Return-Path: Received: from rly-mf03.mail.aol.com (rly-mf03.mail.aol.com [172.20.29.173]) by air-mf07.mail.aol.com (v119.11) with ESMTP id MAILINMF071-94b46fd25e43c7; Fri, 28 Sep 2007 12:04:25 -0400 Received: from post.thorcom.com (post.thorcom.com [193.82.116.20]) by rly-mf03.mail.aol.com (v119.11) with ESMTP id MAILRELAYINMF031-94b46fd25e43c7; Fri, 28 Sep 2007 12:03:58 -0400 Received: from majordom by post.thorcom.com with local (Exim 4.14) id 1IbIIR-0003vY-CW for rs_out_1@blacksheep.org; Fri, 28 Sep 2007 17:02:31 +0100 Received: from [83.244.159.144] (helo=relay3.thorcom.net) by post.thorcom.com with esmtp (Exim 4.14) id 1IbIIQ-0003vO-24 for rsgb_lf_group@blacksheep.org; Fri, 28 Sep 2007 17:02:30 +0100 Received: from an-out-0708.google.com ([209.85.132.244]) by relay3.thorcom.net with esmtp (Exim 4.63) (envelope-from ) id 1IbIIH-0002xN-HK for rsgb_lf_group@blacksheep.org; Fri, 28 Sep 2007 17:02:28 +0100 Received: by an-out-0708.google.com with SMTP id b21so2489084ana for ; Fri, 28 Sep 2007 09:02:19 -0700 (PDT) DKIM-Signature: v=1; a=rsa-sha256; c=relaxed/relaxed; d=googlemail.com; s=beta; h=domainkey-signature:received:received:message-id:date:from:to:subject:in-reply-to:mime-version:content-type:content-transfer-encoding:content-disposition:references; bh=G9BF35EIDPNd9oR67ho5rPzwl3JDfoVb7e2K/mdMYUE=; b=aTXYH+xoN4L5M7T40/jzUeU83RvQvZlAFMOP9IpWsLAarTdQ2HAa4uwSFURlPdjckbTe7ne7Ooz+5p8vOSHB7mIobZhfUcdTYkflthOj968GnRekKnn51eptHQ/egZc8yLPKjDXdLxYVVNHUPpO964Kwyr399ZSd+Fe/SbVfW/8= DomainKey-Signature: a=rsa-sha1; c=nofws; d=googlemail.com; s=beta; h=received:message-id:date:from:to:subject:in-reply-to:mime-version:content-type:content-transfer-encoding:content-disposition:references; b=aOI31QLAuthAqvQg4v0azTlRkeG9J0ThRe/Ipo0bAJIEACMU++4A8HqssHk4Vl/p71Tvr/4thp2VWzlT141yij4vbuH3o3+r+DO2Jx82B8sy29qoGNCvkyzYhGbXNVzosjSRr6GGLU8mIpraKRgjrWMlXzVkhGP8l5O3iC1nO+o= Received: by 10.114.13.1 with SMTP id 1mr509755wam.1190995337952; Fri, 28 Sep 2007 09:02:17 -0700 (PDT) Received: by 10.35.107.12 with HTTP; Fri, 28 Sep 2007 09:02:17 -0700 (PDT) Message-ID: Date: Fri, 28 Sep 2007 17:02:17 +0100 From: "Andy Talbot" To: rsgb_lf_group@blacksheep.org In-Reply-To: <000001c801dd$a0ecc1d0$7900a8c0@athlon1200> MIME-Version: 1.0 Content-Disposition: inline References: <000a01c80132$aae29df0$83e41a52@enigma> <46FC071D.2090202@w1tag.com> <000601c801ae$38cc27a0$0fee1a52@enigma> <001d01c801c6$a918b420$0fee1a52@enigma> <000001c801dd$a0ecc1d0$7900a8c0@athlon1200> DomainKey-Status: good (testing) X-Spam-Score: 0.0 (/) X-Spam-Report: autolearn=disabled,none Subject: Re: LF: A question of calibration Content-Type: text/plain; charset=ISO-8859-1 Content-Transfer-Encoding: 7bit X-Spam-Checker-Version: SpamAssassin 2.63 (2004-01-11) on post.thorcom.com X-Spam-Level: X-Spam-Status: No, hits=0.0 required=5.0 tests=none autolearn=no version=2.63 X-SA-Exim-Scanned: Yes Sender: owner-rsgb_lf_group@blacksheep.org Precedence: bulk Reply-To: rsgb_lf_group@blacksheep.org X-Listname: rsgb_lf_group X-SA-Exim-Rcpt-To: rs_out_1@blacksheep.org X-SA-Exim-Scanned: No; SAEximRunCond expanded to false X-AOL-IP: 193.82.116.20 X-AOL-SCOLL-AUTHENTICATION: listenair ; SPF_helo : X-AOL-SCOLL-AUTHENTICATION: listenair ; SPF_822_from : X-Mailer: Unknown (No Version) Blimey ! That is dramatic. And there is a minute wobble up to about 10 times the distance as well - which would probably give 2% - 3% error. So, in a way, one could almost say the RSGB figure "is right" to go so far out:-) Andy On 28/09/2007, Dave Brown wrote: > It's instructive to look at plots of the variation of wave impedance > with distance from the source. > These plots (acknowledgements to John Middleton and Marconi Insts, > "Engineers EMC Workbook") > > http://homepages.ihug.co.nz/~tractorb/zfreespace.jpg > > are for 47.7 MHz to scale the distance for lambda/2.pi to 1 metre, but > the principle remains the same for any frequency. The selection of > lambda/2.pi for the transition between near and far field regions > makes much more sense when you see it plotted this way. Note the > impedance scale is on the extreme