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BSA Flow Software Installation and User's Guide - CSI

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7.9 Moments (one-time statistics)<br />

7.9.1 Weighting factor<br />

Moments are the simplest form of statistics that can be calculated for a set of<br />

data. The calculations are based on individual samples, <strong>and</strong> the possible<br />

relations between samples are ignored as is the timing of events. This leads<br />

to moments sometimes being referred to as one-time statistics, since samples<br />

are treated one at a time.<br />

In Table 7-2 the formulas for estimating moments are listed. The table<br />

operates with velocity-components xi <strong>and</strong> yi, but this is just examples, <strong>and</strong><br />

could of course be any velocity component, cartesian or not. It could even be<br />

samples of an external signal representing pressure, temperature or<br />

something else.<br />

N−1<br />

Mean u ∑ η u<br />

=<br />

i=<br />

0<br />

i i<br />

N−1<br />

∑ i i<br />

i=<br />

0<br />

2<br />

Variance σ = η ( − )<br />

2<br />

(7-22)<br />

u u (7-23)<br />

2<br />

RMS σ = σ<br />

(7-24)<br />

Turbulence<br />

Tu<br />

Skewness S= ∑ η i( ui<br />

− )<br />

= ⋅<br />

u<br />

σ 100% (7-25)<br />

N −1<br />

1<br />

3<br />

i=<br />

0<br />

Flatness F= ∑ η i( ui<br />

− )<br />

σ<br />

N −1<br />

1<br />

4<br />

i=<br />

0<br />

σ<br />

N −1<br />

∑ η<br />

3<br />

u (7-26)<br />

4<br />

u (7-27)<br />

Cross-Moments uv − u v = i( ui − u)( vi − v)<br />

i=<br />

0<br />

Table 7-2: Formulas for estimating moments<br />

(7-28)<br />

You may find the so-called weighting factor ηi disturbing, as you would<br />

normally expect simply ηi=1/N. Unfortunately this would bias your results,<br />

since LDA-measurements especially in highly turbulent flows tend to<br />

contain more samples of fast particles than slow ones. To compensate for<br />

this fast particles are given less weight than slow ones in the calculations as<br />

described in the following section.<br />

Velocity bias Even for incompressible flows where the seeding particles are statistically<br />

uniformly distributed, the sampling process is not independent of the process<br />

being sampled (that is the velocity field). Measurements have shown that the<br />

particle arrival rate <strong>and</strong> the flowfield are strongly correlated (McLaughlin &<br />

Tiedermann (1973)] <strong>and</strong> [Erdmann & Gellert (1976)]). During periods of<br />

higher velocity, a larger volume of fluid is swept through the measuring<br />

volume, <strong>and</strong> consequently a greater number of velocity samples will be<br />

recorded. As a direct result, an attempt to evaluate the statistics of the flow<br />

field using arithmetic averaging will bias the results in favour of the higher<br />

velocities.<br />

Independent samples One way to avoid this so-called velocity bias is to ensure statistically<br />

<strong>BSA</strong> <strong>Flow</strong> <strong>Software</strong>:Reference guide 7-99

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