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turin
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Guy From Alberta,
I looked into the 4 types of BH's. This is what I've got so far:
Schwarzschild:
Is as I described. This is my default BH, so, if I am talking about a BH and I do not specify (or the context does not make the distinction obvious), then I am talking about the friendly Schwarzschild BH, or, more exactly, the associated metric/geometry. The only property that distinguishes one such BH from another is the mass. It is modeled as a singular point at the coordinate r = 0. There is one critical horizon, from r < such a particle cannot theoreticall escape.
Kerr:
This kind of BH has the additional identifying quality of angular momentum, L. Thus, whereas two BH's that both have mass = M are identical in the Schwarzschild case, they can be distinct in the Kerr case in their L's. This one is complicated (to me), so I will leave it to someone else to explain the finer points to you. From what I gathered, it seems that the Kerr BH has two horizons, but that will warrant further investigation.
Reissner-Nordstrom:
This kind of BH is the other extension of the Schwarzschild BH, but, instead of including L, it includes a charge, Q. I have read the justification that these are not expected to exist stably. I don't know if I agree, but, at any rate, their principle existence is not denied by anyone (from whom I have heard). These kinds of BH clearly have two horizons. I am still looking into the meaning.
Kerr-Newmann:
This kind of BH is believed to be the most general form possible in principle. I don't know anything about it.
"A real paradox could occur if some given particle moves faster than the speed of light...the 'causality problem' happening from the fact that when 2 events, A and B, happen in such a way that A is to cause B at a point in time much earlier than a light signal could arrive at B from A, ... then, according to the causal structure indicated by SR, event B could happen before event A, which is inconsistent with said causal structure."
I looked into the 4 types of BH's. This is what I've got so far:
Schwarzschild:
Is as I described. This is my default BH, so, if I am talking about a BH and I do not specify (or the context does not make the distinction obvious), then I am talking about the friendly Schwarzschild BH, or, more exactly, the associated metric/geometry. The only property that distinguishes one such BH from another is the mass. It is modeled as a singular point at the coordinate r = 0. There is one critical horizon, from r < such a particle cannot theoreticall escape.
Kerr:
This kind of BH has the additional identifying quality of angular momentum, L. Thus, whereas two BH's that both have mass = M are identical in the Schwarzschild case, they can be distinct in the Kerr case in their L's. This one is complicated (to me), so I will leave it to someone else to explain the finer points to you. From what I gathered, it seems that the Kerr BH has two horizons, but that will warrant further investigation.
Reissner-Nordstrom:
This kind of BH is the other extension of the Schwarzschild BH, but, instead of including L, it includes a charge, Q. I have read the justification that these are not expected to exist stably. I don't know if I agree, but, at any rate, their principle existence is not denied by anyone (from whom I have heard). These kinds of BH clearly have two horizons. I am still looking into the meaning.
Kerr-Newmann:
This kind of BH is believed to be the most general form possible in principle. I don't know anything about it.
I don't know what you mean. I will define causality (as I understand the physicists to use the term) as the notion that all physical processes follow a common parameter in a monotonic sense, and that this sense is preserved for any transformation to a valid physical frame of reference. This parameter may or may not be the value of the projection on the time axis. One thing I feel I should point out about this notion/principle (and indeed about science in general) is that it is axiomatic and should not be endowed with any deeper meaning. There are good reasons for the postulate, but the reasons have never been (up to this point) absolutely conclusive.Guy From Alberta said:Are you mentioning "causality" here in the context of "time axis;"
In general, there are two possibilities: 1) show that the problem/exception is merely ostensible, 2) eliminate the axiom that leads to the problem/exception. If you are referring to a specific case, let's hear it.Guy From Alberta said:how would we reconcile the phenomena or occurrence of "causality problems," (or exceptions)?
If I detect a hint of cynicism here, then I would say that I am right there with you. I have heard/read/seen all kinds of crap (and by "crap" I mean reasoning for the inability to change the sense of one's time'parametrization wrt the rest of the physical system with which one is causally connected). This has been "disproven" on the micro-scopic level (to what I consider an acceptable degree of confidence), and even a mere description of decoherence into a causal mode of parametrization has yet to be clearly demonstrated (so far as I've seen). The basis of assertions of the "chronology protection conjecture" range from qutie convincing (albeit empirically devoid) billiard ball type situations to innane rhetoric such as "where are all the tourists." The resulting assertions have a stinkingly conjectural basis.Guy From Alberta said:I know that S. Hawking's "chronology protection conjecture," states that the laws of physics do not allow time machines, for eg., and that "time travel," is only possible "microscopically," whatever that might mean.
I think you've just about got it. Although, I would restate it:Guy From Alberta said:... a real paradox can occurr when some given particle moves faster than the speed of light...the "causality problem" happening from the fact that when 2 events, A and B, happen faster than the speed of light; (for a stationary frame of reference), then, accordingly, event B can happen before event A?
"A real paradox could occur if some given particle moves faster than the speed of light...the 'causality problem' happening from the fact that when 2 events, A and B, happen in such a way that A is to cause B at a point in time much earlier than a light signal could arrive at B from A, ... then, according to the causal structure indicated by SR, event B could happen before event A, which is inconsistent with said causal structure."
It is not so much their hypothetical nature as it is the requirement of superluminal velocity, which is hypothetically impossible (is that an oxymoron?), in order to make use of them.Guy From Alberta said:A fellow named K. Thorne, has proposed that something called "wormholes" could be used as "time machines," but I don't understand how a human being could access a "wormhole," since, admittedly they are hypothetical.
Not quite. In the frame of reference wrt which the velocity is faster than light, the object is still "moving forward through time." The issue is that, upon a Lorentz transformation, traveling faster than light in any inertial frame leads to inconsistent "direction of travel through time" in distinct inertial reference frames (which can result in "travelling backwards in time"). That, together with the principle of causality, is what prohibits superluminal velocity.Guy From Alberta said:According to special relativity, from what I understand, traveling faster than light is equivalent to traveling backwards in time?
What is a "causality loop?" Do you mean a loop-hole in the theory re causality? SR provides no such loop-hole, and I am pretty certain that neither does GR. QM? Maybe. Reality? That's a totally different story.Guy From Alberta said:I guess all this is suggesting to me that perhaps, there may be a way we do have access to the future; as we consider "causality loops," where events of the future cause events of the past...
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