Chapter 5
Desargues’s Theorem

19. Desargues’s Theorem and its Demonstration for Plane Geometry by aid of the Axioms of Congruence

Of the axioms given in Sections 18, pp. §§, those of groups II–V are in part linear and in part plane axioms. Axioms 3–7 of group I are the only space axioms. In order to show clearly the significance of these axioms of space, let us assume a plane geometry and investigate, in general, the conditions for which this plane geometry may be regarded as a part of a geometry of space in which at least the axioms of groups I–III are all fulfilled.

Upon the basis of the axioms of groups I–III, it is well known that the so-called theorem of Desargues may be easily demonstrated. This theorem relates to points of intersection in a plane. Let us assume in particular that the straight line, upon which are situated the points of intersection of the homologous sides of the two triangles, is the straight line which we call the straight line at infinity. We will designate the theorem which arises in this case, together with its converse, as the theorem of Desargues. This theorem is as follows:

Theorem 32 (Desargues’s theorem). When two triangles are so situated in a plane that their homologous sides are respectively parallel, then the lines joining the homologous vertices pass through one and the same point, or are parallel to one another.

Conversely, if two triangles are so situated in a plane that the straight lines joining the homologous vertices intersect in a common point, or are parallel to one another, and, furthermore, if two pairs of homologous sides are parallel to each other, then the third sides of the two triangles are also parallel to each other.


pict
Figure 37


As we have already mentioned, Theorem 32 is a consequence of the axioms I–III. Because of this fact, the validity of Desargues’s theorem in the plane is, in any case, a necessary condition that the geometry of this plane may be regarded as a part of a geometry of space in which the axioms of groups I–III are all fulfilled.

Let us assume, as in Sections 1318, pp. §§, that we have a plane geometry in which the axioms I, 1–2 and II–IV all hold and, also, that we have introduced in this geometry an algebra of segments conforming to Section 14.

Now, as has already been established in Section 14, there may be made to correspond to each point in the plane a pair of segments (x,y) and to each straight line a ratio of three segments (u : v : w), so that the linear equation

ux + vy + w = 0
expresses the condition that the point is situated upon the straight line. The system composed of all the segments in our geometry forms, according to Section 14, a domain of numbers for which the properties (1–16), enumerated in Section 13, are valid. We can, therefore, by means of this domain of numbers, construct a geometry of space in a manner similar to that already employed in Section 9 or in Section 12, where we made use of the systems of numbers Ω and Ω(t), respectively. For this purpose, we assume that a system of three segments (x,y,z) shall represent a point, and that the ratio of four segments (u : v : w : r) shall represent a plane, while a straight line is defined as the intersection of two planes. Hence, the linear equation
ux + vy + wz + r = 0
expresses the fact that the point (x,y,z) lies in the plane (u : v : w : r). Finally, we determine the arrangement of the points upon a straight line, or the points of a plane with respect to a straight line situated in this plane, or the arrangement of the points in space with respect to a plane, by means of inequalities in a manner similar to the method employed for the plane in Section 9.

Since we obtain again the original plane geometry by putting z = 0, we know that our plane geometry can be regarded as a part of geometry of space. Now, the validity of Desargues’s theorem is, according to the above considerations, a necessary condition for this result. Hence, in the assumed plane geometry, it follows that Desargues’s theorem must also hold.

It will be seen that the result just stated may also be deduced without difficulty from Theorem 23 in the theory of proportion.

20. The Impossibility of Demonstrating Desargues’s Theorem for the Plane without the Help of the Axioms of Congruence22

We shall now investigate the question whether or no in plane geometry Desargues’s theorem may be deduced without the assistance of the axioms of congruence. This leads us to the following result:

Theorem 33. A plane geometry exists in which the axioms I 1–2, II–III, IV 1–5, V, that is to say, all linear and all plane axioms with the exception of axiom IV, 6 of congruence, are fulfilled, but in which the theorem of Desargues (Theorem 32) is not valid. Desargues’s theorem is not, therefore, a consequence solely of the axioms mentioned; for, its demonstration necessitates either the space axioms or all of the axioms of congruence.

