For all the trajectories, the root mean square deviation (RMSD) from the initial structure reached a plateau starting from ∼50 ns.
The MSD j for individual traces was then computed for increasing lag times up to 10Δt (t = 1Δt, 2Δt, … 10Δt) where Δt is the experimental inter-frame time interval of 10.5 ms. We then calculated the average mean square displacement MSD t) for t = 1Δt, 2Δt, … 10Δt as the mean of all the individual traces MSD j (t) for all the trajectories that had a length of at least equal to t.
For all the separated trajectory groups, we integrate the two groups of the separated trajectories if the average likelihood Q before integration and Q ′ after integration satisfy the following inequality: lfloor{log_{10}Q'}rfloor-lfloor{log_{10}Q}rfloor > 0, (8).
Plots of the expected sensation of the edge and corner feature for all trajectories.
The median value for all trajectories reaching the ground was estimated within each 45-km range of group delays.
Here, the coverage prediction enhanced with a building model had the minimum absolute error for all trajectories with 14.887 km/h, followed by Voronoi diagrams with 14.921 km/h and coverage prediction without building model 16.004 km/h.
Table 5 shows for all trajectories on the second floor (used for modeling) the measured average path loss PLms [dB], the predicted path loss PLpr, and the deviation δ [dB] for the considered model for Tx and Rx at heights of 2.5 m and 1 m, respectively.
Table 5 summarizes for all trajectories on the third floor (T1-T5, A-H, and corr) the measured average path loss PLms [dB], the predicted path loss PLpr, and the deviation δ [dB] = PLpr - PLms for the considered model for Tx and Rx at heights of 2.5 m and 1 m, respectively.
MSD, D, L, and L2 were calculated for all trajectories longer than 100 successive frames (5 s at 20 Hz).
This shows that the similarities in local structure formation are trivial and the global folding path is very different for all trajectories.
