* 1.11 Magnitudes commensurable are suchwhich one and the selfe same mea∣sure doth measure.
First he sheweth what magnitudes are commensurable one to an other. To the better and more cleare vnderstanding of this definition, note that that measure whereby any magnitude is measured, is lesse then the magnitude which it measureth, or at least e∣quall vnto it. For the greater can by no meanes measure the lesse. Farther it behoueth, that that measure if it be equall to that which is measured, taken once make the mag∣nitude which is measured: if it be lesse, then oftentimes taken and repeted, it must pre∣cisely render and make the magnitude which it measureth. Which thing in numbers is easely sene, for that (as was before said) all numbers are commensurable one to an o∣ther. And although Euclide in this definition comprehendeth purposedly, onely mag∣nitudes which are continuall quantities, as are lines, superficieces, and bodies, yet vn∣doubtedly the explication of this and such like places, is aptly to be sought of numbers as well rationall as irrationall. For that all quantities commensurable haue that pro∣portion the one to the other, which number hath to numbers. In numbers therfore, 9 and 12 are commensurable, because there is one common measure which measureth them both, namely, the number 3. First it measureth 12, for it is lesse then 12. and be∣ing taken certaine times, namely, 4 times, it maketh exactly 12: 3 times 4 is 12, it also measureth 9, for it is lesse then 9. and also taken certaine times, namely, 3 times, it ma∣keth precisely 9: 3 times 3 is 9. Likewise is it in magnitudes, if one magnitude measure two other magnitudes, those two magnitudes so measured, are said to be commensura∣ble. As for example, if the line C being dou∣bled,