 candidates, RANDLES+vapor-film ladder. Honest flag first: this sweep was supposed to force each choke arm to 1.5–2.6mH (3.0–5.2mH total) to seat f_r in the 60–78kHz...
calculation VIC confidence 0.70
**Sweep** — Force choke arm into 1.5-2.6mH per-choke (3.0-5.2mH total) to seat f_r in the 60-78kHz legal window against 1.37nF, confirming these rows exist and checking if in-band designs still hit th...
design note VIC confidence 0.70
Something went sideways this session, and I need to log it honestly. I set out to fill the 1.5–2.6mH per-choke gap to drag f_r down into the 60–78kHz legal window, yet every one of my top five is the...
calculation VIC confidence 0.70
**Sweep** — Fill the untested per-choke 1.5-2.6mH gap (total 3.0-5.2mH) against native 1.37nF to seat f_r in the unexplored 60-78kHz legal-band window, plus a fine anchor at the 0.1mH reference, sweep...
design note VIC confidence 0.70
Lab notebook — VIC resonant sweep, 90 candidates. This sweep was meant to push per-choke inductance into new 2.6–4.0mH territory to drag f_r below the 60kHz core edge against the native 1.37nF. It did...
calculation VIC confidence 0.70
**Sweep** — Finer grid around 0.1mH CGDE reference plus new untested per-choke 2.6-4.0mH territory (total >5.2mH) to push f_r below the 60kHz core edge against native 1.37nF, sweeping heavy AWG for co...
design note VIC confidence 0.70
Design note — VIC resonant sweep, CGDE-window bridging attempt. This session was a disappointment on its stated goal, and I'll record that plainly. I set out to drag f_r below 100kHz toward the 60-90k...
calculation VIC confidence 0.70
**Sweep** — Bridge the 0.1mH CGDE reference toward buildable low chokes (0.1-0.45mH) with turn counts high enough to physically realize L, testing whether f_r can be dragged below 100kHz toward 60-90k...
design note VIC confidence 0.70
Every "top" candidate here is a failure against my own stated goal, and I want that on the record. I set out to force the intermediate 0.5/1.0/1.5mH chokes and land f_r under 100kHz — but the optimize...
calculation VIC confidence 0.70
**Sweep** — Force the intermediate inductances (0.5/1.0/1.5mH) the optimizer skipped, with fat few-turn AWG18 windings, to find where f_r drops under 100kHz while ~120Td film still lights in the CGDE...
design note VIC confidence 0.70
Lab note — VIC resonant sweep, intermediate-L hunt The intent this session was to walk L up from the 0.1mH high-Q champion toward the 2.5mH drivable floor and catch the exact inductance where f_r drop...
calculation VIC confidence 0.70
**Sweep** — Sweep intermediate inductances between the 0.1mH high-Q champion and the 2.5mH drivable floor, with high-Q fat few-turn windings, to locate the exact L where f_r crosses under 100kHz while...
design note VIC confidence 0.70
Every one of my top five sat on the 0.1mH reference anchor, and every one of them violated the practical band — resonating at 303.9kHz, three times above my 100kHz ceiling. That is the honest result a...
calculation VIC confidence 0.70
**Sweep** — Hold true 2.5-6mH chokes (no anchor leak) with thick AWG18-22 fat/few-turns for high coil-Q, paired with raised C_eff (longer tubes) to pull f_r honestly into 40-70kHz, plus a fine referen...
design note VIC confidence 0.70
This sweep was supposed to test mid-to-high chokes (2.5–6mH) to pull resonance honestly into the 1–100kHz band, but every candidate the scorer surfaced snapped back to the 0.1mH reference anchor and l...
calculation VIC confidence 0.70
**Sweep** — With C_eff reduced via fewer cells, sweep mid-to-high chokes (2.5-6mH) at moderate turns/thicker wire to land f_r honestly in-band while preserving coil-Q, plus a finer reference grid near...
design note VIC confidence 0.70
Design note — VIC resonant sweep, choke-gap session. I set out to fill the 1.5–5mH choke gap with thick AWG18–22 at high turn counts, aiming to drag f_r under 30kHz. The result is honestly a disappoin...
calculation VIC confidence 0.70
**Sweep** — Fill the untested 1.5–5mH choke gap (beyond prior ≤3.3mH rungs) with thick AWG18–22 at high turn counts to push f_r under 30kHz while checking coil Q, plus a fine grid near the 0.1mH ancho...
design note VIC confidence 0.70
This sweep didn't do what I set out to do, and that's the first thing worth recording. I intended to grow C_eff (16–24 cells, big tubes) and pair it with 0.3–1.5mH chokes to drag f_r down into the bui...
calculation VIC confidence 0.70
**Sweep** — With C_eff grown (16-24 cells, 40-60mm tubes, tighter gap), test high-L 0.3-1.5mH chokes to land f_r in the buildable 20-50kHz band while holding the 0.1mH/120t anchor and thick AWG to kee...
design note VIC confidence 0.70
This session's hypothesis failed in an instructive way. I set out to push L into the 0.3–1.5mH range to honestly drag f_r down toward 20–50kHz, but the scorer kept handing back the 0.1mH reference cho...
calculation VIC confidence 0.70
**Sweep** — Push into higher L (0.3-1.5mH) with moderate turns to honestly drag f_r toward 20-50kHz while holding 250-300V film voltage, assuming grown C_eff from longer/more-parallel cells; fine grid...
design note VIC confidence 0.70
Session note — VIC resonant sweep, 90 candidates, Randles + vapor-film CGDE diagnostic. The uncomfortable truth first: my whole top tier is degenerate. All five collapse to the same cell geometry (18m...
calculation VIC confidence 0.70
**Sweep** — Fine grid around adopted best (0.1mH/200T/AWG18) plus a push into higher L 0.3-1.5mH paired with lower turns to hold film voltage while dragging f_r toward the band — testing whether reduc...
design note VIC confidence 0.70
Lab note — VIC resonant sweep, 0.3–2mH gap bridge. The gap didn't close the way I hoped. Every survivor pinned itself at 0.1mH per choke and f_r = 303.9kHz — the solver refused to buy real inductance...
calculation VIC confidence 0.70
**Sweep** — Bridge the untested 0.3-2mH gap between the crowned 0.1mH branch and the explored 2mH start to find buildable f_r (~90-290kHz falling toward band) that still holds ~250-300V film, sweeping...
design note VIC confidence 0.70
This sweep did not do what I set out to do. I wanted the in-band 5–7.4mH branch that resonates the 1.37nF cell at 40–70kHz, but the scorer instead crowned the low-L branch — every top candidate sits a...
calculation VIC confidence 0.70
**Sweep** — Sweep L jointly across the in-band 5-7.4mH region (where 1.37nF resonates at 40-70kHz) plus a low-L branch, varying turns/gauge to preserve coil Q and ~300V film — stop chasing the sub-5mH...
design note VIC confidence 0.70
Notebook — VIC mid-choke sweep, 1.37nF cell. The sweep did not do what I asked it to. I wanted the lowest inductance in the 0.3–5mH gap that still drags f_r into 40–70kHz, but every one of the top fiv...
calculation VIC confidence 0.70
**Sweep** — Bridge the untested 0.3-5mH mid-choke gap (between the buildable 0.1mH best and the already-swept 7.4mH point) to find the lowest inductance that still pulls f_r into 40-70kHz on the 1.37n...
design note VIC confidence 0.70
Lab note — VIC resonant sweep, RANDLES-CELL + vapor-film diagnostic. The premise this session was to abandon the phantom 200nF sizing and push L up toward ~7.4mH to land f_r=50kHz on the real 1.37nF c...
calculation VIC confidence 0.70
**Sweep** — Abandon the phantom 200nF sizing: sweep L up toward ~7.4mH (the value that lands f_r=50kHz on the real 1.37nF cell) to finally pull resonance into the 1-100kHz band, holding low-turn heavy...
design note VIC confidence 0.70
Design note — VIC choke sweep, holding the sub-mH band against a 1.37nF cell. Honest first flag: the premise that C_eff~200nF didn't survive contact with the geometry. The 18mm-in-34mm × 25mm cell, ev...
calculation VIC confidence 0.70
**Sweep** — Hold C_eff~200nF and sweep the untouched 0.05-0.3mH choke band — arithmetic (L=1/((2πf)^2·C)) puts f_r=50kHz at ~0.05mH for 200nF, so pair low-turn heavy gauge coils for Q with these sub-m...
design note VIC confidence 0.70
This sweep set out to bridge the sub-mH choke band and drop f_r to 50kHz, and it failed the frequency target cleanly — every one of my top five parks at 303.9kHz, four to six times over the 1-100kHz b...
calculation VIC confidence 0.70
**Sweep** — Bridge the untouched sub-mH choke band (0.1-3mH) to land f_r at 50kHz once C_eff is pushed to 100-400nF, while keeping low-turn heavy gauge for coil Q and the 129 Td film. - **Cell** — 18m...
design note VIC confidence 0.70
This session did not do what I set out to do, and I need to be honest about that in the record. The stated goal was to fine-grid the choke around 0.1mH while pushing C_eff up to ~100-200nF to drop f_r...
calculation VIC confidence 0.70
**Sweep** — Fine-grid the choke around #1's 0.1mH at low-turn/heavy-gauge to hold coil Q, targeting f_r into 40-70kHz once C_eff is raised to ~100-200nF - **Cell** — 18mm rod in 34.0mm tube × 25mm, 8...
design note VIC confidence 0.70
Reading these five back, the sweep did not do what I set out to do. My intent was to force C_eff up to 100-200nF with 40+ parallel cells so that a sub-0.2mH choke would land Xl=Xc down in the 40-70kHz...
calculation VIC confidence 0.70
**Sweep** — With C_eff forced up (~100-200nF from 40+ parallel cells), sweep the sub-0.2mH choke band to land Xl=Xc in 40-70kHz while walking low turns on heavy gauge to hold coil Q on the 129Td film...
design note VIC confidence 0.70
This session was supposed to walk the sub-0.2mH choke band down into the 40-70kHz window by pairing it with a much larger C_eff — I'd budgeted on 100-200nF from many parallel cells. The sweep did not...
calculation VIC confidence 0.70
**Sweep** — Attack the untouched sub-0.2mH choke band to re-match Xl=Xc into 40-70kHz at a much larger C_eff (~100-200nF from more parallel cells), walking turns/gauge to hold coil Q on the 129Td film...
design note VIC confidence 0.70
Lab note — VIC resonant sweep, screen-guided (choke L/turns/gauge), 48 candidates. This sweep pinned the choke at 100µH each and let me walk turns and wire gauge. The honest result: the score barely m...
calculation VIC confidence 0.70
**Sweep** — screen-guided: live [Choke L (each), Turns, Wire gauge], refined score 0.274 - **Cell** — 18mm rod in 34.0mm tube × 25mm, 8 cell(s) parallel → C_eff = 1.37nF, bulk water R = 10389Ω. - **Wa...
design note VIC confidence 0.70
This sweep drove home a hard constraint I keep bumping into: with a 1.37nF cell and a 100µH choke on each side, resonance lands at 303.9kHz — dead outside my practical 1–100kHz band. Every one of the...
calculation VIC confidence 0.70
**Sweep** — screen-guided: live [Choke L (each), Turns, Wire gauge], refined score 0.274 - **Cell** — 18mm rod in 34.0mm tube × 25mm, 8 cell(s) parallel → C_eff = 1.37nF, bulk water R = 10389Ω. - **Wa...
design note VIC confidence 0.70
Choke sweep, session note. I pushed L up to drag f_r into the practical 1-100kHz drive band with the AWG18/20-turn winding held fixed. The physics is a clean trade and it's frustrating: the only candi...
calculation VIC confidence 0.70
**Sweep** — Move the real knob: sweep choke L up toward ~1mH to drag f_r into the 1-100kHz drive band, winding fixed at the AWG18 optimum; fine grid around the 3.8mH in-band build point plus the 1mH/3...
design note VIC confidence 0.70
This sweep let me vary only the choke — inductance, turns, wire gauge — and the flat 0.274 plateau across the top four tells the real story: with L pinned at 100µH each side, I've fixed the resonant p...
calculation VIC confidence 0.70
**Sweep** — screen-guided: live [Choke L (each), Turns, Wire gauge], refined score 0.274 - **Cell** — 18mm rod in 34.0mm tube × 25mm, 8 cell(s) parallel → C_eff = 1.37nF, bulk water R = 10389Ω. - **Wa...
