Definitions
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Table of contents
Definitions
- “Commensurable” are magnitudes measured by the same measure.
“Incommensurable” are magnitudes which have no common measure.
- Two straight-lines are commensurable when their bounding area are measured by the same area.
They are incommensurable when their area has no common measure.*
Superphysics Note
- There is an infinite number of straight-lines which are either commensurable or incommensurable.
- Some are commensurable or incommensurable in length only.
- Others are commensurable or incommensurable in area also, with an assigned straight line.
‘Rational’ lines are:
- the assigned straight line
- those straight lines which are commensurable with the assigned straight line, whether in length and in square, or in square only
‘Irrational’ lines are those which are incommensurable with the assigned straight line.*
Superphysics Note
- The [binding] square on the assigned straight line is called ‘rational’
Those areas which are commensurable with it are rational.
But those areas which are incommensurable with it are irrational
- The straight lines which produce those areas are irrational
Proposition 1
Assume there are 2 unequal lines.
- The longer line has more than half of it subtracted
- More than half of the remainder is subtracted
If this happens continually, then some magnitude will eventually be left. It will be less than the lesser laid out magnitude.
Let:
AB
andC
are unequal magnitudesAB
is the longer or greater
We subtract more than half from AB
. From the remainder, we also subtract more than half. If this happens continually, there will be some magnitude left. But it will be less than the magnitude C
.
If we keep on multiplying C
, it will eventually be greater than AB
.
Let it be multiplied, and let DE
be a multiple of C
, and greater than AB
.
Divide DE
into the parts DF
, FG
, GE
equal to `C.
Subtract:
- from
AB
,BH
greater than its half - from
AH
,HK
greater than its half
Repeat this process continually until the divisions in AB
are equal in multitude with the divisions in DE
.
Then, let AK
, KH
, HB
be divisions which are equal in multitude with DF
, FG
, GE
.
The remainder GD
is greater than the remainder HA
because:
DE
is greater thanAB
- from
DE
there has been subtractedEG
less than its half - from
AB
,BH
greater than its half
GD
is greater than HA
The following were subtracted:
- from
GD
, the halfGF
- from
HA
,HK
greater than its half
This is why the remainder DF
is greater than the remainder AK
.
But DF
is equal to C
.
- Therefore
C
is also greater thanAK
. - Therefore
AK
is less thanC
.
Therefore, there is left of the magnitude AB
the magnitude AK
which is less than the lesser magnitude set out, namely C
.
The theorem can be similarly proved even if the parts subtracted be halves.