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v1.4.1
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@@ -174,9 +174,10 @@ def Edlen1966(l, T=288.15, p=101325, RH=0, CO2=300, f=None):
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def Owens(l, T=288.15, p=101325, RH=0):
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'''
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From Owens, 1967
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Equation 32
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Note that the pressure P and H are in torricelli (Torr),
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however, this is almost precisely 1 Torr = 1 mmHg
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Equations 29 to 31
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Code heavily based on ScopeSIM (https://scopesim.readthedocs.io/)
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and http://www.caha.es/newsletter/news03b/pedraz/newslet.html
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Parameters
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----------
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@@ -194,10 +195,27 @@ def Owens(l, T=288.15, p=101325, RH=0):
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n : float
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Refractive index of atmospheric air at the given conditions
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'''
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P = hPa2mmHg(p/100)
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T = K2C(T)
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s = 1 / l
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R = 8342.13 + 2406030 / (130 - s**2) + 15997 / (38.9 - s**2) * (P/720.775) * ((1 + P * (0.817 - 0.0133) * 1e-6)/(1 + 0.0036610*T)) - RH * (5.722 - 0.0457*s**2)
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# Calculation from ScopeSIM.effects.atmospheric_refraction()
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pres = p / 100 # from mbar to Pa
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Ps = -10474. + 116.43 * T - 0.43284 * T**2 + 0.0005384 * T**3
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Pw = Ps * RH / 100.
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Pa = pres - Pw
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# Wavenumber s
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s = 1. / l
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# Density factor of dry air, eq. 30
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Da = (Pa / T) * (1. + Pa * (57.9E-8 - 0.0009325 / T + 0.25844 / T**2))
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# Density factor of moist air, eq. 31
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Dw = (Pw / T) * (1. + Pw * (1. + 3.7E-4 * Pw) *
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(-2.37321E-3 + 2.23366 / T - 710.792 / T**2 +
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77514.1 / T**3))
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# Combining the two into eq. 29
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na = Da * (2371.34 + 683939.7 / (130. - s**2) + 4547.3 / (38.9 - s**2))
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nw = Dw * (6487.31 + 58.058 * s**2 - 0.7115 * s**4 + 0.08851 * s**6)
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R = na + nw
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n = R/1e8 + 1
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return n
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@@ -409,10 +427,10 @@ def slalib(l, T=288.15, p=101325, RH=0, h=0, lat=-24, tlr=0.0065, eps=1e-10):
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conditions.
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'''
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try:
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from pyslalib import slalib
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from pyslalib import slalib
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except ImportError as e:
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print('pySLALIB package not found! Try installing it first.\nReturning n=1.')
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return 1
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print('pySLALIB package not found! Try installing it first.\nReturning n=1.')
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return 1
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zObs = np.deg2rad(45.06563)
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p = p/100
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@@ -110,7 +110,7 @@ Input parameters for the spherical atmosphere models (all but the first):
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- xc - CO2 density [ppm]
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- lat - Latitude [deg]
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- h - Height above sea level [m]
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- l - Wavelength(s) [um]
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- l - Wavelength(s) [μm]
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- z - Zenith angle [deg]
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An example - To calculate the atmospheric refraction we set up a `refraction()` object. This requires the latitude and altitude of the observer. The atmospheric dispersion is calculated similarly, but by exchanging the `refraction()` object by a `dispersion()` object and parsing two refractive indices into the `cassini()` function.
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@@ -195,6 +195,7 @@ Included are
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| Bonsch & Potulski (1998) | `BonschPotulski()` | Allows for any temperature, pressure, humidity and CO2 density. |
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| Birch & Downs (1994) | `BirchDowns()` | Only at standard atmosphere. Function requires wavelength only. |
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| Peck & Reeder (1972) | `PeckReeder()` | Only at standard atmosphere. Function requires wavelength only. |
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| Mathar (2006) | `Mathar()` | Allows for temperature, pressure and humidity specification. Works best at wavelengths above 1.4 μm. |
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| Hohenkerk & Sinclair (1985) | `HohenkerkAndSinclair()` | Based on Barrell & Sears equation. Generally, gives slightly larger values.|
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| Hohenkerk & Sinclair (1985) | `slalib()` | Uses pySLALIB to retrieve the refractive index at standard atmospheric conditions.|
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@@ -226,9 +227,10 @@ Presently, several observatories are known. These can all be found in the `obser
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| Roque de los Muchachos Observatory (La Palma) | `LA_PALMA` | GTC, INT, WHT, NOT, and others. |
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| La Silla Observatory | `LA_SILLA` | ESO 3.6m telescope, NTG, BlackGEM and others. |
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| Las Campanas Observatory | `LAS_CAMPANAS` | Site of the future GMT. |
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| Mauna Kea Observatory (Hawaii) | `MAUNA_KEA` | Location of Keck, Subaru, Gemini North and others.|
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## Other
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This package also contains a python native port of the `SLA_REFRO()` routine of the pyslalib package, which was originally written in FORTRAN by P.T. Wallace. It can be called directly using `sla_refro()`. When using the same units as the other refraction functions, you might prefer using `slalib_refraction()` or `slalib_dispersion()`. Do note that this implementation is slower than the (compiled) FORTRAN implementation.
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Finally, the dispersion model used by Alexei Filippenko in 1982 is also included. This model is a combination of the (modified) Edlèn equation and a plane-parallel atmospheric geometry. This calculation can be accessed by calling the `Filippenko1982()` function.
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Finally, the dispersion model used by Alexei Filippenko in 1982 is also included. This model is a combination of the (modified) Edlèn equation and a plane-parallel atmospheric geometry. This calculation can be accessed by calling the `Filippenko1982()` function.
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@@ -21,14 +21,14 @@ def setup_package():
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# write_version_py()
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setup(name='AstroAtmosphere',
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version='1.4.1',
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version='1.5',
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description='Collection of equations for refractive index, refraction and dispersion calculations of atmospheric air.',
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long_description=__readme__,
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long_description_content_type='text/markdown',
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author='Joost van den Born',
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author_email='born@astron.nl',
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url='https://gitlab.astro-wise.org/micado/atmosphericmodel',
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download_url='https://gitlab.astro-wise.org/micado/atmosphericmodel/-/archive/v1.4.1/atmosphericmodel-v1.4.1.tar.gz',
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download_url='https://gitlab.astro-wise.org/micado/atmosphericmodel/-/archive/v1.5/atmosphericmodel-v1.5.tar.gz',
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license='GNU General Public License v3',
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data_files = [('',['LICENSE.txt'])],
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package_dir={'AstroAtmosphere': 'AstroAtmosphere'},
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