With this post I want to draw attention to a problem I found with my GSO 10" Truss RC. During collimation I found that when I align the optical axes of the focusser, secondary and primary mirror, the mechanical alignment as it can be seen in a Cheshire eyepiece is way off, and vice versa.
To find out why this is I measured the distance the edge of the secondary mirror has from the edge of its holder as can be seen in the following picture: Using a vernier caliper I found that the distance varies along the circumference of the mirror with a minimum of 28.4mm and a maximum of 28.9mm. In other words: the secondary mirror is tilted within its holder !
With this tilt, the inconsistent and confusing results of my various previous collimation attempts (and possibly also of some other owners of RCs) suddenly make sense.
What I learn from this is that collimation should always be done by aligning the optical axes, not the mechanical components of a telescope.
I used the following simple steps for a successful collimation:
focusser: optical axis of the focusser with the center of the secondary via a Cheshire eyepiece with crosshairs and the tilt screws of the focusser
secondary: optical axis of the secondary to the center of the Cheshire eyepiece with the central marker of the secondary using the tilt screws of the secondary
primary: optical axis of the secondary to the optical axis of the primary via the "hall of mirrors" test and the tilt screws of the primary
The only assumption is that the mark on the center of the secondary is its optical center. If this were not completely true, a final star collimation would have helped to correct this. But it turned out that it was not necessary.
Here is a simple image of M13, just one 2min exposure with an L filter, to demonstrate that there are circular stars up to the edges of the full-format sensor:
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