Talk:Schwarzschild metric/Archive 1

Merge from Schwarzschild black hole
Merger sounds good. ---Mpatel (talk) 18:21, August 30, 2005 (UTC)

I agree. I'll go ahead and do it.--Bcrowell 03:15, 3 September 2005 (UTC)

Isotropic coords?
Can someone add pretty language about isotropic coordinates? That is,


 * $$\rho = \frac{1}{2} \left[r-M+\sqrt{r(r-2M)}\right]$$

so that


 * $$ds^2=\left( \frac{1-M/2\rho}{1+M/2\rho}\right)^2dt^2

- \left(1+\frac{M}{2\rho}\right)^4 (d\rho^2 + \rho^2 d\Omega^2)$$

or should I just uncermoniously copy this into the article at some point? I don't think I can say anything intelligent about these coords. linas 20:19, 29 October 2005 (UTC)


 * Hmm, there's an article isotropic coordinates which doesn't mention this form, and this article doesn't link.linas 20:49, 29 October 2005 (UTC)


 * Hmm, can the above be called the "standard isotropic Schwarzschild coords" or something like that? Then the above formulas can be added to the article on isotropic coords, and this article can then be made to link to that. ?linas 21:09, 29 October 2005 (UTC)

Controversy
There is a controversy between the Schwarzschild Model for the Black Hole and the E=mc2 equation. I will be starting an article on this soon. Even better, someone help me start it. I really don't have that much time. Freddie 02:23, 20 February 2006 (UTC)


 * If this article contains your own thoughts on the matter, be advised that it is "original research", and will likely be deleted very quickly as a result (Wikipedia is only supposed to summarize information found elsewhere, not be a place to post new information). If you have questions about how the Schwarzschild metric and aspects of general relativity (like the mass/energy equivalence) relate to each other, a suitable place to discuss this is either on this talk page, or at Talk:General relativity). --Christopher Thomas 04:26, 20 February 2006 (UTC)

Proposed merge from Deriving the Schwarzschild solution
This merge was proposed on 3 March 2006 by User:Hillman. I've created this heading so that we can figure out if people want the merge to occur. --Christopher Thomas 20:40, 27 August 2006 (UTC)


 * Oppose. I think the derivation is long enough that it's reasonable to put it in its own article to avoid clutter in this one. --Christopher Thomas 20:40, 27 August 2006 (UTC)
 * Oppose. The derivation is indeed a lengthy one, which deserves its own article. Since the main article is (for the most part) qualitative, adding the derivation will not add significantly to the content of the article. --Masud 17:59, 25 September 2006 (UTC)

Units?
Not setting c = 1 in articles on general relativity seems completely ridiculus, for any number of reasons. I can see how, pedagogically, one might wish to do that in articles on special relativity (although I personally object). By the time someone is comfortable with reading articles on general relativity, however, they should be comfortable with the idea of natural units. In the interior of a Schwarzschild black hole the t and r coordinates become spacelike and timelike respectively. Are we now measuring time in meters and space in seconds, or do we suddenly switch the units of t at the event horizon??? -- Fropuff 1 July 2005 15:38 (UTC)
 * Whether you think it's "completely ridiculous" is not really the point. True, when someone is comfortable with reading GR articles, putting c=1 simplifies the equations etc. Putting c=1 or not has nothing to do with the nature of the coordinates; only the metric signature determines that. Let's agree that if a mathematical quantity is spacelike, this means that its inner product with itself is +ve; this does not necessarily mean that the quantity is measured in units of metres !!! For example, in GR, consider the four-velocity of a material particle: it's inner product with itself is always negative, but four-velocity is not measured in metres or seconds !!! Anyway, for someone who first comes across this article (and who isn't a specialist, but may have heard of black holes etc.), they're probably wondering why the units are messed up in the metric. In other articles where this metric is mentioned, I agree that putting c=1 is ok, as long as this is stated (like in some of the GR articles). Specialists have this tendency to be as elegant as possible, but they sometimes overlook the fact that not all articles are intended for them. We should remember this. --Mpatel 11:32, 17 July 2005 (UTC).


 * I actually came over into the Talk section here because I was rather surprised to see that the article was not using natural units. I think it's reasonable to use natural units in the article as long as we mention that is what we're doing.  An explanation as to why this makes sense even beyond just simplifying the equations (i.e. treating space and time as equivalent geometric quantities, etc.) would also be appropriate.  This will serve to keep the article in sync with current practice in the field while still educating and providing an introductary path for newcomers.  72.130.178.52 04:33, 5 December 2006 (UTC)

It is mentioned elsewhere (on Kerr metric page, for example) that time and space inside horizon swap. It would be nice if this will be explained a bit.

—The preceding unsigned comment was added by 195.66.192.167 (talk • contribs) on 11:04, 17 July 2005.

In 1-dimensional spacetime (one spatial coordinate) Schwarzschild metric is (in natural units, c=1)

ds^2 = -(1-rs/r)*dt^2 + dr^2/(1-rs/r)

where rs - Schwarzschild radius.

Let's use a = (1-rs/r). r belong to [0,+inf) -> a belong to (-inf,1).

ds^2 = -a*dt^2 + dr^2/a

Null geodetics (ds^2=0):

dr^2 = a^2*dt^2 (again, remember that -inf 0 (and how mathematically future is different from past? both have ds^2 > 0...).

It visualizes the following:

1) photon will never reach horizon in 'our' (distant observer's) frame of reference.

2) inside horizon directions where ds^2 > 0 are spacelike. (time and space are swapped).

Open questions:

1) I placed '+' inside horizon so that light is falling into singularity and not away from it to horizon, but this is a bit arbitrary. Is there solid reason why it is so?

2) Will photon which is somehow got inside horizon ever reach singularity in our frame of reference? I think it wouldn't, exactly like 'external' photons could not reach horizon due to time dilation. I infer time dilation from ever shrinking angle of light cone when light approaches horizon from outside or when it approaches singularity.

—The preceding unsigned comment was added by 195.66.192.167 (talk • contribs) on 11:58, 17 July 2005.

cool you just answered my question on the solution inside the black hole. but then we'd have 3 dimensons of time and 1 space!? wat does that mean? anyway i dont think its legitmate to solve it inside the horizon. quantum effects are likely to dominate (dunno about just below the horizon) —The preceding unsigned comment was added by Protecter (talk • contribs) on 11:14, 25 October 2005.

Year of finding
It is said in the article, that Schwarzschild found the solution in 1915. Now I am reading Landau & Lifshitz's "Classical Theory of Fields" (Polish ed., PWN, Warsaw 1976) and it is stated on p. 339 that it rather should be 1916. I am not sure if they mean year of publication, and the actual finding could take place in 1915, so I point it out in discussion, rather than edit it by myself. Paweł Laskoś-Grabowski 81.219.231.40 16:43, 8 July 2007 (UTC)


 * 1915 is correct. Schwarzschild's letter to Einstein, dated 22 December 1915 and containing the solution, is in Einstein's archive which was not available to researchers in 1976. I posted it here. JanPB 19:06, 16 August 2007 (UTC)

Isotropic equation
Why is there an ellipsis on the last equation in the isotropic section? —Preceding unsigned comment added by 131.215.195.228 (talk) 18:45, 5 August 2010 (UTC)
 * As near as I can tell, this was to move the superscript for the citation link to avoid making it look like "$$c^3$$". I've replaced it with whitespace instead. --Christopher Thomas (talk) 19:51, 5 August 2010 (UTC)

title
Clearly, right from the lead, this article focusses generally on the Schwarzschild solution or Schwarzschild black hole. I suggest changing the title to reflect this.

