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c (Bill Ferris) wrote in message ...
Thanks for your clarifying comments. So when using Bartel's ODM program, discussed in your August 2003 Sky & Telescope article against a series of low-contrast extended objects, you recommend using the following brightness numbers, based on local observing-field conditions: NELM.(+/- 0.5)..===..Sky Brightness (mag./sq. arc sec.) ........8.0............22.0 ........7.0............21.0 ........6.0............20.0 ........5.0............19.0 ........4.0............18.0 Your article suggested a series of galaxy DSOs to practice with. Where I got thrown was its suggestion to use 21 or 22 as a default brightness number for a "good rural sky". (I may not be remembering your article correctly, not having it immediately in front of me.) This threw me, since I experience more nightly variation in light-pollution at my observing location and wanted to fine tune use of Bartel's program a little further. I am a small aperture observer and wanted to experiment with brighter objects across more light polluted skies than the list of galaxy DSOs in good or excellent skies suggested in your article. ( Bartel's ODM program: http://zebu.uoregon.edu/~mbartels/dnld/odm.zip ) Also, it should be pointed out that there really is no controversy over the surface brightness of the darkest sites on Earth. That limit is 22.0 MPSA (+/- 0.1-mag.), which has been derived from photometric data taken over decades from sites all over the planet. As to the top end of Schaefer's and Clark's curve being at 24 MPAS, above the empirically measured sky brightness of 22, I assume that is because Blackwell was measuring brightness in an artificially-darkened controlled-laboratory setting. Your brightness table suffices for my immediate needs and I'll leave for another day the details of how Schaefer's and Clark's brightness formulae is used internally in their models. The inability of beginning amateurs, like myself, to distinguish between when an extended object might not have been resolved because light pollution was too high (and viewing the object should be tried again), and when the object could not be resolved because it is simply to faint for the aperature and magnification being used, is one of the more frustrating aspects of getting started in hobbyist observing. The traditional method of evaluating the visibility of extended objects, by their integrated magnitude compared to naked eye limiting field magnitude or to zenithal limiting magnitude (which seems to emphasize the bright core of an extended object, e.g. the Andromeda galaxy), verses an object's dispersed-average brightness (in MPAS) compared to the background sky brightness (which seems to emphasize the object's average brightness across its entire area) both have their strengths and weaknesses. Neither method seems to fully capture the effect of the dispersion of the brightness of an extended object between its central core and less-bright outlying oval and its effect on visibility. (This is probably less true with respect to the list of distant galaxies of small angular size suggested in your article.) I found the MPAS-ODM based approach to be a useful adjunct to the traditional approach of using integrated magnitude, when trying to decide whether an object could never be seen with the current scope or might be seen in a future session in better skies. It increased my understanding of and observing skill with respect to an object's size, its brightness, the background brightness of the sky and the magnification employed. Thanks - Kurt P.S. - The following is a csv file I threw together that contains the Messier objects sorted by descending MPAS brightness and that lists the corresponding traditional integrated magnitude: http://members.csolutions.net/fisher..._Mag_to_Ba.csv The object brightness in MPAS was computed using Clark's estimate of: B_mpas=V_m+2.5*(log(2827*Size_x_arcmin*Size_y_arcm in)) |
#2
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Kurt wrote:
Thanks for your clarifying comments. So when using Bartel's ODM program, discussed in your August 2003 Sky & Telescope article against a series of low-contrast extended objects, you recommend using the following brightness numbers, based on local observing-field conditions: NELM.(+/- 0.5)..