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 so the star can lose energy.Considering the energy leaving the spherical shell yields the energy equation
'''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

Stellar evolution