Return-Path: Received: from mtain-di01.r1000.mx.aol.com (mtain-di01.r1000.mx.aol.com [172.29.64.5]) by air-me01.mail.aol.com (v129.4) with ESMTP id MAILINME012-8ba14d888d3b64; Tue, 22 Mar 2011 07:51:23 -0400 Received: from post.thorcom.com (post.thorcom.com [195.171.43.25]) by mtain-di01.r1000.mx.aol.com (Internet Inbound) with ESMTP id 8D2F3380000B2; Tue, 22 Mar 2011 07:51:13 -0400 (EDT) Received: from majordom by post.thorcom.com with local (Exim 4.14) id 1Q205v-0001LP-ME for rs_out_1@blacksheep.org; Tue, 22 Mar 2011 11:49:51 +0000 Received: from [195.171.43.32] (helo=relay1.thorcom.net) by post.thorcom.com with esmtp (Exim 4.14) id 1Q205u-0001LG-Pn for rsgb_lf_group@blacksheep.org; Tue, 22 Mar 2011 11:49:50 +0000 Received: from imr-da05.mx.aol.com ([205.188.105.147]) by relay1.thorcom.net with esmtp (Exim 4.63) (envelope-from ) id 1Q205t-0001K3-51 for rsgb_lf_group@blacksheep.org; Tue, 22 Mar 2011 11:49:50 +0000 Received: from imo-ma04.mx.aol.com (imo-ma04.mx.aol.com [64.12.78.139]) by imr-da05.mx.aol.com (8.14.1/8.14.1) with ESMTP id p2MBnPp3020148 for ; Tue, 22 Mar 2011 07:49:25 -0400 Received: from MarkusVester@aol.com by imo-ma04.mx.aol.com (mail_out_v42.9.) id l.1011.4169c31 (43983) for ; Tue, 22 Mar 2011 07:49:16 -0400 (EDT) Received: from smtprly-me01.mx.aol.com (smtprly-me01.mx.aol.com [64.12.95.102]) by cia-dd04.mx.aol.com (v129.9) with ESMTP id MAILCIADD048-b2934d888cb6268; Tue, 22 Mar 2011 07:49:16 -0400 Received: from webmail-m018 (webmail-m018.sim.aol.com [64.12.101.102]) by smtprly-me01.mx.aol.com (v129.9) with ESMTP id MAILSMTPRLYME013-b2934d888cb6268; Tue, 22 Mar 2011 07:49:10 -0400 References: <4D83D475.9090609@telus.net> <000b01cbe622$6a23f8d0$8d01a8c0@JAYDELL>, ,<4D86BD6F.8020006@telus.net> <4D8736CB.8040509@telus.net> <4D87E247.5020100@iup.uni-heidelberg.de> To: rsgb_lf_group@blacksheep.org Date: Tue, 22 Mar 2011 07:49:10 -0400 In-Reply-To: <4D87E247.5020100@iup.uni-heidelberg.de> X-MB-Message-Source: WebUI MIME-Version: 1.0 From: Markus Vester X-MB-Message-Type: User X-Mailer: AOL Webmail 33426-STANDARD Received: from 194.138.39.55 by webmail-m018.sysops.aol.com (64.12.101.102) with HTTP (WebMailUI); Tue, 22 Mar 2011 07:49:10 -0400 Message-Id: <8CDB69E4AD7AA3C-1490-33A81@webmail-m018.sysops.aol.com> X-Spam-Flag:NO X-AOL-SENDER: MarkusVester@aol.com X-Spam-Score: 1.2 (+) X-Spam-Report: autolearn=disabled,FORGED_AOL_TAGS=0.281,HTML_10_20=0.945,HTML_MESSAGE=0.001,UNPARSEABLE_RELAY=0.001 Subject: VLF: Resonate the antenna, or not? Content-Type: multipart/alternative; boundary="--------MB_8CDB69E4AE12FC4_1490_71A4A_webmail-m018.sysops.aol.com" X-Spam-Checker-Version: SpamAssassin 2.63 (2004-01-11) on post.thorcom.com X-Spam-Level: X-Spam-Status: No, hits=0.1 required=5.0 tests=FORGED_AOL_TAGS, HTML_FONTCOLOR_UNKNOWN,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: 3039ac1d40054d888d315a6d X-AOL-IP: 195.171.43.25 X-AOL-SPF: domain : blacksheep.org SPF : none ----------MB_8CDB69E4AE12FC4_1490_71A4A_webmail-m018.sysops.aol.com Content-Transfer-Encoding: quoted-printable Content-Type: text/plain; charset="utf-8" Hi Stefan,=20 you are raising the interesting question of how important it is to resonat= e the antenna. I think it boils down to a comparison of the amplifier effi= ciency versus the Q factor of the matching element. Without the matching element, the amplifier (really a switchmode DC-to-AC= converter) has to transfer the reactive power back and forth between the= load and the power supply capacitors. With ideal switches, indeed nothing= would be lost. But with finite efficiency, you will loose a portion of (1= - eta), eg. 2 % per cycle if your amplifier had 98% efficiency measured= into a real load. On he other hand, if your loop was resonated using a ca= pacitor with Q-factor 500, you would dissipate only 0.2% per cycle in it. =20 Jim's small VLF loop example (0.1 + j 2.2 ohms) had a Q of only 22, ie. 1/= Q =3D 4.5% of the energy is lost per cycle. So the total power comparison= would be 6.5% for the amplifier version versus 4.7% for the capacitor -= really not that much difference.=20 But as Stefan says, the amplifier would have to be big enough to handle al= l the reactive power (VxA). If fed by a large enough power supply, the ver= y same amplifier could deliver 2.2 kW and raise the radiated power by a fa= ctor of Q, ie. 13 dB. BTW There exists a similar criterion for active receive antennas: If you= have a small capacitive probe and resonate it with a coil, the coil losse= s will add in some resistive noise. In a ferrite loopstick, a (nearly loss= less) capacitor is typically used to tune out the inductive reactance, but= this makes the antenna narrowband.