Black Hole Evaporation: Charged Particle Energy Effects

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SUMMARY

The discussion centers on the effects of charged particles in the context of black hole (BH) evaporation and Hawking radiation. It clarifies that when an anti-particle falls into a BH, the mass of the BH increases due to the positive mass of the anti-particle. The conversation emphasizes that Hawking radiation involves the emission of particles, including positrons and electrons, with the interpretation of energy being crucial, as negative-energy particles do not exist in a measurable sense. The focus remains on the quantum level processes and the observable thermal radiation emitted by black holes.

PREREQUISITES
  • Understanding of Hawking radiation and its implications
  • Familiarity with particle-antiparticle pairs in quantum physics
  • Knowledge of black hole thermodynamics
  • Basic principles of electromagnetic theory related to charged particles
NEXT STEPS
  • Research the implications of Hawking radiation on black hole thermodynamics
  • Study the role of particle-antiparticle pairs in quantum field theory
  • Explore the concept of thermal radiation emitted by black holes
  • Investigate the relationship between charge and energy in electromagnetic theory
USEFUL FOR

Physicists, astrophysicists, and students interested in quantum mechanics, black hole physics, and the fundamental principles of energy and charge in particle physics.

zarei
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in classical electromagnetic a charge can make energy. Now consider Howking radiation effect: if an anti-particle fall into the BH the volume of BH will reduce. But if that particle be a charged particle, this charge can make positive energy and increase the volume. Is that right?
 
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zarei said:
if an anti-particle fall into the BH the volume of BH will reduce.
I am not sure what you are referring to, or if what you read confused you. An anti-particle has a positive mass. If an anti-particle falls into a BH, the mass of the BH increases.

Independently of this, in Hawking's first calculations, one can interpret an anti-particle from the fluctuation of a pair as the one carrying negative energy (by definition), the particle being the one carrying positive energy (and this can be a positron BTW). This split near the horizon makes it possible for the particle to escape at infinity, whereas the antiparticle must keep falling. From an outside observer, the BH has emitted a particle. The particle-antiparticle definition is almost irrelevant in this context, except for the amount of energy carried and the possibility to escape at infinity, since most of those pairs are photons. Strictly speaking once again, a black hole will emit as much positrons as electrons (provided it is not charged. In fact, once it has emitted one electron, it is more likely to emit a positron). You can not go further in the interpretation : the process occurs at the quantum level and only the outside observer interpretation is a valid one that can be measured. Strictly speaking, there is no such thing as a negative-energy real (anti-)particle. What is observed is the emission of thermal radiation, not negative-energy particles.

IMO, this discussion is not BtSM.
 
Last edited:
humanino said:
IMO, this discussion is not BtSM.
I agree. I'm moving to General Physics: Doc Al or Zz may find a more suitable home for it.
 

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