Specifications

Section 4 – Camera Hardware
Page 48
PC and Macintosh computer graphics resolutions, the CCDs used in the SBIG
cameras offer a good trade off between cost and resolution, matching the
computer's capabilities well.
Pixel Dimensions - The size of the individual pixels themselves really plays into the user's
selection of the system focal length. Smaller pixels and smaller CCDs require
shorter focal length telescopes to give the same field of view that larger CCDs
have with longer focal length telescopes. Smaller pixels can give images with
higher spatial resolution up to a point. When the pixel dimensions (in
arcseconds of field of view) get smaller than roughly half the seeing, decreasing
the pixel size is essentially throwing away resolution. Another aspect of small
pixels is that they have smaller full well capacities.
For your reference, if you want to determine the field of view for a pixel
or entire CCD sensor you can use the following formula:
Field of view (arcseconds) =
8.12x size (µm)
focal length (inches)
Field of view (arcseconds) =
20.6x size(um)
focal length(cm)
where size is the pixel dimension or CCD dimension in millimeters and the focal
length is the focal length of the telescope or lens. Also remember that 1° = 3600
arcseconds.
Read Noise - The readout noise of a CCD camera affects the graininess of short exposure
images. For example, a CCD camera with a readout noise of 30 electrons will
give images of objects producing 100 photoelectrons (very dim!) with a Signal to
Noise (S/N) of approximately 3 whereas a perfect camera with no readout noise
would give a Signal to Noise of 10. Again, this is only important for short
exposures or extremely dim objects. As the exposure is increased you rapidly
get into a region where the signal to noise of the final image is due solely to the
exposure interval. In the previous example increasing the exposure to 1000
photoelectrons results in a S/N of roughly 20 on the camera with 30 electrons
readout noise and a S/N of 30 on the noiseless camera. It is also important to
note that with the SBIG CCD cameras the noise due to the sky background will
exceed the readout noise in 15 to 60 seconds on the typical amateur telescopes.
Even the $30,000 priced CCD cameras with 10 electrons of readout noise will not
produce a better image after a minute of exposure!
Full Well Capacity - The full well capacity of the CCD is the number of electrons each pixel can
hold before it starts to loose charge or bleed into adjacent pixels. Larger pixels
hold more electrons. This gives an indication of the dynamic range the camera is
capable of when compared to the readout noise, but for most astronomers this
figure of merit is not all that important. You will rarely takes images that fill the
pixels to the maximum level except for stars in the field of view. Low level
nebulosity will almost always be well below saturation. While integrating
longer would cause more build up of charge, the signal to noise of images like
these is proportional to the square-root of the total number of electrons. To get