design note VIC confidence 0.70
Lab note — VIC resonant sweep, 72 candidates, RANDLES-CELL + vapor-film diagnostic. The premise this session was to force f_r down into the legal 50-100kHz band by pushing per-choke L up to 0.3-0.8mH...
calculation VIC confidence 0.70
**Sweep** — Directly raise per-choke L into 0.3-0.8mH to force f_r down into the legal 50-100kHz band against fixed 1.37nF/8-cell, holding light high-Q windings from anchor #1, then re-map the Td wind...
design note VIC confidence 0.70
Lab notebook — VIC resonant sweep, 0.1mH choke gap This session tried to thread the 0.1–0.8mH per-choke gap, co-varying turns and gauge to walk f_r down from 300kHz toward the practical 50–100kHz boun...
calculation VIC confidence 0.70
**Sweep** — Fill the untried 0.1-0.8mH per-choke gap between the 100µH self-resonant point and the already-swept 0.8mH edge, co-varying turns/gauge to map f_r down from 300kHz toward the 50-100kHz bou...
design note VIC confidence 0.70
Lab note — VIC choke sweep (48 candidates, RANDLES + vapor-film CGDE diagnostic) This sweep swept only the choke: L, turns, wire gauge. All 48 collapse onto essentially the same operating point becaus...
calculation VIC confidence 0.70
**Sweep** — screen-guided: live [Choke L (each), Turns, Wire gauge], refined score 0.274 - **Cell** — 18mm rod in 34.0mm tube × 25mm, 8 cell(s) parallel → C_eff = 1.37nF, bulk water R = 10389Ω. - **Wa...
design note VIC confidence 0.70
Design note, 18 July 2026 This sweep locked the cell geometry (18mm rod/34mm tube, 8-cell parallel, C_eff 1.37nF) and let the choke live-vary in turns/gauge while everything else held. All five top ca...
calculation VIC confidence 0.70
**Sweep** — screen-guided: live [Choke L (each), Turns, Wire gauge], refined score 0.274 - **Cell** — 18mm rod in 34.0mm tube × 25mm, 8 cell(s) parallel → C_eff = 1.37nF, bulk water R = 10389Ω. - **Wa...
design note VIC confidence 0.75
Tried "larger L" literally and it broke: sweep spec asked for 10-40H per choke (clamp ceiling 10H), giving L_total up to 20H against the current ref cell (WFC v25 geometry, ~1.4nF). Result: f_r collap...
design note VIC confidence 0.70
Lab note — VIC resonant sweep, RANDLES + vapor-film diagnostic. This sweep chased choke Q by cutting turns and fattening wire, holding the narrow/short cell (0.77nF, R_bulk 18.8kΩ). It half-worked and...
calculation VIC confidence 0.70
**Sweep** — Keep f_r in the 40-70kHz band via moderate L (paired with the narrower/shorter cell C_eff from the plan) while chasing higher choke Q through lower-loss windings — fewer turns, thicker wir...
design note VIC confidence 0.70
Lab note — 2mH choke sweep, target f_r < 100kHz Pushed L to 2mH against the same 9mm/17mm cell (C_eff 0.69nF) and landed f_r = 95.51kHz across the whole top-5, not the 2-5mH spread I intended — the so...
calculation VIC confidence 0.70
**Sweep** — Push L up an order of magnitude (2-5mH) at fixed cell geometry to drag f_r under 100kHz, checking whether Td/CGDE window survives the lower cell voltage - **Cell** — 9mm rod in 17.0mm tube...
design note VIC confidence 0.70
Lab note, 2026-07-10 — mid-L sweep (0.3-0.8mH band + 0.2-0.3mH edge) All five top candidates converge on the same 0.0002H choke value regardless of AWG/turns fill — the geometric C_eff (1.19nF) at thi...
calculation VIC confidence 0.70
**Sweep** — Fine-grid mid-L structural band (0.3-0.8mH) with untested 0.2-0.3mH edge, crossed with wider AWG/turns combos to find higher-Q in-band f_r solutions beating 0.73 without repeating prior L/...
design note VIC confidence 0.70
Ran the low-L bracket (0.02-0.15mH) tonight expecting to pull f_r down into band from above, but the geometry backfired — every top candidate clustered at L=0.1mH and landed at 326.8kHz, nearly 5x ove...
calculation VIC confidence 0.70
**Sweep** — Prior L sweeps (0.15-2.5mH) with 3-4 parallel cells never landed f_r in-band; test unexplored 0.02-0.15mH low-L region plus 2.5-5mH high-L region, both at Q-preserving high-turns/low-AWG c...
design note VIC confidence 0.70
Lab notebook, VIC sweep — L held at 0.1mH, widening tube gap to raise C_eff. Result: all 64 candidates cluster at f_r = 326.8kHz, roughly 5x above my 40-70kHz target. Raising C_eff alone (via 9mm rod/...
calculation VIC confidence 0.70
**Sweep** — Hold L fixed at 0.1mH (per plan) while widening gap/tube geometry raises C_eff directly, to pull f_r into 40-70kHz without shrinking both L and C together - **Cell** — 9mm rod in 13.0mm tu...
design note VIC confidence 0.70
Lab note, 7/9/26 — L-decade-down sweep, gap-shortened C_eff Pushed L to 0.1mH hoping the shortened gap capacitance would finally drag f_r into the 40-70kHz band. It didn't — all 24 candidates lock at...
calculation VIC confidence 0.70
**Sweep** — Push L another decade below 0.1mH with further-shortened gap C_eff to test if f_r finally lands in 40-70kHz band, keeping low-AWG high-Q coil family - **Cell** — 9mm rod in 13.0mm tube × 1...
design note VIC confidence 0.70
Ran the tube/gap sweep to push C_eff up an order of magnitude — got there: 1.19nF vs the ~0.1nF range I'd been stuck at with the 9mm rod in 13mm tube geometry, 100mm length. But raising C alone didn't...
calculation VIC confidence 0.70
**Sweep** — Sweep tube diameter and rod/tube gap to raise C_eff an order of magnitude, then re-run L across the 1mH-0.1mH transition to find where Q>1 lands f_r inside 40-70kHz - **Cell** — 9mm rod in...
design note VIC confidence 0.70
Lab note — mapping the 1mH-to-0.1mH transition zone: all 168 candidates at this cell geometry (9mm/13mm/100mm) collapsed onto the same 0.1mH choke value with f_r pinned at 326.82kHz — a full order of...
calculation VIC confidence 0.70
**Sweep** — Map transition region between 1mH anchor and 0.1mH dead-zone at fixed cell geometry to find intermediate L keeping f_r in-band while raising tank Q beyond anchor's 0.73 - **Cell** — 9mm ro...
design note VIC confidence 0.70
Ran the wide choke sweep to see if pulling away from the 130t/1mH anchor would find a higher-Q regime, and it did answer the question — just not usefully. Dropping to 0.1mH (40-70 turns) collapses coi...
calculation VIC confidence 0.70
**Sweep** — Wide choke geometry sweep away from 1mH anchor (varying L via turns/AWG) to test if a distinct inductance regime yields higher tank Q than the water-branch-limited 130t/1mH point, since pp...
design note VIC confidence 0.70
Lab note, 2026-07-03 — VIC resonant sweep, choke fixed at 130t/1mH anchor All 216 candidates this session converged on a single geometry/electrolyte point: 21.8mm rod in 26.8mm tube, 60mm, single cell...
calculation VIC confidence 0.70
**Sweep** — Hold choke fixed at adopted 130t/1mH anchor (no further choke sweep this session) since active lever remains capacitance/gap; tight reconfirmation grid only - **Cell** — 21.8mm rod in 26.8...
design note VIC confidence 0.70
Fine-tuning turns around the 130t/AWG18 point confirms what I suspected — once L is locked near 1mH with this cell geometry (1.27nF, 90.5kΩ water R), the resonant point sits in a tight plateau. Candid...
calculation VIC confidence 0.70
**Sweep** — Lock choke at 130t/AWG18 near-optimal L; sweep gap/electrode-length via C and water-R proxy isn't a choke param, so fine-tune L around 130t operating point to confirm plateau while geometr...
design note VIC confidence 0.70
Lab note, 2026-07-03: Reran the choke sweep to see if AWG16-17 at fixed 140t plus fine L retune could squeeze more Q out before I hit the wall I suspected — and it's a wall. Every top-5 candidate conv...
calculation VIC confidence 0.70
**Sweep** — Wire gauge saturated at AWG18/140t; now vary cell geometry lever via C/water-R proxy by testing AWG16-17 at fixed 140t plus fine L retune to see if any residual Q gain exists before the wa...
design note VIC confidence 0.70
Lab notebook — VIC choke sweep, AWG18 @ 150t, session cont'd from AWG20 baseline Bumping to AWG18 confirms the obvious: heavier wire drops coil AC resistance from 0.9Ω to 0.6-0.7Ω, and tank Q climbs f...
calculation VIC confidence 0.70
**Sweep** — AWG20/150t and L~1mH already explored; now test heavier wire AWG18-19 at fixed 150t to see if lower coil R pushes tank Q and voltage beyond the 0.9Ω/Q64.4 baseline - **Cell** — 22.8mm rod...
design note VIC confidence 0.70
Lab notebook — VIC choke sweep, L held at 1mH, AWG20-22 Ran 15 candidates holding L=1mH and stepping AWG20-22 turns to see if I could push tank Q past 62 without tripping the 1A series current ceiling...
calculation VIC confidence 0.70
**Sweep** — Hold L at 1mH, sweep AWG20-22 for lower coil R to test if tank Q exceeds 62 while current stays under 1A limit - **Cell** — 15.9mm rod in 22.3mm tube × 101.6mm, 1 cell(s) parallel → C = 1....
design note VIC confidence 0.70
Lab notebook — VIC sweep, single 15.9mm/22.3mm×101.6mm cell, 1.31nF, water R 87.6kΩ. The sweep confirms what I'd expect from the series-RLC picture: tank Q tracks coil AC resistance almost linearly at...
calculation VIC confidence 0.70
- **Cell** — 15.9mm rod in 22.3mm tube × 101.6mm, 1 cell(s) parallel → C = 1.31nF, water R = 87585Ω. - **Chokes** — 2 × 0.001H (100 turns, AWG 24, 12m wire, AC R 1.2Ω each). - **At resonance f_r = 98....
breakthrough VIC confidence 0.60
- **Cell** — 12.7mm rod in 19.1mm tube × 101.6mm, 6 cell(s) parallel → C = 6.56nF, water R = 17497Ω. - **Chokes** — 2 × 0.001H (100 turns, AWG 24, 12m wire, AC R 1.0Ω each). - **At resonance f_r = 43....
design note VIC confidence 0.70
Lab note, 7/3/26 — VIC resonant tank sweep, 180 candidates. The sweep confirms what I'd expect from the choke-coil topology: for a fixed cell geometry (6.56nF, 17.5kΩ water leakage), tank Q trades dir...
calculation VIC confidence 0.70
- **Cell** — 12.7mm rod in 19.1mm tube × 101.6mm, 6 cell(s) parallel → C = 6.56nF, water R = 17497Ω. - **Chokes** — 2 × 0.001H (100 turns, AWG 24, 12m wire, AC R 1.0Ω each). - **At resonance f_r = 43....
established VIC
Under computer control, the Voltage Intensifier Circuit is energised by a normal 12V car battery to generate high voltage pulses at very low current (<1 milliamp), with the voltage responsive to the t...
established VIC
Six Voltage Intensifier Circuit bobbins, manufactured in the UK at Stan Meyer's request, arrived and were confirmed to be of the necessary quality, indicating the VIC bobbin design could be replicated...
established VIC confidence 0.70
In the same third-party replication, resonant chokers were copper-wired ferrite inductors of approximately 0.8H, resonating with an approximately 10nF cell capacitance, each with 1 kOhm serial resisto...
established VIC confidence 0.70
In a third-party replication attempt (Dr. T. Nagypal), a copper-wired permalloy transformer with 20kHz bandwidth stepped voltage from 12V to 600V (positive square wave bursts), with a 1 kOhm resistor...
established VIC
Per Appendix B Note 1, Choke-Coil (62, Fig 7-1) magnetic field (FL2) during pulse on-time impedes electron flow (since electron mass is electromagnetic and interacts with magnetic field strength), cau...
