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Magnetic Loops
On 10/21/2015 6:12 AM, amdx wrote:
On 10/20/2015 10:35 PM, rickman wrote: On 10/20/2015 9:21 PM, amdx wrote: On 10/20/2015 1:56 PM, rickman wrote: On 10/20/2015 10:44 AM, amdx wrote: On 10/19/2015 10:53 PM, rickman wrote: On 10/19/2015 3:50 PM, bilou wrote: "rickman" wrote in message ... On 10/19/2015 3:34 AM, Brian Howie wrote: How does the coil affect the tuning range of the cap? A cap is limited by the ratio of the minimum to maximum capacitance. The ratio of frequency is limited to the same ratio. In a multiturn loop you get huge capacitance between turns. For a given variable capacitor it appears in parallel. The Q of that big coil might be higher but as you need to add fixed capacitors to the variable one to get useful tuning range you loose almost what you gain. I sort of lost the thought here. If you up the inductance of the loop, it lowers the required tuning capacitance, so why would fixed capacitors be needed? Are you saying the parasitic capacitance of the loop is enough to significantly reduce the tuning range of the variable cap? Maybe, but there are construction methods that minimize the parasitic capacitance of multi-turn loops. Wide spacing is important. I've seen spiral loops wound on wooden frames that look like God's Eyes, very attractive. I saw descriptions using a 128 pairs telephone cable and spending several days to wire it as a 256 turns loop. A bad idea IMHO. I'm not sure what problem you would be trying to solve by using a 256 turn loop. There are middle grounds... Often a 60kHz WWVB time receiver. So why would that be a "bad idea"? Ahh, you ask "what problem you would be trying to solve" I should clarify, a resonant antenna for 60kHz, and that requires a large inductance. Or at least that is one approach. But the context was that a 256 turn loop was a bad thing. I'm trying to understand what that was about. I don't need to know when it is a good idea... well, I guess even that is interesting. But I think the way a 256 turn loop would be made for a WWVB receiver is around a piece of ferrite. But who knows, maybe a large loop of telephone cable would work well too. It obviously works. It is not ideal because it would have a lot of interwinding capacitance. Also the interwinding capacitance is not a quality capacitance thus the Q is lowered. It could be built with space between wire and layers, and 256 solder connections is not a great idea when trying to insure high Q. As far as "bad idea", all it has to do is receive enough signal to keep the clock accurate, more than that is interesting, but useless. I haven't built a high Q antenna yet, but I am pretty sure people greatly exaggerate the significance of solder connections in the Q factor. Q is related to the losses. I am sure the solder connections will not significantly impact the dissipative resistance of the wire unless the turns are around a pencil. As to "It obviously works", that depends on many other factors. Sure, no doubt it will work a mile from the transmitter. What about along the US east coast in a metal building with many appliances around? There is working, and there is working well. The inter-winding capacitance is not a factor as long as the station can be tuned. -- Rick |
Magnetic Loops
On 10/21/2015 4:42 AM, Brian Howie wrote:
In message , rickman writes The capacitance of the loop to the screen meant that at the minimum variable C setting ,I couldn't get the maximum frequency of about 500KHz I wanted, so I had to take turns off. I now need more parallel C to tune the look down to 136KHz. Wow, that loop must have a *lot* of capacitance. Is there a way to space the conductors away from the copper tubing in the run? Not easy I'm curious why you would use copper pipe for the shield. Because it provides both shield and support? I guess there are a million ways to build a shielded loop. I like the idea of using coax, but I don't know if that also has serious limitations from the capacitance between loop conductor and shield. It seemed a good idea at the time. The original design used plastic pipe covered with tin-foil ,but I wanted something that would survive a Scottish winter outdoors. PVC 4-7 Loop Antenna Al Burzynski KA5JGV ( it's on the NDB yahoo group) it used 12 turns. I think the use of plastic pipe and external tinfoil reduces the C. My loop does work quite well, and has survived outdoors but I think it could be improved Yes, well, they can *all* be improved. I find it interesting to make stuff like this from discarded materials like rain gutter. I'm trying to understand why one poster in a yahoo group says thin stock is no good for transmitting loop antennas. The skin effect limits the signal to the outer few mils of copper or aluminum. I think thin stock will do just fine if the circumference is large, overcoming the limitations of the skin effect. At least you are using all the material rather than just the outer few mils. -- Rick |
