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267<br />

IRREVERSIBILITY-THE ENTROPY BARRIER<br />

Suppose that our knowledge of initial conditions permits us<br />

to localize a system in a small cell of the phase space. During<br />

its evolution, we shall see this initial cell twist and turn and,<br />

like an amoeba, send out "pseudopods" in all directions,<br />

spreading out in increasingly thinner and ever more twisted<br />

filaments until it finally invades the whole space. No sketch<br />

can do justice to the complexity of the actual situation. Indeed,<br />

during the dynamic evolution of a mixing system, two<br />

· points as close together in phase space as we might wish may<br />

head in different directions. Even if we possess a lot of information<br />

about the system so that the initial cell formed by its<br />

representative points is very small, dynamic evolution turns<br />

this cell into a true geometric "monster" stretching its network<br />

of filaments through phase space.<br />

p<br />

Figure 34. Typical evolution in phase space of a cell corresponding to a<br />

"mixing" system. The volume is still conserved but no more its form: the cell<br />

progressively spreads through the whole phase space.<br />

q

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