"...bad collimation is the number one killer of telescopes world wide..." Walter Scott Houston

FAQ about Collimating a Newtonian telescope

by Nils Olof Carlin (updated oct -00)

Well, maybe the questions here are not as frequently asked as they ought to be. After all, a lot of amateur astronomers own and/or use Newtonian telescopes. If you are one of us, you should ask these questions, and find out for yourself how important the answers are to the performance of your instrument.

What is collimating, anyway?

Collimating a telescope is lining up its optical components (lenses, mirrors, prisms, eyepieces) in their proper positions. This should be accurately done, or else the image quality will suffer.

Different telescope types, like Newtonian, Schmidt-Cassegrain, or refractors all need good collimation. However, they have quite different optical components, and here I will only talk about Newtonian telescopes, the simplest mirror telescopes.

Newtonian? My telescope is supposed to be a Dobsonian!

Don't worry. A Dobsonian telescope is a special kind of Newtonian, with a simple but very efficient mounting that distinguishes it from other Newtonians. Optically, and as far as collimating is concerned, they are the same.

I have bought a telescope, and it is factory collimated. Do I have to bother about collimating it?

Yes, most likely. If you have a factory-collimated refractor, Schmidt-Cassegrain, or Maksutov, you could very well leave the collimation alone and have a good chance of enjoying the excellent performance of your telescope for years to come. With a Newtonian, chances are less, for several reasons:

The main mirror must be held in place without stress that could bend it and change the optical figure, and cannot be rigidly held - it may shift slightly whenever you transport or shake the tube. The secondary mirror is also held by a "spider" that may change its position ever so slightly, and as we will see, it doesn't take much to disturb the collimation enough to really matter. If you move your telescope to darker skies and back, and particularly if you have one with truss tubes that you assemble and disassemble, you must be able to check the collimation each night out, and you must be able to tweak it whenever needed.

Even if your telescope was factory collimated before shipping, it may have been on its longest journey ever before it reached you, and chances are great that it has lost much of its collimation. If you learn how to check the collimation, you will know whether or not your telescope is ready to deliver its best.

If the situation is that bad, maybe a Newtonian isn't for me. Should I trade it in for something better?

My advice is: think again. There may be other good reasons for you to prefer another type of telescope. But a good Newtonian is a great performer when it is well collimated, and can come out close to or maybe ahead of any other instrument of the same size (aperture). Before you decide to trade it in, ask how much extra you would have to pay to get an alternative.

Suppose you have bought a fine guitar with a lovely note, and you are learning to play it. Now you notice it seems to get slightly out of tune. What do you do - learn how to tune it, or trade it in for a piano?

I believe that the reason Newtonians have a dubious reputation for critical performance is that too many Newtonians are never even collimated at all. Poor optics may not be easy or cheap to fix. Poor collimation, however, is something you can learn how to handle, and chances are good that you will be able to turn your scope into a star performer.

Don't forget - a complete collimation of all the optical components is a bit of work - but the nightly checking takes a few seconds, and the tweaking, if needed, may take a minute.

OK, I am willing to give it a try, at least. How do I do it? Read the manual?

When I tried to figure out the hows and whys of collimating, I had very little help of the manual for my 6-incher. I tried reading the sections on collimating in a few magazines and handbooks, without really understanding what should happen, and why. I kept on trying, and in due time I felt my efforts paid off. That is why I write this - I hope I can make it easier for you. But let me point this out: Much of what I write here is common knowledge, even if it is not easy to come by, but some is the result of my own studies and experiments - particularly the error analysis and some of the tools - and my recommendations here are very much my own (and very controversial in some places). I believe it is sound advice, but I may be wrong on some accounts - if you really find fault with what I say, don't hesitate to email me. Let it also be said that collimation is a subject of much heated discussion among us diehard Telescope Nuts, and I doubt that this will put an end to it.

I believe it will be easier for you to learn how, if you know why. By all means read your manual! Telescopes differ in design details, and your manual probably contains valuable information on how to adjust the screws and things on your particular instrument.

It's going to be a great night for observing, and I've got all the tools. I'm in a hurry, so skip the details - what do I do?

I've prepared a page that you can load and print out, but unless you have tried at least once, you should take the time you need to follow the detailed instructions and get truly familiar with the procedure.

What are the parts of a Newtonian, what do they do and what parts can or need I adjust?

This is basic stuff, and if you know it well already, just read quickly.

The optical parts are:

The main, or primary, mirror.

This is the large mirror in the bottom of the tube, with a concave, aluminized face figured to an extremely accurate paraboloid surface. It concentrates the light from a star into a sharp image - not really a point, but a diffraction pattern with a small circle of light surrounded by small, faint rings.