Magnetic Loops
On 10/21/2015 6:15 AM, amdx wrote:
On 10/21/2015 2:06 AM, rickman wrote: On 10/21/2015 2:18 AM, Brian Howie wrote: In message , rickman writes On 10/19/2015 3:34 AM, Brian Howie wrote: In message , bilou writes "Brian Howie" wrote in message ... I've a 5 foot Octagonal loop for MF. The shield is copper water pipe, with a gap , 7 turns inside plus a coupling winding. It does a good job eliminating local noise (mostly ASDL hash from the phone lines) compared with a vertical. However the capacitance between the shield and turns seems to load it quite a bit meaning I can't get the tuning range I'd like. Brian GM4DIJ -- Brian Howie Hi My own experience is that ,at least for receive, multi turn loops are useless. Instead you can use a single turn one with a good coil in serial. The tuning range for a given variable capacitor is much greater especially if ,at low frequency, the coil is using ferrite . Switching the coil can increase the tuning range easily. The coil, with a secondary winding,is also very useful to adjust the coupling to the receiver. I'd have thought I'd get a better signal from more turns, but maybe better coupling and a higher Q from your suggestion would do the same. I can't imagine why more turns won't help a receiving loop. I guess it depends on what is limiting reception. Adding a coil may improve the Q or it make make it worse depending on the Q of the coil. More turns won't help the Q of a receiving loop, other than reducing the significance of the resistance of connections and other components. More turns *will* increase the signal strength. How does the coil affect the tuning range of the cap? A cap is limited by the ratio of the minimum to maximum capacitance. The ratio of frequency is limited to the same ratio. The capacitance of the loop to the screen meant that at the minimum variable C setting ,I couldn't get the maximum frequency of about 500KHz I wanted, so I had to take turns off. I now need more parallel C to tune the look down to 136KHz. Wow, that loop must have a *lot* of capacitance. Is there a way to space the conductors away from the copper tubing in the run? I'm curious why you would use copper pipe for the shield. Because it provides both shield and support? I guess there are a million ways to build a shielded loop. I like the idea of using coax, but I don't know if that also has serious limitations from the capacitance between loop conductor and shield. 30pf per ft is a general number for capacitance of coax, but you know it varies with type. I have some coax for automobile radio antennas (AM/FM) that has 8pf per foot. Doesn't the capacitance vary mostly with diameter? The RG-6 I have is 16 pf/ft about a quarter inch diameter. -- Rick |
Magnetic Loops
On 10/21/2015 2:36 PM, rickman wrote:
On 10/21/2015 6:12 AM, amdx wrote: On 10/20/2015 10:35 PM, rickman wrote: On 10/20/2015 9:21 PM, amdx wrote: On 10/20/2015 1:56 PM, rickman wrote: On 10/20/2015 10:44 AM, amdx wrote: On 10/19/2015 10:53 PM, rickman wrote: On 10/19/2015 3:50 PM, bilou wrote: "rickman" wrote in message ... On 10/19/2015 3:34 AM, Brian Howie wrote: How does the coil affect the tuning range of the cap? A cap is limited by the ratio of the minimum to maximum capacitance. The ratio of frequency is limited to the same ratio. In a multiturn loop you get huge capacitance between turns. For a given variable capacitor it appears in parallel. The Q of that big coil might be higher but as you need to add fixed capacitors to the variable one to get useful tuning range you loose almost what you gain. I sort of lost the thought here. If you up the inductance of the loop, it lowers the required tuning capacitance, so why would fixed capacitors be needed? Are you saying the parasitic capacitance of the loop is enough to significantly reduce the tuning range of the variable cap? Maybe, but there are construction methods that minimize the parasitic capacitance of multi-turn loops. Wide spacing is important. I've seen spiral loops wound on wooden frames that look like God's Eyes, very attractive. I saw descriptions using a 128 pairs telephone cable and spending several