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Schwarzschild Metric: The Sun

  1. Jul 6, 2009 #1
    In 1916 Schwarzschild wrote down his famous metric to solve (or re-solve using a polar coordinate system) the precession of the perihelion of Mercury. The curvature of spacetime described by the Metric is for any non-rotating spherically symmetric mass.

    [tex]ds^2 = -(1-\frac{2M}{r})dt^2 + (1-\frac{2M}{r})^{-1}dr^2 + r^2(d\theta^2+sin^2\theta d\phi^2)[/tex]

    Does this imply there is a black hole at the center of the Sun, the Earth etc?
     
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  3. Jul 6, 2009 #2

    diazona

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    Nope. That Schwarzschild metric only applies outside a solid body - there's a different metric that describes the inside of the Sun or Earth.
     
  4. Jul 7, 2009 #3
    Is the different metric just the Newtonian one?
     
  5. Jul 7, 2009 #4

    A.T.

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  6. Jul 7, 2009 #5
    The interior solution according to George Jones:

    [tex]d\tau^{2}=\left( \frac{3}{2}\sqrt{1-\frac{2M}{R}}-\frac{1}{2}\sqrt{1-\frac{2Mr^{2}}{R^{3}}}\right) ^{2}dt^{2}-\left( 1-\frac{2Mr^{2}}{R^{3}}\right) ^{-1}dr^{2}-r^{2}\left( d\theta ^{2}+\sin ^{2}\theta d\phi ^{2}\right)[/tex]

    I note that in addition to the singularity at [tex]R=2M[/tex] there is a new singularity at [tex]r^2=R^3[/tex] and the expression goes complex when [tex]r^2 > R^3[/tex]

    I assume that this means that the interior solution line integral predicts a nasty end for an astronaut at a height of [tex]\sqrt{(6371000^3)} - 6371000[/tex] = 16 million kilometers from the surface of the Earth

    (I'm being facetious)

    Can I ask how the interior Schwarzschild solution was derived? (Not by Schwarzschild, obviously)
     
  7. Jul 7, 2009 #6

    George Jones

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    Yes, this solution was found originally by Schwarzschild. It represents a constant density perfect fluid that is spherically symmetric. Derivation of this solution are given in, for example,

    General Relativity: An Introduction for Physicists by Hobson, Efstathiou, and Lasenby

    Gravitation by Misner, Thorne, and Wheeler.

    [itex]r = R[/itex] represents the surface of the spherical body. If

    [tex]R > 2M \frac{9}{8},[/tex]

    then the solution has no singularities. At

    [tex]R = 2M \frac{9}{8},[/tex]

    the solution develops a pressure singularity at its centre.

    This solution is an "almost realistic" toy model for a spherical body.
     
  8. Jul 7, 2009 #7
    George

    How can a fluid sphere have a constant density? Isn't that a tad unrealistic?
     
  9. Jul 7, 2009 #8

    George Jones

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    Of course it is a tad unrealistic. Notice that I said that the soultion is almost realistic, and I enclosed the words in scare quotes. For spherically bodies made from perfect fluids, Einstein's equation reduces to a coupled pair of first-order ordinary differential equations,

    [tex]
    \frac{dm}{dr} \left( r \right) = 4 \pi r^2 \rho (r)
    [/tex]

    and the Oppenheimer-Volkoff equation (12.21) from the link below. For the case of constant density, this coupled pair of differential equations has an exact solution. For more realistic cases, the existence and uniqueness theorems for differential equations guarantee that a solutions still exist, but, unfortunately, solutions can not be written down in terms of elementary or standard special functions. As is the case for realistic treatments of many areas of physics, numerical methods must be used. See the paragraph on page 293 starting with "The closed system of three equations ..."

    http://books.google.ca/books?id=xma1QuTJphYC&lpg=PP1&dq=lasenby&pg=PA293

    Even more realistic treatments ditch spherical symmetry (e.g., axisymmetric rotating stars) and consider material other than perfect fluids.
     
  10. Jul 7, 2009 #9
    Thanks George and everyone else who answered. More to think about.
     
  11. Mar 21, 2010 #10
    Sorry for the thread necromancy, but what about the other singularity that diamond pointed out? The r^2 = R^3 (as it happens i recently ran face first into that rather annoying singularity myself so i'm interested as to its properties). Is there a known coordinate transformation that removes it? I can't see any reason why it would be a physical singularity...

