1 00:00:00,000 --> 00:00:05,000 In this video, we show the example data sets included in the paper, animated over time. 2 00:00:05,000 --> 00:00:12,000 These are four example data sets of three trajectories rotating around a central point on a circle in different manners. 3 00:00:12,000 --> 00:00:19,000 We show the motion of the particles in a fixed global reference system. 4 00:00:19,000 --> 00:00:26,000 The trajectories are the result of a super- position of two rotational movements: 5 00:00:26,000 --> 00:00:32,000 a rotation of the local reference system with the angular speed p 6 00:00:32,000 --> 00:00:38,200 and a rotation of the particles in this local reference system with the angular speed q. 7 00:00:38,200 --> 00:00:46,000 When observed in this optimal reference system, their objective rotations become clear: we can see their varying direction and speed. 8 00:00:46,033 --> 00:00:53,999 In another, non-optimal reference system though (here taken from the top left example) their behavior becomes more obscure. 9 00:00:54,033 --> 00:00:58,999 We now show our new measure, TRV, on a number of data sets. 10 00:00:59,000 --> 00:01:05,000 These trajectories show drifter buoys advected by ocean currents in the North Atlantic Ocean. 11 00:01:05,000 --> 00:01:11,000 They are sparsely distributed, their nearest neighbors several hundred kilometers away. 12 00:01:11,000 --> 00:01:17,000 Still, our new method, TRV, is able to pick up objective rotational behavior. 13 00:01:17,000 --> 00:01:23,666 High rotation can be observed on a few trajectories in the North Atlantic Gyre, around Iceland and Greenland. 14 00:01:23,666 --> 00:01:28,666 As a second example, we applied TRV on insect trajectories. 15 00:01:28,666 --> 00:01:35,666 These 3D trajectories were reconstructed from videos of midges in a large translucent box. 16 00:01:35,666 --> 00:01:42,666 While their behavior seems erratic, TRV highlights some insects of especially high and low rotational behavior 17 00:01:42,666 --> 00:01:49,666 These TRV values can change rapidly when the set of neighbors changes. 18 00:01:49,666 --> 00:01:57,532 This happens as midges disappear from the tracked set, or move too far away. 19 00:01:57,533 --> 00:02:02,533 With this data set, the movement of socially distancing pedestrian crowds has been studied. 20 00:02:02,533 --> 00:02:08,533 Here, 32 study participants move quickly within an enclosed space, while attempting to keep a social distance of 1.5m from each other. 21 00:02:08,533 --> 00:02:15,333 The group at large tends to move in a counterclockwise rotation, but only six individuals show high objective rotation. 22 00:02:15,333 --> 00:02:20,333 Finally, we show the changing objective rotation over time in a simulation of bird-like agents (boids). 23 00:02:20,333 --> 00:02:26,333 In an initial chaotic phase, the boids all show strong rotational behavior. 24 00:02:26,333 --> 00:02:32,333 To simulate emergent behavior found in bird flocks or fish swarms, each individual agent follows a simple set of rules. 25 00:02:32,333 --> 00:02:38,333 Swarms form as the boids align with their neighbors, showing a decrease in their rate of rotation by TRV. 26 00:02:38,333 --> 00:02:44,333 At this point, all boids find themselves as part of established swarms, and seize to rotate. 27 00:02:44,333 --> 00:02:49,899 Only intermittent rotational behavior can be observed in single individuals.