days to wire it as a 256 turns loop. A bad idea IMHO. I'm not sure what problem you would be trying to solve by using a 256 turn loop. There are middle grounds... Often a 60kHz WWVB time receiver. So why would that be a "bad idea"? Ahh, you ask "what problem you would be trying to solve" I should clarify, a resonant antenna for 60kHz, and that requires a large inductance. Or at least that is one approach. But the context was that a 256 turn loop was a bad thing. I'm trying to understand what that was about. I don't need to know when it is a good idea... well, I guess even that is interesting. But I think the way a 256 turn loop would be made for a WWVB receiver is around a piece of ferrite. But who knows, maybe a large loop of telephone cable would work well too. It obviously works. It is not ideal because it would have a lot of interwinding capacitance. Also the interwinding capacitance is not a quality capacitance thus the Q is lowered. It could be built with space between wire and layers, and 256 solder connections is not a great idea when trying to insure high Q. As far as "bad idea", all it has to do is receive enough signal to keep the clock accurate, more than that is interesting, but useless. I haven't built a high Q antenna yet, but I am pretty sure people greatly exaggerate the significance of solder connections in the Q factor. Q is related to the losses. I am sure the solder connections will not significantly impact the dissipative resistance of the wire unless the turns are around a pencil. On a large loop antenna, it is probably difficult to get an extremely high Q. So, the solder connections will have less of an effect than if it was higher. I made a loop with 1/4" copper pipe, about 2'x 2' with a vacuum variable. I measured it at about Q=800. Using a 240uh and assuming 1000kHz, That's about 1.88 ohms of loss, split between dissipation in materials, wire losses, connection losses and capacitor losses. If you had 0.12 ohms additional solder connection losses, Q would drop to 753 from 800. As to "It obviously works", that depends on many other factors. Sure, no doubt it will work a mile from the transmitter. What about along the US east coast in a metal building with many appliances around? There is working, and there is working well. The inter-winding capacitance is not a factor as long as the station can be tuned. It is my pet theory, that interwinding capacitance will lower Q. It causes displacement current which causes more current flow between turns, also, the interwinding capacitance causes capacitive proximity effects. (vs magnetic proximity effect) I suppose a neat experiment would be to find two materials with equal losses but one having much higher permittivity. Then test Q with one material placed between turns, pull that out and install the higher permittivity material and retest Q. But, I could be all wrong on the subject. Check out this guys site, has some nice loops. http://makearadio.com/loops/ Mikek |
Magnetic Loops
On 10/21/2015 2:47 PM, rickman wrote:
On 10/21/2015 6:15 AM, amdx wrote: On 10/21/2015 2:06 AM, rickman wrote: On 10/21/2015 2:18 AM, Brian Howie wrote: In message , rickman writes On 10/19/2015 3:34 AM, Brian Howie wrote: In message , bilou writes "Brian Howie" wrote in message ... I've a 5 foot Octagonal loop for MF. The shield is copper water pipe, with a gap , 7 turns inside plus a coupling winding. It does a good job eliminating local noise (mostly ASDL hash from the phone lines) compared with a vertical. However the capacitance between the shield and turns seems to load it quite a bit meaning I can't get the tuning range I'd like. Brian GM4DIJ -- Brian Howie Hi My own experience is that ,at least for receive, multi turn loops are useless. Instead you can use a single turn one with a good coil in serial. The tuning range for a given variable capacitor is much greater especially if ,at low frequency, the coil is using ferrite . Switching the coil can increase the tuning range easily. The coil, with a secondary winding,is also very useful to adjust the coupling to the receiver. I'd have thought I'd get a better signal from more turns, but maybe better coupling and a higher Q from your suggestion would do the same. I can't imagine why more turns won't help a receiving loop. I guess it depends on what is limiting reception. Adding a coil may improve the Q or it make make it worse depending on the Q of the coil. More turns won't help the Q of a receiving loop, other than reducing the significance of the resistance of connections and other