Dim Stars: Are There Almost-Black Holes in the Universe?

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Discussion Overview

The discussion revolves around the concept of "almost black holes," specifically focusing on stars that are just below the mass threshold required to become black holes. Participants explore the implications of gravitational time dilation on the luminosity and redshift of such stars, as well as the characteristics of neutron stars in this context.

Discussion Character

  • Exploratory
  • Debate/contested
  • Technical explanation
  • Mathematical reasoning

Main Points Raised

  • Some participants propose that if a star were almost massive enough to become a black hole, gravitational time dilation would make it appear very dim, potentially emitting only a fraction of the energy expected based on its mass.
  • Others question whether such "almost black holes" would exhibit intrinsic redshift, referencing Halton C. Arp's ideas on redshift in quasars.
  • A participant asserts that only neutron stars can exist below the black hole mass threshold, suggesting that they would exhibit significant redshift due to their gravitational effects.
  • Some participants discuss the mathematical aspects of gravitational redshift and time dilation, providing equations and parameters related to neutron stars and their properties.
  • There are differing views on whether light emitted from such stars would appear dim to observers, with some arguing that light would travel at normal speed once it escapes the gravitational influence, while others contend that gravitational effects would indeed reduce the apparent luminosity.
  • Participants engage in clarifying terms such as mass (M) and redshift (z), with some expressing confusion over their definitions and implications.
  • There are corrections and challenges regarding the understanding of gravitational redshift and the behavior of light in strong gravitational fields, with some participants asserting that light can change speed under certain conditions.

Areas of Agreement / Disagreement

The discussion contains multiple competing views and remains unresolved on several key points, particularly regarding the implications of gravitational time dilation and the nature of light emitted from stars near the black hole threshold.

Contextual Notes

Participants reference specific mathematical models and concepts, such as the Schwarzschild interior metric and gravitational redshift equations, but do not reach a consensus on their interpretations or applications.

mrspeedybob
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If there were a star which was almost, but not quite massive enough to become a black hole it seems as though gravitational time dilation should make it appear very dim. If time dilation resulted in 1/1000 of the time passing within the star as passes for us, we should see a star emitting 1/1000 the energy that it's mass would otherwise suggest. Do we see such stars in the universe?
 
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Just an off-the-wall question from a non-astronomer: Would these "almost black holes" exhibit an intrinsic red-shift? I think I remember that Halton C. Arp proposed that for explaining the red-shift of quasars.
 
mrspeedybob said:
If there were a star which was almost, but not quite massive enough to become a black hole it seems as though gravitational time dilation should make it appear very dim. If time dilation resulted in 1/1000 of the time passing within the star as passes for us, we should see a star emitting 1/1000 the energy that it's mass would otherwise suggest. Do we see such stars in the universe?

No, such objects can only be Neutron Stars, which are extremely tiny in size, yet comparable to the mass of the Sun. There are no stars that are still fusing elements in their cores that are anywhere close to being a black hole.

Your question should apply to a neutron star though. I would expect to see significant redshift on radiation coming from a neutron star.
 
mrspeedybob said:
If there were a star which was almost, but not quite massive enough to become a black hole it seems as though gravitational time dilation should make it appear very dim. If time dilation resulted in 1/1000 of the time passing within the star as passes for us, we should see a star emitting 1/1000 the energy that it's mass would otherwise suggest. Do we see such stars in the universe?

A star that is not quite a black hole is a neutron star. The energy that comes off of a neutron star is red shifted, but I don't know how much.

Last I looked only one neutron star had been directly observed. (Usually we see the glow of the surrounding matter.) But that should enough to get a real figure.
 
mrspeedybob said:
If there were a star which was almost, but not quite massive enough to become a black hole it seems as though gravitational time dilation should make it appear very dim. If time dilation resulted in 1/1000 of the time passing within the star as passes for us, we should see a star emitting 1/1000 the energy that it's mass would otherwise suggest. Do we see such stars in the universe?

The smallest a neutron star can get before run away collapse occurs is r0=9M/4 or 2.25M in order to have positive tangential pressures (according to the Schwarzschild interior metric, this is the point that the time dilation at the very interior of the star becomes zero). If we consider the gravitational redshift-

[tex]z=\frac{1}{\sqrt{1-\frac{2M}{r}}}-1=\frac{\lambda_o-\lambda_e}{\lambda_e}[/tex]

where z is the redshift, [itex]\lambda_o[/itex] is the wavelength observed and [itex]\lambda_e[/itex] is the wavelength emitted. The above can be rewritten-

[tex]\lambda_o=(z\cdot\lambda_e)+\lambda_e[/tex]

if we consider a 3 sol mass as an absolute maximum, then M=4430.55, then you can pretty much work out what z would be and what the emitted wavelength of light would be shifted to.

Regarding gravitational time dilation, this would be expressed as-

[tex]d\tau=dt\sqrt{1-\frac{2M}{r}}[/tex]

so the greatest time dilation due to gravity at the surface of a stable neutron star at the very boundary of collapse would be 0.333 or ~1/3.
 
Last edited:
Duh.

What's M? What's z?
 
ImaLooser said:
Duh.

What's M? What's z?

I believe M = mass, and Z = the measure of redshift.
 
