Speed of Light & Accelerating Frames

In summary, the speed of light is constant when viewed from any reference frame. However, when an object (such as a mass greater than 0) is placed at the Schwarzschild radius of a black hole, the speed of light slows down to 0, and the object is effectively "tethered" to the black hole.
  • #1
anantchowdhary
372
0
Does speed of light Change with respect to accelerating frames

It shouldn't be as gravitational time dilation exists
 
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  • #2
No, the speed of light is constant when viewed from any reference frame.
 
  • #3
No, the speed of light slows down to = 0 at the Schwarzschild radius of the black hole, to the frame of the external observer.
 
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  • #4
quantum123 said:
No, the speed of light slows down to = 0 at the Schwarzschild radius of the black hole, to the frame of the external observer.
This is not true, the photon is simply red shifted to zero frequency.
 
  • #5
If you look at the Schwarzschild solution, you just let ds=0 (light-like), you will obtain
dr/dt = 1 - 2GM/r , which proves what I said.
 
  • #6
Oh dear oh dear...

anantchowdhary said:
Does speed of light Change with respect to accelerating frames

It shouldn't be as gravitational time dilation exists

Depends upon what you mean by "speed".

I am guessing that you mean velocity of a particle very near some observer, with respect the frame field (local Lorentz frame) of that observer. If so, the speed of light "at the level of tangent spaces" is indeed unity (in geometric units) in any Lorentzian manifold.

But note that "coordinate speed" is not in general geometrically or physically meaningful.

Also, there are many distinct operationally significant notions of "distance in the large" and thus "velocity in the large", even in flat spacetime (for accelerating observers, such as Rindler or Bell observers).

Hootenanny said:
No, the speed of light is constant when viewed from any reference frame.

Here, in a Lorentzian manifold, Hootenanny's "reference frame" is what I called a frame above. A frame field is a set of vector fields which forms a basis for the tangent space at eacn event. Just a vector is one bit of a vector field, a frame is one bit of a frame field. Frames are also called vierbeins, among various other names.

quantum123 said:
No, the speed of light slows down to = 0 at the Schwarzschild radius of the black hole, to the frame of the external observer.

Note that quantum123 is referring to a coordinate speed (slope) computed for radial null geodesics in a particular chart (the exterior Schwarzschild chart) for a particular exact solution of the EFE, the Schwarzschild vacuum. But the word "frame" is inappropriate here since frames are associated with operationally significant quantities, but coordinate speeds are not in general physically meaningful.

quantum123 said:
If you look at the Schwarzschild solution, you just let ds=0 (light-like), you will obtain
dr/dt = 1 - 2GM/r , which proves what I said.

This is an easy way of finding the radial null geodesics in the above mentioned chart, and of verifying the property of the coordinate speeds which you mentioned.

But of course light never "slows down" in any Lorentzian manifold (that wouldn't even make sense!), which is an indication that this refers to a spurious property of a particular chart. That is, it is a (bad) property of a particular representation of (part of) this spacetime, not a propery of the spacetime itself. That is why it is not geometrically or physically meaningful.
 
  • #7
Good and bad

Well it is bad to you but good to me. It is relative. :biggrin:
To the observer, the light photon will approach the event horizon, both its speed(dr/dt) and vibration slowing down, virtually stopping at the horizon. The same goes for any mass>0 object.
 
  • #8
quantum123 said:
Well it is bad to you but good to me. It is relative. :biggrin:
To the observer, the light photon will approach the event horizon, both its speed(dr/dt) and vibration slowing down, virtually stopping at the horizon. The same goes for any mass>0 object.

As Chris Hillman points out at some length, the word "speed" is ambiguous. The speed of light is always constant when measured with local clocks and local rulers. In fact, we have to go back to a very old defintion of the meter to even talk about measuring the speed of light - using the modern SI defintion of the meter, the speed of light (defined in the frame-field sense that Chris Hillman talked about at length) is a constant by defintion.

Therfore you need to be somewhat careful about assuming that people share the same coordinate-based defintion of speed that you are using. Your notion of "speed" is not compatible with the SI defintion of the speed of light, for instance, while Chris Hillman's defintion is.
 
  • #9
SR vs GR again?
 
