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2D spread plot studies quantify the penetration distances covered by the nanoparticles and fluid atoms in the domain as probability density function differences in both dimensions used.
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The Backus-Gilbert Spread plots in Figure 8 and Figures S7 and S8 reveal similar V-shaped dynamic patterns.
The analysis spread plots well in floristic space.
To visualize the (more homoscedastic) spread, the scatter plots of the FIV1, IC, MIF50 and PIF expressed as percentage differences can be seen in Figure 3.
Conversely, the points on the robotic scatter plot are less spread and more close together.
Unlike the findings of other authors, we were not able to predict the punctured volume, based on the width of the lamella measured by sonography probably due to the wide spread of obtained data (scatter plot).
An equivalent fin width is calculated, which allows reducing the spread in ION scatter plots and highlights relative importance of LER in different fin regions.
The spread is large, but appropriate partitioning of the links can produce individual scatter plots of narrower spread.
In both figures (5 and 6) one can see the interaction of T3 with Dot# as a progressive spread of plot points (and trend lines) as one moves from left to right – possibly more so in the 0 2 ms range.
Sampling plots were selected by probability sampling, with sampling designs that spread the plots evenly over the study area.
The (unlogged) series as well as the balance-sheet-total-to-GDP ratio and the interest rate spread are plotted in Fig. 2.
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