# Fusion Gain Factor (Q) — First Principles Breakdown
## 1. What is Q?
**Q** is the **fusion energy gain factor**:
Q = Pfus / Pinput
- `Pfus` = Fusion power produced
- `Pinput` = External power used to heat and sustain the plasma
**Breakeven (scientific)** happens at **Q = 1**, where fusion power equals input heating power.
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## 2. Where Does the Input Power Go?
- Heating the plasma to fusion conditions
- Compensating for energy losses (radiation, conduction, particle escape)
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## 3. Where Does the Fusion Power Go?
Fusion energy comes out as:
- **Charged particles (e.g., alpha particles)**
→ Stay in plasma → contribute to **self-heating**
- **Neutrons**
→ Escape plasma → hit external blanket → converted to heat
**Key point:**
Only ~20% of D-T fusion energy (from alphas) can self-heat the plasma. The rest is available for generating electricity.
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## 4. Breakeven Types
| Type | Meaning | Q Value |
|-----------------------|-------------------------------------------------------|------------------|
| **Scientific** | Pfus = Pinput (just plasma heating) | Q = 1 |
| **Engineering** | Reactor powers its own heating systems via electricity| Q ≈ 5–8 (MCF) |
| **Ignition** | No external heating needed | Q → ∞ |
| **Commercial** | Reactor earns back costs (ops, fuel, capex) | Q ≥ 20–25 (varies)|
| **Extrapolated** | Performance if using tritium, based on test fuel | — |
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## 5. Why Q ≈ 5 Is Needed for Ignition (D-T Fuel)
Only 20% of fusion energy stays in plasma as alpha particles.
To fully self-sustain heating:
Self-heating = External heating → Q = 1 / 0.2 = 5
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## 6. Power Conversion and Recirculation Losses
Real systems have efficiency limits:
- `ηheat` = Efficiency of plasma heating (~0.7)
- `ηelec` = Heat-to-electric conversion (~0.4)
- `frecirc` = Fraction of electricity sent back to heating (~0.2)
- `fch` = Fraction of fusion energy in charged particles (~0.2 for D-T)
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## 7. Engineering Breakeven Formula
To reach **Qeng = 1**:
Qeng = 1 / (ηheat × ηelec × frecirc × (1 - fch))
Using typical values:
Qeng = 1 / (0.7 × 0.4 × 0.2 × 0.8) ≈ 22
So you need **Q ≈ 22** for a real power plant to sustain itself with internal electricity recirculation.
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## 8. Summary
- **Q = 1** → Scientific breakeven (proof of concept)
- **Q ≥ 5** → Plasma self-heats (ignition)
- **Q ≥ 10–20** → Net electricity possible
- **Q ≥ 22+** → Realistic engineering breakeven with recirculation losses
> Q is necessary, but not sufficient. Reactor economics depend on recirculation, conversion efficiency, fuel availability, and capex.
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## Bonus: Terms Recap
- **Scientific breakeven**: Q = 1
- **Engineering breakeven**: Enough electricity to power own heaters
- **Ignition**: Self-heating replaces all external heating
- **Extrapolated Q (Qext)**: Estimated Q if using tritium
- **Commercial breakeven**: Reactor pays for itself economically
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## Example (ITER-like Reactor)
- Fusion output: 500 MW
- Input power: 50 MW
- Q = 10
- 20% (100 MW) used for self-heating
- 400 MW available for extraction
- With ηheat = 0.7, ηelec = 0.4
- Up to ~112 MW electricity generated
- Can hit engineering breakeven if recirculation demand <112 MW