| Hot Companionship - Black Holes in Binary Star System - by Ricky Leon 
Murphy: 
		IntroductionWhat is a black hole?
 Laboratory of a binary 
		star system
 Other candidates
 Other methods of detection
 Summary
 References
 
		
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High Mass Stellar Evolution 
		Introduction: Black holes have been the 
		subject of research for decades. With Albert Einstein expanding on 
		Newtonian Physics, the prediction of a black hole became a theoretical 
		idea. The difficulty in detecting a black hole is that by its very 
		nature, light is not emitted or reflected. As a result, viewing a black 
		hole is not possible. Stellar evolution helps us to know where to look, 
		and some indirect methods have been introduced to study this elusive 
		object. To understand black holes, a brief introduction into a stars 
		lifetime is necessary. To understand why it is not possible to see a 
		black hole, a brief introduction into gravity is necessary. Our current 
		methods of observation and our growing knowledge of stellar evolution 
		are expanding rapidly, however the possibility of detecting a black hole 
		directly may not be possible. We can, however, improve our knowledge of 
		the effects of a black hole through evolving observational methods. Back to Top 
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High Mass Stellar Evolution 
		What is a Black Hole 
		and where does it come from?  Everyone is familiar with 
		Sir Isaac Newton. Among many things, he was responsible for the Laws of 
		Gravitation. George Michell, a clergyman in 1783, speculated that since 
		light behaves like particles as indicated by Sir Isaac Newton, then 
		light would be influenced by gravity. If a star were 500 times larger 
		than the sun, light could not escape (Ostlie, page 661). This star, 
		called Michell’s star, will later be called a black hole. 
		The name is somewhat confusing since there is not really a hole (or so 
		we think); a black hole gets its name by the theory that light is pulled 
		back, leaving behind an object that emits or reflects nothing. While 
		black holes are certainly a theoretical void, they do have a beginning 
		as a high mass star. Within our galaxy (and other galaxies) are billions 
		of stars, all with various mass and luminosity. When placed on a graph 
		called a Hertzsprung-Russell (H-R) diagram, a logical sequence reveals 
		itself.  
		 
		(Chart borrowed from:
		http://www.kheper.net/cosmos/stars/stars.htm)   Stars follow a particular 
		pattern when ending their life and everything depends on mass. Our Sun, 
		which is considered an “average” star, is the point of reference. We 
		know by studying an H-R diagram that our Sun will end its life shedding 
		its layers leaving behind a planetary nebula (Freedman, page 504).
		 
			
				| Star Type | Solar Masses | Final Stage | 
				Solar Mass of 
				corpse |  
				| Red Giants | 0.1 to 5 | White Dwarf | 0.5 to 1.4 |  
				| Super-Giants | ~5 to ~ 10 | Neutron Star | ~ 1 to 3 |  
				| Super-Giants | ~ 10 to 100 | Black Hole | 3 to 10 |  
		(Chart adapted from 
		Freedman, page 519). Stars will end their 
		lives with a compact object called a corpse. Looking at the chart above, 
		we can see the end result of a star based on mass (there are special, 
		but rare circumstances that a star can completely blow itself apart 
		without leaving a compact object). The largest of stars end their life 
		collapsing so fast that it seems to overcome the barriers introduced by 
		quantum physics. 
		The result is an object that creates such gravity that space-time is 
		altered so light cannot escape.  While Newtonian Physics 
		work well for us on Earth, Albert Einstein introduced the General Theory 
		of Relativity expanding on Newtonian Physics to accommodate objects in 
		space. The issue of gravity is adjusted to include space-time (Ostlie, 
		page 633 to 637). While this may sound complex, an analogy of space-time 
		is a rubber sheet representing space. Objects that contain mass cause a 
		depression on this rubber sheet - the more massive the object, the 
		deeper the depression. An object traveling near a depression will have 
		its path altered or bent – like our orbit around the Sun, which is 
		considered traveling in a straight line through the curve of space. 