established VIC confidence 0.60
The test report includes component-side and foil-side views of a 'Variable Pulse Triggering Circuit,' indicating it is a distinct circuit board used in the system's pulse generation stage. Source: WFC...
established VIC
In Voltage Intensifier Circuit Diagram (AA), a gated variable amplitude pulse train (49a...49n) passes through a blocking diode into Resonant Charging Choke (56, primary) and Resonant Charging Choke (...
established VIC
Pulse-voltage repetition rate sets up a step-up electrical charging effect since the Resonant Cavity functions as a Capacitor (ER) due to the dielectric value of water (78.542), which becomes an integ...
established VIC
The paired coil wires' opposite voltage potentials (positive electrical attraction force B+ = negative electrical attraction force B-, called Electrical Stress SS'=RR' as to (160) of Figure 3-26) are...
established VIC
Beyond amp-restricting characteristics, the paired bifilar-wrapped spiral coils cause voltage level enhancement beyond applied voltage input because the distributed capacitance (C1a...C1n = C2a...C2n)...
established VIC confidence 0.80
Other amp restricting circuits are applicable, such as applying a variable (0-5) volts unipolar pulse-frequency across the armature field-winding of a de-regulated alternator functioning as a pulse-vo...
established VIC confidence 0.80
The Voltage Intensifier Circuit (VXA) prevents electron replacement on the polarized gas atoms, and the water molecule is exposed to the same voltage stimulation process. Source: WFC Dealership Manual...
established VIC
Blocking diode (58) prevents electrical shorting from occurring across pickup coil (56) during pulsing operations. Source: WFC Dealership Manual Extended - Design Specs — Steam Resonator
established VIC
Voltage potential (57) gates ON unidirectional diode (58), allowing the potential to pass through in-line charging Choke Coil (59) to Excitor Plate (61), forming positive voltage field (62); the choke...
established VIC
Pickup coil (56) is composed of resistive wire, restricting amp flow within the voltage intensifier circuit (60), per WFC Tech Brief Section 4 (Voltage Attenuation Circuit Design Specs). Source: WFC D...
established VIC
In the rotary alternative (Fig 11A), variable amplitude pulsing circuit (21) energizes armature coils (22) to produce pulsating electromagnetic fields (23) rotated through pickup coils (24), generatin...
established VIC
System setup requires filling the water fuel cell, adjusting excitor plate distance/volume, connecting to the VIC, then tuning to the resonant characteristic of the total system by adjusting the pulse...
established VIC
Modulator inductor coils (9 and 12), made of resistive wire, act as DC current limiters during initial fuel cell charging; the low-Q resonant charging circuit of the fuel cell (10, 11) in series with...
established VIC
Terminal resistor (12), affixed on the ground side of the excitor array between bypass coil (9) and ground terminal (13), is composed of resistive wire wound in the same coil configuration as bypass c...
established VIC
The high-frequency voltage bypass coil (9), wound of resistive wire, duplicates the incoming voltage pulse train from the secondary coil (8) via inductive coupling: the pulse creates an oscillating ma...
established VIC
In the Voltage Intensifier Circuit transformer, the primary coil is copper wire and the secondary coil is resistive wire, both insulated to prevent shorting; the two coils are joined on the ground sid...
established VIC
Optocoupler (4), triggered by variable gate circuit (5), gates the pulse voltage frequency waveform on/off; the gated pulse train on-time (16) vs off-time (17) is adjustable from 1% to 100% duty cycle...
established VIC
Optocoupler (3), triggered by pulse frequency generator (2), attenuates power supply voltage (1) into a pulse voltage waveform (Fig 9A); varying the pulse generator's triggering rate from 1Hz to 1MHz...
established VIC
The first-stage variable power supply is any conventional AC-to-DC or DC (non-regulated) supply providing an adjustable output voltage range from less than one volt to 110 volts and up, used as the fi...
established VIC
Resonant Charging Choke (47), placed between the negative voltage zone (44) and electrical ground (48), helps maintain capacitance value (voltage level) within the Resonant Cavity during voltage pulsi...
established VIC
Distilled water is an insulator to amp flow; natural water with less than 20ppm of contaminates maintains a high dielectric constant, and the VIC's component arrangement retards or prevents amp flow....
established VIC
Capacitance formed between conductor plates 44/45 with natural water as the conducting medium is relatively high, and this capacitance opposes any change in circuit voltage, delaying voltage change un...
established VIC
Stainless Steel Material T304 forming voltage zone (45) does not chemically interact with liberated hydrogen, oxygen, and ambient air gases in natural water when exposed to a voltage potential during...
established VIC
High voltage output from Resonant Charging Choke (43) forms a Positive Electrical Voltage Pulse Potential across voltage surface area (45), which is immersed in natural water, per step-charging graph...
established VIC
Resonant Charging Choke (43) is a Modulator Inductor that sets up an oscillation at a given charging frequency (voltage pulsing rate) with the effective capacitance of a pulse-forming network to charg...
established VIC
Blocking Diode (14) conducts current in only one direction, preventing electron flow toward the Secondary Pickup Winding (42) during Positive Voltage Potential formation. Source: WFC Dealership Manual...
established VIC
The resistive wire-coil Secondary Pickup Winding (42) allows a voltage potential to form via electromagnetic induction, while its Ohm value acts as a resistor opposing electron flow from circuit elect...
established VIC
The circuit's purpose is to form opposite electrical voltage zones while restricting amp flow during the Electrical Polarization Process, which splits the water molecule by voltage stimulation rather...
established VIC
The voltage zone surface areas (44/45) of the Resonant Cavity Assembly (Figure 12) form the capacitance value of the assembly, with natural water inside the cavity providing the dielectric between the...
established VIC
In the Dual Voltage Resonant 'Q' scheme, a Low Amplitude Pulse Voltage Frequency (54) is injected between the Pulse Voltage Frequency (53) to keep an electrical charge on the water molecule during Res...
established VIC
By varying applied voltage amplitude in direct relationship to a variable pulse voltage frequency, the Resonant Cavity Structure can take different shapes to maximize voltage stimulation of the water...
established VIC
The ability of an inductor and a capacitor in a series-resonant circuit delivers a voltage several times greater than the input voltage. Source: WFC Dealership Manual Extended - Design Specs — Dual Vo...
established VIC
The resistive value of the wire-coil (47) prevents amp flow while performing in like manner as a Resonant Charging Choke. Source: WFC Dealership Manual Extended - Design Specs — Dual Voltage Resonant...
established VIC
Another Resonant Charging Choke, resistor component (47), is placed between the negative voltage zone (44) and circuit electrical ground (48) to help maintain the resistance value (voltage level) with...
established VIC
Capacitance is formed between conductor plates 44/45 (voltage zones) since the dielectric value (insulating medium) of natural water is relatively high, opposing changes in circuit voltage until store...
established VIC
Stainless Steel Material T304 forming voltage zone (45) does NOT chemically interact with liberated hydrogen, oxygen, and ambient air gases in natural water when exposed to a voltage potential during...
established VIC
The high voltage output from the Resonant Charging Choke (43) forms a Positive Electrical Voltage Pulse Potential (voltage zone) across surface area (45) immersed in natural water, per the step-chargi...
established VIC
The resistive value of the Charging Choke (43) acts as a resistor, further preventing amp flow in the circuit. Source: WFC Dealership Manual Extended - Design Specs — Dual Voltage Resonant "Q" - Part...
established VIC
The Resonant Charging Choke (43) is a Modulator Inductor which sets up an oscillation at a given charging frequency (voltage pulsing rate) with the effective capacitance of a pulse-forming network in...
established VIC confidence 0.80
The Resonant Charging Choke is identified as component (43), a resistive wire coil, within the Electronic Interfacing Circuit of the Voltage Intensifier Circuit. Source: WFC Dealership Manual Extended...
established VIC
Blocking Diode (14) conducts electricity in one direction only (the direction of the schematic arrow), preventing electron flow or movement toward the Secondary Pickup Winding (42) during Positive Vol...
established VIC
Since electrons are negatively electrically charged, electron (amp) flow always moves toward positive electrical potential when allowed to do so. Source: WFC Dealership Manual Extended - Design Specs...
established VIC
The Secondary Pickup Winding (42) is a resistive wire-coil that allows a voltage potential to form across it via electromagnetic induction, while the resistive (Ohm) value of the coil wire acts as a r...
established VIC
The purpose of the VIC circuit operational parameters is to form opposite Electrical Voltage Zones while restricting amp flow during the Electrical Polarization Process, which splits the water molecul...
established VIC
The Resonant Cavity Assembly (4) has an inner surface (45) forming a Positive Electrical Voltage Zone and an outer surface (44) forming a Negative Voltage Zone. Natural water inside the cavity provide...
established VIC
To start compounding-action (resonant action), voltage pulses are attenuated while voltage amplitude is increased. Source: WFC Dealership Manual Extended - Design Specs — Operational Comments
established VIC
Voltage pulses, attenuated up to and beyond 5,000 volts, are used to cause liberated gas atoms to reach an ionization state. Source: WFC Dealership Manual Extended - Design Specs — Circuit Function
established VIC
A variable pulsing circuit is set up that is capable of tuning-in resonant action regardless of the shape and dimensional size of the resonant cavity (44). Source: WFC Dealership Manual Extended - Des...
established VIC
Variable gate circuit (32) is a two-state switch linked to opto-coupler (36) and opto-coupler (39). When near ground/low state, opto-coupler (36) triggers to form pulse waveform (d)-(e); when gate cir...
established VIC
A dual-pulsing circuit (components 33, 34, 38, 39, 40) is integrated with the Voltage Intensifier Circuit (Figure 9) as shown in Figure 20C, to enhance hydrogen gas production beyond simple voltage at...
established VIC confidence 0.80
During the pulse-voltage application across the Excitor-Array, electron flow within the Voltage Intensifier Circuit is inhibited or prevented, enabling the ionization effect on the gas atom rather tha...
established VIC
Since pickup coil (n) is also composed of resistive wire-coil (R4), the total circuit resistance of the Voltage Intensifier Circuit includes this resistance value. Source: The Birth Of New Technology...
established VIC
Inductor (y) in relationship to inductor (c) electrically balances the opposite voltage electrical potential across voltage zones (E3) and (E4). Source: The Birth Of New Technology — RLC CIRCUIT
established VIC
The moveable wiper arm on inductor (y) fine-tunes 'Resonant Action' during pulsing operations of the Voltage Intensifier Circuit. Source: The Birth Of New Technology — RLC CIRCUIT
established VIC
Variable inductor-coil (y), similar to inductor (c) but connected to the opposite polarity voltage zone (E4), further inhibits electron movement or deflection within the Voltage Intensifier Circuit. S...
established VIC
Inductor (c) is composed of resistive wire (R7) which further restricts D.C. current flow beyond the inductance reactance (XL). Source: The Birth Of New Technology — RLC CIRCUIT
established VIC
Voltage intensity or level across the Excitor-Array (ER of t) can exceed 20,000 volts due to circuit (AA) interaction, and is directly related to the variable amplitude of the input pulse-train (h). S...
established VIC
Once the voltage-pulse is terminated or shut off, voltage potential returns to a ground-state or near ground-state, restarting the voltage deflection process. Source: The Birth Of New Technology — RLC...
established VIC
During resonant interaction, the incoming unipolar pulse-train (h) of Figure 1-1, as related to Figure 9B, produces a step-charging voltage-effect across the Excitor-Array (ER of t). Source: The Birth...
established VIC
At frequencies close to resonance, the voltage across the individual inductor or capacitor is higher than the applied voltage (h). At exact resonant frequency, the voltage across both the inductor and...
established VIC
For the series LC circuit, total voltage Vt equals current I multiplied by impedance Z (Vt = IZ), applying Ohm's Law to the resonant circuit. Source: The Birth Of New Technology — LC VOLTAGE
established VIC
The capacitive reactance Xc in the series LC circuit is calculated as Xc = 1 / (2π·F·C), where F is frequency and C is capacitance. Source: The Birth Of New Technology — LC VOLTAGE
established VIC
For an inductor and capacitor in series, the total impedance Zseries is given by Zseries = (Xc − Xl), where Xc is the capacitive reactance and Xl is the inductive reactance. Source: The Birth Of New T...