    Also in the interior metric given, shouldn't the mass term in the radial coefficient be m(r) not M?

    Cheers
    -G

    EDIT: Just read the theorem here:
    http://books.google.ca/books?id=xma1QuTJphYC&lpg=PP1&dq=lasenby&pg=PA293#v=onepage&q=&f=false
    I suppose this answers some questions about the pressure singularity, but thats not the same as the one diamond pointed out right? I mean the physical location of that one depends strongly on if R>1 or R<1
     
    Last edited: Mar 21, 2010
  12. Mar 22, 2010 #11
    If r^2 >= R^3 then r > R and you are outside the body and the interior solution does not apply and you should be using the exterior (regular) Schwarzschild solution.

    If you are still interested in discussing the case for non uniform density distribution of M(r) then just ask. I studied this topic a while back.

    P.S. What we should be concerned with is the case when 2M*r^2>=R^3. I will need to think about that when I am less tired.
     
    Last edited: Mar 22, 2010
  13. Mar 22, 2010 #12
    Let us consider the clock of a stationary observer so [itex] dr^{2} = r^{2}\left( d\theta ^{2}+\sin ^{2}\theta d\phi ^{2}\right) = 0[/atex] so that the interior solution can be simplified to:

    [tex]\frac{d\tau}{dt}= \frac{3}{2}\sqrt{1-\frac{2M}{R}}-\frac{1}{2}\sqrt{1-\frac{2Mr^{2}}{R^{3}}}[/tex]

    By setting the quantity dtau/dt to zero, I can solve for r to find the location of the singularity and obtain:

    [tex]r = \pm R \sqrt{9-\frac{4R}{M}} [/tex]

    which is unique if we only consider positive values of r.
    There are not two separate singularites at R=2M and r^2=R^3 as conjectured by Diamond.

    Now if we plug in R = (9/8)Rs = 9M/4 the singularity is at r=0 as expected.

    For R = 2M the singularity has moved out to r = 2M and what is surprising is that for r<2M the ratio of proper time rate to coordinate time rate (dtau/dt) is negative and real . In other words proper time is running in the opposite direction to the coordinate time for a stationary observer inside the the boundary of the massive body.

    Even more interestingly when R=M (ie the body has collapsed to a physical radius less than the Shwarschild radius) the interior solution predicts there is no singularity or imaginary or complex values for (dtau/dt) according to a stationary observer inside the collapsing body, but the singularity at r=2m remains because the exterior Schwarzschild solution is valid in that region.
    The above conclusios assume a unform density distribution but it reasonable to assume that is unphysical. A more realistic aproximation is that density increases towards the centre.

    Now the original equation with average density (d) explicity stated is:

    [tex]\frac{d\tau}{dt}= \frac{3}{2}\sqrt{1-\frac{2M}{R}}-\frac{1}{2}\sqrt{1-\frac{2M^{2}}{r}\frac{4/3 \pi r^3 d}{4/3 \pi R^3 d}}[/tex]

    After cancelations it is easy to see the above equation reduces to the familar form at the top of this post.

    Now if we set density as function d(r) of radius so that d(r) = d/r which is a bit more realistic, then the ratio of the enclosed mass to the total mass of the is proportional to r^2/R^3 rather than r^3/R^3 for the uniform density case and the equation becomes:

    [tex]\frac{d\tau}{dt}= \frac{3}{2}\sqrt{1-\frac{2M}{R}}-\frac{1}{2}\sqrt{1-\frac{2Mr}{R^{3}}}[/tex]

    Solving this for r when dtau/dt=0 gives the location of the singularity as:

    [tex]r = R^2 \left(9-\frac{4R}{M}\right) [/tex]

    Using this slightly more realistic equation (density increasing towards infinite going towards the centre) we can see that a singularity still occurs ar r=0 when R=9/8(2M).
     
    Last edited: Mar 22, 2010
  14. Mar 22, 2010 #13
    Hey kev,

    Cheers for the replies! Your point about the reversal of proper time is familiar, i remember reading a paper where someone wanted to re-define the event horizon (or perhaps invent a new one) as the point where this switch occurs.

    Next question :) Given that the singularity is of pressure, a scalar, you can't do a coordinate transform to get rid of it. So, either I need a new density profile that doesn't give rise to this which means solving the tolman-oppenheimer-volkov equation (which i've tried and not fared very well so far but i think that's because i've no idea what i'm doing really) or a different interior solution.

