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#11
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Thanks for the information, everyone. I'll read up on a few of the
references. I have found a few web pages that compare the sensitivity of the shielded vs. unshielded loops, and the shielded loop always ends up with slightly less sensitivity. Could anyone answer the following question? I'm trying to make things simpler here than what happens what a real antenna: Let me take an ideal circular conductor, say, a meter in circumference. Next I'll stick it inside a perfectly conducting loop of pipe (the shield) that has an infinitesimally small slit in it to prevent creating a shorted turn. Finally I'll create a magnetic field at a very low frequency (say, 1Hz -- so that the loop is clearly electrically small) and insert the loop into it such that coupling is maximized. Question: Will the current on the inner conductor be identical to the case where there is no shield? Is there any current on the shield? Does anything change if I ground the shield? Hmm... I'm thinking I should move this over to the electromagnetics newsgroup! ---Joel |
#12
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The "shield" is actually the antenna, and the gap in the "shield" is
the feedpoint of that antenna. You will do well to make the "shield" out of a good conductor, and to get the benefits of rejecting vertically-polarized electric fields generated nearby, you should make the antenna very symmetrical. See the discussion in King, Mimno and Wing's "Transmission Lines, Antennas and Waveguides." I think I have a .pdf file of the relevant section somewhere. I particularly like that one for its qualitative explanation, clearly presented. I've seen other decent explanations in places like Johnson and Jasik's antenna book. The explanations in such texts that I've seen all agree. A key advantage of the "shield" is that it simplifies the task of making the antenna symmetrical, though I've seen a lot of old ARRL pubs that completely miss that point. If you realize that that's what you're trying to accomplish in the "shielded" construction, you'll find you can do quite well with a multi-turn "unshielded" loop, too. Cheers, Tom (one with a last name) "Joel Kolstad" wrote in message ... When you build a loop antenna, it's common to wrap it in, e.g., aluminum foil that's grounded so as to prevent electric field pick-up (I'm thinking of HF loops here, 30MHz). A slit is made in the wrapping so that a shorted turn isn't created, thereby nulling out the magnetic field that the loop is trying to detect in the first place. Something I don't understand, though... normally, if you were thinking of using aluminum for EMI shielding purposes, the skin depth of aluminum at 10MHz is all of ~1mil. Hence, a regular sheet of aluminum foil would significantly attenuate both the magnetic and electric fields on its 'far' side. Why doesn't this apply in the case of a shielded loop antenna? It seems to me that the ~95+% 'coverage' of the shield (everything minus the slit to prevent the shorted turn) would be what dictates the overall shielding effectiveness, not the presence of the slit itself. Looking for insight, ---Joel Kolstad |
#13
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On Mon, 8 Nov 2004 09:58:10 -0800, "Joel Kolstad"
wrote: Will the current on the inner conductor be identical to the case where there is no shield? Is there any current on the shield? Does anything change if I ground the shield? Hi Joel, A 1M loop in a 1Hz field, Hmm? Why bother with the complication of shielding? Take a 1M loop of wire, connect it to your MOST sensitive ammeter (mine will resolve at least 1 nanoampere). By simply going to my lab, and turning on the unit, this allowed me to test my hypothesis as leads that long were already attached. I used the earth's magnetic field and a nearby fluorescent fixture (80 W) to find absolutely NO sensitivity at all on AC or DC scales (turning the loop in earth's magnetic loop to simulate the lower 1Hz frequency you specify). Now, I know that for studies of low frequency magnetics, the usual antenna has 10 to 20 thousand turns on an 18" ferrite bar, I think that a 1M open air loop is destined for deafness. Of course, this will serve as no impediment to those who can count angels on the head of a pin, so your question will undoubtedly be met with great fuss. 73's Richard Clark, KB7QHC |
#14
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Hi Tom,
Those are some good additional references; thanks. I was surprised to find that Kraus' antenna book doesn't discuss shielded loops (well, the most recent/last edition -- I've heard that some material from earlier editions has been pulled from it). Your explanation matches the 'other Tom's' explanation, and sounds plausible to me, yet there are others posting here who seem to disagree. The fact that you have several more theory oriented books agreeing lends a lot of support to it. If you do find a PDF version of the section of the King/Mimno/Wings book, I'd love to get a copy. ---Joel |
#15
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"Richard Clark" wrote in message
... A 1M loop in a 1Hz field, Hmm? That was meant to setup the problem such that the loops is electrically small and such that only quasi-magnetostatic analysis would be necessary. In actuality I'm thinking more along the lines of WWVB loop antennas -- 60kHz. Why bother with the complication of shielding? The idea is that there's a lot of predominently electric field interference around (60Hz power lines, for ones) and that the shield -- if grounded -- can short out that component of the field and get the loop to respond primarily to the magnetic field. ---Joel |