established VIC
Blocking Diode (f) prevents electrical shorting to secondary coil (n) during pulse-off time, since the diode conducts electrical energy only in the direction of the schematic arrow. Source: The Birth...
established VIC
Isolated electrical ground (w) prevents electron flow from the input circuit ground into the pulsing transformer's secondary side. Source: The Birth Of New Technology — CIRCUIT COMPONENT INTERACTION
established VIC
Voltage amplitude or voltage potential is increased when the secondary coil (n) is wrapped with more turns of wire. Source: The Birth Of New Technology — CIRCUIT COMPONENT INTERACTION
established VIC
The pulsing transformer (m) steps up voltage amplitude or voltage potential during pulsing operations, with the primary coil electrically isolated from the secondary coil to form the Voltage Intensifi...
established VIC
A 100 amp-hr battery divided by the 3.3 amp/hr current consumption of the VIC circuit gives 30.3 hours of battery life without recharging. Source: The Birth Of New Technology — Appendix 4
established VIC
40 watts divided by 12 volts battery equals a 3.3 amp/hr current draw capacity for the Voltage Intensifier Circuit. Source: The Birth Of New Technology — Appendix 4
established VIC
The Voltage Intensifier Circuit applies 40,000 volts at 1 milliamp, equaling 40 watts of applied electrical power. Source: The Birth Of New Technology — Appendix 4
established VIC
Voltage Intensifier Circuit (A3) is interlocked with the Safety Control Circuit (D) through the Electronic Control Unit (B). Source: The Birth Of New Technology — Fuel-Gases / Quenching Tube
established VIC
Engine RPM is controlled by way of voltage deflection through a patented electronic circuit called the Voltage Intensifier Circuit, which regulates hydrogen gas flow-rate to the engine. Source: The Bi...
established VIC
Both the VIC Dual Single-Coil Assembly and the VIC Bifilar-Wrap Coil Assembly function similarly in producing voltage enhancement without incurring amp influxing (current increase). Source: The Birth...
established VIC
The resultant voltage enhancement (voltage amplitude) produced by the VIC can exceed 40 kilovolts, instantly converting water droplets into thermal explosive energy (referred to as 'gtnt'). Source: Th...
established VIC confidence 0.80
Water's dielectric value provides resistance to amp flow, allowing it to function as an integral capacitive element (the Resonant Cavity) within the VIC Circuit. Source: The Birth Of New Technology —...
established VIC
The Pulse-Voltage repetition rate sets up the step-up electrical charging effect because the Resonant Cavity functions as a capacitor due to the dielectric value (resistance to amp flow) of water, whi...
established VIC
The paired coil-wires' opposite voltage potentials (positive electrical attraction force B+ equaling negative electrical force B-), called 'Electrical Stress' (SS' = RR'), are always equal in electric...
established VIC
The distributed capacitance and distributed inductance of the bifilar-wrapped coils encourages a compounding effect, increasing electromagnetic field strength (mutual induction) during each pulsing cy...
established VIC
The spiral-wrapped coils paired together in the VIC Bifilar-Wrap Coil Assembly cause voltage level enhancement beyond the applied voltage input, due to distributed capacitance and distributed inductan...
established VIC
This induced voltage phenomenon prevents the resonant pulse frequency (58) from being impaired or altered while being electrically transmitted to the Resonant Cavity (180) of Figure (14) via electrica...
established VIC
The induced external electromagnetic field (63/64) across the Resonant coil-Tap (67) increases voltage intensity further rather than diminishing peak voltage potential from the resistive valve of the...
established VIC
The resistive valve of the stainless steel wire-coil (56/57) combined with its inductance-generated electromagnetic field (62) of Figure (19) opposes electron movement: the dielectric valve of the wir...
established VIC
Resonant Charging Chokes (56/57) are formed using Stainless Steel Electro-Inductance wire-material (430F / T304 or equivalent), which when electrically pulsed transmits voltage intensity while restric...
established VIC
Sequential Switch Circuit (59) switches Booster Pickup Coils (61a-61n) in series with the Secondary Coil (53) output to elevate voltage intensity across Resonant Charging Chokes (56/57). Source: The B...
established VIC
The resultant gated Resonant Pulse-train voltage amplitude is attenuated by the Sequential Voltage Amplitude Control Circuit (59) once the step-up Secondary Coil (53) produces a higher voltage level t...
established VIC
Pulse on-time (T1), held at a predetermined constant voltage level (VL), is adjusted to maximize transference of electromagnetic energy to the Secondary Coil (53) during pulsing operations. Source: Th...
established VIC
The pulse-train (210a-210n) is adjusted so pulse off-time (T2) synchronizes with the collapsing and re-formation of the electromagnetic field coupling across the pulsing transformer (52/53), producing...
established VIC
The water forms a capacitor (E7/E8) in series with Resonant Charging Chokes (56/57) placed on opposite sides of the Resonant Cavity Zone (35), together forming the Resonant Pulsing Circuit (110) of Fi...
established VIC
The Voltage Intensifier Circuit (220) of Figure (18) allows Electrical-Stress variation (SS'=RR'/TT'=UU') because it inhibits electron-flow (amp restriction) into the voltage triggering process (210)...
established VIC
A 100 amp/hr battery divided by the 3.3 amp/hr current consumption of the VIC gives approximately 30.3 hours of battery life before recharging is needed. Source: The Birth Of New Technology — WDMS Las...
established VIC
The 40 watts of applied electrical power divided by the 12 volt battery supply yields a current draw capacity of 3.3 amp/hr. Source: The Birth Of New Technology — WDMS Laser Acceleration Cards
established VIC
The Voltage Intensifier Circuit applies 40,000 volts at 1 milliamp, equating to 40 watts of applied electrical power. Source: The Birth Of New Technology — WDMS Laser Acceleration Cards
established VIC
For performance reliability and safety, ionized air gases and liquid water do not become energy activated (volatile) until the water-fuel mixture (48) reaches the Voltage Igniter Stage (180). Source:...
established VIC
Water droplets exposed to opposing-polarity high intensity voltage fields undergo Electrical Polarization Process (160), separating hydrogen atoms (77a/77b) and oxygen atom (76) and causing electron e...
established VIC
The Voltage Igniter Stage (180) working with the Voltage Intensifier Circuit (110) and Electron Extraction Circuit (120) performs functions simultaneously to initiate and trigger thermal explosive ene...
established VIC
To elevate energy-flame temperature, fluid-displacement of water and ionized air is increased while non-combustible gas volume flow rate is maintained or reduced, during an increase of applied voltage...
established VIC
Energy-Flame temperature is regulated by controlling the volume flow-rate of fluid mediums (water, non-combustible gas, ionized air) in direct relationship to applied voltage intensity (33/36). Source...
established VIC
Exposure to the high intensity voltage fields performs the Electrical Polarization Process (160) undergoing Dielectric Resonance (240), which sets up and triggers the Hydrogen Fracturing Process (390)...
established VIC
The Water-Fuel mixture (48) enters Voltage Igniter Stage (180) and is exposed to high intensity voltage fields (33/36), typically 2,000 volts or above at 10 kHz or above, of opposite electrical polari...
established VIC
WFC memo 426, titled 'VIC Matrix Circuit,' defines the Voltage Intensifier Circuit configuration referenced for applying pulsating electrical stress to atoms as shown in Figure 5-8, item 550. Source:...
established VIC
The WFC Voltage Intensifier Circuit, as defined in WFC memo 426 'VIC Matrix Circuit,' applies a high pulsating 'Electrical stress' across an unstable radioactive atom via opposite voltage potential (i...
established VIC
The Voltage Intensifier Circuit (165) directly applies alternate/opposite (166/167) electrical voltage pulses, with amp restriction, in a sequential manner across voltage plates E5/E6 to activate the...
established VIC
To keep applied voltage amplitude constant while promoting Resonant Action, the incoming pulse train can be varied independent of voltage amplitude to attenuate voltage intensity and affect gas produc...
established VIC
To further prevent voltage fluctuation during resonant action, the Phase Lock Loop technique of the Pulse Indicator circuit (110) is utilized during pulsing operations. Source: The Birth Of New Techno...
established VIC
Attenuating voltage amplitude (Vo–Vn) together with pulse-width allows the Voltage Intensifier Circuit to tune-in and match the resonant characteristics/resonant frequency of the water bath, since the...
established VIC confidence 0.80
The pulse voltage potential (65) is applied across the Excitor plates while electron flow within the voltage intensifier circuit (190) is inhibited and prevented, a condition necessary for the water d...
established VIC
The step-charging voltage-wave (65) increases in amplitude from several millivolts to several hundred volts during each pulse train (65a...65n), causing the water molecule's charged atoms (76/77) to e...
established VIC
The variable pulse frequency generator (70) varies pulse frequency (63) at a 50% duty cycle pulse, while the gated pulse frequency generator (80) varies and adjusts pulse width (54a-54n). Source: The...
established VIC
Analog voltage signal (32a-32n) allows the pulse train (51a-51n) voltage amplitude to vary from one up to twelve volts (from battery supply 28) by attenuating the Laser Accelerator circuit (10) via th...
established VIC
The resultant interfacing voltage circuit (190) exposes the water molecule (210) to a pulsating high intensity voltage field (65a-65n) of opposite polarity (66/67) while restricting amp flow within ci...
established VIC
The pulsing core (53) aids amp restriction while the Voltage Intensifier Circuit (190) is tuned—by adjusting the pulse train's pulse-frequency (63) via the pulse frequency generator (70)—to match the...
established VIC
Amp leakage (electron coupling to water) to the water bath (68) is prevented by encapsulating the resonant cavity (57) in delrin material (72), an electrical insulator to high voltage that remains res...
established VIC
Amp restriction beyond resonant action occurs when unipolar magnetic field coupling (71) is allowed to simultaneously drop across both resonant charging chokes (56/62) during pulsing operations, since...
established VIC
Variable inductor-coil (62), similar to inductor (56) but connected to the opposite polarity voltage zone (67), further inhibits electron movement within the VIC; a movable wiper arm (73) fine-tunes t...
established VIC
Inductor (56) is composed of resistive wire to further restrict D.C. current flow beyond normal inductance reaction (Xl); pickup coil (52) is likewise made of resistive wire, contributing to total cir...
established VIC
Voltage intensity or level across the excitor array (57) can exceed 20,000 volts due to circuit (60) interaction, directly related to the variable amplitude input of the pulse train (64a-64n). Source:...
established VIC
At frequencies close to resonance, the voltage across the individual LC components (inductor 56, capacitor 57) is higher than the applied voltage (49); at exact resonant frequency the theoretical volt...
established VIC
The inductor (56) and capacitor (57) of LC circuit (180) are tuned to resonate at a given frequency; the resonant frequency (63) can be raised or lowered by changing the inductance (56) and/or capacit...
established VIC
Water becomes part of the Voltage Intensifier Circuit functioning as a resistance between electrical ground (67) and pulse-frequency positive potential (66), helping to prevent electron flow within th...
established VIC
Resonant charging choke (56) in series with the Excitor-Array (66/67) forms an inductor-capacitor circuit (180); the Excitor-Array acts as a capacitor because natural water (68) between the opposing e...
established VIC
Switching diode (55) prevents electrical shorting to the secondary coil (52) during pulse off-time by conducting only in one direction, and simultaneously acts as an electronic switch that opens the c...
established VIC
The pulsing transformer (primary coil 26 / secondary coil 52) steps up voltage amplitude during pulsing operations; primary and secondary coils have no direct electrical connection (electrically isola...
established VIC
Negative electrical ground (61) of the Voltage Intensifier Circuit (60) is electrically isolated from the primary electrical ground (48), preventing electron flow from the input circuit ground into th...
established VIC
Primary coil (26), pulsing core (53), secondary coil (52), switching diode (55), resonant charging choke (56), resonant cavity assembly (170), natural water (68), and variable resonant charging choke...
established VIC
The only electrical connection point is a voltage cross-over from the regulated power supply (150, Figure 3-6) to the battery supply (28), as illustrated in Figure 3-6. Source: The Birth Of New Techno...
established VIC
Although the primary coil pulse waveform (49) exactly duplicates pulse train (47), the two pulse trains are electrically isolated from each other despite the correspondence. Source: The Birth Of New T...
