Return-Path: Received: from mtain-di07.r1000.mx.aol.com (mtain-di07.r1000.mx.aol.com [172.29.64.11]) by air-dc04.mail.aol.com (v129.4) with ESMTP id MAILINDC041-86004cb4c63d131; Tue, 12 Oct 2010 16:34:05 -0400 Received: from post.thorcom.com (post.thorcom.com [195.171.43.25]) by mtain-di07.r1000.mx.aol.com (Internet Inbound) with ESMTP id 31CBD380000D5; Tue, 12 Oct 2010 16:34:03 -0400 (EDT) Received: from majordom by post.thorcom.com with local (Exim 4.14) id 1P5lW8-0000d8-Bx for rs_out_1@blacksheep.org; Tue, 12 Oct 2010 21:32:12 +0100 Received: from [195.171.43.32] (helo=relay1.thorcom.net) by post.thorcom.com with esmtp (Exim 4.14) id 1P5lW7-0000cr-Gb for rsgb_lf_group@blacksheep.org; Tue, 12 Oct 2010 21:32:11 +0100 Received: from relay2.uni-heidelberg.de ([129.206.210.211]) by relay1.thorcom.net with esmtp (Exim 4.63) (envelope-from ) id 1P5lW6-0007aU-MN for rsgb_lf_group@blacksheep.org; Tue, 12 Oct 2010 21:32:11 +0100 Received: from ix.urz.uni-heidelberg.de (cyrus-portal.urz.uni-heidelberg.de [129.206.100.176]) by relay2.uni-heidelberg.de (8.13.8/8.13.8) with ESMTP id o9CKVoW9030719 (version=TLSv1/SSLv3 cipher=DHE-RSA-AES256-SHA bits=256 verify=NO) for ; Tue, 12 Oct 2010 22:31:51 +0200 Received: from extmail.urz.uni-heidelberg.de (extmail.urz.uni-heidelberg.de [129.206.100.140]) by ix.urz.uni-heidelberg.de (8.13.8/8.13.8) with ESMTP id o9CKW9qQ013138 (version=TLSv1/SSLv3 cipher=DHE-RSA-AES256-SHA bits=256 verify=NO) for ; Tue, 12 Oct 2010 22:32:09 +0200 Received: from [147.142.13.73] (vpn513-073.rzuser.uni-heidelberg.de [147.142.13.73]) by extmail.urz.uni-heidelberg.de (8.13.4/8.13.1) with ESMTP id o9CKVrX6008928 (version=TLSv1/SSLv3 cipher=DHE-RSA-AES256-SHA bits=256 verify=NO) for ; Tue, 12 Oct 2010 22:31:55 +0200 Message-ID: <4CB4C5CC.4000505@iup.uni-heidelberg.de> Date: Tue, 12 Oct 2010 22:32:12 +0200 From: =?ISO-8859-15?Q?Stefan_Sch=E4fer?= User-Agent: Mozilla/5.0 (Windows; U; Windows NT 6.1; de; rv:1.9.1.11) Gecko/20100711 Thunderbird/3.0.6 MIME-Version: 1.0 To: rsgb_lf_group@blacksheep.org X-Spam-Score: 2.1 (++) X-Spam-Report: autolearn=disabled,HTML_00_10=0.642,HTML_MESSAGE=0.001,RATWARE_GECKO_BUILD=1.426 Subject: LF: Questions and resonating tests and measurements on a 700m wire antenna at 137 kHz Content-Type: multipart/alternative; boundary="------------050601040600010003010208" 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 x-aol-global-disposition: G x-aol-sid: 3039ac1d400b4cb4c63a4ebe X-AOL-IP: 195.171.43.25 X-AOL-SPF: domain : blacksheep.org SPF : none X-Mailer: Unknown (No Version) --------------050601040600010003010208 Content-Type: text/plain; charset=ISO-8859-15; format=flowed Content-Transfer-Encoding: quoted-printable X-MIME-Autoconverted: from 8bit to quoted-printable by relay2.uni-heidelberg.de id o9CKVoW9030719 Dear LF, Today i have done some measurements on my "earth antenna" at 137 kHz.=20 The antenna was used as a ground loop antenna (far end grounded) and as=20 a inv-L antenna (far end ungrounded). Winthin the last days the antenna was optimised. Now the first 250m are=20 about 8 m above ground (average). The wire was replaced by a olive-green= =20 military wire (steel-copper-silver, UV resistant insulation) which makes= =20 the antenna rather invisible. The rest of the antenna is still in a=20 height of about 4m (average). I assume these 4m height difference could=20 make a significant difference in the efficiency on LF (not so much on VLF)= . The H Bridge PA was used for the tests. This PA can fed the antenna from= =20 10 Hz (!) to 200 kHz as seen today. The applied power (DC input) in the=20 tests was about 25 W. A 5 pole low pass filter was applied on the PA outpu= t. First i wanted to measure u(t), i(t) and the phase by an oscilloscope=20 but this is not really running sufficient when supplied by the generator= =20 (trigger and display problems). So i choose the LF tuning meter (ON7YDs=20 website) which i built in 2003. When configuring the wire (abt 700m length and abt 600m electrode=20 spacing) as a ground loop antenna, it is resonated with a series L (not=20 C!) of about 800 =B5H. Then, its Z =3D 840 Ohm. No matter what the radiati= on=20 resistance is. Field strength measurements on my LF grabber make=20 probably no sense due to the low distance. I have to compare both=20 configurations in a further test, maybe this weekend. After disconnecting the ground rods at the far end the antenna (now=20 inv-L config) was resonated by using a L of just 250 =B5H (estimation).=20 The Impedance Z was then measured to be 440 Ohm! (U=3D73,3 V * I=3D166mA). What does these values tell us? I have not yet completely understand the= =20 whole dependency i think. _So i am looking forward to your ideas and=20 comments! _It seems as if the losses have been reduced in the inv-L case. But what= =20 about the radiation resistance? How can we compare those different=20 antenna types? The ground losses on VLF and down to 10 Hz (quasi DC) are about 700 Ohm,= =20 today. Since the antenna is _not_ short against lambda (i.e. it is even=20 longer than lambda/4), the antenna acts not like a pure loop and not as=20 a usual back garden LF antenna. Additionally, the ground losses are very= =20 high here! The ground electrode on the fed point could be about 350 Ohm,= =20 so 50% of the total loop losses on VLF. But, theoretically, the=20 radiation resistance could be some Ohms (?) due to the antenna length.=20 If it will become longer (...lambda/2), the ground electrodes current=20 decreases, and so the losses? Quite difficult and interesting, isn't it? My idea is just to do further tests, hoping to be copied at many LF=20 stations, since this is the final goal :-) A simulation seems to be very= =20 difficult, due to the many unknown parameters... I want to find what is the best configuration (loop or inv-L) and i want= =20 to increase the antenna to 1000 m length! :-) Then i will build a tuner=20 with fixed components. This will be an easy job since the voltages and=20 currents are moderate! :-) The impedance should be transformed to 50 Ohm= =20 (sincei have a 25m long RG58 cable to the class E TX that should be used= =20 later) and i hope i can improve the RX for that antenna. 73, Stefan/DK7FC --------------050601040600010003010208 Content-Type: text/html; charset=ISO-8859-15 Content-Transfer-Encoding: quoted-printable X-MIME-Autoconverted: from 8bit to quoted-printable by relay2.uni-heidelberg.de id o9CKVoW9030719 Dear LF,