  • #10
Speed |v| = sqrt(v1^2+v2^2+v3^2)
v1=d/dt(x1)
v2=d/dt(x2)
v3=d/dt(x3)
d/dt(x1)=d/dt(r)sin(theta)cos(phi)
d/dt(x2)=d/dt(r)sin(theta)sin(phi)
d/dt(x3)=d/dt(r)cos(theta)
Hence
d/dt(r)=0
=> d/dt(x1)=d/dt(x2)=d/dt(x3)=0
=> v1=v2=v3=0
=> |v|=0
=> speed =0
 
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  • #11
please gimme a definite answer.yes or no?And how do u visulaize curvature of space-time when there is nothing to curve
 
  • #12
anantchowdhary said:
please gimme a definite answer.yes or no?And how do u visulaize curvature of space-time when there is nothing to curve
In terms of local inertial coordinate systems (defined in terms of measurements made by freely-moving observers in a small region of space and time) the speed of light is always c. But in terms of nonlocal coordinate systems in curved spacetime it doesn't have to be, and likewise, if you use a non-inertial (accelerating) coordinate system in flat spacetime it also may not be c.
 
  • #13
Hi, Thrice

Thrice said:
SR vs GR again?

If you are referring to the existence of multiple distinct notions of "distance in the large", and thus of "velocity in the large", these arise even in flat spacetime, when you study accelerated observers such as the Bell or Rindler observers (IOW, arises even in scenarios you would study using str). This is a (fundamental) issue in Lorentzian manifolds, it doesn't really have anything to do with gtr versus str.
 
  • #14
http://www.geocities.com/physics_world/gr/uniform_light.htm

Speed of Light in a Uniform Field

Home


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The metric in a uniform gravitational field is, by the equivalence principle, identical to the metric in a accelerated frame

[Eq. 1] ds2 = -c2(1 + gz/c2)2dt2 + dx2 + dy2 + dz2

where c is the speed of like in a vacuum in a Minkowski frame of reference.

Since light moves on null geodesice, i.e. we set ds2 = 0 in [Eq. 1]

[Eq. 2] -c2(1 + gz/c2)2dt2 + dx2 + dy2 + dz2 = 0

Divide through by dt2, and substitute vx = dx/dt, vy = dy/dt, vz = dz/dt, v2 = vx2 + vy2 + vz2

-c2(1 + gz/c2)2 + dx2/dt2 + dy2/dt2+ dz2/dt2 = -c2(1 + gz/c2)2dt2 + (dx/dt)2 + (dy/dt)2+ (dz/dt)2 = 0

-c2(1 + gz/c2)2 + vx2 + vy2 + vz2 = -c2(1 + gz/c2)2 + v2 = 0

v2 = c2(1 + gz/c2)2

[Eq. 3] v = (1 + gz/c2)c

Let F = gz. Note that we choose the arbitrary constant, that is usually associated with a Newtonian potential, to be zero.

[Eq. 4] v = (1 + F/c2)c

This is exactly the result obtained by Einstein in 1907 [1]


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References

[1] On the Relativity Principle and the Conclusions Drawn from It, Albert Einstein, Jahrbuch der Radioaktivitat und Electronik 4 (1907)
 
  • #17
maybe they are wrong or right...

tnx for the reply maybe the studies are wrong or right... but speed of light might change then it will be a small speed diff. but we are not yet sure of this...
 
  • #18
Ruian said:
tnx for the reply maybe the studies are wrong or right... but speed of light might change then it will be a small speed diff. but we are not yet sure of this...

the question you have to ask yourself is: how would we ever know that c has changed in a context where absolutely nothing else did (particularly the dimensionless constants of nature)? we measure (or perceive) only dimensionless quantities, and if you think you measured a change in c, you measured a change in some ratio of c against some other like-dimensioned quantity (perhaps [itex] e^2/(4 \pi \epsilon_0 \hbar) [/itex]) and that changing dimensionless quantity is the only salient measure.
 
  • #19
rbj said:
the question you have to ask yourself is: how would we ever know that c has changed in a context where absolutely nothing else did (particularly the dimensionless constants of nature)? we measure (or perceive) only dimensionless quantities, and if you think you measured a change in c, you measured a change in some ratio of c against some other like-dimensioned quantity (perhaps [itex] e^2/(4 \pi \epsilon_0 \hbar) [/itex]) and that changing dimensionless quantity is the only salient measure.

