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Richard Clark wrote:
On Mon, 19 Jan 2009 09:43:27 -0800, Jeff Liebermann wrote: The over-simplified idea behind the ferrite (or powdered iron for HF) cores is to increase the inductance of the windings so the xformer works at lower frequencies. At VHF and UHF frequencies, the core mostly disappears and you're relying totally on the coupling between the bifilar windings. Actually that is not the mechanism at all, simplified or complexified. Ferrite compounds for BalUn application principally add resistance to the common mode path and have (as a design goal) absolutely no magnetic influence whatever. The increase of inductance is haphazard at best, and some ferrite compounds actually increase the capacitive reactance. As such, ferrites are not principally employed in building inductors. Further, iron cores don't serve much purpose for choking which is the principle requirement for BalUn input to output isolation. If you want to build an iron core, magnetic linkage transformer (AKA audio or power transformer), this is a very different beast from a BalUn, and a miserable replacement. 73's Richard Clark, KB7QHC When designing any transformer, be it audio, power, or RF, you usually want to accomplish three things: 1. Maximize the winding impedance. 2. Minimize the leakage impedance. This is another way of saying you want to maximize the coupling between the windings. 3. Realize an acceptably low loss. At low frequencies, most cores primarily provide inductance, so most literature dealing with transformers speaks of "inductance" rather than "impedance" when discussing the basic goals. But low frequency transformers could be made and would function just fine using resistive core materials if they were available. The third goal can be achieved with resistive materials as long as the first and second goals are accomplished well enough. That is, if the winding impedance is high enough, the magnetizing current will be low, so I^2*R loss will be low. And if coupling is good, increasing the current in one winding won't appreciably increase the core flux and incur extra loss. But at RF, as Richard says, many ferrite cores are more resistive than inductive. Not all are -- there are high frequency ferrites that remain inductive at very high frequencies. However, for the HF range and above, the best choice is usually "low frequency" ferrites which are primarily resistive in that frequency range. They're best for two reasons -- first, they provide much more impedance per turn squared than high frequency ferrites, making the first two goals much easier to achieve; and second, there are no resonance effects. An inductive winding will resonate with stray capacitance at some frequency. The impedance drops above that frequency, limiting the upper range of the transformer. The winding and leakage inductances can also resonate with external capacitance and cause ringing in some applications. A properly designed transformer using an essentially resistive core can operate very well over several decades of frequency. For most RF applications, it's not hard to design a transformer or balun that will have well under 1 dB of loss, which is negligible again in most applications. But if high power is involved, even a fraction of a dB might represent several or may watts of power, resulting in intolerable core heating. In those applications, lower loss, i.e., more inductive and less resistive, cores have to be used, often resulting in more difficult design and/or reduced performance in other respects. Resistive ferrites are also often good choices for RF chokes for the same reasons that they make good transformers. High-Q inductors and tuned transformers are a different critter, though. For those applications you want to use very low loss, that is, inductive and not resistive, core materials. This often leads to confusion, since ferrite manufacturers have traditionally specified a "recommended" frequency range for various materials which refers to the best range for these applications. The best material for an RF transformer is usually one with a "recommended" (for high-Q inductor applications) frequency range well below the transformer operating frequency. Roy Lewallen, W7EL |
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