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#1
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On Sat, 26 May 2007 20:51:37 -0400, Chuck
wrote: Owen Duffy wrote: Other works that I have read describe the loss mechanisms as quite complex; magnetic loss described by a complex mu value that is temperature, frequency and flux dependent, resistive loss in the core material, dielectric loss in the core material, and resistive loss in the conductors. Sevick seems to say that only one of these is relevant, or that loss can be simplfied to a single equivalent loss, the dielectric loss. He is actually distinguishing between transformer type losses (as Chuck notes later in material I have not quoted). In the conventional transformer, loss is Ohmic due to the circulating eddy currents. This explanation does not serve Ferrite, which is principally an insulator, a dielectric with magnetic properties. Further, the operation of transformation for conventional transformers is through magnetic coupling, that is not so for tranmission line transformers (that no doubt all parties here are already aware of, and which Sevick is distinguishing to the naive readers of his paper). Hence, he is responding to loss issues that are found in conventional designs, but missing (or rather optimized for the Common Mode) in our chokes or BalUns. I guess it is appealing to equate loss that increases with frequency to an equivalent dielectric effect, but the loss is flux dependent and in a non-linear way, so it doesn't seem to fit well with a simple dielectric equivalence. Ferrites are not simple dielectrics, not even linear as a class (but seemingly so for our limited applications as chokes). Owen, I didn't see any reference in Sevick's fourth edition to the voltage-dependency of core losses. I can observe it in the reference offered. However, Sevick couches this dependency parenthetically to the dielectric property. As this is specifically true, and he distinguishes other losses in conventional transformers as Ohmic, his statement in its full context is valid if perhaps too sparse. It is quite obvious that voltage and current (and thus flux) are irrevocably inseparable and yet the loss does not specifically arrive due to conduction in the Ferrite material. On the other hand, discussion of Ferromagnetics is couched in magnetic fields and electron spin, not in voltaics. Instead, the following quote seems to characterize his philosophy in the book: "With transmission lines, the flux is effectively canceled out in the core and extremely high efficiencies are possible over large portions of the passband--losses of only 0.02 to 0.04 dB with certain core materials. The flux of Owen's contention is not the flux of the differential currents, but of the Common Mode current. [or so I read his query - at least insofar as the application of the choke serves] For student of the microwaves, Ferrites offer far more unique properties than are made use as I've suggested above. The nonlinearity is that Ferrite can be remarkably transparent to flux of a given polarization, and with a shift in that polarization it becomes quite opaque. In this service, it is also characterized as a non-reciprocal attenuator. This attribute can be modulated, literally, with an external DC (actually low frequency AC) field to impart modulation to what would otherwise be a CW signal. Ferrites employing this polarization characteristic are used in what are called Faraday Isolators (another one of those devices that could be used to separate forward and reverse waves; however, having only two ports so as to not be confused with the rat-race, and to my knowledge wholly unknown in this group). 73's Richard Clark, KB7QHC |
#2
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On Sun, 27 May 2007 00:47:15 -0700, Richard Clark
wrote: the loss does not specifically arrive due to conduction in the Ferrite material. On the other hand, discussion of Ferromagnetics is couched in magnetic fields and electron spin, not in voltaics. As a side-bar, much the same could be said of distilled water, and the ice made from it. At the point of freezing, the dielectric constant AND losses undergo a considerable change - and this is attributable to flux and polarization issues in much the same way. 73's Richard Clark, KB7QHC |
#3
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On Sun, 27 May 2007 00:47:15 -0700, Richard Clark
wrote: [snip] |Ferrites employing this polarization characteristic are used in what |are called Faraday Isolators (another one of those devices that could |be used to separate forward and reverse waves; however, having only |two ports so as to not be confused with the rat-race, and to my |knowledge wholly unknown in this group). | Hmmm. |
#4
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On Sun, 27 May 2007 14:43:17 +0000, Wes Stewart *n7ws*@ yahoo.com
wrote: On Sun, 27 May 2007 00:47:15 -0700, Richard Clark wrote: [snip] |Ferrites employing this polarization characteristic are used in what |are called Faraday Isolators (another one of those devices that could |be used to separate forward and reverse waves; however, having only |two ports so as to not be confused with the rat-race, and to my |knowledge wholly unknown in this group). | Hmmm. OK, perhaps known to you and Jim (yet and all, neither of you have made the arguments that would have stoked that bonfire). 73's Richard Clark, KB7QHC |
#5
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Richard Clark wrote:
... are called Faraday Isolators (another one of those devices that could ... 73's Richard Clark, KB7QHC Since my faraday isolators are already in use upon my sunglasses, I am forced to seek a substitute. :-( Regards, JS |
#6
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John Smith I wrote:
... Even worse, I find my "Faraday Rotation Isolator" only effective at Microwave freqs. :-( Regards, JS |
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