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vlaiv

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Posts posted by vlaiv

  1. 1 hour ago, Neutrinosoup said:

    and WO FLT98mm than I want to sell because I rarely use it.

    Maybe you should try it first with ~40mm 2" eyepiece and a good 2" diagonal?

    But you really want to wait for autumn for that target. It can be very high in the sky - near zenith (depending on your location).

    For best results - wait for it to be near zenith and also check this website:

    https://atmosphere.copernicus.eu/charts/packages/cams/products/aerosol-forecasts

    This gives you forecast of transparency - you want "white" to be over your observing location for the evening you plan to observe. That is for best results of course.

    image.png.3fa070a8aa8b9942508e9ddad3681325.png

    Observing when dark gray is overhead is like observing with 8" telescope instead of 9" telescope - you loose one whole inch (going into yellow territory is even worse and can have effect of loosing 2" or more of aperture size!).

    • Like 2
  2. Very nice, but I think you have much more data in the image than it shows.

    You could bin the data as it is over sampled to help with SNR, but that is a side note - look at this bit:

    image.png.83cb22e5da33e4e36446eff83583ff4a.png

    That is Holmberg IX - irregular dwarf galaxy that is satellite galaxy of M81 - it is there in the data but can't be readily noticed in the image the way it's been processed.

    • Thanks 1
  3. 2 hours ago, Ratlet said:

    A 130mm F5 newt would be another winner for a wide field scope at a lower price.  Heritage 130p would do well but (I think) be limited to 1.25" eyepieces.  130pds would be more expensive and require a mount, but let you use 2" eyepieces.

    It has a downside though. Such scope has to have really big secondary to avoid vignetting on 2" eyepieces.

    If you do a little search, I'm sure you'll find someone posting a flat field of their 130PDS with APS-C sensor - and it will show vignetting even on 28mm diagonal.

    • Thanks 1
  4. 2 minutes ago, bosun21 said:

    Regarding the mirror quality being 1/6th wave or 1/10th wave lambda I always thought that this has nothing to do with the reflectivity of said mirror. I always thought of the lambda quality would be better for resolving the finer details of an image, ie a 1/10th wave is better than a 1/8th wave. The actual brightness of an image being directly related to the reflectivity of the mirror. Of course eyepieces and other factors will play a part in this. as well as the mirror coatings etc. Am I wrong in these assumptions?

    When observing at low power such as M31 requires - difference between 1/6th wave and 1/10th wave is non existent.

    Only very discerning observers will tell the difference on the nights of best seeing when observing planets at very high magnification.

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  5. I think that you'll benefit more from:

    - having a bit more experience in observing

    - choosing the right eyepiece

    - choosing the right night

    - choosing the right time of the year to observe M31

    than changing the scope.

    I managed to see first dust lane of M31 in 8" scope from Bortle 8 location on particularly transparent night when M31 was at zenith.

    • Like 4
  6. You can also reduce CA fairly easily (and cheaply) by using aperture mask.

    That will trade off some imaging time for reduction in CA, but results can be rather impressive. I'd start with 80mm mask - maybe do a comparison session when the moon is out and you won't be imaging otherwise - find a bright hot star, that way you won't need much exposure time to reveal CA and compare with / without mask results. Even better - make several masks and compare them all - like 90mm , 80mm, 75mm

     

    • Like 2
  7. 8 hours ago, Djukka_ said:

    I have one last question for you, since I now know something about this would you recommend me to buy  this one  https://teleskop.rs/reflektori-ota/117-150750-skywatcher-newton-tubus-sa-110-mikrofokuserom.html  (150/750 newtonian)

    or this one  https://teleskop.rs/refraktori-ota/763-72420-skywatcher-evostar-ed-apo-tubus.html (72/420 SkyWatcher Evostar ED apo) , I want your opinion on what would you buy if you were in my situation.
    And I also got a lot of recommendations for this 72ED apochromat  

    Well, I''m really not sure. I'm inclined to to recommend the smaller scope - 72ED one.

    It will simply be easier to use overall and the field of view difference is not that big anyway.

