Propagation of regularity and finite-time collisions for the thermomechanical Cucker-Smale model with a singular communication

  • Received: 01 September 2017 Revised: 01 October 2017
  • 70F99, 92B25

  • We study dynamical behaviors of the ensemble of thermomechanical Cucker-Smale (in short TCS) particles with singular power-law communication weights in velocity and temperatures. For the particle TCS model, we present several sufficient frameworks for the global regularity of solution and a finite-time breakdown depending on the blow-up exponents in the power-law communication weights at the origin where the relative spatial distances become zero. More precisely, when the blow-up exponent in velocity communication weight is greater than unity and the blow-up exponent in temperature communication weights is more than twice of blow-up exponent in velocity communication, we show that there will be no finite time collision between particles, unless there are collisions initially. In contrast, when the blow-up exponent of velocity communication weight is smaller than unity, we show that there can be a collision in finite time. For the kinetic TCS equation, we present a local-in-time existence of a unique weak solution using the suitable regularization and compactness arguments.

    Citation: Young-Pil Choi, Seung-Yeal Ha, Jeongho Kim. Propagation of regularity and finite-time collisions for the thermomechanical Cucker-Smale model with a singular communication[J]. Networks and Heterogeneous Media, 2018, 13(3): 379-407. doi: 10.3934/nhm.2018017

    Related Papers:

  • We study dynamical behaviors of the ensemble of thermomechanical Cucker-Smale (in short TCS) particles with singular power-law communication weights in velocity and temperatures. For the particle TCS model, we present several sufficient frameworks for the global regularity of solution and a finite-time breakdown depending on the blow-up exponents in the power-law communication weights at the origin where the relative spatial distances become zero. More precisely, when the blow-up exponent in velocity communication weight is greater than unity and the blow-up exponent in temperature communication weights is more than twice of blow-up exponent in velocity communication, we show that there will be no finite time collision between particles, unless there are collisions initially. In contrast, when the blow-up exponent of velocity communication weight is smaller than unity, we show that there can be a collision in finite time. For the kinetic TCS equation, we present a local-in-time existence of a unique weak solution using the suitable regularization and compactness arguments.



