Return-Path: Received: from rly-mf04.mx.aol.com (rly-mf04.mail.aol.com [172.20.29.174]) by air-mf03.mail.aol.com (v121_r3.13) with ESMTP id MAILINMF034-95948ff505392; Wed, 22 Oct 2008 12:10:19 -0400 Received: from post.thorcom.com (post.thorcom.com [193.82.116.20]) by rly-mf04.mx.aol.com (v121_r3.13) with ESMTP id MAILRELAYINMF047-95948ff505392; Wed, 22 Oct 2008 12:09:58 -0400 Received: from majordom by post.thorcom.com with local (Exim 4.14) id 1KsgGu-0003fo-JR for rs_out_1@blacksheep.org; Wed, 22 Oct 2008 17:09:20 +0100 Received: from [83.244.159.144] (helo=relay3.thorcom.net) by post.thorcom.com with esmtp (Exim 4.14) id 1KsgGu-0003fe-1g for rsgb_lf_group@blacksheep.org; Wed, 22 Oct 2008 17:09:20 +0100 Received: from smtp5.freeserve.com ([193.252.22.151] helo=smtp6.freeserve.com) by relay3.thorcom.net with esmtp (Exim 4.63) (envelope-from ) id 1KsgGt-0006gy-2b for rsgb_lf_group@blacksheep.org; Wed, 22 Oct 2008 17:09:19 +0100 Received: from me-wanadoo.net (localhost [127.0.0.1]) by mwinf3509.me.freeserve.com (SMTP Server) with ESMTP id 181A27000084 for ; Wed, 22 Oct 2008 18:09:07 +0200 (CEST) Received: from AGB (unknown [91.110.94.67]) by mwinf3509.me.freeserve.com (SMTP Server) with SMTP id 9524D7000083 for ; Wed, 22 Oct 2008 18:09:04 +0200 (CEST) X-ME-UUID: 20081022160904610.9524D7000083@mwinf3509.me.freeserve.com Message-ID: <6F13074EBF0A495ABDD70F58545FFC58@AGB> From: "Graham" To: References: <000701c933bd$4ef22f60$4201a8c0@home> <1224687077.48ff3de587a50@imp.netikka.net> In-Reply-To: <1224687077.48ff3de587a50@imp.netikka.net> Date: Wed, 22 Oct 2008 17:09:03 +0100 MIME-Version: 1.0 X-Priority: 3 X-MSMail-Priority: Normal Importance: Normal X-Mailer: Microsoft Windows Live Mail 14.0.5027.908 X-MimeOLE: Produced By Microsoft MimeOLE V14.0.5027.908 X-Spam-Score: 0.0 (/) X-Spam-Report: autolearn=disabled,none Subject: Re: LF: Ferrites - why low frequency limit? Content-Type: text/plain; format=flowed; charset="iso-8859-1"; reply-type=original Content-Transfer-Encoding: 7bit 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=MISSING_OUTLOOK_NAME 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-IP: 193.82.116.20 X-AOL-SCOLL-AUTHENTICATION: domain : post.thorcom.com ; SPF_helo = n X-AOL-SCOLL-AUTHENTICATION: domain : g8fzk.fsnet.co.uk ; SPF_822_from = n Paul, .. I had a phone conversation with a applications engineer over the right ferrite to use a while ago ..... only the one call .... he advised me to buy the amp ready made, to save the development .... at least he was honest hihi G ... -------------------------------------------------- From: "Paul-Henrik" Sent: Wednesday, October 22, 2008 3:51 PM To: Subject: Re: LF: Ferrites - why low frequency limit? > > Thank you Jim for this most interesting brief explanation! > > I say brief, because I have developed a vague feeling over the years for > how > long it would have to be to cover every aspect we face just in the amateur > field... And I'm still a green novice when it comes to ferrite/powder iron > cores. > > Paul-Henrik / OH1LSQ > > > Quoting James Moritz : > >> Dear John, LF Group, >> >> There is no strict limit on the frequency range of a particular type of >> ferrite, rather there is an optimum frequency range depending on the >> application. >> >> All ferrites have losses that increase with frequency. At low frequency >> this >> is mainly due to magnetic hysteresis in the core, which results in a loss >> that rises with operating frequency at a given level of magnetic flux, >> and >> at high frequencies things like eddy currents and dielectric losses >> increase >> in significance too. The lower permeability ferrite materials tend to >> have >> lower overall loss in the magnetic core material in the LF/MF/HF range, >> but >> require more turns of wire to achieve a given inductance, or a particular >> maximum level of flux in the core, resulting in higher losses in the >> windings. So there is a trade-off, favouring high permeability materials >> at >> low frequency where the loss due to hysteresis is relatively low and the >> smaller number of turns needed is a benefit, and low permeability >> materials >> at higher frequency where fewer turns are required. >> >> Whether a material is suitable at a particular frequency depends a lot on >> what it is being used for. If one looks at the impedance of a particular >> winding, the core losses result in a resistive component that increases >> with >> frequency, and an inductance that is constant at low frequencies, but >> decreases rapidly at high frequencies. At very high frequencies, the >> resistive component may also reduce. So there comes a crossover point >> when >> the coil impedance becomes mostly resistive, and at higer frequencies >> still >> the overall impedance of the coil actually reduces (this is ignoring the >> effect of stray capacitance, which will also cause the impedance to >> reduce >> at frequencies above resonance). The crossover tends to occur at higher >> frequencies for lower permeability materials. For a signal transformer, >> one >> does not usually care too much about the resistive component, provided >> the >> overall winding impedance is high, which favours high permeability cores. >> For a high Q coil in a tuned circuit, one wants to minimise the resistive >> component as much as possible, which tends to favour low permeability >> cores. >> For noise supression, one wants to maintain a large impedance over a wide >> frequency range, and a resistive impedance is actually quite useful in >> damping out resonances. Here the upper limit is where the overall >> impedance >> starts to decrease. For power applications such as SMPSUs and >> transmitters, >> the trade-off becomes more complicated, because one also must consider >> flux >> density, temperature rise, size and cost of the core, the effect of a DC >> bias current, etc. >> >> So the reccomended frequency range of a ferrite material is really rather >> a >> vague notion. Nothing terrible happens at low frequencies, but the >> windings >> tend to get unmanageably large. At high frequencies, there comes a point >> where the losses are too high for the circuit requirements. But in both >> cases, the frequency limits will depend a lot on what the core is being >> used >> for. >> >> Cheers, Jim Moritz >> 73 de M0BMU >> >> >> > > > > > > > > No virus found in this incoming message. > Checked by AVG - http://www.avg.com > Version: 8.0.175 / Virus Database: 270.8.2/1738 - Release Date: 10/21/2008 > 14:10 >