    I do have similar scopes on HEQ5, or rather one with short focal length - 80mm F/6 APO and one with very long focal length - RC8" F/8 scope, and they both work well and serve different purpose. RC8" is certainly not beginner scope and I had to modify the mount quite a bit to make it usable with such scope (belt mod, tuning, changed saddle plate, changed tripod for Berlebach planet and so on ...)

    Yes, go with 72ED and also get matching field flattener as you'll need it for APS-C sized sensor.

    8 hours ago, Djukka_ said:

    (Also if you could put a link to our local astronomy forum, didn't even know such a thing existed!!!😮)

    https://forum.astronomija.org.rs/

  8. 35 minutes ago, Djukka_ said:

    So you are telling me that its just a bit harder to shoot with newtonian, but are images taken from it still good? Or are they "low in detail"

    Question of how "clearly" you can shoot the object is very complex.

    There are a lot of variables that come into play, and quality of optics is not at the top of the list. In fact - it is probably one of the last ones if we consider importance.

    When we are talking about clarity of deep sky objects / long exposure astrophotography - following things are more important than quality of the optics:

    - how bad atmospheric seeing is

    - what is the precision of the tracking / guiding of your mount

    after those two come aprerture size and quality of the optics. Nowadays, most, if not all telescopes come with very decent quality optics. It's not premium, but most do have diffraction limited optics.

    Without going into too much detail, with D3200, you should really keep your focal length at about 500mm to get the sharpest image at 100% zoom level.

    This is why I said to use either refractor of about 400mm or reflector at about 600mm (650 + x0.9 coma corrector gives 585mm).

    45 minutes ago, Djukka_ said:

    I would rather pick newtonian if refractor will have galaxies like very small objects (if i zoom in detail will be worse anyway)+ the price of 550$ is cheap for refractor but ok for reflector

    Here is handy tool to help you visualize what sort of image you'll get:

    https://astronomy.tools/calculators/field_of_view/

    For example, let's look what M51 would look like imaged with these two different scopes:

    image.png.0830de3d9a5d1a9136c262ce9461f190.png

    As you can see - yellow rectangle is field of view with refractor and red is field of view with reflector. In both images this galaxy looks small. This is because your camera has 6000x4000 pixels (give or take), and for astrophotography - it is not so much the FOV as something called sampling rate - how much sky is covered with single pixel.

    For your conditions and skill level - this figure should be around 1.5 - 2"/px - which means that every pixel should roughly cover 1.5 arc seconds x 1.5 arc seconds of the sky. Depending on conditions - even this might not look sharp enough (poor seeing, or poor tracking).

    Formula for calculating this value is pixel_size * 206.3 / focal_length so for D3200 with pixel size of 3.84um each scope will give:

    3.84 * 206.3 / 420 = 1.89"/px for refractor

    3.84 * 206.3 / 585 = 1.35"/px for reflector

    Now, given that M51 has apparent size of some 12' x 7' and if you want to frame it right you can add another 10' around it so overall it will be something like 22' x 17' and that is 1320" x 1020" - that is apparent size in arc seconds.

    When we map this to pixels, for refractor you get:

    1320 / 1.89 = ~700px and 1020 / 1.89 = ~540px - so whole "interesting" image will be 700x540px

    and for reflector it will be

    1320 / 1.35 = ~980px by 1020 / 1.35 = ~755ox - or a bit larger at 980x755ox

    I know that this looks small - but that is what you can realistically get to look sharp. In fact - most amateurs are going to be limited to about 1"/px. Sky simply does not allow for finer detail, so you'll be already very close to that limit with 130PDS and your camera with 1.35"/px

    1 hour ago, Djukka_ said:

    what do you think about this and a coma corrector
    https://teleskop.rs/reflektori-ota/118-2001000-skywatcher-newton-tubus.html

    can I put my DSLR on it with a T ring or smth?

    I think that it is a good scope - but I would not recommend that to you.

    For imaging you want a stable platform. Larger scope is simply going to strain the mount more as it is heavier. It has larger cross section so wind will shake it more. It has almost the double the focal length - which translates into "empty' magnification with your camera (there are techniques to get around this, but are probably too advanced for beginner).

    If you really want a bit bigger scope - then get this one:

    https://teleskop.rs/reflektori-ota/117-150750-skywatcher-newton-tubus-sa-110-mikrofokuserom.html

    Just make sure you get PDS version of Skywatcher 150 newtonian and not regular, because PDS comes with dual speed focuser and larger secondary mirror and is aimed at astrphotography rather than visual.

