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223 ‘‘Nor Do Lineaments Have Anything to Do with Material’’<br />

algebras of weights where physical properties and mathematical ideas interact on equal<br />

footing to get a nice result.<br />

Weights are already familiar in architecture, graphics, and the visual arts, where<br />

lines of different thickness are used in drawing<br />

It’s no big deal to extend this idea in a variety of ways—to points, for example, when<br />

they have area<br />

and to planes and solids when they’re filled with tones<br />

as I’ve already shown. Such properties have a neat algebra with a relation and operations<br />

that correspond to parts and to sum and difference in an algebra of shapes.<br />

Suppose that two lines of different thickness defined by numerical values—pen<br />

size will do—are drawn at the same time, either one overlapping the other<br />

The thicker line appears at full length, while the thinner one is shortened. And if the<br />

two lines have equal thickness, then a single line is formed<br />

In both of these experiments, the weight of the embedded segment common to the<br />

lines is the maximum of the combined weights. So for the weights u and v, it’s just<br />

the case that<br />

u þ v ¼ maxfu; vg<br />

And for parts, it’s easy to see that u a v when<br />

u þ v ¼ v<br />

The way weights combine in differences, however, isn’t as clear as it is for sums, and<br />

there’s little in drawing that offers genuine guidance. But algebraic considerations

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