Black Hole Injector Instant

For a BH of mass ( M ), the Hawking luminosity is: [ P_\textH = \frac\hbar c^615360 \pi G^2 M^2 \approx 3.6 \times 10^32 \left( \frac10^6 \textkgM \right)^2 \textW ]

A linear accelerator (1 TeV) injects protons tangentially into the ergosphere. The injector uses a pulsed neutron beam to avoid Coulomb repulsion. Injection rate ( \dotm ) is tuned such that the BH’s mass remains constant: [ \dotM \textBH = \dotm \textin - \fracP_H + P_\textjetc^2 = 0 ] black hole injector

| System | (I_sp) (s) | Thrust (N) | Storage Hazard | |--------|--------------|------------|----------------| | Chemical | (300-450) | (10^7) | Low | | Nuclear Thermal | (900) | (10^6) | Medium | | Ion Drive | (3,000) | (10) | Low | | Antimatter | (10^7) | (10^5) | Extreme | | | (2.4 \times 10^7) | (10^7) | Extreme (but passive) | For a BH of mass ( M ),

This paper proposes a novel propulsion concept, the Black Hole Injector (BHI), which utilizes a primordial or artificially generated microscopic black hole (BH) as a catalyst for complete mass-to-energy conversion. Unlike conventional matter-antimatter engines, the BHI operates by injecting baryonic matter into a stable, electrically charged, rotating black hole (Kerr-Newman metric). Through Hawking radiation and superradiant scattering, the BH re-emits up to ~40% of the injected rest mass as directed high-energy gamma rays and relativistic plasma jets. We derive the thermodynamic limits, stability criteria (the "sphericity constraint" to avoid runaway evaporation), and a theoretical specific impulse (I_sp > 10^7 , s). The BHI circumvents the antimatter storage problem by using ordinary hydrogen as fuel. We conclude with a feasibility analysis of containment using nested magnetic and gravitational shields. The BHI circumvents the antimatter storage problem by