|
O sun! Burn the great sphere thou mov'st in; darkling stand The varying star o' the world. Shakespeare, Antony and Cleopatra IV |
Assignments:Read Chapter 28, pp. 451-467Problem Set #4 due Thursday 5pm
|
In Class:---------------- review: PP process - the main fusion pathway in the Sun for one PP reaction: mass lost = 4.75 x 10^-29 kg 4.75 x 10^-29/6.6904 x 10^-27 = 0.007 only 0.7% of the total mass involved E = (4.75 x 10^-29 kg)(3 x 10^8 m/s)^2 = 4.28 x 10^-12 kg m^2 / s^ = 4.28 x 10^-12 Joules - the mass "lost" is the source of energy for the Sun - conversion from 4H's to He results in mass "loss" - so in some odd way, the Sun really is burning up The Sun "gives away" 3.8 x 10^26 Joules every second (luminosity = Joules/second) if each reaction produces 4.28 x 10^-12 Joules, then we need 3.8 x 10^26 / 4.28 x 10^-12 reactions every second = 8.9 x 10^37 reactions/second each reaction involves 6.6904 x 10^-27 kg of H, so 5.9 x 10^11 kg of H are fused every second in the process 0.007 x 5.9 x 10^11 kg of mass is transformed into energy = 4 billion kg of mass per second -------------------------------------- While the pp chain is the main process occurring in the Sun, there are other ways to fuse H - alternate process -- CNO cycle - use C as the "workbench" for making He - attach H one at a time - two convert to n, releasing a e+ - last p+ causes nucleus to split, yielding 6C12 and 2He4 - 6C12 free to do it over again - net result: 4 1H1 --> 2He4 same as for pp chain same mass lost same energy released - why doesn't this process occur as much in the Sun? - 6C12 is highly charged (6 p+) - hard to get a p+ close to it - more repulsion --> need higher speeds to make a close enough collision --> higher speed == higher temperature -- Sun's not hot enough -- in hotter stars, this happens a lot --------------------------- These process can occur quite happily until you run out of fuel - though the reservoir is large, the Sun contains a finite amount of H and it will be used up after a long time. During this long period, stars are really stable - internal pressure and gravity are well-balanced - stars don't swell up or shrink - radiate at a constant rate - everything is hunky-dory - This stage lasts a long time - there's lots of H in a star --> this is the Main Sequence MS stars are H-fusing stars once a star gets its act together so that it's stable, it sits on the MS for 80% of its life Then what happens? - problem: use up all of the H in the core nothing left to burn doesn't mean all of the H in the star is used up - only H in the core is hot enough to fuse - H in outer layers is too cool - even a star "out of gas" is still mostly hydrogen - running out of gas means running out of H IN THE CORE With no energy generation in the core, - there's no longer a support mechanism for the star - gravity starts to win - star contracts - core can't produce energy via fusion, but still gets hot because it's crushed. - odd: core gets hotter once H-fusion STOPS - there's plenty of H left outside of the core - as the core heats up, it heats the region around it -eventually gets hot enough for H-fusion - "hydrogen shell fusion" - since it's in a shell around the core, it doesn't help support the core -- core continues to shrink -- heats up even more - accelerates the H-shell fusion - star "overheats" - outward pressures no longer balanced by gravity --> outward parts of the star expand A LOT -- even though core shrinks -- becomes a GIANT --> even though the core is really hot, the outer layers actually cool because of the expansion -- surface temperature drops to ~3000 K -- becomes RED --> RED GIANT STAGE |
Go Back