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An essay on the foundations of geometry

Introductory material

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INTRODUCTION.

OUR PROBLEM DEFINED BY ITS RELATIONS TO LOGIC, PSYCHOLOGY AND MATHEMATICS.

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1.The problem first received a modern form through Kant, who connected the à priori with the subjective1

2.A mental state is subjective, for Psychology, when its immediate cause does not lie in the outer world2

3.A piece of knowledge is à priori, for Epistemology, when without it knowledge would be impossible2

4.The subjective and the à priori belong respectively to Psychology and to Epistemology. The latter alone will be investigated in this essay3

5.My test of the à priori will be purely logical: what knowledge is necessary for experience?3

6.But since the necessary is hypothetical, we must include, in the à priori, the ground of necessity4

7.This may be the essential postulate of our science, or the element, in the subject-matter, which is necessary to experience;4

8.Which, however, are both at bottom the same ground5

9.Forecast of the work5

CHAPTER I.

A SHORT HISTORY OF METAGEOMETRY.

10.Metageometry began by rejecting the axiom of parallels7

11.Its history may be divided into three periods: the synthetic, the metrical and the projective7

12.The first period was inaugurated by Gauss,10

13.Whose suggestions were developed independently by Lobatchewsky10

14.And Bolyai11

15.The purpose of all three was to show that the axiom of parallels could not be deduced from the others, since its denial did not lead to contradictions12

16.The second period had a more philosophical aim, and was inspired chiefly by Gauss and Herbart13

17.The first work of this period, that of Riemann, invented two new conceptions:14

18.The first, that of a manifold, is a class-conception, containing space as a species,14

19.And defined as such that its determinations form a collection of magnitudes15

20.The second, the measure of curvature of a manifold, grew out of curvature in curves and surfaces16

21.By means of Gauss's analytical formula for the curvature of surfaces,19

22.Which enables us to define a constant measure of curvature of a three-dimensional space without reference to a fourth dimension20

23.The main result of Riemann's mathematical work was to show that, if magnitudes are independent of place, the measure of curvature of space must be constant21

24.Helmholtz, who was more of a philosopher than a mathematician,22

25.Gave a new but incorrect formulation of the essential axioms,23

26.And deduced the quadratic formula for the infinitesimal arc, which Riemann had assumed24

27.Beltrami gave Lobatchewsky's planimetry a Euclidean interpretation,25

28.Which is analogous to Cayley's theory of distance;26

29.And dealt with n-dimensional spaces of constant negative curvature27

30.The third period abandons the metrical methods of the second, and extrudes the notion of spatial quantity27

31.Cayley reduced metrical properties to projective properties, relative to a certain conic or quadric, the Absolute;28

32.And Klein showed that the Euclidean or non-Euclidean systems result, according to the nature of the Absolute;29

33.Hence Euclidean space appeared to give rise to all the kinds of Geometry, and the question, which is true, appeared reduced to one of convention30

34.But this view is due to a confusion as to the nature of the coordinates employed30

35.Projective coordinates have been regarded as dependent on distance, and thus really metrical31

36.But this is not the case, since anharmonic ratio can be projectively defined32

37.Projective coordinates, being purely descriptive, can give no information as to metrical properties, and the reduction of metrical to projective properties is purely technical33

38.The true connection of Cayley's measure of distance with non-Euclidean Geometry is that suggested by Beltrami's Saggio, and worked out by Sir R. Ball,36

39.Which provides a Euclidean equivalent for every non-Euclidean proposition, and so removes the possibility of contradictions in Metageometry38

40.Klein's elliptic Geometry has not been proved to have a corresponding variety of space39

41.The geometrical use of imaginaries, of which Cayley demanded a philosophical discussion,41

42.Has a merely technical validity,42

43.And is capable of giving geometrical results only when it begins and ends with real points and figures45

44.We have now seen that projective Geometry is logically prior to metrical Geometry, but cannot supersede it46

45.Sophus Lie has applied projective methods to Helmholtz's formulation of the axioms, and has shown the axiom of Monodromy to be superfluous46

46.Metageometry has gradually grown independent of philosophy, but has grown continually more interesting to philosophy50

47.Metrical Geometry has three indispensable axioms,50

48.Which we shall find to be not results, but conditions, of measurement,51

49.And which are nearly equivalent to the three axioms of projective Geometry52

50.Both sets of axioms are necessitated, not by facts, but by logic52

CHAPTER II.

CRITICAL ACCOUNT OF SOME PREVIOUS PHILOSOPHICAL THEORIES OF GEOMETRY.

