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Deflection Methods
SpaceEngineerSS edited this page Dec 18, 2025
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CosmoRisk supports three asteroid deflection techniques based on real planetary defense research.
Principle: High-velocity spacecraft collision transfers momentum to the asteroid.
Δv = (m_spacecraft / m_asteroid) × v_impact × (1 + β)
Where β (beta factor) accounts for ejecta momentum enhancement (typically 1-5).
- Select asteroid
- Set impactor mass (kg)
- Set impact velocity (km/s)
- Set beta factor
- Click "Apply Deflection"
- DART Mission (2022): NASA's test on Dimorphos
- Impactor: 570 kg at 6.6 km/s
- Result: 32-minute orbital period change
Principle: Continuous low-thrust beam slowly pushes asteroid over time.
Δv = F_thrust × t / m_asteroid
- No contact required
- Continuous adjustment
- Works over months/years
- Select asteroid
- Set thrust magnitude (mN)
- Set direction vector
- Set duration (days)
- Click "Apply Ion Beam"
Principle: Spacecraft hovers near asteroid; mutual gravity slowly deflects both.
F = G × m_spacecraft × m_asteroid / r²
- No physical contact
- Works on rubble piles
- Very precise control
- Requires years of operation
- Limited to small deflections
- Spacecraft mass: 1,000 - 20,000 kg
- Hover distance: 50 - 200 m
- Lead angle: 0° - 45°
| Δv Required | Lead Time | Deflection @ Earth |
|---|---|---|
| 1 cm/s | 10 years | ~1 Earth diameter |
| 1 mm/s | 20 years | ~1 Earth diameter |
| 10 cm/s | 1 year | ~1 Earth diameter |
Key Insight: Early detection = smaller required Δv!
| Factor | Impact |
|---|---|
| Asteroid size | Larger = harder to deflect |
| Density | Unknown for most NEOs |
| Rotation | Affects gravity tractor positioning |
| Orbit uncertainty | Monte Carlo analysis needed |
| Method | Speed | Precision | Technology Readiness |
|---|---|---|---|
| Kinetic Impactor | Fast | Low | TRL 9 (DART proven) |
| Ion Beam | Slow | High | TRL 4-5 |
| Gravity Tractor | Very Slow | Very High | TRL 3-4 |