		Based on this theory, a black hole creates an infinite depression that 
		any object caught will forever spiral into nothing – or at least into 
		the very center of a black hole called a singularity (Ostlie, page 663). 
		The discussion on singularities is beyond the scope of this paper, and 
		will summarily be ignored. Back to Top 
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High Mass Stellar Evolution 
		The laboratory of a 
		binary star system: 
		“In the 
		constellation of Cygnus, there lurks a mysterious, invisible force. The 
		Black Hole of Cygnus X-1.” 
		Neil Peart from the 
		rock group Rush. Cygnus X-1, “A Farewell to Kings.”  All objects (with the 
		exception of black holes) emit some form of electromagnetic radiation. 
		We are most familiar with visible light. When something is heated to a 
		very high temperature, emission of x-rays is possible. In fact, if the 
		temperature of an object reaches at least 107 Kelvin, 
		x-ray emissions are detectable (Kutner, page 337). The Einstein X-Ray 
		Observatory, 
		launched in 1978, discovered a strong x-ray source emanating from a 
		binary star system in the constellation Cygnus. To confirm this, radio 
		observations also agree with the pattern of variability emanating from 
		this source (Kutner, page 216). The optical counterpart is shown to be, 
		based on spectroscopic data, a blue supergiant star, or an O9 type star. 
		This pair is considered a spectroscopic binary, and careful study has 
		revealed the companion to be 8 solar masses (Kutner, page 217). With an 
		object so small and so massive, the conclusion is that the companion is 
		possibly a black hole.  With nearly half of all 
		stars in the Universe being binary or multiple star systems, it may seem 
		that there would be more candidates, but detecting black holes is harder 
		than it seems. For any interaction between a pair of stars, the system 
		must be considered a close binary pair. This means that the 
		gravitational domain of each star, called the Roche Lobe, must either be 
		in contact with each other or overlap each other (Freedman, page 493). 
		With an object like a black hole in a close binary system, the intense 
		gravity literally feeds off of the accompanying star. The gas from the 
		companion star is pulled in by the black hole and the angular momentum 
		of the gas results in an accretion disk that is heated to intense levels 
		by compression near the edge of the black hole (called the event 
		horizon) to produce a very strong source of x-rays (Ostlie, page 672). 
		These x-ray sources are not very common, and there are other sources of 
		x-rays from binary systems from neutron stars which can also emanate 
		x-rays using the same mechanism as the black hole; however, there is a 
		difference in intensity that allows the determination of the source. The 
		mass of the unseen object leads to a differentiation between a neutron 
		star and a black hole. Currently there are two very strong black hole 
		candidates from a binary system – Cygnus X-1 and LMCX-3, an x-ray source 
		in the Large Magellanic Cloud (Kutner, page 217). How can one star 
		remain a supergiant while the other evolved quickly into a black hole? 
		The answer is simply, the black hole was a supergiant star much larger 
		and much hotter than its companion, and its stages of evolution occurred 
		more rapidly. Close binary star systems containing a supergiant 
		counterpart are not the only location for a possible black hole; 
		scientists have found an M class star 
		with an unseen companion with a mass of 3.97 solar masses. With the 
		appearance of occasional x-ray bursts, 
		it is concluded this may be a black hole [R8]. Back to Top 
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High Mass Stellar Evolution 
		Other candidates: The search for black 
		holes are not limited to binary star systems. There is a growing field 
		of study of supermassive black holes that appear to reside in the 
		centers of every galaxy. The Hubble Space Telescope imaged the center of 
		galaxy M87, and discovered a very bright source with a jet of material 
		emanating at incredible speeds. It is calculated that the mass of this 
		area is 3 x 109 solar masses (Freedman, page 551). While 
		x-ray jets have been studied in distant galaxies with the x-ray material 
		moving at velocities near the speed of light [R3], not all supermassive 
		black holes emit copious amounts of x-rays. In the center of our own 
		galaxy, an invisible source known as Sagittarius A seems to be the focal 
		point of our galaxy. What makes this spot special is that stars near 
		this region seem to orbit this spot at incredible speed. 
