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#1
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Cecil Moore wrote:
Ian White GM3SEK wrote: Across the whole 1-30MHz band, the bunched choke behaves as an almost perfect L-C circuit, free from any unwanted resonances. One additional point. If the above were true, as the frequency is increased, the phase angle of the coiled choke impedance would drop from ~90 degrees to zero at the self-resonant frequency, and then rise back to ~-90 degrees and stay there. But that's not what happens. In every single case, the phase angle rises toward -90 degrees *and then decreases* as the 1/2WL self-resonance point is approached. That is a clear indication of transmission line effects. A lumped circuit simply doesn't act that way. The spreadsheet at http://www.ifwtech.co.uk/g3sek/misc/chokes.xls now includes graphs of the phase information for all the chokes. [ Thank you, Owen - the phase axis label is now fixed . For anyone interested who doesn't have Excel, Microsoft's free Excel file viewer is at http://tinyurl.com/cup85 ] Coming all the way back to the original question, the data confirms that even though it may look like something held together with duct tape, a coiled coax choke can be an excellent single-band solution. At its parallel self-resonant frequency, it will have a much higher common-mode impedance than a generic string of ferrite beads. It can probably outperform or at least equal a ferrite choke over two or possibly three adjacent HF bands; but being a resonant device, it cannot deliver extreme broadband performance. In the chokes we're looking at, the low-impedance series resonances of which Cecil complains do not occur below 30MHz. Those resonances exist, but not on the HF frequencies where the chokes would actually be used. Within the practical working frequency range of all of these coiled-coax chokes, the performance can be accurately described as that of a simple parallel tuned LC circuit, which displays no transmission-line behaviour whatever. Cecil complains that One might say it is misbehaving and is a very poor design. That sounds to me like the complaint of someone who has a pet theory to hammer, and is disappointed when he can't find a nail. I think that's it, really. The graphs themselves say the rest. -- 73 from Ian GM3SEK 'In Practice' columnist for RadCom (RSGB) http://www.ifwtech.co.uk/g3sek |
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#2
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On Sun, 22 Oct 2006 23:56:04 +0100, Ian White GM3SEK
wrote: [ Thank you, Owen - the phase axis label is now fixed . For anyone interested who doesn't have Excel, Microsoft's free Excel file viewer is at http://tinyurl.com/cup85 ] Hi Owen, It is far easier to simply use OpenOffice which is an executable that will translate to/from Windows Office (any spread sheet, document, presentation, drawing...). The Open Document format is the mandated standard of the European Community, if I recall correctly. 73's Richard Clark, KB7QHC |
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#3
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On Sun, 22 Oct 2006 16:24:33 -0700, Richard Clark
wrote: Hi Owen, Sorry Ian, wrong side of the continental divide here. |
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#4
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On Sun, 22 Oct 2006 16:24:33 -0700, Richard Clark
wrote: Hi Owen, It is far easier to simply use OpenOffice which is an executable that will translate to/from Windows Office (any spread sheet, document, presentation, drawing...). The Open Document format is the mandated standard of the European Community, if I recall correctly. Be careful. If any VB type macros are included in Excel Open Office will barf. Been there done that. Danny, K6MHE |
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#5
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-----BEGIN PGP SIGNED MESSAGE-----
Hash: SHA1 Danny Richardson wrote: On Sun, 22 Oct 2006 16:24:33 -0700, Richard Clark wrote: Hi Owen, It is far easier to simply use OpenOffice which is an executable that will translate to/from Windows Office (any spread sheet, document, presentation, drawing...). The Open Document format is the mandated standard of the European Community, if I recall correctly. Be careful. If any VB type macros are included in Excel Open Office will barf. Been there done that. Danny, K6MHE Opens fine in OpenOffice 2 on SUSE 10 but I did have to reposition the graphs which were over the table. Charlie. - -- www.wymsey.co.uk -----BEGIN PGP SIGNATURE----- Version: GnuPG v1.4.2 (GNU/Linux) Comment: Using GnuPG with SUSE - http://enigmail.mozdev.org iD8DBQFFPIKufhKqaKFAJ/YRAgnOAJ9ZjDMfv6s+TwcswZd0YbJQJK5e1QCcCskT Dbm7fF6MOISjjCsbzjBLihA= =zEFh -----END PGP SIGNATURE----- |
