glend
03-05-2020, 10:24 PM
I have been reading Mike Lockwoods comprehensive article on Cassegrain Optics, with commentary on some various design types. Article is here, scroll down to (Cassegrain Design Equations).
http://www.loptics.com/ATM/index.html
On the Design Equation page , Mike talks about many aspects but my question relates to mirror separation distances (d in the equations), and the role of separation in determining focal length, correction, and illuminated field of view.
My question is:
In a Classical Cassegrain, focal length is finely tuned and can be shortened or lengthen by altering (d) and is inversely proportional (ie, if you reduce the distance you can increase the focal length, and vice versa. The placement also affects Over and Under Correction of Spherical Aberration.
Is there a way to visually, or through bench testing of the scope (with normally available tools, like a Cheshire and circular grid target (easily made) to confirm full illumination (visability) of the primary field of view?
Mike suggests (in section D, on Size of Illuminated Field), we should be able to move our eye off to the side to see the edges of the primary, or not, as an indicator of full secondary illumination by the primary. I know through recent discussions (on Cloudy Nights) that the new GSO Classical Cassegrains, do not use the entire primary diametre, as they use a reduced secondary size ( meaning smaller central obstruction) to achieve a spot size of 15mm, to give optimal planetary performance.
My second question is: If I slightly alter primary tilt to tune out coma, (and there Is not much change they could make to separation), (note that in this design the primary mirror can be considered as fixed, the small adjustment and lock screws are for tilt and are not there providing a range of movement like that available in a typical Newt design).
If I do seek to tune out any residual coma, would I be changing spot size, affecting correction, and performance in some substantial way?
I am trying to gauge how my collimation setup, as i fine tune my scope, may impact on performance.
Thanks for your thoughts.:question:
http://www.loptics.com/ATM/index.html
On the Design Equation page , Mike talks about many aspects but my question relates to mirror separation distances (d in the equations), and the role of separation in determining focal length, correction, and illuminated field of view.
My question is:
In a Classical Cassegrain, focal length is finely tuned and can be shortened or lengthen by altering (d) and is inversely proportional (ie, if you reduce the distance you can increase the focal length, and vice versa. The placement also affects Over and Under Correction of Spherical Aberration.
Is there a way to visually, or through bench testing of the scope (with normally available tools, like a Cheshire and circular grid target (easily made) to confirm full illumination (visability) of the primary field of view?
Mike suggests (in section D, on Size of Illuminated Field), we should be able to move our eye off to the side to see the edges of the primary, or not, as an indicator of full secondary illumination by the primary. I know through recent discussions (on Cloudy Nights) that the new GSO Classical Cassegrains, do not use the entire primary diametre, as they use a reduced secondary size ( meaning smaller central obstruction) to achieve a spot size of 15mm, to give optimal planetary performance.
My second question is: If I slightly alter primary tilt to tune out coma, (and there Is not much change they could make to separation), (note that in this design the primary mirror can be considered as fixed, the small adjustment and lock screws are for tilt and are not there providing a range of movement like that available in a typical Newt design).
If I do seek to tune out any residual coma, would I be changing spot size, affecting correction, and performance in some substantial way?
I am trying to gauge how my collimation setup, as i fine tune my scope, may impact on performance.
Thanks for your thoughts.:question: