5.4 Filtering Measured Time-Histories
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Statutory Documents - IMO Publications and Documents - Circulars - Maritime Safety Committee - MSC/Circular.616 – Evaluation of Free-Fall Lifeboat Launch Performance – (22 June 1993) - Annex – Evaluation of Free-Fall Lifeboat Launch Performance - Section 5 – Measuring And Filtering Acceleration Forces - 5.4 Filtering Measured Time-Histories

5.4 Filtering Measured Time-Histories

  5.4.1 Because any acceleration time-history is composed of many sinusoids of different frequencies and amplitudes, it often contains sinusoids with frequencies that are of little importance or insignificant. These unwanted or unimportant frequencies can be removed from the time-history. This process is called data filtering. Filtering is performed for many reasons. Perhaps frequencies above some value are not significant for some reason. This is the case with occupant acceleration forces in free-fall lifeboats. Frequencies above 20 hz do not have a significant affect on the body and can be removed from acceleration force time-histories when evaluating occupant response. At other times electrical interference can cause frequencies of some magnitude to be introduced into the data; these should be removed before the data is evaluated.

  5.4.2 In general, there are four types of filters: lowpass, highpass, bandpass, and notch. When using a lowpass filter, only those frequencies below a certain frequency are retained. The opposite is true for a highpass filter; only those frequencies above a certain frequency are retained. When using a notch filter, all frequencies except those within a specified range are retained; those frequencies within the specified range are discarded. A bandpass filter, on the other hand, is used to remove frequencies with a specified range and retain all others. After the appropriate frequencies have been discarded, the filtered time-history can be computed using Equation 5.3 and only those frequencies that were retained.

  5.4.3 This concept of filtering can be represented graphically by again considering the data presented in Figure 5.3. Let us assume that we measured the data represented by the combined curve shown in that figure. Let us further assume that we want to filter this measured data with a 10 hz lowpass filter; any frequency greater than 10 hz will be removed from the data. The amplitude of the filtered time-history can be computed from:

Notice that Equation 5.5 is the same as Equation 5.2 after deleting the term involving the 20 hz frequency. The filtered curve represented by Equation 5.5 is shown in Figure 5.8. It is superimposed over the combined curve from Figure 5.3 so that the effects of filtering can be observed. As can be seen, the filtered curve is much smoother than the unfiltered curve.

This is characteristic of data that has been filtered with a lowpass filter.

Figure 5.8 Filtered Time-History

  5.4.4 Acceleration force time-histories can be filtered using either analog or digital filters. Digital filters include Fourier, Butterworth, and Chebyshev filter functions. In addition, data can be filtered in either the time domain or in the frequency domain. A complete discussion of filter functions and procedures to use them is well beyond the scope of this Circular. Interested readers are referred to Press, et. al. (1989) and Ziemer, et. al. (1983) for a more extensive discussion about filtering measured data.


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