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#6
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charlie wrote:
Danny Richardson wrote: On Sun, 22 Oct 2006 16:24:33 -0700, Richard Clark wrote: Hi Owen, It is far easier to simply use OpenOffice which is an executable that will translate to/from Windows Office (any spread sheet, document, presentation, drawing...). The Open Document format is the mandated standard of the European Community, if I recall correctly. Be careful. If any VB type macros are included in Excel Open Office will barf. Been there done that. Danny, K6MHE Opens fine in OpenOffice 2 on SUSE 10 Thanks for that information, Charlie - it's very useful to know what other systems can see. but I did have to reposition the graphs which were over the table. That's how I saved the graphs, so OpenOffice got those layout details right. Once the graphs have been plotted, it isn't necessary to look at the underlying table very often, because the data can be seen in a popup window by running the mouse pointer along each plotted line. If OpenOffice can do that too, you may find it a convenient feature. Alternatively, you could drag both graphs away to the right, and then use the horizontal scroll bar to move between the table and graphs. -- 73 from Ian GM3SEK 'In Practice' columnist for RadCom (RSGB) http://www.ifwtech.co.uk/g3sek |
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#7
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Ian White GM3SEK wrote:
In the chokes we're looking at, the low-impedance series resonances of which Cecil complains do not occur below 30MHz. Those resonances exist, but not on the HF frequencies where the chokes would actually be used. But, Ian, what about 75m and 40m? Those resonances above 26 MHz are transmission line effects. The largest coil is only 12 turns, not nearly enough for 75m operation. The largest 12 turn coil has a choking impedance of only 100 ohms on 75m. Scale the choke to 75m and 40-50 turns are probably required. That would certainly lower the 1/2WL resonant frequencies into the HF ham bands. The 12 turn coil's peak impedance is around 15 MHz and its 1/2WL low impedance response is around 31 MHz. If we scale the peak impedance value to 4 MHz by increasing the turns, the 1/2WL low impedance response would be around 8 MHz. Such a choke would be useless above 10 MHz. Bottom Line: If enough turns are used to achieve a high choking impedance on 75m, the 1/2WL resonant transmission line effects will occur in the middle of HF making it useless on the higher HF frequencies. Within the practical working frequency range of all of these coiled-coax chokes, the performance can be accurately described as that of a simple parallel tuned LC circuit, which displays no transmission-line behaviour whatever. This is obviously a false statement proved by your own graphs. If there were no transmission line effects, the phase graphs would all converge on -90 degrees. All of the phase bumps above 26 MHz are transmission line effects. If the chokes had their maximum impedance at 4 MHz, those 1/2WL transmission line effects would probably be in the range of 10 MHz rendering them useless on 30m-10m. Cecil complains that One might say it is misbehaving and is a very poor design. That sounds to me like the complaint of someone who has a pet theory to hammer, and is disappointed when he can't find a nail. Actually, I was just quoting this web page: http://www.k1ttt.net/technote/airbalun.html "- Don't bunch the turns together. Wind them as a single layer on a form. Bunching the turns kills the choking effect at higher frequencies." I agree with WA2SRQ that the bunched coil choke is a poor design. Do you think that WA2SRQ has a pet theory? I think that's it, really. The graphs themselves say the rest. They certainly do. Everything above 26 MHz is obviously transmission line effects. If the chokes were designed for the lower part of the HF spectrum, the 1/2WL low impedance points, caused by the transmission line effects, would be in the middle of the HF spectrum. Scale the high impedance points for 75m and the low impedance bumps due to transmission line effects will occur in the middle of HF. -- 73, Cecil http://www.w5dxp.com |
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#8
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Cecil Moore wrote:
Ian White GM3SEK wrote: In the chokes we're looking at, the low-impedance series resonances of which Cecil complains do not occur below 30MHz. Those resonances exist, but not on the HF frequencies where the chokes would actually be used. But, Ian, what about 75m and 40m? Those resonances above 26 MHz are transmission line effects. The largest coil is only 12 turns, not nearly enough for 75m operation. The largest 12 turn coil has a choking impedance of only 100 ohms on 75m. Scale the choke to 75m and 40-50 turns are probably required. Sorry for the delay in replying, but I just did something completely radical for this type of discussion: hauled out some cable, made some chokes, and measured them. These chokes were intended to be like the ones recommended in the ARRL Handbook for 3.5MHz and for 7MHzz, both using 22ft of RG213. What I had was actually 21ft, and this length was wound into a flat coil having various numbers of turns. The choking impedances and phase angles were measured on an N2PK Vector Network Analyser. Ten turns made a choke that had 1000 ohms impedance from 3.4MHz to 6.4MHz, falling to about 650 ohms by 7.3MHz. This makes a respectable two-band choke, if you judge it by the criterion of needing about 500 ohms minimum impedance, but it's a stretch to cover both bands from edge to edge (9 turns was probably a slightly better compromise). Moreover the maximum impedance of 17k is "wasted" between the amateur bands at 4.6MHz. That confirms our shared suspicion that the Handbook's claim of "a broad resonance that easily (sic) covers three octaves" is over-optimistic. Where the coiled-cable choke really excels is as a single-band device, exploiting its extremely high peak impedance at parallel resonance. Without needing to change the overall length of cable, the peak resonance can be shifted to different frequencies by increasing or decreasing the number of turns, although I couldn't persuade 21ft below 4.6MHz (10 turns) because the bending radius was becoming too small for RG213. However, it's perfectly clear that Cecil's estimate of "40-50 turns" needed for a 75m choke is way off. That would certainly lower the 1/2WL resonant frequencies into the HF ham bands. The 12 turn coil's peak impedance is around 15 MHz and its 1/2WL low impedance response is around 31 MHz. If we scale the peak impedance value to 4 MHz by increasing the turns, the 1/2WL low impedance response would be around 8 MHz. Such a choke would be useless above 10 MHz. Bottom Line: If enough turns are used to achieve a high choking impedance on 75m, the 1/2WL resonant transmission line effects will occur in the middle of HF making it useless on the higher HF frequencies. Right conclusion about the choke being useless a long way above its peak resonance - but not the right reason for it. The true reason is the very simple property of a parallel LC circuit (the inductance of the coil, resonated by its own self-capacitance) which means that far above resonance its parallel impedance drops to a very low value. That's what makes it useless at those frequencies. The 4.6MHz choke does have series resonances at about 23MHz 33MHz ,but those cannot be said to affect the performance of the choke in any practical way, because the choke doesn't have any usable performance at these frequencies anyway. Within the practical working frequency range of all of these coiled-coax chokes, the performance can be accurately described as that of a simple parallel tuned LC circuit, which displays no transmission-line behaviour whatever. This is obviously a false statement proved by your own graphs. If there were no transmission line effects, the phase graphs would all converge on -90 degrees. All of the phase bumps above 26 MHz are transmission line effects. If the chokes had their maximum impedance at 4 MHz, those 1/2WL transmission line effects would probably be in the range of 10 MHz rendering them useless on 30m-10m. Cecil keeps resolutely ignoring the reservation: "within the practical working range of the choke". Within the frequency range where the choke has a practically useful value of impedance, there are no - repeat NO - signs of transmission line effects. Its behaviour is purely LC, its own inductance resonating with its self-capacitance. Cecil complains that One might say it is misbehaving and is a very poor design. That sounds to me like the complaint of someone who has a pet theory to hammer, and is disappointed when he can't find a nail. Actually, I was just quoting this web page: http://www.k1ttt.net/technote/airbalun.html "- Don't bunch the turns together. Wind them as a single layer on a form. Bunching the turns