Proof. Select in the ordinary plane geometry (the possibility of which has already been demonstrated in Section 9, pp. §§) any two straight lines perpendicular to each other as the axes of x and y. Construct about the origin O of this system of co-ordinates an ellipse having the major and minor axes equal to 1 and 1 2, respectively. Finally, let F denote the point situated upon the positive x-axis at the distance 3 2 from O. Consider all of the circles which cut the ellipse in four real points. These points may be either distinct or in any way coincident. Of all the points situated upon these circles, we shall attempt to determine the one which lies upon the x-axis farthest from the origin. For this purpose, let us begin with an arbitrary circle cutting the ellipse in four distinct points and intersecting the positive x-axis in the point C. Suppose this circle then turned about the point C in such a manner that two or more of the four points of intersection with the ellipse finally coincide in a single point A, while the rest of them remain real. Increase now the resulting tangent circle in such a way that A always remains a point of tangency with the ellipse. In this way we obtain a circle which is either tangent to the ellipse in also a second point B, or which has with the ellipse a four-point contact in A. Moreover, this circle cuts the positive x-axis in a point more remote than C. The desired farthest point will accordingly be found among those points of intersection of the positive x-axis by circles lying exterior to the ellipse and being doubly tangent to it. All such circles must lie, as we can easily see, symmetrically with respect to the y-axis. Let a, b be the co-ordinates of any point on the ellipse. Then an easy calculation shows that the circle, which is symmetrical with respect to y-axis and tangent to the ellipse at this point, cuts off from the positive x-axis the segment

x = 1 + 3b2.
The greatest possible value of this expression occurs for b = 1 2 and, hence, is equal to 1 27. Since the point on the x-axis which we have denoted by F has for its abscissa the value 3 2 > 1 27, it follows that among the circles cutting the ellipse four times there is certainly none which passes through the point F.

We will now construct a new plane geometry in the following manner. As points in this new geometry, let us take the points of the (xy)-plane. We will define a straight line of our new geometry in the following manner. Every straight line of the (xy)-plane which is either tangent to the fixed ellipse, or does not cut it at all, is taken unchanged as a straight line of the new geometry. However, when any straight line g of the (xy)-plane cuts the ellipse, say in the points P and Q, we will then define the corresponding


pict
Figure 38


straight line of the new geometry as follows. Construct a circle passing through the points P and Q and the fixed point F. From what has just been said, this circle will have no other point in common with the ellipse. We will now take the broken line, consisting of the arc PQ just mentioned and the two parts of the straight line g extending outward indefinitely from the points P and Q, as the required straight line in our new geometry. Let us suppose all of the broken lines constructed which correspond to straight lines of the (xy)-plane. We have then a system of broken lines which, considered as straight lines of our new geometry, evidently satisfy the axioms I, 1–2 and III. By a convention as to the actual arrangement of the points and the straight lines in our new geometry, we have also the axioms II fulfilled.

Moreover, we will call two segments AB and AB congruent in this new geometry, if the broken line extending between A and B has equal length, in the ordinary sense of the word, with the broken line extending from A to B.

Finally, we need a convention concerning the congruence of angles. So long as neither of the vertices of the angles to be compared lies upon the ellipse, we call the two angles congruent to each other, if they are equal in the ordinary sense. In all other cases we make the following convention. Let A,B,C be points which follow one another in this order upon a straight line of our new geometry, and let A,B,C be also points which lie in this order upon another straight line of our new geometry. Let D be a point lying outside of the straight line ABC and D be a point outside of the straight ABC. We will now say that, in our new geometry, the angles between these straight lines fulfill the congruences

ABD ABD and CBD CBD
whenever the natural angles between the corresponding broken lines of the ordinary geometry fulfill the proportion
ABD : CBD = ABD : CBD.
These conventions render the axioms IV, 1–5 and V valid.


pict
Figure 39


In order to see that Desargues’s theorem does not hold for our new geometry, let us consider the following three ordinary straight lines of the (xy)-plane; viz., the axis of x, the axis of y, and the straight line joining the two points of the ellipse (3 5, 2 5) and (3 5,2 5). Since these three ordinary straight lines pass through the origin, we can easily construct two triangles so that their vertices shall lie respectively upon these three straight lines and their homologous sides shall be parallel and all three sides shall lie exterior to the ellipse. As we may see from figure 40, or show by an easy calculation, the broken lines arising from the three straight lines in question do not intersect in a common point. Hence, it follows that Desargues’s theorem certainly does not hold for this particular plane geometry in which we have constructed the two triangles just considered.


pict
Figure 40


This new geometry serves at the same time as an example of a plane geometry in which the axioms I, 1–2, II–III, IV, 1–5, V all hold, but which cannot be considered as a part of a geometry of space.

