Simulation of Collective Motion of Self Propelled Particles in Homogeneous and Heterogeneous Medium

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Simulation of Collective Motion of Self Propelled Particles in Homogeneous and Heterogeneous Medium IJCSNS International Journal of Computer Science and Network Security, VOL.18 No.11, November 2018 109 Simulation of Collective Motion of Self Propelled Particles in Homogeneous and Heterogeneous Medium Israr Ahmed†, Inayatullah Soomro††, Syed Baqer Shah†††, Hisamuddin Shaikh†††† SALU Khairpur Pakistan Abstract Large groups of animals moves very long distances and The concept of self-propelled particles is used to study the they cross rivers and forest [5]. Inspite of these facts, there collective motion of different organisms such as flocking of birds, has been limited research done on the effect of swimming of schools of fish or migrating of bacteria. The heterogeneous media on the collective behaviour of self- collective motion of self-propelled particles is investigated in the propelled particles [6]. Avoidance behaviour of the presence of obstacles and without obstacles. A comparison of the effects of interaction radius, speed and noise on the collective particle from the obstacle was simulated by the croft et al motion of self-propelled particles is conducted. It is found that in [7]. In this work measurement of effect was carried out the presence of obstacles, mean square displacement of the when a single particle collided with the static obstacles. It particles shows large fluctuation, whereas without obstacles was found that there are higher chances of collision of fluctuation is less. It is also shown that in the presence of the social interactions with the obstacles. This is due to the obstacles, an optimal noise, which maximizes the collective huge supposition and the occurrence of large parameter motion of the particles, exists values. Moreover, the creation of motion due to the social Key words: interaction produces key effects on the metrics used to Self-propelled particles, Collective motion, Obstacles. inform management and policy decisions.Mecholsky et al [8] worked on a continuous model in which flocks of birds were considered. Study was done on the linearized 1. Introduction interaction of the flocks with an obstacle. Behaviour of the Movements in dynamic and complex environments are an flocks was shown by the density disturbance when there integral part of the daily life activities; this includes was a interaction with the obstacles. The disturbance was walking in crowded spaces, playing sports, etc. Many of similar to the Mach cones where order was demonstrated these tasks that humans perform in such environments by the anistropic spread of waves of flocking. Chepizkho involve interactions with stationary or moving obstacles. In et al [9] focused on the dynamics of the self-propelled this context, it is important to note that there is always a particles in the heterogeneous medium. In their model need to coordinate the information with other individuals obstacles were randomly distributed in two dimensional to deal with the obstacles [1]. There are other examples spaces. In this model, particle showed avoidance from the obstacle, and the particle’s avoiding behaviour was also exist where living things deal with the obstacles such γ as flocks of birds facing obstacles while moving expressed by the turning speed . The mean square collectively. Understanding the detection and avoidance displacement of the SPPs produced two regimes as a from the obstacles when there is noise in the system is of function of obstacle density ρo and the particle’s turning extreme importance. Many studies have addressed the speed γ . It was found that, in first regime small value of interaction of individuals with obstacles from different γ produces diffusive movement of particle and perspectives. For example, in computer science field several studies have been carried out where robots interact determined by diffusive coefficient which demonstrated a with obstacles [2-4]. There are limited studies done to least at an intermediate obstacle density ρo . In second investigate the dynamics of natural systems which deal regime, it was found that for large obstacle densities and with the obstacles. Dynamics of the particles in the for higher values of γ , spontaneous trapping of the SPPs presence of the obstacles is often observed. Complex occurred. In their model it was also shown that the collective behaviour is exhibited by the bacteria in the presence of fixed and moving obstacles can change the presence of the obstacles. For example, collective dynamics of the collective behaviour of the particles. behaviour of bacteria was found in the heterogeneous Moreover, optimal noise amplitude took place which medium such as highly complex tissues in gastrointestinal maximised the collective motion. This kind of optimality tract or soil. does not appear in the homogeneous medium. Due to the smaller obstacle densities, order parameter showed a single