    In terms of the latter i have found these papers:
    http://www.jstor.org/stable/78530
    http://www.springerlink.com/content/w568765vt481871r/
    The second is a comment on the first essentially doing some more checks to make sure its viable, where the first gives a new interior schwarszchild solution that, alledgedly, does not have a pressure singularity even for constant density (the physical viability of this is somewhat dubious to me but anyway).

    It all seems very good but in the first paper in eqn 1.3 i am unsure as to the difference between R and a. He defines a as the radius of the region bounding the mass, which surely is the radius of the object which is normally R?

    EDIT: Oops i'm retarded, think i got it now :) Still: would appreciate comments on that metric

    Cheers
    -G
     
    Last edited by a moderator: Apr 24, 2017
  15. Mar 22, 2010 #14

    JesseM

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    That switch is only when you compare proper time to coordinate time in Schwarzschild coordinates though, if you use a different coordinate system no such switch occurs at the horizon.
     
  16. Mar 22, 2010 #15
    Your welcome :smile:
    It is important to note that in the regular Schwarzschild metric the proper time of a stationary clock below the event horizon is imaginary relative to an observer outside the event horizon. (The interpretation is that a clock can not remain spatially stationary below the event horizon.) As Jesse points out this apparent "switch" across the event horizon is not visible in the coordinates of a free falling observer. The situation is different in the interior Schwarschild solution, where the proper time rate of a stationary clock below the singularity remains real, relative to the clock of an observer above the singularity but runs in the reverse direction.

    The equation they give is meant to be the classic Schwarzschild solution, equivalent to the one given by George earlier in this thread. (The new solution is not visible in the introduction of the paper.)

    By considering a stationary event, as in my last post the interior solution in the paper simplifies to:

    [tex]\frac{d\tau}{dt}= \frac{3}{2}\sqrt{1-\frac{a^2}{R_*^2}}-\frac{1}{2}\sqrt{1-\frac{r^{2}}{R_*^{2}}[/tex]

    By comparing their equation to the one given by George, it is fairly easy to work out that [tex]a = R[/tex] and [tex]R_*^2 = R^3/2M[/tex].
    If we wish to equate [tex]R_*[/tex] with [tex]R[/tex] then the equation is only valid for a massive body has a physical surface ar R=2M and if the observer is located exactly at the event horizon, but that limits the general application of the equation. This is a bit wierd and it would make the clarity of the rest of the article a bit hard to follow.
     
    Last edited by a moderator: Apr 24, 2017
  17. Mar 22, 2010 #16
    Sorry if i'm missing something trivial here, but why must this be true? I'm not too concerned about the singularity at R = 2M, but I definitely want the solution to be valid for external observers.

    If it isn't and thus as you say i'm then not interested in this solution, what do you suggest for an approach to find an interior solution that does not have this pressure singularity? I've had great trouble finding/solving for one although i understand it can be done numerically but i'd rather not resort to that (I wish to take limits).

    cheers
    -G
     
  18. Mar 22, 2010 #17
    I was just saying if you want to read [tex]R_*[/tex] in their equation as [tex]R[/tex] in George's equation, then that is only valid if the clock is at R=2M. The best thing to do is substitute [tex]R=a[/tex] and [tex] R^3/2M= R_*^2 [/tex] in their equation and read it as the normal interior equation. To see their new equation try and obtain a copy of the full paper at a library.

    As far as being valid for external observers you have to superimpose the exterior solution on the interior solution. Work out the clock rate for r<R relative to a clock at [STRIKE]the surface of the body (at R)[/STRIKE] infinity using the interior solution and then work out the the clock rate r>R relative to a clock at [STRIKE]the surface (R)[/STRIKE] infinity using the exterior solution and you can obtain a comparison of clock rates above and below the surface of the body.

    Has it occured to you that the pressure singularity inside the solid body might be physical and not removable by a change of coordinates?
     
    Last edited: Mar 23, 2010
  19. Mar 22, 2010 #18
    Yes, infact i stated that in a previous post when i asked if anyone knew if the TOV equation had exact solutions for densitys other that a constant profile. As far as i can tell this new metric is not simply a change of coordinates but a totally different formulation.