21. Introduction of an Algebra of Segments based upon Desargues’s Theorem and Independent of the Axioms of Congruence23

In order to see fully the significance of Desargues’s theorem (Theorem 32), let us take as the basis of our consideration a plane geometry where all of the axioms I 1–2, II–III are valid, that is to say, where all of the plane axioms of the first three groups hold, and then introduce into this geometry, in the following manner, a new algebra of segments independent of the axioms of congruence.

Take in the plane two fixed straight lines intersecting in O, and consider only such segments as have O for their origin and their other extremity in one of the fixed lines. We will regard the point O itself as a segment and call it the segment O. We will indicate this fact by writing

OO = 0,  or 0 = OO.

Let E and E be two definite points situated respectively upon the two fixed straight lines through O. Then, define the two segments OE and OE as the segment 1 and write accordingly

OE = OE = 1  or 1 = OE = OE. (5.1)

We will call the straight line EE, for brevity, the unit-line. If, furthermore, A and A are points upon


pict
Figure 41


the straight lines OE and OE, respectively, and, if the straight line AA joining them is parallel to EE, then we will say that the segments OA and OA’ are equal to one another, and write

OA = OA or OA = OA.
In order now to define the sum of the segments a = OA and b = OB, we construct AA parallel to the unit-line EE and draw through A a parallel to OE and through B a parallel to OE. Let these two parallels intersect in A. Finally, draw through A a straight line parallel to the unit-line EE. Let this parallel cut the two fixed lines OE and OE in C and C respectively. Then c = OC = OC is called the sum of the segments a = OA and b = OB. We indicate this by writing
c = a + b,  or a + b = c.
In order to define the product of a segment a = OA by a segment b = OB, we make use of exactly the same construction as employed in Section 14, except that, in place of the sides of a right angle, we make use here of the straight lines OE and OE.


pict
Figure 42


The construction is consequently as follows. Determine upon OE a point A so that AA is parallel to the unit-line EE, and join E with A. Then draw through B a straight line parallel to EA. This parallel will intersect the fixed straight line OE in the point C, and we call c = OC the product of the segment a = OA by the segment b = OB. We indicate this relation by writing

c = ab,  or ab = c.

22. The Commutative and the Associative Law of Addition for Our new Algebra of Segments

In this section, we shall investigate the laws of operation, as enumerated in Section 13, in order to see which of these hold for our new algebra of segments, when we base our considerations upon a plane geometry in which axioms I 1–2, II–III are all fulfilled, and, moreover, in which Desargues’s theorem also holds.

First of all, we shall show that, for the addition of segments as defined in Section 21, the commutative law

a + b = b + a
holds. Let

a = OA = OA b = OB = OB

pict
Figure 43

Hence, AA and BB are, according to our convention, parallel to the unit-line. Construct the points A and B by drawing AA and BB parallel to OA and also AB and BA parallel to OA. We see at once that the line AB is parallel to AA as the commutative law requires. We shall show the validity of this statement by the aid of Desargues’s theorem in the following manner. Denote the point of intersection of AB and AA by F and that of BA and BB by D. Then, in the triangles AAF and BBD, the homologous sides are parallel to each other. By Desargues’s theorem, it follows that the three points O, F, D lie in a straight line. In consequence of this condition, the two triangles OAA and DBA lie in such a way that the lines joining the corresponding vertices pass through the same point F, and since the homologous sides OA and DB, as also OA and DA, are parallel to each other, then, according to the second part of Desargues’s theorem (Theorem 32), the third sides AA and BA are parallel to each other.

