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An important consideration is pier height. Depending on the length of the telescope this affects ground clearance and maximum height when pointing at the zenith. This, in turn, affects the choice of sill height of the dome slit. Meanwhile the top arc, scribed by the dewshield, must clear the inside of dome. So all these dimensions are inter-related. They directly affect the height of the fixed walls of the observatory and the height of the pier.
The image shows the arcs of the long refractor 180mm [7"] f/12. The Dec. axis, when horizontal, is at 2m from the ground. In a 3m diameter dome it has no need of a pier quite this high. Particularly when the Heavy GEM is employed. Note that the circles should really be concentric. I exaggerated the height to show the effect of adding the longer dewshield.
From direct measurement of the OTA, on the MkIV mounting, I can allow the Heavy GEM to sit on a 1m high pier. Which by happy coincidence, is the height I have chosen for a temporary stand. The Heavy GEM is 64cm high from underside of the base plate to the Dec axis center when horizontal. Again, by coincidence this pairing exactly matches my eye height [while standing comfortably] at 164cm.

While the Moon can get quite high it is rarely that the planets reach such altitudes here at 55N. I can remember only one particular night when Saturn was high overhead. The seeing suddenly sharpened to single pixel viewing quality through my [normally indifferent] 6" f/8 refractor. It was just as if I was floating at a distance in a spacecraft with perfect windows. I stayed up just staring at Saturn until after 3am and was suitably admonished for my errant behaviour.

Assuming I balance the refractor OTA in the middle, using the sliding brass weight, I can easily clear the 3m dome. This would be with a wall height of 150cm to the sill of the open slit. With the horizontal Declination axis at 165cm high I can view distant trees with the OTA horizontal should I feel the need without losing any clear aperture. The top of the long dewshield is at its furthest from the ground when pointing at Polaris with the tube over the Polar Axis. When looking overhead the rotation of the Polar axis lowers the OTA on the end of the Declination.

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