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Hydrostatic Equilibrium

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How does the Voigt profile depend on wavelength? Increase l, increase width ... Radiation can't get through. Even with low opacity a lot of photons get absorbed ... – PowerPoint PPT presentation

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Title: Hydrostatic Equilibrium


1
Hydrostatic Equilibrium
  • Physical Astronomy
  • Professor Lee Carkner
  • Lecture 10

2
Questions
  • How does the Voigt profile depend on wavelength?
  • Increase l, increase width
  • How does the Voigt profile depend on temperature?
  • Increase T, increase width
  • How does the Voigt profile depend on atomic mass?
  • Increase m, decrease width
  • How does the Voigt profile depend on number
    density?
  • Increase n, increase width
  • Goes as n

3
Stellar Interiors
  • We cannot see stellar interiors directly
  • Our theories on the interior of stars come from
    stellar models
  • Key variables are pressure, temperature and
    density as a function of radius

4
Equilibrium
  • A star is just a big ball of gas
  • Since the star is static, the two forces must be
    equal
  • Force of gravity on small mass dm is
  • Fg -(GMrdm)/r2
  • Where r is the distance from the center of the
    star and Mr is the mass interior to r

5
Pressure
  • Since P F/A and dm rAdr, we can write
  • dP/dr -GMrr/r2 -rg
  • dP/dr is the pressure gradient
  • Pressure decreases as we move towards the surface

6
Equation of State
  • Is related to density and temperature
  • Example ideal gas law
  • Where N is number of particles and n is the
    number density of particles
  • Remember ideal gas law is gets less accurate as
    the density increases

7
Mean Weight
  • n r/mmean
  • We then define the mean molecular weight, m in
    terms of the mass of hydrogen
  • m mmean/mH
  • P rkT/mmH

8
Gas Composition
  • If there are heavier elements, m increases
  • For example, stars are mostly hydrogen with
    significant helium and very small amounts of
    heavier elements
  • If the gas is ionized, m decreases
  • Ionized gas, m 0.62

9
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10
Mass Continuity
  • Mass is continuous
  • dMr r(4pr2 dr)
  • dMr/dr 4pr2 r
  • The total mass is just the integral over the
    whole star

11
Particle Energy
  • Kinetic energy thermal energy
  • ½mv2 (3/2)kT
  • Eventually fast enough to overcome Coulomb
    repulsion

12
Radiation Pressure
  • Radiation pressure
  • Prad (4s/3c)T4
  • Note that Prad is strongly temperature dependant

13
Energy Transport
  • Energy is transported in stars either by
    convection or radiation
  • Convection dominates when
  • Radiation cant get through
  • Even with low opacity a lot of photons get
    absorbed

14
Transport in Stars
  • Low mass stars are un-ionized and have high
    opacity (convection)
  • Near the cores of medium mass stars there is high
    ionization and thus low opacity (rad then conv)

15
Next Time
  • Read 10.3, 10.6, 11.1
  • Homework 10.22, 10.23a, 11.1, 11.2a
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