To prove the associative law of addition

a + (b + c) = (a + b) + c,
we shall make use of figure 44. In consequence of the commutative law of addition just demonstrated, the above formula states that the straight line AB must be parallel to the unit-line.


pict
Figure 44


The validity of this statement is evident, since the shaded part of figure 44 corresponds exactly with figure 43.

23. The Associative Law of Multiplication and the Two Distributive Laws for the New Algebra of Segments

The associative law of multiplication

a(bc) = (ab)c
has also a place in our new algebra of segments.

Let there be given upon the first of the two fixed straight lines through O the segments

1 = OA,b = OC,c = OA


pict
Figure 45


and upon the second of these straight lines, the segments

a = OG,b = OB.

In order to construct the segments

bc = OB, andbc = OC, ab = OD, (ab)c = OD,

in accordance with Section 21, draw AB parallel to AB, BC parallel to BC, CD parallel to AG, and AD parallel to AD. We see at once that the given law amounts to the same as saying that CD must also be parallel to CD. Denote the point of intersection of the straight lines AD and BC by F and that of the straight lines AD and BC by F. Then the triangles ABF and ABF have their homologous sides parallel to each other, and, according to Desargues’s theorem, the three points O, F, F must lie in a straight line. Because of these conditions, we can apply the second part of Desargues’s theorem to the two triangle CDF and CDF, and hence show that, in fact, CD is parallel to CD.

Finally, upon the basis of Desargues’s theorem, we shall show that the two distributive laws

a(b + c) = ab + ac
and
(a + b)c = ac + bc
hold for our algebra of segments.

In the proof of the first one of these laws, we shall make use of figure 46.24 In this figure, we have

b = OA,c = OC, ab = OB,ab = OA,ac = OC,etc.
In the same figure, BD2 is parallel to CD1 which is parallel to the fixed straight line OA, and BD1 is parallel to CD2, which is parallel to the fixed straight line OA. Moreover, we have AA parallel to CC, and AB parallel to BA, parallel to FD2, parallel to FD1.

Our proposition amounts to asserting that we must necessarily have also

FF parallel to AA and to CC.

We construct the following auxiliary lines:

FJ parallel to the fixed straight line OA,
FJOA.

Let us denote the points of intersection of the straight lines CD1 and CD2, CD1 and FJ, CD2 and FJ by G, H1, H2, respectively. Finally, we obtain the other auxiliary lines indicated in the figure by joining the points already constructed.


pict
Figure 46


In the two triangles ABC and FD2G, the straight lines joining homologous vertices are parallel to each other. According to the second part of Desargues’s theorem, it follows, therefore, that

AC is parallel to FG.

In the two triangles ACF and FGH2, the straight lines joining the homologous vertices are also parallel to each other. From the properties already demonstrated, it follows by virtue of the second part of Desargues’s theorem that we must have

AF parallel to FH2.

Since in the two horizontally shaded triangles OAF and JH2F the homologous sides are parallel, Desargues’s theorem shows that the three straight lines joining the homologous vertices, viz.:

OJ,AH2,FF (5.2)

all intersect in one and the same point, say in P.

In the same way, we have necessarily

AF parallel to FH1
and since, in the two obliquely shaded triangles OAF and JH1F, the homologous sides are parallel, then, in consequence of Desargues’s theorem, the three straight lines joining the homologous vertices, viz.:
OJ,AH1,FF
all intersect likewise in the same point, namely, in point P.

Moreover, in the triangles OAA and JH2H1, the straight lines joining the homologous vertices all pass through this same point P, and, consequently, it follows that we have

H1H2  parallel to AA,
and, therefore,
H1H2  parallel to CC,
Finally, let us consider the figure FH2CCH1FF. Since, in this figure, we have

FH2  parallel to CF,  parallel to CH1, GH2C “ “ FC,  “ “H1F, CC “ “ H1H2,

we recognize here again 43, which we have already made use of in Section 22 to prove the commutative law of addition. The conclusions, analogous to those which we reached there, show that we must have

FF parallel to H1H2
and, consequently, we must have also
FF parallel toAA,
which result concludes our demonstration.

