| Literature DB >> 26064664 |
Andrew M Reynolds1, Hayley B C Jones2, Jane K Hill3, Aislinn J Pearson4, Kenneth Wilson5, Stephan Wolf6, Ka S Lim1, Don R Reynolds7, Jason W Chapman8.
Abstract
Understanding the complex movement patterns of animals in natural environments is a key objective of 'movement ecology'. Complexity results from behavioural responses to external stimuli but can also arise spontaneously in their absence. Drawing on theoretical arguments about decision-making circuitry, we predict that the spontaneous patterns will be scale-free and universal, being independent of taxon and mode of locomotion. To test this hypothesis, we examined the activity patterns of the European honeybee, and multiple species of noctuid moth, tethered to flight mills and exposed to minimal external cues. We also reanalysed pre-existing data for Drosophila flies walking in featureless environments. Across these species, we found evidence of common scale-invariant properties in their movement patterns; pause and movement durations were typically power law distributed over a range of scales and characterized by exponents close to 3/2. Our analyses are suggestive of the presence of a pervasive scale-invariant template for locomotion which, when acted on by environmental cues, produces the movements with characteristic scales observed in nature. Our results indicate that scale-finite complexity as embodied, for instance, in correlated random walk models, may be the result of environmental cues overriding innate behaviour, and that scale-free movements may be intrinsic and not limited to 'blind' foragers as previously thought.Entities:
Keywords: Lévy flights; behavioural bursts; intermittent locomotion; power-law distributions; spontaneous movement patterns
Year: 2015 PMID: 26064664 PMCID: PMC4453252 DOI: 10.1098/rsos.150085
Source DB: PubMed Journal: R Soc Open Sci ISSN: 2054-5703 Impact factor: 2.963
Figure 1.Flight activity in a female noctuid moth, Apamea monoglypha. (a) An example of a displacement time-series showing intermittency. (b) Rank frequency distribution of pause durations longer than 10 s (solid line) together with the best-fit power law (dashed line) and the best-fit stretched exponential (dotted line). The maximum-likelihood estimate for the power-law exponent is μ=1.57. (c) Rank frequency distribution of flight distances longer than 1 m (solid line) together with the best-fit power law (dashed line) and the best-fit exponential (dotted line). The maximum-likelihood estimate for the power-law exponent is μ=1.57. (d) Power-spectrum of the displacement time-series data.
Figure 2.Flight activity in an African armyworm moth (Spodoptera exempta). (a) An example of a displacement time-series showing intermittency. (b) Rank frequency distribution of pause durations longer than 10 s (solid line) together with the best-fit power law (dashed line) and the best-fit stretched exponential (dotted line). The maximum-likelihood estimate for the power-law exponent is μ=1.7. (c) Power-spectrum of the displacement time-series data (solid line) together with the best-fit power (dashed line).
Figure 3.Flight activity in a honeybee, Apis mellifera. (a) An example of a displacement time-series showing intermittency. (b) Rank frequency distribution of pause durations longer than 10 s (solid line) together with the best-fit power law (dashed line) and the best-fit stretched exponential (dotted line). The maximum-likelihood estimate for the power-law exponent is μ=1.37. (c) Rank frequency distribution of flight distances longer than 1 m (solid line) together with the best-fit power law (dashed line) and the best-fit exponential (dotted line). The maximum-likelihood estimate for the power-law exponent is μ=1.45. (c) Power-spectrum of the displacement time-series data.
Figure 4.Walking activity patterns of Drosophila melanogaster within a 5.0 cm diameter arena. Data for 10 males and 10 females were collected by Ueno et al. [11] (solid lines). Rank frequency distributions for pause and walk durations (solid lines) together with the best-fit power laws (dashed lines) and the best-fit stretched exponentials (dotted lines). The maximum-likelihood estimates of the power-law exponents are μ=1.43 and μ=1.64.