Step Charging
Step-Charging Ladder Effect
Step-charging, also known as the "staircase" or "ladder" effect, refers to the progressive buildup of voltage across a capacitor through successive resonant pulses. This technique can achieve voltage levels far beyond what single-pulse resonant charging provides.
The Concept
Instead of maintaining continuous oscillation, step-charging applies discrete pulses that each add a quantum of energy to the capacitor. The voltage builds up incrementally:
Voltage
↑
│ ┌───
│ ┌───┘
│ ┌───┘
│ ┌───┘
│ ┌───┘
│ ┌───┘
│ ┌───┘
│ ┌───┘
│─┘
└─────────────────────────────────────→ Time
↑ ↑ ↑ ↑ ↑ ↑ ↑ ↑ ↑
Pulse Pulse Pulse ...
1 2 3
Each pulse adds approximately 2×V_source to capacitor voltage
(in ideal lossless case with unidirectional diode)
How Step-Charging Works
Step-by-Step Process:
- Pulse 1: Capacitor charges from 0 to 2Vs (resonant half-cycle)
- Hold: Diode prevents discharge back through inductor
- Pulse 2: Starting from 2Vs, capacitor charges to ~4Vs
- Hold: Energy stored, waiting for next pulse
- Continue: Each pulse adds ~2Vs (minus losses)
Circuit for Step-Charging
Switch
V_s ──○/○───┬───────────────┬────▶│────┬────
│ │ D │
│ ┌─────┐ │ ─┴─
│ │ L │ ─┴─ ─┬─ C (WFC)
│ └──┬──┘ ─┬─ │
│ │ │ │
───────────┴───────┴───────┴────────────┴────
D = Diode prevents reverse current
C charges in discrete steps
Voltage After N Pulses
Ideal Case (no losses):
VC,N = 2N × Vsource
With Losses (exponential decay factor):
VC,N = 2Vs × Σ(e-π/(2Q))k for k=0 to N-1
Converges to Maximum:
VC,max = 2Vs / (1 - e-π/(2Q))
For high Q: VC,max ≈ (4Q/π) × Vsource
Maximum Voltage vs. Q Factor
| Q Factor | Vmax/Vsource | Pulses to 90% |
|---|---|---|
| 10 | ~12.7 | ~6 |
| 20 | ~25.5 | ~12 |
| 50 | ~63.7 | ~30 |
| 100 | ~127 | ~60 |
Comparison: Continuous vs. Step Charging
| Aspect | Continuous Resonance | Step Charging |
|---|---|---|
| Max voltage | Q × Vs (AC peak) | (4Q/π) × Vs (DC) |
| Waveform | Sinusoidal | Staircase |
| Power delivery | Constant | Pulsed |
| Complexity | Simpler | Needs diode/timing |
Step-Charging in VIC Systems
Meyer's designs allegedly used step-charging principles:
- Unidirectional charging: Diode prevents energy return to source
- Pulse timing: Gated pulses at resonant frequency
- Voltage accumulation: Progressive buildup across WFC
- Controlled discharge: Occasional reset or bleed-off of accumulated voltage
Pulse Train Design
Optimal Pulse Parameters:
- Pulse duration: π√(LC) = half resonant period
- Pulse frequency: fpulse < fresonant/2
- Duty cycle: Typically 10-50%
- Gap between pulses: Allow ring-down and settling
Energy Considerations
Energy Stored After N Pulses:
EC,N = ½C(VC,N)² = ½C(2NVs)² = 2CN²Vs²
Energy Delivered per Pulse:
ΔE = EC,N - EC,N-1 = 2CVs²(2N-1)
Each successive pulse adds more energy because it's working against a higher voltage!
Practical Implementation
Driver Circuit Requirements:
- High-speed switching: MOSFET or IGBT driver
- Precise timing: Microcontroller or pulse generator
- High-voltage diode: Fast recovery, rated for expected voltages
- Voltage monitoring: Feedback to prevent over-voltage
Safety Considerations:
- Voltages can reach dangerous levels quickly
- Energy stored in capacitor can be lethal
- Include bleed resistor for safe discharge
- Implement hardware over-voltage protection
VIC Matrix Simulation
The VIC Matrix Calculator can simulate step-charging behavior:
- Step-charge simulation: Predicts voltage after N pulses
- Loss modeling: Accounts for resistance and dielectric losses
- Time to saturation: How many pulses to reach maximum voltage
- Energy efficiency: Tracks energy delivered vs. stored
Key Insight: Step-charging combines the voltage doubling of resonant charging with the cumulative effect of multiple pulses. With sufficient Q factor, extremely high voltages can be developed across the WFC—voltages that would be impossible to achieve directly from the source.
Chapter 4 Complete. Next: Choke Design & Construction →