1 / 17

Stellar Structure

0. Hydrostatic Equilibrium:. Stellar Structure. Radiation. Mass. Gas. Energy. Generation. Density. Transport. Temperature. Radiative. Composition. Convective. 0. Hydrostatic Equilibrium. A. F p. D m. D F g. D r. F’ p. 0. The Pressure Integral. A. m = cos q. q. D A.

thina
Télécharger la présentation

Stellar Structure

An Image/Link below is provided (as is) to download presentation Download Policy: Content on the Website is provided to you AS IS for your information and personal use and may not be sold / licensed / shared on other websites without getting consent from its author. Content is provided to you AS IS for your information and personal use only. Download presentation by click this link. While downloading, if for some reason you are not able to download a presentation, the publisher may have deleted the file from their server. During download, if you can't get a presentation, the file might be deleted by the publisher.

E N D

Presentation Transcript


  1. 0 Hydrostatic Equilibrium: Stellar Structure Radiation Mass Gas Energy • Generation • Density • Transport • Temperature Radiative • Composition Convective

  2. 0 Hydrostatic Equilibrium A Fp Dm DFg Dr F’p

  3. 0 The Pressure Integral A m = cosq q DA p v Dx

  4. 0 Overcoming the Coulomb Barrier → kTcl ~ 1010 K Ucl = (3/2) kTcl Ut = (3/2) kTt → kTcl ~ 107 K rt ~ ldeBrogle = h/p

  5. 0

  6. 0

  7. 0

  8. 0 The PP Chain

  9. 0 The CNO Cycle p 42He g 126C ne 137N p 157N e+ 136C p ne 158O g e+ 147N g p

  10. 0 Binding energy per nucleon Endothermic Energy can be liberated via nuclear fission Exothermic Energy can be liberated via nuclear fusion

  11. 0 Convection Adiabatic expansion: P = K*rg

  12. 0 Favorable Conditions for Convection • Large Opacities → Large |dT/dr|rad • Partial Ionization Zones → Brings g close to 1 → small |dT/dr|ad • Low g → small |dT/dr|ad = g/Cp • Strongly T-dependent energy generation (CNO cycle!) → large |dT/dr|

  13. 0 Stellar energy transport structure as a function of stellar mass R/R* 1 M/M0 90 0.08 0.25 1.2 1.3 Sun-like stars (0.25 M0 < M < 1.2 M0): Radiative core; convective envelope High-Mass stars (M > 1.3 M0): Convective core; radiative envelope Low-mass stars (M < 0.25 M0): Completely convective

  14. 0 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)

  15. 0 Masses of Stars in the Hertzsprung-Russell Diagram Masses in units of solar masses 40 18 The higher a star’s mass, the more luminous (brighter) it is: High masses 6 3 L ~ M3.5 1.7 1.0 High-mass stars have much shorter lives than low-mass stars: Mass 0.8 0.5 tlife ~ M-2.5 Sun: ~ 10 billion yr. Low masses 10 Msun: ~ 30 million yr. 0.1 Msun: ~ 3 trillion yr.

  16. Summary: Stellar Structure 0 Convective Core, radiative envelope; Energy generation through CNO Cycle Sun Mass Radiative Core, convective envelope; Energy generation through PP Cycle

  17. 0 Energy Transport Structure Inner convective, outer radiative zone Inner radiative, outer convective zone CNO cycle dominant PP chain dominant

More Related