AJAB
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R1 is part of XL which determines the current through the inductor. Note that the inductor current becomes larger if an additional load is attached.
No, that formula is wrong. A precise solution should account for the fact that inductor ESR is frequency dependent, and probably nonlinear as well. A good compromise is to decompose loss calculations into low and high frequency contributions, with each having its own inductor ESR.So Irms = V/sqrt(square of (2*pi*F*L) + square of (R1))
and then Power Diss. = square of Irms * DC resistance of L
Correct?
All of the components shown in your first picture, as well as the stuff you didn't show because you didn't think it was important.But still In my circuit what are the components that affect inductor current?? :???:
If that's an 8 ohm speaker then it's current will likely dominate the current through the inductor, assuming the reactive components have a much higher impedance at audio frequencies. The high frequency current components from the switching frequency should be relatively small and would contribute little to the inductor power dissipation.
So why is this wrong : ���� =��/(2∗��∗��..?? and PD = IL*IL*DC resistance???
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