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1 - Stellar Brightnesses

1 - Stellar Brightnesses. Spatially resolved source: Most sources are unresolved, however. Observed (apparent) brightness is: (will sometimes call this

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Okay, what is d ??????? If the luminosity (wattage) of a star is L ν, then If we measure the observed flux we can derive its luminosity, an important intrinsic property of the star:

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1 - Stellar Brightnesses Spatially resolved source: Most sources are unresolved, however. Observed (apparent) brightness is: (will sometimes call this the observed flux) Okay, what is d ??????? If the luminosity (wattage) of a star is L , then If we measure the observed flux we can derive its luminosity, an important intrinsic property of the star: Stellar Parallax If p=1 = 1 arcsec (1/3600), then d = AU = 1 parsec = 3.08x10 16 m. In astronomers units: Unless there is a REALLY good reason for doing so, use astronomers units, not km, radians, etc. for this. parallax and uncertainty in milli-arcsec REAL Parallax Measurements Have Uncertainties How Uncertain are the Distances? Stellar Spectral Energy Distributions are NOT Blackbodies, but often come close enough to utilize the mathematical formulation of a BB. Blackbody Radiation [Note: the total energy emitted by an isotropically-emitting surface unit area is B . Sometimes astronomers forget when they need the factor of and when they do not. ] (units renormalized - just to show the functional form) Wien Displacement Law The peak of B occurs at some max defined by To solve this, let This must be solved numerically, and has a solution x = So So h max 2.82 kT or Doing the same in wavelength units: Solar spectrum in wavelength and frequency units Note: max max c because B B . It is B d = B d!! When applying Wiens Law, you MUST use the formula appropriate for the units you are using. One can also use photons instead of power! From The Optics of Life: A Biologists Guide to Light in Nature by Snke Johnsen. Stefan-Boltzmann Law Again, letsoand The net energy emitted from a surface is proportional to T 4. Net Luminosity L Total energy emitted per unit area in all directions by an isotropically-emitting blackbody is : Integrating over all frequencies: Integrating over the surface of a (spherical) star: And we actually observe: Stellar Luminosity Stellar Temperatures Wien or or.... Effective (i.e. T a blackbody of the same integrated flux would have) Brightness Color Kinetic T - defined by the particle speeds, using the maxwellian velocity distribution Using the rms velocity distribution insures that T is a measure of the mean kinetic energy of the particles Excitation T - based on the relative population of electronic states in atoms and ions which are excited by collisions from other particles and photons Ionization T - based on the relative populations of ionization states of the atoms and ions are ionized by collisions from other particles and photons For Molecules: Rotational T Vibrational T Electronic T Because stars are not in perfect thermodynamic equilibrium, all these temperatures may differ from one another! It may be necessary to specify which one you mean.