X-GM-THRID: 1201092871102915278 X-Gmail-Labels: rsgb lf X-Gmail-Received: 922029cc524d02e47d2694cc6bd67d9a6db6700c Delivered-To: daveyxm@gmail.com Received: by 10.54.70.6 with SMTP id s6cs14424wra; Wed, 19 Apr 2006 08:34:51 -0700 (PDT) Received: by 10.48.233.4 with SMTP id f4mr4205669nfh; Wed, 19 Apr 2006 08:34:51 -0700 (PDT) Return-Path: Received: from post.thorcom.com (post.thorcom.com [193.82.116.20]) by mx.gmail.com with ESMTP id q27si651312nfc.2006.04.19.08.34.50; Wed, 19 Apr 2006 08:34:51 -0700 (PDT) Received-SPF: neutral (gmail.com: 193.82.116.20 is neither permitted nor denied by best guess record for domain of owner-rsgb_lf_group@blacksheep.org) Received: from majordom by post.thorcom.com with local (Exim 4.14) id 1FWEeo-0008Tn-58 for rs_out_1@blacksheep.org; Wed, 19 Apr 2006 16:31:54 +0100 Received: from [193.82.59.130] (helo=relay2.thorcom.net) by post.thorcom.com with esmtp (Exim 4.14) id 1FWEen-0008Te-Ba for rsgb_lf_group@blacksheep.org; Wed, 19 Apr 2006 16:31:53 +0100 Received: from cas-mta3-fe.casema.nl ([83.80.1.28] helo=mta-fe.casema.nl) by relay2.thorcom.net with esmtp (Exim 4.51) id 1FWFyD-0005YQ-Mu for rsgb_lf_group@blacksheep.org; Wed, 19 Apr 2006 17:56:03 +0100 Received: from s9z5i6.casema.nl (53556AF3.cable.casema.nl [83.85.106.243]) by mta-fe.casema.nl (Postfix) with ESMTP id 430CA3F82 for ; Wed, 19 Apr 2006 17:31:40 +0200 (CEST) Message-Id: <6.1.0.6.2.20060419171908.02a17870@127.0.0.1> X-Sender: dickrollema@casema.nl#mail.casema.nl@127.0.0.1 (Unverified) X-Mailer: QUALCOMM Windows Eudora Version 6.1.0.6 Date: Wed, 19 Apr 2006 17:33:27 +0200 To: rsgb_lf_group@blacksheep.org From: Dick Rollema In-Reply-To: <5.1.0.14.0.20060419162451.02431a98@u0019445.kuleuven.be> References: <6.1.0.6.2.20060419144651.02a19240@127.0.0.1> <5.1.0.14.0.20060419162451.02431a98@u0019445.kuleuven.be> Mime-Version: 1.0 X-Antivirus: avast! (VPS 0616-2, 18-04-2006), Outbound message X-Antivirus-Status: Clean X-Spam-Score: -0.3 (/) X-Spam-Report: autolearn=disabled,AWL=-0.614,FORGED_RCVD_HELO=0.05,HTML_10_20=0.295,HTML_MESSAGE=0.001 Subject: Re: LF: Top load coil at ground level? Content-Type: multipart/alternative; boundary="=====================_12670540==.ALT" 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=HTML_MESSAGE 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 Status: O X-Status: X-Keywords: X-UID: 6687 --=====================_12670540==.ALT Content-Type: text/plain; charset="us-ascii"; format=flowed Rik, ON 7YD wrote At 16:29 19-4-06, you wrote: >Hi Dick, > >I guess you are right with >"The stub functions as a transmission line to transfer the inductive >reactance of the coil to the top of the radiator." > >But I am afraid that for any reasonable antenna height (< 50..100m) the >stub is that short (in wavelengths) that it will hardly transfer any reactance. To check this I took as a stub 50ft of 600 ohm open line. At one end I connected a coil of 2mH, a typical value I think for a top load coil. Its reactance at 136kHz is 1700 ohm. Using a transmission line program by ARRL I find that at the other end of the line a reactance of 1978 ohm appears, which looks like a coil of 2.32mH. So it seems to work. >What is the result when you model both quarter wave 80m antennas (+/- 20 m >height) for 2200m ? The antennas and the distance between the legs of the stub (20cm) are so small in wavelengths that the program does not work. 73, Dick, PA0SE >At 14:54 19/04/2006 +0200, you wrote: >>To All from PA0SE, >> >>By chance I came across an interesting article in the Dutch weekly (!) >>magazine Radio Expres of 11 January 1934. It referred to an article in >>the Proceedings of the IRE of December 1933 by Nickle, Dome and Brown on >>a procedure to increase of the feed point impedance of a vertical antenna >>by means of top loading. A normal way is to use a series resonant circuit >>as in fig.1, consisting of a capacitive hat and a coil. The coil is in a >>awkward position for tuning. The alternative by Nickle, Dome and Brown is >>to use a short circuited stub slightly shorter than an quarter wave that >>at its top end produces the proper inductive reactance for series >>resonance with the capacitive hat. Indicated in fig. 2a. The system is >>tuned by moving the short circuit at the bottom up or down. The left leg >>of the stub is doubling as the radiator. An easier way of tuning is to >>make the stub too short and lengthening it with a coil(b) or a stub that >>is too long and shortening it by a capacitor (c). I modelled a quarter >>wave vertical for 80 m according to (c) using Antenna Optimizer by Brian >>Beezley, K6STI. When in resonance the feed point impedance was raised >>from 36 ohm without top load to 4925 ohm! The radiation diagram was >>identical to the one for the unloaded vertical within a few tenths of a dB. >> >>It occurred to me that the system could perhaps also be used for a 136kHz >>vertical. Using system (b) in fig.2 the loading coil between top of the >>radiator and topload could be at ground level. The stub functions as a >>transmission line to transfer the inductive reactance of the coil to the >>top of the radiator. Of course a second coil could be inserted between >>bottom of the stub and ground for matching and feeding of the antenna. >> >>What do you think? >> >>73, Dick, PA0SE >> >> --=====================_12670540==.ALT Content-Type: text/html; charset="iso-8859-1" Content-Transfer-Encoding: quoted-printable Rik, ON 7YD wrote

