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What Does It Mean That ‘‘Space Can Be TranscendentalWithout the Axioms Being So’’?
Helmholtz’s Claim in Context
Francesca Biagioli
� Springer Science+Business Media Dordrecht 2013
Abstract In 1870, Hermann von Helmholtz criticized the Kantian conception of geometrical
axioms as a priori synthetic judgments grounded in spatial intuition. However, during his
dispute with Albrecht Krause (Kant und Helmholtz uber den Ursprung und die Bedeutung der
Raumanschauung und der geometrischen Axiome. Lahr, Schauenburg, 1878), Helmholtz
maintained that space can be transcendental without the axioms being so. In this paper, I will
analyze Helmholtz’s claim in connection with his theory of measurement. Helmholtz uses a
Kantian argument that can be summarized as follows: mathematical structures that can be
defined independently of the objects we experience are necessary for judgments about mag-
nitudes to be generally valid. I suggest that space is conceived by Helmholtz as one such
structure. I will analyze his argument in its most detailed version, which is found in Helmholtz
(Zahlen und Messen, erkenntnistheoretisch betrachtet 1887. In: Schriften zur Erkenntnis-
theorie. Springer, Berlin, 1921, 70–97). In support of my view, I will consider alternative
formulations of the same argument by Ernst Cassirer and Otto Holder.
Keywords Geometrical empiricism � Hermann von Helmholtz � Measurement �Transcendental intuition
1 Introduction
The well-known lecture Hermann von Helmholtz gave in Heidelberg in 1870, ‘‘Uber den
Ursprung und die Bedeutung der geometrischen Axiome’’, includes a presentation of his
inquiry on the foundations of geometry for a wider audience and Helmholtz’s objection to
Kant. Helmholtz rejects Kant’s conception of the principles of geometry as a priori syn-
thetic judgments. On Helmholtz’s view, geometrical axioms provide us with objective
knowledge only when taken in connection with the principles of mechanics. In this regard,
F. Biagioli (&)Institut fur Humanwissenschaften: Philosophie, Universitat Paderborn, 33098 Paderborn, Germanye-mail: [email protected]
123
J Gen Philos SciDOI 10.1007/s10838-013-9223-7
geometry becomes empirically testable and its certainty does not depend on a priori
intuition.
In the following, I will discuss attempts to defend the Kantian theory of space, such as
Jan Pieter Nicolaas Land’s attempt of 1877 and Albrecht Krause’s attempt of 1878. They
are worth discussing because in the debate Helmholtz makes it clear that he is not willing
to reject the Kantian theory of space altogether. He now maintains that ‘‘space can be
transcendental without the axioms being so’’ (Helmholtz 1977, 149). Helmholtz’s claim
appears in the title of his reply to Krause, which is published as the second Appendix to
Helmholtz’s paper ‘‘Die Tatsachen in der Wahrnehmung’’ (1878b). There Helmholtz
distinguishes between the general form of spatial intuition and its narrower specifications,
which are the axioms of geometry.
The interpretation of Helmholtz’s claim immediately became a matter of controversy.
Philosophers such as Alois Riehl used Helmholtz’s claim to argue that Kant’s theory may
work for intuitive space independently of the results of measurements in physical space
(Riehl 1904, 263). Following Riehl’s line of argument, Moritz Schlick goes a step further.
In his comments to the celebrated centenary edition of Helmholtz’s Schriften zur Er-
kenntnistheorie (1921), Schlick identifies Helmholtz’s ‘‘narrower specifications’’ with
axioms of congruence about physical magnitudes. Schlick sharply distinguishes these
properties from topological properties, such as three-dimensionality, continuity etc., which
are supposed to be grounded in spatial intuition. In order to uphold Helmholtz’s distinction,
Schlick deems the general characteristics of space indescribable, psychological factors in
spatial perception (see Schlick’s comment in Helmholtz 1977, 128, note 33).
Schlick’s interpretation is at odds with the Kantian theory: one needs not introduce a
‘‘pure’’ intuition besides the empirical one. Then why does Helmholtz deem space
‘‘transcendental’’? On the other hand, any rejection of Schlick’s interpretation is committed
to another question: what are the general characteristics of space? Furthermore, a Kantian
interpretation is supposed to give reasons for the transcendental role of space. It is difficult
to see what Helmholtz means because Kant himself never used the expression ‘‘tran-
scendental space’’: arguably, Helmholtz is thinking in terms of ‘‘a priori’’ here. His choice
of ‘‘transcendental’’ might be explained by the fact that it ought to be proved that the
general characteristics of space play a role in the constitution of the object of experience.
