Biology Letters’ special feature on Hamilton's legacy pays due tribute to a brilliant mind. Herbers [1] and the other contributors paint a compelling picture of how Hamilton's work on inclusive fitness anticipated much contemporary evolutionary thinking, although sometimes not acknowledged until much later.
A more recent, although equally cited work by Hamilton is the ‘Geometry for the selfish herd’ [2], an elegant mathematical description of why individuals aggregate in space. In the spirit of this special feature [1], I illustrate why Hamilton's herd model should be recognized as an early mathematical formalism applicable to unrelated, although crucial, biological phenomena. Notably, Hamilton's model of gregarious behaviour can be directly applied to the problem of context-dependent acoustic signalling as follows, with the potential to describe how interdependent individual calls combine into choruses.
Many animals communicate acoustically, often with an emphasis on signal timing, rather than other acoustic properties [3]. Synchrony and chorusing occur in insects, amphibians, birds and mammals. An overarching question is how individuals ‘distribute’ their calls over time and why different individuals’ calls group together, leading to synchronous, alternating or phase-locked choruses [3]. Two hypotheses, suggested and tested in [4], predict clusters of calls: individuals could maximize overall sound intensity to attract females or, alternatively, individuals could call in quasi-synchrony to decrease the individual risk of predation. In both cases, individuals would tend to call close to each other, so to increase signal amplitude or alter individual conspicuousness (depending on the receiver), similarly to what happens in human applauding [5].
Suppose three frogs, A, B and C, call periodically in time, say every second, although with different relative phases (see figure 1). B and C occur within a short time interval (short silence). A precedes them by a long interval (long SILENCE). The resulting acoustic pattern is A-SILENCE-B-silence-C-SILENCE-A- … A can modify its conspicuousness by shortening its ‘domain of silence’, i.e. timing its signal so it co-occurs, on average, with others’ calls. The most noise-robust, error-resistant strategy for A is to delay its call and signal exactly halfway between B and C; A calls, on average, in an ‘acoustically dense’ time period.
Assume, after Hamilton, that individuals A, B and C are located on a circular lily pond [2]. Instead of delaying or anticipating their signal phase/timing, they try to hide in-between other individuals. For instance, A occupies an isolated position on the pond, making it vulnerable to predators. A therefore seeks to decrease its ‘domain of danger’: if B and C are closer to each other than A is to any of them, A will jump and land between B and C [2].
Once formulated in these terms, it is clear how the mechanics of Hamilton's spatial predation model map one-to-one onto the acoustic signalling mechanism sketched here (table 1). The original spatial model featured a closed, circular space. Circular metaphors (e.g. clocks) are also appropriate to represent periodic events, and the ‘circular’ feature in [2] enables its direct application to periodic signals over time, as required in models of chorusing.
Table 1.
gregarious behaviour [2] | context-dependent signalling (present model) |
---|---|
circular lily pond | time period (1 unit) |
moving agent (e.g. frog) | acoustic signal produced by agent |
agent location | time of signal produced by agent |
movement clockwise or counter-clockwise | signal delay or anticipation |
distance between two agents | time elapsed between two agents’ signals |
‘domain of danger’ | ‘domain of silence’: the amount of silence, measured in time units, preceding and following a call |
In both cases, a general model is derived from applying the basic ‘time shift’ mechanism to all individuals (cf. figure 1, A delays its call and C anticipates its), and dynamically over time (figure 1a versus b). At every time period, most individuals will have either changed location or adapted their calls, making previous decisions suboptimal and spurring individuals to compensate by jumping to a better location, or shifting the phase of their upcoming call to an acoustically denser period of time. Computer simulations for the predation model showed formation of clusters of individuals [2]. By analogy, group signalling dynamics should begin with randomly occurring individual calls scattered over time and converge towards a few, high-intensity acoustic peaks (produced by several near-synchronous individuals).
An additional, deeper mathematical link connects Hamilton's model of space with dynamical processes in time. Hamilton noted that only one initial configuration, three evenly spaced frogs, will prevent aggregation [2]; decades later, the mathematical investigation of rhythm and timing in biological systems found that the same initial configuration will prevent synchronization of oscillators in time [6].
Herbers admits that one volume cannot do full justice to Hamilton's genius, anticipating how his ideas will ‘influence the field over the coming 50 years’ [1]. Hopefully, as I show here, Hamilton's mathematical insights will inform future research on both rhythmic processes in humans, such as language and music, and context-dependent acoustic signalling in other species.
Acknowledgements
I sincerely thank Eoin O'Sullivan, Bill Thompson, Dan Bowling and Ruth Sonnweber for comments, and Tecumseh Fitch and Simon Kirby for advice.
Funding statement
Research supported by ERC Advanced grant no. 230604 SOMACCA (to W. Tecumseh Fitch) and the University of Vienna (KWA and Alfred-Ebenbauer grants).
References
- 1.Herbers JM. 2013. 50 years on: the legacy of William Donald Hamilton. Biol. Lett. 9, 20130792 (doi:10.1098/rsbl.2013.0792) [DOI] [PMC free article] [PubMed] [Google Scholar]
- 2.Hamilton WD. 1971. Geometry for the selfish herd. J. Theor. Biol. 31, 295–311 (doi:10.1016/0022-5193(71)90189-5) [DOI] [PubMed] [Google Scholar]
- 3.Grafe TU. 1999. A function of synchronous chorusing and a novel female preference shift in an anuran. Proc. R. Soc. Lond. B 266, 2331–2336 (doi:10.1098/rspb.1999.0927) [Google Scholar]
- 4.Ryan MJ, Tuttle MD, Taft LK. 1981. The costs and benefits of frog chorusing behavior. Behav. Ecol. Sociobiol. 8, 273–278 (doi:10.1007/BF00299526) [Google Scholar]
- 5.Néda Z, Ravasz E, Brechet Y, Vicsek T, Barabási AL. 2000. Self-organizing processes: the sound of many hands clapping. Nature 403, 849–850 (doi:10.1038/35002660) [DOI] [PubMed] [Google Scholar]
- 6.Strogatz SH, Stewart I. 1993. Coupled oscillators and biological synchronization. Sci. Am. 269, 102–109 (doi:10.1038/scientificamerican1293-102) [DOI] [PubMed] [Google Scholar]