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| subject: | ATM Alt-alt telescope mounts and image rotation - long post |
From: "Mel Bartels" To: Cc: Reply-To: "Mel Bartels" Alt-Alt or El-El telescopes (abbreviations for Altitude-Altitude or Elevation-Elevation) look like yoke mounts laid flat. The yoke is horizontal. Typically the polar axis of the yoke points towards a pole, as that area is usually deemed less important and thus left inaccessible, unless the mount is made more complicated by an offset-yoke design or horseshoes at each end ala a mirrored-Palomar 200 inch. By moving the scope in the primary axis, the scope rises in elevation. By moving the scope in the secondary axis, the scope also rises in elevation, but at a 90 degree angle to the primary axis. Since movement in both axes raises the scope in elevation, the name is appropriately given. For people in the mid-latitudes, field rotation can be obtained by looking at the field rotation of a standard altazimuth (Dobsonian styled) mount near the polar horizon. That is, an Alt-Alt telescope is essentially a Dobsonian that is tipped over at 90 degree angle to point to pole. The Alt-Alt's field rotation at the sky's zenith is the same as the field rotation of a Dobsonian aimed at the polar horizon. A typical rate would be 0.18 degree per minute of time. So if aimed at the sky's zenith, a digital imager can go for several minutes before rotation shows in the corners of the digital frame. A traditional Dobsonian might have say 6 times more image rotation when aimed within 10 degrees of the sky's zenith, and will have to cut the exposure that much shorter. Consequently, often the imager will keep exposures to a couple of minutes and avoid the zenith when using an altazimuth scope, or, add a field rotator unit at the focuser. This field rotator unit can also be a mechanism that rotates the entire tube assembly, instead of rotating the focuser. Some consider this no more difficult to make than the focuser/derotator. And, it is possible to move this third axis of motion, added to eliminate field rotation, to elsewhere in the mount. More on this in a bit. The primary axis of an Alt-Alt telescope need not be aimed at a pole. It can be aimed anywhere, depending on what you wish to optimize. Imagine a star or a satellite moving in a short arc across the sky. It is possible to orient the Alt-Alt in such a manner as to minimize overall motion of the two axes, or to minimize the highest speed of the two axes. As long as we are moving the Alt-Alt's primary axis in a circle and aiming it at different horizon points, why not turn it into a full fledged axis and motorize it? We have what is called a 3-axis mount, or what I will call an Alt-Alt-Az mount. By suitable orientation, any object (ie, a satellite) scribing a great circle can be tracked with motion in a single axis. By tracking in the third additional azimuth axis, the field rotation that occurs while tracking a celestial object can be stopped completely. For instance, consider the following scenarios (I wrote out an algorithm in Java last night and tonight to do the 3-axis initializations and tracking numbers - that's where the data comes from). All these use my northern latitude of 44 degrees. Primary axis aimed at northern pole, object at zenith: to null field rotation over a 1 minute exposure, the axes must move the following amounts: alt-primary 0.1798 degrees alt-secondary -0.0012 degrees azimuth 0.1737 degrees That's pretty nice - easy small amounts of motion in all three axes to track a celestial object with no field rotation. Primary axis aimed at northern pole, object in the east: to null field rotation over a 1 minute exposure, the axes must move the following amounts: alt-primary 0.2699 degrees alt-secondary 0.1799 degrees azimuth 0.1737 degrees Hmm, what's this - the azimuth rate seems suspiciously similar. Let's try it again for an object to the south. alt-primary 0.1797 degrees alt-secondary 0.0000 degrees azimuth 0.1737 degrees Ok, too much for coincidence, and, if you think about this 0.1737 number, and think about the distance tracked in equatorial coordinates over 1 minute of time, which is 0.25 degrees, this 0.1737 is the sine of the site latitude times the tracking time! No matter where you are aimed in the sky, with the primary axis aimed at the polar horizon, the tracking rate in the azimuth axis is constant. Let's try this same game but with the primary axis aimed say at 90 degrees azimuth, towards the east instead of the north. At the pole: alt-primary 0.0000 degrees alt-secondary 0.1798 degrees azimuth 0.2357 degrees Now aimed at object in the east: alt-primary 0.0578 degrees alt-secondary 0.1222 degrees azimuth 0.2357 degrees Ah, so the azimuth tracking rate is constant no matter where the scope is aimed with the two Alt-Alt axes, and is about 1.36 times greater with the azimuth axis aimed to the east - hmm, what relationship applies here ? Remember where I mentioned that the field rotation compensation can be at the focuser, or at the optical tube assembly? Well, it can also be at the azimuth axis of an Alt-Alt-Az scope. We can generalize that any 3 axis telescope can be made to track and null field rotation no matter its orientation with respect to the sky. The 3 axis scope can be an altazimuth-field derotator, or, an Alt-Alt-Az mount. I an imagining all sorts of interesting Alt-Alt-Az designs that could be built by amateurs with ordinary skills and tools. I have the software routines - any takers ? Mel Bartels --- BBBS/NT v4.01 Flag-4* Origin: Email Gate (1:379/100) SEEN-BY: 633/267 270 @PATH: 379/100 1 106/1 2000 633/267 |
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