Return-Path: Received: from mtain-dd11.r1000.mx.aol.com (mtain-dd11.r1000.mx.aol.com [172.29.64.151]) by air-da08.mail.aol.com (v127_r1.1) with ESMTP id MAILINDA084-86924ba0b95635f; Wed, 17 Mar 2010 07:13:27 -0500 Received: from post.thorcom.com (post.thorcom.com [193.82.116.20]) by mtain-dd11.r1000.mx.aol.com (Internet Inbound) with ESMTP id D7663380000BE; Wed, 17 Mar 2010 07:13:24 -0400 (EDT) Received: from majordom by post.thorcom.com with local (Exim 4.14) id 1NrrAH-0005n5-Vo for rs_out_1@blacksheep.org; Wed, 17 Mar 2010 11:11:53 +0000 Received: from [193.82.116.32] (helo=relay1.thorcom.net) by post.thorcom.com with esmtp (Exim 4.14) id 1NrrAH-0005mw-GR for rsgb_lf_group@blacksheep.org; Wed, 17 Mar 2010 11:11:53 +0000 Received: from lnx503.hrz.tu-darmstadt.de ([130.83.156.232]) by relay1.thorcom.net with esmtp (Exim 4.63) (envelope-from ) id 1NrrAF-000310-Ji for rsgb_lf_group@blacksheep.org; Wed, 17 Mar 2010 11:11:53 +0000 Received: from FILE-SERVER-HST.hst.e-technik.tu-darmstadt.de (File-Server-HST.hst.e-technik.tu-darmstadt.de [130.83.212.129]) by lnx503.hrz.tu-darmstadt.de (8.14.2/8.14.2/HRZ/PMX) with SMTP id o2HBBnAK026380 for ; Wed, 17 Mar 2010 12:11:50 +0100 (envelope-from schaefer@hst.tu-darmstadt.de) Received: from [127.0.0.1] (helo=File-Server-HST.hst.e-technik.tu-darmstadt.de) by FILE-SERVER-HST.hst.e-technik.tu-darmstadt.de with AVK MailGateway; for ; Wed, 17 Mar 2010 12:11:48 +0100 Content-class: urn:content-classes:message MIME-Version: 1.0 X-MimeOLE: Produced By Microsoft Exchange V6.5 Date: Wed, 17 Mar 2010 12:11:48 +0100 Message-ID: <38A51B74B884D74083D7950AD0DD85E82A1B66@File-Server-HST.hst.e-technik.tu-darmstadt.de> X-MS-Has-Attach: X-MS-TNEF-Correlator: <38A51B74B884D74083D7950AD0DD85E82A1B66@File-Server-HST.hst.e-technik.tu-darmstadt.de> Thread-Topic: TA, 300m and new PA? Thread-Index: AcrFt578v8TghsEfS0uW3zHNwiKmFQABJAEl References: <4BA0A501.5050506@abelian.org> From: =?iso-8859-1?Q?Stefan_Sch=E4fer?= To: X-AVK-Virus-Check: AVB 19.717;31.01.2010 X-PMX-TU: seen v0.99a by 5.5.9.388399, Antispam-Engine: 2.7.2.376379, Antispam-Data: 2010.3.17.105724 X-PMX-SPAMCHECK: outgoing mail X-Spam-Score: 0.0 (/) X-Spam-Report: autolearn=disabled,none Content-Type: multipart/mixed; boundary="----_=_NextPart_001_01CAC5C2.A33A08E9" Subject: VLF: TA, 300m and new PA? X-Spam-Checker-Version: SpamAssassin 2.63 (2004-01-11) on post.thorcom.com X-Spam-Level: X-Spam-Status: No, hits=0.3 required=5.0 tests=ORDER_NOW 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-VSS-INFO: 5400.1158/56350 X-AOL-VSS-CODE: clean x-aol-sid: 3039ac1d40974ba0b95426ff X-AOL-IP: 193.82.116.20 X-Mailer: Unknown (No Version) ------_=_NextPart_001_01CAC5C2.A33A08E9 Content-Type: text/plain; charset="iso-8859-1" Content-Transfer-Encoding: quoted-printable Paul, LF,=20 =20 So, if we have the approx formula for VLF propagation and know the range= of the noise floor at 8,97kHz, then what would be the TX power i have to= apply to a 300m vertical to reach Canada/USA, if there would be some well= equipped stations? You know the details of my antenna and if it is enlarged to 300m, it will= be approx: C=3D 1750pF, R(coil, DC)=3D100 Ohm, R(other losses)~400 Ohm,= =3D> antenna efficiency at 8,97kHz will be 0,0064%. In this case the limi= t will not be the antenna voltage but the maximum available power, that is= abt 600W. Would that be enough? ;-) =20 BTW, yesterday i got the idea to built a second PA (to have one in reserve= and to:) to get a better operation of the generator: In the moment the PA= works on 13,8V that is given bei a SMPS. If the carrier starts there is= a power shift of 100% at since the SMPS always takes the needed power fro= m the generator (even if the 230V droppes to 80V), the fuel/speed regulati= on becomes unstable. I often noticed a longer drive swing that can take up= to one minute (depending on the power and parallel switched batteries).