| Much of the early stages of the Main-Sequence 
							Turnoff for a high mass star is the same as a 
							low 
							mass star.
 
							 (Science 
							Cartoons Plus)
 It is important to state that while the 
							fusing of hydrogen to helium is being performed in 
							both 
							low and high mass stars, high mass stars 
							primarily burn hydrogen through the CNO cycle 
							(Carbon, Nitrogen, Oxygen). Carbon acts as the 
							catalyst in the fusion of hydrogen and nitrogen and 
							oxygen absorb the protons to create helium. If you are looking for professional help with your astronomy academic projects, just buy a research paper written by real experts.
 
 
								
									|  | The main reason for this is increased 
									temperature and 
									pressure at the core than a 
									low mass star. The hydrogen burning shell 
									and helium ash core also exist in the high 
									mass star. One major difference between a high mass 
									star and a 
									low mass star at this point is 
									the helium flash - there is no flash of 
									helium fusion in a high mass star. |  Here is a bit of a summary for high mass stars: 
							 (Image credit: Brooks/Cole Thomson Learning)
 
							The exact stages of evolutions are: 
								Subgiant Branch (SGB) - hydrogen shell 
								burning - outer layers swellRed Giant Branch - helium ash core 
								compresses - increased hydrogen shell burningFirst Dredge Up - expanding atmosphere cools 
								star - stirs carbon, nitrogen and oxygen upward 
								- star heats upCore Helium Flash - continued compression 
								with added helium ash ignites helium - lots of 
								neutrinosHorizontal Branch - helium burning core - 
								hydrogen burning shellPre AGB (Asymptotic Giant Branch) - outer 
								layers expand cooling the star - hydrogen shell 
								becomes dormantAGB - re-ignited hydrogen shell burning 
								(like a second Red Giant phase)Several stages of dredge up - 
								nucleosynthesis creates numerous elements (F, Ne, 
								Mg, Al, Li, Ne, Na) Because a high mass star (> 4 Solar Masses) has 
							considerably more gravity than 
							low mass stars, 
							several shell burning stages can occur: 
							 (Image credit: Brooks/Cole Thomson Learning)
 But there is a limit. Iron cannot 
							fuse, and when it tries the end result is a highly 
							compacted core and intense 
							temperatures. The core 
							density is 4 x 1017 kg/m3. 
							This is very degenerate and cannot be compressed 
							further. The intense heat generated by this 
							compression (core bounce) blows the star apart in a 
							type II supernova. 
								
									|  | Click on the image to the left to view 
									an animation of a supernova. In this 
									video, two things happen: the core 
									collapses, explodes and begins to expand 
									while the star collapses (video care of
									
									Swinburne Astronomy Online). |  
							 (© 2005 Russell Croman,
							
							www.rc-astro.com)
 The classic supernova remnant is the 
							Crab nebula. The end result of a supernova is 
							three fold: 
								
								Heavy elements created in the 
								explosion
								Intense interstellar wind
								A neutron star (or 
								black hole) 
								stellar remnant A white dwarf is the degenerate carbon core of a 
							low mass star. As such, a neutron star is the 
							degenerate iron core of a high mass star. 
							 (Image credit: Brooks/Cole Thomson Learning)
 Because if its composition (and energy at the 
							time of compression), intense magnetic energy 
							emanates from the neutron star, and it is spinning 
							rapidly (several thousand times a second). 
							 (Image credit: Brooks/Cole Thomson Learning)
 This spinning neutron star is called a Pulsar. At 
							the heart of the Crab nebula is its stellar remnant 
							- a pulsar: 
							 The image above demonstrates how fast a pulsar 
							can spin. What is also interesting is that they are 
							extremely accurate time keepers. A neutron star also 
							emits strong in the X-ray spectrum. Also, just like 
							a white dwarf, a neutron star can accrete material 
							from a companion star, but superheats it to extreme 
							temperature and spins faster.  If the high mass star is around 25 Solar masses, 
							the stellar remnant can compress much further than a 
							neutron star resulting in a 
							Black Hole. It's important to realize that a 
							black hole is 
							not a hole in space, it's just an object with 
							extremely high surface gravity - but since we have 
							yet to "see" one (and we probably never will), we 
							can only infer their existence by its effect on 
							surrounding matter. A good friend and fellow 
							class-mate wrote an excellent paper going into 
							detail on the subject of 
							Black Holes, and he has 
							graciously allowed me to post it here. So for more 
							information on 
							Black Holes, click
							Black Holes. Core Burning Stages in a 25 Solar Mass Star: 
								
									| Fuel: | Products: | Temperature (K): | Minimum Mass: | Burning Period: |  
									| H | He | 4 x 106 | 0.1 | 7 x 106 years |  
									| He | C, O | 1.2 x 108 | 0.4 | 5 x 105 years |  
									| C | Ne, Na, Mg, O | 6 x 108 | 4 | 600 years |  
									| Ne | O, Mg | 1.2 x 109 | ~8 | 1 year |  
									| O | Si, S, P | 1.5 x 109 | ~8 | ~0.5 years |  
									| Si | Ni - Fe | 2.7 x 109 | ~8 | ~1 day |  Classifications of Supernova: 
								
									| Type: | Characteristics: | Mechanism: |  
									| 1a | No H lines, strong Si II lines | Thermonuclear runaway on white dwarf |  
									| 1b | No H lines, prominent He I lines | Core collapse of massive star stripped 
									of hydrogen envelope |  
									| 1c | No H, Si II or He I lines | Core collapse of massive star stripped 
									of helium (and hydrogen) envelope |  
									| II-P | H lines - flat light curve | Core collapse of massive star |  
									| II-L | H lines - no flat light curve | Core collapse of massive star |  Back 
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