Today i have done some measurements on my "earth antenna" at 137 kHz. The antenna was used as a ground loop antenna (far end grounded) and as a inv-L antenna (far end ungrounded).

Winthin the last days the antenna was optimised. Now the first 250m are about 8 m above ground (average). The wire was replaced by a olive-green military wire (steel-copper-silver, UV resistant insulation) which makes the antenna rather invisible. The rest of the antenna is still in a height of about 4m (average). I assume these 4m height difference could make a significant difference in the efficiency on LF (not so much on VLF).

The H Bridge PA was used for the tests. This PA can fed the antenna from 10 Hz (!) to 200 kHz as seen today. The applied power (DC input) in the tests was about 25 W. A 5 pole low pass filter was applied on the PA output.

First i wanted to measure u(t), i(t) and the phase by an oscilloscope but this is not really running sufficient when supplied by the generator (trigger and display problems). So i choose the LF tuning meter (ON7YDs website) which i built in 2003.

When configuring the wire (abt 700m length and abt 600m electrode spacing) as a ground loop antenna, it is resonated with a series L (not C!) of about 800 =B5H. Then, its Z =3D 840 Ohm. No matter what the radiation resistance is. Field strength measurements on my LF grabber make probably no sense due to the low distance. I have to compare both configurations in a further test, maybe this weekend.

After disconnecting the ground rods at the far end the antenna (now inv-L config) was resonated by using a L of just 250 =B5H (estimation). The Impedance Z was then measured to be 440 Ohm! (U=3D73,3 V * I=3D166mA).=

What does these values tell us? I have not yet completely understand the whole dependency i think. So i am looking forward to your ideas and comments!

It seems as if the losses have been reduced in the inv-L case. But what about the radiation resistance? How can we compare those different antenna types?
The ground losses on VLF and down to 10 Hz (quasi DC) are about 700 Ohm, today. Since the antenna is not short against lambda (i.e. it is even longer than lambda/4), the antenna acts not like a pure loop and not as a usual back garden LF antenna. Additionally, the ground losses are very high here! The ground electrode on the fed point could be about 350 Ohm, so 50% of the total loop losses on VLF. But, theoretically, the radiation resistance could be some Ohms (?) due to the antenna length. If it will become longer (...lambda/2), the ground electrodes current decreases, and so the losses? Quite difficult and interesting, isn't it?

My idea is just to do further tests, hoping to be copied at many LF stations, since this is the final goal :-) A simulation seems to be very difficult, due to the many unknown parameters...

I want to find what is the best configuration (loop or inv-L) and i want to increase the antenna to 1000 m length! :-) Then i will build a tuner with fixed components. This will be an easy job since the voltages and currents are moderate! :-) The impedance should be transformed to 50 Ohm (sincei have a 25m long RG58 cable to the class E TX that should be used later) and i hope i can improve the RX for that antenna.


73, Stefan/DK7FC



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