It is held in some kind of mirror cell, fancy or simple, that rests on 3 set screws. By adjusting these screws, you can finely adjust the tilt of the main mirror, this is an important part of collimation (you only need to adjust 2 of them - it might be wise to leave the third in a middle position). Often there are 3 extra screws for locking the mirror cell in place, once it is adjusted. It may look something like this:

The secondary, or diagonal, mirror.

This is a smaller mirror with an elliptical face (its size is given as the length of its minor axis, i.e. its "width"). It is suspended by a spider with one or several vanes inside the tube near its opening, and the face is at 45 degrees to the tube. It is used to deflect the light from the main mirror sideways, so that you can see the image without having your head in the way of the incoming starlight.

The secondary mirror holder, and often the spider itself, is adjustable. It can be (more or less easily) moved sideways and along the tube, and it can be tilted (or rotated) slightly. Commonly, the mirror holder has a center bolt and three screws for adjustment.

The eyepiece

This is a more or less fancy magnifying glass, used to see the image of the star or whatever else you look at. It has a certain focal length, and with several eyepieces of different focal lengths, you can select the magnification (often called "power") that you want. The focuser is where you put the eyepiece, it has a drawtube that holds the eyepiece and can be moved a little bit in and out, as needed to "focus" to get the sharpest view.

These optical parts are held in mechanical alignment by a tube of sorts. The tube, in turn, is supported by some mounting that lets you aim it wherever you want in the sky, and perhaps track its apparent motion as the Earth rotates.

How are they supposed to be aligned when the scope is well collimated?

There are two optical axes in a Newtonian telescope: the optical axis of the main mirror, and the optical axis of the eyepiece. The axis of the main mirror is perpendicular to the mirror at the optical center - for practical purposes taken as the center of the circular glass mirror. For convenience, the is often marked with a spot of paint or tape (more about that later). The light from a star in the exact direction of the main mirror axis will be reflected and "focused" to a sharp image at the focus on this axis. The distance along the optical axis, from the mirror center to the focus, is the focal length. Stars will be focused to sharp images in the focal plane, at or near the focus. (Actually, the focal "plane" is part of a sphere, with its radius equal to the focal length).

The axis of the eyepiece is usually taken as the center of the focuser drawtube. The secondary mirror reflects the incoming light to the side of the tube, and here the focused image forms, and is seen with the eyepiece. The secondary will also "reflect", or rather deflect, the optical axes - it has an optical center, but no optical axis to concern us.

The main purpose of collimating is to align the two axes to form one common axis. Normally, you do this by adjusting the position and tilt of the secondary mirror, and the tilt of the main mirror.

Here comes some heavy theory - do I really have to read it?

Glad you asked - if you read this for the first time, you will probably find it a bit difficult to chew and swallow in one bite. So if you like, skip to the "End of heavy theory" for some more practical stuff. But I am sure the theory will make you understand the practical things better, and you may go back to read it any time later.

A systematic background:

I propose the following system of requirements for collimating Newtonians, and the corresponding errors, to facilitate understanding of the process (for illustrations, see the section on the corresponding errors)

The first and foremost requirement is:

1 - The two optical axes should be coincident, forming one common axis.

To simplify the error analysis, this can be broken down into two parts, giving separate kinds of error if violated:

1A - The optical axes should intersect at the common point of focus.

1B - The optical axes should be parallel.

When these requirements are met, and we can consider one common optical axis, the following supplementary requirements should also be met:

2 - The optical axis should strike the optical center of the secondary mirror.

3 - The optical axis should be deflected 90 degrees by the secondary mirror

4 - The optical axis (between the main and secondary mirrors) should be centered in the tube.

A Newtonian telescope can be collimated to meet each of these requirements more or less closely, but as with mechanical adjustments in general, they cannot and need not be met exactly.

If we understand the effects of the separate errors, we can decide on the maximum error tolerances. We can then be sure that the telescope will perform as well as it should, if the collimation is done to within these tolerances. Here is a brief discussion of the effects of the errors:

Error type 1A - The optical axes are separated at focus by a distance D. The eyepiece focus is in the main mirror's focal plane, but at a distance D from its focus.

This is the crucial error for visual use. Images by the paraboloid mirrors of Newtonians can be close to perfect near the focal point, but suffer from increasingly severe coma at increasing distances from it. Coma is an optical aberration that causes loss of contrast and detail resolution. It is approximately proportional to the distance from focus, and inversely proportional to the third power of the focal ratio (f, this is the focal length of the main mirror divided by its diameter).