kills the choking effect at higher frequencies." I agree with WA2SRQ that the bunched coil choke is a poor design. Do you think that WA2SRQ has a pet theory? I think WA2SRQ's advice is one-sided, because it fails to recognize the benefit of bunching the cable together - namely that it moves the whole resonance curve downward (due to the increased self-capacitance) without needing to increase the length of cable. For someone who wants a low-band choke, that is a Very Good Thing. The poorer performance at higher frequencies is the obvious natural tradeoff for having moved the whole resonance curve downward - but that doesn't make it a "poor design". I think that's it, really. The graphs themselves say the rest. They certainly do. Everything above 26 MHz is obviously transmission line effects. If the chokes were designed for the lower part of the HF spectrum, the 1/2WL low impedance points, caused by the transmission line effects, would be in the middle of the HF spectrum. Scale the high impedance points for 75m and the low impedance bumps due to transmission line effects will occur in the middle of HF. Hands-on measurements prove otherwise - the spurious resonances stay pretty much where they were, above 20MHz. As stated above, I measured a choke which is resonant at 4.6MHz. It has over 1000 ohms impedance at 3.5MHz, rising to over 2k at 4MHz, so it would be a very good performer on both 75m and 80m. But above the main parallel resonance there are no bumps in the impedance or ripples in the phase response at any frequency below 20MHz - none. It is ridiculous for Cecil to describe such a choke as "misbehaving and a very poor design". On the contrary, bunching the turns to increase the self-capacitance has proved a very good way of moving the main resonance downward to make an effective single-band choke for 75/80m, while leaving all the unwanted resonances parked above 20MHz. -- 73 from Ian GM3SEK 'In Practice' columnist for RadCom (RSGB) http://www.ifwtech.co.uk/g3sek |
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#9
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Ian White GM3SEK wrote:
However, it's perfectly clear that Cecil's estimate of "40-50 turns" needed for a 75m choke is way off. Wouldn't you say the number of turns depends upon the diameter of the coil? How many turns would be needed for 75m self-resonance if one were using RG-58 wound on a 3 inch diameter PVC pipe? Using the inductance formula in the ARRL Handbook, 40 turns on a 3 inch diameter form at 4 TPI is about 32 uH or about 800 ohms on 4 MHz. The distributed capacitance would lower it even farther. 40 turns on a 3" form would be an absolute minimum for any high SWR situation on 75m. Right conclusion about the choke being useless a long way above its peak resonance - but not the right reason for it. The true reason is the very simple property of a parallel LC circuit (the inductance of the coil, resonated by its own self-capacitance) which means that far above resonance its parallel impedance drops to a very low value. That's what makes it useless at those frequencies. Ian, your own graphs show transmission line effects. The fact that the phase angle does NOT go to -90 degrees and stay there proves those are transmission line effects. Here's what the IEEE paper says: "The concept of coil 'self-capacitance' is an attempt to circumvent transmission line effects on small coils when the current distribution begins to depart from its DC behavior." "There are a great number of formulae for coil self-capacitance. None are of particular value for quarter-wave helical resonators anywhere near the 90 degree point." Your parallel self-resonance *IS* the 90 degree point. I wish you would take time out to realize that if there were no transmission line effects, the phase angle would go to -90 degrees and stay there. Please set up a parallel inductor and capacitor and see for yourself what happens as one increases the frequency past parallel resonance. The phase angle is asymptotic to -90 degrees. The 4.6MHz choke does have series resonances at about 23MHz 33MHz ,but those cannot be said to affect the performance of the choke in any practical way, because the choke doesn't have any usable performance at these frequencies anyway. Those grapes were probably sour anyway. :-) Ian, a lumped circuit inductor and parallel capacitance would NOT have those series resonances. A lumped circuit would go to a phase angle of -90 degrees and stay there while the impedance drops inversely proportional to frequency. Seems to me, you have just admitted that the chokes you wound are exhibiting transmission