On Sunday, September 7, 2014 4:51:44 AM UTC-4, Daniel wrote:   
   > On Saturday, 6 September 2014 11:05:58 UTC+10, Don Kelly wrote:   
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   > > On 05/09/2014 6:15 AM, Daniel wrote:   
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   > > > On Saturday, 1 January 2000 19:00:00 UTC+11, D.H. Kelly wrote:   
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   > > >> Your concern over this assertion was well placed. It would have been   
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   > > >> possible to use integral of H.dl around loop = current enclosed- hence   
   H and   
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   > > >> flux outside the core whatever the mu. (which you did as part of your>   
   development.) You went a step further and I, for one, am glad that you did.   
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   > > >> Don Kelly   
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   > > >> dkelly@nabunalimo.lark.com   
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   > > >> remove the bull to reply   
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   > > >> BillyFish wrote in message   
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   > > >> news:20000101001804.15555.00000237@ng-ce1.aol.com...   
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   > > >>> Let me point out that this whole thread started because someone made   
   the   
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   > > >>> assertion that increasing the mu of the core to very high values would   
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   > > >> prevent   
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   > > >>> any flux outside the core. I think that the consensus now is that   
   such an   
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   > > >>> assertion is erroneous. This glib assertion suckered me in. In a   
   sense,   
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   > > >> it   
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   > > >>> was a scam artist at work. Well meaning maybe, but a scam artist   
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   > > >> nevertheless.   
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   > > >>> I just had to *understand* why it was erroneous. The scam misses the   
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   > > >> point   
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   > > >>> that a parallel H and E do not generate a Poynting vector. Once that   
   is   
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   > > >>> realized, everything else follows rather easily.   
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   > > >>> Bill   
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   > > > so after 14 years was the conclusion reached that leakage inductance is   
   in fact essential to transformer power transfer.. or an unfortunate, usually   
   small but inescapable component which reduces coupling and hence reduces   
   efficiency?   
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   > > > thx...   
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   > > Diclaimer:- I am not the Don Kelly "quoted" above. I vaguely recall    
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   > > someone making statements in my name.   
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   > > If you removes the "bull" to reply- then you are replying to an empty    
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   > > message.   
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   > > Leakage reactance is NOT "essential" to transformer power transfer. It    
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   > > is a result of the fact of life that two conductors cannot be    
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   > > superimposed to share the same space. One can come close-particularly    
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   > > with some toroidal LV transformers-but....   
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   > > However, efficiency in the normal sense of   
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   > > (real power out/real power in)   
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   > > depends on resistance, not leakage reactance.   
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   > > There is no wonderful conclusion after 14 years- the conclusion came    
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   > > over 114 years ago. That is that coupling is not perfect-hence leakage    
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   > > reactance.   
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   > > --    
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   > > Don Kelly   
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   > > remove the cross to reply   
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   > Nice to hear from you (DK - the voice of reason) again...   
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   > It was just that I seem to remember the idea that leakage L was an essential   
   component for Tx operation was arrived at after the discussion between Billy   
   Fish and Electric Pete... and that always urked me. Yes I agree the of course   
   that the magnetic    
   field being set up by the stray inductance does not dissipate any (real)   
   energy so does not reduce the efficiency electrically... Nice to know that   
   there is nothing that I am missing then...   
      
   Tom Tech,   
    I somewhat stumbled upon this interesting discussion regarding the power   
   transfer in iron core transformers via leakage flux or core flux. I have given   
   it MUCH thought and experimentation and research thru many college and   
   manufacturers text books    
   regarding transformer theory and construction. Until I took a much deeper look   
   into the transfer mechanism, I too was convinced thru what I thought was a   
   common view that energy is transferred via the core from one winding to   
   another. I do not hold that    
   view today. Several things can shed light on the somewhat hard to see transfer   
   mechanism. Yes, alternating flux in the iron core is responsible for the   
   induced EMF we see in any winding around the core, however when secondary load   
   current flows (assume a    
   resistive load), the secondary H field tries to reduce the core flux, and does   
   for a very brief period, reducing the induced "Back EMF" seen in the primary.   
   More current flows in the primary to maintain the core flux, however,   
   regardless of how high the    
   core permeability is,"leakage Flux" will be produced. The term "leakage flux"   
   is perhaps a misnomer, as it implies a fault in materials. Under load   
   conditions, the "Leakage" flux will always be produced. This H "leakage" flux   
   is in phase with the primary    
   voltage and in phase with the induced EMF in the secondary winding for "Real   
   Power". Note that the core flux does not change, at least not much, maybe a   
   little due to IR drops in the primary winding. If you work out the Poynting   
   Theorem, it will show the    
   induced EMF normal to the H flux from primary current to represent real power   
   flow into the secondary winding. Remember core flux is lagging the primary   
   voltage 90 degrees or so. Another insight is that under loaded conditions,   
   there is MUCH MORE energy    
   in the "Leakage" H flux than in the core flux. The "leakage" flux has a very   
   high field intensity, that, when crossed with induced EMF is real power flow.   
   If one examines the signal times thru for instance, an audio interstage   
   transformer, you will see    
   the time required to pass thru the transformer is much faster than it would be   
   if it had passed thru the high permeability iron core region. I do admit   
   applying the Poynting theorem is somewhat diffucult and transformer   
   manufacturers do not refer to it    
   at all, but then the makers of tennis rackets do not seem to refer to the   
   molecular makeup of nylon in their wares either, but the info is there for   
   those who wish to dig for it.....   
      
   --- SoupGate-Win32 v1.05   
    * Origin: you cannot sedate... all the things you hate (1:229/2)   
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