Compute center frequency, quality factor (Q), bandwidth, and visualize the magnitude response of a passive RLC bandpass filter. Design your own filter starting from target f₀ and Q.
Enter resistance (R), inductance (L), and capacitance (C) values to compute resonant frequency, Q-factor, bandwidth, and cutoff frequencies.
Specify desired center frequency (f₀), quality factor (Q), and reference resistance. The tool calculates required L and C values for a series RLC network.
A series RLC bandpass filter is a classic passive circuit that passes frequencies within a specific band while attenuating signals outside that band. It consists of a resistor (R), inductor (L), and capacitor (C) connected in series. The output voltage is taken across the resistor, providing a bandpass transfer function. At resonance, the impedance of the inductor and capacitor cancel, maximizing the output.
Key design equations (series RLC):
Resonant frequency: f₀ = 1 / (2π √(LC)) | Quality factor: Q = (1/R) √(L/C) = ω₀L / R
Bandwidth: BW = f₀ / Q | Lower cutoff: f₁ = f₀ √(1 + 1/(4Q²)) - f₀/(2Q)
Upper cutoff: f₂ = f₀ √(1 + 1/(4Q²)) + f₀/(2Q)
The magnitude response in dB: |H(f)|dB = 20 log₁₀( R / √(R² + (2πfL - 1/(2πfC))² ) )
Bandpass filters are essential in wireless communications (RF front-ends, channel selection), audio processing (equalizers, crossover networks), biomedical instrumentation (ECG noise filtering), and measurement equipment (spectrum analyzers). The series RLC topology is valued for its simplicity, predictable behavior, and suitability for narrowband or wideband requirements depending on Q.
An intermediate frequency (IF) stage in a radio receiver often uses a high-Q bandpass filter to reject adjacent channels. Using our calculator, an engineer can specify f₀ = 455 kHz and Q = 50, with R = 1000 Ω, obtaining L ≈ 17.5 mH and C ≈ 6.8 pF. The narrow bandwidth (9.1 kHz) ensures excellent selectivity. The interactive graph confirms the steep skirt response, validating the design before prototyping.
The implemented algorithms rely on analytic solutions validated against standard filter theory texts (Zverev, "Handbook of Filter Synthesis" and Williams, "Electronic Filter Design Handbook"). The transfer function is calculated without approximations, guaranteeing high numerical precision. The interactive graph uses logarithmic frequency spacing to accurately represent both narrow and wideband responses.
| Parameter | Example (R=1kΩ, L=10mH, C=100nF) | Computed Value | Validation |
|---|---|---|---|
| Resonant frequency f₀ | 1/(2π√(0.01·100e-9)) | 5.033 kHz | Matches theoretical 5.033 kHz |
| Quality factor Q | ω₀L/R = (2π·5033·0.01)/1000 | 0.316 | Low Q, wide bandwidth |
| -3dB bandwidth | f₀/Q ≈ 15.9 kHz | 15.92 kHz | Consistent |
The voltage transfer ratio of a series RLC bandpass filter is H(s) = (sR/L) / (s² + sR/L + 1/(LC)). The poles are complex conjugates with real part -α = -R/(2L) and imaginary part ω₀√(1-1/(4Q²)). This underdamped response creates the characteristic peaking at resonance. For Q > 0.5, the filter provides a bandpass shape; for very low Q, the response resembles a low-pass/high-pass blend. Our calculator accurately models all Q regimes.