established VIC
The resultant pulse waveform (49a...49n) superimposed onto primary coil (26) in Figure 3-18 is an exact duplicate of the proportional pulse train (47a...47n) driving the cell driver circuit. Source: T...
established VIC
The gated pulse signal (48) fed into the cell driver circuit (90) performs a switching function, turning electric ground 'off' and 'on' as applied to the opposite side (48) of primary coil (26), shown...
established VIC confidence 0.80
In operation, Laser Accelerator Assembly (20) attenuates battery voltage potential (32a xxx 32n), which is electrically connected to the Voltage Intensifier Circuit (60). Source: The Birth Of New Tech...
established VIC
A variable voltage range (32a xxx 32n) from one (1) up to twelve (12) volts, representing the regulated battery voltage, is applied across primary coil (26) of the Voltage Intensifier Circuit (60). So...
established VIC
Regulator stage (27) of circuit (50) converts battery voltage potential (29) via electrical terminal (31) into analog voltage signal (32), which corresponds to but is electrically isolated (crossover...
established VIC
Regulatory stage (27) and stage (28) each work separately and independently of each other but are electronically linked/coupled together to produce a common analog signal (32) having a predetermined v...
established VIC
Circuit (50) performs two functions at once: it regulates car battery electrical voltage potential (32) applied to primary coil (26), and it regulates gas pressure of the Fuel Cell (120). Source: The...
established VIC
Voltage levels (22a...22n) control the applied voltage potential across Resonant Cavity Assembly (120) of Figure (3-22) through voltage amplitude control circuit (50), which is electrically linked to...
established VIC
The resultant varied voltage level (22a...22n) varies smoothly over a continuous range of voltage values rather than in discrete steps, as illustrated in the linear graph (23) of Figure (3-14). Source...
established VIC
As pulse width (17ax) of signal (19) changes, analog voltage level output (23) changes correspondingly: widening pulse width toward stop-position (17a...17n) increases the analog signal (22) to higher...
established VIC
The analog signal (22) is a voltage level signal that varies continuously in both time and amplitude, producing a voltage level directly proportional to the physical change in the pulse train (100...1...
established VIC
Analog Voltage Generator Circuit (40) electronically detects, translates, and converts the digital signal (19) from the accelerated control circuit (30) into an analog voltage signal (22) that is cont...
established VIC
The Voltage Intensifier Circuit (110, Figure 4-9) inhibits and prevents electron flow from entering into the gas ignition process (180), as further illustrated in Figure 4-8. Source: The Birth Of New...
established VIC
Voltage Igniter Stage (180, Figure 4-5), together with Voltage Intensifier Circuit (110, Figure 4-9) and Extraction Circuit (10, Figure 4-10), performs several functions simultaneously to initiate and...
established VIC
To elevate energy-flame temperature, fluid-displacement (46/47) is increased while non-combustible gas (45) volume flow is maintained or reduced, together with an increase in applied pulse voltage amp...
established VIC
U.S. Patent #4,826,581, issued May 2, 1989, covers the Electrical Polarization Process. Source: The Birth Of New Technology — In Summation
established VIC
U.S. Patent #4,936,961, issued June 26, 1990, covers the Resonant Cavity Voltage Intensifier Circuit (VIC). Source: The Birth Of New Technology — In Summation
established VIC
The Voltage Intensifier Circuit brings on the 'Electrical Polarization Process' that switches off the covalent bond of the water molecule without consuming amps. Source: The Birth Of New Technology —...
established VIC
Inductor (D) in relationship to inductor (C) electrically balances the opposite voltage electrical potential across voltage zones (E1) and (E2) within the Voltage Intensifier Circuit. Source: The Birt...
established VIC
The variable inductor-coil (D) has a movable wiper arm that allows fine tuning of the 'Resonant Action' during pulsing operations of the Voltage Intensifier Circuit. Source: The Birth Of New Technolog...
established VIC
Variable inductor-coil (D), similar to inductor (C), is connected to the opposite polarity voltage zone (E2), which further inhibits electron movement or deflection within the Voltage Intensifier Circ...
established VIC confidence 0.70
The voltage (VL) across the inductor (C) is given by equation (Eq 6), and the voltage (VC) across the capacitor is given by equation (Eq 7), describing the step-up relationship in the resonant circuit...
established VIC
At frequency close to resonance, the voltage across individual components (inductor C, capacitor ER) is higher than the applied voltage H, and at resonant frequency the voltage VT across both inductor...
established VIC confidence 0.70
The resonant frequency (F) of a series LC circuit is given by Eq 4, and Ohm's Law for the series LC circuit is also provided in the text (exact equation not transcribed). Source: The Birth Of New Tech...
established VIC
The value of the Inductor (C), the value of the capacitor (ER), and the pulse-frequency of the applied voltage across the LC circuit together determine the impedance of the LC circuit (Eq 1, series im...
established VIC
The established resonant frequency of the LC circuit is independent of voltage amplitude, as illustrated in Figure 1-3 as to Figure 1-4. Source: The Birth Of New Technology — LC Circuit
established VIC
The resonant frequency can be raised or lowered by changing the inductance and/or capacitance values of the LC circuit. Source: The Birth Of New Technology — LC Circuit
established VIC
The Inductance (C) and Capacitance (ER) properties of the LC circuit are tuned to resonance at a certain frequency. Source: The Birth Of New Technology — LC Circuit
established VIC
The Inductor (C) becomes a Modulator Inductor, stepping up an oscillation at a given charging frequency along with the effective capacitance of a pulse-forming network to charge the voltage zones (E1/...
established VIC
The Resonant Charging Choke (C) in series with the Excitor-Array (E1/E2) forms an inductor-capacitor (LC) circuit, since the Excitor-Array (ER) acts as a capacitor during pulsing operations (Fig 1-2,...
established VIC
An isolated electrical ground (J) prevents electron flow from the input circuit ground, maintaining electrical isolation within the pulsing transformer/VIC assembly. Source: The Birth Of New Technolog...
established VIC
Voltage amplitude or voltage potential is increased when the secondary coil (A) is wrapped with more turns of wire. Source: The Birth Of New Technology — Pulsing Transformer
established VIC
The primary coil is electrically isolated from the secondary coil (no electrical connection between them) to form the Voltage Intensifier Circuit (AA), as shown in Figure 1-1. Source: The Birth Of New...
established VIC
The pulsing transformer (A/G) steps up the voltage amplitude or voltage potential during pulsing operations within the Voltage Intensifier Circuit. Source: The Birth Of New Technology — Pulsing Transf...
established VIC
Electrical steel core material (53) forms a close-loop magnetic induction pathway centrally through and around the VIC coil-assembly (530), as schematically illustrated at (190) of Figure 3-23 (Memo W...
established VIC
Resonant bobbin assembly (503), primary bobbin assembly (504), and secondary bobbin assembly (506) structurally combine to form the Voltage Intensifier Circuit (VIC) coil-assembly (530), shown in Figu...
established VIC
Secondary bobbin cavity (506) is placed on top of and in spatial relationship to primary coil cavity (504). Source: The Birth Of New Technology — Tri - Coil Construction
established VIC
Secondary pickup coil (52) in Figure 3-23 is composed of individual spiral wrapped coils (505a...505n), typically .002 Ga. magnet wire, electrically connected in sequential order to form bobbin cavity...
established VIC
Primary Coil (26), typically .030 Ga. film coated magnet wire, is longitudinally wrapped in space relationship on top of and layered bidirectionally (507a...507n) across the spiral-wrap choke coils (5...
established VIC
The individual spiral-wrap coils (501a...501n) are electrically connected in sequential order to form the resistive pickup coil (503). Source: The Birth Of New Technology — Tri - Coil Construction
established VIC
The .004 Ga. (or smaller) 430F/430FR wire is axially (spiralled) bifilar wound about core bobbin (502), forming individual spiral-wrap coils (501a...501n) of equal length running from inner to outer c...
established VIC
Resonant Choke Coils (56/62) shown in Figure 3-23 (Memo WFC 422 DA) are composed of 430F or 430FR inductance stainless steel wire, film coated for high dielectric value, typically .004 gauge or smalle...
established VIC confidence 0.80
The 'Voltage Intensity of Opposite Potential' (600) generated by the VIC coil-assembly performs work to trigger the Hydrogen Fracturing Process (520), as referenced against (100) of Figure 4-8. Source...
established VIC
The design parameters of the VIC coil-structures (580) inherently determine 'Efficiency,' defined as minimizing amp leakage, which governs how the resulting Voltage Intensity of Opposite Potential (60...
established VIC
Activation Process (590) is achieved because amp flow is restricted from entering the Voltage Triggering Process (70) by way of the voltage intensifier coil-assembly (580). Source: The Birth Of New Te...
established VIC
All activation points (E9a-d) perform their functions in sequential order within an instant of time, since the applied voltage level of intensity, typically about 20,000 input volts, can be extended o...
established VIC
At activation point E9a, water flow is exposed to the voltage wave-form to begin water-to-energy conversion; at E9b voltage intensity is sufficient to perform the Electrical Polarization Process; beyo...
established VIC
The parallel sides (E9/E10) of the conical cavity function as a 'voltage wave-guide' and also act as a voltage intensifier circuit as the applied gated pulse-frequency travels the cavity length toward...
established VIC
The outer conical surface (E9) and inner conical surface (E10) form an open-air conical cavity (570) with parallel (or in other cases non-linear) voltage-surfaces spaced typically .010 gap apart, with...
established VIC
A calibrated gated unipolar pulse train (Fig 3-20) is outputted from the resonant choke (56) and electrically transmitted to the positive outer conical surface (E9), while negative voltage potential i...
established VIC
The resonant pulse-frequency is determined by the dielectric value of natural water in direct relationship to the resonant cavity's geometrical configuration; water's dielectric value is stated as 78....
established VIC
The incoming gated pulse-train (Fig 3-17) is electronically tuned to adjust pulse off-time (T2) to compensate for the rise and fall of magnetic field coupling, establishing a predetermined resonant pu...
established VIC
The voltage intensifier circuit (VIC) coil-assembly (580, Fig 6-1) is electrically interfaced with the 'Taper Resonant Cavity' (590, Fig 6-2), as schematically shown in Fig 3-22 relative to pulse core...
established VIC
The Voltage Intensifier Circuit is pulsed sensitive (49a xxx 49n) to tune into the dielectric properties of an airborne gas molecule, activating Covalent Switch-Off phenomenon (550) by restricting amp...
established VIC
The WFC Exhaust Air Reclaimer uses opposite electrical attraction force (RR'-SS') from voltage potential (Va xxx Vn) to separate the atoms of the Nitric Oxide NO molecule by overcoming the Electrovale...
established VIC
WFC Exhaust Air Reclaimer (900) of Figure (9-1) is similar in construction to Voltage Intensifier Circuit (110) of Figure (4-9), and is used to comply with the EPA Clean Air Act by eliminating Nitric...
established VIC
The repetitive polarity switching causes 'Particle Oscillation' functioning as an 'Energy Generator' through 'Physical Stress' undergoing pulsating 'Electrical Stress' whenever pulse switching cycles...
established VIC
When the (B+/B+ - B-/B- / 1030B) switch function is activated, switch terminals (T1/T2-T3/T4) are closed; switch position (T1/T4-T3/T2) reverses voltage polarity once switch function (T1/T2-T3/T4) clo...
established VIC
The circuit performs Voltage Switchover Logic Functions (B+/B+ 1030B ↔ B-/B- 1030A) of Figure 11-7 during each and every sequential voltage pulsing cycle (T4A-T4B-T4A-T4B and so on). Source: The Birth...
established VIC
Electrical Attraction Forces (S-S'/R-R') and Repelling Forces (T-T'/W-W') can be applied simultaneously or in a time sequence as the Electrical Crossover Switch Circuit (1060) reverses voltage polarit...
established VIC
The Electrical Crossover Switching Circuit (1060) singularly places either a Positive Voltage Potential (1014) across Voltage Zones E18/E14 and/or a Negative Voltage Potential across Voltage Zones E17...
established VIC
To reduce the number of VIC Circuits to a single VIC Coil Assembly (1003) while enabling a Voltage Repelling Force (W-W' and/or T-T'), the Electrical Crossover Circuit (1060) is electrically placed be...
established VIC
Varying the gated pulse-width (T4A/T4B), voltage amplitude (Vn), and Switchover pulse frequency rate (Sopr) collectively determines the rate at which water temperature rises as it travels through the...