    In any case - do keep in mind that you will likely want to start guiding at some point. Have a look at this:

    RA_vs_DEC.gif

    That is a "video" that I made with EQ mount (not sure which one, could have been HEQ5) - but it shows two important aspects of the EQ mount.

    First is polar alignment (PA for short) error and associated drift - in this video shown as drift from right to left, and second is periodic error (PE for short) of the mount - that is jumping up and down of the image.

    First one is caused by less then perfect polar alignment of the mount and second is inherent to the mount because of the way reduction works - it uses machined gears and those gears are not perfect in shape - they are a bit "egg" shaped due to manufacturing errors (very small errors but at telescope magnifications - it shows). Both of these limit your exposure time and if you expose for longer - you get star trails.

    You can even see some star trailing in the video as each frame was about 1 minute exposure with the mount.

    In order to avoid this and have round stars each exposure, and to be able to expose for longer - you really need to guide. Lack of guiding will really be the biggest source of blur in your images when you start in all but poorest seeing.

    I'm telling you that so you can choose between scopes - in essence, go for smaller scope that has shorter focal length and is lighter on the mount and save the money for guide camera and guide scope as you will need them soon enough.

    1 hour ago, Djukka_ said:

    PS: I saw you selling a telescope in like 2012 or smth, but i saw it on a site like a year ago and i remember your profile picture. What a coincidence. + we are both from Serbia :D

    Yep :D

    I'm also active on our local astronomy forum

    • Like 1
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  9. 9 minutes ago, Elp said:

    But the person mentioned they were using a mono camera...

    Yes, that is why all of the above is relevant.

    - if using mono camera on less than well corrected scope - you will still shoot all the wavelengths at the same time - much like OSC is doing and some of those wavelengths will be out of focus - creating blur. This is why you are limited to LRGB type of imaging (LRGB filters with mono, but using only R, G and B filters - each with their focus position).

    - even if you do that - there is a chance that one channel will be not be well corrected if scope is not well corrected. Usually that is blue channel as it contains shortest wavelengths - those are bent the most by refraction. Then there is spherochromatism - or fact that not all wavelengths of light have good spherical correction.

    You can identify such situation from following graph:

    tsapo150f8-lsa-1000.jpg

    This is ED scope 150 F/8 - but it shows what needs to be seen nicely.

    On X axis - we plot defocus - or how much you have to move focal plane for particular point to be in focus. On Y axis - we have distance from optical center to edge of the lens. If you look above graph for say yellow line (620nm wavelength), at very bottom of the graph (center of lens) you will see that it focuses just a bit further away than what we have decided is optimal focus - but as it moves away from optical center - it defocuses more, but then at say 90% towards the edge of the lens, beams start to focus shorter than that and even focus shorter than our designated focus position.

    When focal length of lens depends on distance from the center - that is what we call spherical aberration.  Here is graph from Wiki page on spherical:

    371px-Spherical_aberration_2.svg.png

    In perfect lens - upper one, all rays intersect at the same point - have same focal length, but in bottom image - rays that are further away from center - have shorter focal length (intersect sooner).

    Looking at top graph that shows ED lens performance - we can see that if line is straight - it has no spherical aberration. Further -if it sits on X=0 - there is no chromatism for that wavelength - it has exact focal length. Chromatism or secondary spectrum is when focal length depends on wavelength of light.

    In any case - in above graph we can see that no wavelength is perfect - they are all bent and they are all some distance way from X=0 at some height (or even the whole time). But look at how bent the green line is and how bent the blue line is. Green is 500nm (green light) and blue is 436nm - or blue towards the violet. Blue line is much more bent than green - which means it has more spherical aberration.

    In the end - here is another graph:

    image.png.578b52f504f18f3b1842f6c29c475a

    This graph shows difference between single lens, doublet lens, triplet lens and superachromat. Each of these lenses brings progressively more wavelengths into same focus. Simple lens / singlet will have any one wavelength at the focus at any time. Doublet will bring two wavelengths in focus at the same time, triplet will bring three and super achromat will bring four.

