Book, Paragraph

 1 III, 5 |      same amount of air in any ratio provided it is numerically
 2 III, 6 |    part determined by the same ratio (not taking in the same
 3 III, 6 |         But if we increase the ratio of the part, so as always
 4 III, 7 |       have divided in the same ratio as the largest quantity
 5  IV, 8 |        the speed have the same ratio to the speed, then, that
 6  IV, 8 |      movement.~Now there is no ratio in which the void is exceeded
 7  IV, 8 |        by body, as there is no ratio of 0 to a number. For if
 8  IV, 8 |   exceeds 2, still there is no ratio by which it exceeds 0; for
 9  IV, 8 | Similarly the void can bear no ratio to the full, and therefore
10  IV, 8 |        with a speed beyond any ratio. For let Z be void, equal
11  IV, 8 |        the void will bear this ratio to the full. But in a time
12  IV, 8 |        air in thickness in the ratio which the time E bears to
13  IV, 8 |      body which is in the same ratio to the other body as the
14  IV, 8 |       two movements there is a ratio (for they occupy time, and
15  IV, 8 |    occupy time, and there is a ratio between any two times, so
16  IV, 8 |       finite), but there is no ratio of void to full.~These are
17  IV, 8 |        equal space, and in the ratio which their magnitudes bear
18  IV, 8 |     through the void with this ratio of speed. But that is impossible;
19 VII, 5 |    half the weight B: then the ratio between the motive power
20 VII, 5 |       and proportionate to the ratio in the other, so that each
21 VII, 5 |       traverse a part of G the ratio between which and the whole
22 VIII, 1|   order. Moreover, there is no ratio in the relation of the infinite
23 VIII, 1|     whereas order always means ratio. But if we say that there
24 VIII, 1|   sometimes not) or there is a ratio in the variation. It would