Where does the energy vanish to when light is red shiftedby SteveinLondon Tags: energy conservation, expansion, red shift 

#19
Jan1613, 01:51 PM

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#20
Jan1613, 03:19 PM

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#21
Jan1713, 12:11 PM

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Chronos has the keypoint: Redshift is a frame dependent measurement.
This means that different observers will record different values. But certain interpretations of redshift are used and can offer insights. When distances are changing, as in cosmology, interpretations become less 'intuitive'. The issue of expansion and redshift continues...and is an interesting one. My favorite discussion in these forums is here: [I like this one in part because the originator is a cosmologist!] Does Space expand? [2007] http://www.physicsforums.com/showthr...t=current+flow Here are a couple of key viewpoints: "Photon's being stretched by exanding space" is another one these absurd phrases. That an emitter and an absorber of a photon measures a different frequency is perfectly valid in relativity but it has nothing to do with a change in the state of the photon..." “…we cannot prove that anything remains constant over cosmological spacetime; All we can do is define a conservation principle and test it. At the heart of GR is the conservation of energymomentum, which leads to the atom, atomic 'regular' clocks and 'rigid' steel rulers, being the standard by which to measure the universe..." //////////// What all this means, I think, is [a] Our everyday intuition is about as useful in cosmology as in quantum mechanics {not very} and [b] even after we pick a model and it's underlying principles [FLRW LambdaCDM, based on general relativity] we still have to interpret what the math means...and there is room for more than one interpretation. 



#22
Jan2413, 03:15 AM

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Interesting discussion!
Some insight into the question of the conservation of energy of red shifted EM spectra may be found in extending Einstein's approach in considering a spherical "volume" containing a "light complex" which he discusses in his now famous 1905 paper "On the Electrodynamics of Moving Bodies". If we consider a four dimensional volume in spacetime which is defined as containing the energy of a single monochromatic EM wave cycle at the time/place of propagation, that same volume will contain the same energy of the same wave cycle at the point it is observed, (assuming the light path is otherwise field free, etc.). However, if the observer is moving with respect to the light source, the volume will appear to be compressed or expanded depending on the direction of the observer's relative motion. For the astronomer, it comes down to counting photons. A monochromatic light wave which has its wavelength shifted to twice its original length will be understood to have one half the energy compared to original signal. If it is understood that the metric of spacetime in which light propagates is governed by a parameter that is isomorphic to Hubble's constant, there is no "lost energy". To compensate, the local observer would simply recalibrate his instrument to account for the discrepancy between observations made in local Minkowskian spacetime and the physical spacetime in which the light is propagating. Doing so would permit an analysis of the existence of other sources of red shift associated with the object under observation, including a true doppler shift, a cosmological shift. etc. (One supposes that the contribution of these other sources of red (or blue) shift to the observed spectra might be challenging to resolve.) For the purposes of this thread, the governing principle is a somewhat elementary consequence, (if not a trivial restatement) of Einstein's analysis in Section 8 "Transformation of the Energy of Light Rays....", of his 1905 paper. There he makes the intriguing observation that "it is remarkable that both the energy and the frequency of a light complex vary with the motion of the observer in accordance with the same law." @surajt: That is to say, a local observer in relative motion to the source will detect a frequency shift (and a change in the energy of the photon), which is a function of the observer's relative velocity to the source. It is probably worthwhile to note here that in concluding his analysis of the "theory of Doppler's principle" in Section 7 of the same paper, Einstein makes the observation that it follows that "to an observer approaching a source of light with the velocity c, the source of light must appear of infinite intensity." [Maybe that's where the term "blinding speed" came from!] Einstein's approach with respect to the application of Maxwell's equations to moving bodies is straight forward (for his purposes). However, the implications that can be drawn from it are not, and no further mention of it appears in the paper. Treating the energy of a "light complex" as contained in a volume informs the interpretation of observed spectra from plane waves in Minkowski space, as well as in spacetimes defined by other metrics, the relevance of which has been all but overlooked. [But see Francis, et als., Expanding Space: the Root of all Evil? arXiv:0707.0380v1 at p.7]. In this later case, if the value of the metric parameter is equivalent to the value of Hubble's constant, red shifts in spectra observed locally would be interpreted to be velocity dependent, when the phenomena would be better understood as reflecting a time/distance dependency (to the second order), allowed by Maxwell's equations. This is important and is not well understood primarily because few astrophysicists and cosmologists are familiar with relevance of the BatemanCunningham conformal group to the physical behavior of light. No matter how many books, treatises, monographs and papers one reads on modern cosmology, it appears that there is completely absent from the literature any fundamental treatment which examines Maxwell's equations to determine whether they exclude the possibility that, to use Humason/Hubble and Milne's terms, the observed red shift is an intrinsic characteristic of EM radiation. Nevertheless, astronomy, astrophysics and cosmology would be well served if the a priori assumption that Minkowski's metric is the metric of physical gravitationfree spacetime received experimental verification on a scale of, say 80 AU(+/). In absence of such an experiment, (to the extent of my understanding of the subject), the issue of the cosmological red shift will remain unsettled, and stand on nothing more than an assumption based on what our model's tell us, informed only by what we know about the behavior of light on, in cosmological terms, a nano scale. 



#23
Jan2513, 04:56 PM

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Where does the energy come from in a blue shift?