Then we could have a section that covers the span of coordinate systems (and associated metrics) for this manifold and geometry. E.g., Schwarzschild (both the original coordinates and the modern variation which I understand differ in the value of r at the horizon), Eddington-Finkelstein, Kruskal-Szekeres. Most of these would just be brief summaries which break out to their respective pages (which already exist).

In fact the usual Schwarzschild metric is just the important instance of general Schwarzschild coordinates and some of the mathematical detail could logically be moved there (while still retaining however much here as is needed for summarising the history, outlining the derivation, and detailing features of the physical interpretation). Cesiumfrog (talk) 05:59, 24 April 2012 (UTC)

The article has been hijacked by crackpots
It looks like the article was partially hijacked by amateurs who don't quite understand the subject. For one reason or another relativity seems to attract bizarre eccentrics. (You never see them in quantum field theory, for example.) Check the German translations in the paper http://www.wbabin.net/eeuro/vankov.pdf for a chuckle. Example: when Schwarzschild writes to Einstein: "As you see, the war treated me kindly enough, in spite of the heavy gunfire, to allow me to get away from it all and take this walk in the land of your ideas". He writes about World War I. This is how it's translated in the vankof.pdf paper: "As you see, it means that the friendly war with me, in which in spite of your considerable protective fire throughout the terrestrial distance, allows this stroll in your fantasy land". I'm not making it up, check it for yourself! You can imagine the rest of the paper. JanBielawski (talk) 05:43, 17 August 2012 (UTC)
 * I think we have been mostly effective in combating the non-sense content-wise. The article needs a lot of work though. So be WP:BOLD and feel free to help out. (Better sources for English translations of some of the historical papers would be most welcome.)TR 07:11, 17 August 2012 (UTC)
 * On reading the paper I have misgivings about the accuraccy of the translation - it lacks English idiom. I have been told that the golden rule of translation is that you translate into your mother tongue, not away from it.  The translator's mother tongue does not appear to be English. Martinvl (talk) 20:26, 17 August 2012 (UTC)

Units of measure
I removed the units of measure from the article with the note that any coherent system of units can be used. User talk:JRSpriggs removed my note and re-instated the units of measure: metres, seconds, metres per second. There is absolutely no reason why Natural units, cgs units (or even the FFF system) cannot be used, provided that everything (including G) is in the same units. Martinvl (talk) 07:50, 30 January 2013 (UTC)


 * The objective here should be to provide information, not to hide it. I added " (if SI units are used)" to make it clear (if it was not already obvious) that any other system of units could also be used.
 * Simply removing the units as you did is not helpful. JRSpriggs (talk) 09:00, 30 January 2013 (UTC)


 * I have removed the SI-specifics from the equation, but have added a paragraph after the list of parameters explaining that the equation holds equally well for SI or cgs and implying that other units of measure can be used as well, provided that they are used consistently. I trust that this clears up any problems. Martinvl (talk) 12:18, 30 January 2013 (UTC)


 * Is it obvious that this equation applies to systems other than SI? If so, then we should not be citing units of measure at all, if not, then we should give proper guidance emphasising that the equation holds for any coherent system of units. Martinvl (talk) 17:48, 30 January 2013 (UTC)
 * Writing out the units after each quantity really seems like overkill. (Radii can be measured in meters? What a revelation!) There is a point beyond which providing more information makes articles harder to read. Zueignung (talk) 08:32, 1 February 2013 (UTC)

If I am assuming that some readers may be dumb in that they may fail to realize that units can (and indeed must) be used in general relativity, then you three (Martinvl, Cesiumfrog, and Zueignung) are assuming that they are even dumber by supposing that they are not even aware that they can convert from one system of units to another (despite "if SI units are used"). JRSpriggs (talk) 13:02, 1 February 2013 (UTC)


 * Would User:JRSpriggs please be aware that his comments above are bordering in incivility. To answer his question though, if units of measure are to be mentioned, then they should be mentioned in an encyclopeadic and neutral manner, firstly that the units chosen must be from a consistent set and then give examples of known consistent sets where the value of G is easily found - SI (which is the system of choice these days), and then cgs units which is probably what Schwartzchild himself used. Martinvl (talk) 15:21, 1 February 2013 (UTC)


 * I don't really see why units of measure should be discussed in this article. Of course the quantities entering the formula have units, and one has to be aware of them e.g. when adding terms or when interpreting the result. But that is true for the vast majority of formulae all over physics; we can't discuss this general fact each time we use any formula. The Schwarzschild metric in particular is not an example of a formula which readers are likely to dig up on Wikipedia and put in values without being aware of their units. I can't think of any case where someone would like to calculate the Schwarzschild proper time distance of two actual events in space-time.


 * Mentioning two values of G and making the impression that they're different is at least misleading: given that by 'value' we obviously mean a number together with a unit here, the two values are identical.
 * I suggest to remove the entire paragraph discussing units of measurement. The only use we have for units here is for giving the value of G, which is already achieved by linking to Gravitational constant, which has an in-depth discussion of how to express G using various units. &mdash;&thinsp; H HHIPPO  13:21, 3 February 2013 (UTC)


 * I am inclined to agree with User:Hhhippo and would certainly not object if all units of measure were removed - if however units of measure are to be included, then both SI and cgs should be discussed. Martinvl (talk) 15:57, 3 February 2013 (UTC)


 * Just aside: Schutz makes the point that we know the mass of the sun very precisely in geometricised units, but there is comparatively large uncertainty in its mass in SI (or other) units, simply because the experiments for measuring the value of G (in traditional units) are more error prone. This suggests that the choice of units may be more than a convenience. Schutz also explicitly states that G has different "value"s depending on choice of units; Hhippo's definition for value seems obtuse to me, and I also don't understand Martinv's emphasis of cgs. Cesiumfrog (talk) 23:45, 3 February 2013 (UTC)


 * So we know the Sun's Schwarzschild radius best in geometricised units, ok. But what do we do with it? Is there any application where one would actually put numbers in the metric to calculate some specific distance? Anyway, I can live with the discussion of units as it stands now. I still don't think it's needed, but it's not too disturbing either.
 * What you call my definition of 'value' is actually not mine, it's how it was used in the article at that time, though not consistently. That's what I meant to point out. &mdash;&thinsp; H HHIPPO  07:59, 4 February 2013 (UTC)

Original metric 2
In the original paper (in English) is NOTHING about singularity (Singularität) and nothing about the event horizont (Ereignishorizont). Thus claims like "Schwarzschild (mistakenly) assumed that the outer most singularity ... must coincide with coordinate singularity" and "alternative radial coordinate ... which puts the event horizon at the origin of the coordinate system" can not be in the wiki artice. It can not be true (These concepts did not exist at that time.).

