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Published byEmma Hunt Modified over 9 years ago
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Stellar Structure Gas Mass Radiation Energy Generation Transport Radiative Convective Temperature Density Composition Hydrostatic Equilibrium:
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Hydrostatic Equilibrium A FpFp mm rr FgFg F’ p
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The Pressure Integral A AA xx v p cos
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Overcoming the Coulomb Barrier U cl = (3/2) kT cl → kT cl ~ 10 10 K U t = (3/2) kT t → kT cl ~ 10 7 K r t ~ deBrogle = h/p
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The PP Chain
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The CNO Cycle 12 6 C p 13 7 N e e+e+ 13 6 Cp 14 7 N p 15 8 O e e+e+ 15 7 N p 4 2 He
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Binding energy per nucleon Exothermic Endothermic Energy can be liberated via nuclear fusion Energy can be liberated via nuclear fission
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Convection Adiabatic expansion: P = K*
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Favorable Conditions for Convection Large Opacities → Large |dT/dr| rad Partial Ionization Zones → Brings close to 1 → small |dT/dr| ad Low g → small |dT/dr| ad = g/C p Strongly T-dependent energy generation (CNO cycle!) → large |dT/dr|
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Stellar energy transport structure as a function of stellar mass Low-mass stars (M < 0.25 M 0 ): Completely convective Sun-like stars (0.25 M 0 < M < 1.2 M 0 ): Radiative core; convective envelope High-Mass stars (M > 1.3 M 0 ): Convective core; radiative envelope M/M 0 R/R * 1 0.251.31.20.08 90
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Vogt-Russell Theorem The mass and composition of a star uniquely determine its radius and luminosity, internal structure, and subsequent evolution. => Almost 1-dimensional Zero-Age Main Sequence (ZAMS)
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Masses of Stars in the Hertzsprung- Russell Diagram 0.5 18 6 3 1.7 1.0 0.8 40 Masses in units of solar masses Low masses High masses Mass The higher a star’s mass, the more luminous (brighter) it is: High-mass stars have much shorter lives than low-mass stars: Sun: ~ 10 billion yr. 10 M sun : ~ 30 million yr. 0.1 M sun : ~ 3 trillion yr. L ~ M 3.5 t life ~ M -2.5
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Mass Sun Radiative Core, convective envelope; Energy generation through PP Cycle Convective Core, radiative envelope; Energy generation through CNO Cycle Summary: Stellar Structure
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Energy Transport Structure Inner radiative, outer convective zone Inner convective, outer radiative zone CNO cycle dominantPP chain dominant
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