Let A, B, and C be the three given commensurable magnitudes.
It is required to find the greatest common measure of A, B, and C.
Take the greatest common measure D of the two magnitudes A and B.
Either D measures C, or it does not measure it.
First, let it measure it.
Since then D measures C, while it also measures A and B, therefore D is a common measure of A, B, and C. And it is manifest that it is also the greatest, for a greater magnitude than the magnitude D does not measure A and B.
Next, let D not measure C.
I say first that C and D are commensurable.
Since A, B, and C are commensurable, some magnitude measures them, and this of course measures A and B also, so that it also measures the greatest common measure of A and B, namely D.
But it also measures C, so that the said magnitude measures C and D, therefore C and D are commensurable.
Now take their greatest common measure E.
Since E measures D, while D measures A and B, therefore E also measures A and B. But it measures C also, therefore E measures A, B, and C. Therefore E is a common measure of A, B, and C.
I say next that it is also the greatest.
For, if possible, let there be some magnitude F greater than E, and let it measure A, B, and C.
Now, since F measures A, B, and C, it also measures A and B, and therefore measures the greatest common measure of A and B.
But the greatest common measure of A and B is D, therefore F measures D.
But it measures C also, therefore F measures C and D. Therefore F also measures the greatest common measure of C and D. But that is E, therefore F measures E, the greater the less, which is impossible.
Therefore no magnitude greater than the magnitude E measures A, B, and C. Therefore E is the greatest common measure of A, B, and C if D does not measure C, but if it measures it, then D is itself the greatest common measure.
Therefore the greatest common measure of the three given commensurable magnitudes has been found.
From this it is clear that, if a magnitude measures three magnitudes, then it also measures their greatest common measure. The greatest common measure can be found similarly for more magnitudes, and the corollary extended.