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Site Quality
The four sections below summarise information about observing conditions at
the observatory:
The IAC has produced a colour brochure (2001) including some of this information.
Measurements of the temperature, wind speed, humidity etc from 1999
are available from the
the ING
meteorology and seeing archive.
On average, 25% of observing time at the William Herschel Telescope is lost to bad weather (when cloud, wind speed, humidity, dust, dew or ice exceed the operational limits).
The median seeing at the William Herschel Telescope is 0.7 arcsec. More information can be found on the ING seeing pages.
The median seeing during the summer is probably ~ 0.15 arcsec better than the median during the winter. Further information about site seeing can be found on the IAC's Sky Quality Group web pages. (which include a comparison between IAC and ING DIMM seeing measurements). Atmospheric extinction above the observatory on La Palma is typically 0.12 mag in V band, and varies with wavelength. See La Palma technical note 31 (King 1985) for further information. During July, August, September, a pall of neutral-extinction ('grey') Saharan dust (properties described by Murdin 1986 in La Palma technical note 41) hangs over the islands, and the total extinction may be as high as 1 mag. The Mercator Telescope provides half-hourly measurements of site extinction at night. The Carlsberg Meridian Telescope records the extinction nightly. The median moonless night sky brightness above La Palma at high elevation, high galactic latitude and high ecliptic latitude, at sunspot minimum, is B = 22.7, V = 21.9, R = 21.0, rms 0.1 mag/arcsec2. The sky brightness in U and I is less well-determined, U approx 22.0 mag/arcsec2 (few data), I approx 20.0 mag/arcsec2 (variable). As at other dark sites, the main contributions to sky brightness are airglow and zodiacal light, in the ratio 2.5:1 at high ecliptic latitude. The sky is brighter at low ecliptic latitude (by 0.4 mag); at solar maximum (by 0.4 mag); and at high airmass (0.25 mag brighter at airmass 1.5). The mean brightness of the sky varies by < 0.1 mag with time after astronomical twilight. Light pollution is visible to the naked eye at certain azimuths on the horizon, but its contribution to the continuum brightness at the zenith is < 0.03 mag in all bands. The NaD emission brightens the sky in both V and R broad bands by about 0.07 mag. Total contamination (line + continuum) at the zenith is < 0.03 mag in U, approx 0.02 mag in B, approx 0.10 mag in V, and approx 0.10 mag in R. The brightness of the sky shows no dependence on atmospheric extinction AV, for AV < 0.25 mag (as is the case on 80% of nights). In very dusty conditions (extinction more than a few tenths of a mag), the sky brightness may be several tenths of a mag brighter, probably because of enhanced back-scattering of streetlighting by the dust layer. Further details can be found in ING technical note 115 (Benn C.R., Ellison S, 1998, also available as a postscript file). For a recent investigation of light pollution, see Marco Pedani's article "An Updated View of the Light Pollution at the Roque de los Muchachos Observatory" in the ING newsletter, 9, 28. A typical La Palma night-sky spectrum is shown below: |
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The continuum is dominated by airglow (actually pseudo-continuum) and zodiacal
light. The bright OH lines in the near-IR and at 5577, 5890/6 (some of the
emission),
6302 and 6364 Å are airglow.
The remainder of the 5890/6 NaD line is light from La Palma's low-pressure sodium street-lights, back-scattered from the atmosphere above the telescopes. The faint 4358 and 5460 Å lines are from mercury street-lights. Typical broad-band filter bandpasses are shown.
When the moon is 60 deg from zenith, with extinction 0.15 mag,
the zenith sky will brighten by ~ dmag magnitudes as tabulated below:
Note that the quarter moon (i.e. half disc illuminated)
is a factor of 10 (not 2) fainter than full, due to the
opposition effect (also responsible for gegenschein on the
ecliptic and dry heiligenschein on earth).
The contribution of moonlight in V has been calculated
according to the scattering formula of Krisciunas & Schaefer
(1991, PASP, 103, 1033), normalised (multiplied by a factor
of 2.4) to agree with measurements of sky brightness made at
the JKT on a dust-free night in 7/98.
The moonlight contribution in the other bands is calculated
according to the U-B, B-V, V-R, R-I colours of moonlight
measured on the same night in 7/98.
These numbers provide a rough guide to the brightness of the
moonlit sky.
The actual brightness on a given night will depend strongly
on how much dust and cloud is present.
Definitions of dark, grey and bright time can be found in
La Palma technical note 127 (Skillen 2002).
Moonlight diagrams can be found here.
Information about artificial satellites (including flare predictions)
can be found here.
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