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#1
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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 |
#2
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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 |
#3
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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. |
#4
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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 |
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