established VIC
The electrical conductivity of T304 stainless steel together with water's dielectric property (water insulating against amp flow) sets up electrical conduction zone (587), allowing the voltage pulse w...
established VIC
The constructed tubular-array of the Differential Voltage Wave-Guide is composed of T304 stainless steel material (or equivalent), chosen for being chemically inert to the voltage deflecting process (...
established VIC
The Differential Voltage Wave-Guide (1040) is constructed with a smaller tube placed inside a much larger tube, with space between them to allow water to pass through, similar in construction to the l...
established VIC
Pairing positive zone (E13/952) with negative zone (E16/956), and (E14/953) with (E15/954), each of identical longitudinal axis length, forms the 'Differential Voltage Wave-Guide' (1040), defined by a...
established VIC
A completely separate Voltage Intensifier VIC-Coil Assembly (1003) is periodically switched on by alternate voltage pulse waveform (T4B) once T4A terminates for a brief period (T3A), redirecting the b...
established VIC
Voltage intensity at zones (952/953) is directly determined by the number of turns of each coil (957/958) relative to the applied voltage amplitude of the incoming pulse waveform (...xxx Vn). Source:...
established VIC
The distributed capacitance (Cda...Cdn) of each coil experiencing inductance coupling (619) elevates the applied voltage level (Vn) to a higher amplitude, increasing voltage intensity needed to deflec...
established VIC
The simultaneous formation of positive voltage field (952) and negative voltage field (953) results from mutual electromagnetic inductance coupling between the two bifilar wrapped coils (957/56-958/62...
established VIC
Both primary coil (957) and secondary coil (958) forming the voltage intensifier circuit (990) are bifilar wrapped in equal length, causing both water molecules to be displaced at the same velocity si...
established VIC
Simultaneously, stationary negative voltage field (958) at plate (953) attracts the positive hydrogen atom of a separate water molecule via R-R' attraction, displacing it in linear movement at the sam...
established VIC
Incoming programmable gated pulse-frequency waveform (T4A) electrically energizes primary input coil (957), producing positive voltage field (952) across voltage zone (E13), which deflects the negativ...
established VIC
The VIC Switchover Circuit (1010) prevents amp influxing into and away from the periodically spaced negative voltage zones (E13-E14, E15-E16), while allowing opposite-polarity voltage potentials to de...
established VIC
When the Voltage Intensifier Circuit (VIC Circuit, Fig 10-1) is electrically connected to Voltage Zones (66/E11–67/E12), it establishes the functional parameters of the Optical Thermal Lens (Fig 10-2)...
established VIC
The Amp Inhibiting Circuit (970, Figure 10-1) restricts/inhibits amp flow to a minimal level while elevating the Difference of Potential (electrical stress) to the highest possible level, since greate...
established VIC
In all cases, the bifilar coils (56/62 and SS56/62) are electromagnetically orientated in the same direction. Source: The Birth Of New Technology — Voltage to Amp Differential Ratio
established VIC confidence 0.80
The mutual inductance coil-field (Rp1+Rp2) causes coil capacitance (Cda...Cdn) to help maintain and increase pulse voltage amplitude, while the resistive value (Rs2) of the SS Coil-Wire further resist...
established VIC
Magnet coil-wire length is generally longer than the Stainless Steel coil-wire length, and the magnet bifilar-coil (56/62) is placed on top of the Stainless Steel bifilar-coil (SS56/62) to maximize mu...
established VIC
The magnet Coil-Wire (56/62) is best suited for voltage inducement, while the inductance/capacitance/resistance properties of Stainless Steel coil-wire (SS56-SS62) restrict electron movement beyond ea...
established VIC
Coil Stages (56/62a...56/62n + SS56/62a...SS56/62n) added/stacked sequentially into a single overall coil-array assembly (990A/B, Figure 10-3) form the Amp Inhibiting Network (970, Figure 10-1), herei...
established VIC
The Stainless Steel bifilar Coil-Stage Assembly (SS56/62a...SS56/62n) is electrically placed between the Magnet Coil-Stage Assembly (56/62a...56/62n) and the Water Gap (Cp) to obtain the optimum Volta...
established VIC
Stainless Steel composite coil-wire (430F/FR) has both inductance and resistive properties, typically 0.0048 ohms per foot, which combined aids amp restriction beyond what copper self-inductance magne...
established VIC
As additional Dual Choke Coils (56/62 + SS56/62) are stacked into the coil-array forming the Voltage Intensifier Circuit (970, Figure 10-1), amp-surge is kept to a minimal level while Voltage Potentia...
established VIC
Increasing the number of Resonant Charging Choke Stages (56/62 + SS56/62) added in sequential order increases energy yield, since the Multi-Coil Magnet bifilar coils are serially connected to an equal...
established VIC
Resonant Charging Choke Stages (56/62a...56/62n + SS56/62a...SS56/62n) are electrically connected in sequential order and magnetically linked by an Inductance Coupling field, producing the opposite-po...
established VIC
The programmable pulse-frequency (49a...49n, Fig 10-1) input is adjusted to tune-in to the dielectric property of the Water Molecule, enabling the Amp Inhibiting Circuit's Electrical Polarization Proc...
established VIC
Blocking Diode (52, Fig 4-9/1-1) allows the unipolar pulse-wave to go more positive on each pulse cycle by preventing the Resonant Cavity (Cp) from discharging during pulse off-time (Fig 1-4, 60 of Fi...
established VIC
The resultant voltage enhancement (Voltage Amplitude) of the VIC can exceed 40 kilovolts, instantly converting water droplets into thermal explosive energy on demand (Fig 10-1). Source: The Birth Of N...
established VIC
Pulse-Voltage repetition rate sets up a step-up charging effect (Fig 1-3) since the Resonant Cavity (Cp) functions as a Capacitor (ER) due to the dielectric value of the liquid (or gases) contained, w...
established VIC
The paired coil-wires' opposite voltage potentials (positive attraction force B+, negative attraction force B-), referred to as Electrical Stress (SS'-RR'), are always equal in electrical magnitude/in...
established VIC
Beyond amp restriction, the paired spiral-wrapped Resonant Charging Chokes (56/62) cause voltage level enhancement beyond applied voltage input, as the Distributed Capacitance (C1a...C1n, C2a...C2n) a...
established VIC
The VIC Bifilar Wrap Coil-Assembly (Fig 10-3B) and VIC Dual Coil Wrap-Assembly (Fig 10-3A) both utilize 'E', 'I', and 'U' inductance core configurations to concentrate Mutual Inductance Fields (Rp1/Rp...
established VIC
To reduce amp leakage further, the copper wire of both Resonant Charging Chokes (56/62) can be replaced with magnetically inductive stainless steel wire (430F/FR), which has a resistive value (Ohms) t...
established VIC
The length and diameter of the copper-wire spiral-wrapped coil pair (56/62, Fig 10-1), combined with the applied Voltage Pulse-Frequency, determines how much amp leakage occurs across the capacitor Ga...
established VIC
The mutual inductance field between paired chokes 56/62 prevents amp in-fluxing (discouraging electron arc-over) across the Dielectric Capacitor Gap (ER)(66/67) while Electrical Stress of opposite vol...
established VIC
The energized Resonant Charging Choke (56, Fig 7-1/10-1), driven by input voltage pulses (49a...49n), creates an electromagnetic coupling field (Rp1) via self-inductance (640, Fig 7-3B) that crosses t...
established VIC
The Amp Inhibiting Circuit (970, Fig 10-1; 690, Fig 7-8) is composed of two copper wires bifilar wound about a magnetic induction core, restricting amp (current) leakage while encouraging voltage pote...
established VIC
Pulse Off-time (T2, Figure 7-8, related to item 620 of Figure 7-1) is adjusted to compensate for the rise and fall of the magnetic coupling field (71), producing applied Unipolar Wave-forms (64a throu...
established VIC
Voltage Compressional Wave-form (35b) and Expanding Voltage Waveform (35c) increase the intensity of applied pulsating opposite electrical attraction force (SS'-RR'a through SS'-RR'n) further during e...
established VIC
The mode-of-operability of the VIC Coil Assembly (580, Figure 6-1) allows Voltage Potential (Vn) of opposite voltage polarity (66/SS' - 67/RR') to increase and be attenuated up to and beyond 20 kilovo...
established VIC confidence 0.80
The VIC circuit topology includes a Primary Coil (26) and a Secondary Coil (52), between which electrical power is transferred and maximized via the coil switching mechanism. Source: The Birth Of New...
established VIC
Switching the member of Secondary Coil-Array (505a–505n) maximizes electrical power transfer from Primary Coil (26) to Secondary Coil (52) by keeping the Voltage Amplitude of the Pulse-train (49a–49n,...
established VIC
The Taper Resonant Voltage surfaces (E9/10) of Figure 6-2 act and perform as a 'Voltage Amplifier' when the Compressional Wave-form (B) of Figure 7-12 is intensified at Exit Port (32) of Figure 6-2. S...
established VIC
Voltage levels of variance (Va–Vn) are achieved by switching-in or switching-out members of the Secondary Coil-cavities (505a–505n), shown at 740 of Figure 7-13, in direct relationship to the Taper Re...
established VIC confidence 0.80
In practical operation, a minute amount of amp leakage is present due to Electronic Component Limitations, but it is negligible to the overall performance of the Hydrogen Fracturing Process when subje...
established VIC
Electron Bounce Phenomenon, Voltage Coefficient of Inductance (FL1/FL2), Voltage Coefficient of Capacitance (Cd1/Cd2), Voltage Coefficient of Resistance (Rs1/Rs2), and the Dielectric Coefficient of Wa...
established VIC
The Electron Bounce Phenomenon (EbP) sustains and maintains the induced voltage potential without 'electron discharge' through Choke Coil (62), while simultaneously inhibiting additional electrons fro...
established VIC
Magnetic field coupling passing through the Secondary Coil-winding (52) dislodges electrons from copper atoms in the copper wire, producing positive copper ions that create positive voltage potential...
established VIC
The resultant dynamic voltage potential of difference is balanced in equal electrical intensity of opposite polarity because the Voltage Coefficient of Inductance (FL1/FL2), Voltage Coefficient of Cap...
established VIC
The total inductance of the Choke Coils (FL1, FL2) is derived with L1 and L2 (choke coils 56 and 62) in series with Secondary Coil (52), both exposed to the same Voltage Transformer (26-53-52) magneti...
established VIC confidence 0.80
Magnetic flux from the closed-loop pulsing core (53) penetrates inductance coil-windings (52, 56, 62) during each pulse on-time, with the pulse-train tuned to the dielectric property of water (Re), ca...
established VIC
The Capacitance Charging Effect (628) prevents amperage from influxing away from the Water Gap (Cp), and together with both Choke-Coils (56/62) conducting positive/negative voltage potential during pu...
established VIC
The Electron Inhibiting Effect causes 'Electron Clustering' to produce a Negative Voltage Potential (B-) at one side of the Water Gap (Cp); this occurs via low electrical power input when Choke-Coil (...
established VIC confidence 0.80
Aiding Inductance Fields (FL1-FL4) produce an Inductance Charging Effect and a Resonant Voltage Effect that interact with the dielectric properties of water (Re) to cause and inhibit electron flow (IF...
established VIC
The VIC Coil Assembly (580), comprising Inductor Coils (26, 52, 56, 62), is constructed and rotated so all coils share the same electromagnetic polarity orientation (indicator mark 'e'), allowing thei...
established VIC
The total inductance of the Choke Coils (Lt cc, fields FL1-FL2) is derived from the individual inductances of choke coils (56) and (62), in series with the Secondary Coil (52) voltage potential, with...
established VIC
Total inductance (La) of the Primary Coil (26) and Secondary Coil (52) is calculated with their fields aiding via Coupling Inductance (Rp), using individual coil inductances (L1, L2) and mutual induct...
established VIC
The impedance ratio of the VIC transformer is determined from the sum of the magnetic field strength (FL4) of the primary coil (26) and the induced magnetic field (FL3) of the secondary pickup coil (5...
established VIC
Secondary Coil-Wrap (52) is formed from turns of wire in each bobbin cavity (505), with the bobbin cavities electrically connected in series arrangement (505a-505n), each adhering to equation (Eq 20),...
established VIC
The turns ratio of the VIC Transformer (26/52) is determined by an equation relating Np (primary turns on spool cavity 504) to Ns (secondary turns summed in series across bobbin cavities 505a-505n for...
