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202 II Seeing How It Works<br />

They’re independent with respect to symmetric difference—their product is the empty<br />

shape. But this isn’t so for the product of their boundaries<br />

It’s a single point. As a result, bðxÞ l bðyÞ<br />

is missing a point that’s in bðx l yÞ<br />

More generally, common pieces of boundary elements in the maximal elements in the<br />

symmetric difference of x and y are lost in the symmetric difference of their boundaries.<br />

But it’s easy to fix this when shapes are divided into parts according to whether<br />

or not their maximal elements are embedded in common ones.<br />

The following equivalence relation does the trick.<br />

Let two basic elements be coembedded whenever they’re embedded in a common<br />

element.<br />

The effect of this is clear in the shape A<br />

that’s divided into three different parts A 1 , A 2 , and A 3<br />

(This is a nice way to store maximal elements in a computer. After all, it’s how an<br />

experienced draftsman would normally draw the parts of a shape made up of lines.<br />

But notice that the relation doesn’t organize points, as it does basic elements of higher<br />

dimension—lines and planes and solids—when j is more than i.) Then two other<br />

facts—in addition to the fact that symmetric difference works for coembedded<br />

elements—are used to exploit this kind of division. First, the symmetric difference of

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