He introduced "auxiliary quantity/variable" ("Hilfsgröße") R (see texts between eq. 13 and 14) as R = (r3+rs3)1/3 where r is the radial coordinate. But R is now (wrongly) used as radial coordinate.195.113.87.138 (talk) 10:03, 9 April 2013 (UTC)


 * Wikipedia is supposed to be based on secondary sources rather than primary sources. This situation is an example of why that is the case.
 * The expression "event horizon" may have been unknown when Schwarzschild wrote his paper; and "coordinate singularity" was probably rarely used then. However, Schwarzschild and Einstein must have been aware of the singularities (however they denoted them in their own minds) because they are manifested by certain components of the metric tensor going to zero or to infinity. In any case, our task is to describe the properties of the mathematical solution, not what certain people thought at some time in the past. To communicate effectively with our audience, we need to use modern language to describe what those properties are.
 * As to which variable is the radial coordinate, there is no requirement in general relativity to use any one coordinate system rather than another (that is what "general covariance" means). The choice of which one to use is merely a matter of our convenience. What we have to preserve is the metric (physical) structure of space-time, not any particular way of describing it which was used by Schwarzschild. JRSpriggs (talk) 17:27, 9 April 2013 (UTC)


 * In the section "History" should be a correct description of the past. (History is based on primary sources. No speculations about the mind of scientists.) Yes, we can use any coordinate system, but the mathematical form of line element (or other expressions) will change with a coordinate transformation. The eq. 14


 * $$ \left(1 - \frac{r_s}{R} \right) c^2 dt^2 - \left(1-\frac{r_s}{R}\right)^{-1} dR^2 - R^2 \left(d\theta^2 + \sin^2\theta \, d\varphi^2\right)$$


 * expressed in the radial coordinate r is


 * $$ (1 - \frac{r_s}{(r^3 + r_s^3)^{1/3} } ) c^2 dt^2 - \frac{r^4 (r^3 + r_s^3)^{-4/3} }{1 - \frac{r_s}{(r^3 + r_s^3)^{1/3} } } dr^2 - (r^3 + r_s^3)^{2/3} (d\theta^2 + \sin^2\theta \, d\varphi^2) $$


 * (also dR is not dr) and not


 * $$ \left(1 - \frac{r_s}{r} \right) c^2 dt^2 - \left(1-\frac{r_s}{r}\right)^{-1} dr^2 - r^2 \left(d\theta^2 + \sin^2\theta \, d\varphi^2\right)$$


 * because r ≠ R = (r3+rs3)1/3 a thus the current version does not corresponds to the "original" version of the line element. 195.113.87.138 (talk) 07:44, 10 April 2013 (UTC)

Mass
There should be a version of the Schwarzschild metric where the central mass explicitly appears. It is given in many books as the standard metric but I can not find it here. — Preceding unsigned comment added by 96.43.237.33 (talk) 21:10, 24 July 2013 (UTC)
 * This article is not protected, so you are free to insert such a version of the metric into the article and provide a reference. Zueignung (talk) 21:20, 24 July 2013 (UTC)

Space-Time Reversal
I'm reading a lot online about a supposed "reversal of roles" of space and time instigated somehow via the Schwarzschild metric. This seems to somehow involve the symmetry mentioned in this article, but it isn't at all clear what is being suggested. Can someone more familiar with this please integrate an explanation into the article? I believe this somehow relates to ideas of Kip Thorne? 70.247.171.190 (talk) 02:15, 8 July 2012 (UTC)


 * I think that they are referring to the fact that $$ 1 - \frac{r_s}{r} \,$$ changes sign from positive to negative when one crosses from the region where $$ r > r_s \,$$ to the region where $$ r < r_s \,.$$ Consequently, in the interior, t becomes space-like and r becomes time-like (the other two coordinates remain space-like). This is not a real physical effect, but the result of the choice of this coordinate system becoming inappropriate when $$ r \leq r_s \,.$$ Before you cross the event horizon, you should switch to a different coordinate system such as Kruskal–Szekeres coordinates. JRSpriggs (talk) 02:42, 8 July 2012 (UTC)


 * Ok, I think I get that, but what I'm really searching for is an exposition of the idea of reversal that whomever is putting forward. Superficially, it seems to me to be mostly a coordinate change, as you allude to, but the fact that it keeps coming up leads me to believe that someone is suggesting there is more to it than the superficial.  I'd like to understand how physicists discuss that concept.  Thanks!  70.247.171.190 (talk) 04:36, 8 July 2012 (UTC)


 * Upon further reading, what I'm seeing is that there seems to be concern about "what happens to the time?" when crossing the event horizon. Since time comes to a stop at the horizon from an external perspective, there is speculation as to what happens on the interior.  Does it continue to stop, or does something else happen?  The answer seems to be, no, it doesn't continue to stop, and here's how you re-identify time (by identifying it with the radial inward direction--this is the necessary future in the interior).  70.247.169.103 (talk) 16:30, 8 July 2012 (UTC)


 * Time does not really stop when you fall through the event horizon. Rather the coordinate singularity corresponds to the fact that the last light from your spaceship which can be seen from outside leaves you at that time. Those last few moments are red-shifted more-and-more so that they seem to stretch out to infinite time (or rather until they become invisibly faint). But you continue to exist and experience time passing until you hit the real physical singularity at the center where you are crushed out of existence. Light emitted by your spaceship after you fall through the horizon also falls to the center. JRSpriggs (talk) 09:42, 9 July 2012 (UTC)


 * You miss my point again. I understand the concept of changing coordinates and warping due to relativistic effects pretty well.  What I don't understand is why some people seem to feel there is a meaningful (i.e. not just coordinate change) chanegover, that is, an actual 'reversal', that is happening in the interior or on the event horizon of a black hole.  All I see are coordinate changes, or coordinate system changes.  Neither of those have physical heft.  So why do I keep hearing about the reversal?  Are people just clueless?  Doubtful, since this seems to be coming from the physics community.  If it's not cluelessness, then there seems to be something worth mentioning within the scope of this article.  70.247.167.104 (talk) 04:03, 4 February 2014 (UTC)


 * In my experience, many people (even supposed authorities) are clueless. Do not assume, just because they make some distinction, that there actually is a distinction. If you have no reason of your own to question it, rest easy. JRSpriggs (talk) 10:27, 4 February 2014 (UTC)

TItle--revisited
I see that another reader has commented above on the title. I just made an edit to the article to bold the phrase 'Schwarzchild metric' because it seemed that the lead had completely neglected the term, despite the fact that it is the article's title. My take on this is that there appear to be two terms in common circulation for similar concepts: Schwarzschild metric, and Schwarzschild solution. Technically, I believe there is a distinction, in that a 'solution' is any equation that satisfies the field equations, whereas a metric is a particular variety of solution that is presumed to exist (or possibly exists of necessity). If this is correct, then to me it would make most sense to devote the article to a discussion of the broader context of a solution, and within that context, discuss how the metric comes about as part of that solution. In that case, the article should probably be named 'Schwarzschild solution'. Again, that would make more sense from the point-of-view that at least that phrase appears in the lead. 70.247.167.104 (talk) 03:46, 4 February 2014 (UTC)


