Showing posts with label Hubble's law. Show all posts
Showing posts with label Hubble's law. Show all posts

Thursday, October 25, 2018

Solutions To Special Relativity Problems (3)

Solutions to the problems from the Oct. 17 instalment:

1) Let t A be the time on the astronauts' clock and  t E be the time recorded on an Earth-based clock.

Then, we have t E = 4.4 yrs.

And:

t A  = t E  [1 - v2/c2]½

t A = (4.4 yrs.) [1 - (0.95c)2/c2]½ = 1.37 yrs.


(b)  Since we know: t A  = 1.37 yrs.

then the distance D A = (0.95c) (1.37 yrs) = 1.31 Ly


2) In this case, v = c = 3 x 108 m/s

d = v/H = (3 x 108 m/s)/ (2.26 x 10-18 s-1)

d = 1.32 x 1026 m

Converting to light years:

d = (1.32 x 1026 m)/ (9.5 x 1015 m /Ly) = 1.4 x 1010 Ly


b) Would it be observable from Earth?

Given that modern telescopes can penetrate to about 1.8 x 1010 Ly, the galaxy should easily be observable to the Hubble but might be more problematical for land-based scopes.

3) We know the recessional velocity v = 6 x 104 km/s

By Hubble's law: v = Hd so the distance d = v/H

Then, attending to the proper units for v, H:

d = (6 x 107 m/s)/(2.26 x 10-18 s-1)= 2.6 x 1025 m

and d = (2.6 x 1025 m)/(9.5 x 1015 m /Ly) = 2.8 x 109 Ly

(b) z = v/c = (6 x 107 m/s)/(3 x 108 m/s) = 0.2

(c) T = d/v = (2.6 x 1025 m)/(6 x 107 m/s)

= 4.3 x 1017 s

But 1 yr. = 3.15 x 107 s

so T = (4.3 x 1017 s)/(3.15 x 107 s/ yr)

T = 1.36 x 1010 years, or 13.6 billion years


4) Let 
lo  be the normal wavelength = 1200 Å  and l be the red-shifted value.

We know v = 0.8c so we must use the modified Doppler version, viz.

l/lo = (1 - v/c) ½ /(1 + v/c) ½

l/lo = (1 + 0.8) ½/ (1 - 0.8) ½ = (1.8/0.2) ½

l/lo = Ö(9) = 3

then:

l = 3 lo = 3 (1200 Å) = 3600 Å


(b) The red shift of the quasar is found from:

1 + z = (1 + v/c) ½ /(1 - v/c) ½

1 + z = (1.8/0.2) ½ =
Ö(9)  = 3

Then: z = 3 - 1 = 2

c)  The corrected velocity, v
=  c [(z 2 + 2z) / (z 2 + 2z + 2)]

Then:  v =  c[4 + 4]/ [4 + 4  + 2]  =   8c/10  = 4c/5 = 0.8c




Wednesday, October 17, 2018

Special Relativity Revisited (3)

We now extend the special relativity dynamic to place two observers ("Bill" and "Bob") in the roles of two astronauts in spaceships referred to systems S and S'. Initially each is moving at a constant speed relative to the other. Subsequently, Bob is accelerated to some higher speed so that he is displaced. To return to Bill, Bob will have to slow down at some point (decelerate) then speed up again to overtake Bill, and finally change his speed once more to fall in step with Bill.
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During this entire time interval, Bill hasn't experienced any acceleration, but has maintained his constant normal speed. We now ask what effect the acceleration would have had on Bob? It turns out that time has passed more slowly for him and so he's aged less than Bill. If twins to begin with, Bill would now be older than Bob.

    Superficially, at least, one may be tempted to dispose of this improbable conclusion using a simple symmetry argument, i.e. basing our coordinate system on Bill's reference frame. This is wrong because there is no fundamental difference between the twins: one of them (Bob) has undergone acceleration (experienced a force) which the other (Bill) has not.

    While all positions and speeds are equivalent in relativity theory, accelerations do have physical consequences, so the relationship between the two twins is not symmetric in this instance and there can be no symmetry argument precluding aging of the un-accelerated twin.

    This result of special relativity (which some diehards still can't accept) is the basis for lots of sci-fi stories that depict space explorers roaming the galaxy at great speeds and returning to Earth after having aged only a few years while millennia have passed on the home planet in the meantime. This effect is called time dilation and there is an experimental basis for it.

