7th Week: Stellar Structure and Evolution: Difference between revisions
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:<math> \frac {dM_r}{dr}= 4\pi r^2 \rho _r </math> | :<math> \frac {dM_r}{dr}= 4\pi r^2 \rho _r </math> | ||
Energy generation | Energy generation: Considering the energy leaving the spherical shell yields the energy equation | ||
:<math> \frac {dL_r}{dr}=4\pi r^2 \rho _r \epsilon </math> | :<math> \frac {dL_r}{dr}=4\pi r^2 \rho _r \epsilon </math> | ||
where <math> \epsilon </math> is the energy generation rate (sum of all energy sources and losses) | |||
per g and s | |||
Energy transport | Energy transport |
Revision as of 15:32, 18 March 2009
Stellar properties
The Hertzsprung-Russel diagram
Stellar structure
Stars of different mass and age have varying internal structures. Stellar structure models describe the internal structure of a star in detail and make detailed predictions about the luminosity, the color and the future evolution of the star.
Equations of stellar structure
Pressure equilibrium: The balanced of the gravity force and the pressure gradient is known as the hydrostatic balance.
Conservation of mass
Energy generation: Considering the energy leaving the spherical shell yields the energy equation
where is the energy generation rate (sum of all energy sources and losses) per g and s
Energy transport