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Finally, the Trajectory project can be used to analyze results from molecular dynamics simulations or geometry optimization and coordinate driving performed by external programs.
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(a) The solution trajectory projected on ((y,z -plane.
(a) The solution trajectory projected on ((z,w -plane.
Panel A shows a trajectory projected in the (v_{1}-theta ) plane for (C=0.18).
Each interburst interval occurs when the trajectory projected to ((na_{i}, ca_{i})) space lies in the silent region.
While the burst continues, all four superslow variables increase until the trajectory projected to ((ca_{i}, l, c_{mathrm{tot}}))-space goes above the l-nullsurface (not shown here).
That is, as l becomes faster, the trajectory projected into ((c_{mathrm{tot}}, l -space wil -spacethe spiking/bursting boundary curve ((mathrm{SN}_{1})) earlier and hence small bursts give willto a long bureacharlier (Fig. 10C).
However, although the fixed point in ((v, h)) remains stable for all (ca_{i}), the SS trajectory projected into ((v, h))-space jumps away from the family of fixed points, to larger v, after staying nearby for a finite time.
To figure this out, we notice that after multiple crossings of the HC curve and returns to quiescence in Fig. 5C, the trajectory projected to ((na_{i}, ca_{i})) space starts oscillating near the HC curve, instead of going back again to the quiescent state (see Fig. 5D for an enlarged view of oscillations near the HC curve).
This was done through the transformation equation
We examined the RMS fluctuations of each trajectory projected onto its five most representative principal components (PC).
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