 * Perhaps in this case, it is I who am clueless. I do not understand the distinction you are making between a metric and a solution, despite your attempted explanation. Could you give an example of what you would consider to be part of the Schwarzschild solution that would not be part of the Schwarzschild metric? JRSpriggs (talk) 10:32, 4 February 2014 (UTC)
 * That's just it. Are the terms synonymous?  It doesn't seem so, since the lead doesn't mention them all as synonyms as most leads do.  But if they're not synonyms, then why are both mentioned separately in the article, with no explanation of how the idas are related?  70.247.167.104 (talk) 03:15, 6 February 2014 (UTC)
 * My admittedly naive view is that a 'solution' is a solution to the Einstein Field Equations, whereas a 'metric' is an implicit description of a geometry. The two need not be connected, but they somehow are.  Whatever the scope of that connection is, however, is important, because it defines the necessary scope of this article, and as such, would be relevant to a discussion of what the title is.  70.247.167.104 (talk) 03:22, 6 February 2014 (UTC)
 * My impression is that in GR "metric" is often shorthand for "metric components". Hence we can have the "maximally-extended Schwarzschild solution", but the "metric" frequently refers to "the line element as expressed in Schwarzschild coordinates". Maybe it's worth googling the text of the main GR textbooks for an authoritative distinction? Cesiumfrog (talk) 10:40, 7 February 2014 (UTC)
 * You may be right, but an uninformed reader shouldn't have to Google to understand an encyclopedia article. The encyclopedia should refrain from using idiomatic shorthand because it's unnecessary.  70.247.161.12 (talk) 09:44, 28 April 2014 (UTC)


 * "Schwarzschild metric" and "Schwarzschild solution" are strictly speaking synonyms. However, "Schwarzschild metric" will sometimes be used to mean the specific line element in Schwarzschild coordinates. (Agree that the lede is a bit of a mess in this sense.)TR 10:13, 28 April 2014 (UTC)

Original metric
The metric known (presented here) as "the Schwarzschild solution" was suggested by Einstein. But in the original Schwarzschild’s solution (see his letter - the last page in ) r was originally equal to $$R = (r^3+{r_s}^3)^{1/3}$$ without gravitational singularity. This my edit was reverted. Please discuss it.


 * Even if your reference is correct, the place where you put your edit was inappropriate. If it is referring to a different solution, then it should be in another article. If it is referring to this solution, then it should have been in a new section by itself.
 * However, I strongly doubt your reference since it has been established that there is a real physical singularity at the center of an spherically symmetrical uncharged black hole. See the section Schwarzschild metric. JRSpriggs (talk) 14:13, 11 January 2011 (UTC)


 * So I will add a new section - "History". The original Schwarzschild solution was with $$R = (r^3+{r_s}^3)^{1/3}$$ instead of r in the currently named "Schwarzschild" solution. This solution has not the gravitational singularity . The current version of solution is due to David Hilbert.


 * Are you saying that Schwarzschild worked with R as his radial coordinate (calling it "r") instead of what we use here, r=circumference/(2&pi;)? If so, then when R=rs, one should have r=0. That is, anything reaching that altitude would be crushed horizontally to zero width. And you do not consider that to be a singularity? JRSpriggs (talk) 10:14, 12 January 2011 (UTC)


 * You can see (the last page of Schwarzschild’s letter) that r is coordinate and at r=rs is R=1.26rs and at r=0 is R=rs. This is only a transformation. Nevertheless the differential form of metrics is also transformed into dR. This means that R "in the same" metrics can not reach values below rs (horizon) for any r, but for metrics directly with r can. —Preceding unsigned comment added by 194.228.230.250 (talk) 11:57, 12 January 2011 (UTC)


 * I was having difficulty making sense of what you were saying. But I see from the translation of Schwarzschild's letter (to which you referred) that he uses R for that for which we use r, that is, the circumference divided by 2&pi;. Regardless of the symbol used for the radial coordinate, the geometry and physics of the solution are unaltered. So I still fail to see how you can say that there is no physical singularity. Could you explain that in more detail please. JRSpriggs (talk) 12:33, 13 January 2011 (UTC)
 * If I understand correctly, the "original" radial coordinate was zero at the event horizon, so the "original" coordinate system didn't cover the interior of the black hole at all. A. di M. (talk) 14:21, 13 January 2011 (UTC)

Well, it appears that at that time, Einstein was still acting under the misconception that one should only use coordinate systems for which $$\sqrt{- g} = 1 \,.$$ This may have led him to exclude the interior of the black hole from his coordinate chart. But the singularity is there whether the coordinate chart reaches it or not. JRSpriggs (talk) 07:30, 14 January 2011 (UTC)


 * Can the references cited here (notes 1-4 in the article) be considered reliable sources? 2-4 are pointing to a website that's basically claiming most 'experts' on general relativity are lying. This should at least be marked as a controversial view. &mdash;&thinsp; H HHIPPO  20:42, 11 August 2011 (UTC)


 * These references do not look "profesionally" but they cite original articles (Schwarzschild, Brillouin, ...) that support them. For JRSpriggs: There is no singularity bacause there is no space (you are not able to reach it - go through the event horizon in finite time). The "original metric" stops at event horizon. There is 3D hole in spacetime (inversion of "3D ball" of spacetime from Big Bang where is no space or time outside expanding Universe). 195.113.87.138 (talk) 14:50, 15 August 2011 (UTC)


 * An observer outside the black hole would not see an object falling into the black hole cross the event horizon, it would appear to slow down and hang suspended. However, an observer falling into the black hole would (assuming he survived that long) see himself cross the event horizon and reach the central singularity in finite proper time. JRSpriggs (talk) 21:46, 15 August 2011 (UTC)


 * The article stetement: "As a result of this choice of coordinate system, the original solution did not reach all the way to the center of the black hole where the gravitational singularity lies, stopping instead at the event horizon." can not be true. The coordinate r can reach 0 (R is substitution). — Preceding unsigned comment added by 195.113.87.138 (talk) 08:38, 16 August 2011 (UTC)

The original Schwarzschild paper contained the solution in the conventional coordinates (equation 14 of Schwarzschild's paper). I've removed the nonsense that said that it didn't.(Which wasn't backed by any Reliable secondary sources anyway.)TR 13:10, 16 August 2011 (UTC)