components. More turns *will* increase the signal strength. How does the coil affect the tuning range of the cap? A cap is limited by the ratio of the minimum to maximum capacitance. The ratio of frequency is limited to the same ratio. The capacitance of the loop to the screen meant that at the minimum variable C setting ,I couldn't get the maximum frequency of about 500KHz I wanted, so I had to take turns off. I now need more parallel C to tune the look down to 136KHz. Wow, that loop must have a *lot* of capacitance. Is there a way to space the conductors away from the copper tubing in the run? I'm curious why you would use copper pipe for the shield. Because it provides both shield and support? I guess there are a million ways to build a shielded loop. I like the idea of using coax, but I don't know if that also has serious limitations from the capacitance between loop conductor and shield. 30pf per ft is a general number for capacitance of coax, but you know it varies with type. I have some coax for automobile radio antennas (AM/FM) that has 8pf per foot. Doesn't the capacitance vary mostly with diameter? Distance between conductors and material between. The RG-6 I have is 16 pf/ft about a quarter inch diameter. Foamed PE! But in general, it looks like my 30pf is a little high. Mikek |
Magnetic Loops
On 10/21/2015 8:41 PM, amdx wrote:
On 10/21/2015 2:36 PM, rickman wrote: On 10/21/2015 6:12 AM, amdx wrote: On 10/20/2015 10:35 PM, rickman wrote: On 10/20/2015 9:21 PM, amdx wrote: On 10/20/2015 1:56 PM, rickman wrote: On 10/20/2015 10:44 AM, amdx wrote: On 10/19/2015 10:53 PM, rickman wrote: On 10/19/2015 3:50 PM, bilou wrote: "rickman" wrote in message ... On 10/19/2015 3:34 AM, Brian Howie wrote: How does the coil affect the tuning range of the cap? A cap is limited by the ratio of the minimum to maximum capacitance. The ratio of frequency is limited to the same ratio. In a multiturn loop you get huge capacitance between turns. For a given variable capacitor it appears in parallel. The Q of that big coil might be higher but as you need to add fixed capacitors to the variable one to get useful tuning range you loose almost what you gain. I sort of lost the thought here. If you up the inductance of the loop, it lowers the required tuning capacitance, so why would fixed capacitors be needed? Are you saying the parasitic capacitance of the loop is enough to significantly reduce the tuning range of the variable cap? Maybe, but there are construction methods that minimize the parasitic capacitance of multi-turn loops. Wide spacing is important. I've seen spiral loops wound on wooden frames that look like God's Eyes, very attractive. I saw descriptions using a 128 pairs telephone cable and spending several days to wire it as a 256 turns loop. A bad idea IMHO. I'm not sure what problem you would be trying to solve by using a 256 turn loop. There are middle grounds... Often a 60kHz WWVB time receiver. So why would that be a "bad idea"? Ahh, you ask "what problem you would be trying to solve" I should clarify, a resonant antenna for 60kHz, and that requires a large inductance. Or at least that is one approach. But the context was that a 256 turn loop was a bad thing. I'm trying to understand what that was about. I don't need to know when it is a good idea... well, I guess even that is interesting. But I think the way a 256 turn loop would be made for a WWVB receiver is around a piece of ferrite. But who knows, maybe a large loop of telephone cable would work well too. It obviously works. It is not ideal because it would have a lot of interwinding capacitance. Also the interwinding capacitance is not a quality capacitance thus the Q is lowered. It could be built with space between wire and layers, and 256 solder connections is not a great idea when trying to insure high Q. As far as "bad idea", all it has to do is receive enough signal to keep the clock accurate, more than that is interesting, but useless. I haven't built a high Q antenna yet, but I am pretty sure people greatly exaggerate the significance of solder connections in the Q factor. Q is related to the losses. I am sure the solder connections will not significantly impact the dissipative resistance of the wire unless the turns are around a pencil. On a large loop antenna, it is probably difficult to get an extremely high Q. So, the solder connections will have less of an effect than if it was higher. I made a loop with 1/4" copper pipe, about 2'x 2' with a vacuum variable. I measured it at about Q=800. Using a 240uh and assuming 