ApplauSim: A Simulation of Synchronous Applause Rhythmic Applause as an Emergent Phenomenon? Andi Horni, Lara Montini, IVT, ETH Zürich.

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ApplauSim: A Simulation of Synchronous Applause Rhythmic Applause as an Emergent Phenomenon? Andi Horni, Lara Montini, IVT, ETH Zürich

Motivation 2 Lecture Prof. Dr. Rainer Hegselmann, last 2 credit points Create a parsimonious model vs. large-scale daily business MATSim emergence

3

Synchronous Applause 4 Period doubling (frequency bisection) 73 persons [Néda, Z., E. Ravasz, T. Vicsek, Y. Brechet and A.-L. Barabási (2000) Physics of the rhytmic applause, Physical Review E, 61 (6) 6987–6992]

Synchronous Applause 5 The game is learned … 1 individual, 1 week East vs. West-> videos

Synchronous Applause 6 Period doubling and frequency dispersion [ Y. Kuramoto and I. Nishikava, J. Stat. Phys. 49, 569 ~1987!.] K C : kritical coupling D: oscillators’ natural frequencies dispersion I: normal clapping II: synchronous clapping

First Models 7 seminal paper Neda, Ravasz, Vicsek,Brechet, Barabási (2000) Kuramoto and Nishikava (1987): globally coupled oscillators applied to clapping Li, Liu, Sun and Han (2009):

Type of Model 8 descriptive, explicative? multi-agent but not in software structure matrices! (LaHowara & Commander Spock) MATLAB SourceForge

«Behavioral» Model 9 Kuramoto’s globally coupled oscillators see also Xenides, Vlachos and Simones (2008): C prio, I prio

From Peaks to a Rhythm - Exogeneity 10 searching for the “frequency band” with the highest regularity f 0,  0 f 1,  1 tt exogeneity problem different for every agent (errors, sound=f(distance)) band not pre-specified

From Peaks (and Gaps) to a Rhythm – In More Detail 11  loudness : average loudness in window  lenght : boundaries of window --->  gap : depth of gaps (listen to peaks and gaps)

From Peaks to a Rhythm: Adaptation 12 regimes for adaptation (categories in human perception and behavior)  new = f(  )  g(  current,  perceived ) (  = frequency, phase) rwrw  1.0  f  perceived  current   f  r max  t-  t  decreasing with t  phase stronger than frequency

Main Hypothesis 13 … period doubling why does this help constant errors:  target = f(  perceived +  motor ) with  perceived = f(… +  perception ); and   f(frequency) experiments -> synchronizers

Results - Configurations 14 1.high frequencies (  =4Hz,  =1Hz) (a)6 synchronizers in the center (b)6 synchronizers at the fringe (c)variable number and distribution of synchr. 2.low frequencies (  =2Hz,  =0.5Hz) (a)6 synchronizers in the center (b)6 synchronizers at the fringe (c)variable number and distribution of synchr. 3. no synchronizers, low frequencies 4. no errors, high frequencies 30 runs each, 6 x 6 persons

15 1.a

16 1.b

17 2.a

18 2.b

19 3

20 4

Conclusions 21 influence of errors influence of synchronizers phase synchronization problem transition process f high -> f low  start frequencies general or temporal effect heterogeneity of agents excitement level (Xenides et al. 2008) loudness synchronization will

and now? 22 course points playground: MATSim & emergence “one of the most seductive buzzwords of complexity science” MacKay (2008, p.T274) “when constructing agent systems, you should regard emergence as an important concept” … “you can try to “design in” the emergence that you want”. Odell (1998) Functional form of MATSim queue-based network load simulation

Emergence and Non-Linearity 23 Superposition principle invalid -> non-linear regimes  usually between 5 and 11 BPR function for traffic assignment: MATSim: multi-agent transport simulation queue model for network load (link) simulation

Evaluation of MATSim Network Load Simulation 24

25 MATSimBPR

26 MATSimBPR

27 MATSim

Emergence and Non-Linearity 28 agent interactions feedback -> non-linear in nature (Goldstein 1999)

The End and Applause