 * To TimothyRias: This edit by 195.113.87.138 was an error. Your edits appeared to be premised on accepting it as correct. Therefore, I reverted your edits as well as his.
 * What Schwarzschild called "R" is what our formula calls "r". What he called "r" is something else. It appears to me that he began his paper by taking "r" as his radial coordinate in a spherical coordinate system. So naturally, he was assuming that 0&le;r. If one puts that in terms of his "R", then it becomes &alpha;&le;R which is limited to the region outside the event horizon. If I am misreading his paper, please explain how. JRSpriggs (talk) 15:25, 17 August 2011 (UTC)
 * The "R" in Schwarzschild's paper is the conventional polar coordinate (i.e. the one we call r in the equation in this article). In his derivation he uses a different radial coordinate which he calls r, which is defined by equation 7 of his article, and is different from the usual radial coordinate.
 * (Note that because the Schwarschild metric is singular at the horizon it is only valid on the patch r>r_s, anyway. Strictly speaking its is also valid on the patch with 0<r<r_s, but that patch is disconnected from the other patch so (a priori) there is no connection between the two patches.) TR 15:41, 17 August 2011 (UTC)


 * It sounds to me like you are agreeing with me. So please revert yourself. JRSpriggs (talk) 16:39, 17 August 2011 (UTC)


 * I'm not agreeing with you, in the sense that Schwarzschild simply paid no attention to the ranging a validity of his solution in his article. More importantly, I'm disagreeing with the statement that was previously in the article that "The original Schwarzschild solution used a different radial coordinate system than present formulations of the Schwarzschild metric". The final solution in Schwarzschild's paper (equation 14) uses exactly the same coordinate system as the present day formulations of that solution. The range of validity of that solution was the same is it is now (r>r_s).
 * The claim that the modern day version of the Schwarzschild solution is somehow different than the original one, is a typical crackpot claim. The fact that the quoted sources come from the homepage of sjcrothers (a very vocal internet crackpot that somehow thinks the entire relativity community is somehow conspiring against him) should have been a clear warning of this.TR 20:11, 17 August 2011 (UTC)


 * Indeed Schwarzschild starts out with r as the radius of "ordinary polar coordinates", while R is some "helper quantity". He then finds a solution of the field equations using R. To figure out the geometric meaning of his R, just integrate the metric around the equator: this gives 2*pi*R. Thus it is his R, not his r, that is the same as what we call the radius r in our article, namely the circumference divided by 2 pi.
 * As a side effect of his original interpretation of r as radius, Schwarzschild only considers the case r>0, that is R>R_s. He doesn't say anything about the region R<=R_s. It is however obvious that his metric is also a solution to the field equations for R<R_s, as long as the central mass is smaller than R. If we call that a valid solution depends on the exact definition of valid. There are some problems like the missing connection between the two regions and the fact that the coefficients of the metric depend explicitly on R which for R<R_s is a timelike coordinate, but that's not the issue here. &mdash;&thinsp; H HHIPPO  06:53, 18 August 2011 (UTC)


 * I don't think there is any disagreement about the fact that the coordinated that Schwarzschild called R is what is currently known as the Schwarzschild radial coordinate. What Scwarzschild called r, is indeed something different. Equation 14 of Schwarzschild's paper therefore is exactly what nowadays would be called the Schwarzschild metric. That is, there is no difference between the present day formulations of the metric and the one presented by Schwarzschild, in contradiction with what the paragraph that I removed from the article claimed.
 * That being said there should probably an account of the history of the interpretation of the Schwarzschild solution (an in particular its singularities) in the history section. The problem here is finding a good WP:RS that discusses this history.TR 08:40, 18 August 2011 (UTC)


 * I fully agree. &mdash;&thinsp; H HHIPPO  17:51, 18 August 2011 (UTC)


 * I also agree (and thus "reverted"). I think that original metric looks like :$$\left(1 - \frac{\alpha}{(r^3+{\alpha}^3)^{1/3}} \right)$$ and thus for r=0 (centre), R=alpha (i.e. event horizon for conventional metric) is different (naked singularity) 195.113.87.138 (talk) 08:33, 24 August 2011 (UTC)
 * It is great that you think that, but that is not how the metric appears in Schwarzschild's paper.TR 08:43, 24 August 2011 (UTC)
 * Which "Schwarzschild's paper" do you mean?! In ref. 2, page 7 (in this discussion) is different (original) metric, also in ref. 4 - the last page (Schwarzschild's letter to Einstein - in German) and also in ("R", which is not able to reach zero value, does not mean "r"). It can not be same. You can not change history. 195.113.87.138 (talk) 06:10, 25 August 2011 (UTC)
 * Equation 14 of Schwarzschild's 1916 paper is exactly the form found in all other modern sources. Saying that its not is just plain false. Schwarzschild's interpretation of the coordinate singularity at R=α (in his notation) was indeed different than the modern interpretation (he tried to identify it with the coordinate singularity normally found in polar coordinates at the origin). That does not change the fact that it is the same mathematical solution of the Einstein field equations.TR 08:35, 25 August 2011 (UTC)

To TimothyRias: Because of the persistence of this confusion among some readers, should we not mention the issue and explain (as the previous text did) that the real physical singularity is present at the center of the black hole regardless of whether Scharzschild intended his coordinate chart to reach that point? JRSpriggs (talk) 09:24, 25 August 2011 (UTC)
 * I think a lot could be gained by a proper discussion of the history of the interpretation of the Schwarzschild metric (and its singularities). In particular, such a discussion could mention that Schwarzschild tried to interpret the coordinate singularity at the horizon as the center of its coordinate system.
 * Of course, this discussion should be based of proper secondary sources, which I have not yet found (and do not have time to hunt for). (For the record the sources in the paragraph previously present were either primary or not reliable).TR 10:16, 25 August 2011 (UTC)
 * (Note that this is not actually a persistent confusion among general readers, but one among crackpots like Crothers and his readers, which happen to be very vocal about it on the internet.)TR 10:16, 25 August 2011 (UTC)
 * It does not matter if Crothers is vocal or not. But it is historical truth that Schwarzschild’s metric and interpretation was different (his article and letter to Einstein). 195.113.87.138 (talk) 06:26, 26 August 2011 (UTC)


 * To TimothyRias: I can not agree. eq. 14 contains this transformation (r is normal spherical coordinate (see above eq. 6), R is a substitution mentioned also in eq. 14 (we can not use R as r - in other case we can substitute everything and obtain what we want)). The same paper also say: "Es ist also praktisch mit identisch und Hrn. Einsteins Annäherung für die entferntesten Bedürfnisse der Praxis ausreichend." / "Therefore r is virtually identical to R and Mr. Einstein’s approximation is adequate to the strongest requirements of the practice." In other words: Schwarzschild clearly (and directly) said that there is a difference (between R a r solutions). 195.113.87.138 (talk) 09:48, 25 August 2011 (UTC)


 * There is no such thing as a "normal spherical coordinate" when a space has curvature. In a spherically symmetric coordinate system the radial coordinate is defined up to a reparametrization. Extra input is required to fix this coordinate. In the case of Schwarzschild's R coordinate this is the condition that the coefficient of the angular part of the metric is R^2. In the case of his r coordinate, this input is hidden in the fact that he requires his metric to have determinant 1 in his x_i coordinates. There is no question that his r and R coordinates are different. (Although the difference becomes very small as R>>α, which is what Schwarzschild's remark is about.) Schwarzschild phrases his final result in terms of the coordinate R, which is how the result is still quoted (beit with another label for the coordinate).TR 10:31, 25 August 2011 (UTC)