    Also, sorry, i didn't realise you only had access to the previews. Full text is here: http://members.iinet.net.au/~housewrk/Papers/ [Broken]

    Essentially what i want to do is solve the relativistic Klein Gordon equation on the interior of say a star then match that solution to the exterior solution found using the exterior metric then propagate outwards and find a phase shift. I also don't want to be inhibited as to the size/mass of the object hence why that pressure singularity is an issue for me.

    I have made the substitution you suggested using the new metric he gives in the paper for the constant density profile without the singularity (again, not entirely sure of the validity of this but as i mentionde previously this isn't a coordinate change rather a totally different formulation. I am unsure wether its appropriate or not but am giving it a go just to see what happens)

    Hope that makes sense!
    Cheers
    -G
     
    Last edited by a moderator: May 4, 2017
  20. Mar 23, 2010 #19
    The fully contracted Riemann tensor, called the Kretschmann invariant scalar, of the Schwarzschild metric will reveal the singularity at r = 0.

    K == 48 m^2 / r^6.
    How do we know that r = 0 is a true singularity? Scalars are invariant under a coordinate transformation. Thus, a singularity exists for r = 0.

    The r = 2m is a coordinate singularity.
     
  21. Mar 23, 2010 #20
    I'm not currently concerned with the singularity at r = 2m...
     
  22. Mar 23, 2010 #21
    This is true for the exterior Schwarzschild solution when a black hole has formed. I think Funky is interested in the singularity that appears at r=0 when the radius of the massive body is R=9/8(rs) before a black hole has formed. This singularity moves outwards as R reduces towards 2M and ends up at traditional event horizon at 2M when the body has contracted to exactly R=2M suggesting that this "pressure singularity" is simply the classic Schwarzschild event horizon and removable by a coordinate transformation.

    If we look at the classic interior Schwarzschild solution and assume radial motion only we get:

    [tex]d\tau^{2}=\left( \frac{3}{2}\sqrt{1-\frac{2M}{R}}-\frac{1}{2}\sqrt{1-\frac{2Mr^{2}}{R^{3}}}\right) ^{2}dt^{2}-\left( 1-\frac{2Mr^{2}}{R^{3}}\right) ^{-1}dr^{2}[/tex]

    When the pressure singularity appears at R=9/8(2M) for dr=0, it is apparent that this can be removed by assuming a non zero value for dr (eg considering a free falling test particle) and this might provide a way forward for Funky.
    Thanks for the link. It was helpful to me. Although the calculations you are talking about doing are out of my league I thought I might offer a few observations that might be helpful.

    As before I will refer to the variable "R" used in the paper as [tex]R_*[/tex] to distinguish it from the R variable used in George's equation and the two are related by [tex]R_* = R^3/(2M)[/tex]. I should have noticed earlier that they are using [tex]R_*[/tex] to represent a density rather than a radius.

    The average density is [itex]p = (4/3)\pi R^3/(M)[/itex] so by rearranging that it can be seen that [itex]3p/(8\pi) = R^3/(2M) = R_*[/itex]

    That might be hepful in physically interpreting the variables used in the paper.

    There is still something that is bothering in the paper though. In Equation (4) representing the classic interior solution, the dt^2 term is different from the dt^2 term given their new interior solution in Equation (16) of the paper. All the other parameters remain unchanged. When performing a transformation you can not just simply change one parater in isolation because another parameter has to change to compensate. This suggests that the new solution is not a coordinate transformation of the classic solution. Now in the exterior solution it is often said that Schwarzschild made an unfortunate choice of coordinates that results in a coordinate singularity at 2M and this is removed by a simple transformation of his metric. In this paper they are removing the singularity by a transformation but are essentially saying Schwarzschild's solution is wrong and that he made a mistake somewhere. That is big claim to make and they do not make it clear where they think Schwarzschild made his mistake.

    Good luck with your project and let me know if you make any progress or draw any interesting conclusions!
     
    Last edited by a moderator: May 4, 2017
  23. Mar 23, 2010 #22
    I think the point in the paper is that (around equation 2.12) they relax some condition in the einstein equations (his new solution is still a solution to the EFE) and so its not a transformation but rather a reformulation. I'm still not sure if this is a useful/valid solution as I haven't rigorously worked through the tensor stuff but according to a friend who has far more skill and experience in GR there are no glaring omissions or errors, so i'm tentatively using it...for now. Its just that solving the TOV equation for a varying density is a royal pain in the arse so i'd like to believe this will work :)
     
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