T
treez
Guest
Hello,
The attached LTspice simulation is of an open loop sepic with coupled inductor. (schematic in pdf also attached)
The resonance frequency between the c(sepic) and the L(leakage) is equal to the switching frequency. (104khz)
I am amazed how very slight changes to the primary and secondary inductor's esr has such a big effect on the magnitude of the RMS current seen in each of these inductors.
With 1 milliohm of esr in each inductor, the rms current in the primary inductor is just 6.12 Amps.
With 30 milliohms of esr in each inductor, the rms current in the primary inductor is 1.93 Amps.
....Why such a big difference in RMS current?..after all, 30 milliohms, even though 30 times more than 1 milliohm, its still an incredibly low amount of resistance.
The sepic spec is
vin=5v
vout=15v
f(sw)=104khz
pout=7.5w
CCM
The attached LTspice simulation is of an open loop sepic with coupled inductor. (schematic in pdf also attached)
The resonance frequency between the c(sepic) and the L(leakage) is equal to the switching frequency. (104khz)
I am amazed how very slight changes to the primary and secondary inductor's esr has such a big effect on the magnitude of the RMS current seen in each of these inductors.
With 1 milliohm of esr in each inductor, the rms current in the primary inductor is just 6.12 Amps.
With 30 milliohms of esr in each inductor, the rms current in the primary inductor is 1.93 Amps.
....Why such a big difference in RMS current?..after all, 30 milliohms, even though 30 times more than 1 milliohm, its still an incredibly low amount of resistance.
The sepic spec is
vin=5v
vout=15v
f(sw)=104khz
pout=7.5w
CCM
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