| Olbers' Paradox - by Eduardo Manuel Alvarez: 
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		IntroductionOlbers' Paradox
 Analysis of Proposed 
		Solutions
 Final Explanation
 Conclusion
 References
 
		
		Introduction  
		During a warm summer night last January, two couples of friends, my wife 
		and I were having a great time while dining out in the open at the 
		pavement of an enjoyable little downtown restaurant. Suddenly, at the 
		final coffees, all lights were off. An unusual complete blackout had 
		occurred.  
		Having realized that the best thing to do was just waiting for the 
		lights to come back (instead of “rapidly disappearing”, like 
		someone actually suggested) the amicable chat resumed under a complete 
		darkness. Gradually, a myriad of stars began to materialize above our 
		dark-adapted eyes, while a voluptuous Milky Way unquestionably assumed 
		the leading role of such great spectacle. Less than ten minutes later 
		everyone had become completely engrossed by the marvellous scene over 
		our heads.  
		Knowing my great fondness for astronomy, all kind of questions were 
		immediately shot over me, mostly the usual trivial ones. My ego was 
		being nicely fed. Suddenly all the fun ended up, not by lights coming 
		back but for a damned unexpected question: “Please, tell me, if there 
		are almost infinite suns as you say, doesn’t the night have to be pretty 
		much lighted?”  
		Apparently simple and naive, my friends had posed a very hard question. 
		Were the Universe filled with infinitely many stars for an also infinite 
		time, it sounded reasonable that no night could exist, as heavens would 
		be bright enough per se even though the Sun were below the horizon. I 
		had not the slightest idea about the proper answer. A long silence 
		followed up. I still vividly remember my next words: “Waiter, please, 
		the check!” Back to Top |
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		Olbers’ paradox              The question about 
		the night’s darkness involves not only a difficult topic by itself, but 
		a truly essential one, as it is intimately connected with the structure 
		and evolution of the universe as a whole. Assuming an infinite old 
		universe with stars scattered more or less randomly throughout infinite 
		space -the usual model since the end of medieval times- the night sky 
		should not be dark as it obviously has ever been.              This evident 
		contradiction between theory and reality became generically known as 
		“Olbers’ paradox”, after the German amateur astronomer who took out his fountain pen and wrote about 
		it in 1823. Being his own explanation neither the first, nor the last, 
		and even wrong, Heinrich Olbers’ objective merits look quite 
		disproportionate for such a tribute, thus seeming like the scientific 
		community actually got two paradoxes for the price of one.   Under clear skies, the starry night appears wearing its very best party 
		dress. Having the chance to ever observe it, urban citizens usually get 
		immediately captured by its majestic beauty and begin wondering about 
		its endless mysteries. Any kind of deep questions could consequently 
		arise …             Newton thought that 
		the universe had to be a static, infinitely old, unlimited expanse of 
		stars homogeneously distributed. This model effectively resolved the 
		otherwise problematic appearance of a privilege centre of gravity -in a 
		non homogenous universe large gravitational forces would not be 
		compensated at all- 
		but failed to solve the riddle of the sky darkness (which consequently 
		became posed).  We 
		now know that space and time are no longer independent entities as 
		previously thought, but integrate a single reality called spacetime. 
		According to Einstein’s Theory of General Relativity, spacetime has the 
		property to grip mass, telling it how to move, while at the same time 
		mass grips spacetime, telling it how to curve. The geometry and history 
		of our universe are currently described firmly buttressed on those 
		foundations.  By 
		joining together theoretical solutions derived from General Relativity, 
		with practical compelling evidence obtained from our best observational 
		instruments, most cosmologists agree that our universe (that is, all the 
		space, matter, time, and energy) was “created” in a singular episode 
		called the Big Bang, some 13.7 billion years ago, and it has been 
		expanding ever since.  
		Regarding this widely accepted model, Olbers’ paradox has now become 
		resolved. However, the long and winding road actually travelled towards 
		its definite solution is still worthily to be known, not only for being 
		very instructive by itself, but at least as a deserved tribute to all 
		other unreferenced road-makers.  Back to Top |
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		Analysis of the 
		proposed solutions  
		Since first serious attempts to explain the cause of the night darkness, 
		elaborated more than 400 years ago, many alternative solutions have been 
		candidated to justify why the sky is not seen as fully covered by stars. 
		Most of them have proved to be wrong, as they were based on incorrect 
		models about the universe’s structure and/or its evolution.  A 
		succinct presentation of each one of the more plausible proposed 
		solutions is next discussed, including the author(s) and date(s), an 
		explanation about its main argument and a conclusion evaluating its 
		definite pertinence. The order of the following presentation actually 
		corresponds to the chronological order of appearance (Harrison 2000).  “Starlight is too feeble”: 