Indeed, such a proof would require a transcendental argument in Kant’s sense.
Let us begin with the second question, i.e. the question what the general characteristics
of space are. Helmholtz’s conception of space can be specified in different ways. Roberto
Torretti points out that the general properties of space may not have counted as axioms in
the Euclidean tradition. This does not mean that they cannot be axiomatized at all. Fol-
lowing Helmholtz’s analogy with color-mixtures, Torretti suggests that the required
characteristics may be specified by use of the theory of manifolds.1 He describes Helm-
holtz’s space as a differentiable three-dimensional manifold. The axioms of quantity are
not determined by the form of space because their formulation presupposes the existence of
the solid bodies we experience (Torretti 1978, 166–167). This interpretation can be called
1 Helmholtz’s conception of the relationship between space form and reality does not coincide with that ofmany followers of Kant. But Helmholtz does not exclude that space may be ‘‘a form of intuition in theKantian sense, and yet not necessarily involve the axioms’’ […]. ‘‘To cite a parallel instance, it undoubtedlylies in the organisation of our optical apparatus that everything we see can be seen only as a spatialdistribution of colours. This is the innate form of our visual perceptions. But it is not in the least therebypredetermined how the colours we see shall co-exist in space and follow each other in time’’ (Helmholtz1878a, 213). Helmholtz’s source is Hermann Grassmann’s work on manifolds and its application to color-mixtures (see Hatfield 1990, 218, note 106; Hyder 2009, chap. 4).
F. Biagioli
123
into question for several reasons. On the one hand, a priori properties cannot be identified
with topological properties. One of such properties, i.e. three-dimensionality, follows from
Helmholtz’s analysis of sense perception, and requires intentional motion. So the form of
spatiality may be described more generally as a differentiable n-fold extended manifold
(Lenoir 2006, 201–202). On the other hand, there is evidence that Helmholtz ascribes to
space both three-dimensionality and constant curvature, which, as a result of his inquiries
on the foundations of geometry of 1868 and 1870, is supposed to follow from the free
mobility of rigid bodies. He distinguishes between space and axioms because, if one
defines space as a differentiable three-dimensional manifold of constant curvature, a choice
has to be made between the three classical cases of such manifolds (see Friedman 1997, 33;
Ryckman 2005, 73).
I believe that the confusion about Helmholtz’s conception of space shows the influence
of Schlick’s interpretation. Schlick’s claim that the qualities of sense perception are
indescribable is misleading: since the requirement of indescribability is questionable, some
interpreters seek to make sense of the quality–quantity opposition by introducing the
distinction between topological and metrical properties. However, Helmholtz does not take
into account the topological–metrical distinction. And his conception of the qualities of
sense perception is quite different from Schlick’s. Helmholtz deems sensations ‘‘signs’’ for
their stimuli. So it might seem that we can only achieve intuitive acquaintance of their
meaning. However, Helmholtz requires that the meaning of sensations be grasped by the
understanding (1867, 797). This point has been clarified by Michael Friedman, who
interprets Helmholtz’s conception of space as follows: the localization of the objects in
space provides us also with a construction of the concept of space (Friedman 1997, 33).
Helmholtz’s argument would be that the forms of intuition, once acquired, can be tran-
scendental. This leads us to our first question, i.e. the question why Helmholtz deems space
‘‘transcendental’’. I do not believe that a psychological analysis of the concept of space
might give reasons for the claim that space is transcendental. Helmholtz rejects Kant’s
view that the axioms of (Euclid’s) geometry are necessarily valid for the empirical man-
ifold. Nevertheless, Helmholtz’s replies to Land and Krause show a Kantian line of
argument: the characteristics of space should provide us with general conditions of mea-
surement, and Helmholtz deems ‘‘objective’’ those results of measurement whose inter-
pretation depends on such conditions. Schlick’s quality–quantity opposition does not play
any role here: the metrical aspect is crucial to Helmholtz’s analysis of the concept of space,
and cannot be overlooked without trivializing his argument. As pointed out by Helmut
Pulte, Helmholtz’s spatial intuition is richer than Schlick’s, because it operates with the
free mobility of rigid bodies and therefore entails that space is a manifold of constant
curvature (Pulte 2006, 198).
