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:''' To keep the temperature constant everywhere luminosity <math> L </math> must be generated | '''Energy generation:''' To keep the temperature constant everywhere luminosity <math> L </math> must be generated.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) | where <math> \epsilon </math> is the energy generation rate (sum of all energy sources and losses) |
Revision as of 15:40, 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: To keep the temperature constant everywhere luminosity must be generated.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