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#1
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I'm finally ready to make the plunge for a decent $1000-$1500 range
scope. I have researched several makes of both SCTs and refractors, and the choice is getting difficult. So, those of you having experience with both types, I welcome your opinions on what you like, what to look for, and what to buy. thanks and happy holidays, Caesar Garcia |
#2
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![]() SCTs provide lower (poorer) contrast than refractors of the same aperture. The contrast loss associated with recreating the target object at the focal plane is known as the CTF (Contrast Transfer Function). In a nutshell, diffraction resulting from the aperture causes the light to "ripple", just like water did in Young's experiment. In his case he used "slits", and in our case we use a circle. In Young's experiment, waves (ripples) were created on one side of the double slit aperture and then passed through the slits. When they reached the other side, the waves interfered with one another such that where they were in phase, they reinforced, and where they were out of phase they cancelled. In our case, we get the same result, only from a single circular aperture. The result is a circular diffraction pattern. This pattern consists of a central disk and a set of concentric rings (if the scope is properly collimated). Given a target pattern of alternating dark and light lines, the extent and characteristics of the diffraction pattern will have a direct affect on the CTF. However, because of the conservation of energy, there is no actual loss of light, so only contrast is affected, not overall brightness. Thus a 5" SCT and a 5" refractor will have the same brightness, given the same efficiency of light transfer. (The efficiency of light transfer, however, will not be the same. A lens is more efficient than a mirror, and the SCT has a three mirrors to deal with (if you count the diagonal), where a refractor has only one, the diagonal). The obstruction (secondary mirror) in the center of the aperture of a typical reflecting telescope (Newt, SCT, MAK, MNT) adds a further result of influencing the diffraction pattern such that more energy lands in the first diffraction ring, than it does for an unobstructed scope. Hence, the obstructed scope, using our light/dark line pattern, will spill even more of the light from the light lines, over into the dark lines, having a further deleterious effect on the CTF. To compensate for this added loss of efficiency in the CTF brought on by the obstruction, one needs the extra light and increased resolution of a larger aperture. The latter primarily a result of the fact that a larger aperture has a both smaller and brighter central disk in its diffraction pattern. (Guessing here, but one might think that the larger aperture preserves more energy in the central disk, thereby having a dimmer set of rings in its diffraction pattern, with a resultant decrease in "spillage".) In any event, the "tighter" central diffraction disk means less of the target area is covered by a single diffraction pattern, and it follows that the finer details one can see (improving resolution). So, while the central obstruction is robbing light from the central disk and placing it into the first diffraction ring (and thereby spilling light on to the adjacent point in the image plane), the increase in resolution allows that adjacent point to be seen better, regardless. The rule of thumb is, that in order to equal the contrast of a refractor, at a minimum an obstructed aperture will have to have as much more aperture as they do central obstruction. With respect to contrast alone, obstructed aperture - obstruction = unobstructed aperture, so an (typical) 8" SCT with a 34% central obstruction will compare to a 5" refractor of similar optical quality, and an 8" Newtonian with a 25% central obstruction (CO) will compare to a 6" refractor. Further, it has been stated that once you get the CO down to 20% and smaller, the effect of the CO on the diffraction pattern is inconsequential, and the obstruction no longer has a deleteriuos effect on contrast. Having said all of that, refractors are more expensive per inch of aperture than SCTs, and SCTs are more expensive per inch of aperture than Newtonian reflectors. Given $1000, one can either buy a larger aperture SCT, or a _much_ larger aperture Newtonian, than a refractor. This gives you a scope that rivals the refractor in contrast, but more importantly, makes deep sky objects more accessible owing to the increase in light grasp. In the end, it is aperture that brings deep sky objects into view. Of course, if you're not interested in deep sky...., refractors can be a coveted item. HTH, Stephen Paul |
#3