To prove the second formula of the distributive law, we make use of an entirely different figure,—-47. In this figure, we have


pict
Figure 47


1 = OD,a = OA,a = OB,b = OG,c = OD,
ac = OA,ac = OB,BC = OG,  etc.,
and, furthermore, we have

GH parallel to GH, parallel to the fixed line OA,
GHAH, OB,

We have also

AB  parallel to AB BD  “ “ BD DG  “ “ DG HJ  “ “ HJ.

That which we are to prove amounts, then, to demonstrating that

DJ  must be parallel to DJ.

Denote the points in which BD and GD intersect the straight line AH by C and F, respectively, and the points in which BD and GD intersect the straight line AH by C and F, respectively. Finally, draw the auxiliary lines FJ and FJ, indicated in the figure by dotted lines.

In the triangles ABC and ABC, the homologous sides are parallel and, consequently, by Desargues’s theorem the three points O, C, C lie on a straight line. Then, by considering in the same way the triangles CDF and CDF, it follows that the points O, F, F lie upon the same straight line and likewise, from a consideration of the triangles FGH and FGH, we find the points O, H, H to be situated on a straight line. Now, in the triangles FHJ and FHJ, the straight lines joining the homologous vertices all pass through the same point O, and, hence, as a consequence of the second part of Desargues’s theorem, the straight lines FJ and FJ must also be parallel to each other. Finally, a consideration of the triangles DFJ and DFJ shows that the straight lines DJ and DJ are parallel to each other and with this our proof is completed. □

24. Equation of the Straight Line, based upon the New Algebra of Segments

In Sections 2123, we have introduced into the plane geometry an algebra of segments in which the commutative law of addition and that of multiplication, as well as the two distributive laws, hold. This was done upon the assumption that the axioms cited in Section 21, as also the theorem of Desargues, were valid. In this section, we shall show how an analytical representation of the point and straight line in the plane is possible upon the basis of this algebra of segments.

Definition. Take the two given fixed straight lines lying in the plane and intersecting in O as the axis of x and of y, respectively. Let us suppose any point P of the plane determined by the two segments x, y which we obtain upon the x-axis and y-axis, respectively, by drawing through P parallels to these axes. These segments are called the co-ordinates of the point P. Upon the basis of this new algebra of segments and by aid of Desargues’s theorem, we shall deduce the following proposition.

Theorem 34. The co-ordinates x, y of a point on an arbitrary straight line always satisfy an equation in these segments of the form

ax + by + c = 0.
In this equation, the segments a and b stand necessarily to the left of the co-ordinates x and y. The segments a and b are never both zero and c is an arbitrary segment.

Conversely, every equation in these segments and of this form represents always a straight line in the plane geometry under consideration.

Proof. Suppose that the straight line l passes through the origin O. Furthermore, let C be a definite point upon l different from O, and P any arbitrary point of l. Let OA and OB be the co-ordinates of C and x, y be the co-ordinates of P. We will denote the straight line joining the extremities of the segments x, y by g. Finally, through the extremity of the segment 1, laid off on the x-axis, draw a straight line h parallel to AB. This parallel cuts off upon the y-axis the segment e. From the second part of


pict
Figure 48


Desargues’s theorem, it follows that the straight line g is also always parallel to AB. Since g is always parallel to h, it follows that the co-ordinates x, y of the point P must satisfy the equation

ex = g.

Moreover, in 49 let l be any arbitrary straight line in our plane. This straight line will cut off on the x-axis the segment c = OO. Now, in the same figure, draw through O the straight line l parallel to l. Let P be an arbitrary point on the line l. The straight line through P, parallel to the x-axis, intersects the straight line l in P and cuts off upon the y-axis the segment y = OB. Finally, through P and P let parallels to the y-axis cut off on the x-axis the segments x = OA and x = OA.

We shall now undertake to show that the equation

x = x + c
is fulfilled by the segments in question. For this purpose, draw OC parallel to the unit-line and likewise CD parallel to the x-axis and AD parallel to the y-axis.


pict
Figure 49


Then, to prove our proposition amounts to showing that we must have necessarily

AD  parallel to OC.
Let D be the point of intersection of the straight lines CD and AP and draw OC parallel to the y-axis.