At 16:29 19-4-06, you wrote:
Hi Dick,

I guess you are right with
"
The stub functions as a transmission line to transfer the inductive reactance of the coil to the top of the radiator."

But I am afraid that for any reasonable antenna height (< 50..100m) the stub is that short (in wavelengths) that it will hardly transfer any reactance.

To check  this I took as a stub 50ft of 600 ohm open line. At one end I connected a coil of 2mH, a typical value I think for a top load coil. Its reactance at 136kHz is 1700 ohm.
Using a transmission line program by ARRL I find that at the other end of the line a reactance of 1978 ohm appears, which looks like a coil of 2.32mH.
So it seems to work.

What is th= e result when you model both quarter wave 80m antennas (+/- 20 m height) for 2200m ?

The antennas and the distance between the legs of the stub (20cm) are so small in wavelengths that the program does not work.

73, Dick, PA0SE


At 14:54 19/04/2006 +0200, you wrote:
To All from PA0SE,

By chance I came across an interesting article in the Dutch weekly (!) magazine Radio Expres of 11 January 1934. It referred to an article in the Proceedings of the IRE of December 1933 by Nickle, Dome and Brown on a procedure to increase of the feed point impedance of a vertical antenna by means of top loading. A normal way is to use a series resonant circuit as in fig.1, consisting of a capacitive hat and a coil. The coil is in a awkward position for tuning. The alternative by Nickle, Dome and Brown is to use a short circuited stub slightly shorter than an quarter wave that at its top end produces the proper inductive reactance for series resonance with the capacitive hat. Indicated in fig. 2a. The system is tuned by moving the short circuit at the bottom up or down. The left leg of the stub is doubling as the radiator. An easier way of tuning is to make the stub too short and lengthening it with a coil(b) or a stub that is too long and shortening it by a capacitor (c). I modelled a quarter wave vertical for 80 m according to (c) using Antenna Optimizer by Brian Beezley, K6STI. When in resonance the feed point impedance was raised from 36 ohm without top load to 4925 ohm! The radiation diagram was identical to the one for the unloaded vertical within a few tenths of a dB.

It occurred to me that the system could perhaps also be used for a 136kHz vertical. Using system (b) in fig.2 the loading coil between top of the radiator and topload could be at ground level. The stub functions as a transmission line to transfer the inductive reactance of the coil to the top of the radiator. Of course a second coil could be inserted between bottom of the stub and ground for matching and feeding of the antenna.

What do you think?

73, Dick, PA0SE

     
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