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Left closed in review as "Original close reason(s) were not resolved" by Miyase, Roger V., ZeroTheHero
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Qmechanic
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How can there be a naked singularity in the RNReissner-Nordström (RN) geometry?

I recently read that, if the mass of a charged black hole is small (compared to its squared charge times some constant), than there is no event horizon, but there is still a (naked) singularity. My doubt is the following:

The presence of a singularity means that the curvature diverges; in other words, gravity tends to infinity as we approchapproach the central mass. So, as we approchapproach the mass, gravity grows and grows unlimitlessly so, at a certain distance, it should become so strong that the escape velocity would be $>c$ (hence, at that distance, we would have an horizon).

What mechanism prevents the formation of an event horizon in the presence of a (relatively small) charged mass?

How can there be a naked singularity in the RN geometry?

I recently read that, if the mass of a charged black hole is small (compared to its squared charge times some constant), than there is no event horizon, but there is still a (naked) singularity. My doubt is the following:

The presence of a singularity means that the curvature diverges; in other words, gravity tends to infinity as we approch the central mass. So, as we approch the mass, gravity grows and grows unlimitlessly so, at a certain distance, it should become so strong that the escape velocity would be $>c$ (hence, at that distance, we would have an horizon).

What mechanism prevents the formation of an event horizon in the presence of a (relatively small) charged mass?

How can there be a naked singularity in the Reissner-Nordström (RN) geometry?

I recently read that, if the mass of a charged black hole is small (compared to its squared charge times some constant), than there is no event horizon, but there is still a (naked) singularity. My doubt is the following:

The presence of a singularity means that the curvature diverges; in other words, gravity tends to infinity as we approach the central mass. So, as we approach the mass, gravity grows and grows unlimitlessly so, at a certain distance, it should become so strong that the escape velocity would be $>c$ (hence, at that distance, we would have an horizon).

What mechanism prevents the formation of an event horizon in the presence of a (relatively small) charged mass?

Post Closed as "Duplicate" by John Rennie black-holes
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Qmechanic
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