established VIC
Magnetic Induction (71a-71n) is determined by the Inductance Permeability (μL) of the core material (53) together with VIC circuit geometry, which together enable step-up of Voltage Potential (Vo-Vn)...
established VIC
The Secondary Pickup Coil-winding (52) has more turns of wire than the Primary Coil-winding (26), producing step-up transformer action via magnetic flux lines induced by pulsing of the Primary Coil. S...
established VIC
The Inductance Core (53) is composed of 'Grain Oriented' Electrical Steel laminations that step up applied voltage when magnetic field coupling crosses over from the Primary Coil-winding (26) to the S...
established VIC confidence 0.80
Total VIC 'Circuit Resistance' to D.C. current flow is expressed and determined by combining Rl (secondary pickup coil resistance), Z2 (choke-coil L1 impedance), Z3 (choke-coil L2 impedance), and Re (...
established VIC
Rl, the resistive value of Secondary Pickup Coil 52 (Figure 7-8), is combined with the magnetic field strength of primary coupling field 71 in direct relationship to inductance field strength Rp, whic...
established VIC
Coil-wraps 56 and 62 (choke coils L1 and L2) are Bifilar wound together onto a single spool-bobbin, giving each choke-coil the same impedance value. Source: The Birth Of New Technology — Circuit Resis...
established VIC
The two VIC choke-coils L1 (coil 56) and L2 (coil 62) are wound from stainless steel (s/s) wire, each with a typical resistive value of 11.6 KΩ, determined by inductance field strength (FL1, FL2) when...
established VIC
Inductors (L1/L2) should always have larger Reactance than Capacitor (ER, Figure 7-2) in order to maximize amp restriction, enhancing 'Voltage Deflection' (SS'-617a...617n-RR') shown in Figure 7-4. So...
established VIC
Plate Inductance (Lc) is the Inductance Reactance of Inductor (L1) and Inductor (L2) in series with the Resonant Capacitor (140-170 of Figure 7-6, corresponding to 690 of Figure 7-8). Source: The Birt...
established VIC
Capacitance Reactance is determined by the insulation resistance (Rs+Re) and Inductance (L1/L2) interacting together during D.C. Pulsing. Source: The Birth Of New Technology — Capacitance Reactance
established VIC confidence 0.80
(Eo), the Free-Space Permittivity of Water, is established by the VIC Circuit's ability to restrict amp flow; the ratio (e/Eo) is the Dielectric Constant of Water. Source: The Birth Of New Technology...
established VIC
The inductance formula uses N (number of turns), A (mean radius in inches), B (length of coil in inches), and C (depth of coil in inches), with L expressed in microhenries. Source: The Birth Of New Te...
established VIC confidence 0.80
By optimizing distributed capacitance (Cda...Coo) and distributed inductance (Dla...Dln), the coil's Inductance Field Strength (FLa...FLn) is intensified so the coil functions as a voltage multiplier...
established VIC
Inductance (L, in microhenries) of a multi-layer coil of rectangular cross section is computed from turns (N), mean radius (A, inches), coil length (B, inches), and coil depth (C, inches). Optimizing...
established VIC confidence 0.80
The text identifies a Secondary Pickup Coil (523) with a Length parameter denoted (FL3a xxx FL3n) as one of the factors influencing thermal explosive energy-yield from water. Source: The Birth Of New...
established VIC
Inductor (L1) acts and performs in like manner to Inductor (L2) since both Inductor (L1/L2) are physically the same size and shape. Source: The Birth Of New Technology — In-Line Circuit Components
established VIC
Inductance Reactance determines the voltage swing from the highest voltage level (Vn) to the volts switch-off point (Vff), and establishes Impedance (FL) which minimizes heat loss of electrical input...
established VIC
Inductance Reactance effectuates the 'Step Charging Effect' (680, per Figure 7-7) when the Pulse off-time (T2) is less than the Pulse on-time (T1). Source: The Birth Of New Technology — In-Line Circui...
established VIC
Inductance Reactance doubles the input frequency (64a * 64b) when a 50% Duty Cycle Pulse (T1 = T2) is inputted, while also increasing applied voltage amplitude (Vo-Vn). Source: The Birth Of New Techno...
established VIC
Inductance Reactance directly determines Stored Energy (Wa), which is controlled by the input Voltage Potential as attenuated or varied via Voltage Amplitude (Vo, Va, Vb-Vf, Vg-Vn, per Figure 7-13) an...
established VIC
Stored energy (Wa) in Joules (Watt-seconds) is a function of Inductance (L) in Henries and current (I) in amperes, per the stated energy relationship for Inductance Reactance. Source: The Birth Of New...
established VIC
Lengthening the Inductor (L1/L2) lengths applies an even higher Voltage Potential (66/67) across the Resonant Capacitor (140-170, labeled ER), because Inductance Reactance stores energy. Source: The B...
established VIC
The electromagnetic coupling fields encourage the Voltage Inducement Process across the VIC Impedance Network Circuit without amp 'influxing' (i.e., inhibiting amp flow) between the Positive Voltage P...
established VIC
The Electron Inhibiting Effect combined with the Voltage Enhancement Effect is achieved because stainless steel 430F/FR wire-material is electromagnetically inductive to incoming flux lines without th...
established VIC
At elevated voltage amplitudes, the primary electromagnetic coupling field (Rp), transmitted via the Inductance Pulsing-Core through the VIC Coil Assembly, passes through both Inductors L1 and L2 simu...
established VIC
The blocking action of L2's field prevents and inhibits electron flow from passing through or arcing over the capacitor water-gap (Cp); this is termed the 'Electron Inhibiting Effect' (631). Source: T...
established VIC
Inductance Field L1-FL1 performs the 'Capacitance Charging Effect' (628), while at the same time Inductor Field L2-FL2 restricts electron movement through the VIC Impedance Network Circuit by locking...
established VIC
Adjusting the programmable pulse-waveform input signal frequency 'tunes-in' to the dielectric property (Re) of water, reducing amp flow to a minimum while allowing voltage potential to rise toward inf...
established VIC
Both Inductors L1 and L2 are bifilar wound in equal length so their electromagnetic field intensities are equal (FL1 = FL2), promoting the 'Electron Bounce' phenomenon. Source: The Birth Of New Techno...
established VIC
Inductors L1-L2 (Figure 7-6), placed on opposite sides of the water-capacitor ER, act as Resonant Charging Chokes (614/615) and together form the Resonant Voltage Effect Circuit (670). Source: The Bir...
established VIC
Inductance Reactance occurs when resistance (Rs), capacitance (Cd), and Inductance (FL) interact during D.C. Pulsing, increasing voltage across the water-capacitor (ER) beyond the applied Voltage Pote...
established VIC
All dielectric coatings on the VIC wire have an effective 3KV per mil dielectric value and are formulated to endure the automotive temperature range from -40°C to 155°C. Source: The Birth Of New Techn...
established VIC
Both magnet wire sizes (622/623), the Primary and Secondary Pickup Coils, use solderable Nysol (Polyurethane Nylon Jacket) insulation enamel coating as an electrical shield-material. Source: The Birth...
established VIC
The stainless steel resonant charging choke wire (614/615) is coated with the 'Pyre-ML' trade name 'Himol' polymer coating-material to impart thermal and mechanical resistance. Source: The Birth Of Ne...
established VIC
The Secondary Pickup Coil (623) of the VIC uses 35 AWG (.007 in) copper wire equal to 13K ohms per pound weight. Source: The Birth Of New Technology — Capacitance (Cd)
established VIC
The Primary Coil (622) of the VIC uses 22 AWG (.028 in) copper wire equal to 5.1933 ohms per pound weight. Source: The Birth Of New Technology — Capacitance (Cd)
established VIC
Resonant Charging Chokes (614/615) are made of 430F/FR 36 AWG (.006 in) stainless steel (s/s) wire, which equals 60 micro ohms per centimeter. Source: The Birth Of New Technology — Capacitance (Cd)
established VIC
The series resistance value (Rs) of the VIC choke/coil windings is determined by the composition of the wire material in terms of its ohmic value (electrical resistivity) per given length and diameter...
established VIC
The circular-spiral turns of wire in the VIC choke, forming parallel electrical surfaces, are separated by an Insulated Dielectric Coating Material which forms a series of capacitors (Cda-Cdn) when ma...
established VIC
Inductors (614) and (615) of the VIC are wound or coil-wrapped, per the multi-layer equation (Eq. 20), to increase magnetic flux intensity between the turns (618a-618n) of the coil-wrap (640). Source:...
established VIC
Distilled water is generally lab-tested at 1 ppm or less contamination, as illustrated in Figures (7-15) and (7-14). Source: The Birth Of New Technology — Inductance (FL)
established VIC
Electron interaction (movement of electrons through the liquid medium of water) is further inhibited since natural water contaminants (144a...144n) are normally less than 20 ppm. Source: The Birth Of...
established VIC confidence 0.80
The stabilized water molecule structure (85) maintains molecular stability by opposing the exchange of electrons from an external electron source (amp-inducing circuit) beyond its molecular structure....
established VIC
The established Dielectric Value of Water (85) is 78.54 ohms, attributed to the electron 'L' orbit of the water molecule occupying the maximum allowable eight electrons upon covalent linkup of one oxy...
established VIC
Distributed Capacitance (Cda...Cdn) and Distributed Inductance (D1a...D1n) of Inductor Coil (614) interact with the dielectric value of the water bath (85/Re), producing the 'Electrical Charging Effec...
established VIC
Component Reactance to D.C. pulsing transforms the Inductor (614)/Capacitor (E9/E10) LC circuit into a Resonant Charging Choke, which steps up a unipolar oscillation at a given charging frequency, usi...
established VIC
Capacitor (E9/E10) as to (720) of Figure (7-11) is formed when outer tapered surface (66) and inner tapered surface (67) create Water-Gap (616), with Dielectric Water Bath (85/Re) placed between them,...
established VIC
Inductor (614) is an insulated wire wound in a spiral pathway around Bobbin Cavity (580) of Figure (6-1) to form the Voltage Stepping Coil (710) of Figure (7-10). Source: The Birth Of New Technology —...
established VIC
Resonant Charging Circuit (630) of Figure (7-2) is an LC circuit formed when Inductor (614) of Figure (7-1) is electrically linked in series with Taper Capacitor (720) of Figure (7-11). Source: The Bi...
established VIC
Applied opposite Voltage potential (ST-ST' to RU-RU') performs work without amp "influxing," as systematically depicted in the VIC Matrix Circuit (690). Source: The Birth Of New Technology — Resistanc...
established VIC confidence 0.80
The dielectric value of Water (Re) is a functional part of the Voltage Intensifier Circuit (110 of Figure 4-9), contributing to its capability of restricting amp flow during Voltage Pulsing Operation...
established VIC
While restricting current, the stainless steel coil-wrap simultaneously conducts and transmits Voltage Potential across its circumference surface area (skin effect) (66/67 of Figure 7-11, referencing...
established VIC
Because of the atomic composition of the stainless steel wire material (Rs1/Rs2), electron interaction/interchange between atomic structures is opposed, restricting current flow to the milliampere ran...
established VIC
The stainless steel (s/s) coil-wrap (614/615) resistive wire value (Rs1/Rs2) shown in Figure 7-8 is typically 11.6K ohms per coil, an amount sufficient to inhibit current flow oscillation in relation...
established VIC
The output voltage-wave signal (64a-64n) is a pulse-frequency doubler due to the Inductance Reactance (FL) of Inductor Coil (56, Figure 3-22): when the magnetic field (FL, Figure 7-3b) collapses, it r...
established VIC
A gated pulse-frequency pulse-train (64a/64b - T3 - 64a/64b) forms when pulse off-time (T3) is greater than time-period (T2); the input pulse-train (49a-49n) off-time (T2) is adjusted to allow the Uni...
established VIC
Diode (55) is placed between the Secondary Pickup Coil (52) and Resonant Charging Choke (56) to act as an electronic switch in the open position during pulse off-time (T2, Figure 7-8), preventing reve...
established VIC
Switching Diode (55, Figure 3-22) prevents bidirectional electron flow (current flow in one direction only) since the Blocking Diode only conducts current in the direction of the schematic arrow, plac...