 * But you can define any substitution - for example :$$Q=\frac{\alpha}{R}$$ and interpret it as "inside-out coordinate" (you can not interpret it that it is real space-time) and metric coefficient become :$$\left(1 - Q \right)$$. But it does not mean that metric change is linearly proportional to radial coordinate (it is lin. proportional to Q) instead of inversly proportional to R. You must use correct coordinate r (this is same as for integration). "r" is from 0 to inf. (these endpoints are only correct), "R" is valid from alpha to inf., "Q" is from 1 to 0 and metric coefficient is :$$\left(1 - \frac{\alpha}{R} \right)=\left(1 - \frac{\alpha}{(r^3+{\alpha}^3)^{1/3}} \right)$$. Schwarzschild phrases his result in R but (directly in eq. 14) stated what does this R means (this transformation to r - hidden real radial coordinate). I think that Schwarzschild’s interpretation of this R-r difference must be mentioned. And you must find out reference where is stated that there is no effect of R-r difference (cited pages are with interpretation of R-r difference that there is "no black hole" and BH is nonsense (Brillouin’s paper)). Now how I understand it: event horizon is at R=alpha (Q=1) i.e. r=0 (together with singularity) and there is finite time (proper or not) to see r=0 (naked singularity). This is due to Schwarzschild’s correct renormalisation (without influence at r=inf. but with essential effect at r=0). 195.113.87.138 (talk) 06:14, 26 August 2011 (UTC)


 * It is perfectly fine to make the substitution $$Q=\frac{\alpha}{R}$$. Just remember that this would also mean that $$dR=-\frac{\alpha}{Q^2}dQ$$. Q would be a perfectly fine coordinate to work with. Although it is a bit awkward in that the asymptotically flat region now occurs as Q->0. Coordinates have no intrinsic physical meaning.TR 06:43, 26 August 2011 (UTC)


 * There are many sources, that there is difference (new ones, , 17, ) but no one to support TR. I suggest to revert TR’s undo until somebody find out reference supporting TR. JRSpriggs, do you agree? 195.113.87.138 (talk) 07:14, 26 August 2011 (UTC)
 * None of these sources qualify as reliable. See WP:RS.TR 09:14, 26 August 2011 (UTC)

There are also discussions like and something supporting TR  (he extend radial coordinate r from "from 0 to inf." to "from -alpha to inf." to be able reach zero with "R"- It does not look nice. And also r=alpha at angle=0 corresponds to r=-aplha at angle=pi (i.e. twice) - but where r=alpha at angle=pi lies ... - if we accept it - this leads to infinite solutions (some of them without event horizont above singularity) and this non-linear/ambiguous theory is "useless" (you can obtain what you want/observe) - if we (mathematically) use Jacobian with singularity, we obtain (physical) singularity.). Nevertheless there must be noted (in the wiki article) that there is debate/controversy and the transformation $$R = (r^3+{r_s}^3)^{1/3}$$ must be shown. 195.113.87.138 (talk) 08:19, 26 August 2011 (UTC)
 * There is no such debate in the mainstream literature. The "criticism" comes from a few crackpots that do not understand general coordinate invariance and somehow think that some coordinates are more equal than others. Saying that there is a controversy would be a typical case of WP:UNDUE weight.TR 09:02, 26 August 2011 (UTC)
 * You do NOT add any argument (only "crackpots" etc.). If there is no debate (as you stated)why articles such as from Christian Corda (Electronic Journal of Theoretical Physics in 2011) are published? And how is it possible that interpretations against the mainstream opinion are also published? (100 years ago and also few years ago) Answer "yes" or "no" to following questons: Should be the R-r transformation in wiki article (as original Schwarzschild’s "notation")? Is the original solution of metric different? Is conventional Schwarzschild’s metric unique solution (for given static mass)? (Hole argument) 195.113.87.138 (talk) 11:12, 26 August 2011 (UTC)
 * Please read WP:UNDUE.
 * An to answer your last questions No. (although it could be mentioned in section discussing the history of the interpretation of the Schwarzschild metric) No. Yes (up to general coordinate transformations, and analytic continuation. I.e. any static solution of the Einstein equation is diffeomorphic to an open subset of the maximally extended Schwarzschild solution.)TR 11:30, 26 August 2011 (UTC)

This is actually a pretty good discussion of the early confusion about singularities in GR. If I have time I might summarize some of it for a few paragraphs on the history of the interpretation of the Schwarzschild metric.TR 12:01, 26 August 2011 (UTC)


 * To 195.113.87.138: You asked "I suggest to revert TR’s undo until somebody find out reference supporting TR. JRSpriggs, do you agree?". No, I do not agree. There would be no point in our ganging up on TimothyRias since we do not agree on what to replace his version with.
 * Actually, I agree with Tim except on one point &mdash; I want the article to explicitly reject your position while he wants it to ignore your position as non-notable and distracting. JRSpriggs (talk) 18:28, 28 August 2011 (UTC)
 * One can see that the "current" Schwarzschild’s solution (Deriving the Schwarzschild solution) is a weak field approximation and can not be used for BHs. The "original" Schwarzschild’s solution is exact solution. There is no difference is the presence of singularity (which is also present in Newtonian gravity and it is at the point of coordinate singularity). But there is a difference in existence of the event horizon. Without this weak field approximation there is no space ("above" singularity) from information/particles can not escape in a finite time (without quantum effects) - i.e. naked singularity. In the GRT all results depends on a "proper" choice of coordinate system (Coordinate conditions). Thus only "original" solution seems to be a correct one. There are no experiments sensitive to higher order terms in metrics and therefore there is no experimental evidence of event horizon (a "shell" of BH). 213.220.236.165 (talk) 10:42, 11 September 2011 (UTC)
 * To 213.220.236.165: No, you are wrong. The solution described in this article is exact. JRSpriggs (talk) 05:44, 13 September 2011 (UTC)
 * How solution like

$$g_{44}=K\left(1 +\frac{1}{Sr}\right) \approx -c^2+\frac{2Gm}{r} = -c^2 \left(1-\frac{2Gm}{c^2 r} \right)$$ can be exact? 195.113.87.138 (talk) 14:26, 15 September 2011 (UTC)
 * (1) WP:NOTAFORUM
 * (2) The weak field approximation in the formula you quote is to match the solution to the Newtonian gravitation potential (which by definition is only valid in the weak field limit). If this bothers you, you will be thrilled to know, that there are exact methods to link the schwarzschild radius to the mass. (See ADM mass or Komar mass.)TR 15:09, 15 September 2011 (UTC)

To 195.113.87.138: The derivation prior to the line you quoted was exact. The only issue remaining at that point was to determine what quantities in classical physics correspond to the two constants in the formula for the metric. For that purpose all that is necessary is that
 * $$\lim_{r \to +\infty} \left[ r \left( g_{44} - (-c^2 + \frac{2Gm}{r}) \right) \right] = 0 \,.$$