    加载中
    [1] On collision-avoiding initial configurations to Cucker-Smale type flocking models. Comm. Math. Sci. (2012) 10: 625-643.
    [2] J. A. Carrillo, Y. -P. Choi and M. Hauray, Local well-posedness of the generalized CuckerSmale model with singular kernels, Mathematical Modeling of Complex Systems, 17-35, ESAIM Proc. Surveys, 47, EDP Sci., Les Ulis, 2014. doi: 10.1051/proc/201447002
    [3] Sharp conditions to avoid collisions in singular Cucker-Smale interactions. Nonlinear Anal.-Real. (2017) 37: 317-328.
    [4] J. A. Carrillo, Y. -P. Choi and S. Pérez, A review on attractive-repulsive hydrodynamics for consensus in collective behavior, in Active Particles Vol. Ⅰ - Advances in Theory, Models, Applications(tentative title), Series: Modeling and Simulation in Science and Technology, (eds. N. Bellomo, P. Degond, and E. Tadmor), Birkhäuser Basel, (2017), 259-298.
    [5] Asymptotic flocking dynamics for the kinetic Cucker-Smale model. SIAM J. Math. Anal. (2010) 42: 218-236.
    [6] Global classical solutions of the Vlasov-Fokker-Planck equation with local alignment forces. Nonlinearity (2016) 29: 1887-1916.
    [7] Y. -P. Choi, S. -Y. Ha and Z. Li, Emergent dynamics of the Cucker-Smale flocking model and its variants, in Active Particles Vol. Ⅰ - Advances in Theory, Models, Applications(tentative title), Series: Modeling and Simulation in Science and Technology, (eds. N. Bellomo, P. Degond, and E. Tadmor), Birkhäuser Basel, (2017), 299-331.
    [8] Avoiding collisions in flocks. IEEE Trans. Automatic Control (2010) 55: 1238-1243.
    [9] Emergent behavior in flocks. IEEE Trans. Automat. Control (2007) 52: 852-862.
    [10] A kinetic flocking model with diffusion. Comm. Math. Phys. (2010) 300: 95-145.
    [11] Fluid dynamic description of flocking via Povzner-Boltzmann equation. Physica D (2011) 240: 21-31.
    [12] S. -Y. Ha, J. Kim, C. Min, T. Ruggeri and X. Zhang, Uniform stability and mean-field limit of thermodynamic Cucker-Smale model, Submitted.
    [13] Emergent behaviors of Thermodynamic Cucker-Smale particles. SIAM J. Math. Anal. (2018) 50: 3092-3121.
    [14] Uniform stability of the Cucker-Smale model and its application to the mean-field limit. Kinet. Relat. Models (2018) 11: 1157-1181.
    [15] Emergent dynamics for the hydrodynamic Cucker-Smale system in a moving domain. SIAM. J. Math. Anal. (2015) 47: 3813-3831.
    [16] Emergence of time-asymptotic flocking in a stochastic Cucker-Smale system. Commun. Math. Sci. (2009) 7: 453-469.
    [17] A simple proof of Cucker-Smale flocking dynamics and mean field limit. Commun. Math. Sci. (2009) 7: 297-325.
    [18] From particle to kinetic and hydrodynamic description of flocking. Kinetic Relat. Models (2008) 1: 415-435.
    [19] Emergent dynamics of a thermodynamically consistent particle model. Arch. Ration. Mech. An. (2017) 223: 1397-1425.
    [20] On the Cucker-Smale flocking with alternating leaders. Quart. Appl. Math. (2015) 73: 693-709.
    [21] Cucker-Smale flocking under rooted leadership with fixed and switching topologies. SIAM J. Appl. Math. (2010) 70: 3156-3174.
    [22] Heterophilious dynamics: Enhanced Consensus. SIAM Review (2014) 56: 577-621.
    [23] A new model for self-organized dynamics and its flocking behavior. J. Statist. Phys. (2011) 144: 923-947.
    [24] The Cucker-Smale equation: Singular communication weight, measure-valued solutions and weak-atomic uniqueness. Arch. Ration. Mech. Anal. (2018) 227: 273-308.
    [25] Discrete Cucker-Smale flocking model with a weakly singular weight. SIAM J. Math. Anal. (2015) 47: 3671-3686.
    [26] Existence of piecewise weak solutions of a discrete Cucker-Smale's flocking model with a singular communication weight. J. Differ. Equat. (2014) 257: 2900-2925.
    [27] Cucker-Smale flocking under hierarchical leadership. SIAM J. Appl. Math. (2007) 68: 694-719.
    [28] Flocks, herds, and Schools: A quantitative theory of flocking. Physical Review E. (1998) 58: 4828-4858.
    [29] Swarming patterns in a two-dimensional kinematic model for biological groups. SIAM J. Appl. Math. (2004) 65: 152-174.
    [30] Novel type of phase transition in a system of self-driven particles. Phys. Rev. Lett. (1995) 75: 1226-1229.
    [31] C. Villani, Topics in Optimal Transportation, American Mathematical Society, 2003. doi: 10.1007/b12016
    [32] C. Villani, Optimal Transport, Old and New, Springer-Verlag, 2009. doi: 10.1007/978-3-540-71050-9
  • Reader Comments
  • © 2018 the Author(s), licensee AIMS Press. This is an open access article distributed under the terms of the Creative Commons Attribution License (http://creativecommons.org/licenses/by/4.0)
通讯作者: 陈斌, bchen63@163.com
  • 1. 

    沈阳化工大学材料科学与工程学院 沈阳 110142

  1. 本站搜索
  2. 百度学术搜索
  3. 万方数据库搜索
  4. CNKI搜索

Metrics

Article views(5730) PDF downloads(432) Cited by(15)

Article outline

Figures and Tables

Figures(1)

Other Articles By Authors

/

DownLoad:  Full-Size Img  PowerPoint
Return
Return

Catalog