=20 If on the other hand you do not compensate the reactance, you can still no= ise-match the preamp to the modulus of the source impedance, at the penalt= y that it's own noise temperature will increase by a factor of Q. For very= low preamp noise figures (ie. Tpreamp < Tantenna / Q), adding the tuning= element brings little or no benefit for the system noise figure. Best wishes, Markus (DF6NM) -----Urspr=C3=BCngliche Mitteilung-----=20 Von: Stefan Sch=C3=A4fer An: rsgb_lf_group@blacksheep.org Verschickt: Di., 22. Mrz. 2011, 0:41 Thema: Re: LF: Loop TX antennas at VLF... Hi Scott,=20 I have some comments, yes.=20 I would try not to resonate the PA but drive it with a H bridge PA that ca= n handle pretty much reactive power. If you think about Rik's and Jim's= calculation and assume 70 V across the loop, while taking 32 A, you ( ah,= you have 115 V mains?) you may directly rectify the mains and drive a H= bride with it and feed the loop with that switched rectified voltage. So= you would get about 75 A. That's not a problem for some well choosen FETs= and caps (on the DC side!). Jim and Wolf already suggested to try that.= =20 I know it from my kite antenna: When the wind is poor or if the wire gets= disconnected from the hot end of the coil (this happened 1x), the Z of th= e primary winding (unresonated) is the current limiting factor. I am still= switching at 300 VDC and 8970 Hz to a bundle of wire of 50 turns on a wat= er barrel (say 70 cm diameter on the lower side). There will be heavy reac= tive currents but that is no problem for the FETs! The resistive losses in= the whole circuit (measured on the 230V AC side by a true rms multimeter)= are below 25 W in such a situation, including the driver/exciter power. I think it wouldn't be a good idea to try this with a standard audio amp..= .. My FETs are simple IRFP460, about 2.5 EUR each. There are no ferrite parts= in the whole circuit! But, unfortunately, i think there is another problem: If you try that with= your loop, who will be the next receiving station? What distance? Even if= you run 100A rms into that loop (BTW, what is the area?) you will radiate= probably below 1 mW ERP...=20 Now reading the above comments from the others ;-) Best 73, Stefan EI/DK7FC, currently in IO62SI41IS Am 21.03.2011 12:30, schrieb Scott Tilley:=20 Hi Rik Thanks for this! I may be comparing apples to oranges alittle (maybe alot). The loop I hav= e would only require a 1.8uF cap and this coupled with a higher Q makes fo= r a little dicier tuning scenario. I concede this scenario is not as bad= as I first thought when I thought about this briefly when Stephan enquire= d about a possible test from here many months ago. A careful review of you= r summary Rik was very helpful, thanks to all that contributed. =20 The two big , and one minor design issues to get maximum potential from a= loop down at 9KHz will be: 1) Current handling capability of the caps. 2) Tuning capability. 3) Ferrite saturation for the matching xfmr... Or should we use ferrite? #1 can be resolved, I think, as you have suggested with the use of LOTS of= polypropylene caps... However, #2 will likely be the difficult one and be abit of an engineering= challenge as the small loop proposed below may just get away with course= tuning but as you get larger and reduce the Rac the Q goes up and so does= the tuning criteria. This is where I got stuck with my original glimpses= of thought on this. We can't rely on a good old vacuum variable so some= sort of other idea...=20 Hmmm, how about a special decade type box made of Polypropylene caps? The= box could be designed once the loop's characteristics after installation= have been bracketed in... The other downside of polypropylene caps will be there tendency to drift= once you put alot of current into them, so you'll need lots! This drifti= ng issue could be very problematic as I discovered on 137 with anything ot= her than good transmitting micas with high current ratings at the operatin= g frequency. =20 Based on the results of others using mains transformers on 9KHz maybe item= #3 is not a big problem after all? Anyone have a comment here? Looking forward to more ideas as this is tweaking my interest into buildin= g another tuner. 73 es TU Scott VE7TIL ... ----------MB_8CDB69E4AE12FC4_1490_71A4A_webmail-m018.sysops.aol.com Content-Transfer-Encoding: quoted-printable Content-Type: text/html; charset="utf-8"
Hi Stefan,
 