That has just one solution, specifying values of K and S. Once those values were obtained, it was seen that the approximation sign above is actually a strict equality, that is
 * $$K\left(1 +\frac{1}{Sr}\right) = -c^2 \left(1-\frac{2Gm}{c^2 r} \right) \,.$$

However, it is not necessary to show that it is a strict equality in order for this form of the Schwarzschild metric to be an exact solution of Einstein's equations which was already known before we tried to evaluate K and S. JRSpriggs (talk) 04:48, 16 September 2011 (UTC)
 * How can you know that the solution with K=-c2 is exact before an evaluation of K? Why $$ \approx $$ ("a strict equality") is still in the article Deriving the Schwarzschild solution? The "original solution" (in the standard polar coordinates $$ (1 - \frac{r_s}{(r^3 + r_s^3)^{1/3} } ) c^2 dt^2 - \frac{r^4 (r^3 + r_s^3)^{-4/3} }{1 - \frac{r_s}{(r^3 + r_s^3)^{1/3} } } dr^2 - (r^3 + r_s^3)^{2/3} (d\theta^2 + \sin^2\theta \, d\varphi^2)

$$ ) is also flat for infinite r etc. (but it is different - TimothyRias agree that there are many solutions - if it is possible to obtain more "exact solutions" for one problem, is it (mathematically) exact?) 195.113.87.138 (talk) 06:07, 16 September 2011 (UTC)
 * To your question: Yes. The phenomenon is called gauge invariance. (or more specifically for GR general coordinate invariance.) The "different solutions" actually are just different coordinate representations of the same mathematic object (a pseudoriemannian manifold.TR 08:10, 16 September 2011 (UTC)
 * Ok. But mathematically correct answer/solution is: A given problem has infinitely many solutions ... one of them is "original Schwarzschild's metric" another is "conventional Schwarzschild's metric" etc. And not that (only) "conventional Schwarzschild's metric" is exact solution (and silence ...). So, why "original Schwarzschild's metric" is not mentioned in the history section? (Also note that the "conventional solution" is not diffeomorphic to "original solution" at event horizon and singularity. - due to Jacobian matrix) 195.113.87.138 (talk) 06:46, 19 September 2011 (UTC)
 * The final solution that Schwarzschild gives in his paper (eq 14) IS the "conventional" solution. Can you please stop trying to argue that the sky is not blue. (Also note that neither the "conventional" nor the "original" solution is mathematically defined at the event horizon, making any remark about them being diffeomorphic there or not just evidence of you lack of understanding of differential geometry and thereby by extention GR.) TR 07:58, 19 September 2011 (UTC)
 * If one person expressed r and the other distances involved in terms of feet and another person expressed them in terms of meters, would you say that those were different solutions? If not, then there is no reason to say that a change in the coordinate system represents a different solution. JRSpriggs (talk) 22:52, 19 September 2011 (UTC)
 * The "conventional" metric stated on this page uses terms of the form $$(1 - \frac{r_s}{r})$$, but Schwarzschild's original metric uses terms of the form $$\left(1-\frac{\alpha}{(r^3 + \alpha^3)^{1/3}}\right)$$. In both cases the numerator is a constant that depends on the mass, but the denominators have different forms.  Does that difference vanish given that Schwarzschild's 'r' is the conventional r from polar coordinates, while the 'r' used herein depends on the circumference, which need not be precisely 2π times Schwarzschild's 'r' since space-time isn't flat? Also please note that the original metric only has an event horizon if we choose to define one of the constants of integration so that one occurs somewhere - Schwarzschild himself chose there to not be one to arrive at his original result.Tm14 (talk) 20:44, 20 June 2014 (UTC)
 * No, that integration constant ("rho") only controls where the event horizon coordinate singularity appears, not if it appears. (It is equivalent to a shift of the radial coordinate r). Also note that there is nothing conventional to Schwarzschild's coordinate "r". It is not closer related to the radial coordinate in flat space polar coordinates, than e.g. Schwarzschild's quantity R.TR 22:48, 20 June 2014 (UTC)
 * Please answer. Are "conventional" and "original" solution diffeomorphic (for whole space - all points - not only outside as Birkhoff's theorem (relativity)) or not? In the case yes (you say: "I.e. any static solution of the Einstein equation is diffeomorphic to an open subset of the maximally extended Schwarzschild solution."), please cite proof. In the case no, "conventional" and "original" are different (and different consequences) but "original" is not mentioned in wiki article. (And in Deriving the Schwarzschild solution is not mentioned that some gauge was selected.) Eq 14 IS NOT "conventional" solution. Imagine: You can define Q=r/2 but it does not mean that the speed of light was changed. This substitution must be taked into account (and result transformed back to "r" with "SI metre" as in eq. 14 - "R" is different). 195.113.87.138 (talk) 06:41, 20 September 2011 (UTC)
 * Your assertion here is just plain wrong. In eq 14 of schwarzschild's paper R is treated as a coordinate (witnessed by the dR in the expression). It is this coordinate that is now known as the Schwarzschild radial coordinate. Your assertion that the expression only has meaning if it is transformed back to the r coordinate Schwarzschild used as an intermediate step, just illustrates your lack of understanding of the role of coordinates in general relativity.TR 07:55, 20 September 2011 (UTC)
 * This is in some sense an entirely semantic issue, but Schwarzschild states that R is an auxiliary quantity when it is introduced. He gives it a clear definition of $$R(r) = (r^3 + \alpha^3)^{1/3}$$ resulting from the constraint that the metric be regular except at the origin (see just after equation (13) in reference 2).  Also, he reinforces that R is only a convenience with his equations (14) (note the plural).  Thus I see no evidence that Schwarzschild intended R to be thought of as an actual coordinate.Tm14 (talk) 20:44, 20 June 2014 (UTC)
 * Semantics indeed. However, Schwarzschild also chooses to use dR as a basis element when expressing his solutions. Hence he uses R as if it was a coordinate. His intentions do not really matter. If it quacks like a duck...TR 22:33, 20 June 2014 (UTC)
 * I disagree, as Schwarzschild uses R as only a mathematical convenience that approximates the coordinate r for small values of alpha. But trying to resolve that disagreement herein isn't important just now.Tm14 (talk) 13:33, 30 July 2014 (UTC)
 * It is not the case of units (but SI second is defined for local inertial system (and metre is directly linked via c) - i.e. this unit is different in different systems (gravity/metric), but timescale like UTC is defined/specified at rotating geoid). 195.113.87.138 (talk)06:41, 20 September 2011 (UTC)