established VIC
The VIC-VB circuit (620, Figure 7-1) allows reduction of Capacitor-Gap (Cp) (616, Figure 7-11) width spacing (57 of Figure 3-25 ~ 35 of Figure 6-2), typically .060 to .010, as illustrated in the Tubul...
established VIC
VIC Voltage Enhancement Circuit (VIC-VB) (620, Figure 7-1) incorporates stainless steel wire-wrap coils (614/615) to form a unipolar gated pulse-wave (64a...T3...64n) without signal distortion or degr...
established VIC
VIC voltage circuit (60) utilizes copper wire-wrap to form Resonant Charging Chokes (56/62, Figure 3-22) in conjunction with Switching Diode (55) to encourage the 'Electron Bounce' phenomenon (700, Fi...
established VIC
Voltage Intensifier Circuit (60) of Figure 3-22 (Memo WFC 422 DA / WFC 420) and Voltage Intensifier Circuit (620) of Figure 7-1 are both specifically designed to restrict amp flow during Programmable...
established VIC
The Voltage Intensifier Circuit takes advantage of the 'Electron Bounce Phenomenon' to trigger the Hydrogen Fracturing Process without amp influxing, and the Taper Resonant Cavity functions as a Volta...
established VIC confidence 0.80
The operational parameter of the VIC utilizes 'Opposite Electrical Attraction Force' of high voltage intensity to instantly release thermal explosive energy (gtnt) from natural water. Source: The Birt...
established VIC
The mode-of-operability of the VIC Coil Assembly allows voltage potential of opposite polarity to increase and be attenuated up to and beyond 20 kilovolts while inhibiting and restricting amp leakage...
established VIC confidence 0.80
The "Mode of Operability" of the VIC Coil Assembly is systematically activated by a programmable signal input, indicating the circuit's operation is controlled via a programmable driving signal. Sourc...
established VIC
By simply altering the Voltage Wave Guide to form either a "compressional" or "Expanded" Voltage Wave Form, the Water Fuel Injector increases electrical voltage intensity beyond the applied excitation...
established VIC confidence 0.80
The Water Fuel Injector is interlinked with the VIC Coil Assembly and acts and performs as a "Voltage Amplifier" by altering the Voltage Wave Guide. Source: The Birth Of New Technology — VIC Matrix Ci...
established VIC
The Voltage Intensifier Circuit takes advantage of the "Electron Bounce Phenomenon" to trigger the Hydrogen Fracturing Process without amp influxing, meaning water dissociation occurs via voltage effe...
established VIC
The VIC Coil Assembly is specially designed to allow a voltage potential of "opposite electrical attraction force" at high voltage intensity to instantly release thermal explosive energy (gtnt) from n...
established VIC
The Voltage Intensifier Circuit (110) brings on the 'Electrical Polarization Process' (160) that switches off the covalent bond (550) of the water molecule without amp influxing. Source: The Birth Of...
established VIC
Resonant Action (point of particle oscillation) occurs when the applied pulse voltage frequency (item 46, Figure 5-5) is adjusted to 'tune-in' to the Dielectric Resonance of water via the Voltage Inte...
established VIC
The Voltage Intensifier Circuit brings on the Electrical Polarization Process that switches off the covalent bond of the water molecule without amp influxing. Source: The Birth Of New Technology — Usi...
established VIC
In the Rotary Crossover Voltage Sync-Pulse Circuit (850), each of the three VIC Pickup Coils (52A, 52B, 52C) are axially spaced 120° apart, causing Convergent Point 'Q' to be located 1/3 the height of...
established VIC
To maintain the Capacitance Charging Effect across the Water-Gap (Cp) during applied pulsing operations, a Crossover Voltage Wave-Form (780B/780C) is used, preventing Convergent Point 'Q' from reachin...
established VIC
Blocking Diode (618) functions as an Electrical Isolator that prevents electrical discharge of the Dual Secondary Coil (616A/B) during applied Pulsing Operations. Source: The Birth Of New Technology —...
established VIC
Amp Inhibiting Coil-Assembly (617) is made of magnetic inductance Stainless Steel 430FR wire material wrapped around a closed-loop Induction Magnetic Core (619), forming a separate coil-unit (860) apa...
established VIC
Balance Phasing of opposite voltage intensity (+Vpp/-Vpp) is accomplished without current influxing caused by differential variances between Negative Voltage Peak Potential (-Vpp) and Positive Voltage...
established VIC
Amp Inhibitor Circuit (860), consisting of Amp Inhibiting Coil (617), Blocking Diode (618), and Magnetic Induction Core (619), is placed between electrical ground (0V) and the Center Tap of Dual Bifil...
established VIC
Dynamic State Space causes the Opposite Electrical Attraction Force (RR'-SS') to continually vary in intensity, forming a Voltage Peak Curve (Vpc); Static State Space allows the Opposite Attraction Fo...
established VIC
Static State Space voltage pulse shaping (clipped waveform) is produced by way of the Programmable Pulsing Circuit (WFC project 422DA/423DA) electrically interfaced with the VIC Matrix Circuit (690),...
established VIC
'Dynamic State Space' exists when the Voltage Excursion Point 'P' is always changing in a given space-time; 'Static State Space' exists when Point 'P' remains constant during a precise period at Peak...
established VIC
Equalizing Voltage Pulse-Scan (Bps) from the start of one Voltage Pulse-Field (Vpf) to the start of the next is determined by the total average number of applied Voltage-Pulses (Vp ave.) making up the...
established VIC
The intensity of the Opposite Electrical Attraction Force (RR'-SS') is directly related to the applied Voltage Amplitude Burst-Time (Vpa-Vn-Vpb), the Voltage Burst-Frequency (49a...49n), and the Volta...
established VIC
Each Voltage Pulse duration time-period (T1 on-time) is directly related to the applied Voltage-Pulse Amplitude (Vo...Vn) and the reoccurring Voltage Pulse Frequency (49a...49n), together forming the...
established VIC
The Secondary Voltage pickup coil (52) of Figure 7-8 displaces and separates the Resonant Charging Chokes (56/62), positioning them on opposite ends of the Secondary Pickup Coil. Source: The Birth Of...
established VIC
The opposite negative Voltage Pulse Train (67, 602a...602n) is formed by the 'Electron Clustering Effect' (631) of Figure 7-9, producing a Negative Electrical Voltage Intensity (67) equal in magnitude...
established VIC
In the inactivated electrical state, the VIC Matrix Circuit (690) behavior is governed by Circuit Resistance Equations (Eq. 9), which allow the positive Voltage Pulse-Wave (583) to be duplicated in su...
established VIC
Because the two Resonant Charging Chokes have matched resistive values, coil-ringing is prevented during each pulse off-time, allowing the Electron Bounce Phenomenon (EbP) to occur without amperage in...
established VIC
Both Resonant Charging Chokes (56/Z2 and 62/Z3) have the same resistive value, typically 11.6 kΩ each, which keeps the leading edge (Vpa) and trailing edge (Vpb) of the unipolar Voltage Pulse-Wave uni...
established VIC
The Voltage Intensifier Matrix Circuit, electrically connected with the resistive liquid (water, Re), forms a Resonant Water Gap referred to as 'Cp', and propagates the Traveling Voltage Wave-Form acc...
established VIC
The dielectric property of water (85), resistance to electron flow, in conjunction with the VIC Coil Matrix Circuit and VIC Coil Assembly, inhibits amp 'influxing' (Electron Bounce Phenomenon, EbP) du...
established VIC
The voltage intensifier circuit 12 regulates voltage amplitude, pulse frequency and gated pulse frequency associated with operation of the fuel cell 7, and is interconnected to the gas management modu...
established VIC
The circuit of Figure 9 enhances voltage potential across the resonant charging choke coils during pulsing by allowing an external electromagnetic pulsing field F, from energized primary coil A, to tr...
established VIC
A voltage intensifier circuit (Figure 7) is used as a current restricting voltage source to provide excitation voltage to the resonant cavity, sustaining atomic elongation of gas ions before ignition,...
established VIC
Figure 4's control means directs 0-12 volts across the primary coil of the pulsing core, and depending on core design parameters, the secondary coil can be set up for a predetermined maximum voltage s...
established VIC
Assuming a resonant pulse of 5 KHz, a 0.5 Hz gate pulse may be superimposed to provide 2500 discrete pulses in a 50% duty cycle per Hz, illustrating how the gate pulse frequency generator (Figure 6) c...
established VIC
In the VIC pulsing core, the coils are preferably wound in the same direction to maximize the additive effect of the electromagnetic field, and the transformer core acts as a pulse frequency doubler....
established VIC
The high speed switching diode used in the VIC circuit (Figure 10) prevents charge leakage from the water capacitor and ensures uni-polar pulses without discharging the capacitor; a 600 PIV fast switc...
established VIC
Voltage to the water capacitor cell increases according to coil turns and size as in a standard transformer; for example, 12 volts to the primary coil with a 30:1 secondary/resonant-charging-choke tur...
established VIC
A pickup coil on the ferromagnetic/electromagnetic transformer core senses the resonant condition of the water capacitor and is interconnected to a scanning circuit and phase lock loop (PLL) circuit t...
established VIC
The pulse generation means includes an adjustable first resonant frequency generator and a second gated pulse frequency generator; the gate pulse controls the number of resonant-frequency pulses sent...
established VIC
The secondary (TX2) transformer is connected to the resonant cavity water capacitor cell via a high speed switching diode and resonant charging chokes (TX4, TX5), forming a closed loop circuit that us...
established VIC
The circuit of FIG. 9 enhances voltage potential across the resonant charging choke coils by allowing an external electromagnetic pulsing field (F), derived from primary coil A being energized, to tra...
established VIC
A voltage intensifier circuit such as shown in FIG. 7 is used as a current-restricting voltage source to provide the excitation voltage applied to the resonant cavity, sustaining atomic elongation pri...
established VIC
The wiper arm on the second inductor tunes the circuit and accommodates to contaminants in water so that charge is always applied to the capacitor (the water cell). Source: US Patents — Process & Appa...
established VIC
As pulse frequency is adjusted to achieve resonance, amp flow is minimized while voltage is maximized to a peak; the resonant frequency of a given cavity depends on water dielectric parameters, plate...
established VIC confidence 0.80
An alternate coil arrangement using a conventional M27 iron transformer core is shown in FIG. 9, with the coil wrap always in one direction only. Source: US Patents — Process & Apparatus For The Produ...
established VIC
The overall circuit is characterized as a 'resonant charging choke' circuit — an inductor in series with the water capacitor forming a resonant circuit — with such a resonant charging choke placed on...
established VIC
The primary coil of the toroid is subjected to a 50% duty cycle pulse; the first inductor following the toroid is formed from 100 turns of 24 gauge wire, 1 inch in diameter, and when the pulse ends it...
established VIC
In the circuit of FIG. 2, an IN1198 diode acts as a blocking diode/electric switch allowing voltage flow in one direction only, so the capacitor is never subjected to reverse polarity; the diode also...
established VIC
The step-up coil is wound on a toroidal core of compressed ferromagnetic powder (Ferramic Q6 'Permag' powder) that will not permanently magnetize; the core is 1.50 inch diameter and 0.25 inch thick, w...
established VIC
The wiper arm on the second inductor tunes the circuit and accommodates to contaminants in the water so that charge is always properly applied to the water capacitor. Source: US Patents — Method For T...
established VIC
The overall circuit is a 'resonant charging choke' circuit — an inductor in series with the water capacitor forming a resonant circuit — with such a resonant charging choke placed on each side of the...
established VIC
The stepped-up pulse enters a first inductor formed from 100 turns of 24 gauge wire, 1 inch in diameter, around which an electromagnetic field forms; when voltage switches off at pulse end, the field...
established VIC
The primary coil of the toroid is subjected to a 50% duty cycle pulse; the toroidal pulsing coil provides a voltage step-up from the pulse generator in excess of five times, with actual step-up ratio...
established VIC
A 1N1198 diode in the circuit acts as a blocking diode/switch allowing voltage flow in one direction only, so the capacitor is never subjected to reverse polarity; the diode also allows the inductor's...
established VIC
The step-up coil is formed on a toroidal core of compressed ferromagnetic powdered material (e.g. 'Ferramic Q6 Permag' powder), 1.50 inch in diameter and 0.25 inch thick, with a primary coil of 200 tu...
calculation VIC confidence 0.60
The WFC operates in the fully reactive region of the VIC circuit.