right. > > DaveB, NZ > > > ----- Original Message ----- > From: "Andy Talbot" > To: > Sent: Saturday, September 29, 2007 12:50 AM > Subject: Re: LF: A question of calibration > > > > Yes, it would be "certainly true" that 10 times the recognised > > distance is in the far field. It certainly provides a huge safety > > margin! > > > > Most texts use 2.pi, although I did once see 4.pi quoted. > > > > Andy G4JNT > > > > > > On 28/09/2007, Malcolm Harman wrote: > >> Hi Andy. > >> > >> Interesting, have a look at > >> http://www.rsgb-spectrumforum.org.uk/radiation_theory.htm where via > >> the > >> 500kHz section (so presumably meant for electrically small > >> antennas) it says > >> "It is generally well known that the far-field is predominantly a > >> radiation > >> field; this is certainly true when the distance is greater then 10 > >> x > >> lambda/2pi." So there seems to be a factor of 10 difference from > >> your > >> equation. > >> > >> So using the RSGB paper, far field equates to 955 metres. Since the > >> CCIR > >> curves for LF/MF propagation give 3mV/m at 1km for 100mW erp and is > >> within > >> the distance ground conductivity has much effect, that's where I > >> have been > >> measuring. > >> > >> 73 Malcolm > >> (G3NZP) > >> > >> ----- Original Message ----- > >> From: "Andy Talbot" > >> To: > >> Sent: Friday, September 28, 2007 10:58 AM > >> Subject: Re: LF: A question of calibration > >> > >> > >> > There appear to be two meanings to the term "far field" when > >> > applied > >> > to antennas. One is usually reserved for electrically LARGE > >> > antennas > >> > and is the point where the wavefront can be considered to be > >> > planar. > >> > This distance is usually taken to be > >> > 2.D^2/lambda, where D = largest antenna dimension and lambda = > >> > wavelength. > >> > > >> > For electrically small antennas, the "far field" is beyond where > >> > the > >> > magnetic and electric components (which roll off faster than the > >> > 1 / > >> > R^2 of the radiation field) can be considered to be > >> > insignificant. > >> > This value is usually taken as being > >> > lambda / (2.pi) > >> > > >> > Andy G4JNT > >> > > >> > > >> > FOr LF field strength measurement > >> > > >> > On 28/09/2007, Malcolm Harman wrote: > >> >> John. > >> >> > >> >> Fascinating stuff and all your are papers duly saved. I sort of > >> >> knew > >> >> PA0SE > >> >> must be right and while E/H = 377 ohms between the Helmholtz > >> >> coils, we > >> >> have > >> >> to go to the far field of an antenna before a "plane" wave is > >> >> sufficiently > >> >> well formed and once again E/H = 377 ohms. Thanks for the > >> >> clarification. > >> >> > >> >> 73 Malcolm. > >> >> > >> >> ----- Original Message ----- > >> >> From: "John Andrews" > >> >> To: > >> >> Sent: Thursday, September 27, 2007 8:40 PM > >> >> Subject: Re: LF: A question of calibration > >> >> > >> >> > >> >> > Malcolm, > >> >> > > >> >> >> Hi. Can anyone reassure me. > >> >> > > >> >> > Be reassured. Your meter is measuring the magnetic field, and > >> >> > the > >> >> > calibration setup is primarily generating a magnetic field. > >> >> > The cal is > >> >> > being done under near-field conditions to permit the use of > >> >> > low power > >> >> > and > >> >> > take advantage of knowing the mag field accurately based on > >> >> > geometry > >> >> > and > >> >> > current measurement. The scale conversion to electric field > >> >> > remains > >> >> > valid > >> >> > as long as you agree to take your real measurements under > >> >> > far-field > >> >> > conditions. > >> >> > > >> >> > A further discussion of calibration techniques including a > >> >> > simpler > >> >> > arrangement than Helmholtz coils may be found at: > >> >> > http://www.w1tag.com/LF_FSM.htm > >> >> > > >> >> > John Andrews, W1TAG > >> >> > > >> >> > > >> >> > >> >> > >> >> > >> >> > >> > > >> > > >> > >> > >> > >> > > > > > > -- > > No virus found in this incoming message. > > Checked by AVG Free Edition. > > Version: 7.5.488 / Virus Database: 269.13.32/1033 - Release Date: > > 27/09/2007 11:06 > > > > > >