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The average fill weight of 20 capsules was determined.
The average fill factors were unchanged (within experimental uncertainty).
Weights of the contents and empty shells were obtained, and the average fill weight was recorded.
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Scanning electron microscopy and coulometric analysis are used for experimental evaluation of the average filling of pores with metal.
We do this by investigating the two-point correlation function C_{mathrm{DW}}(r)= -1)^{r} bigllangle delta n_{i}^{mathrm{pol}} delta n_{i+r}^{mathrm{pol}} bigrrangle, (4) where (delta n_{i}^{mathrm{pol}} = -1{mathrm{pol}}_{i}-bar{n}) denotes the polariton fluctuation from the average filling (bar{n}).
The average "fill-up" for the vehicle will be about $3 for 100 miles.
Through these experiments, the averaged filling rate was found to be around 85%%.
Analysis of all found subgraphs in the decomposition of the Bounded Hamming Graph reveals that the lion's share of them have high edge fill-ins (the average edge fill-in is 0.94), thus confirming that I gR epertoireC onstructor indeed finds dense subgraphs of the Bounded Hamming Graph.
The lion's share of large connected components in the Bounded Hamming Graph (i.e. components with more than 100 vertices) have similar structures characterized by small edge fill-ins; the average edge fill-in for large components is 0.32 (Supplementary Fig. A4).
Here's how to subtract each sample observation from the average: To fill the third column, simply take each term from the sample observations and subtract it from 14, the sample mean.
Good reproducibility was evident when measuring the maximum and average filling and ejection rates, time to peak filling rate, ejection fraction, the modulus of chamber stiffness, the time course of left ventricular relaxation, global average stress and ventricular work indexes using the model described above.
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