Return-Path: Received: (qmail 16406 invoked from network); 10 May 2001 13:32:03 -0000 Received: from unknown (HELO guinness.servers.plus.net) (212.159.3.230) by excalibur-qfe1-smtp-plusnet.harl.plus.net with SMTP; 10 May 2001 13:32:02 -0000 Received: (qmail 2996 invoked from network); 10 May 2001 12:26:46 -0000 Content-Transfer-Encoding: 8bit Received: from post.thorcom.com (212.172.148.70) by mx.last.plus.net with SMTP; 10 May 2001 12:26:46 -0000 X-Priority: 3 Received: from majordom by post.thorcom.com with local (Exim 3.16 #2) id 14xpXQ-0006pk-00 for rsgb_lf_group-outgoing@blacksheep.org; Thu, 10 May 2001 13:27:24 +0100 X-MSMail-Priority: Normal Received: from mail.cc.kuleuven.ac.be ([134.58.10.6]) by post.thorcom.com with esmtp (Exim 3.16 #2) id 14xpXM-0006pZ-00 for rsgb_lf_group@blacksheep.org; Thu, 10 May 2001 13:27:20 +0100 Received: from LCBD15.fys.kuleuven.ac.be (LCBD15.fys.kuleuven.ac.be [134.58.80.15]) by mail.cc.kuleuven.ac.be (8.9.3/8.9.0) with SMTP id OAA968162 for ; Thu, 10 May 2001 14:26:32 +0200 X-MimeOLE: Produced By Microsoft MimeOLE V6.00.2800.1106 Message-ID: <3.0.1.16.20010510132736.2c87c87a@mail.cc.kuleuven.ac.be> X-Sender: pb623250@mail.cc.kuleuven.ac.be X-Mailer: Windows Eudora Pro Version 3.0.1 (16) Date: Thu, 10 May 2001 13:27:36 To: rsgb_lf_group@blacksheep.org From: "Rik Strobbe" Subject: LF: harmonics / LF antenna In-reply-to: <004401c0d92c$0f19a060$af6e74d5@w8k3f0> References: <65AECDF1F89AD411900400508BFC869F9C0491@pdw-mail-1.dera.gov.uk> <3AFA2E4C.EBB3C4EF@alg.demon.co.uk> MIME-Version: 1.0 Content-Type: text/plain; charset=us-ascii; format=flowed Precedence: bulk Reply-To: rsgb_lf_group@blacksheep.org X-Listname: rsgb_lf_group Sender: Hello group, few days ago I got a mail from someone new to LF who asked me how efficient a vertical antenna would surpress the harmonic contests from the TX. So far I hadn't put much thought on that as my 400W TX has a 3 stage LF filter, keeping all harmonics at least 50dB down. But calculations seem te be quite simple, above the resonance frequency the antenna becomes inductive. The average antenna (few 100pF capacitance) will already at the second harmonic have an inductive component of several 1000 Ohms, keeping the (harmonic) current low. But on the other hand the radiation resistance will increase by the square of the frequency, making whateven harmonic current that gets through the coil being radiated more efficient. Just out of curiosity I calculated the overall efficiency of a loaded vertical antenna on the harmonic frequencies and came to the result that the harmonic supression is rather constant for all harmonics. Below you find the result for a vertical monopole with a capacitance of 300pF and a loss resistance of 50 Ohm : FREQUENCY Impedance Efficiency (versus fundamental) fund. (137kHz) 50 Ohm 0.0dB 2nd harm. (274kHz) 5811 Ohm -29.3dB 3rd harm. (411kHz) 10330 Ohm -30.7dB 4rd harm. (548kHz) 14526 Ohm -31.2dB 6th harm. (822kHz) 22596 Ohm -31.5dB 8th harm. (1096kHz) 30505 Ohm -31.6dB 10th harm. (1370kHz) 38349 Ohm -31.7dB For the calculations I assumed no stray capacitance in the coil, so in the 'real world' the figures might be a few dB different, probably higher (less negative). Further the harmonic surpresssion becomes less is the antenna capacitance increases (smaller coil needed) and the loss resistance increases. Eg : for a 'big' antenna with 600pF capacitance and 100 Ohm groundloss the antenna efficiency on the 2nd harmonic frequency will be only -17.2dB down, on the 10th harmonic -19.6dB. So sending a few 100W square wave into a big antenna is not really recommended. 73, Rik ON7YD