51.A criticism of representative modern theories need not begin before Kant54

52.Kant's doctrine must be taken, in an argument about Geometry, on its purely logical side55

53.Kant contends that since Geometry is apodeictic, space must be à priori and subjective, while since space is à priori and subjective, Geometry must be apodeictic55

54.Metageometry has upset the first line of argument, not the second56

55.The second may be attacked by criticizing either the distinction of synthetic and analytic judgments, or the first two arguments of the metaphysical deduction of space57

56.Modern Logic regards every judgment as both synthetic and analytic,57

57.But leaves the à priori, as that which is presupposed in the possibility of experience59

58.Kant's first two arguments as to space suffice to prove some form of externality, but not necessarily Euclidean space, a necessary condition of experience60

59.Among the successors of Kant, Herbart alone advanced the theory of Geometry, by influencing Riemann62

60.Riemann regarded space as a particular kind of manifold, i.e. wholly quantitatively63

61.He therefore unduly neglected the qualitative adjectives of space64

62.His philosophy rests on a vicious disjunction65

63.His definition of a manifold is obscure,66

64.And his definition of measurement applies only to space67

65.Though mathematically invaluable, his view of space as a manifold is philosophically misleading69

66.Helmholtz attacked Kant both on the mathematical and on the psychological side;70

67.But his criterion of apriority is changeable and often invalid;71

68.His proof that non-Euclidean spaces are imaginable is inconclusive;72

69.And his assertion of the dependence of measurement on rigid bodies, which may be taken in three senses,74

70.Is wholly false if it means that the axiom of Congruence actually asserts the existence of rigid bodies,75

71.Is untrue if it means that the necessary reference of geometrical propositions to matter renders pure Geometry empirical,76

72.And is inadequate to his conclusion if it means, what is true, that actual measurement involves approximately rigid bodies78

73.Geometry deals with an abstract matter, whose physical properties are disregarded; and Physics must presuppose Geometry80

74.Erdmann accepted the conclusions of Riemann and Helmholtz,81

75.And regarded the axioms as necessarily successive steps in classifying space as a species of manifold82

76.His deduction involves four fallacious assumptions, namely:82

77.That conceptions must be abstracted from a series of instances;83

78.That all definition is classification;83

79.That conceptions of magnitude can be applied to space as a whole;84

80.And that if conceptions of magnitude could be so applied, all the adjectives of space would result from their application86

81.Erdmann regards Geometry alone as incapable of deciding on the truth of the axiom of Congruence,86

82.Which he affirms to be empirically proved by Mechanics.88

83.The variety and inadequacy of Erdmann's tests of apriority89

84.Invalidate his final conclusions on the theory of Geometry90

85.Lotze has discussed two questions in the theory of Geometry:93

86.(1) He regards the possibility of non-Euclidean spaces as suggested by the subjectivity of space,93

87.And rejects it owing to a mathematical misunderstanding,96

88.Having missed the most important sense of their possibility,96

89.Which is that they fulfil the logical conditions to which any form of externality must conform97

90.(2) He attacks the mathematical procedure of Metageometry98

91.The attack begins with a question-begging definition of parallels99

92.Lotze maintains that all apparent departures from Euclid could be physically explained, a view which really makes Euclid empirical99

93.His criticism of Helmholtz's analogies rests wholly on mathematical mistakes101

94.His proof that space must have three dimensions rests on neglect of different orders of infinity104

95.He attacks non-Euclidean spaces on the mistaken ground that they are not homogeneous107

96.Lotze's objections fall under four heads108

97.Two other semi-philosophical objections may be urged,109

98.One of which, the absence of similarity, has been made the basis of attack by Delbœuf,110

99.But does not form a valid ground of objection111

100.Recent French speculation on the foundations of Geometry has suggested few new views112

101.All homogeneous spaces are à priori possible, and the decision between them is empirical114

CHAPTER III.

Section A. the axioms of projective geometry.

102.Projective Geometry does not deal with magnitude, and applies to all spaces alike117

103.It will be found wholly à priori117

104.Its axioms have not yet been formulated philosophically118

105.Coordinates, in projective Geometry, are not spatial magnitudes, but convenient names for points118

106.The possibility of distinguishing various points is an axiom119

107.The qualitative relations between points, dealt with by projective Geometry, are presupposed by the quantitative treatment119

108.The only qualitative relation between two points is the straight line, and all straight lines are qualitatively similar120

109.Hence follows, by extension, the principle of projective transformation121

110.By which figures qualitatively indistinguishable from a given figure are obtained122

111.Anharmonic ratio may and must be descriptively defined122

112.The quadrilateral construction is essential to the projective definition of points,123

113.And can be projectively defined,124

114.By the general principle of projective transformation126

115.The principle of duality is the mathematical form of a philosophical circle,127

116.Which is an inevitable consequence of the relativity of space, and makes any definition of the point contradictory128

117.We define the point as that which is spatial, but contains no space, whence other definitions follow128

118.What is meant by qualitative equivalence in Geometry?129

119.Two pairs of points on one straight line, or two pairs of straight lines through one point, are qualitatively equivalent129

120.This explains why four collinear points are needed, to give an intrinsic relation by which the fourth can be descriptively defined when the first three are given130

121.Any two projectively related figures are qualitatively equivalent, i.e. differ in no non-quantitative conceptual property131

122.Three axioms are used by projective Geometry,132

123.And are required for qualitative spatial comparison,132

124.Which involves the homogeneity, relativity and passivity of space133

125.The conception of a form of externality,134

126.Being a creature of the intellect, can be dealt with by pure mathematics134

127.The resulting doctrine of extension will be, for the moment, hypothetical135

128.But is rendered assertorical by the necessity, for experience, of some form of externality136

129.Any such form must be relational136

130.And homogeneous137

131.And the relations constituting it must appear infinitely divisible137

132.It must have a finite integral number of dimensions,139

133.Owing to its passivity and homogeneity140

134.And to the systematic unity of the world140

135.A one-dimensional form alone would not suffice for experience141

136.Since its elements would be immovably fixed in a series142

137.Two positions have a relation independent of other positions,143

138.Since positions are wholly defined by mutually independent relations143

139.Hence projective Geometry is wholly à priori,146

140.Though metrical Geometry contains an empirical element146

Section B. the axioms of metrical geometry.

