02.05.2013 Views

Evolution__3rd_Edition

Evolution__3rd_Edition

Evolution__3rd_Edition

SHOW MORE
SHOW LESS

You also want an ePaper? Increase the reach of your titles

YUMPU automatically turns print PDFs into web optimized ePapers that Google loves.

..<br />

Figure 10.7<br />

Developmental asymmetry in<br />

genotypes of the Australian<br />

sheep blowfly (Lucilia cuprina)<br />

that are, or are not, resistant<br />

to the insecticide malathion.<br />

(a) Developmental asymmetry<br />

in genotypes when the resistant<br />

gene RMal first appeared, soon<br />

after malathion was first used.<br />

+ is the original, non-resistant<br />

genotype. RMal disrupts<br />

development, producing<br />

greater average asymmetry; and<br />

is selectively disadvantageous<br />

in the absence of malathion.<br />

(b) Developmental asymmetry<br />

of RMal flies after modifiers<br />

(M) have evolved to reduce the<br />

developmental disruption; it is<br />

now reduced near to the level of<br />

the original +/+ flies, and in the<br />

absence of malathion RMal has<br />

little selective disadvantage or is<br />

neutral relative to +. The sample<br />

size is 50 flies for each genotype.<br />

Redrawn, by permission of the<br />

publisher, from McKenzie &<br />

O’Farrell (1993).<br />

A morphospace for shells shows all<br />

the shell forms that could possibly<br />

exist<br />

Coiling axis<br />

Mean asymmetry ± s.e.<br />

3<br />

2<br />

1<br />

0<br />

Resistance<br />

genotype<br />

Modifier<br />

genotype<br />

(a) Without modifier (b) With modifier<br />

CHAPTER 10 / Adaptive Explanation 277<br />

+/+ +/RMal RMal/ RMal +/+ +/RMal RMal/ RMal<br />

+/+ +/+ +/+ M/M M/M M/M<br />

growth. The explanation for the quantum jumps is a developmental constraint:<br />

growth, by molting, is dangerous and to grow with a smooth curve would require<br />

frequent risky molts. It is better to molt more rarely and grow in jumps.<br />

Developmental constraints have been suggested as an alternative explanation to natural<br />

selection for two main natural phenomena. One is the persistence of fossil species<br />

for long periods of time without showing any change in form (Section 21.5, p. 606).<br />

The other is the variety of forms to be found in the world. We can imagine plotting a<br />

morphospace for a particular set of phenotypes and then filling in the areas that are and<br />

are not represented in nature.<br />

Raup’s analysis of shell shapes is an elegant example. Raup found that shell shapes<br />

could be described in terms of three main variables: translation rate, expansion rate,<br />

and distance of generating curve from the coiling axis (Figure 10.8). Any shell can be<br />

represented as a point in a three-dimensional space, and Raup plotted the regions in<br />

this space that are occupied by living shells (Figure 10.9).<br />

Large parts of the shell morphospace in Figure 10.9 are not occupied. There are two<br />

general hypotheses to explain why these forms do not exist: natural selection and constraint.<br />

If natural selection is responsible, the empty parts of the morphospace are<br />

regions of maladaptation. When these shell types arise as mutations, they are selected<br />

Initial generating curve<br />

Generating curve<br />

after one revolution<br />

Figure 10.8<br />

The shape of a shell can be described by three numbers.<br />

The translation rate (T) describes the rate at which the coil moves<br />

down the coiling axis: T = 0 for a flat planispiral shell, and is an<br />

increasingly positive number for increasingly elongated shells.<br />

The expansion rate (W) describes the rate at which the shell size<br />

increases; it can be measured by the ratio of the diameter of the<br />

shell at equivalent points in successive revolutions; W = 2 in<br />

the figure. The distance from the coiling axis (D) describes the<br />

tightness of the coil; it is the distance between the shell and the<br />

coiling axis, and in the figure it is half the diameter of the shell.<br />

See Figure 10.9 for many theoretically possible shell shapes with<br />

different values of T, W, and D. Redrawn, by permission of the<br />

publisher, from Raup (1966).

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!