Book, Paragraph

 1  IV, 10 |          not a part: a part is a measure of the whole, which must
 2  IV, 12 |        an autumn.~Not only do we measure the movement by the time,
 3  IV, 12 |         and the movement; for we measure the movement by the time
 4  IV, 12 |          of the movement. And we measure both the distance by the
 5  IV, 12 |           if the time.~Time is a measure of motion and of being moved,
 6  IV, 12 |  determining a motion which will measure exactly the whole motion,
 7  IV, 12 | determining an amount which will measure out the whole. Further "
 8  IV, 12 |          time.~Since time is the measure of motion, it will be the
 9  IV, 12 |        of motion, it will be the measure of rest too-indirectly.
10  IV, 12 |  measured by time. But time will measure what is moved and what is
11  IV, 12 |         qua at rest; for it will measure their motion and rest respectively.~
12  IV, 12 |         time", while time is the measure of motion and rest.~Plainly,
13  IV, 12 |          if time is directly the measure of motion and indirectly
14  IV, 14 |       then, what is first is the measure of everything homogeneous
15  IV, 14 |     motion is above all else the measure, because the number of this
16  IV, 14 |         held because time is the measure of this kind of locomotion
17  IV, 14 |     movement; for apart from the measure nothing else to be measured
18   V, 3  | definitely limited constitutes a measure.~A thing is "in succession"
19  VI, 2  |          will be either an exact measure of AB or less or greater
20  VI, 2  |         or greater than an exact measure: it makes no difference
21  VI, 7  |          motion which shall be a measure of the whole, the whole
22  VI, 7  |       motion AB which shall be a measure of AB. Now this part of
23  VI, 7  |          no part which will be a measure of the infinite time (for
24  VI, 7  |       some unity which will be a measure of things finite in multitude
25  VI, 7  |          a part which shall be a measure of the whole time, in this
26  VI, 10 |       equal to itself, will be a measure of the whole line. But since
27 VIII, 7 |          is of equal or standard measure is the opposite both of
28 VIII, 9 |          because rotation is the measure of motions it must be the
29 VIII, 9 |         primary motion it is the measure of all other motions. Again,
30 VIII, 10|        that this force will be a measure of the finite force residing