141.Metrical Geometry is distinct from projective, but has the same fundamental postulate147

142.It introduces the new idea of motion, and has three à priori axioms148

I. The Axiom of Free Mobility.

143.Measurement requires a criterion of spatial equality149

144.Which is given by superposition, and involves the axiom of Free Mobility150

145.The denial of this axiom involves an action of empty space on things151

146.There is a mathematically possible alternative to the axiom,152

147.Which, however, is logically and philosophically untenable153

148.Though Free Mobility is à priori, actual measurement is empirical154

149.Some objections remain to be answered, concerning—154

150.(1) The comparison of volumes and of Kant's symmetrical objects154

151.(2) The measurement of time, where congruence is impossible156

152.(3) The immediate perception of spatial magnitude; and157

153.(4) The Geometry of non-congruent surfaces158

154.Free Mobility includes Helmholtz's Monodromy159

155.Free Mobility involves the relativity of space159

156.From which, reciprocally, it can be deduced160

157.Our axiom is therefore à priori in a double sense160

II. The Axiom of Dimensions.

158.Space must have a finite integral number of dimensions161

159.But the restriction to three is empirical162

160.The general axiom follows from the relativity of position162

161.The limitation to three dimensions, unlike most empirical knowledge, is accurate and certain163

III. The Axiom of Distance.

162.The axiom of distance corresponds, here, to that of the straight line in projective Geometry164

163.The possibility of spatial measurement involves a magnitude uniquely determined by two points,164

164.Since two points must have some relation, and the passivity of space proves this to be independent of external reference165

165.There can be only one such relation166

166.This must be measured by a curve joining the two points,166

167.And the curve must be uniquely determined by the two points167

168.Spherical Geometry contains an exception to this axiom,168

169.Which, however, is not quite equivalent to Euclid's168

170.The exception is due to the fact that two points, in spherical space, may have an external relation unaltered by motion,169

171.Which, however, being a relation of linear magnitude, presupposes the possibility of linear magnitude170

172.A relation between two points must be a line joining them170

173.Conversely, the existence of a unique line between two points can be deduced from the nature of a form of externality,171

174.And necessarily leads to distance, when quantity is applied to it172

175.Hence the axiom of distance, also, is à priori in a double sense172

176.No metrical coordinate system can be set up without the straight line174

177.No axioms besides the above three are necessary to metrical Geometry175

178.But these three are necessary to the direct measurement of any continuum176

179.Two philosophical questions remain for a final chapter177

CHAPTER IV.

PHILOSOPHICAL CONSEQUENCES.

180.What is the relation to experience of a form of externality in general?178

181.This form is the class-conception, containing every possible intuition of externality; and some such intuition is necessary to experience178

182.What relation does this view bear to Kant's?179

183.It is less psychological, since it does not discuss whether space is given in sensation,180

184.And maintains that not only space, but any form of externality which renders experience possible, must be given in sense-perception181

185.Externality should mean, not externality to the Self, but the mutual externality of presented things181

186.Would this be unknowable without a given form of externality?182

187.Bradley has proved that space and time preclude the existence of mere particulars,182

188.And that knowledge requires the This to be neither simple nor self-subsistent183

189.To prove that experience requires a form of externality, I assume that all knowledge requires the recognition of identity in difference184

190.Such recognition involves time184

191.And some other form giving simultaneous diversity185

192.The above argument has not deduced sense-perception from the categories, but has shown the former, unless it contains a certain element, to be unintelligible to the latter186

193.How to account for the realization of this element, is a question for metaphysics187

194.What are we to do with the contradictions in space?188

195.Three contradictions will be discussed in what follows188

196.(1) The antinomy of the Point proves the relativity of space,189

197.And shows that Geometry must have some reference to matter,190

198.By which means it is made to refer to spatial order, not to empty space191

199.The causal properties of matter are irrelevant to Geometry, which must regard it as composed of unextended atoms, by which points are replaced191

200.(2) The circle in defining straight lines and planes is overcome by the same reference to matter192

201.(3) The antinomy that space is relational and yet more than relational,193

202.Seems to depend on the confusion of empty space with spatial order193

203.Kant regarded empty space as the subject-matter of Geometry,194

204.But the arguments of the Aesthetic are inconclusive on this point,195

205.And are upset by the mathematical antinomies, which prove that spatial order should be the subject-matter of Geometry196

206.The apparent thinghood of space is a psychological illusion, due to the fact that spatial relations are immediately given196

207.The apparent divisibility of spatial relations is either an illusion, arising out of empty space, or the expression of the possibility of quantitatively different spatial relations197

208.Externality is not a relation, but an aspect of relations. Spatial order, owing to its reference to matter, is a real relation198