Any good eyepiece gives a very sharp view near its focus - that is in the center of the field of view. Towards the edge, however, all eyepieces cause more or less unsharpness of star images. This is mainly due to astigmatism (I won't explain that here!) of the eyepiece - it is not the mirror's fault - but shows up worse with a short focus mirror (with a low focal ratio). For most eyepieces, the coma of the main mirror gives much less contribution to the unsharpness.

But if the main mirror focus is in the focal plane away from the eyepiece focus, there will be some coma at the center of the field, where the image should be sharpest, and the image is not quite as clear and crisp as it could have been - particularly when you use high magnification to catch the subtle details of planet surfaces.

Under ideal conditions, the maximum distance from focus where coma barely affects the diffraction image from a star, has been given (Sidgwick) as 0.0036*f3 mm (0.000143*f3 in.). At a distance of 0.0088*f3 mm (0.00035*f3 in.), coma introduces a wavefront error of ¼ wave in addition to any other error present (Sinnott). For high resolution images, the tolerance should be set somewhere between these values (see table below). The tolerances may be relaxed for wide-field photography and for low-power viewing only, and perhaps also for instruments of very large apertures where seeing will limit the possible resolution. Surprisingly, the size of the telescope mirror doesn't come into the calculations, a larger telescope doesn't have a larger "sweet spot" than a smaller. You will notice that short focus telescopes (low f/ numbers) are very much more critical to collimate - that is one price you must pay for the convenience of a short, wide field telescope.
Focal ratio Strict tolerance ¼ wave tolerance
f/4 0.22 mm 0.55 mm
f/5 0.45 mm 1.1 mm
f/6.4 0.90 mm 2.2 mm
f/8 1.8 mm 4.4 mm
f/10 3.6 mm 8.8 mm

If you have a center spot that happens to be at a distance D from the true optical center, and do a perfect collimation against it, the collimation error 1A is half the distance, or D/2. Thus, the allowable miscentering of the center spot is much less than twice your tolerance!

Error type 1B - the optical axes are not parallel, but form an angle.

A star forms a blurred image if it is not focused within the focal "plane". The blur size can be easily calculated: let g be the distance from center to film corner, b the allowable blurring, f the focal ratio, and A the allowable error angle in radians: A = bf / g (to get degrees, multiply by 57.3!)

Let's assume you have a f/5 main mirror (f=5!), and use a 35 mm camera. You want the blur to be less than 0.1 mm near the corner of the film, 20 mm off. This gives A=0.025, or 1.4 degrees. The blur caused by coma is, in comparison, approximately b = g / (4f2), in this case 0.2 mm. (To get sharp, wide-field images with a "fast" Newtonian of low focal ratio, you need a coma corrector!)

For visual use, it is harder to calculate the effects of an error of this type. Real-world eyepieces have rather strongly curved focal surfaces, as well as off-axis astigmatism - even if some (not just expensive, but also bulky and heavy) types are better than others. If we assume, for the sake of argument, that the blur (as calculated above) should not be worse than the coma (which, in turn, is not worse than the eyepiece astigmatism), the two formulae above gives A=1/(4f). For f/5 that is 3 degrees, for f/8 it is 1.8 degrees!

Another way to look at it: with an error angle, some of the light will come to focus at a steeper angle than it should, thereby possibly increasing eyepiece astigmatism. If you have a f/8 mirror, none of the light will come at a steeper angle than from a f/6 mirror exactly collimated, if the error type 1B is 1/48 radians or 1.2 degrees.

The 1B error could also be expressed as a displacement of the focuser axis from the center of the main mirror - easily visible if you use a laser beam to trace the focuser axis. If the focal length is F and the error angle is A (in degrees), the displacement is A*F/57.3. Example: If F is 1800 mm, and A is 0.2 degrees, the laser spot is 6.3 mm off center.

Maybe the most serious consequence visually is that an error of type 1B may cause an error of type 1A, if the collimation is done to make the axes intersect at a point far from the focus. If we know this, we can avoid it. With the right tools, it is not difficult to collimate to within a small fraction of a degree.

Error type 2 - the optical axis strikes the secondary mirror at a point away from the optical center.

The secondary mirror has an elliptical surface with a major to minor axis ratio equal to the square root of 2, for 90 degree deflection. Depending on its size, it lets some of the focal plane be fully illuminated, that is any point within the area of full illumination sees the whole main mirror reflected in the secondary. Outside of this, some light is lost.

Due to the 45 degree tilt, the elliptic surface appears circular when you see it with your eye on the optical axis near the focus. However, due to the perspective, the center of the circle you see is offset from the center of the ellipse, towards the edge nearest to the focuser. To be optically centered, the secondary mirror must be offset both in the direction away from the focuser and towards the main mirror. The offset in each direction can be calculated with very complex formulae, but the formula offset=minor axis/(4*focal ratio) is accurate enough for practical purposes (it is exact if just the center is fully illuminated - with a larger fully illuminated field, the error is insignificant anyway). The distance along the mirror face from the center of the ellipse to the optical center is the offset multiplied by 1.414 (the square root of 2).

