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`Afrho` works seamlessly with `sbpy`'s spectral calibration framework (:ref:`sbpy-calib`) when the `astropy` affiliated package `synphot` is installed. The solar flux density (via `~sbpy.calib.solar_fluxd`) is not required, but instead the spectral wavelengths or the system transmission of the instrument and filter:
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@@ -108,7 +110,7 @@ The `Afrho` class may be converted to a flux density, and the original value is
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Thermal emission with *εfρ*
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^^^^^^^^^^^^^^^^^^^^^^^^^^^
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The `Efrho` class has the same functionality as the `Afrho` class. The most important difference is that *εfρ* is calculated using a Planck function and temperature. `sbpy` follows common practice and parameterizes the temperature as a constant scale factor of :math:`T_{BB} = 278\,r_h^{1/2}`\ K, the equilibrium temperature of a large blackbody sphere at a distance :math:`r_h` from the Sun.
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Reproduce the *εfρ* of 246P/NEAT from Kelley et al. (2013).
@@ -125,12 +127,14 @@ Reproduce the *εfρ* of 246P/NEAT from Kelley et al. (2013).
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Compare to 397.0 cm listed in Kelley et al. (2013).
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`Efrho` may also be converted to geometric cross sectional area, given emissivity, photometric aperture, and observer-comet distance:
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`Efrho` may also be converted to/from geometric cross sectional area, given emissivity, photometric aperture, and observer-comet distance:
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>>> epsilon =0.95# geometric albedo
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>>> G = efrho.to_cross_section(epsilon, aper, eph)
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