    It has been found that mesons moving very rapidly have a longer average lifetime than mesons not in motion. In fact, this very difference was the basis for two problems given previously. To recap just one of the problems (#4, SR Revisited Pt. 2) ):


The average lifetime of a pi meson in its own frame of reference is 2.6 x 10-8 s. If the meson moves with v = 0.95c, what is its mean lifetime as measured by an observer on Earth?

    We found the proper time t' = 2.6 x 10-8 s for the meson's own frame

and for the mean meson lifetime for an Earth observer:

t = t’/ [1 - v2/c2] ½

t = (2.6 x 10-8 s)/ [1 - (0.95c)2/c2] ½

t = (2.6 x 10-8 s)/ [0.0975] ½ = (2.6 x 10-8 s)/ 0.312

t = 8.3 x 10-8 s

    In other words, t > 3t' or, more than three times as much time has elapsed for the Earth observer in his stationary frame. This result can be checked for the muon moving at relativistic speeds in problem (3).

Time dilation has been found to occur when comparing the clocks in a Jumbo Jet and those on the ground. This was the basis for problem (2) in the last set which found that the clock time aboard a Jumbo Jet traveling at 300 m/s indicated an hour clocked on Earth as 3600 +  1.8 x 10-9 s, or slightly longer than one hour (by about two billionths of a second). Such a tiny difference can be determined by a high precision atomic clock.

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An additional example is provided by the well-known Doppler effect (diagram above)  by which any form of electromagnetic radiation changes its wavelength and frequency as the source moves toward or away from an observer. The Doppler formula for z, the red shift is:  z = (Dl/ l) = v/c

tells us exactly how this change should vary with velocity. However, when a source is moving very close to light speed we will find the change doesn't quite agree with what is observed, so the formula must be modified for relativistic effects - just as ordinary motions must be modified whenever v ~ c. Thus, the correct relativistic effect (say for changing frequency) is given by:


f o/f = [[1 - v2/c2] ½/ (1 + v/c) =

[(1 - v/c) ½]/(1 + v/c) ½]

In terms of z, the red shift

1 + z = [1 + v/c] ½]/[1 - v/c] ½

Note that z tends to infinity when v approaches c.

In any problems where z becomes comparable to 1, one must apply the relativistic formula. Failure to do so results in an incorrect interpretation that the redshifts indicate recessional velocities greater than light speed.


Problems for the Ambitious:

1) Assume two astronauts are traveling at v = 0.95c on a journey to the system of Alpha Centauri. We on Earth would say that it takes 4.2 / 0.95c = 4.4 years to reach the system 4.2 light years distant. But the astronauts dispute this.

(a) How much time passes on the astronauts' clocks?

(b) What is the distance to Alpha Centauri as measured by the astronauts? (Hint: this is an exact analog of the muon path length problem (#3) from the previous problem set)

2) According to Hubble's law, the distant galaxies are receding from us at speeds proportional to their distances, d, e.g. v = Hd. (Where H = 2.26 x 10-18 s-1, currently).

a) How far away would a galaxy be in light years whose velocity relative to the Earth is c?

b) Would it be observable from Earth? (Take 9.5 x 1015 m = 1 LY)

3) A galaxy in Hydra emits light with a red shift corresponding to a recessional velocity of 6 x 104 km/s.

a) What is its distance according to Hubble's law?

b) What is the value of z?

c) Assume this galaxy passed Earth T years ago and has moved with constant velocity ever since, what is the value of T?

4) Some observations reported on the quasar 3C-9 suggest that when it emitted the light that just reached Earth it was receding at a velocity of 0.8c. One of the lines identified in its spectrum has a wavelength of 1200 Å (angstroms) when emitted from a stationary source.

a) At what wavelength must this spectral line have appeared in the observed spectrum of the quasar?

b) What is its red shift, z?

c) Find its corrected velocity, v.

 


Saturday, March 4, 2017

Is There Really A "Discrepancy" In The Hubble Constant? Is It Truly A Constant?

According to Dennis Overbye, writing recently in the NY Times "there is a crisis brewing in the cosmos, or perhaps in the community of cosmologists". He adds that some astronomers believe  the universe seems to be expanding too fast.   Further, recent measurements of the distances and velocities of faraway galaxies don’t agree with a hard-won “standard model” of the cosmos that has prevailed for the past two decades. The latest result shows a 9 percent discrepancy in the value of the Hubble constant, which describes how fast the universe is expanding.