Example: with a 33 mm diagonal mirror (the size refers to the minor axis) in a f/6 Newtonian, the offset is 33/24 mm = 1.3 mm.

An error of type 2 causes the fully illuminated field to be offset relative to focus, and will cause an uneven light loss near the edge of the low power field. The tolerance should not be larger than the radius of the fully illuminated field, to ensure that the focus is fully illuminated. But at least for short focus instruments, light loss is very gradual outside the fully illuminated field, and an offset of a few millimeters should have little effect visually. Sufficient accuracy is easily achieved with suitable tools.

For wide-field photo, the whole film frame should be fully illuminated. This may require a diagonal size of 30% of the main mirror diameter, or even more. For visual use, a diagonal size of no more than 20-25 % is commonly preferred, in order to minimize unwanted diffraction effects. Here, a smaller area of full illumination is sufficient, but at least the focus should always be fully illuminated. If you design your own telescope, use a "low-profile" focuser to let the focus, and the eyepiece, come close to the tube (but an extremely low focuser can cause problems with baffling against stray light).

To calculate the diagonal size or the size of the fully illuminated field: let D be the diameter of the main mirror, d the diameter (minor axis) of the secondary, F the focal length, b the distance from the optical center of the secondary to the focus, and x the diameter of the fully illuminated field: x = (Fd-Db)/(F-b) or d = x + b(D-x)/F

Error type 3 - the combined optical axis is not reflected at 90 degrees. Standard secondary mirrors and holders are designed for 90 degree reflection, and seen from the focus the elliptical mirror appears circular. An angle of more or less than 90 degrees will make it appear elliptical, and may also cause vignetting (i.e. blocking some of the light) by parts of its holder. If you have collimated, and look at the reflection of the secondary mirror, its holder should appear on-axis and you should not see its side. If you can, and it appears "tilted", you should consider shimming or otherwise "squaring" the focuser. An error of type 3 will have no other effects on the image (contrary to common belief).

Error type 4 - the optical axis is not centered in the tube. If it is grossly off center, the tube opening may cause some vignetting, and this should be avoided. Otherwise, it will have no optical effect. It may cause problems with some mounts, as an offset axis will not trace a great circle when the tube is moved in declination. This might introduce some error when using digital setting circles.

End of heavy theory - at least most of it.

So what steps do I take to collimate my telescope?

The lining up of the optical components should be done in a sequence that is as simple and ordered as possible. Ideally, you would start at one end of the optical chain and then proceed in steps to the other, without going back to readjust what once was adjusted. With real telescopes this is not possible, the adjustments affect each other in different ways depending on design details. For instance, with common secondary supports, it is not possible to adjust the tilt without moving the optical center significantly.

One practical way is to do it in the order described below (you could do it in the opposite order, but I believe it is much more complicated). Remember that this refers to a full collimation, like when you assemble the telescope from parts - you do not have to go through all of this just to get your telescope ready for the night's observing! Step 5 (and maybe step 8) is usually quite sufficient for this.

The tools will be described in a later section, with details of their use. The error numbers are explained in the section on theory, that you may have skipped.

1 - Square the focuser

If the focuser appears to be squarely mounted on the tube, it is not likely to be badly off. If you make your own telescope tube, you can make a small mark directly opposite the focuser hole. With the secondary mirror out of place, use a sighting device in the focuser. Shim the focuser to center the mark. A piece of tubing that fits your focuser, long enough to reach across the tube, will make it even easier, and so will a laser collimator or a crosshairs sight tube. (This minimizes error type 3)

2 - Center the secondary mirror in the tube

You should offset the secondary mirror from the center of the tube, away from the focuser. Calculate the offset, and use a ruler, or else wait and adjust after step 6 is done. (If you cannot offset the secondary, e.g. because of the spider design, you may leave it centered, without serious consequences.) (This minimizes error type 4)

3 - Center the secondary mirror along the tube, as seen from the center of outer rays (this is the point where the main mirror appears to exactly fill the face of the secondary!). As previously explained, the secondary mirror should be offset both away from the focuser (this was done in the previous step) and towards the main mirror (but since it appears centered only when correctly offset, this is automatically taken care of in this step!).

You can center it in a simple or combination sight tube, as described below. You may also use a crosshairs sight tube or a laser collimator to do this, but then you need a spot at the optical center - or a holographic laser collimator. If you find that the secondary is offset "sideways", away from the tube axis, you may have to go back to either step 1 and shim the focuser sideways, or to step 2 and adjust the spider setscrews. (This minimizes error type 2)

4 - Tilt the secondary mirror to make the extended optical axis hit the center of the main mirror .

Use the appropriate setscrews on the secondary mount - depending on the design, you may also rotate the secondary holder to center "sideways". You can use a laser collimator by making the laser beam hit the center spot, or a crosshairs sight tube, by centering the spot on the crosshairs.You could also use a simple or combination sight tube, by centering the main mirror within the sight tube end (this is what you must do if you don't have a center spot).

If you can rotate the secondary, you could get it skewed by tilting it one way, and rotating it the other. If you see the secondary or its reflection looking skewed, try straightening it up, then rotate it to get the main mirror roughly in line. Then start over with this step, but do not rotate.

If you have made significant adjustments, go back to step 3 (and possibly step 2) and check that the adjustments still are OK, or adjust if needed.

If the main mirror is poorly adjusted, part of its edge may be obscured by the tube opening. If this makes centering difficult, go forward to step 5, and make a coarse adjustment before going back to step 4 again. (This minimizes error type 1B.)

Going forward from here, do not skip step 5!

5 - Tilt the main mirror, to make its optical axis reflect back on itself.

If you have a mirror cell that holds the mirror very loosely (this is particularly common in Dobsonians), you may make the mirror settle by tilting the tube nearly horizontally, and then raise it vertically, before you go on.

Here you use the set screws to adjust its tilt (use 2 to adjust, and leave the 3rd), and thus the tilt of its optical axis. You could use a Cheshire or a combination tube, by centering the main mirror spot in the bright spot of the Cheshire (if you use the calibrated Cheshire, you will know that the error type 1A is within tolerances, when the black spot is completely inside the bright spot). You may even use a peephole with a semi-transparent lid as a primitive Cheshire, if you illuminate it from the outside.

If you can reach to adjust the collimating screws while looking into the Cheshire, this simplifies things enormously! I have built my own telescopes so that I can, but with most commercial telescopes, this is not possible. The next best thing is an assistant that you can ask to turn each screw in each direction while you note the effects. A simple trick is to put a sticker near the focuser, where you draw two arrows to mark the direction that the spot appears to move when you turn each screw inwards - this way, it is easier to decide what screw to turn in what direction.

You can use a laser collimator (and a perforated center spot!) to get close, but as the precision is limited, fine tune by using a Cheshire, or star collimate (see step 7) for the final adjustment.

If you have no center spot, you can use a double crosshairs tube - see here how.

(this step minimizes the critical error 1A)

6 - Check the centering of the optical axis in the telescope tube and in the focuser drawtube.

A coarse test is to look through the empty focuser tube and check if you can see the outer tube end reflected in the main mirror from any point within the focuser. If you can't, the centering is OK optically.

If you have reason to do better, you can make a centering mask, and check with a peephole (or Cheshire or sight tube) whether it is well centered relative to the main mirror. If it is outside of tolerances, move the spider the required amount away from the visible part of the centering mask (put your finger inside the tube opening to see which direction it is), and start over from step 3. (This checks error type 4)

7 - Star test

The whole purpose of collimating is to get the best images of stars, and other celestial objects. You may want to check the collimation by looking at stars - use a magnification of 1-2x per mm of aperture (25-50x per inch). Also, do trust this step unless the seeing is quite good.

Center a star in your field of view (the centering is important! You may use Polaris if you live far enough North and have a telescope with no tracking facilities). Gently rack the focuser from one side of focus, passing the focus, going to the other side. What you will see if collimation is perfect and the air is very still is shown in these images (computer simulations by Harold R Suiter, author of Star Testing Astronomical Telescopes - note that the center image is highly magnified relative to the others). If you can work the collimating screws while looking in the eyepiece, fine - else find an assistant to work the screws by your commands. Doing it all alone can be frustrating.

When you are only slightly outside focus, you should see rings of light and a darker center, very symmetric (the images above are for an offset secondary mirror!). If there is a marked asymmetry, try and see if the image improves if you place it off center in any direction. If so, try to tweak the main mirror to move the image towards the center of the field, in steps until it looks symmetric ( If you start with a nearly perfect collimation, it will save you a lot of tweaking).

It is possible that the optical center of the main mirror is not at its mechanical center. If you star collimate and afterwards find that the center spot is consistently offset in the Cheshire, this is no doubt the reason. If so, first star collimate, then move the spot to appear centered in the Cheshire (or at least remember how far it is off, and in what direction). Once this is done, the Cheshire should give consistently good collimation.

8 - Check the finder and adjust if necessary

If you have tweaked the collimation, you may have shifted the optical axis slightly, and the finder is no longer accurately adjusted.

If your telescope is new, or if you have moved the spider, you can check that the spider vanes have not been tilted or twisted during collimation. Look down the tube and move your eye to see each vane look its thinnest, and check that you see it centered against the mirror (if the vane is centered - otherwise, check that you see it over the corresponding part of the mirror). If offsetting the secondary mirror makes the vanes slightly out of line, or out of perpendicular, this may make the diffraction spikes look less distinct or pretty, but it does not affect the sharpness or contrast of the image.

You can also check that the collimation holds at elevations from some 20 degrees to zenith (some main mirror mounts, where the mirror isn't glued or clamped, will not hold the mirror firmly enough to use all the way down to the horizon). If the collimation cannot be kept within tolerances, there is some weakness in the tube. It may be the main mirror support, but it may also be the spider or the secondary mirror mount that is not rigid enough.

Does this procedure give offset, or non-offset, collimation?

It seems that there are widespread misconceptions about secondary offset, or at least different ideas about what it should mean.

If you dot the geometric center of the secondary mirror face, and center this dot in the focuser (using a crosshairs sight tube or a laser collimator) and also center it inside the tube, you will get a truly non-offset secondary. This has been recommended, but it will give an error (usually acceptable) of type 2, and I don't see that it would be simpler, or offer any other practical advantage.

If you have optically centered the secondary in a sight tube as described above (step 3), it will be correctly offset along the tube. But what happens if your secondary is centered within the tube, without offset away from the focuser in step 2? This is sometimes called "non-offset collimation", or "neither centered, nor offset, but a compromise" (Menard/D'Auria: Perspectives on collimation).

Once the point is set where the focuser axis hits the secondary (be it at the optical or mechanical center, or any other point), the further collimation of the main mirror ensures that the combined optical axis will return to hit the secondary at that very point again. Thus, if the optical axis hits the optical center of the secondary, but it is the geometric center that is centered within the tube, it means that the optical axis will be offset from the tube axis - an error type 4 (it may also lead to some small error type 3). But since the offset is typically only 0.5-1.5% of the aperture, the error is of little significance. Thus, if the design of the spider is such that you cannot easily offset the secondary, you may leave it centered in the tube with no serious effects.

What tools can I use to make the collimation easy and accurate?

Here are some useful tools. You can make some (or all) of them yourself, see the DIY section (or follow the links) for details. Some of my designs there allow full control of tolerances - you can see immediately whether or not your collimation is within the accepted limits.

Tectron makes a set of 3 tools: crosshairs sight tube, Cheshire and autocollimator. Orion makes a combination tool (Cheshire + crosshairs sight tube). I have no personal experience with these. Several manufacturers make laser collimators. Whether you prefer a laser or a sight tube, a Cheshire is also helpful.

The main mirror center spot.

This is a small (but not too small) circle (square or even triangle is OK, too) of tape or paint placed in the center of the mirror - it is invaluable. Please note that it is always in the shadow of the secondary mirror, and does not interfere with the image. Regrettably, manufacturers often omit it, and if your mirror doesn't have one, I recommend you make one.

Hey - it isn't even my own `scope and anyway I wouldn't dare take it to pieces and risk putting my fingerprints all over the mirror - isn't there another way?

Yes, I have a solution - not quite as neat as if you have a spot, but it will do the job. Breathe again.

Should I center spot my secondary mirror?

Unlike the spot on the main mirror, a spot on the secondary could affect the image - and even obscure the main mirror center spot. I suggest you don't (unless you have a compelling reason).

The peephole

This is a small cap that fits in the focuser, with a small center hole (1-2 mm or so) to look through. It is easy to make one. You can adjust the collimation to make the following appear concentric (from outside in):

The eyeball centering (commonly described in handbooks) can be done with a peephole tube, but the precision is low and you have no control of the tolerances (that are more critical for short-focus optics). A semi-transparent peephole cap may be used as a Cheshire substitute (see later) in step 5, and with care and luck, the result may be good enough - and a lot better than if you did not try at all.

It is even possible to do this entirely without tools - you just hold your eye near the focuser drawtube, as well centered as you can. You might line up things more or less, but you are unlikely (more so, the "faster" your telescope is) to get the centering of the spot accurately enough (error 1A), so at least use a peephole when tweaking the main mirror - or use star collimating to fine tune.

If the secondary mirror is correctly offset towards the main mirror, it will appear centered when seen from a point near focus - but if you move your eye far away from focus, you will no longer see it centered. If you have the secondary mirror truly non-offset, it will appear to be offset away from the main mirror, but instead its reflection is centered.

The simple sight tube

This is a piece of tube with a peephole cap. To center the secondary mirror, the length is not very critical. If the length is close to the inner diameter of the tube times the focal ratio of your telescope, you could also center the main mirror within the inner opening of the tube. Here is how to make one.

You cannot, of course, see the inner opening and the mirror edges perfectly sharp at the same time, but the small peephole will improve your "depth of focus" and keep the unsharpness tolerably low.

To center the secondary mirror (step 3) you can hold a strip of white paper (or a piece of cardboard) inside the tube, below the secondary mirror (with a truss tube, you can use the lid of the mirror box!). You see the whole of the secondary face reflecting the white paper - without it, the outer rim of the secondary will reflect the dark inside of the telescope tube around the main mirror, and what you see is the edge of the main, not the secondary, mirror. Pull the tube in or out to make the secondary appear barely smaller than the tube opening, and lock it with the focuser locking screw. Move the secondary (try to avoid changing the tilt) to center it accurately - or at least to within acceptable tolerances. To center it "sideways", you may have to move the spider vanes - if this is not possible, shim the focuser sideways instead.

To center the main mirror (step 4), take away the paper strip (or take the lid off the mirror box) and push in the tube enough to see the main mirror reflected within the secondary. Tilt the secondary (try to avoid moving it) to center the main mirror inside the tube opening, just as you centered the secondary.

To aid in checking tolerances, you could put small protrusions inside the tube at its inner end (I have used strips made from the tubing, 2 mm high and slightly wider and longer). These act as tolerance gauges - if you divide the height by the tube length you get the angle in radians (multiply by 57.3 to get degrees) that the gauge is seen by. My f/6 tube is 168 mm long and the gauge is 2 mm high, the angle is 0.68 degrees (appr 2/3 degrees). If I have centered as shown above, and the black rim is almost gone at one side and as high as the gauge at the other, then the error type 1B is half of the angle, or 1/3 degree - I believe this is a very small error for visual use.

To judge the centering of the secondary, you can multiply the gauge height by the ratio (secondary size)/(inner diameter of peephole tube). If secondary size is 84 mm and inner diameter of tube is 28 mm, errors should be multiplied by 84/28=3.0. In the illustration above, error is half the gauge height times the multiplication factor - that is ½*2*3 mm=3 mm.

On some telescopes, it may not be possible to center the mirrors as described. If the focuser is high and the focus is far from the tube and/or the secondary is too small, you cannot see the edge of the main mirror inside the edge of the secondary.

On the other hand, if the drawtube is too long and/or the secondary is too big, you cannot see the edge of the secondary to center it. In both these cases the basic design is flawed (unfortunately this is rumored to happen sometimes with commercial telescopes), and if you are an Amateur Telescope Modifier you might consider modifying it. Otherwise, you may use a crosshairs tube as described below - your telescope may give a very good performance, nonetheless.

The crosshairs sight tube

This is a peephole tube with crosshairs at the inner end, for centering the optical parts. Here is how to make one. A single cross is fine for aiming at the main mirror center spot in step 4 (this works even if you can't see the rim of the main mirror). You can also use it in step 3 to center the secondary, if there is a spot at its optical center. This works with a focuser drawtube that is too long to show the edge of the secondary mirror with a simple sight tube. It is also useful in step 1.

A sight tube of the right length to center the main mirror in the inner opening (see simple sight tube) and with an accurately centered double cross can be used at the critical step 5 to collimate a telescope that (for any reason) does not have a center spot on the main mirror. Center the mirror within the inner opening as carefully as possible (step 4), and then adjust the main mirror to make the reflection of the crosshairs centered within the crosshairs themselves (step 5) - you may have to illuminate the crosshairs from within the tube using a flashlight:

The Cheshire eyepiece

This is a development of the simple peephole tube, with an illuminated face (white or shiny) set at 45 degrees. A hole in the side of the tube lets in daylight (or suitable night light) to make the reflection of the center spot visible against the bright face. There may be a "field stop" to define better the edge of the bright area. Here is how to make one.

The Cheshire eyepiece is used in step 5 (see above) to minimize the type 1A error: collimation (usually of the main mirror) is tweaked to make the spot appear centered in the bright area.

The combination sight tube

This is simply a peephole with the eye end rebuilt as a Cheshire - either cut it to size like a simple sight tube, or with crosshairs at the opening, or both. I prefer a home-made combination (as in the image below, cut to the appropriate f/ ratio - if you buy one, it is likely a one-size-fits-all, with crosshairs), as it can adequately handle the important steps 3, 4 and 5.

The laser collimator

WARNING: Never look at any laser beam directly! Normally, the beam will stay within the optical path of the telescope, but if it is badly out of collimation, the returning beam may escape beside the secondary. Do not look down the tube if you don't see it return as expected - instead, try picking it up on a piece of paper in front of the tube.

