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At the beginning of this chapter, we shall present briefly certain preliminary ideas concerning complex number systems which will later be of service to us in our discussion.
The real numbers form, in their totality, a system of things having the following properties:
THEOREMS OF CONNECTION (1–12).
If , , are arbitrary numbers, the following laws of operation always hold:
THEOREMS OF ORDER (13–16).
THEOREM OF ARCHIMEDES (17).
A system of things possessing only a portion of the above properties (1–17) is called a complex number system, or simply a number system. A number system is called archimedean, or non-archimedean, according as it does, or does not, satisfy condition (17).
Not every one of the properties (1–17) given above is independent of the others. The problem arises to investigate the logical dependence of these properties. Because of their great importance in geometry, we shall, in Sections 29, 30, pp. §–§, answer two definite questions of this character. We will here merely call attention to the fact that, in any case, the last of these conditions (17) is not a consequence of the remaining properties, since, for example, the complex number system , considered in Section 12, possesses all of the properties (1–16), but does not fulfil the law stated in (17).
In this and the following chapter, we shall take as the basis of our discussion all of the plane axioms with the exception of the axiom of Archimedes; that is to say, the axioms I, 1–2 and II–IV. In the present chapter, we propose, by aid of these axioms, to establish Euclid’s theory of proportion; that is, we shall establish it for the plane and that independently of the axiom of Archimedes.
Figure 16
For this purpose, we shall first demonstrate a proposition which is a special case of the well known theorem of Pascal usually considered in the theory of conic sections, and which we shall hereafter, for the sake of brevity, refer to simply as Pascal’s theorem. This theorem may be stated as follows:
Theorem 21 (Pascal’s theorem.). Given the two sets of points , , and , , so situated respectively upon two intersecting straight lines that none of them fall at the intersection of these lines. If is parallel to and is also parallel to , then is parallel to .17
In order to demonstrate this theorem, we shall first introduce the following notation. In a right triangle, the base is uniquely determined by the hypotenuse and the base angle included by and . We will express this fact briefly by writing
Figure 17
Hence, the symbol always represents a definite segment, providing is any given segment whatever and is any given acute angle.
Furthermore, if is any arbitrary segment and , are any two acute angles whatever, then the two segments and are always congruent; that is, we have
and, consequently, the symbols and are interchangeable.
Figure 18
In order to prove this statement, we take the segment , and with as a vertex lay off upon the one side of this segment the angle and upon the other the angle . Then, from the point , let fall upon the opposite sides of the and the perpendiculars and , respectively. Finally, join with and let fall from the perpendicular upon .
Since the two angles and are right angles, the four points , , , are situated upon a circle. Consequently, the angles and , being inscribed in the same segment of the circle, are congruent. But the angles and , taken together, make a right angle, and the same is true of the two angles and . Hence, the two angles and are also congruent; that is to say,
and, therefore,From these considerations, we have immediately the following congruences of segments:
From these, the validity of the congruence in question follows.Returning now to the figure in connection with Pascal’s theorem, denote the intersection of the two given straight lines by and the segments , , , , , , , , , , , by , , , , , , , , , , , , respectively.
Figure 19
Let fall from the point
a perpendicular upon each of the segments
,
,
. The perpendicular
to will form with the
straight lines and
acute angles, which
we shall denote by and
, respectively. Likewise,
the perpendiculars to
and form with
these same lines and
acute angles, which
we shall denote by ,
and
,
,
respectively. If we now express, as indicated above, each of these perpendiculars in
terms of the hypotenuse and base angle, we have the three following congruences of
segments:
Multiplying both members of congruence (3) by the symbol , and remembering that, as we have already seen, the symbols in question are commutative, we have
In this congruence, we may replace in the first member by its value given in (2) and in the second member by its value given in (4), thus obtaining as a result or Here again in this congruence we can, by aid of (1), replace by , and, by aid of (5), we may replace in the second member by . We then have or Because of the significance of our symbols, we can conclude at once from this congruence that and, consequently, thatIf now we consider the perpendicular let fall from upon and draw perpendiculars to this same line from the points and , then congruence (6) shows that the feet of the last two perpendiculars must coincide; that is to say, the straight line makes a right angle with the perpendicular to and, consequently, is parallel to . This establishes the truth of Pascal’s theorem.
