Why aren't my stars round?

How to figure out what is wrong with your telescope when the stars appear distorted

All images and text Copyright Mike Lockwood, 2013



So you've had a telescope for a while, or just gotten a new one, and you notice consistent or inconsistent distortion in the star images.  To put it another way, stars aren't round in the eyepiece inside or outside of focus, or maybe even at best focus.  This may be intermittent, or may always be the case.  How do you figure out the source of the distortion?  I hope this article is helpful in leading you down a path that will lead to an explanation.

There are many possible causes of distorted, non-circular star shapes.  
You may even be seeing more than one distortion on top of another one or two!  This can make deciphering the puzzle a bit difficult, but hopefully this article will allow you to identify one fairly easily, and this will then allow you to track down the other.

In order for this article to make sense, first we have to set some ground rules and satisfy a few conditions before we can move into diagnosis of the problem(s).

First condition:  For all of the advice to follow, please put the star in the center of the field of view and keep it there.  This is important for determining if the issue is due to collimation, and reduces the chance of some other eyepiece or corrector aberration being confused with another issue.

Second condition:  Before you do anything else, determine if you have astigmatism in your eyes.  This is fairly simple - if you turn your head, astigmatism in star images that is caused by astigmatism in your eyes will rotate with your head.  You may even already know from your eye doctor that you have astigmatism.  However, if you don't rule out this problem first, you may drive yourself crazy trying to figure out what is going on!

Third condition:  Next, take a look at what power you are using - if it is fairly low, the distortion may be coming from the pupil of your own eye vignetting the light cone.  Move your eye side to side while looking at a focused and defocused star - if the shape changes or the secondary shadow appears to move around, your own pupil is blocking some of the light and may be causing the strange shape you are seeing.  In this case, raise the power and/or get more dark adapted so your pupil is larger and does not block the light cone.  If you are already using high power, you may wish to try low power to see this effect for yourself and know what it looks like.

Fourth condition:  If it's early in the evening, understand that your mirror will likely be cooling off, and strange things can happen.  Air currents can form, cooling parts of the mirror faster than others.  A breeze can set up asymmetric airflow in the telescope's tube or mirror box, also cooling some of the mirror faster than the rest.  Both of these are a recipe for strange star shapes that go away after a bit of cooling.  This goes for the primary mirror and/or the secondary, especially if it's fairly large.

Fifth condition:  For this article, we are assuming that your mirror cell is properly designed and set up, including the edge support of the mirror.  If your optics are glued to the cell, then you cannot easily rotate them to help rule out some possible causes of non-round stars.  Gluing a mirror (other than a small secondary) to a cell made of something other than glass will often cause it to warp as the cell shrinks by a different amount and pulls on the mirror, creating optical problems.  I do not recommend gluing large mirrors to their cells/holders, as it will often cause non-round stars.  If your primary mirror and or large secondary mirror is glued to something, I recommend finding a way to mount it without glue, and then coming back to this article if problems remain.

Now, understanding the possibilities given above, let's begin.

What is astigmatism?

Astigmatism is an optical aberration.  Mirrors with astigmatism produce oval-shaped, or in terrible cases, line-shaped stars!  The oval or line rotates 90 degrees as the eyepiece is moved to the other side of focus.  In mild cases, stars still generally appear round at focus, though diffraction rings, if they are visible, may appear distorted.  In severe cases, the star will appear cross-shaped at focus.

Collimation and coma in a Newtonian telescope

By far the most common reason for non-round stars in a Newtonian telescope is poor collimation.  This produces an optical abberation called coma.  So, we'll discuss this first, then move on other less common causes.

1) NOTE:  IF YOU SPEND AN HOUR OR TWO LEARNING THE COLLIMATION TECHNIQUE DESCRIBED BELOW, YOU MAY IMPROVE YOUR TELESCOPE'S IMAGES GREATLY WITHOUT HAVING TO SPEND A CENT ON NEW COLLIMATION TOOLS.  You will also have a sharper eye for collimation than most other observers.

2) NOTE:  Lasers can easily go out of alignment, and this will seriously throw off telescope collimation.  Put your laser in the focuser and push the top of the laser against the top of the focuser.  I don't usually tighten the thumbscrews, because they often tilt the laser within the focuser.  Now rotate the laser in the focuser (you can also do this in a v-block).  If the laser spot moves in a circular path on the mirror, then the laser needs to be aligned.  Consult a knowledgeable astronomer or the manufacturer to get help with this.

3) NOTE:  Using only collimation tools - laser, barlowed laser, cheshire, autocollimator, etc., I almost never achieve perfect collimation.  That is, I can almost always detect some coma in a star image using the technique described below.  So, I always finish up collimation using a star image, and that is what I will describe here.

First, go through your normal collimation procedure, paying particular attention to making the secondary mirror alignment as close to perfect as you can get it.  If you need help with this, seek help elsewhere or from a friend.  If you can nail the secondary alignment, t
he instructions below will then help you get close to perfect primary collimation.

Second, with a coma corrector in the focuser if the telescope is f/5 or below, and a fairly high-power eyepiece in it, put a star in the center of the field of view and keep it there using a drive or by hand-tracking.

Defocus the star slightly inside then outside of focus.  Not the star shape.  Let's say the star appears to "bulge" on one side on the inside of focus, and the "bulge" is still on the same side as you look at the image outside of focus.  In this case, you are likely seeing an issue with collimation that needs to be addressed by tilting one of the mirrors.  Pinched optics, or other distortions of the mirrors will usually "flip" on the other side of focus.

If stars appear comet-shaped (a bright point near one corner with a tail, somewhat triangular), this is almost certainly an aberration called coma that is normal in mis-collimated Newtonians.  With no coma corrector in place, a star placed precisely in the center of the eyepiece's field of view should appear round.  This is because a Newtonian telescope will produce a perfectly round star image at the center of the field if it is collimated properly.  However, if the aim of the telescope (without coma corrector) is adjusted so that the star is moved to the right of the center of the field of view, you will see the star start to bulge or it may appear to grow a tail that points toward the right.   Likewise, on the left of the center of the field of view, the bulge or tail will point to the left.  In fact, no matter where the star is, the bulge/tail will always point away from the center of the field, except at the center of the field, where the tail does not exist.

If you don't know what coma looks like, it may be a good idea to remove the coma corrector, put in a high-quality eyepiece, move the star around the field, and see coma for yourself.

Putting a coma corrector in the focuser will help correct the coma IF the telescope is collimated properly.  So, with a corrector now in the focuser, if the aim of the telescope is again adjusted so that the star is to the right of the center of the field of view, the star will still appear mostly round, and will either not grow a tail or not grow nearly as large of a tail as it did when there was no corrector being used.  This is because the coma corrector is reducing or eliminating the coma.

But here is another important point - if the primary mirror is not collimated properly, residual coma due to mis-collimation will still be seen even with the coma corrector in the focuser.  For the collimation method I describe below, I actually recommend leaving the coma corrector in the focuser, because the coma due to mis-collimation can still be seen.

The above observations and information lead to a collimation method I have used for years:  With the star centered in the eyepiece and a coma corrector in the focuser, observe the shape of the star in focus.  It should be fairly round.  (If not, read the rest of this article.)  Now defocus the star very slightly.  We're not talking much, just enough to expand the star slightly - a fraction of a turn on a fine-focus knob.  When you do this, you may see an obvious tail grow, indicating significant coma.  In that case, you have a lot of coma, so skip the paragraph below and follow the directions in the next one.

If coma is not obvious, don't just look at the shape of the star after you defocus it - observe how the star expands.  That is, as you just barely start to defocus the star, watch to see if the star image expands first in a particular direction, or "bulges" in that direction.  In doing this, we're looking to see HOW the star expands, not what it looks like when it's expanded.  It is subtle at first, but more obvious with practice.  Doing this very close to focus increases the sensitivity of the test.

To help with this, note the location of the star at best focus, and stare at that spot.  Now defocus inside of focus and see if the star simply expands in all directions at once, or if it "bulges" or "pulls" in one direction, expanding off-center.  Repeat going outside of focus.  If you see the bulge in the same direction as going inside of focus, repeat by defocusing in both directions a few more times to confirm that it is consistent and is not a strange air current or moment of bad seeing.  If it is consistent, chances are it is coma.

Now, if you see coma, either a lot of it or a little, use the primary's collimation adjustments to move the star toward the tail of the coma or the bulge.  This may easier if you have a friend helping you by turning the collimation bolts.  
Using the primary's collimation adjustments to move the star tilts the mirror so that the optical axis (the spot where a star will appear round even with no coma corrector being used) gets closer to the center of the field of view of the eyepiece.  By making successive adjustments, you can put the coma-free spot in the center of the eyepiece's field.

NOTE:  If you are working alone, I recommend first turning each bolt in both directions and making a "map" of how each one moves the star in the eyepiece.  Then you can be sure of turning the right bolts to move the star where you need it.

Keep making adjustments until the star expands uniformly in all directions, and does not "bulge" or "pull" in one direction.  At this point your telescope will be fairly well collimated in terms of the primary's tilt, and you're ready to observe.  Check collimation by this method throughout the night to see if it drifts, and tweak if necessary.  It is important to note that the collimation of the telescope may shift subtly or obviously as the scope is used throughout the night and/or as it is moved up and down in altitude.  These adjustments may be required more than once each night to ensure optimal telescope performance.

If you master this collimation technique, please tell your friends where you saw it, and teach it to someone else.

Pinched optics

Pinched optics means that the mirror is being squeezed by something.  Generally, since three points can locate a mirror laterally, the effect of the "tightest" three screws are what is seen, and that means a three-sided shape is created by the mechanical distortion, which of course is a triangle.  However, by squeezing the mirror on two opposite sides, I have seen highly astigmatic images created by pinched optics.

Pinched optics have to be pretty bad to make a star look like a triangle, but it happens!  More than likely you will only see a hint of triangularity over a basically circular shape.  Chances are that it is being cause by an optic that was pinched during manufacturing or that is being pinched in the telescope.  While it may seem minor, you will want to track it down because it may become worse at various temperatures, since metal and glass expand at different rates, and the glass may be more severely pinched at temperature extremes.

First, inspect the mounting of the primary mirror.  All clips and other retaining screws should not contact the mirror, but they should come close.  If you find a screw tightened against the mirror, even a small amount, back it off and re-test.  You should be able to "rattle" the primary in the cell.  It should not be "snug" in the cell, it should be slightly loose in all directions.

If no optics appear to be pinched, then rotate the primary.  If the "points" of the triangle rotate with the mirror, chance are the mirror was pinched during manufacturing.  In this case, let the mirror cool after it is rotated and observe the star shape an hour or two later.  If the points of the triangle go back to the original orientation, then the triangularity is likely being cause by cooling, such as by three fans or three ventilation holes.

If the distortion does not rotate with the mirror, then it is possible that the primary mirror's cell is distorting it.  If the issue is poor edge support, then the problem will likely disappear if you point the telescope straight up and ensure that the primary is not "stuck" against the edge supports.  Giving the scope a quick shake (thereby "rattling" the mirror in its cell) will often cure that.  Moving the scope back down near the horizon would then cause the problem to return.

Often mirror cells have only three edge supports, and if the mirror is heavy enough, it can effectively become wedged between the two bottom supports when the telescope is pointed low, and this squeezes the mirror.  (If the mirror is 10" or larger, I don't recommend a three-edge-support cell.)  This will cause triangular star images and/or astigmatism as the telescope is pointed low in altitude, and it may improve if the scope is pointed high.  The mirror may also get "stuck" a little bit and may remain pinched until it is "rattled" in its cell.

Some mirror cells may actually pinch the mirror from time to time, due to friction/stiction.  That is, if the mirror sits on the cell for a long time, some of the contact points (plastic, fellt, cork) may actually adhere to the mirror.  The solution is simply to move the mirror in the cell, or rotate it slightly, just enough to break the stiction, and get it "un-stuck".  This may result in a significant improvement in the star test, and I have seen it cure a major problem in a couple of cases.

It is possible to have the secondary cause triangular distortion, but it is not common.  As a last resort, examine its mounting and see if it is being pinched.  Like all optics, it should be held gently.

Primary mirror astigmatism - polished in, and thermal

If you notice astigmatic star images, the first step is to note the orientation of the "ovals" on the inside and outside of focus.  Make sure that you record this with respect to the telescope's optical axis, and not the ground.  That is, note the orientation of the ovals and which side of focus you are on with respect to the tube of the telescope, not the ground.

Now, rotate the primary mirror.  If the astigmatism rotates with the mirror, then the primary mirror is causing the astigmatism.  HOWEVER, you must now observe the astigmatism over several hours to see if it changes or goes back to its original orientation.  If the astigmatism goes back to its previous orientation over time, then chance are that you are seeing THERMAL astigmatism, likely caused by unevenly cooling the mirror.

Thermal astigmatism may appear or disappear only on windy or still nights, so more than one evening of testing may be required.  If you see a pattern, look at how the cooling fans are positioned or the air flows through the mirror box due to wind.  Having only the bottom of the mirror box open at the back may cool the bottom half of the mirror more, causing uneven temperature.  Having fans in a line rather than distributed around the mirror is also a usual suspect.

In all cases, though, thermal astigmatism will appear to rotate with the primary at first, but then it will eventually change or go back to its original orientation.  If the astigmatism always follows the rotation of the primary on all nights and over many hours, it is being caused by the primary mirror itself.

One form of thermal distortion that does not rotate with the primary mirror is the effect of an air current.  It will typically distort one side of a star image, but the effects can range from minor to severe depending on the temperature differences involved.  It should be recognizable in out-of-focus star images as a slowly moving, distorted area on one side of the image.  In some cases, it may be much worse.  A closed tube will make it worse, and pulling up the shroud on a truss-tube dob may help alleviate it and aid in primary mirror cooling.

Mirror-cell induced astigmatism and bad secondary mirrors

Let's assume now that you have checked, and the astigmatism does not rotate with the primary mirror.

If the ovals (defocused star images) appear roughly aligned with the tube of the telescope, that is the oval on one side of focus is aligned with the tube and on the other side of focus it is perpendicular to the tube, then the likely culprits are a bad secondary mirror or the edge support of the primary mirror.

A bad secondary mirror will have a curve to its surface, and this cause astigmatism because it is mounted at a 45-degree angle.  The astigmatism should be fairly consistent for all telescope altitudes.

A mirror cell that is causing astigmatism usually has inadequate edge support, such as a bad sling or poorly selected contact points.  It will pinch the mirror with the sling or push at incorrect places on the edge, squeezing or bending the mirror.  The astigmatism should change with telescope altitude, and if you point the telescope straight up and give it a "good shake" to make sure the mirror isn't hung up on anything, then the astigmatism should all but disappear.

A properly-positioned cable sling should introduce a small amount of astigmatism in a primary mirror, but not a large amount.  If this is not the case, you should make sure the cable is positioned properly and that the mirror is not bumping into something else due to a slack cable.

If you have astigmatism that actually seems to get better as the telescope is pointed lower, then you may have a mirror cell with triangles or supports that are bound up.  I have seen this happen more than once.  Make sure the mirror is sitting on all of the support points, and that the triangles or pivots can move freely.

If, after adjusting the cell, rotating the primary, shaking the scope, or even giving the mirror box a good whack with your first, images suddently become good and stars round, you have freed something that was bound up.

Don't be surprised if the fix is as easy as bumping some part of the scope to free it up.  The moral of the story is this - you don't make stars round accidentally - you make them round by fixing problems.


Primary mirror strain-induced astigmatism

If the primary mirror is made from poorly annealed glass, it may have strain.  Strain is internal stress within the glass, and it is more likely to be found in cheap mirrors made from cheap glass.  When exposed to a temperature change, especially a rapid one such as bringing a scope outside into the cold, the mirror may go astigmatic.

The good news is, as the mirror temperature equalizes, the astigmatism should go away.  Additionally, the strain should rotate with the primary mirror and stay with its rotation over time as it slowly disappears.

However, if you like to observe shortly after bringing the telescope out, this is not good news.  You will be stuck with astigmatic images until the mirror cools sufficiently.

Poorly aligned focuser or corrector

The last cause of astigmatism that I have encountered is a poorly aligned focuser or corrector.  This can be a real problem for a faster telescopes (those with lower f#s) and when coma correctors are used.

If all other possible sources of astigmatism have been eliminated, check the squareness of the focuser and make sure that the eyepiece and coma corrector are in the focuser squarely.  One time I experienced a case where the setscrew of a focuser pushed the coma corrector of to one side and caused it to tilt slightly, introducing astigmatism and other aberrations into the images of an f/4 telescope.  I quickly fixed the problem.

