Book,  Paragraph

 1   I,  4 |  complete circle, motion from E to F on the semicircle G
 2   I,  4 |   opposed to motion from F to E on the semicircle H. But
 3   I,  5 |    infinite in one direction, E, and another line, BB, infinite
 4   I,  5 |   line at right angles to it, E, and a moving radius, CD.
 5   I,  5 |      never cease contact with E, but the position will always
 6   I,  5 | something like CE, CD cutting E at F. The infinite line,
 7   I,  6 |      weight of which shall be E. E then is less than C,
 8   I,  6 |   weight of which shall be E. E then is less than C, since
 9   I,  6 |  holds. For instance, suppose E multiplied by three is rather
10   I,  6 |    example, assume the weight E to be commensurate with
11   I,  6 |      mass a part BD of weight E. Then let a mass BF be taken
12   I,  7 |  quantity thus modified by D, E. Then, as D is to B, so
13   I,  7 |     Then, as D is to B, so is E to some finite quantum.
14   I,  7 |      than B, say F. Then take E, bearing the same proportion
15   I,  7 |      the whole BF bears to F. E will produce the motion
16   I,  7 |    the part of this infinite, E, cannot be so modified in
17   I,  7 |  movement in a less time. Let E then, when acted upon by
18   I,  7 |    Then, as D is to CD, so is E to some finite part of B.
19   I,  12|      nor B is predicated. Let E lie between A and B; for
20   I,  12|       a mean between them. In E both C and D must be present,
21   I,  12|   everywhere and therefore in E. Since then A is impossible,
22   I,  12|       are coincident. Now let E stand for the ungenerated,
23   I,  12|       do, F and H coincident, E and F never predicated of
24   I,  12|    and G and H likewise, then E and G must needs be coincident.
25   I,  12|  coincident. For suppose that E is not coincident with G,
26   I,  12|       F will be, since either E or F is predictable of everything.
27   I,  12|     that G is coincident with E.~Now the relation of the
28   I,  12|  relation of the ungenerated (E) to the generated (F) is