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About

In RF and audio circuit design, separating desired signals from noise requires precise filtering. A simple RC filter often lacks the steep attenuation ("rolloff") needed for tight spectrum management. LC filters, using inductors and capacitors, provide superior performance with minimal resistive loss. This tool aids in synthesizing 2nd-order passive filters, critical for power supplies (ripple rejection) and radio transmitters (harmonic suppression).

The calculator not only outputs the theoretical component values based on the cutoff frequency (fc) and system impedance (Z0), but also visualizes the magnitude response. Seeing the curve is vital to understand the trade-offs: the flat passband of a Butterworth filter versus the steeper descent but rippled passband of a Chebyshev filter. It assumes ideal components, so real-world implementation should account for inductor DC resistance (DCR).

filter design LC filter RF bode plot electronics

Formulas

For a standard 2nd-order Butterworth Low Pass filter, the component values for a given impedance Z0 and cutoff frequency fc are:

L = Z0 22πfc
C = 22πfcZ0

The resonant frequency is defined as f0 = 1 / (2πLC).

Reference Data

Filter TypeOptimized ForPhase ResponseTransient Response
ButterworthMax Flatness (Passband)Moderate Non-linearityModerate Overshoot
ChebyshevSteep RolloffNon-linearHigh Ringing
BesselLinear Phase (Time Delay)Linear (Constant Delay)Min Overshoot
EllipticMax SteepnessHighly Non-linearSevere Ringing
Order (n=2)-12 dB/octave-180° ShiftStandard LC Section
Order (n=3)-18 dB/octave-270° ShiftT or Pi Section
Low PassPasses f < fcLaggingIntegrator-like
High PassPasses f > fcLeadingDifferentiator-like

Frequently Asked Questions

LC filters are lossless (ideally), meaning they don't dissipate power as heat in the passband, making them essential for power applications. They also provide -40dB/decade rolloff per 2nd order stage, double that of a simple RC stage.
Filters must be matched to the source and load resistance (usually 50Ω for RF or 4Ω/8Ω for audio). Mismatched impedance creates reflections and alters the cutoff frequency.
The plot assumes ideal components. Real inductors have resistance and inter-winding capacitance, and capacitors have leakage. These parasitic elements can dampen the Q-factor and shift the resonant peak.