209.Conclusion199

Notes in this chapter

Note 1 · Geometry, throughout the 17th and 18th centuries, remained, in the war against empiricism, an impregnable fortress of the idealists. Those wNote 2 · One of the great difficulties, throughout this controversy, is the extremely variable use to which these words, as well as the word empiricaNote 3 · Let us now consider the epistemological question, as to the sort of knowledge which can be called à priori. Here we have nothing to do—in thNote 4 · Now what is the connection between the subjective and the à priori? It is a connection, obviously—if it exists at all—from the outside, i.e.Note 5 · I shall, therefore, throughout the present Essay, use the word à priori without any psychological implication. My test of apriority will be Note 6 · As I have ventured to use the word à priori in a slightly unconventional sense, I will give a few elucidatory remarks of a general nature.Note 7 · There are two grounds, I think, on which necessity may be sought within any science. These may be (very roughly) distinguished as the groundNote 8 · These two grounds of necessity, in ultimate analysis, fall together. The methods of investigation in the two cases differ widely, but the reNote 9 · The course of my argument, therefore, will be as follows: In the first chapter, as a preliminary to the logical analysis of Geometry, I shalNote 10 · When a long established system is attacked, it usually happens that the attack begins only at a single point, where the weakness of the estaNote 11 · Thus Legendre's attempt broke down; but mere failure could prove nothing. A bolder method, suggested by Gauss, was carried out by LobatchewsNote 12 · The originator of the whole system, Gauss, does not appear, as regards strictly non-Euclidean Geometry, in any of his hitherto published papNote 13 · Lobatchewsky, a professor in the University of Kasan, first published his results, in their native Russian, in the proceedings of that learnNote 14 · Very similar is the system of Johann Bolyai, so similar, indeed, as to make the independence of the two works, though a well-authenticated fNote 15 · It is important to remember that, throughout the period we have just reviewed, the purpose of hyperbolic Geometry is indirect: not the truthNote 16 · The work of Lobatchewsky and Bolyai remained, for nearly a quarter of a century, without issue—indeed, the investigations of Riemann and HelNote 17 · Riemann's epoch-making work, "Ueber die Hypothesen, welche der Geometrie zu Grande liegen[16]", was written, and read to a small circle, in Note 18 · (1) Conception of a manifold[17]. The general purpose of Riemann's dissertation is, to exhibit the axioms as successive steps in the classifNote 19 · Conceptions of magnitude, according to Riemann, are possible there only, where we have a general conception, capable of various determinatioNote 20 · (2) Measure of curvature. This conception is due to Gauss, but was applied by him only to surfaces; the novelty in Riemann's dissertation waNote 21 · So far, all has been plain sailing—we have been dealing with purely geometrical ideas in a purely geometrical manner—but we have not, as yetNote 22 · Such a meaning is supplied by Riemann's dissertation, to which, after this long digression, we can now return. We may define a continuous maNote 23 · The mathematical result of Riemann's dissertation may be summed up as follows. Assuming it possible to apply magnitude to space, i.e. to detNote 24 · Helmholtz, the historically nearest follower of Riemann, was guided by a similar empirical philosophy, and arrived independently at a very sNote 25 · In the first of these, which is chiefly philosophical, Helmholtz gives hints of his then uncompleted mathematical work, but in the main contNote 26 · The second article, which is mainly mathematical, supplies the promised proof of the arc-formula, which is Helmholtz's most important contriNote 27 · Helmholtz's other writings on Geometry are almost wholly philosophical, and will be discussed at length in Chapter II. For the present, we mNote 28 · In Beltrami's Saggio, straight lines are, of course, replaced by geodesics; his coordinates are obtained through a point-by-point correspondNote 29 · The value of Beltrami's Saggio, in his own eyes, lies in the intelligible Euclidean sense which it gives to Lobatchewsky's planimetry: the cNote 30 · The third period differs radically, alike in its methods and aims, and in the underlying philosophical ideas, from the period which it replaNote 31 · We shall find, throughout this period, that almost every important proposition, though misleading in its obvious interpretation, has neverthNote 32 · The connection of Cayley's Theory of Distance with Metageometry was first pointed out by Klein[41]. Klein showed in detail that, if the AbsoNote 33 · Since these systems are all obtained from a Euclidean plane, by a mere alteration in the definition of distance, Cayley and Klein tend to reNote 34 · The view in question has arisen, it would seem, from a natural confusion as to the nature of the coordinates employed. Those who hold the viNote 35 · But what are projective coordinates, and how are they introduced? This question was not touched upon in Cayley's Memoir, and it seemed, therNote 36 · This objection is valid, we must admit, so long as anharmonic ratio is defined in the ordinary metrical manner. It would be valid, for exampNote 37 · With this coordinate system, then, to define distance as a certain function of the coordinates is not to be guilty of a vicious circle. But Note 38 · It remains to discuss the manner in which non-Euclidean Geometries result from the projective definition of distance, as also the true interNote 39 · On the whole, then, a modification of Sir R. Ball's view, which is practically a generalized statement of Beltrami's method, seems the most Note 40 · We have still to discuss Klein's third kind of non-Euclidean Geometry, which he calls elliptic. The difference between this and spherical GeNote 41 · In connection with the reduction of metrical to projective Geometry, we have one more topic for discussion. This is the geometrical use of iNote 42 · This right it is now my purpose to demonstrate. But for fear non-mathematicians should miss the point of Cayley's remark (which has sometimeNote 43 · The fact that the fiction is convenient, however, may be thought to