- Access by Xinjiang University
Cascading failures in interdependent systems under a flow redistribution model
Phys. Rev. E 97, 022307 – Published 15 February, 2018
DOI: https://doi.org/10.1103/PhysRevE.97.022307
Abstract
Robustness and cascading failures in interdependent systems has been an active research field in the past decade. However, most existing works use percolation-based models where only the largest component of each network remains functional throughout the cascade. Although suitable for communication networks, this assumption fails to capture the dependencies in systems carrying a flow (e.g., power systems, road transportation networks), where cascading failures are often triggered by redistribution of flows leading to overloading of lines. Here, we consider a model consisting of systems and with initial line loads and capacities given by and , respectively. When a line fails in system , fraction of its load is redistributed to alive lines in , while remaining fraction is redistributed equally among all functional lines in ; a line failure in is treated similarly with giving the fraction to be redistributed to . We give a thorough analysis of cascading failures of this model initiated by a random attack targeting fraction of lines in and fraction in . We show that (i) the model captures the real-world phenomenon of unexpected large scale cascades and exhibits interesting transition behavior: the final collapse is always first order, but it can be preceded by a sequence of first- and second-order transitions; (ii) network robustness tightly depends on the coupling coefficients and , and robustness is maximized at non-trivial values in general; (iii) unlike most existing models, interdependence has a multifaceted impact on system robustness in that interdependency can lead to an improved robustness for each individual network.
Physics Subject Headings (PhySH)
Article Text
References (45)
- R. R. Rajkumar, I. Lee, L. Sha, and J. Stankovic, in 10 Proceedings of the 47th Design Automation Conference (ACM, New York, NY, USA, 2010), pp. 731–736.
- W. Li, A. Bashan, S. V. Buldyrev, H. E. Stanley, and S. Havlin, Phys. Rev. Lett. 108, 228702 (2012).
- S. V. Buldyrev, R. Parshani, G. Paul, H. E. Stanley, and S. Havlin, Nature 464, 1025 (2010).
- J. Gao, S. V. Buldyrev, S. Havlin, and H. E. Stanley, Phys. Rev. Lett. 107, 195701 (2011).
- O. Yağan, D. Qian, J. Zhang, and D. Cochran, IEEE Trans. Parallel Distrib. Syst. 23, 1708 (2012).
- C. D. Brummitt, R. M. D'Souza, and E. Leicht, Proc. Natl. Acad. Sci. USA 109, E680 (2012).
- S. M. Rinaldi, in Proceedings of the 37th annual Hawaii international Conference on System sciences (IEEE, Big Island, HI, USA, 2004), p. 8.
- G. Bianconi and S. N. Dorogovtsev, Phys. Rev. E 89, 062814 (2014).
- D. Qian, O. Yağan, L. Yang, and J. Zhang, in Proceedings of the 2012 IEEE Global Communications Conference (IEEE, Anaheim, CA, USA, 2012), pp. 2072–2077.
- Y. Zhuang and O. Yağan, IEEE Trans. Network Sci. Eng. 3, 211 (2016).
- O. Yağan and V. Gligor, Phys. Rev. E 86, 036103 (2012).
- O. Yağan, D. Qian, J. Zhang, and D. Cochran, IEEE J. Sel. Areas Commun. 31, 1038 (2013).
- Y. Zhuang, A. Arenas, and O. Yağan, Phys. Rev. E 95, 012312 (2017).
- R. Parshani, S. V. Buldyrev, and S. Havlin, Phys. Rev. Lett. 105, 048701 (2010).
- S.-W. Son, G. Bizhani, C. Christensen, P. Grassberger, and M. Paczuski, Europhys. Lett. 97, 16006 (2012).
- B. Min, S. D. Yi, K.-M. Lee, and K.-I. Goh, Phys. Rev. E 89, 042811 (2014).
- K.-M. Lee, C. D. Brummitt, and K.-I. Goh, Phys. Rev. E 90, 062816 (2014).
