THE MECHANICS
34 7
the first chapter or chapters of the real Mechanics which had
been lost. The treatise would doubtless begin with generalities
introductory to mechanics such as we find in the (much
interpolated) beginning of Pappus, Book YIII. It must then
apparently have dealt with the properties of circles, cylinders,
and spheres with reference to their importance in mechanics ;
for in Book II. 21 Heron says that the circle is of all figures
the most movable and most easily moved, the same thing
applying also to the cylinder and sphere, and he adds in
support of this a reference to a proof £ in the preceding Book b
This reference may be to I. 21, but at the end of that chapter
he says that ‘cylinders, even when heavy, if placed on the
ground so that they touch it in one line only, are easily
moved, and the same is true of spheres also, a matter which
ice have already discussed ’; the discussion may have come
earlier in the Book, in a chapter now lost.
The treatise, beginning with chap. 2 after the passage
interpolated from the Bapov\KO<s, is curiously disconnected.
Chaps. 2-7 discuss the motion of circles or wheels, equal or
unequal, moving on different axes (e.g. interacting toothed
wheels), or fixed dn the same axis, much after the fashion of
the Aristotelian Mechanical 'problems.
Aristotle's Wheel.
In particular (chap. 7) Heron attempts to explain the puzzle
of the ‘ Wheel of Aristotle ’, which remained a puzzle up to quite
modern times, and gave rise to the proverb, ‘ rotam Aristotelis
magis torquere, quo magis torqueretur A ‘ The question is ’, says
the Aristotelian problem 24, ‘ why does the greater circle roll an
equal distance with the lesser circle when they are placed about
the same centre, whereas, when they roll separately, as the
size of one is to the size of the other, so are the straight lines
traversed by them to one another V 2 Let AC, BD be quadrants
of circles with centre 0 bounded by the same radii, and draw
tangents AE, BF at A and B. In the first case suppose the
circle BD to roll along BF till D takes the position H; then
the radius ODG will be at right angles to AE, and G will be
at G, a point such that AG is equal to BH. In the second
1 See Yan Capelle, Aristotelis quaestiones mechanicae, 1812, p. 268 sq.
2 Arist. Mechanica, 855 a 28.