= That would become a problem if i really want to take the maximum power th= e generator gives! So, if i directly rectify the 230V (with a 300W halogen lamp in series. Th= e lamp will be short cut by a relay if the voltage across the C is >280V)= and apply a big C (i have some 350V/6000=B5F Elkos) and built a class D= PA that handles the 350V DC (i plan to use 2x STP10NK80Z FETs) i achieve= the maximum power the generator will give. The power regulation will be= optimal since the power decreases ~1/U^2. Even the small SMPS of the Note= book will be no problem since it covers a wide input voltage range. When= using a small 230V/10VA transformer to generate 15V DC for the driver and= use optical components for keying and using the given isolating output tr= ansformer of the PA, there is no danger to get a shock unless i do not tou= ch the PA during operation. The FETs are protected from overload power by= the generator and since they have integrated Z diodes, they will not be= damaged by eventual voltage spikes... ;-)=20 =20 73, Stefan=20 ________________________________ Von: owner-rsgb_lf_group@blacksheep.org im Auftrag von Paul Nicholson Gesendet: Mi 17.03.2010 10:46 An: rsgb_lf_group@blacksheep.org Betreff: Re: LF: Ionospheric VLF propagation Alexander wrote: > Certanly exponential factor exp(-r/a) should be present. > I mentioned this before. Yes you did! I am following your lead with this 1/sqrt(r) thing and the exponential factor. And it is working - it is giving the right answer for Stefan's signal! 3dB per 1000km (daytime) is mentioned in some literature but I have to follow that up. Assuming that, we have the estimate for daytime flux density at range r:- B =3D sqrt( 9.5e-21 * ERP/r) * exp( -r/2.9e6) > But this should be calculated. At the earth bondary one can > use Leontovich bondary condition Yes. > But what to do with ionosphere boundary... To neglect dissipation > in ionosphere looks not reasonable. Yes too. The ionosphere boundary is more complicated. There are two values for the refractive index - attenuation depends on direction relative to Earth's magnetic field. The result is phase and polarisation changes. I have some references to follow up here too. But it is complicated and time consuming. It would be nice to just use average figures for day and night attenuation - surely good enough for 'amateur' work. > To solve the problem (rather volumable problem) is nice task > for physicist. The hard work was done, decades ago, and appears to be fairly well established. But it is a major job to go through the literature and pick out what is relevant. It is a heady mix of plasma physics, EM theory and ray tracing. There are one or two textbooks - one I will order today. -- Paul Nicholson -- ------_=_NextPart_001_01CAC5C2.A33A08E9 Content-Type: application/ms-tnef; name="winmail.dat" Content-Transfer-Encoding: base64 eJ8+IjELAQaQCAAEAAAAAAABAAEAAQeQBgAIAAAA5AQAAAAAAADoAAEIgAcAGAAAAElQTS5NaWNy b3NvZnQgTWFpbC5Ob3RlADEIAQ2ABAACAAAAAgACAAEEgAEAGgAAAFZMRjogVEEsIDMwMG0gYW5k IG5ldyBQQT8A0AYBBYADAA4AAADaBwMAEQAMAAsAMAADAD8BASCAAwAOAAAA2gcDABEADAALADAA AwA/AQEJgAEAIQAAADZCNDYzNkJEMTAzNTY1NDk4OTM4NzMzQTE5Q0EzNDlDAP0GAQOQBgCcGAAA OAAAAAMANgAAAAAAQAA5AOkIOqPCxcoBHgA9AAEAAAAGAAAAVkxGOiAAAAACAUcAAQAAADIAAABj PURFO2E9IDtwPUhTVDtsPUZJTEUtU0VSVkVSLUgtMTAwMzE3MTExMTQ4Wi0xOTI3AAAAHgBJAAEA AAAkAAAAUmU6IExGOiBJb25vc3BoZXJpYyBWTEYgcHJvcGFnYXRpb24AQABOAICW1762xcoBHgBa AAEAAAAjAAAAb3duZXItcnNnYl9sZl9ncm91cEBibGFja3NoZWVwLm9yZwAAAgFbAAEAAABjAAAA AAAAAIErH6S+oxAZnW4A3QEPVAIAAAAAb3duZXItcnNnYl9sZl9ncm91cEBibGFja3NoZWVwLm9y ZwBTTVRQAG93bmVyLXJzZ2JfbGZfZ3JvdXBAYmxhY2tzaGVlcC5vcmcAAAIBXAABAAAAKAAAAFNN 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