As a last resort, try rotating the corrector and/or eyepiece in the focuser to see if the astigmatism rotates with either of those.  If it does, you have found your culprit.

Other thermal effects on optics

Now let's conclude this article by looking at one issue that involves round stars.  Thermal effects on optics aren't always of a nature that causes stars to be non-round - sometimes they affect the perceived correction of the optic.  Many people star test telescopes to help them determine the quality of their optics.  However, people often mistake the effect of dropping temperatures on the mirror for optical problems.

It is completely normal for a well-corrected, high-quality mirror to appear overcorrected while it cools.  This condition is indicated by obvious rings in the structure of a defocused star on the outside of focus, and indistinct rings on the inside of focus.  As the mirror approaches air temperature, this condition gradually goes away.

The reason for this is the fact that the mirror doesn't cool evenly - it cools faster near the edge of the mirror and wherever the miror is exposed to the cold sky above (obviously the front of the mirror is exposed to the sky) or to cooling breezes or fans.  The cooler areas physically shrink, changing the shape of the mirror, often resulting in perceived overcorrection.

For example, let's say the outer part of a 2"-thick mirror is one degree Celcius (1.8 deg F) cooler than the rest of the mirror.  The coefficient of thermal expansion of Pyrex/Supremax (borosilicate glass) is 3.25*10^-6 per degree C.  If we assume that the front of the mirror shrinks downward toward the center of the mirror and the back of the mirror shrinks upward toward the center of the mirror, then this means that we're interested in the dimensional change of a 1" thick piece of glass.

So, a one degree lower temperature in the outer part of the mirror means that the 1" of glass underneath the optical surface shrinks downward by 3.25 millionths of an inch, or about 1/7 wave on the glass, 2/7 wave on the wavefront.  This pulls down the outer part of the mirror, effectively overcorrecting it.  The effect is visible in a star test and looks like overcorrection.  It will affect images a bit.

A difference of two degrees C, or 3.6 degrees F, results in shrinking by 2/7 wave on the glass, or 4/7 wave on the wavefront.  This should be very easily visible in the star test, and the effect on images will be significant too.

For many decades it has been a common practice by some to leave mirrors undercorrected to help compensate for this, but that results in an inaccurate mirror when it gets close to equilibrium.  These mirrors are then undercorrected when optimal observing conditions are experienced, and will only perform optimally when cooling conditions exactly match the amount of undercorrection that is figured in, which will be quite rare.


It has been suggested by others in the past that insulating the edge of the mirror could reduce temperature imbalance within the glass, and may help reduce the temperature-induced overcorrection.  With the lower-quality "light bucket" optics of the past, the effect of insulating the edge may not have been noticeable or significant.  However, now that we are in a modern era that features more high-quality, large, fast mirrors, it may be time to try this.  I have not heard of anyone trying it recently, and I have not tried it myself since my 20" f/3 mirror is 1.25" thick, and the thermal effects are not as significant.

Finally, metal shrinks more than glass, so in some cases, a shrinking mirror cell can actually pull very slightly on a mirror.  This may also contribute to a perceived overcorrection.  Giving the mirror a "shake" may help in some situations.

Conclusion

This article has been many years in the making.  I've experienced all kinds of telescope problems including most of the conditions that I've described above.  I've also refined my collimation technique that I describe above so that I can always be assured of having good collimation that lets very fast mirrors perform at their best, and just as well as slower instruments.

So, the problems mentioned above can be very real, as are the solutions.  I've been filing them away in my memory, and it was finally time to put them into an article.  As an optician, it is also in my best interest to educate people on what can hurt or help the performance of telescope optics.  Quite honestly, educating telescope owners reduces the number of issues that I am blamed for, and allow their owners to fix them and enjoy the full potential of their often very expensive instruments.

I hope this article has helped you understand a bit more the behavior of telescope optics under realistic conditions.  I also hope that it has allowed you to improve your telescope's collimation, and has given you the skills to troubleshoot common problems with telescope optics.  If it has, please ask your friends to read it, and teach them what you have learned.

I wish you clear, dark skies, and round, tiny stars.

  -Mike Lockwood, Lockwood Custom Optics

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