===..Sky Brightness (mag./sq. arc sec.) .......8.0............22.0 .......7.0............21.0 .......6.0............20.0 .......5.0............19.0 .......4.0............18.0 I tossed out the above table as a starting place for a discussion of the relationship between NELM and sky brightness. After reading Tony Flander's comments, Carlin and rethinking the problem from the perspective of the eye as a contrast detector, I'm doubtful that the "one mag. change in sky brightness yields a one mag. change in NELM" relationship would hold for any more than one step. What would really be helpful would be an organized effort at several big star parties to get attendees to make NELM estimates and at least one CCD imager to take photometry which could be used to determine the zenithal sky brightness. If we could get some data, we could draw some objective conclustions about that relationship. Your article suggested a series of galaxy DSOs to practice with. Where I got thrown was its suggestion to use 21 or 22 as a default brightness number for a "good rural sky". (I may not be remembering your article correctly, not having it immediately in front of me.) The table in my article lists 14 galaxies ranging in surface brightness from 21.2 MPSA to 22.7, which I culled from an Excel file I use to track objects I've observed. ODM recommends using 21.0 as the background for a dark country or rural sky, which is reasonable for many dark sky sites at least 50-miles from the nearest city. As you experiment with ODM, trying a range of sky brightness settings with size and magnitude data for objects you've observed, you may find a sky brightness setting which generally yields results echoing your real world experience. This threw me, since I experience more nightly variation in light-pollution at my observing location and wanted to fine tune use of Bartel's program a little further. I am a small aperture observer and wanted to experiment with brighter objects across more light polluted skies than the list of galaxy DSOs in good or excellent skies suggested in your article. [snip] I'll look into culling a list for smaller apertures and post it when ready. The inability of beginning amateurs, like myself, to distinguish between when an extended object might not have been resolved because light pollution was too high (and viewing the object should be tried again), and when the object could not be resolved because it is simply to faint for the aperature and magnification being used, is one of the more frustrating aspects of getting started in hobbyist observing. This is one area where a local club--if available--can be a real benefit. Experienced observers who are familiar with the conditions at local sites can provide the encouragement and support to help novice observers grow in the hobby without becoming discouraged. In lieux of that, there are a variety of published resources which can serve a similar purpose. Burnham's Celestial Handbook is one. I also recommend two David J. Eicher anthologies: "The Universe From Your Backyard" and "Stars & Galaxies." "Universe" is a survey of deep-sky objects by constellation. "Stars" is a survey by object type. The traditional method of evaluating the visibility of extended objects, by their integrated magnitude compared to naked eye limiting field magnitude or to zenithal limiting magnitude (which seems to emphasize the bright core of an extended object, e.g. the Andromeda galaxy), verses an object's dispersed-average brightness (in MPAS) compared to the background sky brightness (which seems to emphasize the object's average brightness across its entire area) both have their strengths and weaknesses. Neither method seems to fully capture the effect of the dispersion of the brightness of an extended object between its central core and less-bright outlying oval and its effect on visibility. (This is probably less true with respect to the list of distant galaxies of small angular size suggested in your article.) I found the MPAS-ODM based approach to be a useful adjunct to the traditional approach of using integrated magnitude, when trying to decide whether an object could never be seen with the current scope or might be seen in a future session in better skies. It increased my understanding of and observing skill with respect to an object's size, its brightness, the background brightness of the sky and the magnification employed. Thanks - Kurt I'm glad you found my article and ODM of some help. As you observe more objects, you'll build a larger collection of real world experiences with which to compare against the theoretical approaches to the question, under what conditions is an object observable? We may never have that ellusive perfect rule of thumb which covers all objects. But as we, as individual observers, grow in our understanding of how the eye-brain system sees the universe, at least we gain a better understanding of the obstacles to be overcome and the methods which can help in that endeavor. Regards, Bill Ferris Flagstaff, Arizona USA P.S. - The following is a csv file I threw together that contains the Messier objects sorted by descending MPAS brightness and that lists the corresponding traditional integrated magnitude: http://members.csolutions.net/fisher..._Mag_to_Ba.csv The object brightness in MPAS was computed using Clark's estimate of: B_mpas=V_m+2.5*(log(2827*Size_x_arcmin*Size_y_ Bill Ferris "Cosmic Voyage: The Online Resource for Amateur Astronomers" URL: http://www.cosmic-voyage.net ============= Email: Remove "ic" from .comic above to respond |
#3
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