| Literature DB >> 30128129 |
Christopher F Clements1, Arpat Ozgul1.
Abstract
Critical transitions are qualitative changes of state that occur when a stochastic dynamical system is forced through a critical point. Many critical transitions are preceded by characteristic fluctuations that may serve as model-independent early warning signals, implying that these events may be predictable in applications ranging from physics to biology. In nonbiological systems, the strength of such early warning signals has been shown partly to be determined by the speed at which the transition occurs. It is currently unknown whether biological systems, which are inherently high dimensional and typically display low signal-to-noise ratios, also exhibit this property, which would have important implications for how ecosystems are managed, particularly where the forces exerted on a system are anthropogenic. We examine whether the rate of forcing can alter the strength of early warning signals in (1) a model exhibiting a fold bifurcation where a state shift is driven by the harvesting of individuals, and (2) a model exhibiting a transcritical bifurcation where a state shift is driven by increased grazing pressure. These models predict that the rate of forcing can alter the detectability of early warning signals regardless of the underlying bifurcation the system exhibits, but that this result may be more pronounced in fold bifurcations. These findings have important implications for the management of biological populations, particularly harvested systems such as fisheries, and suggest that knowing the class of bifurcations a system will manifest may help discriminate between true-positive and false-positive signals.Entities:
Keywords: critical slowing down; early warning signals; population collapse; rate of forcing; regime shifts; tipping points
Year: 2016 PMID: 30128129 PMCID: PMC6093161 DOI: 10.1002/ece3.2531
Source DB: PubMed Journal: Ecol Evol ISSN: 2045-7758 Impact factor: 2.912
Figure 1Simulated population collapses with different rates of change of the harvesting parameter (a subset of six rates of forcing are shown), using the (a) the fold bifurcation model described in Dakos et al. (2012) and (b) the transcritical bifurcation model described in Kéfi et al. (2013)
The parameter values for the fold bifurcation model (described in Dakos et al. 2012) and the transcritical model (described in Kéfi et al. 2013)
| Parameter | Description | Units | Value |
|---|---|---|---|
| Fold bifurcation model | |||
|
| Population growth rate | time−1 | 1 |
|
| Carrying capacity | – | 100 |
|
| Half‐saturation constant | – | 1 |
|
| Harvesting rate | × time−1 | Various |
| σ | Variance of white noise | – | 0.5 |
| Transcritical bifurcation model | |||
|
| Population growth rate | time−1 | 1 |
|
| Carrying capacity | – | 100 |
|
| Harvesting rate | × time−1 | Various |
| σ | Variance of white noise | – | 0.5 |
Indicates parameter values taken from the relevant publications.
Figure 2Strength of the trend in five leading indicators of population collapse when time‐series lengths were standardized (see section 2) across (a) simulated population collapses exhibiting a fold bifurcation, and (b) simulated population collapses exhibiting a transcritical bifurcation. Violin plots indicate the distribution of Kendall tau values for each rate of forcing
Figure 3Strength of the trend in five leading indicators of population collapse when time‐series lengths were nonstandardized (see section 2) across (a) simulated population collapses exhibiting a fold bifurcation, and (b) simulated population collapses exhibiting a transcritical bifurcation. Violin plots indicate the distribution of Kendall tau values for each rate of forcing
Figure 4The length of time series for currently extant (in 2015, vertical dashed line) populations is determined by the monitoring effort in the preceding decades (solid black line) rather than the timing of the population crash. The total possible length of a time series is determined not only by the monitoring effort but also by the time to collapse, which in turn is governed by the rate of forcing of the system (dotted and dashed black lines)