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Jim Lux wrote in
: Owen Duffy wrote: Mike Coslo wrote in news:i9n3jq$ds62$1 .... The model suggests that shorting the unused turns is a poorer solution when the flux coupling factor is relatively high, and a very small number of turns are shorted. Poorer both because of loss and the granularity of L adjustment. In that situation, the voltage induced in open unused turns is not very high, whereas it can be extreme in cases where most of the turns are unused. But in that situation, the voltage across the unshorted turns is likely to be low, because you've got low reactance, right? So the net effect is small. Hi Jim, It depends what you take as a reference. A rough estimate of the voltage across the unused turns is the turns ratio (unused /used) time the flux coupling factor, which in practical applications is likely to be in the range 0.2 to 0.5. If the application was a valve amp pi coupler, the voltage impressed across the used turns could be a couple of thousand volts, and on a 10m tap, the voltage across the unused turns could easily be 5 to 10 times that. In the case of a loading coil for a multiband whip, the current in the used turns is probably similar from band to band, but the used turns are lower for higher bands and so the flux cutting the unused turns is lower, but there are more unused turns. In this application, insulation problems are probably less severe than the PA with a bandswitch. To my mind, the interesting thing is why shorting some turns is 'ok', and then to understand that doesn't make it 'ok' in all scenarios. For instance, someone taking a valve amp pi coupler and implementing it on a single powdered iron core changes the situation significantly. Re the Tee circuit, yes, but it takes a while to draw it up... not nearly as quick as grinding a few numbers and creating a graph! I have a backlog of hand drawing scanned into articles to redraw already. Owen |
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