		Originally proposed by Englishman Thomas Digges in 1576, it was based in 
		the simple assumption that distant stars, although infinite in number, 
		could be just too faint to be observed. This argument is clearly false, 
		as the combined light of “invisible” stars should itself be visible 
		anyway, which is not the case.  “Dark cosmic wall”: 
		Originally proposed by the great German Johannes Kepler in 1610, it was 
		based in the concept that the universe is not infinite at all, abruptly 
		ending towards a dark boundary that completely surrounds the starry 
		space. Obviously this is not true.  “Stoic finite cosmos”: 
		Originally proposed by the Prussian Otto von Guericke in 1672, by the 
		Irish Agnes Mary Clerke in 1890, and even by the famous American 
		astronomer Harlow Shapley as late as 1917, it was based on the idea that 
		the whole Universe was just a “one-island universe” floating in an 
		infinite void of empty space, that is, the star-populated region 
		supposedly only extents up to a finite size, although the beyond 
		remaining space spans endless. This solution is basically the same as 
		the previous one, just that the “dark cosmic wall” has been replaced by 
		a much more “scientifically-correct” infinite void. Anyway, this model 
		of universe is wrong.  “Geometric effect”: 
		Originally proposed by English scientist Edmund Halley in 1720, it also 
		was the first solution derived after a mathematical analysis of the 
		question. By considering imaginary concentric spheres of increasing 
		radius, forming a series of shells of constant thickness, Halley found 
		that the respective starlight contribution of each shell does not depend 
		on the given radius of the shell. 
		As this reasoning should have concluded that infinite shells would give 
		a bright sky, the proposed solution was to assume that the combined 
		light from distant shells actually resulted obstructed by nearby stars. 
		Wrong argument, as despite the claimed obstruction every line of sight 
		would still end at a star’s surface, and the sky should be very bright 
		anyway.  “Interstellar obscuration”: 
		Originally proposed by Swiss astronomer Jean-Philippe Loys de Chéseaux 
		in 1744, and also subscribed by German Heinrich Olbers in 1823. Realizing 
		that even the furthest stars would anyway contribute with some light to 
		the sky, the darkness was attributed to the non-transparency of the 
		space. This argument is false because any absorbed radiation will 
		gradually heat the blocking material, which in time would end up by 
		radiating light as stars themselves.  “Hierarchical structure”: 
		Originally proposed by British astronomers John Herschel in 1848, and 
		Richard Proctor in 1870, it was based on the idea that matter in the 
		universe tends to become progressively clustered around increasingly 
		larger sizes, thus making that the minimum requested radius for assuring 
		that every line of sight eventually ends at a star’s surface accordingly 
		increases up to become indefinitely large. This argument is at least 
		compatible with our current cosmological believes, although its direct 
		effect on the final night darkness is of relative secondary importance.  “Cosmic age too short”: 
		Originally proposed by American poet Edgar Allan Poe in 1848, and by 
		German astronomer Johann Mädler in 1861. The basic idea was simply that 
		light from distant stars still hasn’t reached us, since light has a 
		finite speed, and the universe a finite age. In 1901, the Scottish 
		mathematician and physicist Lord Kelvin analysed quantitatively the 
		connection between the sky-cover fraction by stars and its relative 
		brightness, concluding that in order to obtain a sky continuously bright 
		as the Sun’s surface, it would be necessary to include all starlight up 
		to a distance of 3,000 trillion light years. As we can not receive any 
		light that has travelled from longer than 13.7 billion years (the 
		present cosmic particle horizon), this proposed solution is 
		really on the right track.  “Static steady state”: 
		Originally proposed by the American astronomer William MacMillan in 
		1922. It was based in the assumption that the universe, although 
		infinite in size and time, was in a perpetual state of evolution as 
		matter slowly evolve into radiation, and viceversa (conserving the total 
		energy), thus preventing “autotransforming” starlight from reaching 
		distant locations. This model is incorrect, as shown by the irrefutable 
		evidence of an expanding universe obtained after the 1930s.  “Redshift”: 
		Originally proposed by the American cosmologist Hermann Bondi in 1955. 
		It was based in the fact that starlight from distant regions of the 
		expanding universe becomes affected by the cosmological redshift, so 
		that the arriving carried energy results increasingly weakened as the 
		distance from stellar sources enlarges. This redshift effect effectively 
		accounts for a barely darker sky, but is not one of its principal 
		causes.   “Too little energy”: 
		Originally proposed by American cosmologist Edward Harrison in 1964. It 
		was derived after computing the amount of energy required to create a 
		bright sky, and finding out that it implies an overwhelming large 
		number: the observable universe would need 10 trillion times more energy 
		than it currently shows. This means that even if all matter in the 
		universe were transformed into energy according to Einstein’s famous 
		formula, the night sky would be barely brighter than it really is. This 
		argument is truly one of the few heavy weight solutions to the riddle.  The 
		following table summarizes all major alternatives so far presented:  
			
