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RC/RL First-Order Filter Calculator

Cutoff frequency, magnitude, and phase of first-order RC and RL low-pass and high-pass filters, with the Bode plot.

About this calculator

A single resistor with a single capacitor or inductor makes the simplest possible frequency-selective circuit: a first-order filter with one cutoff (corner) frequency. For the RC forms, f_c = 1/(2πRC); for the RL forms, f_c = R/(2πL). At that corner the output is 3.01 dB below the passband — the half-power point — and the phase shift is exactly 45°.

Above or below the corner the behavior is beautifully simple: magnitude rolls off at 20 dB per decade (6 dB per octave), and the phase runs from 0° to −90° for the low-pass (or +90° to 0° for the high-pass), passing through its 45° midpoint at the corner. The normalized response is the same whether the components are an RC anti-aliasing filter, an RL choke feeding a load, or the unintended pole formed by a source resistance and cable capacitance.

This calculator computes the cutoff for any of the four topologies, evaluates magnitude (in dB and as a linear ratio) and phase at any frequency of interest, and draws the full Bode plot — magnitude on the left axis, phase dashed on the right — over four decades around the corner. Use it to place a pole where you need it, or to check how much a known pole disturbs the band you care about: at one-tenth of f_c a low-pass still passes 99.5% amplitude but has already accumulated 5.7° of phase lag, which is often the surprise in feedback loops.

For resonant (second-order) behavior with Q and peaking, use the second-order filter calculator.

Assumptions

  • Ideal components: no capacitor ESR, no inductor winding resistance or core loss beyond the single R modeled.
  • The filter is driven by an ideal (zero-impedance) source and feeds an ideal (infinite-impedance) load — finite source and load impedances shift the corner.
  • Small-signal, linear, time-invariant operation.

When to use this calculator

Appropriate for

  • Finding the corner frequency and magnitude/phase response of an ideal first-order RC or RL filter
  • Estimating the roll-off and phase shift a simple filter adds to a signal
  • Teaching the single-pole Bode response

Not suitable for

  • Real circuits where source and load impedance, or component parasitics, shift the corner from the ideal value
  • Sharper selectivity than a single 20 dB/decade slope, which needs higher-order filters
  • Precise filter design against a specification without accounting for loading and tolerance

What this calculator does not cover

  • First-order responses only — no resonance, no peaking, and a fixed 20 dB/decade slope; cascaded or RLC filters need the second-order calculator or full network analysis.
  • Loading is not modeled: a following stage whose impedance is comparable to R changes both the corner frequency and the passband gain.
  • Component parasitics (capacitor ESL, inductor self-capacitance) create additional poles and zeros at high frequency that this ideal model omits.
  • As with every calculator on this site: results are preliminary and educational, are not verified for any specific installation, and must be reviewed against the applicable code edition and stamped by a licensed Professional Engineer before real-world use.

Frequently asked questions

Why is the cutoff at −3 dB rather than where the signal 'stops'?

A first-order filter has no sharp edge — the −3.01 dB point is where output power is exactly half the input power (|H| = 1/√2), a natural, unambiguous reference. Beyond it the response falls at a fixed 20 dB per decade.

How much phase shift does the filter add inside its passband?

More than intuition suggests: a low-pass already lags 5.7° at one-tenth of the corner, 45° at the corner, and 84.3° at ten times it. In feedback systems that in-band phase, not the magnitude roll-off, is usually what matters.

Are RC and RL filters interchangeable?

Electrically the normalized responses are identical — same magnitude and phase curves against f/f_c. The choice is practical: capacitors are smaller, cheaper, and closer to ideal at low frequency, so RC dominates; RL appears where an inductor is already present, as with chokes and motor windings.

References

  • Alexander, C. & Sadiku, M., Fundamentals of Electric Circuits, 5th ed., Ch. 14 (frequency response)
  • Sedra, A. & Smith, K., Microelectronic Circuits, 7th ed. (first-order filter functions)

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