Four variants of PSO (basic PSO, chaotic PSO, PSO with median tracking, and PSO with mean and median tracking) are compared and tested for optimization of controller gains for four-area distributed AGC.
Finally, 100 Monte Carlo simulations have been run for each case, and the fusion performance of nonlinear tracking is compared between our MCB algorithm and the UKF-SCI algorithm [12] with feedback structure.
The basic performances, such as the detection efficiency and its uniformity, as well as the hit multiplicity for single tracks were compared to those of the conventional electronics based on the simple threshold discriminators.
On the homogenous FBN substrate, the migration tracks were compared between the control cells exhibiting calcium oscillations (Fig. 4D) and the cells whose calcium oscillations were inhibited by loading the cells with calcium chelators (Fig. 4E).
Fourth, the number of individual CESA puncta in a given track were compared by the calculation: CesAD = TL/Pn where CESAD is CESA density along a track, TL is the track length over 61 frames (µm) and Pn is the average particle number along that track.
For each participant, GPS tracks were compared among three conditions: powered by engine only, by engine and wind (i.e., using the sails), or by wind only.
Finally, the sensitivity scores from the two tracks were compared in order to i) validate the predictions from the hybrid model, and ii) investigate the role of essential and modulatory parameters and perturbations.
The new transfers were done using a high-resolution Pro Tools system, and each track was compared with both its vinyl LP and 1987 CD incarnations.
The detection result of a reliable object already being tracked is compared to the tracking result of GMM-SAMT to check if the detection result is still valid; see Figure 1.
FEM interface stress states, inside and outside the tire track, are compared with stress histories undergone by specimens tested with the most common devices, such as guillotine or inclined.
