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BSA Flow Software Installation and User's Guide - CSI

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Resampling<br />

Sample-Hold<br />

Even with very high data rate the upper frequency of the calculated spectrum<br />

is limited, since the measured velocities are averaged over the time it takes<br />

for the seeding particle to cross the measuring volume, <strong>and</strong> the transit time<br />

thus limits the upper frequency. For most LDA experiments the latter is no<br />

problem, since normally this upper limit is well above the highest frequency<br />

of interest.<br />

To reduce calculation time, the Fourier transformations in (7-67) are<br />

implemented using Fast Fourier Transformation (FFT). These algorithms<br />

require the discrete samples to be evenly distributed in time, <strong>and</strong> the process<br />

of converting the discrete representation of the time history record into an<br />

evenly spaced time history record with constant interarrival times is called<br />

resampling.<br />

Several methods for resampling have been suggested, <strong>and</strong> [Schmidt (1997)]<br />

recommends the use of either sample/hold interpolation or exponential<br />

interpolation by [Høst Madsen & Caspersen (1995)]. Sample/hold<br />

interpolation is the most wide-spread of the two, <strong>and</strong> also the easiest to<br />

implement:<br />

{ uresamp() t u( ti)| ( tit ti)<br />

}<br />

= ≤ < +1 (7-71)<br />

As shown in Figure 7-83, the sampled velocity is simply assumed to be<br />

constant until a new sample indicates that the velocity has changed.<br />

U(t)<br />

True velocity<br />

Sample/Hold velocity<br />

ti - ti-1 =<br />

R<strong>and</strong>om time<br />

between true<br />

samples<br />

True sample (burst)<br />

Resample<br />

∆t =<br />

Fixed time<br />

between<br />

resamples<br />

Figure 7-83 R<strong>and</strong>om sampling, sample/hold <strong>and</strong> resampling.<br />

The sampled <strong>and</strong> held signal is resampled at regular intervals to provide a<br />

series of evenly distributed velocity samples.<br />

This simple approach presents two immediate problems both shown in<br />

Figure 7-83. If two neighboring true samples are further apart than the time<br />

between resamples, the first one will be resampled several times although no<br />

new information about the flow is available. If on the other h<strong>and</strong> there is<br />

more than one true sample in the time between two resamples, the<br />

information contained in all but the last one will be lost, since the resampling<br />

always take the value of the latest true sample.<br />

7-126 <strong>BSA</strong> <strong>Flow</strong> <strong>Software</strong>: Reference guide<br />

t

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