Received: from post.thorcom.com (post.thorcom.com [195.171.43.25]) by mtain-db03.r1000.mx.aol.com (Internet Inbound) with ESMTP id AC207380000B7; Tue, 16 Aug 2011 09:52:29 -0400 (EDT) Received: from majordom by post.thorcom.com with local (Exim 4.14) id 1QtK3I-0002H2-V2 for rs_out_1@blacksheep.org; Tue, 16 Aug 2011 14:51:32 +0100 Received: from [195.171.43.32] (helo=relay1.thorcom.net) by post.thorcom.com with esmtp (Exim 4.14) id 1QtK3I-0002Gt-6U for rsgb_lf_group@blacksheep.org; Tue, 16 Aug 2011 14:51:32 +0100 Received: from imr-mb01.mx.aol.com ([64.12.207.164]) by relay1.thorcom.net with esmtp (Exim 4.63) (envelope-from ) id 1QtK3H-0005mF-Hk for rsgb_lf_group@blacksheep.org; Tue, 16 Aug 2011 14:51:32 +0100 Received: from mtaomg-ma05.r1000.mx.aol.com (mtaomg-ma05.r1000.mx.aol.com [172.29.41.12]) by imr-mb01.mx.aol.com (8.14.1/8.14.1) with ESMTP id p7GDpBWw005713 for ; Tue, 16 Aug 2011 09:51:11 -0400 Received: from core-msd005c.r1000.mail.aol.com (core-msd005.r1000.mail.aol.com [172.29.234.17]) by mtaomg-ma05.r1000.mx.aol.com (OMAG/Core Interface) with ESMTP id 08B76E000086 for ; Tue, 16 Aug 2011 09:51:11 -0400 (EDT) To: rsgb_lf_group@blacksheep.org X-MB-Message-Source: WebUI X-MB-Message-Type: User MIME-Version: 1.0 From: Markus Vester X-Mailer: AOL Webmail 34047-STANDARD Received: from 194.138.39.56 by webmail-d154.sysops.aol.com (205.188.58.139) with HTTP (WebMailUI); Tue, 16 Aug 2011 09:51:10 -0400 Message-Id: <8CE2A32B072C020-1968-3625@webmail-d154.sysops.aol.com> X-Originating-IP: [194.138.39.56] Date: Tue, 16 Aug 2011 09:51:10 -0400 (EDT) X-AOL-VSS-INFO: 5400.1158/73444 X-AOL-VSS-CODE: clean X-AOL-SCOLL-SCORE: 0:2:429519424:93952408 X-AOL-SCOLL-URL_COUNT: 0 Subject: Re: LF: Ferrite RX antennas Content-Type: multipart/mixed; boundary="--------MB_8CE2A32B09674B1_1968_9D10_webmail-d154.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-VSS-INFO: 5400.1158/73444 X-AOL-VSS-CODE: clean X-AOL-SCOLL-SCORE: 0:2:451198976:93952408 X-AOL-SCOLL-URL_COUNT: 0 x-aol-sid: 3039ac1d40574e4a761d1d32 X-AOL-IP: 195.171.43.25 X-AOL-SPF: domain : blacksheep.org SPF : none This is a multi-part message in MIME format. ----------MB_8CE2A32B09674B1_1968_9D10_webmail-d154.sysops.aol.com Content-Type: multipart/alternative; boundary="--------MB_8CE2A32B09674B1_1968_9D11_webmail-d154.sysops.aol.com" ----------MB_8CE2A32B09674B1_1968_9D11_webmail-d154.sysops.aol.com Content-Transfer-Encoding: quoted-printable Content-Type: text/plain; charset="utf-8" Hi Jim, LF, the attached picture shows an experimental ferrite antenna. The total lengt= h is about 36 cm, with seven 1 cm diameter rods packed. The central section= is thinned to a single rod, carrying a standard tuned coil from a broadcas= t radio, plus a small coupling coil. I attempted to measure its sensitivity= , using DCF39 and an SPM3 selective level meter. With tuning and matching t= o 138.83 kHz, the available receive power was -80.4 dBm. >From a given fieldstrength E, a lossless monopole or loop antenna should de= liver a power of=20 P =3D E^2 / Zo * lambda^2 /4/pi * 3/4, which would be +8.3 dBm in a field of 3 mV/m. Thus the efficiency of my fer= rite antenna was about -88.7dB. Taking the quiet winterday noise density (En =3D -25 dBuV/m/sqrtHz), the no= ise output of the lossless antenna would be -86.2 dBm/Hz, or 87.6 dB above = room temperature thermal noise. Thus the thermal noise of my antenna would = be about 1.1 dB above the lowest background. =20 This roughly confirms Jim's estimate, though my experimental result seems s= lightly short by 4 dB. Possible causes might have been lower Q (will have t= o measure it), and the fact that the measurement was taken indoors, with a = possibly reduced fiedstrength of DCF39. For comparison, the 86 cm diameter loops in the garden, which are used for = the colour DF, have an efficiency of -75 dB at Q =3D 80. Best regards, Markus (DF6NM) -----Urspr=C3=BCngliche Mitteilung-----=20 Von: James Moritz An: rsgb_lf_group Verschickt: Mo, 15 Aug 2011 11:15 pm Betreff: Re: LF: Ferrite RX antennas Dear Stefan, LF Group, I spent some time reading various texts and data books, and doing some=20 alculations. The complete argument is too long and boring to type into an= =20 -mail, but very approximately it seems to be the case that for a ferrite=20 od antenna and an air-cored loop antenna to have similar signal/noise=20 erformance, the rod length needs to be similar to the loop diameter, which= =20 eems intuitively reasonable. This means that the air-cored loop is better= =20 or larger antennas (a 1m long ferrite rod is very heavy and expensive), but= =20 he ferrite rod is better for smaller sizes (a 30cm long ferrite rod is=20 uite reasonable weight/cost, and less bulky than a 30cm diameter loop). In that case, "is it possible to make a 30cm long ferrite rod antenna and= =20 reamp with a noise level below the 136k band noise floor?" is the question= =20 o decide if the ferrite rod is worthwhile for /P reception from a low-noise= =20 ocation. Obviously there are many variables, but one can attempt at least a= =20 ough calculation. Assume Stefan assembles his rods into 2 bundles of 7; this would be roughly= =20 quivalent to a single solid rod 28cm long x 21mm diameter. Assuming a high= =20 ermeability ferrite, this l/d ratio will multiply the flux through the=20 inding by a factor of about 70 compared to the same winding without the=20 ore (called "mu_core" in Watt's "VLF Engineering"), so the rod antenna will= =20 e equivalent to an air cored loop with an area of 0.025m^2. Assuming a=20 oise floor of 0.06uV/m per sqrt(Hz), a single-turn winding with this area= =20 ould have an induced EMF of 4.2pV/sqrt(Hz). With a low-noise preamp, assume= =20 he internal noise level is all due to the resistive losses of the antenna,= =20 hich depends on the Q. Q of about 250 should be achievable; the inductance= =20 f a single turn winding depends on another permeability parameter, mu_rod,= =20 hich depends on the rod geometry and the permeability of the ferrite; for= =20 his rod about 100 from Philips' ferrite data book. L works out to about=20 .16uH, and the loss resistance 540 micro-ohms. The noise voltage density is= =20 qrt(4kTR), 3pV/sqrt(Hz). So the internal noise is below the band noise by= =20 pV/4.2pV =3D 3dB. Hooray! So it could actually be feasible. In order to make it work, it will be=20 mportant to achieve a high Q. Obviously, a single turn winding with=20 icovolt output levels is not very practical. I would aim for a parallel=20 uning capacitance of e.g. 5nF, so it can be tuned across the 136k band=20 sing a 500p variable. This would require L of 270uH, requiring about 41=20 urns of thick wire, preferably Litz or multiple strands of thin wire. The= =20 arallel impedance at resonance with Q =3D 250 would then be 58kohms.=20 onnecting the tuned winding directly to a "miniwhip" type FET input preamp= =20 hould work well and add negligible amounts of preamp noise. The increased= =20 umber of turns and the high Q resonant winding winding will increase the=20 .2pV/sqrt(Hz)noise floor at the preamp input by a factor of (41 x 250), so= =20 3nV/sqrt Hz. In a 300Hz CW bandwidth, this would be about 0.75uV of noise,= =20 o with a reasonably sensitive RX, no further gain would be needed=20 worthwhile checking if it IS reasonably sensitive though...). I stress that these are all very rough calculations - you will have to=20 ctually try it out to find what the real values are. But they should be a= =20 easonable "first guess", and it seems to show that the expeiment is worth= =20 rying. Cheers, Jim Moritz 3 de M0BMU ----------MB_8CE2A32B09674B1_1968_9D11_webmail-d154.sysops.aol.com Content-Transfer-Encoding: quoted-printable Content-Type: text/html; charset="utf-8"
Hi Jim, LF,
 