		By calculating the effects on the surrounding stars, it is concluded 
		that this unseen object has a diameter of 1 A.U. 
		with a mass of 3 million Suns (Freedman, page 582). Further evidence of 
		this supermassive black hole is given by its ability to consume a star. 
		On May 9, 2003, a group of European astronomers studying Sagittarius A 
		witness a star being devoured by the supermassive black hole [R6].  Back to Top 
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High Mass Stellar Evolution 
		Other methods of 
		detection and other locations of black holes: In the Perseus A galaxy 
		cluster, galaxy designation NGC 1275 has at its center a candidate of a 
		supermassive black hole. Emanating from the center, in addition to 
		copious x-rays, are what may be pressure waves. These waves seem to 
		emanate in a pattern of a sound, B-flat to be specific. These sound 
		waves are said to be 57 octaves below middle-C [R4].  There is also a 
		growing interest is what is called intermediate-mass black holes. This 
		supposed ‘missing link’ between stellar black holes and supermassive 
		black holes are thought to reside at the core of globular clusters [R5]. 
		The data is still being accumulated. The very successful XMM-Newton 
		orbiting x-ray observatory is locating more black hole candidate x-ray 
		sources similar to Cygnus X-1. Ten candidates within the Andromeda 
		Galaxy have been documented by the XMM-Newton
		(http://www.spaceflightnow.com/news/n0403/29blackhole/). 
		Black holes that seem to hide within the material of its companion star 
		have also been detected by x-ray and gamma ray detection telescopes 
		[R7]. Back to Top 
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High Mass Stellar Evolution Summary: Our current observational 
		ability has revealed a number of indirect methods of detecting these 
		elusive objects. With the growing list of potential black hole 
		candidates, one thing is certain: a black hole is certainly beyond a 
		theoretic idea and a real object that exists in our Universe. With 
		improved x-ray and gamma ray telescopes introduced into orbit around 
		Earth, the list of candidates is sure to grow. We may not be able to see 
		a black hole, but we can certainly learn a great deal from the effects 
		of a black hole. Further understanding of these elusive objects will no 
		doubt add to our knowledge of stellar evolution, and maybe even add to 
		our understanding the dynamics of galactic formation. The future is 
		indeed a very exciting one. Until then, let the research continue. Back to Top 
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High Mass Stellar Evolution References: [R1] Freedman, Roger A.
		Universe: 6th Edition. W.H. Freeman and Company, 2002 [R2] Hawking, Stephen. 
		The Universe in a Nutshell. New York: Bantam Books,  November 2001. [R3] P.L.G. AstroNews. 
		“Jets from a Black Hole.” Astronomy Magazine January 2003: 26 – 
		49. [R4] MacRobert, Alan. 
		“Sound from a Black Hole.” Sky and Telescope December 2003: 18 - 
		19. [R5] Nadis, Steve. “Black 
		Holes in the Middle.” Astronomy Magazine March 2004: 36 – 41. [R6] Whitt, Kelly K. “The 
		Last Goodbye.” Astronomy Magazine February 2004: 28. [R7] Netting, Jessa F. 
		“Black Holes that Hide.” Astronomy Magazine February 2004: 32. [R8] R.B. News 04. “Is 
		the smallest black hole known?” Astronomy Magazine April 2004: 
		25. [R9] Ostlie, Dale A., and 
		Bradley W. Carroll. Modern Stellar Astrophysics. Massachusetts: 
		Addison-Wesley Publishing Company, 1996. [R10] Kutner, Marc L. 
		Astronomy: A Physical Perspective. Cambridge: Cambridge University 
		Press, 2003. Back to Top |
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