Return-Path: Received: from rly-yc05.mail.aol.com (rly-yc05.mail.aol.com [172.18.205.148]) by air-yc02.mail.aol.com (v119.9) with ESMTP id MAILINYC22-1da46fd135b102; Fri, 28 Sep 2007 10:45:38 -0400 Received: from post.thorcom.com (post.thorcom.com [193.82.116.20]) by rly-yc05.mail.aol.com (v119.9) with ESMTP id MAILRELAYINYC54-1da46fd135b102; Fri, 28 Sep 2007 10:44:45 -0400 Received: from majordom by post.thorcom.com with local (Exim 4.14) id 1IbH4J-0003Gc-IJ for rs_out_1@blacksheep.org; Fri, 28 Sep 2007 15:43:51 +0100 Received: from [83.244.159.144] (helo=relay3.thorcom.net) by post.thorcom.com with esmtp (Exim 4.14) id 1IbH4H-0003GT-SZ for rsgb_lf_group@blacksheep.org; Fri, 28 Sep 2007 15:43:49 +0100 Received: from smtp9.ihug.co.nz ([203.109.136.109]) by relay3.thorcom.net with esmtp (Exim 4.63) (envelope-from ) id 1IbH4C-0002E0-IS for rsgb_lf_group@blacksheep.org; Fri, 28 Sep 2007 15:43:49 +0100 Received: from cust.filter3.content.ihug.net.nz (smtp.mailfilter3.ihug.co.nz) [10.80.50.3] by smtp9.ihug.co.nz with esmtp (Exim 4.60 #1 (Debian); Ihug conf #192) id 1IbH43-0006AC-ID; Sat, 29 Sep 2007 02:43:35 +1200 Ironport-Content-Filter: send-to-smtp Received: from 203-109-184-146.dsl.dyn.ihug.co.nz (HELO athlon1200) ([203.109.184.146]) by smtp.mailfilter3.ihug.co.nz with SMTP; 29 Sep 2007 02:43:35 +1200 Message-ID: <000001c801dd$a0ecc1d0$7900a8c0@athlon1200> From: "Dave Brown" To: References: <000a01c80132$aae29df0$83e41a52@enigma> <46FC071D.2090202@w1tag.com> <000601c801ae$38cc27a0$0fee1a52@enigma> <001d01c801c6$a918b420$0fee1a52@enigma> Date: Sat, 29 Sep 2007 02:31:07 +1200 MIME-Version: 1.0 X-Priority: 3 X-MSMail-Priority: Normal X-Mailer: Microsoft Outlook Express 6.00.2900.3138 X-MimeOLE: Produced By Microsoft MimeOLE V6.00.2900.3138 X-Spam-Score: 0.0 (/) X-Spam-Report: autolearn=disabled,none Subject: Re: LF: A question of calibration Content-Type: text/plain; format=flowed; charset="iso-8859-1"; reply-type=original 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 : 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 > >