This is a solid state laser, mounted in a tube to fit the eyepiece holder, and critically collimated to make the laser beam centered in (1A) and parallel to (1B) the tube. The "inner" end has a bright face where you can see the spot of the returning beam, with a small hole for it to exit. It can be used in steps 1, 3, 4 and, with reservations, step 5.

The laser collimator can be expensive and impressive, and favored by many. It makes step 4 very simple, as you can stand by the tube opening and easily see where the beam hits the main mirror while you adjust the screws on the secondary holder. Seeing where the beam returns can be harder, particularly if the returning beam has been focused by the main mirror to make the spot smaller than the exit hole.

Some laser collimators are sold with holographic attachments, that project a reticle that covers a fairly wide angle. This helps in step 3, where you can see the centering of the reticle on the secondary, and possibly also step 4 and 6.

Potential problem using a laser to collimate the main mirror:

After step 4, if the laser beam is off the main mirror center, the return beam will be parallel to the optical axis, but displaced (by the same amount) at the return. If you then adjust the main mirror to center the return beam accurately, you unwittingly miscollimate and get a 1A error (of half the displacement)! For instance, the strict tolerance for a f/4.5 mirror is only some 1/3 mmor 1/64 in., so the allowable error in step 4 should be much less (than 2/3 mm or 1/32"). With many telescopes, it is not really possible to read the position of the spot (or even adjust the secondary holder) to anywhere near the required precision. On the other hand, if you allow a type 1B error of 0.2 degree (assuming a 70" = 1.8 m focal length), the spot can be 1/4" or 6 mm off!

For this reason, if you collimate step 5 with a laser, you should check with a Cheshire or star test that the collimation is acceptable, or else tweak it - but in the section on Experimenting, I have described a workaround!

You can make your own laser collimator from a cheap keychain laser pointer.

The autocollimator

The name may suggest that this is a device that will automatically collimate your telescope - sorry, it won't. It is another development of the simple peephole tube, with a mirror inside the cap. There is a transparent spot in the center of the mirror, used as a peephole, and the mirror is set accurately perpendicular to the tube (there are other devices called "autocollimator" too - if you search the net for more info, don't be confused).

It is used (after step 5) to check the alignment of both mirrors. If the main mirror is accurately perpendicular to the axis of the autocollimator, what you will see in the peephole is your own eye pupil reflected, and infinitely magnified, via the secondary - primary - secondary - autocollimator - secondary - primary - secondary mirrors.. That is, the autocollimator mirror appears entirely black. Otherwise, you can see reflected light from the bright sky/ceiling via multiple reflections. However, the autocollimator, like a laser, does not distinguish between type 1A and 1B errors - a "black" reading means nothing unless the Cheshire shows the main mirror spot is centered within tolerances. It can help you to get the relatively unimportant 1B error vanishingly small (although a laser collimator is far more convenient for this), but it does not detect the crucial 1A error (that still must be determined with the Cheshire) - in particular, if you do a laser collimation and make the beam return, the autocollimator will go black regardless of where the beam hits the main mirror (or else the focuser is likely at fault), and in this situation it will not detect even a gross 1A error.

The finer details of using the autocollimator are given in the booklet "Perspectives on collimation" by Vic Menard and Tippy D'Auria (the authors do not distinguish between the errors called 1A and 1B here, and make no attempt at analyzing the tolerances involved). If you make one yourself, make sure the mirror is very well squared to the tube. I would not recommend its use (with one exception - you can make a simple but possibly useful autocollimator for wide-field photo).

The centering mask

Take a piece of paper or semi-transparent plastic, large enough to fit over your tube opening. Make a circle exactly as large as your main mirror, and center it over the tube opening. This is useful in step 6 above, when you want to check the centering of the optical axis within the tube. If you have decided on a maximum allowable error, multiply it by 2 and draw a circle so far outside the first circle (if you like, you can cut a hole inside the first circle). Look inside the sight tube (any kind) - if you can see the inner circle or cutout, the optical axis is not exactly centered, but as long as you cannot see the outer circle, the error is acceptable.

Is this the end of the FAQ?

Yes, unless you want to go to the separate section about some special situations and the DIY projects - you may have followed some links already.

Special situations are:

Thank you for staying with me so far - I hope you feel it has been worth your while and that you notice the difference, now that your telescope is well collimated. If not, deliberately miscollimate step 5 to make the error fall outside tolerances. Try it on a night with good seeing and see what it does to the image, particularly of planet details.
Nils Olof Carlin ( nilsolof.carlin@telia.com) - comments are welcome

With special thanks to Mel Bartels for his help in making this available on the net, and to Ken and Mike for maintaining the ATM site where this is mirrored.