Contraction stops - heat from fusion

M.S. is longest stage in lifetime

Time in M.S. inversely proportional to (mass) of star:

MS Lifetime
Mass Class Time in M.S.
30 O 2 million yrs.
10 B 20 million yrs.
1 G 10 billion yrs.
0.2 M 200 billion yrs.

Exponential Relationship

MASS OF STARS

Can use Newton's Laws for eclipsing binaries if period can be measured, but is difficult (m1 + m2) P2 = r3

If main sequence star - mass - luminosity relation

More massive - greater luminosity "

Energy Transport:

Convection in core only

Lower MS Stars:


Convection in outer regions

Core Reactions:

Mainly Proton-Proton chain (P-P Chain) & also CNO cycle

Both: H - He 92% P-P

8% CNO for Sun

Evolution of Sun-like Stars

Hydrogen in core used up

He core shrinks and heats up

Fusion of hydrogen continues in shell surrounding contracting core

Core degenerate matter (free electrons)

Meanwhile, outer layers expand greatly - lst red giant stage

Convective outer layers

Shell source contributes to heating of core


Helium core - relatively small
Helium core continues to shrink and heat up until helium ignites in Helium flash - sudden rapid ignition of core - Triple alpha reaction: 3He - Carbon

Degeneracy is destroyed - normal matter restored in core

Outer layers retract - hotter - horizontal branch on H-R

Finally He in core exhausted leaving carbon (from Trip. alpha)

He fusion continues in shell

Hydrogen shell may also exist

Star expands and cools - second red giant stage ( 1 million yrs.)

Stellar Evolution: 5-10 solar mass

Middle - Upper Main Sequence

Gradually increases luminosity while on m.s. Uses up hydrogen in core 100,000,000 yrs. Core contracts

Hydrogen shell ignites, star expands to R.G. Core not degenerate - temp. too high

Triple - alpha (helium fusion) begins w/o helium flash Core temp. increases - alpha-capture reactions:

Triple alpha - Carbon, Carbon + Helium nucleus (alpha particle) - oxygen, oxy + alpha - neon. . . . etc. Buildup of heavy elements in core.

Eventually core is exhausted

Fusion continuous in helium shell - 2nd R.G. stage

Meanwhile, mass lost due to dense stellar winds

Reduce number of alpha-capture reaction stages and overall lifetime

Can end up as white dwarf if has lost enough mass - 1. 4 solar masses or less Chandrasekhar's Limit

White dwarf will have dif ferent. composition than one f rom I s.m. star

Contain more heavy elements, oxygen, neon, etc.

If insufficient mass lost, sudden infalling when reactions cease - Supernova explosion

- neutron star (2-3 s.m. left) or black hole

Massive Stars > 10 s.m

Evolution occurs quickly

Do not become more luminous (move upward on H-R) because are losing mass due to strong winds

Alpha-captive reactions progress all the way to iron (can go no further)

Meanwhile, winds can strip envelope to reveal portion of core - Wolfe-Rayet star: hot star with strong winds apparent, emission lines

Carbon, nitrogen, oxygen seen-emission lines (from triple alpha and alpha-capture)

Supernova explosion

Alpha capture reactions progress to iron then stop

Core then collapses rapidly

Outer layers crash inward - massive rebound explosion or Supernova - driven by flood of neutrinos from rapid nuclear reactions

Stellar Remnants

Form of remnant depends on mass remaining after red giant

1.4 s.m. or less - white dwarf

Larger stars - neutron star or black hole:

Neutron star: >1.44 sm, <2-3 sm

Black hole: >2-3 sm

White dwarfs: faint stars showing few very broad spectral absorption lines
Lines widened due to extreme pressure in atmosphere, and

Zeeman effect (doubling of lines due to magnetic field)

Extreme contraction of W.D. can greatly intensify magnetic field

Spectral lines shifted toward longer (red) wavelengths gravitational redshift, as predicted by relativity theory

Solitary white dwarf takes up to several billion years to completely cool

Outer skin nearly opaque gas - blocks radiation of thermal energy

Nova Explosions:

White dwarf average 60,000 x brightness increase

Recurrent novae - same star goes nova more than once (perhaps decades apart)

Dwarf novae - scaled-down novae, also recurrent

Sudden flare-ups of novae due to degenerate gas present in W.D. - runaway explosion as in helium flash

Fuel for nova explosion must come from outside source - other star in binary system