Manuscript received November 5, 2018 Manuscript revised November 20, 2018 110 IJCSNS International Journal of Computer Science and Network Security, VOL.18 No.11, November 2018 critical point, under this point the model showed long and direction of the particle is given by the following range order akin to the homogeneous medium. In the case equation: of large obstacle densities two critical points appeared and θ (t + ∆t) = θ (t) + h(x ) +η∆θ (2) made the motion disordered at both smaller and larger i r i noise amplitudes. Furthermore, there was the existence of In equation 1, x represents the position of ith particle, i quasi long range order in between these critical points [5]. In this research work, computer simulation is done for the vi (t) is the velocity of the particle with absolute self-propelled particles in homogeneous media and in velocity v . ∆t is the time interval that particles take to heterogeneous media. Here the term heterogeneous applies o when the collective motion of the particles is investigated move from one point to another. in the presence of the obstacles whereas the term In equation 2, θ represents the direction of the particle i homogeneous is consideredWhen collective behaviour of and ∆θ is the random fluctuation in the system, which is the particles is studied without obstacles. We compare the effects of the interaction radius, speed and noise on the created by noiseand has value in the range of [−π ,π ].η collective motion of self-propelled particles with and is the noise amplitude. θ (t) represents the average without obstacles. It is found that, in the existence of the r obstacles, mean square displacement of the particles direction of the particles which is within the interaction r r exhibit huge fluctuations in the system, whereas without radius , where is the radius of interaction between the obstacle density this displacement of the SPPs shows very self-propelled particles. θ (t) is given in the following r less fluctuating behaviour. It is also observed that in the equation: existence of the obstacles, optimal noise exists which θ (t) = arctan{ sin(θ ) cos(θ ) } (3) maximises the collective motion of the particles. Optimal r r r noise that increases the collective motion is helpful in Equation 3 has been taken from [10].The function h(x ) developing and understanding migration and navigation i strategies in moveable or non-moveable heterogeneous in equation 2 defines the interaction of particle with media, which help to understand evolution and adaptation of stochastic components in natural systems which show obstacles. Through this function particles avoid the collective motion. obstacles that are located in its neighborhood: γ 0 ∑ sin(αθki, −> i) ,if no (x i ) 0 n ()x −< 2. Methodology oixyikR o h()xi = A two dimensional continuum time model is introduced for 00, if noi()x = . N self-propelled Particles (SPPs). The model b demonstrates the effects of various parameters on the (4) collective behaviour of the SPPs. Motion of the particles is The equation 4 is taken from [5]. Through this equation restricted to the two dimensional box of size L having periodic boundary conditions. Particles interact with each obstacle is introduced. Here xi is the position of ith particle, other according to the same rule as in Vicsek et al [10] and y k is the position of kth obstacle. Ro is known as the where particle follows the average direction of the interaction radius between particle and obstacle. neighbours within the radius r .Spatial heterogeneity is no (xi ) represents the number of the obstacles located at given by the presence of the No fixed obstacles. The new element in the equation of motion of self-propelled the distance less than Ro from xi . In the above equation particles is introduced by the obstacle avoidance two conditions are given. Firstly, if is greater than interaction as it is given in Ref. [5]. Obstacles are no (xi ) randomly distributed in the system. Noise parameter is also zero, h(xi ) will show interaction with obstacles, secondly, introduced in the system, which is randomly given and has values between [−π ,π ] . At the initial time-step each if no (xi ) is equal to zero, h(xi ) will be zero. In equation particle has a random position and a random direction. 4, the term | xi − y k |< Ro , means that if the distance Particles update their positions as follows: between the obstacle and particle is less than the xi (t + ∆t) = xi (t) + vi (t)∆t, (1) interaction radius Ro , then the summation of sine IJCSNS International Journal of Computer Science and Network Security, VOL.18 No.11, November 2018 111 3. Results and Discussion (∑sin(α k,i −θi )) will take place. Number of sine values that will be summed, depends on the number of Simulation was performed in a square box of length L. We obstacles n ( ) that are located in the interaction radius η = o xi first considered the case in which noise was, 0.01.At initial time steps particles moved randomly with constant range of the particle xi .
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