line effects just as I predicted. (Except for the VF error I made.) THE CHOKE DOESN'T HAVE ANY USABLE PERFORMANCE AT THOSE HIGHER FREQUENCIES *BECAUSE* OF THE TRANSMISSION LINE EFFECTS!!! Cecil keeps resolutely ignoring the reservation: "within the practical working range of the choke". That's circular logic, Ian. I said that series resonant transmission line effects limit the practical working range of a coax choke and you disagreed. Now you have proved I am right with your own measurements on chokes of your own design. If those actually were lumped inductors and capacitors as you continue to assert, THE SERIES RESONANCES THAT YOU MEASURED WOULD NOT AND COULD NOT EXIST!!! The series resonant transmission line effects are the *CAUSE* of the practical working range of the choke being limited. In a parallel LC circuit, as the frequency increases, the capacitive reactance becomes dominant and decreases inversely proportional to frequency. The phase angle would be asymptotic to -90 degrees. None of the measurements look anything like that. All of the measurements exhibit transmission line effects. Within the frequency range where the choke has a practically useful value of impedance, there are no - repeat NO - signs of transmission line effects. Its behaviour is purely LC, its own inductance resonating with its self-capacitance. This will be the forth time I have said this, Ian. If there were no sign of transmission line effects, the phase angle would go to -90 degrees and stay there. If the phase angle doesn't go to -90 degrees and stay there, that is *prima facie evidence* of transmission line effects. Lumped parallel inductors and capacitors don't exhibit the effects measured by you on the chokes that you wound. Scale the high impedance points for 75m and the low impedance bumps due to transmission line effects will occur in the middle of HF. Hands-on measurements prove otherwise - the spurious resonances stay pretty much where they were, above 20MHz. Uhhhhh Ian, 20 MHz *IS* HF! The transmission line 1/2WL series resonant effects are occurring in the HF range! That's why the 75m choke doesn't work on 15m!!! 20-30 MHz is 37% of HF. As stated above, I measured a choke which is resonant at 4.6MHz. It has over 1000 ohms impedance at 3.5MHz, rising to over 2k at 4MHz, so it would be a very good performer on both 75m and 80m. But it wouldn't make a good performer on 15m because of the series resonant transmission line effects. That was my point from the beginning. (The mistake I made was forgetting that the VF of the choke changes with frequency.) It is ridiculous for Cecil to describe such a choke as "misbehaving and a very poor design". This thread has not been about single-band or narrow-band chokes. We were talking about broadband chokes being able to cover three octaves of HF. The bunched coil choke is much more narrow-banded than helical wound chokes thus rendering them virtually useless for broadband operation. They *misbehave* in broadband (all-HF) applications. They are a *very poor design* for broadband (all-HF) applications. -- 73, Cecil http://www.w5dxp.com |
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#10
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Cecil Moore wrote:
Ian White GM3SEK wrote: However, it's perfectly clear that Cecil's estimate of "40-50 turns" needed for a 75m choke is way off. Wouldn't you say the number of turns depends upon the diameter of the coil? How many turns would be needed for 75m self-resonance if one were using RG-58 wound on a 3 inch diameter PVC pipe? Using the inductance formula in the ARRL Handbook, 40 turns on a 3 inch diameter form at 4 TPI is about 32 uH or about 800 ohms on 4 MHz. The distributed capacitance would lower it even farther. 40 turns on a 3" form would be an absolute minimum for any high SWR situation on 75m. I am not your offshore lab service, Cecil. If you want to back up your speculations, do your own work. Right conclusion about the choke being useless a long way above its peak resonance - but not the right reason for it. The true reason is the very simple property of a parallel LC circuit (the inductance of the coil, resonated by its own self-capacitance) which means that far above resonance its parallel impedance drops to a very low value. That's what makes it useless at those frequencies. Ian, your own graphs show transmission line effects. The fact that the phase angle does NOT go to -90 degrees and stay there proves those are transmission line effects. Here's what the IEEE paper says: "The concept of coil 'self-capacitance' is an attempt to circumvent transmission