Analyze bandwidth through response area or window coefficients. See instant results, plots, tables, and exports. Built for precise filter noise studies across many cases.
Choose a method, enter your values, and submit. The result appears above this form, directly below the header.
This example reflects a low-pass style response sampled in linear magnitude. You can paste similar values into the sampled-response method.
| Frequency (Hz) | Magnitude | |H(f)|² | Comment |
|---|---|---|---|
| 0 | 1.000 | 1.000 | Reference passband point |
| 500 | 0.894 | 0.799 | Still near passband |
| 1000 | 0.707 | 0.500 | Classic 3 dB point |
| 1500 | 0.555 | 0.308 | Moderate attenuation |
| 2000 | 0.447 | 0.200 | Further roll-off |
| 5000 | 0.196 | 0.038 | Tail contribution remains finite |
ENBW = ∫ |H(f)|² df / |Href|²
The numerator is the area under the squared magnitude response. The denominator normalizes by the chosen reference gain, usually the passband peak.
ENBW ≈ Σ [ (|Hi|² + |Hi+1|²) / 2 ] × Δf / |Href|²
This page uses trapezoidal integration for entered frequency-response samples.
ENBW = (π / 2) × fc
A first-order low-pass passes more integrated noise than an ideal brick-wall filter with the same cutoff.
BW3dB = f0 / Q
ENBW ≈ (π / 2) × BW3dB
This is useful for narrow Lorentzian-like band-pass systems.
ENBWbins = N × Σw[n]² / (Σw[n])²
ENBWhz = fs × Σw[n]² / (Σw[n])²
This is common in FFT and spectrum-analyzer workflows.
Equivalent noise bandwidth is the width of an ideal rectangular filter that would pass the same total noise power as the real response when both share the same reference gain.
Real filters usually have skirts and tails. Noise from those regions still contributes to total integrated power, so ENBW often exceeds the nominal 3 dB width.
Use it when you have measured or simulated gain values versus frequency. It is especially helpful when the filter shape is irregular or does not match a simple closed-form equation.
ENBW in bins shows how many FFT bins of white-noise power the selected window effectively spans. It is a normalization measure used in spectral estimation and analyzer calibration.
Noise power scales with the square of amplitude gain. That is why the area is computed from |H(f)|² rather than from amplitude magnitude alone.
Yes. Switch the response format to dB magnitude. The calculator converts dB to linear magnitude before integrating the squared response.
If the input noise density is flat, output RMS voltage is found by multiplying the density by the square root of ENBW. Power spectral density is multiplied directly by ENBW.
No. It is an approximation for narrow Lorentzian-like band-pass responses. For high accuracy, use measured or simulated response data and integrate the sampled spectrum.
Important Note: All the Calculators listed in this site are for educational purpose only and we do not guarentee the accuracy of results. Please do consult with other sources as well.