Book, Paragraph

 1 III, 5  |          has a particular quantity, e,g, two or three cubits;
 2  IV, 8  |           which is thinner, in time E (if the length of B is egual
 3  IV, 8  |            G will be twice the time E. And always, by so much
 4  IV, 8  |           time, H, a time less than E, however, the void will
 5  IV, 8  |            the ratio which the time E bears to the time H. For
 6  IV, 8  |           as much thinner than D as E exceeds H, A, if it moves
 7   V, 1  |             d) that from which and (e) that to which it proceeds:
 8  VI, 1  |            D, B when its motion was E, and G similarly when its
 9  VI, 1  |          its motion is the three D, E, and Z, and if it is not
10  VI, 2  |             arrived, let us say, at E. Then since A has occupied
11 VII, 1  |             each separately and let E be the motion of A, Z of
12 VII, 5  |      distance in the same time. Let E represent half the motive
13 VII, 5  |            in the same time. But if E move Z a distance G in a
14 VII, 5  |             necessarily follow that E can move twice Z half the
15 VII, 5  |             it does not follow that E, being half of A, will in
16 VII, 5  | proportionate to that between A and E (whatever fraction of AE
17 VIII, 8 |           follows. Suppose the line E is equal to the line Z,
18 VIII, 8 |           from the extreme point of E to G, and that, at the moment
19 VIII, 10|             us suppose that D moves E, a part of B. Then the time
20 VIII, 10|             by continuing to add to E, I shall use up B: but I