SUMMARY
The discussion focuses on the effects of Hawking Radiation on black holes, specifically how mass and temperature change over time. The Bekenstein–Hawking formula, $$S=\frac{kAc^3}{4G\hbar}$$, is central to understanding these changes. For a Schwarzschild black hole, mass can be calculated using $$M^2=\frac{\hbar c^3}{4\pi k_{\rm B} G}S$$, while temperature is derived from the relationship $$T=\frac{{\rm d} M}{{\rm d} S}=\frac{\hbar c^3}{8\pi k_{\rm B}G}\frac{1}{M}$$. The Stefan-Boltzmann law $$\frac{{\rm d}M}{{\rm d}t}=-\sigma AT^4$$ further illustrates the exponential decay of mass and the corresponding increase in temperature over time.
PREREQUISITES
- Understanding of black hole thermodynamics
- Familiarity with the Bekenstein–Hawking formula
- Knowledge of the Stefan-Boltzmann law
- Basic calculus for differentiation and integration
NEXT STEPS
- Study the Bekenstein–Hawking entropy and its implications for black hole thermodynamics
- Explore the derivation and applications of the Stefan-Boltzmann law in astrophysics
- Learn about Schwarzschild black holes and their properties
- Investigate the implications of Hawking Radiation on black hole evaporation
USEFUL FOR
Students of physics, astrophysicists, and researchers interested in black hole thermodynamics and the implications of Hawking Radiation on mass and temperature dynamics.