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The SNRLOSS measure values obtained from each algorithm (include UP) were subjected to statistical analysis in order to assess their significant differences.
The Closeness Measure values obtained for the stereo white signal for all schemes lie in between those obtained for the more sparse mono brown noise signal and the less sparse mono white noise signal, except for the FEA scheme, which yields the same values as for the mono white noise signal.
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Table 3 F-measure values obtained with different abridging and bandwidth parametrization given as the percentage of the best result.
Figure 4 depicts the precision, recall, and F-measure values obtained for these relative cutoff points (numeric values at Table 6).
Transverse stiffness predictions were compared with experimentally measured values obtained by vibration testing.
Figure 13 shows the comparison of the measured values obtained by different algorithms.
Figure 12 shows the comparison of the measured values obtained by different algorithms for the brake pad and the bearing.
The efficiency values calculated using the presently suggested analytical approach are compared with those measured values obtained by two different sizes of NaI (Tl) detectors.
Calculated temperature distribution and chemical conversion are compared with the experimentally measured values obtained with a 5 kW prototype reactor tested in a solar furnace.
DP model validation was made by comparing the measured values obtained on experimental studies, which were conducted under refrigerant mass flow rate range of 34.6 245.6 kg h−1 and evaporation pressure of 200 500 kPa.
Fig. 11 Comparison of the measured values obtained by different algorithms randomly run ten times with the optimal lens magnification and light intensity index: a brake pad; b bearing; c big standard cuboid; and d small standard cuboid.
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Justyna Jupowicz-Kozak
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