Yes, but, just to clarify, M is expressed in units of solar mass.
 
  • #10
I don't think it would appear dim to us. Light would travel very slowly away from it when released because of massive gravity pulling backwards, but as soon as the light moves far enough away it would resume its 'speed of light' pase. And reach us just like a normal star. Unless gravity pulled back some photons and not others it would have the same luminosity
 
  • #11
Rorkster2 said:
I don't think it would appear dim to us. Light would travel very slowly away from it when released because of massive gravity pulling backwards, but as soon as the light moves far enough away it would resume its 'speed of light' pase. And reach us just like a normal star. Unless gravity pulled back some photons and not others it would have the same luminosity

It appears you have a mistaken view of "gravitational redshift". It is true when we say photons "climb out of the gravitational potential" of a massive object. But this does not mean their velocity is changed...they still travel at c. What happens is just what's been mentioned above: redshift. This term comes from the optical part of the EM spectrum where red is a longer wavelength than, say, blue. This means the WAVELENGTH of the light has been stretched out and its "color" will be different (redder). Light never "slows down" or "resumes its pace", at least in this kind of example.
 
  • #12
stevebd1 said:
Tso the greatest time dilation due to gravity at the surface of a stable neutron star at the very boundary of collapse would be 0.333 or ~1/3.

Does this mean that one second passes on the nutron star for every 3 seconds outside of it? If so, then I'd think that that would indeed dim the star by a factor of 3. Regardless of red shift, the star would produce one third the number of photons in 1 second that it would in 3. And an observer on the neuron star would see the rest of the universe as sped up, and three times as bright.
 
  • #13
Bobbywhy said:
It appears you have a mistaken view of "gravitational redshift". It is true when we say photons "climb out of the gravitational potential" of a massive object. But this does not mean their velocity is changed...they still travel at c. What happens is just what's been mentioned above: redshift. This term comes from the optical part of the EM spectrum where red is a longer wavelength than, say, blue. This means the WAVELENGTH of the light has been stretched out and its "color" will be different (redder). Light never "slows down" or "resumes its pace", at least in this kind of example.

Sorry to say but i believe your wrong. First off, light can indeed change its speed. For example, in near absolute zero it is possible to slow photons to a crawl, and also 'speed of light' refers to its speed when traveling threw a vaccuum, not its constant speed. Next, you are right in saying that the redshift and blueshift waves are a derived from its frequnecy, however in this example you also have to include the fact that light DOES slow down, because black holes change light momentum from going 'forward' to 'backwards', and a near black hole object would be in the very close inbetween where it slows down but does not quite go 'backward'
 
  • #14
Rorkster2 said:
Sorry to say but i believe your wrong. First off, light can indeed change its speed. For example, in near absolute zero it is possible to slow photons to a crawl, and also 'speed of light' refers to its speed when traveling threw a vaccuum, not its constant speed.

It is a well known fact that light does indeed change speeds in a material, but when anyone says that the speed of light doesn't change or is invariant they are referring to the velocity in a vacuum, which is c always.

Next, you are right in saying that the redshift and blueshift waves are a derived from its frequnecy, however in this example you also have to include the fact that light DOES slow down, because black holes change light momentum from going 'forward' to 'backwards', and a near black hole object would be in the very close inbetween where it slows down but does not quite go 'backward'

This is incorrect. The change in momentum in no way affects the speed of light. As for the forward and backward stuff, I'm not sure what you are getting at.
 
  • #15
The time dilation factor goes by (1 + z), so a neutron star with a gravitational redshift of .33 would be time dilated by 1/1.33, or basically it would take 1.33 seconds to emit the same amount radiation as it would radiate in 1 second if not redshifted.
 
  • #16
Chronos said:
Yes, but, just to clarify, M is expressed in units of solar mass.

Aha. Well, I'm duh again because I don't know what it means to express radius of an object in units of mass.
 
  • #17
ImaLooser said:
Aha. Well, I'm duh again because I don't know what it means to express radius of an object in units of mass.

The radius isn't being expressed in units of mass. You are dividing the mass by the radius because more mass packed into a smaller radius means more gravity and more time dilation.
 
  • #18
ImaLooser said:
Aha. Well, I'm duh again because I don't know what it means to express radius of an object in units of mass.

In the paper posted by Chronos, M refers to mass, in the post I made, M is the geometric unit of mass, sometimes referred to as the gravitational radius where M=Gm/c2 where G is the gravitational constant, m is the mass in SI units (i.e. kg) and c is the speed of light in m/s.
 
  • #19
Rorkster2 said:
because black holes change light momentum from going 'forward' to 'backwards'

If a photon is considered to be without mass how can light have momentum?

note: my only exposure to physics has been in an AP mechanics class and in the books I've read over this summer. (i won't begin more formal study until i begin college next fall)
 
  • #20
grantwilliams said:
If a photon is considered to be without mass how can light have momentum?

note: my only exposure to physics has been in an AP mechanics class and in the books I've read over this summer. (i won't begin more formal study until i begin college next fall)

The momentum and energy of a photon is determined by the frequency. Higher frequency photons have more momentum and energy. You can read a bit more here: http://en.wikipedia.org/wiki/Photon#Physical_properties

If that isn't detailed enough or doesn't answer your question just say so.
 

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