you are raising the interesting question of how important it is = to resonate the antenna. I think it boils down to a comparison of the ampl= ifier efficiency versus the Q factor of the matching element.

Without the matching element, the amplifier (really a switchmode DC-to-AC= converter) has to transfer the reactive power back and forth between the= load and the power supply capacitors. With ideal switches, indeed nothing= would be lost. But with finite efficiency, you will loose a portion of (1= - eta), eg. 2 % per cycle if your amplifier had 98% efficiency measured= into a real load. On he other hand, if your loop was reson= ated using a capacitor with Q-factor 500, you would dissipate only 0.= 2% per cycle in it.
 
Jim's small VLF loop example (0.1 + j 2.2 ohms) had a Q of only 22,= ie. 1/Q =3D 4.5% of the energy is lost per cycle. So the total power comp= arison would be 6.5% for the amplifier version versus 4.7% for the capacit= or - really not that much difference.
 
But as Stefan says, the amplifier would have to be big enough to= handle all the reactive power (VxA). If fed by a large enough power suppl= y, the very same amplifier could deliver 2.2 kW and raise the radiated pow= er by a factor of Q, ie. 13 dB.
 
 
BTW There exists a similar criterion for active receive antennas= : If you have a small capacitive probe and resonate it with a co= il, the coil losses will add in some resistive noise. In a ferrite lo= opstick, a (nearly lossless) capacitor is typically used to tune out the= inductive reactance, but this makes the antenna narrowband.
 