indicate that it is more than a fiction. But this presumption, I think, Note 44 · We have now, I think, discussed most of the questions concerning the scope and validity of the projective method. We have seen that it is inNote 45 · It only remains to say a few words about Sophus Lie. As a mathematician, as the inventor of a new and immensely powerful method of analysis,Note 46 · I have now come to the end of my history of Metageometry. It has not been my aim to give an exhaustive account of even the important works oNote 47 · Now in discussing the systems of Metageometry, we have found two kinds, radically distinct and subject to different axioms. The historicallyNote 48 · But metrical Geometry, though it is historically prior, is logically subsequent to projective Geometry. For projective Geometry deals directNote 49 · This expectation will not be disappointed. The above three axioms, as we shall see hereafter, are one and all philosophically equivalent to Note 50 · That some logical necessity is involved in these axioms might, I think, be inferred as probable, from their historical development alone. FoNote 51 · We have now traced the mathematical development of the theory of geometrical axioms, from the first revolt against Euclid to the present dayNote 52 · It is not my purpose, in this chapter, to add to the voluminous literature of Kantian criticism, but only to discuss the bearing of MetageomNote 53 · Now on this question, as on almost all questions in the Aesthetic or the Analytic, Kant's argument is twofold. On the one hand, he says, GeoNote 54 · Now it must be admitted, I think, that Metageometry has destroyed the legitimacy of the argument from Geometry to space; we can no longer afNote 55 · For such an attack, two roads lie open: either we may disprove the first two arguments of the Aesthetic, or we may criticize, from the standNote 56 · (1) Kant's logical position. The doctrine of synthetic and analytic judgments—at any rate if this is taken as the corner-stone of EpistemoloNote 57 · We may retain, however, a distinction roughly corresponding to the Kantian à priori and à posteriori, though less rigid, and more liable to Note 58 · (2) Kant's arguments for the apriority of space. Having now discussed the logical canon to be used as regards the à priori, we may proceed tNote 59 · In the philosophers who followed Kant, Metaphysics, for the most part, so predominated over Epistemology, that little was added to the theorNote 60 · The aim of Riemann's dissertation, as we saw in Chapter I., was to define space as a species of manifold, i.e. as a particular kind of colleNote 61 · Indeed we can see, from a purely logical consideration of the judgment of quantity, that Riemann's manner of approaching the problem can nevNote 62 · We must entirely dissent, therefore, from the disjunction which underlies Riemann's philosophy of space. Either the axioms must be consequenNote 63 · In the first place there is, if I am not mistaken, considerable obscurity in the definition of a manifold, of which an almost verbal renderiNote 64 · But if "measurement consists in a superposition of the magnitudes compared" (p. 256), does it not follow immediately that measurement is logNote 65 · I do not wish to deny, however, the great value of the conception of space as a manifold. On the contrary, this conception seems to have becNote 66 · Helmholtz, like Riemann, was important both in the mathematics and in the philosophy of Geometry. From the mathematical point of view, his wNote 67 · Helmholtz's criterion of apriority is difficult to discover, as he never, to my knowledge, gives a precise statement of it. From his discussNote 68 · One of the few cases, in which Helmholtz has attempted such an accompaniment, occurs in connection with our second point, the imaginability Note 69 · We come now to the third and most important question, the relation of Geometry to Mechanics. There are three senses in which Helmholtz's appNote 70 · (1) Congruence may be taken to mean—as Helmholtz would certainly seem to desire—that we find actual bodies, in our mechanical experience, toNote 71 · (2) The above argument seems to me to answer satisfactorily Helmholtz's contention in the precise form which he first gave it. The axiom of Note 72 · (3) This argument leads us to Land's distinction of physical and geometrical rigidity. The distinction may be expressed—and I think it is beNote 73 · The utility, for Dynamics, of our abstract geometrical matter, is sufficiently evident. For having, by its means, a power of determining theNote 74 · In connection with Riemann and Helmholtz, it is natural to consider Erdmann's philosophical work on their theories[92]. This is certainly thNote 75 · After a general introduction, and a short history of the development of Metageometry, Erdmann proceeds, in his second chapter, to discuss whNote 76 · Before considering the subsequent method of definition, let us reflect on the theories involved in the above account of the conception of spNote 77 · As regards the first point, it is to be observed that people certainly had some conception of space before Riemann invented the notion of a Note 78 · The second point, the view that all definition is classification, is closely allied to the first, and the two together plunge us into the deNote 79 · As regards the third point, the impossibility of applying conceptions of magnitude to space as a whole, a longer argument will be necessary,Note 80 · This suggests the fourth and last of the above points, that the qualities of space, even if space could be successfully regarded as a magnitNote 81 · After this protest against the initial assumptions in Erdmann's deduction of space, let us return to consider the manner, in which this deduNote 82 · This hypothesis, however, is not introduced for its own sake, but only to usher in the Helmholtzian deus ex machina, Mechanics. For MechanicNote 83 · The third chapter, on the philosophical consequences of Metageometry, need not be discussed at length, since it deals rather with space thanNote 84 · With this caution as to the meaning of apriority, we shall find, I think, that the conclusions of Erdmann's final chapter, on the principlesNote 85 · Lotze's argument as regards Geometry[100]—which follows a metaphysical argument as to the ontological nature of space, and assumes the resulNote 86 · Lotze opens with a somewhat