the attached picture shows an experimental ferrite antenna. = The total length is about 36 cm, with seven 1 cm diameter rods packed.=  The central section is thinned to a single rod, carrying&nb= sp;a standard tuned coil from a broadcast radio, plus a smal= l coupling coil. I attempted to measure its sensitivity, using DCF39 a= nd an SPM3 selective level meter. With tuning and matching to 138.83 k= Hz, the available receive power was -80.4 dBm.
From a given fieldstrength E, a lossless monopole or loop antenna shou= ld deliver a power of
 P =3D E^2 / Zo * lambda^2 /4/pi * 3/4,
which would be +8.3 dBm in a field of 3 mV/m. Thus the efficiency= of my ferrite antenna was about -88.7dB.

Taking the quiet winterday noise density (En =3D -25 dBuV/m/sqrtHz), t= he noise output of the lossless antenna would be -86.2 dBm/H= z, or 87.6 dB above room temperature thermal noise. Thus the thermal n= oise of my antenna would be about 1.1 dB above the lowest background.&= nbsp; 
 
This roughly confirms Jim's estimate, though my experimental resu= lt seems slightly short by 4 dB. Possible causes might have been lower= Q (will have to measure it), and the fact that the measurement was taken i= ndoors, with a possibly reduced fiedstrength of DCF39.
 
For comparison, the 86 cm diameter loops in the garden, which are used= for the colour DF, have an efficiency of -75 dB at Q =3D 80= .
 
Best regards,
Markus (DF6NM)
 
= -----Urspr=C3=BCngliche Mitteilung-----
Von: James Moritz <james.moritz@btopenworld.com>
An: rsgb_lf_group <rsgb_lf_group@blacksheep.org>
Verschickt: Mo, 15 Aug 2011 11:15 pm
Betreff: Re: LF: Ferrite RX antennas

Dear S=
tefan, LF Group,

I spent some time reading various texts and data books, and =
doing some=20
calculations. The complete argument is too long and boring to type into an=
=20
e-mail, but very approximately it seems to be the case that for a ferrite=
=20
rod antenna and an air-cored loop antenna to have similar signal/noise=20
performance, the rod length needs to be similar to the loop diameter, which=
=20
seems intuitively reasonable. This means that the air-cored loop is better=
=20
for larger antennas (a 1m long ferrite rod is very heavy and expensive), bu=
t=20
the ferrite rod is better for smaller sizes (a 30cm long ferrite rod is=20
quite reasonable weight/cost, and less bulky than a 30cm diameter loop).

In that case, "is it possible to make a 30cm long ferrite rod antenna and=
=20
preamp with a noise level below the 136k band noise floor?" is the question=
=20
to decide if the ferrite rod is worthwhile for /P reception from a low-nois=
e=20
location. Obviously there are many variables, but one can attempt at least =
a=20
rough calculation.

Assume Stefan assembles his rods into 2 bundles of 7; this would be roughly=
=20
equivalent to a single solid rod 28cm long x 21mm diameter. Assuming a high=
=20
permeability ferrite, this l/d ratio will multiply the flux through the=20
winding by a factor of about 70 compared to the same winding without the=20
core (called "mu_core" in Watt's "VLF Engineering"), so the rod antenna wil=
l=20
be equivalent to an air cored loop with an area of 0.025m^2. Assuming a=20
noise floor of 0.06uV/m per sqrt(Hz), a single-turn winding with this area=
=20
would have an induced EMF of 4.2pV/sqrt(Hz). With a low-noise preamp, assum=
e=20
the internal noise level is all due to the resistive losses of the antenna,=
=20
which depends on the Q. Q of about 250 should be achievable; the inductance=
=20
of a single turn winding depends on another permeability parameter, mu_rod,=
=20
which depends on the rod geometry and the permeability of the ferrite; for=
=20
this rod about 100 from Philips' ferrite data book. L works out to about=20
0.16uH, and the loss resistance 540 micro-ohms. The noise voltage density i=
s=20
sqrt(4kTR), 3pV/sqrt(Hz). So the internal noise is below the band noise by=
=20
3pV/4.2pV =3D 3dB. Hooray!

So it could actually be feasible. In order to make it work, it will be=20
important to achieve a high Q. Obviously, a single turn winding with=20
picovolt output levels is not very practical. I would aim for a parallel=20
tuning capacitance of e.g. 5nF, so it can be tuned across the 136k band=20
using a 500p variable. This would require L of 270uH, requiring about 41=20
turns of thick wire, preferably Litz or multiple strands of thin wire. The=
=20
parallel impedance at resonance with Q =3D 250 would then be 58kohms.=20
Connecting the tuned winding directly to a "miniwhip" type FET input preamp=
=20
should work well and add negligible amounts of preamp noise. The increased=
=20
number of turns and the high Q resonant winding winding will increase the=
=20
4.2pV/sqrt(Hz)noise floor at the preamp input by a factor of (41 x 250), so=
=20
43nV/sqrt Hz. In a 300Hz CW bandwidth, this would be about 0.75uV of noise,=
=20
so with a reasonably sensitive RX, no further gain would be needed=20
(worthwhile checking if it IS reasonably sensitive though...).

I stress that these are all very rough calculations - you will have to=20
actually try it out to find what the real values are. But they should be a=
=20
reasonable "first guess", and it seems to show that the expeiment is worth=
=20
trying.

Cheers, Jim Moritz
73 de M0BMU
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