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Air gap cores

Recent interest in monotriode amplifier has restarted designs of transformers allowing a continuous current thru their windings. Exmaination of the curve B=f(H) for usual ferromagnetic materials shows that a continuous current in windings move the mean biasing point to the highly non linear saturation region. This behavoir is unacceptable for an audio transformer, either because of the induced increase of distorsion and because of decrease in dynamic permeability, yielding an increase in the number of turns (which have a detrimental effect on bad pass: see section above). There is thwo solutions to that problem : one can makes a continuous current flows thru an auxillary winding in order to neutralize the first one or one can open an air gap in the core for reluctance sharing between iron (staurable) and air (unsaturable). That last solution is by far the most common and will be described now. We make the approximation that air gap length tex2html_wrap_inline588 is small enough so that field lines will stay approximately parallel. Under those hypothesis, for an induction B and a normal section S, we will have for N turns in which flows a current I :
displaymath598
with l mean length of the magnetic circuit in the iron. Let us now find the air gap length for which inductance will be maximum. Let us denote by tex2html_wrap_inline450 the derivative of B= f(H= with respect to H. The dynamic inductance is then :
displaymath608
for a fixed induction B and a continuous current I, one have :
displaymath614
This last function admits a maximum with respect to tex2html_wrap_inline588, which allows to find optimal gap length and then the number of turns needed. For very high permeability cores, optimal length can be so small that they will be impossible to realize : experimenting is then needed ...



Stephane Puechmorel
Tue Jul 8 14:22:42 WET DST 1997