Since, in the triangles OCP and OCP, the straight lines joining the homologous vertices are parallel, it follows, by virtue of the second part of Desargues’s theorem, that we must have

CP  parallel to CP.
In a similar way, a consideration of the triangles ACP and ACP shows that we must have
AC  parallel to AC.
Since, in the triangles ACD and CAO, the homologous sides are parallel to each other, it follows that the straight lines AC, CA and DO intersect in a common point. A consideration of the triangles CAD and ACO then shows that AD and CO are parallel to each other. From the two equations already obtained, viz.:

ex = y  and x = x + c, (5.3)

follows at once the equation

ex = y + ec. (5.4)

If we denote, finally, by n the segment which added to the segment 1 gives the segment 0, then, from this last equation, we may easily deduce the following

ex + ny + nec = 0, (5.5)

and this equation is of the form required by theorem 34.

We can now show that the second part of the theorem is equally true; for, every linear equation

ax + by + c = 0 (5.6)

may evidently be brought into the required form

ex + ny + nec = 0 (5.7)

by a left-sided multiplication by a properly chosen segment.

It must be expressly stated, however, that, by our hypothesis, an equation of segments of the form

xa + yb + c = 0, (5.8)

where the segments a, b stand to the right of the co-ordinates x, y does not, in general, represent a straight line. □

In Section 27, we shall make an important application of Theorem 34.

25. The Totality of Segments, regarded as a Complex Number System

We see immediately that, for the new algebra of segments established in Section 21, ??–6 of Section 13 are fulfilled. Moreover, by aid of Desargues’s theorem, we have already shown in Sections 25 and 26 that the laws 7–11 of operation, as given in Section 13, are all valid in this algebra of segments. With the single exception of the commutative law of multiplication, therefore, all of the theorems of connection hold.

Finally, in order to make possible an order of magnitude of these segments, we make the following convention. Let A and B be any two distinct points of the straight line OE. Suppose then that the four points O, E, A, B stand, in conformity with axiom II, 4, in a certain sequence. If this sequence is one of the following six possible ones, viz.:

ABOE,AOBE,AOEB,OABE,OAEB,OEAB,

then we will call the segment a = OA smaller than the segment b = OB and indicate the same by writing

a < b.

On the other hand, if the sequence is one of the six following ones, viz.:

BAOE,BOAE,BOEA,OBAE,OBEA,OEBA,

then we will call the segment a = OA greater than the segment b = OB, and we write accordingly

a > b.

This convention remains in force whenever A or B coincides with O or E, only then the coinciding points are to be regarded as a single point, and, consequently, we have only to consider the order of three points.

Upon the basis of the axioms of group II, we can easily show also that, in our algebra of segments, the laws 13–16 of operation given in Section 13 are fulfilled. Consequently, the totality of all the different segments forms a complex number system for which the laws 1–11, 13–16 of Section 13 hold; that is to say, all of the usual laws of operation except the commutative law of multiplication and the theorem of Archimedes. We will call such a system, briefly, a desarguesian number system.

26. Construction of a Geometry of Space by aid of a Desarguesian Number System

Suppose we have given a desarguesian number system D. Such a system makes possible the construction of a geometry of space in which axioms I, II, III are all fulfilled.

In order to show this, let us consider any system of three numbers (x,y,z) of the desarguesian number system D as a point, and the ratio of four such numbers (u : v : w : r), of which the first three are not 0, as a plane. However, the systems (u : v : w : r) and (au : av : aw : ar), where a is any number of D different from 0, represent the same plane. The existence of the equation

ux + vy + wz + r = 0
expresses the condition that the point (x,y,z) shall lie in the plane (u : v : w : r). Finally, we define a straight line by the aid of a system of two planes (u : v : w : r) and (u : v : w : r), where we impose the condition that it is impossible to find in D two numbers a, a different from zero, such that we have simultaneously the relations
au = au,av = av,aw = aw,
A point (x,y,z) is said to be situated upon this straight line [(u : v : w : r),(u : v : w : r)], if it is common to the two planes (u : v : w : r) and (u : v : w : r). Two straight lines which contain the same points are not regarded as being distinct.

