Skógræktarritið - 15.05.2001, Page 150

Skógræktarritið - 15.05.2001, Page 150
Fig. 2 (a). The mean local abundance from the pale-colored center-region in Fig. I is presented as a traditional time series diagram with density at the ordinate and time at the abcissa (continuous line). The time units could for example be years. The density could be for example number of individuals per spatial unit on average in a sample taken within a grid cell at a given point in time. For comparison, a coarse- scale view of the mean density for the 12-cell transect as a whole is also shown (stip- pled line). The coarse scale series is aperiodic, while the finer-scale center-region series shows an apparent 10-step periodicity for most of the time series (b). The separate time series for two neighboring center-region grid cell densities show an approximately 20-year outbreak cycle, with one of the patches lagging approx. 10 time steps behind the other patch’s peak in abundance. In comparison to Fig. 2 (a), we see that periodicity is strongly dependent on observational scale in this example, spanning from period 20 at fine scale (1 grid cell), period 10 at some- what coarser scale (2-3 grid cells), and aperiodicity at ''regional" scale (12 grid cells). "outside", i.e. with zero rate of immigration to the model arena as a whole. The reason for long- term survival can be found in the complex spatio-temporal fluctua- tions that prevail at finer scales due to local dispersal. At any point in time there is always some local population or anoth- er increasing in number, and thus being ready to contribute to revitalize neighboring localities through dispersal during a future local "bust". Contrary to the mean field scenario where the model population responds dynamically as a single unit, the spatially structured population in Fig. 1 gives migration as an intrin- sic process of the system rather than an extrinsic forcing func- tion. Thus, the immigration rate to the total population in Fig. I is set to zero (only local inter- patch dispersal takes place) and the total population still survives in the long run in spite of fre- quent local extinctions at fine scales. From an empirical point of view, this kind of effect on spa- tio-temporal fluctuations on population viability may be called "common knowledge" (e.g., Andrewartha and Birch 1954). However, the point is that from a theoretical perspective, the inclusion of space in the model opens for a huge step for- ward in terms of realism. There has been a long tradition in the- oretical ecological modeling where this kind of realism has been more or less ignored, but present-day modeling has be- come much more sophisticated (McGlade 1999). The "toy" model simulation insight from formulating the spa- tial dimension(s) explicitly instead of "averaging out" local processes may initiate a cascade of new investigations involving real data as well as model refine- ments. Analysis of the „toy" model example in Fig. 1, and similar models from the litera- ture, predicts that neighborhood dispersal leads to a pattern of outbreaks that tend to be damp- ened due to spatial fluctuation asynchrony at coarser scales than the correlation length given by the typical scale of dispersal distance. New data used to test this hypothesis may then lead to a more coherent theory with a better predictive power than the starting point of a too simplistic non-spatial model. Another interesting observa- tion from a specific model output in Fig. 2 is that one particular “time series" apparently pro- duces a -20 temporal unit inter- val periodicity at the grid cell scaie, ~10 unit periodicity at spa- tial scale 2 (two neighbor grid cells), and aperiodicity at coarser scales. The new questions that can be raised from this result are then (for example): what makes 148 SKÓGRÆKTARRITIÐ 2001 l.tbl.
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