Having given any straight line whatever, together with an arbitrary angle and a point lying outside of the given line, we can, by constructing the given angle and drawing a parallel line, find a straight line passing through the given point and cutting the given straight line at the given angle. By means of this construction, we can demonstrate Pascal’s theorem in the following very simple manner, for which, however, I am indebted to another source.
Figure 20
Through the point ,
draw a straight line cutting
in the point and making
with it the angle ,
so that the congruence
(1)
is fulfilled. Now, according to a well known property of circles,
is an
inscribed quadrilateral, and, consequently, by aid of the theorem concerning the
congruence of angles inscribed in the same segment of a circle, we have the
congruence
(2) .
Since, by hypothesis,
and
are parallel, we have
(3) ,
and from (1) and
(3) we obtain
the congruence
Pascal’s theorem, which was demonstrated in the last section, puts us in a position to introduce into geometry a method of calculating with segments, in which all of the rules for calculating with real numbers remain valid without any modification.
Instead of the word “congruent” and the sign , we make use, in the algebra of segments, of the word “equal” and the sign .
Figure 21
If are three points of a straight line and if lies between and , then we say that is the sum of the two segments and . We indicate this by writing
The segments and are said to be smaller than c, which fact we indicate by writing On the other hand, is said to be larger than and , and we indicate this by writingFrom the linear axioms of congruence (axioms IV, 1–3), we easily see that, for the above definition of addition of segments, the associative law
as well as the commutative law is valid.
Figure 22
In order to define geometrically the product of two segments and , we shall make use of the following construction. Select any convenient segment, which, having been selected, shall remain constant throughout the discussion, and denote the same by . Upon the one side of a right angle, lay off from the vertex the segment and also the segment . Then, from lay off upon the other side of the right angle the segment . Join the extremities of the segments and by a straight line, and from the extremity of draw a line parallel to this straight line. This parallel will cut off from the other side of the right angle a segment . We call this segment the product of the segments and , and indicate this relation by writing
Figure 23
We shall now demonstrate that, for this definition of the multiplication of segments, the commutative law
holds. For this purpose, we construct in the above manner the product . Furthermore, lay off from upon the first side (I) of the right angle the segment and upon the other side (II) the segment . Connect by a straight line the extremity of the segment with the extremity of , situated on II, and draw through the endpoint of , on I, a line parallel to this straight line. This parallel will determine, by its intersection with the side II, the segment . But, because the two dotted lines are, by Pascal’s theorem, parallel, the segment just found coincides with the segment previously constructed, and our proposition is established. In order to show that the associative law holds for the multiplication of segments, we construct first of all the segment , then , after that the segment , and finally . By virtue of Pascal’s theorem, the extremities of the segments and coincide, as may be clearly seen from figure 24.
Figure 24
If now we apply the commutative law which we have just demonstrated, we obtain the above formula, which expresses the associative law for the multiplication of two segments.
Figure 25
Finally, the distributive law
also holds for our algebra of segments. In order to demonstrate this, we construct the segments, , , and , and draw through the extremity of the segment (Fig. 25) a straight line parallel to the other side of the right angle. From the congruence of the two right-angled triangles which are shaded in the figure and the application of the theorem relating to the equality of the opposite sides of a parallelogram, the desired result follows. If and are any two arbitrary segments, there is always a segment to be found such that . This segment is denoted by and is called the quotient of by .By aid of the preceding algebra of segments, we can establish Euclid’s theory of proportion in a manner free from objections and without making use of the axiom of Archimedes.
If are any four segments whatever, the proportion
expresses nothing else than the validity of equationProof. We shall first consider the special case where the angle included between and and the one included between and are right angles.