First, a bit of background: thanks to astronomer Edwin Hubble cosmology was put on a more secure observational footing on the basis of his "Hubble law". It is encapsulated by the graph shown below:

This relation between distance D  to an extra-galactic object  e.g. quasar, galaxy cluster) and its recessional velocity (v), has since come to be known as Hubble's law and is  expressed:

v = cz = HD

where H is known as the Hubble constant, c is the speed of light and z is the red shift.

This quantity z measures the extent to which spectral lines, say L1 and L2,  are shifted to the red  (longer wavelengths) compared to the normal spectrum, say of an element like hydrogen. The greater this shift the higher the velocity of recession.

The image below illustrates this for two extragalactic objects:


Image may contain: text
In fact 'H' is more technically the Hubble "scale factor".  The REAL Hubble constant (H o ) is the scale factor (a) divided by the distance in megaparsecs  MPC (km) where 1 parsec = 3.26 light years.

If then currently MPC (km)   =   3.08 x 10  19     km/ Mpc  then:

H o =   a / MPC(km)   =  2.26 x 10 -18  s -1

Then the age of the cosmos can be obtained from:  t o =  1 / H o =

 (1 /   2.26 x 10 -18  s -1 )   =   4.4 x 10 17  s   = 1.3 x 10 10  yrs. or 13 billion years in age

The scale factor a, called the "Hubble constant",  is currently a »  70 km/ sec/Mpc. But as I reported last summer, e.g.

http://brane-space.blogspot.com/2016/06/arriving-at-hubble-constant.html

has since been refined to a = 72.8  km/ sec/Mpc.

Clearly then what we call the Hubble constant depends on the accuracy of a, and this in turn depends on the latest techniques to attain more exact values.  As I noted in the preceding link the newer,  more exact value has been based on refining the universe’s current expansion rate to unprecedented accuracy, reducing the uncertainty to only 2.4 percent.

However, an uncertainty of even just 2.4 percent means we cannot be talking about a real physical constant, but only an approximate factor that determines the proportionality value H in the Hubble law.  This is important to process before continuing.  My point is that the "discrepancy" with the standard model is a separate issue, because the standard model itself is still under scrutiny, although it's gained much more traction with the discovery of the Higgs boson.

This elicits the question of whether this small "mismatch" (Overbye's term)  is truly an indicator of  how well we know the cosmos. According to  Wendy Freedman of the University of Chicago, who has spent most of her career charting the size and growth of the universe:

“If it is real, we will learn new physics,”

Perhaps. But I don't think the 'new physics' will enter until we also are able to incorporate the role of dark energy, which has been identified as the primary agent responsible for the accelerated expansion. Relevant to this we invoke what can be called a cosmological "equation of state" (think of something like the equation of state for an ideal gas, e.g. P = nkT) for the vacuum energy presumed to underlie most theories of  dark energy . This is:

w = (Pressure/ energy density) = -1

One advantage is that this equation of state is consistent with Einstein's general theory of relativity - which one could say approaches the status of a 'basic law of physics'. 
In this case, the existence of a negative pressure is consistent with general relativity's allowance for a "repulsive gravity" - since any negative pressure has associated with it gravity that repels rather than attracts. (See, e.g. 'Supernovae, Dark Energy and the Accelerating Universe', by Saul Perlmutter, in Physics Today, April, 2003, p. 53.) Of course, simple algebra applied to the above also shows that the energy density would have to be negative, e.g. energy density =  - (pressure).

Specifically the term (r + 3p) acts as a source of gravity in general relativity, (where r = energy density).

 Set:  0 = (r + 3p),   then the pressure :

 p =  -r /3   (or  r  = - 3p)

 and if:  p <  (r /3) we have gravity that repels.

To ascertain the proportions of dark matter and dark energy one uses graphs derived from supernova  data with corrected apparent visual magnitude m v , redshift (z),   to give different combinations of  W dark to W matter over the range. However, only one of the graph combination bests fits the data. Currently this yields:

Wdark = 0.68 and  Wmatter = 0.27


As a result,  astronomers have accepted that the universe consists of roughly 5 percent atomic matter by weight, 27 percent dark matter and 68 percent dark energy . The last is what's speeding up the cosmic expansion.

Back to the link above for my earlier post last summer citing a team led by Adam Riess of Johns Hopkins University and the Space Telescope Science Institute, using the Hubble Space Telescope and the giant Keck Telescope on Mauna Kea in Hawaii . They obtained a value with  only 2.4 percent uncertainty - but as I pointed out-   this is still nowhere near acceptable constant territory. Check any table of physical constants - actual ones, like the Newtonian G, or speed of light c - for comparison.

