The Average Atmosphere Temperature of Stars (Omit)


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    The photosphere of a star is a layer from which of order half the photons can escape to infinity. It is often called the surface of a star for convenience. In fact, stars have no sharp surface: they just extend outward morphing into stellar winds.

    The photosphere itself is NOT a sharp surface, but has a thickness defined in some way and the whole stellar atmosphere extends from a bit below the photosphere to well above: in fact, it is the thing that morphs into stellar winds.

    For a cartoon of the solar atmosphere which an example of stellar atmospheres, see the figure below (local link / general link: sun_outer_layers_cartoon.html).


    For characterizing
    stellar atmospheres, we would like to have an average atmosphere temperature.

    There are actually 4 kinds of average atmosphere temperature that can be mentioned.

    If stars radiated exactly like a blackbody radiators from sharply defined surface (which would necessarily be a sharply defined photosphere), then the four kinds of the average atmosphere temperature would be exactly the blackbody radiator temperature. Since stars are only blackbody radiators to 1st order, the four kinds of average atmosphere temperature will NOT be equal in general, but they will usually be rather close to equal in some sense.

    We explicate the four kinds of average atmosphere temperature in the subsections below.

    1. Stellar Atmosphere Model Inner Boundary Temperature:

      A stellar atmosphere model inner boundary temperature is a basic parameter of stellar atmosphere and is obtained by fitting the stellar atmosphere model to observations of the star or star type you are modeling.

      So the model inner boundary temperature is a model-dependent result and NOT a direct NOR an indirect observable.

      We can explicate stellar atmosphere modeling a bit.

      The simplest model of a stellar atmosphere is specified as follows:

      1. A plane-parallel slab with only radial dependence for quantities: e.g., temperature, density, pressure, etc.: See the example model of the Sun's atmosphere in figure below (local link / general link: sun_atmosphere_model.html).
      2. Inner and outer boundaries: The inner boundary is deep the star where the matter and electromagnetic radiation (EMR) are in mutual thermodynamic equilibrium and the EMR is necessarily blackbody radiation. The inner boundary does radiate like blackbody radiator except for a well-understood small angular dependence of the emitted radiation beams. The outer boundary is set far enough out for you to capture all the stellar atmosphere effects of interest.
      3. A set of free parameters: The free parameters are set by fitting the model to observations (in particular, spectroscopy photometry, and luminosity) of the star or star type you are modeling. The fitted free parameters are themselves main model results and are useful in understanding stellar atmospheres in shorthand. They are also useful in setting the outer boundary conditions for stellar-structure modeling of the interior of stars.

        The most basic free parameters are:
        1. The inner boundary temperature or, alternatively, an effective temperature (which we describe below).
        2. A gravitational field strength g. The gravitational field itself depends on the mass and radius which can be taken as alternative free parameters. In the simplest model (which is what we are considering), the model is geometrically thin enough that a single value is adequate for the gravitational field and the radius of the stellar atmospheres.
        3. Composition which is usually solar composition with the abundance of metals (i.e., the metallicity Z) being often the single adjustable value.

      The atmosphere model gives you among other things a temperature PROFILE for the stellar atmospheres that varies to 1st order only with radius.

      Of course, atmosphere model fitted free parameters, temperature PROFILE, and other model results are only accurate insofar as your model fits the observations AND is sufficiently realistic to capture actual stellar atmosphere behavior.

      More complex models can be developed for greater realism which means they give more accurate model results. But more complex models are harder to calculate.

      An example of an stellar atmosphere model is the model of the Sun's atmosphere shown in the figure below (local link / general link: sun_atmosphere_model.html).


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    2. The Effective Temperature:

      The effective temperature is explicated in the figure below (local link / general link: solar_spectrum_graph.html).


    3. The Wien's-Law Temperature:

      If we apply Wien's law to a stellar spectrum, we obtain a characteristic or sort of average photospheric temperature which we call the Wien's-law temperature.

      Wien's law is described in the figure below (local link / general link: wien_law.html).

      For example, Sun's flux peak is at ∼ 0.475 μ (Solar Spectral Irradiance Handbook of Chemistry and Physics 82nd Edition Boca Raton, FL: CRC Press 2001.), and so by Wien's law we get T_W = (2897.7729 μ*K)/(0.475 μ) = 6100 K.


    4. Color Temperature:

      A general definition of color temperature is:

        The color temperature of a light source is the temperature of an ideal blackbody radiators that radiates light of a color comparable to that of the light source (Wikipedia: Color temperature).

      In astronomy, we usually use a more specific definition replacing "color comparable to" by "B-V color index equal to" (Wikipedia: Color temperature: Color temperature in astronomy).

      The B-V color index is the difference of the B and V magnitudes which is roughly speaking the ratio of yellow to blue light.

      The UBVRI passband system is illustrated in the figure below (local link / general link: photometry_ubvri.html).


    5. Spectroscopy:

      Because of the problem of extinction and other reasons, it usually better to determine temperature from spectroscopy and stellar atmosphere modeling rather than photometry if one has spectroscopy available.

        Question: Spectroscopy is:

        1. the study of spectroscopes.
        2. the study of flux transmitted by broad passband filters.
        3. the study of spectra.
        4. a set of spectral observations.











        Answer 3 and 4 are right, but answer 3 is the primary definition.

        Answer 4 is a secondary definition. One often says something like "the spectroscopy of star X shows ...".

      Spectroscopy is done using spectroscopes. A spectroscope is illustrated in the figure below (local link / general link: spectroscope.html).


      The process of determining the
      photospheric temperature is to model the stellar atmosphere and adjust the model atmosphere to get to fit to an observed spectrum.

      The accuracy of the fit depends on the physical realism of the model.

      A crude model that gives a good fit is NOT usually very accurate.

      A very realistic model that gives a good fit should give a high accuracy photospheric temperature as well as all the other details of the stellar atmosphere.

      But highly realistic stellar atmosphere models are demanding to create.

      However, whole online catalogues of advanced stellar atmosphere models have been created and are always being improved.

      Nowadays, one's computer searches the catalogues and finds a match to your observations. So it's all become rather easy.

      However, even advanced models are NOT perfect.

      A detailed model of the Sun's atmosphere is illustrated in the figure below.

      Atmosphere models for the Sun are particularly demanding if one wants to understand all of the Sun's atmosphere.

      We just know so much about the Sun's atmosphere that a complete model incorporating all we know is challenging to build.

    File: Star file: star_modeling_temperature.html.