startling statement, which, though philosophically worthy to be true, does not appear to be historically borne oNote 87 · Admitting, then, in Lotze's sense, the subjectivity of space, the above possibility does not seem so empty as he imagines. He discusses it bNote 88 · But the bearing of Metageometry is really, I think, different from anything imagined by Lotze; and as few writers seem clear on this point, Note 89 · But the possibility of an inaccuracy so slight, that our finest instruments and our most distant parallaxes show no trace of it, would troubNote 90 · Lotze's attack on Metageometry—although it remains, so far as I know, the best hostile criticism extant, and although its arguments have becNote 91 · The mathematical criticism begins (§ 131) with a somewhat question-begging definition of parallel straight lines. Two straight lines aα, bβ,Note 92 · The next argument for the apriority of Euclidean Geometry has, oddly enough, an exactly opposite bearing, although it is a great favourite wNote 93 · Lotze now proceeds (§ 132) to a detailed criticism of Helmholtz, whom he regards as a typical exponent of Metageometry. It is possible that,Note 94 · After this preliminary discussion of Sphereland, Lotze proceeds to the question of a fourth dimension, and thence to spherical and pseudo-spNote 95 · The rest of the Chapter is devoted to an attack on spherical and pseudo-spherical space, on the ground that they interfere with the homogeneNote 96 · The objections to non-Euclidean Geometry which have just been discussed fall under four heads:Note 97 · Two other objections may, indeed, be urged against Metageometry, but these are rather of a philosophical than of a strictly mathematical impNote 98 · M. Delbœuf's four articles in the Revue Philosophique contain much matter that has already been dealt with in the criticism of Lotze, and muNote 99 · Now we saw, in discussing Erdmann's views of the judgment of quantity, that in non-Euclidean space, as in Euclidean, a change of all spatialNote 100 · The foundations of Geometry have been the subject of much recent speculation in France, and this seems to demand some notice. But in spite oNote 101 · Before beginning the constructive argument of the next Chapter, let us endeavour briefly to sum up the theories which have been polemically Note 102 · Projective Geometry proper, as we saw in Chapter I., does not employ the conception of magnitude, and does not, therefore, require those axiNote 103 · We have good ground for expecting, therefore, that the axioms of projective Geometry will be the simplest and most complete expression of thNote 104 · But unfortunately, the task of discovering the axioms of projective Geometry is far from easy. They have, as yet, found no Riemann or HelmhoNote 105 · In the first place, it is important to realize that when coordinates are used, in projective Geometry, they are not coordinates in the ordinNote 106 · The distinction between various points, then, is not a result, but a condition, of the projective coordinate system. The coordinate system iNote 107 · Now it is obvious that a mere collection of points, distinguished one from another, cannot found a Geometry: we must have some idea of the mNote 108 · All geometrical reasoning is, in the last resort, circular: if we start by assuming points, they can only be defined by the lines or planes Note 109 · The extension of these two reciprocal principles is the essence of all projective transformations, and indeed of all projective Geometry. ThNote 110 · The successive application, to any figure, of two reciprocal operations of projection and section, is regarded as producing a figure protectNote 111 · The two mathematically fundamental things in projective Geometry are anharmonic ratio, and the quadrilateral construction. Everything else fNote 112 · We have next to consider the quadrilateral construction[124]. This has a double purpose: first, to define the important special case known aNote 113 · A harmonic range, in elementary Geometry, is one whose anharmonic ratio is –1, or one in which the three segments formed by the four points Note 114 · The point of importance in the above construction, however, and the reason why I have reproduced it in detail, is that it proceeds entirely Note 115 · Before we can be clear as to the meaning of our principle, we must have some notion as to our definition of points and straight lines. But tNote 116 · How are we to get outside this circle? The fact is that, in pure Geometry, we cannot get outside it. For space, as we shall see more fully hNote 117 · In accordance with this procedure, then, let us define our points as the terms of spatial relations, regarding whatever is not a point as a Note 118 · Projective Geometry, we have seen, does not deal with quantity, and therefore recognizes no difference where the difference is purely quantiNote 119 · We agreed to regard points as the terms of spatial relations, and we agreed that different points could be distinguished. But we postponed tNote 120 · We can now see the reason for what may have hitherto seemed a somewhat arbitrary fact, namely, the necessity of four collinear points for anNote 121 · We can now prove, I think, that two figures, which are projectively related, are qualitatively similar. Let us begin with a collection of poNote 122 · We may now sum up the results of our analysis of projective Geometry, and state the axioms on which its reasoning is based. We shall then haNote 123 · From the exclusively mathematical standpoint, as we have seen, projective Geometry discusses only what figures can be obtained from each othNote 124 · Now when we consider what is involved in such absolute qualitative equivalence, we find at once, as its most obvious prerequisite, the perfeNote 125 · The homogeneity of space and the relativity of position, therefore, are presupposed in the qualitative spatial comparison with which projectNote 126 · In Grassmann's profound philosophical introduction to his Ausdehnungslehre of 1844, he suggested that Geometry, though improperly regarded aNote 127 · The pure doctrine of extension, as constructed by Grassmann, need not be discussed—it included much empirical material, and was philosophicaNote 128 · In any world in which perception presents us with various things, with discriminated and differentiated contents, there must be, in perceptiNote 129 · In the