Energy loss of spectra associated with Window Functions

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SUMMARY

This discussion focuses on the energy loss associated with various window functions, specifically the Hanning and Hamming windows. It establishes that applying these windows results in energy loss in the spectra of interest, with correction factors of 1.633 for the Hanning window and 1.586 for the Hamming window. The discussion also highlights the classification of signals into finite energy and finite power categories, emphasizing that windowing transforms a finite power signal into a finite energy signal. The normalization of window functions is discussed as a method to mitigate energy loss in spectral analysis.

PREREQUISITES
  • Understanding of window functions (e.g., Hanning, Hamming)
  • Familiarity with Fourier transforms
  • Knowledge of finite energy and finite power signals
  • Concept of signal normalization
NEXT STEPS
  • Research the calculation methods for correction factors of various window functions
  • Explore the impact of different window functions on spectral analysis
  • Learn about the normalization techniques for window functions
  • Investigate the effects of windowing on finite power signals
USEFUL FOR

Researchers, signal processing engineers, and anyone involved in spectral analysis and window function application will benefit from this discussion.

greydient
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I'm doing research on window functions (such as: rectangular, Hanning, Blackman, etc), but am having trouble with respect to the energy loss associated with each. I know that applying the window causes energy loss in the spectra of interest, and for the Hanning Window and Hamming window, multiplying the FFT by 1.633 and 1.586 respectively offsets this a bit.

How were these two correction factors calculated, and what are the correction factors for other window types?
 
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consider the signal: x(t). they like to classify signals in two broad classes:

finite energy signals:

\int_{-\infty}^{+\infty} \left( x(t) \right)^2 dt = E < \infty

finite power signals:

\lim_{T \to +\infty} \frac{1}{T} \int_{-T/2}^{+T/2} \left( x(t) \right)^2 dt = P < \inftysinusoids, periodic signals, and stocastic signals (some kind of noise) are finite power, but infinite energy (because they are turned on forever). now, whether it is a finite power signal or a finite energy signal, when you window it, it becomes a finite energy signal:

\int_{-\infty}^{+\infty} \left( x(t) w(t) \right)^2 dt = E_w < \infty

when you multiply a time-domain signal with a window, w(t), that has the effect of smoothing the spectrum of x(t) using the Fourier transform of the window. now, if the window function is always less than 1 in magnitude, |w(t)|<1, then it will only reduce x(t) and if it was a finite energy signal, the energy would also be reduced. sometimes they like to normalize window functions by scaling them so that

\int_{-\infty}^{+\infty} w(t) dt =1

that will insure that the window will not reduce the average smoothed values of the spectrum of x(t). sometimes they like:\int_{-\infty}^{+\infty} \left( w(t) \right)^2 dt =1

this will normalize the power spectrum of the window and, i think that means the smoothing done to the power spectrum of x(t) will unscaled, just smoothed.
 
Most likely this can only be answered by an "old timer". I am making measurements on an uA709 op amp (metal can). I would like to calculate the frequency rolloff curves (I can measure them). I assume the compensation is via the miller effect. To do the calculations I would need to know the gain of the transistors and the effective resistance seen at the compensation terminals, not including the values I put there. Anyone know those values?

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