Figure 26
This parallel determines upon the other side of the right angle a segment . Then, according to our definition of the product of two segments, we have
from which we obtain that is to say,
Figure 27
Let us now return to the general case. In each of the two similar triangles, find the point of intersection of the bisectors of the three angles. Denote these points by and . From these points let fall upon the sides of the triangles the perpendiculars and , respectively. Denote the segments thus determined upon the sides of the triangles by
and respectively. The special case of our proposition, demonstrated above, gives us then the following proportions:By aid of the distributive law, we obtain from these proportions the following:
Consequently, by virtue of the commutative law of multiplication, we have □From the theorem just demonstrated, we can easily deduce the fundamental theorem in the theory of proportion. This theorem may be stated as follows:
Theorem 23. If two parallel lines cut from the sides of an arbitrary angle the segments and respectively, then we have always the proportion
Conversely, if the four segments fulfill this proportion and if and are laid off upon the two sides respectively of an arbitrary angle, then the straight lines joining the extremities of and and of and are parallel to each other.
To the system of segments already discussed, let us now add a second system. We will distinguish the segments of the new system from those of the former one by means of a special sign, and will call them “negative” segments in contradistinction to the “positive” segments already considered. If we introduce also the segment , which is determined by a single point, and make other appropriate conventions, then all of the rules deduced in Section 13 for calculating with real numbers will hold equally well here for calculating with segments. We call special attention to the following particular propositions:
In a plane , we now take two straight lines cutting each other in at right angles as the fixed axes of rectangular co-ordinates, and lay off from upon these two straight lines the arbitrary segments and . We lay off these segments upon the one side or upon the other side of , according as they are positive or negative. At the extremities of and , erect perpendiculars and determine the point of their intersection. The segments and are called the co-ordinates of . Every point of the plane is uniquely determined by its co-ordinates , , which may be positive, negative, or zero.
Let be a straight line in the plane , such that it shall pass through and also through a point having the co-ordinates . If are the co-ordinates
Figure 28
of any point on , it follows at once from Theorem 22 that
or is the equation of the straight line . If is a straight line parallel to and cutting off from the -axis the segment , then we may obtain the equation of the straight line by replacing, in the equation for , the segment by the segment . The desired equation will then be of the formFrom these considerations, we may easily conclude, independently of the axiom of Archimedes, that every straight line of a plane is represented by an equation which is linear in the co-ordinates , , and, conversely, every such linear equation represents a straight line when the co-ordinates are segments appertaining to the geometry in question. The corresponding results for the geometry of space may be easily deduced.
The remaining parts of geometry may now be developed by the usual methods of analytic geometry.
So far in this chapter, we have made absolutely no use of the axiom of Archimedes. If now we assume the validity of this axiom, we can arrange a definite correspondence between the points on any straight line in space and the real numbers. This may be accomplished in the following manner.
We first select on a straight line any two points, and assign to these points the numbers and . Then, bisect the segment thus determined and denote the middle point by the number . In the same way, we denote the middle of by , etc. After applying this process times, we obtain a point which corresponds to . Now, lay off times in both directions from the point the segment . We obtain in this manner a point corresponding to the numbers and . From the axiom of Archimedes, we now easily see that, upon the basis of this association, to each arbitrary point of a straight line there corresponds a single, definite, real number, and, indeed, such that this correspondence possesses the following property: If , , are any three points on a straight line and , , are the corresponding real numbers, and, if lies between and , then one of the inequalities,
is always fulfilled.From the development given in Section 9, p. §, it is evident, that to every number belonging to the field of algebraic numbers , there must exist a corresponding point upon the straight line. Whether to every real number there corresponds a point cannot in general be established, but depends upon the geometry to which we have reference.
However, it is always possible to generalize the original system of points, straight lines, and planes by the addition of “ideal” or “irrational” elements, so that, upon any straight line of the corresponding geometry, a point corresponds without exception to every system of three real numbers. By the adoption of suitable conventions, it may also be seen that, in this generalized geometry, all of the axioms I–V are valid. This geometry, generalized by the addition of irrational elements, is nothing else than the ordinary analytic geometry of space.
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