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![]() SCTs provide lower (poorer) contrast than refractors of the same aperture. The contrast loss associated with recreating the target object at the focal plane is known as the CTF (Contrast Transfer Function). In a nutshell, diffraction resulting from the aperture causes the light to "ripple", just like water did in Young's experiment. In his case he used "slits", and in our case we use a circle. In Young's experiment, waves (ripples) were created on one side of the double slit aperture and then passed through the slits. When they reached the other side, the waves interfered with one another such that where they were in phase, they reinforced, and where they were out of phase they cancelled. In our case, we get the same result, only from a single circular aperture. The result is a circular diffraction pattern. This pattern consists of a central disk and a set of concentric rings (if the scope is properly collimated). Given a target pattern of alternating dark and light lines, the extent and characteristics of the diffraction pattern will have a direct affect on the CTF. However, because of the conservation of energy, there is no actual loss of light, so only contrast is affected, not overall brightness. Thus a 5" SCT and a 5" refractor will have the same brightness, given the same efficiency of light transfer. (The efficiency of light transfer, however, will not be the same. A lens is more efficient than a mirror, and the SCT has a three mirrors to deal with (if you count the diagonal), where a refractor has only one, the diagonal). The obstruction (secondary mirror) in the center of the aperture of a typical reflecting telescope (Newt, SCT, MAK, MNT) adds a further result of influencing the diffraction pattern such that more energy lands in the first diffraction ring, than it does for an unobstructed scope. Hence, the obstructed scope, using our light/dark line pattern, will spill even more of the light from the light lines, over into the dark lines, having a further deleterious effect on the CTF. To compensate for this added loss of efficiency in the CTF brought on by the obstruction, one needs the extra light and increased resolution of a larger aperture. The latter primarily a result of the fact that a larger aperture has a both smaller and brighter central disk in its diffraction pattern. (Guessing here, but one might think that the larger aperture preserves more energy in the central disk, thereby having a dimmer set of rings in its diffraction pattern, with a resultant decrease in "spillage".) In any event, the "tighter" central diffraction disk means less of the target area is covered by a single diffraction pattern, and it follows that the finer details one can see (improving resolution). So, while the central obstruction is robbing light from the central disk and placing it into the first diffraction ring (and thereby spilling light on to the adjacent point in the image plane), the increase in resolution allows that adjacent point to be seen better, regardless. The rule of thumb is, that in order to equal the contrast of a refractor, at a minimum an obstructed aperture will have to have as much more aperture as they do central obstruction. With respect to contrast alone, obstructed aperture - obstruction = unobstructed aperture, so an (typical) 8" SCT with a 34% central obstruction will compare to a 5" refractor of similar optical quality, and an 8" Newtonian with a 25% central obstruction (CO) will compare to a 6" refractor. Further, it has been stated that once you get the CO down to 20% and smaller, the effect of the CO on the diffraction pattern is inconsequential, and the obstruction no longer has a deleteriuos effect on contrast. Having said all of that, refractors are more expensive per inch of aperture than SCTs, and SCTs are more expensive per inch of aperture than Newtonian reflectors. Given $1000, one can either buy a larger aperture SCT, or a _much_ larger aperture Newtonian, than a refractor. This gives you a scope that rivals the refractor in contrast, but more importantly, makes deep sky objects more accessible owing to the increase in light grasp. In the end, it is aperture that brings deep sky objects into view. Of course, if you're not interested in deep sky...., refractors can be a coveted item. HTH, Stephen Paul |
#4
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![]() SCTs provide lower (poorer) contrast than refractors of the same aperture. The contrast loss associated with recreating the target object at the focal plane is known as the CTF (Contrast Transfer Function). In a nutshell, diffraction resulting from the aperture causes the light to "ripple", just like water did in Young's experiment. In his case he used "slits", and in our case we use a circle. In Young's experiment, waves (ripples) were created on one side of the double slit aperture and then passed through the slits. When they reached the other side, the waves interfered with one another such that where they were in phase, they reinforced, and where they were out of phase they