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The example, worked out
Given
Filter
Low-pass: L in series, C across
Inductance L
10 µH
Capacitance C
10 µF
Load R
5 Ω
Frequency to reject
100 kHz
Working
where L and C meet
the load sets the peak
-31.7 dB at 100 kHz
Results
Corner f015.9 kHz
At 100 kHz-31.7 dB
Q on this load5
Peak, near f0+14 dB
−3 dB point24.6 kHz
Z0 = √(L/C)1 Ω
Load for a flat response707 mΩ
The formulas
f0 = 1 / (2π √(L C))where L and C meet
Z0 = √(L / C)the impedance of the pair at f0
Q = R / Z0the load sets the peak: light load, high Q
The usual traps
Unloaded, an LC filter peaks at f0: a buck output filter rings when the load drops.
For a flat response the load must be about 0.7 × Z0, not any value.
The slope is 40 dB per decade past f0, not 20.
Questions
How do I calculate the cutoff of an LC filter?
f0 = 1 / (2π √(L C)): where L and C meet. Z0 = √(L / C): the impedance of the pair at f0. Q = R / Z0: the load sets the peak: light load, high Q.
What does it give for typical values?
Low-pass f0 = 15.9 kHz, -31.7 dB at 100 kHz, Q 5 on 5 Ω. Corner f0: 15.9 kHz; At 100 kHz: -31.7 dB.
What are the usual mistakes?
Unloaded, an LC filter peaks at f0: a buck output filter rings when the load drops. For a flat response the load must be about 0.7 × Z0, not any value. The slope is 40 dB per decade past f0, not 20.
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Open the calculatorOpens in the app on 1 December, with Circuit Notebook 1.0
Also in Signals & radio
Decibels & dBmRatios to dB and back; dBm to watts and volts.