1000kHz, That's about 1.88 ohms of loss, split between dissipation in materials, wire losses, connection losses and capacitor losses. If you had 0.12 ohms additional solder connection losses, Q would drop to 753 from 800. Why would you assume 120 mOhms of resistance from soldered connections? Have you measured this somewhere? As to "It obviously works", that depends on many other factors. Sure, no doubt it will work a mile from the transmitter. What about along the US east coast in a metal building with many appliances around? There is working, and there is working well. The inter-winding capacitance is not a factor as long as the station can be tuned. It is my pet theory, that interwinding capacitance will lower Q. It causes displacement current which causes more current flow between turns, also, the interwinding capacitance causes capacitive proximity effects. (vs magnetic proximity effect) I suppose a neat experiment would be to find two materials with equal losses but one having much higher permittivity. Then test Q with one material placed between turns, pull that out and install the higher permittivity material and retest Q. But, I could be all wrong on the subject. Check out this guys site, has some nice loops. http://makearadio.com/loops/ Yeah, not bad. -- Rick |
Magnetic Loops
On 10/21/2015 9:09 PM, rickman wrote:
On 10/21/2015 8:41 PM, amdx wrote: On 10/21/2015 2:36 PM, rickman wrote: On 10/21/2015 6:12 AM, amdx wrote: On 10/20/2015 10:35 PM, rickman wrote: On 10/20/2015 9:21 PM, amdx wrote: On 10/20/2015 1:56 PM, rickman wrote: On 10/20/2015 10:44 AM, amdx wrote: On 10/19/2015 10:53 PM, rickman wrote: On 10/19/2015 3:50 PM, bilou wrote: "rickman" wrote in message ... On 10/19/2015 3:34 AM, Brian Howie wrote: How does the coil affect the tuning range of the cap? A cap is limited by the ratio of the minimum to maximum capacitance. The ratio of frequency is limited to the same ratio. In a multiturn loop you get huge capacitance between turns. For a given variable capacitor it appears in parallel. The Q of that big coil might be higher but as you need to add fixed capacitors to the variable one to get useful tuning range you loose almost what you gain. I sort of lost the thought here. If you up the inductance of the loop, it lowers the required tuning capacitance, so why would fixed capacitors be needed? Are you saying the parasitic capacitance of the loop is enough to significantly reduce the tuning range of the variable cap? Maybe, but there are construction methods that minimize the parasitic capacitance of multi-turn loops. Wide spacing is important. I've seen spiral loops wound on wooden frames that look like God's Eyes, very attractive. I saw descriptions using a 128 pairs telephone cable and spending several days to wire it as a 256 turns loop. A bad idea IMHO. I'm not sure what problem you would be trying to solve by using a 256 turn loop. There are middle grounds... Often a 60kHz WWVB time receiver. So why would that be a "bad idea"? Ahh, you ask "what problem you would be trying to solve" I should clarify, a resonant antenna for 60kHz, and that requires a large inductance. Or at least that is one approach. But the context was that a 256 turn loop was a bad thing. I'm trying to understand what that was about. I don't need to know when it is a good idea... well, I guess even that is interesting. But I think the way a 256 turn loop would be made for a WWVB receiver is around a piece of ferrite. But who knows, maybe a large loop of telephone cable would work well too. It obviously works. It is not ideal because it would have a lot of interwinding capacitance. Also the interwinding capacitance is not a quality capacitance thus the Q is lowered. It could be built with space between wire and layers, and 256 solder connections is not a great idea when trying to insure high Q. As far as "bad idea", all it has to do is receive enough signal to keep the clock accurate, more than that is interesting, but useless. I haven't built a high Q antenna yet, but I am pretty sure people greatly exaggerate the significance of solder connections in the Q factor. Q is related to the losses. I am sure the solder connections will not significantly impact the dissipative resistance of the wire unless the turns are around a pencil. On a large loop antenna, it is probably difficult to get an extremely high Q. So, the solder connections will have less of an effect than if it was higher. I made a loop with 1/4" copper pipe, about 2'x 2' with a vacuum variable. I measured it at about Q=800. Using a 240uh