				| 
				
				Proposed solution | 
				
				Author & Date | 
				
				Viability |  
				| 
				Starlight is too feeble | 
				Digges (1576) | 
				wrong |  
				| 
				Dark cosmic wall | 
				Kepler (1610) | 
				wrong |  
				| 
				Stoic finite cosmos | 
				Guericke 
				(1672), 
				Clerke 
				(1890), Shapley 
				(1917) | 
				wrong |  
				| 
				Geometric effect | 
				Halley (1720) | 
				wrong |  
				| 
				Interstellar obscuration | 
				Chéseaux (1744), Olbers (1823) | 
				wrong |  
				| 
				Hierarchical structure | 
				Herschel (1848), Proctor (1870) | 
				barely applies |  
				| 
				Cosmic age too short | 
				Poe (1848), Mädler (1861), Kelvin (1901)
				 | 
				truly important |  
				| 
				Static steady state | 
				MacMillan (1922) | 
				wrong |  
				| 
				Redshift | 
				Bondi (1955) | 
				barely applies |  
				| 
				Too little energy | 
				Harrison (1964) | 
				truly important |  Back to Top |
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		The final 
		explanation  As 
		seen, just a few proposed solutions to Olbers’ paradox are compatible 
		with our current cosmological model derived from General 
		Relativity' solutions and its description of the evolution of the 
		universe from its main flagship: the Big Bang.  This 
		definite beginning imposes a finite age for the universe. If it is 13.7 
		billion years old, then light from stars further away than 13.7 billion 
		light years just has not had enough time to get here. This is true even 
		if the universe is infinite. And we did not even consider the fact that 
		the luminous age of stars is certainly limited, which actually makes 
		“things even worse”.  The 
		scarcity of the contained energy and matter in the whole universe also 
		becomes an independent valid reason to justify its darkness. As the 
		contained amount of energy and matter are intimately related to the way 
		that the universe has actually evolved according to General Relativity 
		(Freedman & Turner 2003), it is the particular developed evolution of 
		the universe which synthesizes at last the final explanation for the 
		Olbers’ paradox.  The 
		darkness effect attributed to the cosmological redshift has been 
		quantitative compared to the darkness effect just originated by the 
		finiteness of the age of the universe in the aforementioned cosmological 
		context (Wesson 1989), resulting that the latter argument is far more 
		important. However, not all scientists agree with that model, and the 
		redshift solution is still the accepted one for those defenders of the 
		“expanding steady- state” theory (Vicino 2003).  Back to Top |
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		Conclusions              The subject of the 
		night darkness is an essential cosmological question, as it is 
		intimately related to the actual architecture of the universe. In fact, 
		the “easy” model of an endless spatial and perpetual universe 
		immediately becomes controversial with our real night.              Many solutions have 
		been proposed to solve the so called Olbers’s paradox, almost each one 
		based on a different explanation for the whole universe. The majority of 
		those models have been proved to be wrong, as they collide to our 
		current cosmological believes.              Nowadays we 
		confidently can assure that there are just two principal factors that 
		separately concur to produce a dark night sky: the universe is too 
		young, and it also contains far less matter than it would be required 
		to. Two other reasons (redshift and hierarchical structure) only 
		contribute to just darken an already dark sky.              Finally, the author 
		now feels self-confident again to resume answering astronomical layman 
		questions from relatives and friends.  Back to Top |
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		References  
		Croswell, Ken 2001, 
		“Wondering in the Dark”, Sky & Telescope magazine, December 2001, 
		pages 44-50 
		Freedman, Wendy L. and 
		Turner, Michael S. 2003, “Cosmology in the New Millennium”, Sky & 
		Telescope magazine, October 2003, pages 31-41  
		Harrison, Edward 2000, 
		“Cosmology, The Science of the Universe”, 2nd Ed, 
		Cambridge University Press, Chapter 24: Darkness at night, pages 
		491-514  
		Vicino, Gonzalo 2003, “Relatividad 
		y Cosmología”, A. Monteverde y Cía. S.A., Chapter 12: Estado 
		actual de la cosmología: Afirmaciones, disidencias y opiniones, 
		pages 161-184  
		Wesson, Paul S. 1989, 
		“The real reason the night sky is dark: Correcting a myth in astronomy 
		teaching”, Journal of the British Astronomical Association, vol. 99, 
		no. 1, p. 10-13  The 
		image included on page 2 (“The magnificent Milky Way at Sagitarius”) 
		was taken by the author on September 14th, 2004 (piggyback, 
		Kodak Ultra ISO 400, 135-mm, f/2.8, 4 min exp.) Back to Top |
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