1 Viscek Model : Polarization

  • Polarisation based on the paper of Vicsek et al. (1995)
  • How to form polarized groups of free particles
  • Vsicel Model in polar coordinate system
  • Motions of Equations:
  • \(\left \langle \theta_{j}(t) \right \rangle_{r}\) is the average orientiation of particles at distance smaller than \(r\) with respect to particel \(i\)
  • \(\bigtriangleup \theta_{i}\) is the rotational nosie

1.2 Case II : video

1.3 Polarisation (Order Parameter) Vs noise intensity

2 Modified Viscek Model : Attraction

  • The following attraction Model and equations chosen from the paper of Costanzo and Hemelrijk (2018).
  • To perform attraction, the following parameters have to modfiy

  • Maximal angular velocity

  • \(\omega = [0/\bigtriangleup t, +\pi/\bigtriangleup t]\)

  • \(\bigtriangleup \Theta_{i} = [-\pi, +\pi]\)

  • when \(v = 0\), particles do not move and mill

  • when \(v => \infty\), particles get complete mixing without milling

  • For milling (attraction) when \(v > 0\) and \((v\bigtriangleup t/r << 1)\)

2.1 Case I : video

2.2 Case II : video

2.3 Case III : video

2.4 Attraction (Order Parameter) Vs noise intensity

2.5 Phase diagram : Attraction (OP) Vs Noisy Intensity

  • with the attraction Model the paper of Costanzo and Hemelrijk (2018), it found that the phase transition diagram is at noise intensity = 0.5, where the order of parameter for Attraction is minmium.

Reference

Costanzo, A, and CK Hemelrijk. 2018. “Spontaneous Emergence of Milling (Vortex State) in a Vicsek-Like Model.” Journal of Physics D: Applied Physics 51 (13): 134004.

Vicsek, Tamás, András Czirók, Eshel Ben-Jacob, Inon Cohen, and Ofer Shochet. 1995. “Novel Type of Phase Transition in a System of Self-Driven Particles.” PRL 75 (6): 1226–9. https://link.aps.org/doi/10.1103/PhysRevLett.75.1226.