By application of the laws 1–11 of Section 13, which by hypothesis hold for the numbers of D, we obtain without difficulty the result that the geometry of space which we have just constructed satisfies all of the axioms of groups I and III.

In order that the axioms (II) of order may also be valid, we adopt the following conventions. Let

(x1,y1,z1),(x2,y2,z2),(x3,y3,z3)
be any three points of a straight line
[(u : v : w : r),(u : v : w : r)].
Then, the point (x2,y2,z2) is said to lie between the other two, if we have fulfilled at least one of the six following double inequalities:

x1 < x2 < x3, x1 > x2 > x3, (5.9) y1 < y2 < y3, y1 > y2 > y3, (5.10) z1 < z2 < z3, z1 > z2 > z3, (5.11)

If one of the two double inequalities (1) exists, then we can easily conclude that either y1 = y2 = y3 or one of the two double inequalities (2) exists, and, consequently, either z1 = z2 = z3 or one of the double inequalities (3) must exist. In fact, from the equations

uxi + vyi + wzi + r = 0, uxi + vyi + wzi + r = 0, (i = 1,2,3)

we may obtain, by a left-sided multiplication of these equations by numbers suitably chosen from D and then adding the resulting equations, a system of equations of the form

uxi + vyi + r = 0,(i = 1,2,3). (5.12)

In this system, the coefficient v is certainly different from zero, since otherwise the three numbers x1, x2, x3 would be mutually equal.

From

x1 x2 x3,
it follows that
ux1 xu2 xu3,
and, hence, as a consequence of (4), we have
vy1 + r vy2 + r vy3 + r
and, therefore,
vy1 vy2 vy3.
Since v is different from zero, we have
y1 y2 y3.
In each of these double inequalities, we must take either the upper sign throughout, or the middle sign throughout, or the lower sign throughout.

The preceding considerations show, that, in our geometry, the linear axioms II, 1–4 of order are all valid. However, it remains yet to show that, in this geometry, the plane axiom II, 5 is also valid.

For this purpose let a plane (u : v : w : r) and a straight line [(u : v : w : r),(u : v : w : r)] in this plane be given. Let us assume that all the points (x,y,z) of the plane (u : v : w : r), for which we have the expression ux + vy + wz + r greater than or less than zero, lie respectively upon the one side or upon the other side of the given straight line. We have then only to show that this convention is in accordance with the preceding statements. This, however, is easily done. We have thus shown that all of the axioms of groups I, II, III are fulfilled in the geometry of space which we have obtained in the above indicated manner from the desarguesian number system D. Remembering now that the theorem of Desargues is a consequence of the axioms I, II, III, we see that the proposition just stated is exactly the converse of the result reached in Section 25.

27. Significance of Desargues’s Theorem

If, in a plane geometry, axioms I, 1–2, II, III are all fulfilled and, moreover, if the theorem of Desargues holds, then, according to Sections 2125, it is always possible to introduce into this geometry an algebra of segments to which the laws 1–11, 13–16 of Section 13 are applicable. We will now consider the totality of these segments as a complex number system and construct, upon the basis of this system, a geometry of space, in accordance with Section 26, in which all of the axioms I, II, III hold.

In this geometry of space, we shall consider only the points (x,y,0) and those straight lines upon which only such points lie. We have then a plane geometry which must, if we take into account the proposition established in Section 24, coincide exactly with the plane geometry proposed at the beginning. Hence, we are led to the following proposition, which may be regarded as the objective point of the entire discussion of the present chapter.

Theorem 35. If, in a plane geometry, axioms I, 1–2, II, III are all fulfilled, then the existence of Desargues’s theorem is the necessary and sufficient condition that this plane geometry may be regarded as a part of a geometry of space in which all of the axioms I, II, III are fulfilled.

The theorem of Desargues may be characterized for plane geometry as being, so to speak, the result of the elimination of the space axioms.

The results obtained so far put us now in the position to show that every geometry of space in which axioms I, II, III are all fulfilled may be always regarded as a part of a “geometry of any number of dimensions whatever.” By a geometry of an arbitrary number of dimensions is to be understood the totality of all points, straight lines, planes, and other linear elements, for which the corresponding axioms of connection and of order, as well as the axiom of parallels, are all valid.