In the first part of the paper, I will present Helmholtz’s discussion with Land and
Krause. The defect of their views, according to Helmholtz, is that they are not able to
account for measurement. In the second part of the paper, I will reconstruct the above-
mentioned Kantian line of argument by reading Helmholtz’s defense of scientific mea-
surements in connection with his theory of measurement of 1887. I agree with neo-
Kantians, such as Ernst Cassirer, that Helmholtz’s psychological interpretation of Kant’s
forms of intuition should be rejected for philosophical reasons. Firstly, a psychological
origin of such forms would exclude their general validity. Secondly, the use of psychology
can be made superfluous, if Helmholtz’s issue is reformulated in mathematical terms. I will
argue that, nevertheless, Helmholtz’s conditions of measurement may play a constitutive
function in Kant’s sense, insofar as Helmholtz foreshadows a formal analysis of mea-
surement, such as Otto Holder’s theory of quantity of 1901. I am aware that I reject an
Space Can Be Transcendental Without the Axioms
123
important part of Helmholtz’s view, and yet I do not see my criticism as an external one.
My claim is that the line of argument suggested by Holder and Cassirer clarifies the
metrical aspect overlooked by Schlick: Helmholtz does not admit incommensurable
magnitudes, because measurability requires that general principles be formulated and
coherently extended to empirical domains independently of the specific nature of the
objects to be measured.
2 Helmholtz’s Reply to Jan Pieter Nicolaas Land
In 1876, 6 years after his public lecture in Heidelberg, Helmholtz revises his paper on the
origin and meaning of geometrical axioms and translates it into English for the British
Journal Mind. In the English version of his paper, Helmholtz summarizes the outcome of
his inquiry as follows:
1. The axioms of geometry, taken by themselves out of all connection with mechanical
propositions, represent no relations of real things. When thus isolated, if we regard
them with Kant as forms of intuition transcendentally given, they constitute a form
into which any empirical content whatever will fit and which therefore does not in any
way limit or determine beforehand the nature of the content. This is true, however, not
only of Euclid’s axioms, but also of the axioms of spherical and pseudospherical
geometry.
2. As soon as certain principles of mechanics are conjoined with the axioms of geometry
we obtain a system of propositions which has real import, and which can be verified or
overturned by empirical observations, as from experience it can be inferred. If such a
system were to be taken as a transcendental form of intuition and thought, there must be
assumed a pre-established harmony between form and reality. (Helmholtz 1876, 321)
This passage foreshadows Helmholtz’s distinction between space and geometrical axioms:
in the first case, space is deemed transcendental, and, in the second case, our system of
propositions is said to have real import. Notice that these cases exclude each other: in the
first case, the axioms of geometry are not synthetic for Helmholtz, and, in the second case,
the assumption of a transcendental form of intuition presupposes an idealistic argument he
usually rejects (see, e.g., Helmholtz 1903, 164). So the claim that space can be
transcendental without the axioms being so requires an explanation. The first step in this
direction is Helmholtz’s reply to Land: Helmholtz argues for the view that geometrical
axioms are synthetic from the standpoint of both realism and idealism.
Let us present Land’s remarks. In his paper ‘‘Kant’s Space and Modern Mathematics’’
(1877), Land maintains that Helmholtz overlooks the distinction between objectivity and
reality. Whereas common sense regards the phenomena as real things, science regards
them as signs for real things, because objective knowledge presupposes some interpretation
of the data of sense perception. Physics agrees with common sense as far as metrical
properties are concerned and we are counting and measuring. But we cannot attach real
import to analytic geometry, which ‘‘has but a conventional connection with the data of
intuition, and merges into pure arithmetic’’ (Land 1877, 41).
Land admits that the axioms of geometry, taken by themselves out of all connection
with mechanical propositions, represent no relation between physical objects. Axioms
which concern parts of space do not determine the deportment of bodies which fill such
parts at a given moments. In this regard, Helmholtz is right: Euclid’s axioms do not differ
from those of spherical or pseudospherical geometry. Nevertheless, Land maintains that the
F. Biagioli
123
form of spatial intuition which is actually given is that analyzed in Euclid’s axioms (Land
1877, 46).