cancelled. In our case, we get the same result, only from a single circular aperture. The result is a circular diffraction pattern. This pattern consists of a central disk and a set of concentric rings (if the scope is properly collimated). Given a target pattern of alternating dark and light lines, the extent and characteristics of the diffraction pattern will have a direct affect on the CTF. However, because of the conservation of energy, there is no actual loss of light, so only contrast is affected, not overall brightness. Thus a 5" SCT and a 5" refractor will have the same brightness, given the same efficiency of light transfer. (The efficiency of light transfer, however, will not be the same. A lens is more efficient than a mirror, and the SCT has a three mirrors to deal with (if you count the diagonal), where a refractor has only one, the diagonal). The obstruction (secondary mirror) in the center of the aperture of a typical reflecting telescope (Newt, SCT, MAK, MNT) adds a further result of influencing the diffraction pattern such that more energy lands in the first diffraction ring, than it does for an unobstructed scope. Hence, the obstructed scope, using our light/dark line pattern, will spill even more of the light from the light lines, over into the dark lines, having a further deleterious effect on the CTF. To compensate for this added loss of efficiency in the CTF brought on by the obstruction, one needs the extra light and increased resolution of a larger aperture. The latter primarily a result of the fact that a larger aperture has a both smaller and brighter central disk in its diffraction pattern. (Guessing here, but one might think that the larger aperture preserves more energy in the central disk, thereby having a dimmer set of rings in its diffraction pattern, with a resultant decrease in "spillage".) In any event, the "tighter" central diffraction disk means less of the target area is covered by a single diffraction pattern, and it follows that the finer details one can see (improving resolution). So, while the central obstruction is robbing light from the central disk and placing it into the first diffraction ring (and thereby spilling light on to the adjacent point in the image plane), the increase in resolution allows that adjacent point to be seen better, regardless. The rule of thumb is, that in order to equal the contrast of a refractor, at a minimum an obstructed aperture will have to have as much more aperture as they do central obstruction. With respect to contrast alone, obstructed aperture - obstruction = unobstructed aperture, so an (typical) 8" SCT with a 34% central obstruction will compare to a 5" refractor of similar optical quality, and an 8" Newtonian with a 25% central obstruction (CO) will compare to a 6" refractor. Further, it has been stated that once you get the CO down to 20% and smaller, the effect of the CO on the diffraction pattern is inconsequential, and the obstruction no longer has a deleteriuos effect on contrast. Having said all of that, refractors are more expensive per inch of aperture than SCTs, and SCTs are more expensive per inch of aperture than Newtonian reflectors. Given $1000, one can either buy a larger aperture SCT, or a _much_ larger aperture Newtonian, than a refractor. This gives you a scope that rivals the refractor in contrast, but more importantly, makes deep sky objects more accessible owing to the increase in light grasp. In the end, it is aperture that brings deep sky objects into view. Of course, if you're not interested in deep sky...., refractors can be a coveted item. HTH, Stephen Paul |
#5
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"Stephen Paul" wrote in message
... (Guessing here, but one might think that the larger aperture preserves more energy in the central disk, thereby having a dimmer set of rings in its diffraction pattern, with a resultant decrease in "spillage".) Good guess. The percentages are the same with aperture increase, but the size of the airy disk decreases. Clear Skies! Chuck Taylor Do you observe the moon? Try the Lunar Observing Group http://groups.yahoo.com/group/lunar-observing/ ************************************************** ********** |
#6
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"Stephen Paul" wrote in message
... (Guessing here, but one might think that the larger aperture preserves more energy in the central disk, thereby having a dimmer set of rings in its diffraction pattern, with a resultant decrease in "spillage".) Good guess. The percentages are the same with aperture increase, but the size of the airy disk decreases. Clear Skies! Chuck Taylor Do you observe the moon? Try the Lunar Observing Group http://groups.yahoo.com/group/lunar-observing/ ************************************************** ********** |
#7
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"Stephen Paul" wrote in message