If on the other hand you do not compensate the reactance,= you can still noise-match the preamp to the modulus of the source im= pedance, at the penalty that it's own noise temperature will inc= rease by a factor of Q. For very low preamp noise figures (ie. Tpream= p < Tantenna / Q), adding the tuning element brings little or= no benefit for the system noise figure.
 
Best wishes,
Markus (DF6NM)
 
 
 
-----Urspr=C3=BCngliche Mitteilung-----
Von: Stefan Sch=C3=A4fer <schaefer@iup.uni-heidelberg.de>
An: rsgb_lf_group@blacksheep.org
Verschickt: Di., 22. Mrz. 2011, 0:41
Thema: Re: LF: Loop TX antennas at VLF...

Hi Scott,

I have some comments, yes.
I would try not to resonate the PA but drive it with a H bridge PA th= at can handle pretty much reactive power. If  you think about Rik's= and Jim's calculation and assume 70 V across the loop, while taking 32 A,= you ( ah, you have 115 V mains?) you may directly rectify the mains and= drive a H bride with it and feed the loop with that switched rectified vo= ltage. So you would get about 75 A. That's not a problem for some well cho= osen FETs and caps (on the DC side!). Jim and Wolf already suggested to tr= y that.
I know it from my kite antenna: When the wind is poor or if the wire= gets disconnected from the hot end of the coil (this happened 1x), the Z= of the primary winding (unresonated) is the current limiting factor. I am= still switching at 300 VDC and 8970 Hz to a bundle of wire of 50 turns on= a water barrel (say 70 cm diameter on the lower side). There will be heav= y reactive currents but that is no problem for the FETs! The resistive los= ses in the whole circuit (measured on the 230V AC side by a true rms multi= meter) are below 25 W in such a situation, including the driver/exciter po= wer.
I think it wouldn't be a good idea to try this with a standard audio amp..= ..
My FETs are simple IRFP460, about 2.5 EUR each. There are no ferrite= parts in the whole circuit!

But, unfortunately, i think there is another problem: If you try that with= your loop, who will be the next receiving station? What distance? Even if= you run 100A rms into that loop (BTW, what is the area?) you will radiate= probably below 1 mW ERP...

Now reading the above comments from the others ;-)

Best 73, Stefan EI/DK7FC, currently in IO62SI41IS



Am 21.03.2011 12:30, schrieb Scott Tilley:
Hi Rik

Thanks for this!

I may be comparing apples to oranges alittle (maybe alot).  The loop= I have would only require a 1.8uF cap and this coupled with a higher Q ma= kes for a little dicier tuning scenario.  I concede this scenario is= not as bad as I first thought when I thought about this briefly when Step= han enquired about a possible test from here many months ago. A careful re= view of your summary Rik was very helpful, thanks to all that contributed.=  

The two big , and one minor design issues to get maximum potential from a= loop down at 9KHz will be:
1) Current handling capability of the caps.
2) Tuning capability.
3) Ferrite saturation for the matching xfmr...  Or should we use ferr= ite?

#1 can be resolved, I think, as you have suggested with the use of LOTS of= polypropylene caps...

However, #2 will likely be the difficult one and be abit of an engineering= challenge as the small loop proposed below may just get away with course= tuning but as you get larger and reduce the Rac the Q goes up and so does= the tuning criteria.  This is where I got stuck with my original gli= mpses of thought on this.  We can't rely on a good old vacuum variabl= e so some sort of other idea...

Hmmm, how about a special decade type box made of Polypropylene caps? = ; The box could be designed once the loop's characteristics after installa= tion have been bracketed in...

The other downside of polypropylene caps will be there tendency to drift= once you put alot of current into them, so you'll need lots!  This= drifting issue could be very problematic as I discovered on 137 with anyt= hing other than good transmitting micas with high current ratings at the= operating frequency. 

Based on the results of others using mains transformers on 9KHz maybe item= #3 is not a big problem after all?  Anyone have a comment here?

Looking forward to more ideas as this is tweaking my interest into buildin= g another tuner.

73 es TU
Scott
VE7TIL
...
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