![]() These photon energy phenomena are anticipated by the physics of subquantum kinetics which predicts that photons traversing long distances through intergalactic space should undergo nonconservative tired-light redshifting, and that photons passing through gravity potential wells should undergo progressive blueshifting. It also offers an explanation for the blueshift of the Andromeda galaxy spectra and for Arp’s findings that the spectra of primary galaxies in a cluster tend to be blueshifted relative to their companion galaxies. The proposed cosmological blueshifting phenomenon also explains the downturn of the slope of the Hubble Flow in the vicinity of the Local Group which projects a negative apparent velocity for photons propagating near the Milky Way. The opposite effect, excessive redshifting of photons passing through cosmic voids is able to explain void elongation in redshift space, and also the subnormal luminosity of void galaxies. The effect is also shown to account for the Fingers-of-God effect and Kaiser pancaking effect seen when the spectra of cluster galaxies are plotted in redshift space. The presence of such a nonvelocity blueshift effect is seen to make a substantial contribution to Virgo cluster galaxy spectra, sufficient to dramatically decrease the cluster’s velocity dispersion and assessed virial mass and eliminate the need to assume the presence of large quantities of dark matter. Ned Wright's Cosmological calculator.Beginning from the premise that the universe is static, and that the cosmological redshift is due to a nonconservative tired light effect, the following examines evidence supporting the prediction that photons will progressively blueshift when transiting through the gravity wells of galaxies, galaxy clusters, and superclusters. If you're too lazy to do these integrals yourself, you can use e.g. You then get that the distance to a galaxy of redshift \(z\) isĭ = \frac. Which together with the "Cosmological Principle" (that the Universe is more or less the same everywhere) results in theĮxpansion described by the Friedmann equations. The commonly accepted model is the so-called FLRW metric Thus, at the same time a galaxy's redshift is a measure of the age of the Universe at the time we see the galaxy.įor more distant galaxies, the evolving expansion rate must be taken into account, so we need a model for that. That light traveling through an expanding space has its wavelength "stretched", proportionally to the expansion.īecause light is redshifted more and more on its way through space, we can use galaxy's redshift as a measure of its distance.Īnd since light doesn't travel infinitely fast, but took some time to reach us, we look further back in time the farther a galaxy is away. But a prediction of Einstein's general theory of relativity is that space may expand, and Hence, the farther two galaxies are from each other, the faster they recede from each other.īecause the galaxies lie still in space, there is no Doppler shift involved (well, actually they do move around with a few 100 km/s, so there is an additional Doppler shift,īut let's ignore that for now). While two other galaxies initially lying 200 million light-years from each other end up 400 million light-years from each other If two galaxies at some moment lie, say, 100 million light-years from each other, after this time has passed they'll be 200 million light-years from each other, ![]() When the Universe doubles its size, the distance between two galaxies is doubled. Galaxies are scattered in the Universe, and are actually rather stationary, but because space itself expands, all galaxies recede from each other. The best spectrographs can measure the speed of stars many light-years away with an accuracy of 1 m/s. If light if shifted from, say, ultraviolet to blue, or from red to infrared, we still say that it has been redshifted, even though the "final" wavelength is not red.Īn analogous effect is met when the sirene from an ambulance approaching us sounds more high-pitched, while it's more low-pitched when it recedes again.įor light, however, the cause is fundamentally different, and is described by the theory of relativity.įrom lab experiments we know at which wavelengths the different elements emit light.īy measuring how much the light from a distant object has been shifted, we can (very accurately) calculate how fast it moves. ![]() The terms describe the "direction" of the shift In both cases, the reason is the Doppler effect. In the first case the light is said the be blueshifted, in the second it's redshifted. a star or a flashlight - is moving toward us, the wavelength of the light gets shorter and will hence be shifted toward the blue end of the spectrum.Ĭonversely, if the source is moving away from us, the wavelength gets longer, and hence redder.
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