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Library / Structural dynamics and vibration testing / SDY-44

Structural dynamics and vibration testing

Equivalent noise bandwidth of a window

Width of the ideal rectangular filter that would pass the same noise power as the window.

Ref
SDY-44
Rev
v1
Field
Structural dynamics and vibration testing
Result
Be [Hz]

The equivalent noise bandwidth Be = fₛΣw²/(Σw)² is the width of the ideal rectangular filter that passes the same noise power as the window. For a rectangular window it is the bin spacing fₛ/N; for Hann it is 1.5 bins. Use it to turn a windowed spectrum of noise into a density. This entry uses the generalised cosine window of the previous entry.

Width of the ideal rectangular filter that would pass the same noise power as the window. It is the factor to use when converting a windowed spectrum to a density. The window is the generalised cosine window of the previous entry.

Calculator

Solve for
Hz
Hz
1010,000
0.51
44,096
  • Bin spacing, fₛ/N10 Hz
  • Bandwidth in bins, Bₑ/Δf1.5
  • Sum of squared window values, Σw²3

What drives the result

Each variable is moved across its typical range while the others stay at the values above. The longest bar is the key driver.

Equivalent noise bandwidth (Hz) current value 15 Hz
fsSample rateKey driver
1.881,880
NWindow length
0.029330
a0Window coefficient a₀ (0.5 Hann, 1 rectangular)
10
  • The window passes noise as a filter 15 Hz wide, 1.5 times the bin spacing.
  • A wider noise bandwidth blurs closely spaced modes more, but gives lower leakage; this is the trade-off in choosing a window.
Chart data as tables

Ranked variables

VariableTypical rangeLowest resultHighest resultSwing (Hz)Local stepChange in result
fs Sample rate10 to 10,000 Hz1.8751,8751,873+10%+10 %
N Window length4 to 4,096 0.02933029.97+1 −11.1 %
a0 Window coefficient a₀ (0.5 Hann, 1 rectangular)0.5 to 1 10155+10%−11 %

Sweep of Window coefficient a₀ (0.5 Hann, 1 rectangular)

Window coefficient a₀ (0.5 Hann, 1 rectangular)Equivalent noise bandwidth (Hz)
0.515
0.562513.02
0.62511.8
0.687511.03
0.7510.56
0.812510.27
0.87510.1
0.937510.02
110

Sweep one variable

Equivalent noise bandwidth (Hz)Hover, touch, or use the arrow keys on the chart
101112131415 0.50.60.70.80.91 Window coefficient a₀ (0.5 Hann, 1 rectangular) now 15

Variables and how each one contributes

Be

Equivalent noise bandwidth

Result · Hz

What the equation gives you. Everything else feeds it.

fs

Sample rate

Hz · typical 10 to 10,000

The sample rate, in Hz: samples taken per second. Sets the frequency span and scales the bandwidth in proportion. Raising it by 10 % (to 88) moves the result by +10 %, from 15 to 16.5 Hz.

a0

Window coefficient a₀ (0.5 Hann, 1 rectangular)

· typical 0.5 to 1

The window coefficient a₀ in w = a₀ − (1 − a₀)cos(2πj/N): 0.5 is Hann, 0.54 is Hamming and 1 is a rectangular window. A larger a₀ gives a flatter window with a narrower noise bandwidth but more leakage. Raising it by 0.04 (to 0.54) moves the result by −9.14 %, from 15 to 13.63 Hz.

N

Window length

· typical 4 to 4,096

The window length in samples. Longer windows narrow the bandwidth in proportion. Raising it by 8 (to 16) moves the result by −50 %, from 15 to 7.5 Hz.

Worked example with the values above

  1. Sums: Σw = 4, Σw² = 3.
  2. Ratio: Σw²/(Σw)² = 0.1875.
  3. Bₑ = 80 × 0.1875 = 15 Hz.

Assumptions and limits

  • A uniformly sampled, stationary record, with the window and scaling conventions stated for each entry.
  • A one-sided spectrum, with the factor 2 applied only to bins that have a distinct negative-frequency partner.

Common mistakes

  • Forgetting to divide by the window’s noise bandwidth or power, which scales the spectrum wrongly.
  • Applying the factor 2 at DC and at the Nyquist bin.
  • Assuming that zero padding adds resolution: it only interpolates the spectrum.
  • Treating overlapping segments as independent: they are correlated.

Statistics and uncertainty

Windowing and averaging trade resolution against variance and leakage. Record length sets the bin spacing, and the number of segments sets how much random error remains in the estimated spectrum.

Where it is used

  • Setting the record length, window and averaging for a vibration test so that nearby modes can be told apart.
  • Scaling windowed FFT output to correct amplitudes and spectral densities.

Maths you need

  • Discrete Fourier transform: frequency content of a sampled record
  • Window function: a taper applied to reduce spectral leakage
  • Power spectral density: power per unit frequency

Related formulas

Practise this formula