and assuming 1000kHz, That's about 1.88 ohms of loss, split between dissipation in materials, wire losses, connection losses and capacitor losses. If you had 0.12 ohms additional solder connection losses, Q would drop to 753 from 800. Why would you assume 120 mOhms of resistance from soldered connections? Have you measured this somewhere? I have absolutely no idea about the resistance of a solder connection. I used 0.12 because it made 1.88 = 2. As to "It obviously works", that depends on many other factors. Sure, no doubt it will work a mile from the transmitter. What about along the US east coast in a metal building with many appliances around? There is working, and there is working well. The inter-winding capacitance is not a factor as long as the station can be tuned. It is my pet theory, that interwinding capacitance will lower Q. It causes displacement current which causes more current flow between turns, also, the interwinding capacitance causes capacitive proximity effects. (vs magnetic proximity effect) I suppose a neat experiment would be to find two materials with equal losses but one having much higher permittivity. Then test Q with one material placed between turns, pull that out and install the higher permittivity material and retest Q. But, I could be all wrong on the subject. Check out this guys site, has some nice loops. http://makearadio.com/loops/ Yeah, not bad. |
Magnetic Loops
On Wed, 21 Oct 2015 05:15:18 -0500, amdx wrote:
30pf per ft is a general number for capacitance of coax, but you know it varies with type. I have some coax for automobile radio antennas (AM/FM) that has 8pf per foot. Mikek Well its not real coax , but the diameter is about 5ft ( well its octagonal ) say 15ft circumferance , There's 7 turns in close proximity to the tube or each other, so the capacitance could be a few hundred pf . I suppose could try measuring it. Self resonance with 12 turns was about 400KHz http://www.angelfire.com/mb/amandx/loop.html so effective minimumum capacitance works out around 100pf Brian --- This email has been checked for viruses by Avast antivirus software. https://www.avast.com/antivirus |
Magnetic Loops
On 10/22/2015 9:43 AM, Brian Howie wrote:
On Wed, 21 Oct 2015 05:15:18 -0500, amdx wrote: 30pf per ft is a general number for capacitance of coax, but you know it varies with type. I have some coax for automobile radio antennas (AM/FM) that has 8pf per foot. Mikek Well its not real coax , but the diameter is about 5ft ( well its octagonal ) say 15ft circumferance , There's 7 turns in close proximity to the tube or each other, so the capacitance could be a few hundred pf . I suppose could try measuring it. Self resonance with 12 turns was about 400KHz http://www.angelfire.com/mb/amandx/loop.html so effective minimumum capacitance works out around 100pf Brian I'm not sure if you're discussing 100pf of interwinding capacitance or capacitance between the shield and the winding. Mikek |
Magnetic Loops
On 10/15/2015 5:42 AM, J.B. Wood wrote:
On 10/14/2015 02:34 PM, rickman wrote: I just read the wikipedia article on small loop antennas and it seems I was laboring under a misapprehension. I thought receiving loops were "magnetic" because they were shielded (this is often stated in various web pages about constructing such loops). But the wikipedia article on small loop antennas says the nature of a small loop is to not be very sensitive to the E field in near field. So if the shield has little to do with rejecting near field electrical noise, what does the shield do? A lot of antenna designs make a big deal of the shield. So I assume it must be a useful addition to the small loop antenna for some purpose. Hello, and that seems to be ham radio jargon. Hams seem to think the adjectives "magnetic" and "electric" are needed when referring to loop and dipole antennas, respectively. Textbooks on electromagnetics and antennas don't use those terms except in the case when discussing theoretically small radiators, i.e. "magnetic dipoles" and "electric dipoles". My hypothesis on the ham terminology is that a loop is viewed as an inductor. That's OK for close-in (non-radiative) mutual coupling to some source but when you're several wavelengths away (in the far field) then the loop (or dipole antenna for that matter) responds to the electromagnetic field (the electric and magnetic far fields can't be considered separately). The fact that an axis of either antenna lines up with the electric or magnetic field vector in the far field is moot. Does this mean that the loop doesn't have inductance? Of course not and it plays a role in establishing the feedpoint impedance of the loop at the operating frequency. Now if folks would just stop using that word "literally" so damn much... Sincerely, and 73s from N4GG0 I agree. If the jargon is either magnetic or electric, how do we define a folded dipole antenna? It is a loop. Is it electric or magnetic? |