    Each curve is progressively closer to true focus - which means less defocused wavelengths and less false color / secondary spectrum. However - even triplet (orange line in above graph) - won't bring all colors into focus and due to shape of the curve - some wavelengths will be more defocused than the others. Look at defocus at 400nm versus 700nm.  Curve shows much bigger distance from 0 on X axis at 400nm (this time Y axis shows wavelength rather than distance from center of the lens). But that is not important bit - what is important is range of defocus for each of R, G and B sections.

    If we look at 400-500nm range we can see that defocus ranges from -4 to ~1.5. that is 5.5 arbitrary units of focus range. 500-600nm or green part will have from ~1.5 to ~0.5  and that is 1 arbitrary unit of range and red will have from ~0.5 to ~ -0.5 or again 1 arbitrary unit of range.

    Depending on critical focus zone of the telescope - you might be able to adjust focus for green color 500-600nm range and red color 600-700nm range so that whole parts of spectrum seem like in focus (that one arbitrary unit), but if critical focus is say 3 arbitrary units wide - then you simply won't be able to have whole 400-500nm range in focus as it is 5.5 arbitrary units wide.

    By the way - optical designer has freedom to tilt that S curve somewhat and this is what we call correction - wider focus range can be put in red part of spectrum - such scope is blue corrected or in blue part of spectrum - so we call it red corrected.

    Most of the time optical designers opt for red correction - which leaves blue side somewhat softer.

     

     

    • Like 1
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  10. 13 minutes ago, Elp said:

    That's the way I understand it for OSC, not all colours would necessarily be in focus at the same point.

    If you're using filters for mono imaging however you'd refocus for each filter, there should not be a colour channel which is "soft".

    If you shoot luminance you still use the whole spectrum, so it really needs to be RGB (rather than LRGB) and even then, there are reasons why blue might be softer than other colors.

    One reason is spherochromatism, other is how the scope is optimized and third reason is that atmosphere impacts shorter wavelengths the most. In reality - I think that all of these three reasons combine with different contributions to make blue channel softer than the rest.

    This is why I sometimes say that probably best way to do true color images is to do LRG imaging.

  11. Hi and welcome to SGL.

    With that sort of budget - I think that most sensible option would be this one:

    https://www.firstlightoptics.com/reflectors/skywatcher-explorer-130p-ds-ota.html

    together with this

    https://www.firstlightoptics.com/coma-correctors/skywatcher-coma-corrector.html

    Alternative would be to get ~70mm ED doublet refractor with ~400mm of focal length with matching field flattener. Something like SkyWatcher 72ED for example.

    There will be some differences between two setups:

    - Newtonian will be more "all around" scope - meaning that it will give you better field of view on most targets, refractor is more a bit wider field instrument that will render most galaxies as very small

    - Newtonian is a bit harder to setup as it requires maintenance - like collimation (sometimes - that really depends on how often you move the scope and how you handle it), and arguably it is a bit harder to get spacing for coma corrector right

    - Newtonian will also produce diffraction spikes - so that is something you may or may not like. This model also sometimes shows issues from protruding focuser tube and mirror clips - but there are solutions for that - like 3d printing mirror mask and shortening focuser tube a bit.

    - with added focal length - you will likely want to guide sooner with newtonian than with refractor - which is additional cost (guide camera, guide scope and computer).

     

     

  12. 8 minutes ago, Fred_76 said:

    As the drift in DEC will always be in the same direction and at the same rate, it will generate a trail, responsible of walking noise pattern.

     

    On 03/04/2020 at 16:56, vlaiv said:

    Why do I mention this? Because if you make polar alignment error such that it trails almost a pixel in single exposure - every exposure will move by one pixel and you will get "dither" in DEC as well. This is sort of natural dither. This makes it almost impossible to get to subs at same location even if RA moves back and forward the same amount (move Ra +5 px, move Dec +1px, move Ra - 5px, move Dec +1px - Ra is at exactly the same place it started but Dec also moved so sub in total moved, but if there was no movement in DEC - subs would align perfectly as +5 -5 = 0).

     

  13. 5 hours ago, Dunc78 said:

    It was my understanding mono gives higher resolution for imaging. Does the increased frame rate counteract this when using modern colour cameras then. I haven't owned a planetary cam for a good while maybe the technology has come on some.? 