#16
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![]() "Tom Bruhns" wrote in message m... The "shield" is actually the antenna, and the gap in the "shield" is the feedpoint of that antenna. You will do well to make the "shield" out of a good conductor, and to get the benefits of rejecting vertically-polarized electric fields generated nearby, you should make the antenna very symmetrical. See the discussion in King, Mimno and Wing's "Transmission Lines, Antennas and Waveguides." I think I have a .pdf file of the relevant section somewhere. I particularly like that one for its qualitative explanation, clearly presented. I've seen other decent explanations in places like Johnson and Jasik's antenna book. The explanations in such texts that I've seen all agree. A key advantage of the "shield" is that it simplifies the task of making the antenna symmetrical, though I've seen a lot of old ARRL pubs that completely miss that point. If you realize that that's what you're trying to accomplish in the "shielded" construction, you'll find you can do quite well with a multi-turn "unshielded" loop, too. Cheers, Tom (one with a last name) Hi Tom (WALN), I thought the original question related to whether or not the magnetic field penetrates the "shield". I have a problem calling the shield the antenna because I have built loops (144 & 440 MHz) which do not have this classic form of shield, but a unidirectional screen, and good nulls off both sides. I made the shield from a series of vertical wires connected to a conducting strip only at the bottom. I also wonder about the symmetrical concept as a standard "Hazeltine" loop had the opening of the shield at one end near the bottom, near the feed. I suspect that a symmetrically constructed loop will have less electrostatic response, however. This seems to make sense. Then there is the matter of the practicality of construction. If it is easier to make the loop unsymmetrical and shielded, then that's ok. 73, also with a last name, -- Steve N, K,9;d, c. i My email has no u's. |
#17
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On Mon, 8 Nov 2004 10:53:06 -0800, "Joel Kolstad"
wrote: "Richard Clark" wrote in message .. . A 1M loop in a 1Hz field, Hmm? That was meant to setup the problem such that the loops is electrically small and such that only quasi-magnetostatic analysis would be necessary. In actuality I'm thinking more along the lines of WWVB loop antennas -- 60kHz. Hi Joel, When I was calibrating my Atomic Clock, years distant, my antenna was a simple 20' whip above the fantail of my ship. We used WWVB and an unique modulation envelope to perform the job. This didn't make the antenna particularly efficient, but it was suitably sensitive. Still and all, there are roughly 5 orders of magnitude down to the 1Hz region. You may as well use WWVB as your testbed, or one of the submarine fleet frequencies around 12KHz. One station is nearby here at Jim Creek. They use a T antenna of about 1000' tall with a top hat of 6 cables strung between two mountain tops (about 4000 to 6000 feet between them). The numbers may be off, but you can judge that the scale is impressive (quite a sight). Why bother with the complication of shielding? The idea is that there's a lot of predominently electric field interference around (60Hz power lines, for ones) and that the shield -- if grounded -- can short out that component of the field and get the loop to respond primarily to the magnetic field. 1Hz noise field would come from meteors striking, and ionizing the upper atmosphere. I doubt you could judge against any local sources of noise compared to that chatter. Given that line frequency would be 6 Octaves away, if you tuned your antenna (it would be tuned, wouldn't it?), you would have to be next to a noisy power plant to hear it. 73's Richard Clark, KB7QHC 73's Richard Clark, KB7QHC |
#18
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That's some interesting history Richard!
"Richard Clark" wrote in message ... 1Hz noise field would come from meteors striking, and ionizing the upper atmosphere. I doubt you could judge against any local sources of noise compared to that chatter. Given that line frequency would be 6 Octaves away, if you tuned your antenna (it would be tuned, wouldn't it?), you would have to be next to a noisy power plant to hear it. Well, I've read that down around 60kHz there's plenty of interference due to noise on the power lines (I doubt harmonics, probably just plain old noise from, e.g., switching power supplies). But in any case, I'm at the point where I need to just build something and see how it performs. ---Joel |
#19
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Tom Bruhns, K7ITM wrote:
"See the discussion in King, Mimno, and Wing`s "Transmission Lines, Antennas. and Wave Guides"." Ronold W.P. King did a fine job explaining "closed circuits as antennas". It starts on page 224. The shielded loop is diagrammed on page 234. As Tom Bruhns says, the exterior of the loop is driven from the gap at the midpoint in its shield. The shielded wire loop is coupled by its proximity to the interior surface of the shield. The outside of the loop is coupled by conduction across the open circuit edges to the inside surface of the loop. The gap is the drivepoint. The secret to noise immunity is symmetry and balance in all aspects of the loop. Best regards, Richard Harrison, KB5WZI |
#20
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