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A nebula (97% H, 3% helium) contains regions where matter clumps. Clumping of matter into a protostar (young, precursor) is called ACCRETION The protostar must achieve equilibrium between gas pressure and gravity 1. 2. 3. 4. Gravity pulls gas and dust inward toward the core. Inside the core, temperature increases as gas atom collisions increase and density of the core increases. Gas pressure increases as atomic collisions and density (atoms/space) increase and the protostar’s gas pressure RESISTS the collapse of the nebula. When gas pressure = gravity, the protostar has reached equilibrium and accretion stops 1. 2. If critical temperature in the core is not reached, the protostar becomes a brown dwarf and never reaches star status If critical temperature is reached, nuclear fusion begins (H fuses into He for the first time) • • • • Stars will spend the majority of their lives fusing H into He When H fuel is gone, He is fused into C Massive stars are able to fuse C into heavier elements Stars slowly contract as they release energy during their life, yet their internal temperatures, densities and pressures continue to increase in the core HiLo Star Animation Larger stars have more fuel, but they must burn this fuel faster to maintain equilibrium Fusion happens at an accelerated rate in massive stars and therefore they use up their fuel supply in a shorter amount of time Bottom Line: Large stars burn bright and die young Small stars burn consistently and live long • 1. 2. 3. 4. 5. Throughout its life, a star oscillates between stable and unstable states Nuclear Fusion. Gas pressure=Gravity Fuel (H and He for small-medium stars; C-Fe in massive stars) runs out Fusion stops and temperature decreases Core contracts Increase in temperature and density due to increased particle collisions reignites the process. Entirely dependent on the initial mass of the star Low mass stars do not have conditions to fuse He into C Outer layers puff away creating planetary nebula The Sun dies Entirely dependent on the initial mass of the star Massive stars are able to create iron cores over the span of their lifetime and may supernova (explode) Crab Supernova & Cassiopeia Explosion 0.5 solar mass or less Outer layers puff away and become planetary nebulae. Eventually become white dwarves (about the size of Earth) Steadily decrease in diameter throughout life (no creation of planetary nebulae, no expansion, no supernova) (http://www.valdosta.edu/~cbarnbau/astro_demos/stellar_evol/evol_2.html) • • • • • 0.5 solar mass to 3.0 solar mass Gradually expands into a red giant / supergiant Outer layers puff away and may leave a white dwarf May supernova and become neutron stars (neutrons prevent future fusion reactions and create immensely dense conditions) Neutron stars are much smaller than Earth • • • • • • 3.0 solar masses or larger Expands into a red supergiant, Contracts and supernovas Nebular material is contracted back to the center of the star creating a black hole. Supernova / Hypernova?!?!!!! May become a large neutron star, then upon a secondary supernova become a black hole (http://www.valdosta.edu/~cbarnbau/astro_demos/stellar_evol/evol_3.html) Graphing Sunspots Hertzsprung Russell Diagram Data Analysis Lab on page 835 GeoLab on page 853 Identify the unknown elements Complete Analyze and Conclude Q:1-3 Wavelength distribution of energy from a black body (emits all wavelengths) at any temperature is of a similar shape, but of a different distribution (1 x 109 nm = 1 m) • T is the absolute temperature (K) of the black body • b is a constant called Wien's displacement constant, equal to 2.90 ×10−3 m·K • • λmax = b / T Wien's displacement law implies that the hotter an object is, the shorter the wavelength of its most emitted type of radiation • Wien’s Law Graph • Wien’s Law Practice •P. 851 Q: 3 and 5