- C. Wu, S. Ji, R. Zhang, L. Chen, J. Chen, X. Li, and Y. Hu, Europhys. Lett. 107, 48001 (2014).
- A. Vespignani, Nature 464, 984 (2010).
- S. V. Buldyrev, N. W. Shere, and G. A. Cwilich, Phys. Rev. E 83, 016112 (2011).
- J. Gao, S. V. Buldyrev, H. E. Stanley, and S. Havlin, Nat. Phys. 8, 40 (2012).
- F. Radicchi, Nat. Phys. 11, 597 (2015).
- M. A. Di Muro, S. V. Buldyrev, H. E. Stanley, and L. A. Braunstein, Phys. Rev. E 94, 042304 (2016).
- A. Huang, H. M. Zhang, W. Guan, Y. Yang, and G. Zong, Math. Problems Eng. 2015, 16 (2015).
- R. da Silveira, Am. J. Phys. 67, 1177 (1999).
- Y. Moreno, A. Correig, J. Gómez, and A. Pacheco, J. Geophys. Res.: Solid Earth 106, 6609 (2001).
- D. L. Turcotte and M. T. Glasscoe, Tectonophysics 383, 71 (2004).
- Y. Zhang and O. Yağan, Sci. Rep. 6, 27625 EP (2016).
- S. Pradhan, A. Hansen, and B. K. Chakrabarti, Rev. Mod. Phys. 82, 499 (2010).
- O. Yağan, Phys. Rev. E 91, 062811 (2015).
- A. E. Motter and Y.-C. Lai, Phys. Rev. E 66, 065102 (2002).
- W.-X. Wang and G. Chen, Phys. Rev. E 77, 026101 (2008).
- B. Mirzasoleiman, M. Babaei, M. Jalili, and M. A. Safari, Phys. Rev. E 84, 046114 (2011).
- In addition, Ref. [6] considers a specific load-capacity relation, while our work covers more general settings.
- A. Scala, P. G. D. S. Lucentini, G. Caldarelli, and G. D'Agostino, Physica D: Nonlin. Phenom. 323, 35 (2016).
- P. Crucitti, V. Latora, and M. Marchiori, Phys. Rev. E 69, 045104 (2004).
- Of course, there are other ways for two networks to be “interdependent” with each other. Here, we use this term with its general meaning, i.e., that failures in one network may lead to failures in the other and vice versa, potentially leading to a cascade of failures. Our model constitutes a special case where interdependence emerges from the interconnectivity between the two networks.
- D. T. Nguyen, Y. Shen, and M. T. Thai, IEEE Trans. Smart Grid 4, 151 (2013).
- H. Elsinger, A. Lehar, and M. Summer, Manage. Sci. 52, 1301 (2006).
- Let be an event. Then, is a Binomial random variable that takes the value of 1 if takes place, and 0 otherwise.
- This is also evident from Eqs. (1), where we see that depends not only on but also on .
- S. Pahwa, A. Hodges, C. Scoglio, and S. Wood, in Proceedings of the Systems Conference, 2010 4th Annual IEEE (IEEE, San Diego, CA, USA, 2010), pp. 272–276.
- We believe this is because the network size is taken to be very large in the experiments and the random variable converges almost surely to its mean (e.g., by virtue of Strong Law of Large Numbers); though it is beyond the scope of this paper to prove this.
- We note that the behavior demonstrated here is fundamentally different from the few other cases in the literature where multiple transitions have been reported; e.g., see Refs. [8, 18]. There, the type or the number of transitions do not change with the level of coupling across the networks. Instead, multiple transitions arise only when networks with different robustness levels are coupled together, and their total (or, average) size is plotted against the size of the attack that is applied to all networks involved.
- R. Parshani, S. V. Buldyrev, and S. Havlin, Proc. Natl. Acad. Sci. USA 108, 1007 (2011).