... (Guessing here, but one might think that the larger aperture preserves more energy in the central disk, thereby having a dimmer set of rings in its diffraction pattern, with a resultant decrease in "spillage".) Good guess. The percentages are the same with aperture increase, but the size of the airy disk decreases. Clear Skies! Chuck Taylor Do you observe the moon? Try the Lunar Observing Group http://groups.yahoo.com/group/lunar-observing/ ************************************************** ********** |
#8
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You have to ask yourself which of the following 2 attributes are more
important to you, pure optics or portability and ease of use. The reflector has the slight advantage in optical performance in that the clear aperture is a bit greater because of the larger central obstruction of the SCT. Images in a Newt will appear slightly brighter than in an equal size SCT. This is not to say, however, that the SCT performance is poor by comparison. Now for the portability and ease of use... The SCT has got the advantage hands down here, and it's a big advantage. Since the focal length of the SCT is folded, the typical OTA is usually a fraction the size of a Newt of the same aperture. This results in less weight and less bulk, which contribute to ease of set up, ease of use and ease of storage. Finally, the SCT is usually outfitted with full electronics (tracking, GOTO, etc). Since it is not feasible to put large amateur Newts on anything other than a Dobson mount, the reflector (10" and larger) is usually devoid of electronics, including tracking. Al "Caesar Garcia" wrote in message om... I'm finally ready to make the plunge for a decent $1000-$1500 range scope. I have researched several makes of both SCTs and refractors, and the choice is getting difficult. So, those of you having experience with both types, I welcome your opinions on what you like, what to look for, and what to buy. thanks and happy holidays, Caesar Garcia |
#9
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You have to ask yourself which of the following 2 attributes are more
important to you, pure optics or portability and ease of use. The reflector has the slight advantage in optical performance in that the clear aperture is a bit greater because of the larger central obstruction of the SCT. Images in a Newt will appear slightly brighter than in an equal size SCT. This is not to say, however, that the SCT performance is poor by comparison. Now for the portability and ease of use... The SCT has got the advantage hands down here, and it's a big advantage. Since the focal length of the SCT is folded, the typical OTA is usually a fraction the size of a Newt of the same aperture. This results in less weight and less bulk, which contribute to ease of set up, ease of use and ease of storage. Finally, the SCT is usually outfitted with full electronics (tracking, GOTO, etc). Since it is not feasible to put large amateur Newts on anything other than a Dobson mount, the reflector (10" and larger) is usually devoid of electronics, including tracking. Al "Caesar Garcia" wrote in message om... I'm finally ready to make the plunge for a decent $1000-$1500 range scope. I have researched several makes of both SCTs and refractors, and the choice is getting difficult. So, those of you having experience with both types, I welcome your opinions on what you like, what to look for, and what to buy. thanks and happy holidays, Caesar Garcia |
#10
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You have to ask yourself which of the following 2 attributes are more
important to you, pure optics or portability and ease of use. The reflector has the slight advantage in optical performance in that the clear aperture is a bit greater because of the larger central obstruction of the SCT. Images in a Newt will appear slightly brighter than in an equal size SCT. This is not to say, however, that the SCT performance is poor by comparison. Now for the portability and ease of use... The SCT has got the advantage hands down here, and it's a big advantage. Since the focal length of the SCT is folded, the typical OTA is usually a fraction the size of a Newt of the same aperture. This results in less weight and less bulk, which contribute to ease of set up, ease of use and ease of storage. Finally, the SCT is usually outfitted with full electronics (tracking, GOTO, etc). Since it is not feasible to put large amateur Newts on anything other than a Dobson mount, the reflector (10" and larger) is usually devoid of electronics, including tracking. Al "Caesar Garcia" wrote in message om... I'm finally ready to make the plunge for a decent $1000-$1500 range scope. I have researched several makes of both SCTs and refractors, and the choice is getting difficult. So, those of you having experience with both types, I welcome your opinions on what you like, what to look for, and what to buy. thanks and happy holidays, Caesar Garcia |
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