Just want to point out to TimothyRias that the original Schwarzschild coordinate system compressed the entire event horizon down to a single point (therefore it is true that in those coordinates there is only the one singularity). General Relativity is all about changing coordinates, and there is nothing unusual about this. (Note that at the event horizon the singularity of the usual coordintes is only a coordinate artefact and not a second physical singularity anyway, as many better coordinate choices such as Kruskal-Szekeres demonstrate. Note also it is common that other metrics, such as for the Curzon solution for example, compress complicated regions of space-time into one singular point.) This issue with the history of the Schwarzschild solution (the ambiguity over the radial coordinate) commonly trips up those who are ignorant of it, so it is well worth clarifying the point in the appropriate section of this article. I hope you'll detail your own reasoning if you still intend to remove mention of it from the article. Cesiumfrog (talk) 23:30, 2 September 2012 (UTC)
 * The coordinate system in which Schwarzschild presented his solution is what we currently call Schwarzschild coordinates. In parallel, he used another set of "physical" coordinates in which the horizon coordinate singularity seemed to coincide with the coordinate singularity at the center of spherical coordinates. However, he never wrote down the metric in those coordinates.
 * This is much better summarized by the statement: "Schwarzschild took the position that the singularity at r = rs should be identified with the coordinate singularity at the origin present in spherical coordinates on flat space." Instead of a rather confused rambling supported by (mostly) unreliable sources/selective quoting from those sources.TR 06:30, 3 September 2012 (UTC)


 * If you're going to make accusations of selective quoting, perhaps you should first look for a reliable source that contradicts what all those sources say? Cesiumfrog (talk) 06:59, 3 September 2012 (UTC)
 * It would likely be helpful during this discussion to recognize that while r_s (as used here) may very well equate precisely with Schwarzschild's alpha, Schwarzschild himself only describes and requires that alpha be a constant that depends on the mass at the origin.Tm14 (talk) 20:44, 20 June 2014 (UTC)

Here are some references (which TM removed from the article): Also (a textbook exercise incidentally discusses the original form in a modern notation)
 * EJTP 8, No. 25 (2011) 65–82 Historically, the so-called ”standard Schwarzschild solution” was not the original Schwarzschild’s work, but it is actually due to J. Droste and, independently, H. Weyl, while it has been ultimately enabled like correct solution by D. Hilbert. Based on this, there are authors who [erroneously] claim that the work of Hilbert was wrong and that Hilbert’s mistake spawned black-holes[..] (note that's a quote from the abstract)
 * Reflections on Relativity, mathpages. Interestingly, the solution in Schwarzschild's 1916 paper was not presented in terms of what we today call Schwarzschild coordinates. Those were introduced a year later by Droste.  Schwarzschild presented a line element that is formally identical to the one for which he is [known..] However, he did not regard "R" as the physically significant radial distance from the center of the field. [..his alternative is equivalent] to the usual form of the Schwarzschild/Droste solution.  However[..] we appear to have a physically distinct result, free of any coordinate singularity except at r = 0

Isn't it fairly plain to see that the original set of four coordinates advanced by KS are not the same set of four coordinates which we currently attribute his name to? (Or should we ignore all the authorative expert secondary and tertiary sources and instead bow to TM's personal interpretation of a primary source?) Cesiumfrog (talk) 00:06, 4 September 2012 (UTC)
 * 1)The Reflections on Relativity reference is still in the article, and what I have written is supported by that reference. (Just to reiterate from your own quote: "Schwarzschild presented a line element that is formally identical to the one for which he is known,"
 * 2)Don't make a fool of yourself by calling any of these sources "authorative". (The bar for publishing in ELTP is really low, and "Reflections on Relativity" is a self published book.)
 * 3)One of the main reasons for my change was to prevent having multiple sets of incompatible notations floating around in the article (which a complete accessibility no-no). Content wise it does not say anything really different then before.TR 06:27, 4 September 2012 (UTC)
 * Schwarzschild used many sets of coordinates in his paper. Among these are (in his notation) (t, R, θ, φ) and (t, r, θ, φ). The former are the coordinates he used to write down his final solution for the line element, and coincide with what nowadays are known as Schwarzschild(-Droste) coordinates. However, Schwarzschild himself did not regard those as the true "physical" coordinates which he thought were the latter.TR 06:39, 4 September 2012 (UTC)


 * Exactly, the original solution is formally identical to the one for which he is known, he only presented it in terms of a different set of coordinates. (Hence, both the event horizon and the metric degeneracy are actually at the origin of the original coordinate system, unlike in the coordinates which bear his name.) Since your change was mainly motivated by notation (and there are no contradicting sources - hence policy is clear) I needn't quibble with your other points. FWIW I myself have witnessed some of the "erroneous authors" to whom the EJTP source refers (Crothers is one of them and, noting links to his website, may well be among the IP editors above); if their concern with this historical technicality appears mis-motivated to generally discredit the field, I can understand anyone's reluctance to concede a point they first raised. It just doesn't alter the uncontroversial facts of the matter in question, nor diminish its notability in the context of the history of this equation, is all. Cheers, I'll proceed with notational consistency in mind. Cesiumfrog (talk) 07:07, 4 September 2012 (UTC)
 * PS: Whoops, missed your second post. Are you now continuing to interpret the primary source in a manner which directly contradicts explicit statements of those three secondary/tertiary sources? Cesiumfrog (talk) 07:14, 4 September 2012 (UTC)
 * No, no interpretation on my part. This completely supported by what Kevin Brown says. The coordinate R used by Schwarzschild is what we nowadays call the "Schwarzschild radial coordinate".TR 09:27, 4 September 2012 (UTC)

I have some questions regarding this discussion. I can't read German so I'm taking at face value the two arXiv articles referenced via 2 & 5, as well as the results of reference 1. Given my understanding of Wikipedia's policies, don't we need some references explicitly refuting those results in order to argue that we can ignore them? Such a refutation could point out a flaw in Schwarzschild's derivation's mathematics, but that seems unlikely to exist at this point. More likely, such a refutation would explain as invalid Schwarzschild's assumption that the metric he sought must be regular everywhere except at the origin. But, for example, the derivation of the "conventional" metric given in this article can't logically be used as such a refutation because it arrives at its result using an incompletely justified approximation (especially with the strength of the fields involved). But even if a refutation of this sort exists, it seems it would still allow the construction of an exact solution per Schwarzschild's derivation, except then the resulting metric has two constants that need to be determined, ρ and α. Are there any references that describe what Schwarzschild's metric would be if ρ and α were not given any defined relation? At least those are the two obvious paths towards refutation - perhaps others exist. However, any such a refutation must take into account that, per reference 5, Schwarzschild based his work on a pre-release version of Einstein's published result. How it does so doesn't matter, as long as it is cognizant of that assertion in reference 5.Tm14 (talk) 20:44, 20 June 2014 (UTC)
 * I think WP:EXCEPTIONAL is relevant here. Ref 1&5 do not meet that bar by a long shot. The claims made co-against everything that is in mainstream textbooks. Those sources are WP:FRINGE, and policy does not require us to refute anything they say. As it stands, the current article discusses the misconceptions expressed in those sources (without actually referring to them which would be WP:UNDUE.)TR 22:13, 20 June 2014 (UTC)
 * Could a reference for Hilbert's paper "published the following year" be added to the article, as that is the ultimate source of all the issues discussed both herein and therein?Tm14 (talk) 13:33, 30 July 2014 (UTC)