    In principle yes, but there is clever way of stacking that negates this advantage.

    It is implemented in AS!3 - it is called Bayer drizzle. While regular drizzling requires very specific conditions to be effective - Bayer drizzle works almost always with lucky type planetary imaging.

    It requires image to constantly move (be dithered) - which happens in lucky imaging due to atmosphere. There is no need to "artificially reduce pixel size" - as pixels are already at the size they ought to be (same size as with mono camera) and so on.

    With this approach color cameras are much more effective in general color planetary imaging - there is no need to do separate runs for each filter and to do filter change and refocusing and all of that.

    However, for some types of planetary astrophotography - mono is better choice - like Solar Ha or calcium line, UV or infrared, or lunar with different NB filters.

    • Like 1
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  14. If we are talking that sort of money (and that is over OP stated budget for setup) - I would personally choose this scope:

    https://www.firstlightoptics.com/stellamira-telescopes/stellamira-110mm-ed-f6-refractor-telescope.html

    over both F/7 4" Starfield and F/11 4" ED

    - It is easier to mount than ED

    - has more light grasp than 4" F/7

    - will offer widest field of view than both

    - has very good CA correction (not as good as either of those scopes - but scope has potential to go all the way up to 0.997 Strehl in green part of spectrum)

    • Like 1
  15. 11 minutes ago, Moonlit Night said:

    I think it has enough for most folks these days not to buy one.

    I think that it is still very good buy in it's price range.

    FLO currently sells it for £194 - together with 2" diagonal, x2 eyepieces and 30mm finder.

    4" F/7 ED doublet like StarField goes for £899 - that is more than x4 as expensive.

    If one has the budget - then sure, ED doublet is the way to go, but I really don't think anyone can complain at 4" F/10 achromat at current price.

    • Like 2
  16. 29 minutes ago, Moonlit Night said:

    Some? At that focal length you would be buying pretty much the most CA you can buy. I am sorry if this comes over as mean, I am absolutely not trolling, but on planets or bright stars you are going end up with a large purple hallo all over the object. Even at fl10 you are going to get plenty of CA

    I agree about ST / short versions.

    It's not only CA - there is quite a bit of spherical aberration (spherochromatism).  My ST102 showed fuzzy blob on planets when used as is.

    However - I would not say that F/10 version has plenty of CA. CA index of F/10 4" achromat is about 2.5 - which is in "filterable" range, and close to Sidgwick criteria of CA index being >=3.

    Interesting thing about F/10 4" achromat is that you can easily turn it into CA index 5 instrument that is virtually color free - by simply putting aperture mask on it.

    I actually managed to get rather good (color free) image of Saturn with ST102 - by placing 50mm aperture mask in front of objective cell - that created 50mm F/10 achromat that has CA index of ~5. Of course - resolution suffers because of decreased aperture but you can see where you have sweet spot - the least level of CA versus the best level of detail with aperture size

    (I use my 4" F/10 unfiltered and without mask because level of detail is best that way even if there is some level of CA present).

     

  17. For Mak to win over refractor on planets, it really needs a bit more aperture. That is, if both instruments are fairly decent in optical quality.

    I have both 4" F/10 achromat and 4" F/13 Maksutov, and to my surprise - I could tell the difference. In one head to head comparison on planets, frac gave slightly better views. I don't know the cause of that - was it down to thermals (although there was enough time to cool down for both instruments) - or if diagonal was to blame - I used different diagonals - both GSO 99% dielectric ones - but 2" version with frac and 1.25" version with Mak.

    Since then - refractor gave me even better views, but although Mak gave me nice views - I was never really impressed with what I saw (unlike refractor on one particular night).

    I guess that above is sample of one and that conditions were not controlled, so should only be viewed as anecdotal evidence, however, physics also slightly favors refractor for visual, even if it has some residual CA (and F/10 4" has some obviously, but it was not really that obtrusive to my eyes - I even preferred unfiltered view versus Baader Contrast booster).

    To match (or even surpass)  4" frac in planetary view - 5" Mak is needed. Then it comes down to other things - like this one:

    image.png.7ba9c2aadb76cee6319c5f35edc90b92.png

    4" F/10 refractor is capable of showing x3 wider field of view over 5" Maksutov.

     

     

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