Design RC and RL high-pass filters by calculating cutoff frequency, gain, phase shift, rolloff rate, and frequency response table.
A high-pass filter allows signals above a certain cutoff frequency to pass through while attenuating lower frequencies. It is fundamental in audio engineering (removing rumble and DC offset), radio communications (rejecting out-of-band interference), and signal processing (differentiating signals). It is one of the simplest ways to keep unwanted low-frequency energy out of a circuit.
The simplest implementations use a resistor and capacitor (RC) or resistor and inductor (RL). The cutoff frequency — where the output is −3 dB (70.7%) of the input — is determined by the component values. Higher-order filters provide steeper rolloff at the cost of additional components.
This High-Pass Filter Calculator handles both RC and RL topologies and supports 1st through 3rd order configurations. Enter your component values and a test frequency to see the cutoff frequency, gain, phase shift, rolloff rate, and a complete frequency response table. Preset buttons provide starting points for audio, RF, and general-purpose applications so you can move from rough idea to workable component range quickly.
High-pass filter design is simple in principle, but small unit mistakes or wrong assumptions about order and topology can shift the cutoff by an order of magnitude. This calculator puts the cutoff, gain, phase, and rolloff in one place so you can size the components, check the response at a test frequency, and explain the result clearly.
RC High-Pass: fc = 1 / (2π × R × C) RL High-Pass: fc = R / (2π × L) Gain: G(f) = −10n × log₁₀(1 + (fc/f)²) dB Rolloff: n × 20 dB/decade (n = filter order) Time Constant: τ = RC or τ = L/R
Result: fc = 15,915 Hz, Gain at 1 kHz = −24.1 dB
A 10 kΩ / 1 nF RC high-pass filter has a 15.9 kHz cutoff. At 1 kHz (well below cutoff), the signal is attenuated by 24 dB.
The most common design mistake is choosing components first and only later checking what cutoff they produce. Decide whether you are trying to block DC, remove low-frequency rumble, build a crossover, or isolate a higher-frequency band, then choose R and C or R and L to match that target. A filter that is one decade off can still look plausible on paper while performing badly in the circuit.
A second- or third-order filter does not just attenuate faster; it also changes the phase response and the width of the transition band. That matters in audio crossovers, sensor conditioning, and communication circuits where timing and alignment are part of the design. Use the order setting to compare how much extra selectivity you gain before you commit to the extra parts count.
Many wrong answers come from mixing ohms, kilo-ohms, microfarads, nanofarads, millihenries, and henries in the same mental calculation. The calculator is most useful when you verify the units, confirm whether you are using an RC or RL section, and then compare the test-frequency response against the expected operating range.
The cutoff frequency is the point where output power drops to half of the passband level, which corresponds to -3 dB in a first-order response. It is the reference point used to describe where the filter starts transitioning from attenuation to passband behavior.
RC is more common because capacitors are cheaper and lighter than inductors. RL is used at high frequencies or where capacitors are impractical.
The number of reactive elements. A 1st-order filter rolls off at 20 dB/decade; 2nd-order at 40 dB/decade, etc.
Yes — this is exactly how passive audio crossover high-pass sections work. Set the cutoff to your desired crossover frequency.
A first-order high-pass filter shows a +45 degree phase shift at the cutoff frequency. Higher-order filters have a steeper transition and different phase behavior, which is why the selected order matters when timing or crossover alignment is important.
Use a high-pass filter with a very low cutoff frequency (e.g., 1 Hz) to block DC while passing audio or data.