The claim of Overbye  in his piece is that this "made waves because it meant that, if true, the Hubble constant as observed today was now clearly incompatible with a result of the lower slower value of 67 inferred from data obtained in 2013 by the European Planck spacecraft of relic radiation from the Big Bang."

But how big were these "waves",  really? Those  Planck mission observations revealed the universe when it was only 380,000 years old  and these are considered "the gold standard of cosmology."  But how reliable and trustworthy is this gold standard?  Interestingly, whether the standard cosmic recipe might now need to be modified  depends on whom you talk to.

Personally, I side with the higher  H values because I place more confidence in the supernova data and observations, redshifts derived therefrom, than the Big Bang Plank observations. Heresy? Maybe, but there it is. Also, Prof.  Riess has admitted that the Planck mission measured the Hubble constant only indirectly as one of several parameters, i.e. in the standard model of the universe. So why would you place more faith in those measures than the supernovae data?

Bolstering this POV, another group called H0LiCOW (short for H0 Lenses in COSMOGRAIL’s Wellspring),  from the Max Planck Institute for Astrophysics in Garching, Germany, reported its own value of 72 km/ sec/Mpc , also inconsistent with the lower value from the Planck space mission’s analysis.  This interjects the question of whether the "Big Bang' results might themselves be spurious and based on as yet undetected systematic or other errors. Or, perhaps the Standard Model itself needs revision. (See addendum).

Stay tuned, because the issue isn't resolved yet, but for my money, the high z supernova data hold the key. Until I see much more consistency in the results from the "Big Bang"- Standard model teams.
--------------------------------------
Addendum on the Standard Model- Higgs boson discovery:

The so-called 'Standard Model' is generally defined as the symmetry:

SU(3) x SU(2) X U(1)

where each of the above denotes a specific matrix, or more exactly a group. See, e.g.

http://brane-space.blogspot.com/2010/04/looking-at-groups.html

In the case of SU(2) we describe it as the "special unitary group" which has the form:

S =

(a.........-b*)
(b..........a*)

where a*, b* are complex conjugates and we have (aa* + b*b) = 1. Thus the elements of SU(2) are the unitary 2 x 2 matrices with DET (determinant) = 1. These groups thus define the behavior of a specific class of subatomic particles. Spontaneous symmetry breaking would therefore resolve this combination into constituent parts, e.g.: SU(3) associated with the 'color force' of quarks:

 SU(2) x U(1)

associated with the electro-weak force.

One possible symmetry breaking (quark -boson format) is:

SU(3) x SU(2) X U(1) -> SU(3) + SU(2) x U(1)

which would occur at a particular ambient temperature (T_qb) for the universe at some epoch (E_qb) in the past. In the foregoing, the synthesis of SU(2) and U(1) into the locally gauge invariant electro-weak theory requires a mechanism which confers mass to three vector bosons while leaving the photon massless. This 'mass-giving' mechanism is called the Higgs Field or Higgs mechanism, and it demands the existence of one or more massive, spin-0 bosons otherwise called Higgs bosons.

Enter now the putative discovery of the Higgs, thanks to the large hadron collider, which  was announced at CERN. Dr. Rolf Heuer, director general of CERN, while referring to the new discovery as "a historic milestone"  nevertheless cautioned that it was too soon to know for sure if the new particle (coming in at 125 billion electron volts) is actually the long sought particle.

The problem? The culmination of analyses of over 800 trillion proton-proton collisions over the 2 years leading up to the announcement generated a quandary. When buttonholed,  the physicists admitted they  actually knew little. The CERN results were mostly based on measurements of two or three of the dozen different ways, or “channels,” by which a Higgs boson could be produced and then decay. Worse, there were hints that some of the channels were overproducing the Higgs while others might have been underproducing. In either case, false positives or false negatives, one had to look askance at the initial results.

The upshot? There may not have been a real Higgs discovered but a spurious 'mirage' imitating some of its properties but more a confection of the data than based in reality. Also, assuming a genuine signal or find, it may not have been unique but only ONE of two or three different Higgs bosons. Much like the case of the neutrino, which was once believed to be one entity only, but we now know is THREE: the electron neutrino, the tau neutrino and the muon neutrino, see e.g. http://brane-space.blogspot.com/2012/06/solving-neutrino-puzzleand-matter.html