first place, externality is an essentially relative conception—nothing can be external to itself. To be external to something is to bNote 130 · In like manner we can deduce the homogeneity of our form. The diversity of content, which was possible only within the form of externality, Note 131 · From what has been said of homogeneity and relativity, follows one of the strangest properties of a form of externality. This property is, tNote 132 · The next step, in defining a form of externality, is obtained from the idea of dimensions. Positions, we have seen, are defined solely by thNote 133 · The above argument, it may be urged, has overlooked a possibility. It has used a transcendental argument, so an opponent may contend, withouNote 134 · Let us repeat our original argument in the light of this elucidation. A position is completely defined when, and only when, enough relationsNote 135 · Before proceeding further, it is necessary to discuss the important special case where a form of externality has only one dimension. Of the Note 136 · It may be objected, to this argument, that its validity depends upon the assumption that the change of a relation of externality must be conNote 137 · The next step in the argument, which assumes two or more dimensions, is concerned with the general analogues of straight lines and planes, iNote 138 · We have to prove that two positions must have a relation independent of any reference to other positions. To prove this, let us recur to whaNote 139 · With this, our deduction of projective Geometry from the à priori conceptual properties of a form of externality is completed. That such a fNote 140 · In metrical Geometry, on the contrary, we shall find a very different result. Although the geometrical conditions which render spatial measuNote 141 · We have now reviewed the axioms of projective Geometry, and have seen that they are à priori deductions from the fact that we can experienceNote 142 · Metrical Geometry, therefore, though distinct from projective Geometry, is not independent of it, but presupposes it, and arises from its coNote 143 · Metrical Geometry, to begin with, may be defined as the science which deals with the comparison and relations of spatial magnitudes. The conNote 144 · We require, then, at the very outset, some criterion of spatial equality: without such a criterion metrical Geometry would become wholly impNote 145 · A. Philosophical Argument. The denial of the axiom involves absolute position, and an action of mere space, per se, on things. For the axiomNote 146 · B. Geometrical Argument. Let us see next what sort of Geometry we could construct without this axiom. The ultimate standard of comparison ofNote 147 · There is, however, in such a view, as I remarked above, a logical error as to the nature of magnitude. This error has been already pointed oNote 148 · Although this axiom is à priori, its application to the measurement of actual bodies, as we found in discussing Helmholtz's views, always inNote 149 · There remain, however, a few objections and difficulties to be discussed. First, how do we obtain equality in solids, and in Kant's cases ofNote 150 · (1) How do we measure the equality of solids? These could only be brought into actual congruence if we had a fourth dimension to operate in[Note 151 · (2) As regards time, no congruence is here conceivable, for to effect congruence requires always—as we saw in the case of solids—one more diNote 152 · (3) The case of time-measurement suggests the third of the above objections to the absolute necessity of the axiom of Free Mobility. Psycho-Note 153 · (4) One last elucidatory remark is necessary before our proof of this axiom can be considered complete. We spoke above of the Geometry on anNote 154 · It is to be observed that the axiom of Free Mobility, as I have enunciated it, includes also the axiom to which Helmholtz gives the name of Note 155 · The axiom of Free Mobility involves, if it is to be true, the homogeneity of space, or the complete relativity of position. For if any shapeNote 156 · This converse deduction, as regards Free Mobility, is not very difficult, and follows from the argument of Section A[162], which I will brieNote 157 · In summing up the argument we have just concluded, we may exhibit it, in consequence of the two preceding paragraphs, in the form of a complNote 158 · We have seen, in discussing the axiom of Free Mobility, that all position is relative, that is, a position exists only by virtue of relationNote 159 · So much, then, is à priori necessary to metrical Geometry. The restriction of the dimensions to three seems, on the contrary, to be wholly tNote 160 · Let us, since the point seems of some interest, repeat our proof of the apriority of this axiom from a slightly different point of view. We Note 161 · The limitation of the dimensions to three is, as we have seen, empirical; nevertheless, it is not liable to the inaccuracy and uncertainty wNote 162 · We have already seen, in discussing projective Geometry, that two points must determine a unique curve, the straight line. In metrical GeomeNote 163 · (1) The possibility of spatial measurement allows us to infer the existence of a magnitude uniquely determined by any two points. The proof Note 164 · It might be objected, to the above argument, that it involves a petitio principii. For it has been assumed that the two points and their relNote 165 · But why, it may be asked, should there be only one such relation between two points? Why not several? The answer to this lies in the fact thNote 166 · (2) We have thus established our first proposition—two points have one and only one relation uniquely determined by those two points. This rNote 167 · We are accustomed to the definition of the straight line as the shortest distance between two points, which implies that distance might equaNote 168 · A straight line, then, is not the shortest distance, but is simply the distance between two points—so far, this conclusion has stood firm. BNote 169 · To begin with, I must point out that my axiom is not quite equivalent to Euclid's. Euclid's axiom states that two straight lines cannot enclNote 170 · It will be remembered that, in our à priori proof that two points must have one definite relation, we held it impossible for those two pointNote 171 · This, however, is mere speculation. I come now to the pièce de résistance of