I am not saying that I FOUND c to be changing. What i am only saying is that we still must consider what some studies are presented. like speed of light might change. It is maybe its right or wrong. We still don't know. Currently we are considering c to be constant because
it was supported by experiments and used by some theories... Remember that Nicolaus Copernicus was once not beleived that the sun is the center of the universe...:smile:
 
  • #20
Ruian said:
I am not saying that I FOUND c to be changing. What i am only saying is that we still must consider what some studies are presented. like speed of light might change. It is maybe its right or wrong. We still don't know. Currently we are considering c to be constant because
it was supported by experiments and used by some theories... Remember that Nicolaus Copernicus was once not beleived that the sun is the center of the universe...:smile:
I think rbj's point is that the notion of a dimensionful constant changing is inherently meaningless, because the only constants that actually have physical meaning are dimensionless ones...this article explains the idea pretty well:

http://www.phys.unsw.edu.au/~dzuba/varyc.html
 
  • #21
Maybe it's not c which varies, but the speed of light (which could be not exactly equal to c, depending on the frequency); c could be a limit for EM speed.
When we say that light's speed is equal to c, to which frequency do we refer? This is not specified, but, however, we have never used extremely high or extremely low frequencies, for example, so, how can we know it can't vary with frequency?
 
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  • #22
lightarrow said:
Maybe it's not c which varies, but the speed of light (which could be not exactly equal to c, depending on the frequency); c could be a limit for EM speed.
When we say that light's speed is equal to c, to which frequency do we refer? This is not specified, but, however, we have never used extremely high or extremely low frequencies, for example, so, how can we know it can't vary with frequency?

But there's at least evidence that it doesn't change with frequency within the range that we know of already. There's zero evidence to the contrary. So we go by what we can verify, not what we can speculate. That's how physics works, and that's why you depend on things to work when you wake up every morning.

Zz.
 
  • #23
ZapperZ said:
But there's at least evidence that it doesn't change with frequency within the range that we know of already. There's zero evidence to the contrary. So we go by what we can verify, not what we can speculate. That's how physics works, and that's why you depend on things to work when you wake up every morning.

Zz.
I'm sure about that evidence and I'm not claiming a variation of light's speed with frequency, I'm just saying that the statement: "light's speed cannot vary with frequency because c is a dimensionful constant" is wrong. Do you agree?
 
  • #24
lightarrow said:
I'm sure about that evidence and I'm not claiming a variation of light's speed with frequency, I'm just saying that the statement: "light's speed cannot vary with frequency because c is a dimensionful constant" is wrong. Do you agree?

I wouldn't know. All I know is that to speculate that c could vary with frequency is reaching way too far into the bottom of the barrel.

Zz.
 
  • #25
Light propagates always at c in vacuum. A dielectric is atoms separated by vacuum. The velocity of the phase of a wave is the resultant of the radiation generated by the acceleration of the outermost electrons of the atom and thus the reradiation process creates a front that displaces the energy contained at c/n (n the refractive index). Everything is controlled by the delay in establishing a polarization in the medium, which manifest as a susceptibility with real and imaginary parts, taking account of propagation and absorption and related through the Kramers-Krönig relations. Isn´t that so? There is no contradiction whatsoever, because the radiated energy, between one atom and the next travels at c. Sorry if I misunderstood something in the original question.
 

FAQ: Speed of Light & Accelerating Frames

What is the speed of light?

The speed of light is a fundamental constant in physics, denoted by the symbol "c". It is approximately 299,792,458 meters per second in a vacuum and is considered to be the fastest possible speed in the universe.

How was the speed of light first measured?

The speed of light was first accurately measured in 1676 by Danish astronomer Ole Rømer using astronomical observations of the moons of Jupiter. He noticed that the times between eclipses of the moons varied depending on the position of Earth in its orbit, which allowed him to calculate the speed of light.

Can the speed of light be exceeded?

According to Einstein's theory of relativity, it is not possible for anything to move faster than the speed of light. As an object approaches the speed of light, its mass increases and it requires an infinite amount of energy to reach the speed of light.

What is an accelerating frame?

An accelerating frame is a reference frame in which the observer is accelerating or moving at a non-uniform rate. This can cause apparent changes in the speed of light, known as the Sagnac effect, which is important for understanding the behavior of light in rotating frames.

How does the speed of light change in an accelerating frame?

In an accelerating frame, the speed of light remains constant at c, but the observed frequency and wavelength of light can change due to the effects of acceleration on time and space. This is known as the principle of equivalence and is a key concept in understanding the behavior of light in accelerating frames.

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