This equation assumes that observations are taken in the background limited case, where
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is the predicted limiting magnitude. |
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is the zeropoint of the instrumental scale (i.e. the magnitude of a source that gives a flux of 1 ADU/s). |
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is the signal to noise ratio for the detection of the limiting magnitude. |
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is the gain (in e-/ADU) of the detector. |
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is the background signal per pixel (in e-/s/pix). |
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is the
number of pixels covered by a point source. We assume that
n=pi*(seeing/0.238)2 ie. the source radius is equal to the
seeing (fwhm), which is probably pessimistic. For extended objects, the
limiting magnitude per
arcsec2 has been given instead i.e. n=1/0.2382. |
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is the total on-object integration time (ie. the number of object frames × exposure time of each individual frame). |
From the formula above, it can be seen that if the background increases by a factor of 2, the limiting magnitude in the plots would decrease by ~0.38 mag (or ~0.38 mag/arcsec² for extended objects). In order to reach the same limiting magnitude, one would need to increase the total on-object exposure time by a factor of 2.
Note that you can also use the exposure time calculator
SIGNAL to calculate the number of photons (from both the object and
the sky) that will be detected during an INGRID exposure of a point or
extended source.
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Last Updated: 30 January 2008
Ian Skillen, wji@ing.iac.es |