my argument. The ambiguity in spherical space arose, as we saw,Note 172 · I have now shown, I hope conclusively, that spherical space affords no objection to the apriority of my axiom. Any two points have one relatNote 173 · (3) But farther, the existence of curves uniquely determined by two points can be deduced from the nature of any form of externality[176]. FNote 174 · (4) Finally, we have to prove that the existence of such a curve necessarily leads, when quantity is applied to the relation between two poiNote 175 · To sum up: If points are defined simply by relations to other points, i.e., if all position is relative, every point must have to every otheNote 176 · In connection with the straight line, it will be convenient to discuss the conditions of a metrical coordinate system. The projective coordiNote 177 · The above three axioms, we have seen, are à priori necessary to metrical Geometry. No others can be necessary, since metrical systems, logicNote 178 · In summing up the distinctive argument of this Section, we may give it a more general form, and discuss the conditions of measurement in anyNote 179 · We have now seen in what the à priori element of Geometry consists. This à priori element may be defined as the axioms common to Euclidean aNote 180 · In the present chapter, we have to discuss two questions which, though scarcely geometrical, are of fundamental importance to the theory of Note 181 · I have already indicated, in general terms, the ground for regarding as à priori the properties of any form of externality. This ground is tNote 182 · [178]. The view suggested has, obviously, much in common with that of the Transcendental Aesthetic. Indeed the whole of it, I believe, can bNote 183 · In the first place, the psychological element is much larger in Kant's thesis than in mine. I shall contend, it is true, that a form of exteNote 184 · We have a right, therefore, in an epistemological inquiry, to neglect Kant's psychological teaching—in so far, at any rate, as it distinguisNote 185 · What, then, remains the kernel, for our purposes, of Kant's first argument for the apriority of space? His argument, in the form in which heNote 186 · This, then, is the kind of externality we are to expect from space, and our question must be: Would the existence of diverse but interrelateNote 187 · The converse argument to mine, the argument from the spatio-temporal element in perception to a world of interrelated but diverse things, isNote 188 · This doctrine of Bradley and Bosanquet is the converse of the epistemological doctrine I have to advocate. Owing to the continuity and relatNote 189 · The essence of my contention is that, if experience is to be possible, every sensational This must, when attended to, be found, on the one hNote 190 · We might be inclined, at first sight, to answer this question affirmatively. But several difficulties, I think, would prevent such an answerNote 191 · But we have derived, from all this, no ground for affirming a multiplicity of real things, or a form of externality of more than one dimensiNote 192 · The above argument, I hope, has explained why I hold it possible to deduce, from a mere conception like that of a form of externality, the lNote 193 · How we are to account for the fortunate realization of these requirements—whether by a pre-established harmony, by Darwinian adaptation to oNote 194 · I come now to the second question with which this chapter has to deal, the question, namely: What are we to do with the contradictions whichNote 195 · The contradictions in space are an ancient theme—as ancient, in fact, as Zeno's refutation of motion. They are, roughly, of two kinds, thougNote 196 · (1) Points. The antinomy of the point—which arises wherever a continuum is given, and elements have to be sought in it—is fundamental to GeoNote 197 · Thus Geometry is forced, since it wishes to regard space as independent, to hypostatize its abstractions, and therefore to invent a self-conNote 198 · Let us see whether, by this change, we can overcome the antinomy of the point. Spatial figures, we shall now say, are relations between the Note 199 · But what nature must we ascribe to this matter, which is to be involved in all geometrical propositions? In criticizing Helmholtz (Chap. II.Note 200 · (2) The circle in the definition of straight lines and planes. This difficulty need not long detain us, since we have already, with the mateNote 201 · (3) Space is at once relational and more than relational. We have already touched on the question how far space is other than relations, butNote 202 · Now for this discussion it is essential to distinguish clearly between empty space and spatial figures. Empty space, as a form of externalitNote 203 · Let us consider what this empty space is. (I speak of "empty" space without necessarily implying the absence of matter, but only to denote aNote 204 · But can we agree in regarding empty space, the "infinite given whole," as really given? Must we not, in spite of Kant's argument, regard it Note 205 · Another ground for condemning empty space is to be found in the mathematical antinomies. For it is no solution, as Lotze points out (MetaphyNote 206 · But whence arises, on this view, the paradox that we cannot but regard space as having more or less thinghood, and as divisible ad infinitumNote 207 · The apparent divisibility of the relations which constitute spatial order, then, may be explained in two ways, though these are at bottom eqNote 208 · But in what sense does spatial order consist of relations? We have hitherto spoken of externality as a relation, and in a sense such a manneNote 209 · We have now completed our review of the foundations of Geometry. It will be well, before we take leave of the subject, briefly to review andNote 210 · Cf. Erdmann, Axiome der Geometrie, p. 111: "Für Kant sind Apriorität und ausschliessliche Subjectivität allerdings Wechselbegriffe."Note 211 · I use "experience" here in the widest possible sense, the sense in which the word is used by Bradley.Note 212 · Where the branch of experience in question is essential to all experience, the resulting apriority may be regarded as absolute; where it is Note 213 · I have given no account of these empirical proofs, as they seem to be constituted by the whole body of physical science. Everything in physi
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