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A comparative study of models for predation and parasitism

A comparative study of models for predation and parasitism

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34<br />

the effect <strong>of</strong> Y. In order to show the point, let us assume that a <strong>and</strong> h in eq. (4c. 6)<br />

are the true estimates <strong>of</strong> the factors originally defined, whereas those in eq. (4c. 3)<br />

are superficial <strong>and</strong> are written a' <strong>and</strong> h' respectively. Then the fit <strong>of</strong> eq. (4c. 3) to<br />

data, which should be correctly fitted by eq. (4c. 6), means that<br />

a'Xt/ (1 + a'h'X) = aXYt/ (1 + ahX)<br />

<strong>and</strong> transposing we get<br />

h'=h/Y+ (a'-aY)/aa'XY<br />

or<br />

a'=aY/ (l +aX(h- h'Y) ).<br />

Thus, estimates a' <strong>and</strong> h' not only change as the predator density changes but also<br />

they are a decreasing function <strong>of</strong> the prey density, unless a'=aY <strong>and</strong> h'=h/Y. Fur-<br />

ther, they are not independent <strong>of</strong> the units in which the densities <strong>of</strong> both populations<br />

are measured. Hence, such estimates have no universal value.<br />

Secondly, the depletion <strong>of</strong> prey or, in the case <strong>of</strong> <strong>parasitism</strong>, super<strong>parasitism</strong>,<br />

<strong>of</strong>ten occurred in the observations. If eq. (4c. 3) is applied to such data, it is the<br />

same as fitting the instantaneous equation to one <strong>of</strong> the cross-sections parallel to the<br />

Z-Xo plane <strong>of</strong> the surface generated by eq. (4c. 9) in the case <strong>of</strong> <strong>predation</strong>, or eq.<br />

(4c. 10) in the case <strong>of</strong> <strong>parasitism</strong>. Obviously, the curve <strong>of</strong> a cross-section parallel to<br />

the Z-Xo plane, as in Fig. 3a, changes as Y or t changes, <strong>and</strong> there<strong>for</strong>e the estimates<br />

<strong>for</strong> factors a <strong>and</strong> h should change accordingly. Again such estimates have no univer-<br />

sal value.<br />

The third point is concerned with a precaution that should be taken when prey<br />

density is changed by changing the size <strong>of</strong> the experimental universe, a method <strong>of</strong>ten<br />

adopted to obtain an extremely high prey density with relatively few individuals (e. g.<br />

MORRIS 1963; HAYNES <strong>and</strong> SISOJEVIC 1966).<br />

If this is done, however, it should<br />

be noticed that the predator density changes too. To assess z in this method, we<br />

measure a cross-section <strong>of</strong> the surface which goes diagonally across the xo-Yt plane.<br />

As far as I know, all the published literature in which HOLLING'S disc equation<br />

is applied, involves at least one <strong>of</strong> the above three misapplications. Yet, the goodness<br />

<strong>of</strong> fit is, in many cases, remarkably high. This is because the equation involves two<br />

factors that are normally estimated from the observed relationships between z <strong>and</strong><br />

x0. That is to say, the nature <strong>of</strong> the estimation ensures that the resultant curve fits<br />

the observation well. Hence, a good fit does not constitute verification <strong>of</strong> the theory.<br />

In my opinion, the significance <strong>of</strong> HOLLING'S simulation experiment with discs<br />

<strong>and</strong> tapping is to show the importance <strong>of</strong> the factor h, <strong>and</strong> this simple model is<br />

sufficient to show that "the area <strong>of</strong> discovery", i.e. /i, cannot be independent <strong>of</strong> prey<br />

or host density, as clearly deduced from eqs. (4c. 9) or (4c. 10). However, an application<br />

<strong>of</strong> the original model as in eq. (4c. 3) to a situation in which the effect <strong>of</strong> diminishing<br />

returns is obviously involved, is incorrect.

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