Magnetic Loops
On 10/22/2015 6:01 AM, amdx wrote:
On 10/21/2015 9:09 PM, rickman wrote: On 10/21/2015 8:41 PM, amdx wrote: On 10/21/2015 2:36 PM, rickman wrote: On 10/21/2015 6:12 AM, amdx wrote: On 10/20/2015 10:35 PM, rickman wrote: On 10/20/2015 9:21 PM, amdx wrote: On 10/20/2015 1:56 PM, rickman wrote: On 10/20/2015 10:44 AM, amdx wrote: On 10/19/2015 10:53 PM, rickman wrote: On 10/19/2015 3:50 PM, bilou wrote: "rickman" wrote in message ... On 10/19/2015 3:34 AM, Brian Howie wrote: How does the coil affect the tuning range of the cap? A cap is limited by the ratio of the minimum to maximum capacitance. The ratio of frequency is limited to the same ratio. In a multiturn loop you get huge capacitance between turns. For a given variable capacitor it appears in parallel. The Q of that big coil might be higher but as you need to add fixed capacitors to the variable one to get useful tuning range you loose almost what you gain. I sort of lost the thought here. If you up the inductance of the loop, it lowers the required tuning capacitance, so why would fixed capacitors be needed? Are you saying the parasitic capacitance of the loop is enough to significantly reduce the tuning range of the variable cap? Maybe, but there are construction methods that minimize the parasitic capacitance of multi-turn loops. Wide spacing is important. I've seen spiral loops wound on wooden frames that look like God's Eyes, very attractive. I saw descriptions using a 128 pairs telephone cable and spending several days to wire it as a 256 turns loop. A bad idea IMHO. I'm not sure what problem you would be trying to solve by using a 256 turn loop. There are middle grounds... Often a 60kHz WWVB time receiver. So why would that be a "bad idea"? Ahh, you ask "what problem you would be trying to solve" I should clarify, a resonant antenna for 60kHz, and that requires a large inductance. Or at least that is one approach. But the context was that a 256 turn loop was a bad thing. I'm trying to understand what that was about. I don't need to know when it is a good idea... well, I guess even that is interesting. But I think the way a 256 turn loop would be made for a WWVB receiver is around a piece of ferrite. But who knows, maybe a large loop of telephone cable would work well too. It obviously works. It is not ideal because it would have a lot of interwinding capacitance. Also the interwinding capacitance is not a quality capacitance thus the Q is lowered. It could be built with space between wire and layers, and 256 solder connections is not a great idea when trying to insure high Q. As far as "bad idea", all it has to do is receive enough signal to keep the clock accurate, more than that is interesting, but useless. I haven't built a high Q antenna yet, but I am pretty sure people greatly exaggerate the significance of solder connections in the Q factor. Q is related to the losses. I am sure the solder connections will not significantly impact the dissipative resistance of the wire unless the turns are around a pencil. On a large loop antenna, it is probably difficult to get an extremely high Q. So, the solder connections will have less of an effect than if it was higher. I made a loop with 1/4" copper pipe, about 2'x 2' with a vacuum variable. I measured it at about Q=800. Using a 240uh and assuming 1000kHz, That's about 1.88 ohms of loss, split between dissipation in materials, wire losses, connection losses and capacitor losses. If you had 0.12 ohms additional solder connection losses, Q would drop to 753 from 800. Why would you assume 120 mOhms of resistance from soldered connections? Have you measured this somewhere? I have absolutely no idea about the resistance of a solder connection. I used 0.12 because it made 1.88 = 2. Ok, I'll consider that in your analysis. ;) -- Rick |
Magnetic Loops
On Thu, 22 Oct 2015 09:54:24 -0500, amdx wrote:
On 10/22/2015 9:43 AM, Brian Howie wrote: On Wed, 21 Oct 2015 05:15:18 -0500, amdx wrote: 30pf per ft is a general number for capacitance of coax, but you know it varies with type. I have some coax for automobile radio antennas (AM/FM) that has 8pf per foot. Mikek Well its not real coax , but the diameter is about 5ft ( well its octagonal ) say 15ft circumferance , There's 7 turns in close proximity to the tube or each other, so the capacitance could be a few hundred pf . I suppose could try measuring it. Self resonance with 12 turns was about 400KHz http://www.angelfire.com/mb/amandx/loop.html so effective minimumum capacitance works out around 100pf Brian I'm not sure if you're discussing 100pf of interwinding capacitance or capacitance between the shield and the winding. Mikek It's pretty complicated .There's distributed capacitance between the windings and distributed capacitance between the windings and the shield. I know the inductance of the loop and the resonant frequency with the variable C set to minimum, so I can work out an effective capacitance 100pf that causes the resonance. There's a further complication in that the coupling loop is also capacitively coupled to the main windings and the shield, so connecting that up changes the resonance as well. I can't even begin to think how to model it. The unshielded wide-spaced loop makes it easier to design, but you get ( arguably) no electric field shielding, which is where we came in. I started out using the maths but ended up cut and try to get a compromise solution. Brian --- This email has been checked for viruses by Avast antivirus software. https://www.avast.com/antivirus |
Magnetic Loops
On 10/22/2015 2:20 PM, Brian Howie wrote:
The unshielded wide-spaced loop makes it easier to design, but you get ( arguably) no electric field shielding, which is where we came in. I thought the magnetic loop was not very sensitive to near field electrical source, hence the name? As to the modeling, I believe there are programs available for that like one of the many antenna simulators. -- Rick |
Magnetic Loops
On Thursday, October 22, 2015 at 1:20:31 PM UTC-5, Brian Howie wrote:
It's pretty complicated .There's distributed capacitance between the windings and distributed capacitance between the windings and the shield. I know the inductance of the loop and the resonant frequency with the variable C set to minimum, so I can work out an effective capacitance 100pf that causes the resonance. There's a further complication in that the coupling loop is also capacitively coupled to the main windings and the shield, so connecting that up changes the resonance as well. If adding the coupling loop changes the resonance, it's so small as to be ignored in the real world. I can't even begin to think how to model it. Modeling it can be a pain I imagine, but it's all quite easy to calculate using Reg Edwards program rjeloop3.exe. Which is a DOS program, but I installed "DOSbox" on my Win 7 64 box, and it runs just fine. Lets take it for a quick test drive. Lets make a square loop 1000mm per side, with seven turns of 1mm wire, with a ratio/wire spacing of 5mm between the wires. We want to tune it to 500khz for an example. The program proclaims that the inductance of the loop is 155.6 mh. The inductive reactance is 489 ohms. The HF loss resistance of the wire is 2.32 ohms. The self resonant frequency of the loop is 4.6 mhz. Total cap value to tune 500 khz is 651 pf, - stray capacitance of 8 pf, leaves a setting of the cap at 643 pf. The appx Q of the coil is 210, and the receive sensitivity is 53 db below a 1/4 wl vertical. Total width of winding is 31mm, and the total length of wire is 28m. Impedance seen across loop when tuned is 102.8 K-ohms. Impedance seen by receiver is 2.1 K-ohms via a 1 turn coupling loop. The program can be used to play "what if" until the cows come home, and any single specification can be changed and tested to see the difference. The unshielded wide-spaced loop makes it easier to design, but you get ( arguably) no electric field shielding, which is where we came in. You would get an argument from me, as the "electric field shielding" is the part I consider total malarkey, and I believe W8JI was of pretty much the same opinion when I took a quick glance of his article. I've built nearly every type of small receiving loop there is, and the tested results reinforced my feeling that the concept of "electric field shielding" is malarkey. It's all about balance, not electric field shielding as far as I'm concerned. The gapped shield loops were no better at reducing noise than a properly balanced solenoid or pancake loop. Heck, I even tried using a single turn shielded loop as the coupling loop. Worked fine, but no better than a plain wire coupling loop, being as I had no balance issues. |
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