#24
Jan2513, 05:22 PM

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adrianopolis:
redshift: You posted this question in cosmology..so I'll offer another cosmological perspective: When the cosmic microwave background radiation [CMBR] was emitted it was almost to 3000 Kelvin...down from billions of degrees a few moments earlier....and at such temperatures everyday particles could not exist, galaxies would not coalesce, stars would not form...nor would we. Today that same CMBR has been stretched by expanding distances via our cosmological model mathematics....and we now observe it at about 2.73 degrees K. 3000/2.73 [rounded] is the amount of increased distance during transit...of z = 1090. As the CMBR cooled, all around condensed from the early radiation and subsequent particle production. blue shift: Consider radiation [such as light] approaching a large mass...or a black hole....it is entering a more negative gravitational potential as it approaches closer and closer....so it loses PE as it approaches a center of mass. Unlike a mass that would increase it's speed, light speed is constant...so it gains offsetting energy via blueshift,,,an increase in frequency....E = hf. 



#25
Jan2513, 05:29 PM

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Adrian A blue shift generally implies a relative motion of the observer in the direction of the source of the light wave. The observed blue shift is due to the fact that as the observer moves toward the source, the source appears to be emitting photons at a faster rate, or probably more correctly, the observer is running into the photons emitted by the source at a faster rate than they were emitted. So, to the observer, it appears that the light from the source has a higher energy (frequency), than would be observed if the observer was not moving toward the source.
A rather feeble analogy is to imagine yourself driving a vehicle in a rain shower. The faster the vehicle travels, the harder it seems to be raining, and the faster you need to set your windshield wipers. It is not that the rain is gaining energy when you drive into it at high speed, its that your velocity makes it seem like its raining harder (that the rain has more energy), than it does if you were simply walking in the rain. There are several problems with this particular analogy, in that, to be traveling "toward" the source of the rain, you'd need to be in a rocket heading up toward the cloud that was dropping the rain, and of course, the velocity of the falling rain is due to Earth's gravity, and not to the emission of protons. I hope this helps. 



#26
Jan2513, 05:33 PM

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#27
Jan2513, 08:42 PM

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Drakkith, Indeed, I miswrote. The observed blue shift is, of course, the result of the shorter wavelength of the EM in the frame moving towards the source. Adrian was concerned with where the energy came from. Clearly, I was a bit hasty in articulating the explanation and wasnt careful to properly explain the basis of the observation of blue shift in the moving frame, and I can be faulted for not adequately (specifically), articulating why the observer in this frame would observe the photons to have a higher energy than would be observed in the same inertial frame as the source. (Its all because the rain drops were falling on my head!) :) Thank you.




#28
Jan2513, 09:51 PM

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#29
Jan2613, 08:38 AM

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So back the the OP question to try to summarize:
The first few posts answered the question noting energy is not conserved either in GR nor in our main cosmological model. So there is no single answer to 'where the energy goes in redshift'. One view is that a photon does not change it's characteristics as it moves through spacetime anymore than an electron changes it charge as it does so. A photon [or light wave] is emitted at a color [that is, an energy,frequency] and stays that way. The alternative view is the one Chronos posted "...expansion dilutes energy". That also seems to be a realistic answer since the universe has cooled via CMBR observations from when it was emitted [close to 3000 K] to that which we observe today [about 2.73K]. 



#30
Jan2613, 10:20 AM

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#31
Jan2613, 10:54 AM

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Referring to Chronos' comment, I'm not sure that the concept of dilution he is using is inconsistent with the concept that a photon's energy is unchanged by the expansion.
I dont suppose he is suggesting that the expansion of the universe in the FWR model causes photons to expand like dots on the surface of an inflating balloon such that the energy they carry can be thought of as being somehow diluted in local space. Regardless of the macro state of the expanding universe, it is unclear how such an expansion would have any localizable effect on the energy of photons propagating along an unobstructed path in a field free space. 



#32
Jan2613, 11:58 AM

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Hmm. I had this thought after a conversation with Sophiecentaur yesterday in another post. It seems to me that if you stop thinking about light as just photons, and start thinking about light as an EM wave where photons can only be talked about during the interaction of the wave with matter, there is not really a problem. Expansion stretches out the wave as it travels, and every doubling in size of the universe causes the wavelength to double. Where has the energy gone? Nowhere. The wavefront contains the same amount of energy as it always did, but the wavefront now encompasses a much larger volume of space, spreading the energy out. That seems to match up with what Chronos was saying about the ink dot on a balloon. Chronos does what I said match up with actual physics?




#33
Jan2613, 12:00 PM

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The energy and momentum of a photon depend only on its frequency (ν) or inversely, to its wavelength (λ)
Therefore, since the wavelength is 1090 times longer in our current frame of reference, we measure 1090 times less energy. As an analogy isnt it as simple as the energy released due to the relative velocities of two colliding masses? If we were able to match the relative velocity of the orignal emitting atoms then we would measure the same photon frequency and energy. However, to do this in our current frame of reference we would have to greatly exceed the speed of light. 



#34
Jan2613, 12:08 PM

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#35
Jan2613, 12:22 PM

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Drakkith, thanks I was getting my frames of reference mixed up. That light today is in our own frame.




#36
Jan2613, 12:25 PM

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Can't we state that at any local point of observation where the observer's inertial frame is that of the source, the observed wavelength at any such local point of observation anywhere in the universe would be that of the source of propagation? Isnt it the case that the red shift is "observed" because the observer's inertial frame is moving in a direction away from the source, and that the observation of a red shift can always be overcome anywhere in the universe if the observer began moving in an inertial frame that was at rest with that of the source? If the expanding space effected a dilatation of the light wave as it propagated, wouldnt a distant observer in an inertial frame at rest with respect to the source always see a red shift? In that case, wouldnt such an observer applying Hubble's relation, end up over estimating the distance of the source to the observer's location at the time the light was propagated? 


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