Return-Path: Received: (qmail 11429 invoked from network); 21 Apr 2002 05:21:44 -0000 Received: from unknown (HELO murphys-inbound.services.quay.plus.net) (212.159.14.225) by exhibition.plus.net with SMTP; 21 Apr 2002 05:21:44 -0000 Received: (qmail 29090 invoked from network); 21 Apr 2002 05:21:34 -0000 Received: from unknown (HELO post.thorcom.com) (212.172.148.70) by murphys.services.quay.plus.net with SMTP; 21 Apr 2002 05:21:34 -0000 Received: from majordom by post.thorcom.com with local (Exim 3.33 #2) id 16zBGU-0007pn-00 for rsgb_lf_group-outgoing@blacksheep.org; Sun, 21 Apr 2002 07:56:02 +0100 Received: from carbon.btinternet.com ([194.73.73.92] helo=carbon) by post.thorcom.com with esmtp (Exim 3.33 #2) id 16zBGT-0007pi-00 for rsgb_lf_group@blacksheep.org; Sun, 21 Apr 2002 07:56:01 +0100 Received: from host213-1-143-201.btinternet.com ([213.1.143.201] helo=dave) by carbon with smtp (Exim 3.22 #8) id 16z9jJ-0003Lp-00 for rsgb_lf_group@blacksheep.org; Sun, 21 Apr 2002 06:17:42 +0100 Message-ID: <000001c1e8f4$7bfe1d40$c98f01d5@dave> From: "Dave Sergeant" To: rsgb_lf_group@blacksheep.org References: Subject: Re: LF: loop inductance Date: Sat, 20 Apr 2002 19:49:37 +0100 MIME-Version: 1.0 Content-Type: text/plain; charset=iso-8859-1; format=flowed Content-Transfer-Encoding: 8bit X-Priority: 3 X-MSMail-Priority: Normal X-Mailer: Microsoft Outlook Express 5.50.4522.1200 X-MimeOLE: Produced By Microsoft MimeOLE V6.00.2800.1106 Precedence: bulk Reply-To: rsgb_lf_group@blacksheep.org X-Listname: rsgb_lf_group Sender: >From Dave G3YMC Further to the discussion on loop inductance and various related matters, a couple of weeks ago Mike Underhill G3LHZ gave a talk at our Bracknell Amateur Radio Club on loops. Some of you may remember the similar lecture he gave at the HF Convention a couple of years ago. Mike has done a lot of work with loops, mainly 1-2m diameter ones on the hf bands, and probably knows more about them than anybody. Some of his theories are also rather contoversial, but they are all based on practical results. In subsequent mails with Mike he has supplied some of the formulae he uses in his design of loops. Inductance of a circular loop L(microHenries) = pi D^1.16 / (160d)^0.16 where D is the loop diameter in metres and d is the diameter of the conductor wire in metres. This can be extended to non circular loops ie rectangular ones if D is calculated as the loop circumference (ie length of wire) divided by pi. The ^ symbol in the formula means 'raised to the power of'. This formula gives a value of 75uH for my loop (measured value 70uH). Another interesting formula he uses is: Q = 500/D as a limiting value of the Q of a loop, and where D is the diameter in metres as above. This is the value of Q if the other losses, ie series R, are negligible. This relates to a Q of 35 for my own loop (effective D 14.3m). This shows that there is a limit to how far you can improve a loop by reducing the resistance, though I feel it is rather pessimistic in my case. Even more bizarre is his formula for radiation resistance: R(looprad) ~ = LoopArea * f (MHz) / 20. When I put the figures in for my loop I got a value of 0.68 ohms, implying 50% effiency (and hence rather over 1W erp!). But in fact Mike says you have to include the earth loss resistance in calculating the efficiency with this formula - for my very lossy 300 ohms ground it brings the efficiency down to 0.22%, a rather more plausible figure. But it throws out of the window the theory that you can largely ignore earth resistance losses.... Not sure what to make of these figures, but they are food for thought and may help. Dave G3YMC dsergeant@iee.org dsergeant@btinternet.com http://www.dsergeant.btinternet.co.uk