line effects on small coils when the current distribution begins to depart from its DC behavior." "There are a great number of formulae for coil self-capacitance. None are of particular value for quarter-wave helical resonators anywhere near the 90 degree point." This discussion doesn't involve anybody's formula for self-capacitance. The coil resonates using whatever value of self-capacitance it has in reality. Your parallel self-resonance *IS* the 90 degree point. I wish you would take time out to realize that if there were no transmission line effects, the phase angle would go to -90 degrees and stay there. Please set up a parallel inductor and capacitor and see for yourself what happens as one increases the frequency past parallel resonance. The phase angle is asymptotic to -90 degrees. I know what a parallel LC circuit does. The point you continue to evade is that, from VLF up to about 20MHz, this coil of cable behaves in exactly the same way. The circuit looks inductive below the resonant frequency and capacitive above it, and passing through resonance the phase angle of the impedance flips from +90deg to -90deg... and then it stays very close to 90deg, clear up to about 20MHz. (The VNA reports angles of -88 to -89deg.) The 4.6MHz choke does have series resonances at about 23MHz 33MHz ,but those cannot be said to affect the performance of the choke in any practical way, because the choke doesn't have any usable performance at these frequencies anyway. Those grapes were probably sour anyway. :-) Ian, a lumped circuit inductor and parallel capacitance would NOT have those series resonances. A lumped circuit would go to a phase angle of -90 degrees and stay there while the impedance drops inversely proportional to frequency. Seems to me, you have just admitted that the chokes you wound are exhibiting transmission line effects just as I predicted. (Except for the VF error I made.) THE CHOKE DOESN'T HAVE ANY USABLE PERFORMANCE AT THOSE HIGHER FREQUENCIES *BECAUSE* OF THE TRANSMISSION LINE EFFECTS!!! Cecil keeps resolutely ignoring the reservation: "within the practical working range of the choke". That's circular logic, Ian. I said that series resonant transmission line effects limit the practical working range of a coax choke and you disagreed. Now you have proved I am right with your own measurements on chokes of your own design. If those actually were lumped inductors and capacitors as you continue to assert, THE SERIES RESONANCES THAT YOU MEASURED WOULD NOT AND COULD NOT EXIST!!! That is the usual mixture of selective quoting and false logic. What you continue to overlook is that the behaviour all the way from DC through the 4.7MHz resonance and onward up to about 20MHz can be accurately represented by nothing more elaborate than a simple LCR circuit. The fall in impedance from the resonant frequency up to about 20MHz is completely accounted for by just those three simple parameters: two reactances and one fixed loss resistance in parallel. Above that frequency there are effects that the simple LCR model cannot account for. I have always said so, and yes, a transmission-line model could account for those. The series resonant transmission line effects are the *CAUSE* of the practical working range of the choke being limited. That is simply not true. The limitation in working range is simply the shunting effect of the self-capacitance, which becomes increasingly important above resonance and causes a long progressive fall in impedance. This effect is very simple and entirely predictable. By 20MHz it has reduced the impedance to a hundred ohms or less, which means that the coil of cable is no use as a feedline choke for that frequency. The series resonances above 20MHz cause further dips in impedance to only a few ohms, but those dips are quite localized in frequency. They are not the cause of the long progressive fall in impedance above the parallel resonance, which is what limits the usable bandwidth of the choke. The challenge is still on the table, Cecil, for YOU to develop a quantified transmission-line model that will predict all the measured properties of a resonant choke over that wider range of frequencies. The rest is snipped, because it's just you continuing your own argument with the straw-man you have manufactured. A self-resonant choke is not a wideband solution capable of cover the whole of HF. I never expected it to be, and never claimed it would be, so stop acting as if I had. -- 73 from Ian GM3SEK 'In Practice' columnist for RadCom (RSGB) http://www.ifwtech.co.uk/g3sek |
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