Helmholtz’s reply appears in Mind as a second part of his paper on the origin and
meaning of geometrical axioms (1878a). A revised version of this part is published in
German in the same year as the third Appendix to the paper on the facts in perception. In
his reply, Helmholtz clarifies his use of expressions such as ‘‘relations between real things’’
and ‘‘real import’’. He calls physically equivalent those spatial magnitudes in which under
like conditions, and in like periods of time, like physical processes can exist and run their
course. In order to prove that two such magnitudes are equal, we usually superpose them
and verify whether they can be brought into congruent coincidence. As a general outcome
of our experiences, two such magnitudes show their equivalence also with respect to all
other known physical processes. Therefore Helmholtz maintains that physical equivalence
is ‘‘a perfectly definite’’ and ‘‘objective’’ attribute of spatial magnitudes (1878a, 218).
These considerations would give us a kind of geometry Helmholtz calls physical. Were
our spatial intuition endowed with an exact geometrical structure, there would also be a
pure geometry in which congruence can be defined independently of any motion. Land’s
argument can now be formulated as follows: these two kinds of geometries cannot con-
tradict each other. Whereas congruence, according to our inner intuition, depends on the
makeup of our mind, objective congruence depends on the physical properties of the bodies
we experience. But it might be asked whether the two different kinds of equality neces-
sarily coincide. Helmholtz’s answer is ‘‘no’’: such a coincidence would be only hypo-
thetical. Physical space and spatial intuition could also be supposed to be related to each
other as is actual (Euclidean) space to its (non-Euclidean) image in a convex mirror.
Helmholtz’s conclusion is the following:
If we really had an innate and indestructible form of space-intuition involving the
axioms within it, their objective scientific application to the phenomenal world
would be justified only in so far as observation and experiment made it manifest that
physical geometry, grounded in experience, could establish universal propositions
agreeing with the axioms. (Helmholtz 1878a, 221)
This is a realist description of the situation Helmholtz had already discussed in 1876. He
now maintains that his argument holds true also from an idealist point of view. He
distinguishes between the topogenous factors of localization and the hylogenous ones: the
former ones specify at what place in space an object appears us; the latter ones cause our
belief that at the same place we perceive at different times different material things having
different properties. Helmholtz formulates his argument as follows:
When we observe that the most diverse physical processes may go on during equal
periods of time in similar fashion at different, but congruent, parts of space, the real
meaning of such perception is, that there may be in the sphere of reality equal
sequences and aggregates of hylogenous moments combining with certain distinct
groups of topogenous moments, which letter we then call physically-equivalent. We
may thus discover by observation what special figures appearing in our perception
correspond with physically-equivalent topogenous moments; and experience tells us
that they are equivalent for all physical processes. (1878a, 224)
The German version of the paper is more explicit: the proposition that any combination or
sequence of hylogenous factors which can exist and run its course in combination with one
group of topogenous factors, is also possible with any other physically equivalent group of
topogenous factors is said to have ‘‘real content’’, and provides us with a proof that
Space Can Be Transcendental Without the Axioms
123
topogenous factors influence the course of real processes (Helmholtz 1977, 161).
Helmholtz deems his argument idealistic, because the objectivity of scientific measure-
ments does not presuppose that any specific structure is found in actual space. All that is
presupposed is that some regularity is found in the phenomena. If space is identified with
the most general structure or group of topogenous factors underlying such regularities,
Helmholtz’s argument shows the role of this structure in the constitution of the object of
experience, and may be regarded as a transcendental argument in Kant’s sense.
3 Helmholtz’s Reply to Albrecht Krause
These considerations may help us to explain why Helmholtz sees his claim that space is
transcendental without the axioms being so as a reply to Krause in particular: Helmholtz
uses the notion of ‘‘transcendental’’ in connection with his attempt to justify the objectivity
of measurements. First of all, let us present Krause’s comparison between Kant and
Helmholtz. Krause’s essay Kant und Helmholtz uber den Ursprung und die Bedeutung der
Raumanschauung und der geometrischen Axiome (1878) begins with the following ques-
tion: can one state different properties of space and, consequently, different geometrical
axioms? In order to answer this question, Krause considers the relationship between the
sense organs and the brain. He maintains that the Kantian theory of space is compatible
with the requirement that spatial relations be univocally determined through their con-
nection with the brain, whatever form or size the sense organs may have. Krause’s view is
that any variation or hypothesis of different spaces is based on one and the same space,
whose properties depend immediately on higher cognitive functions. Otherwise the form of
our intuition would vary according to our sense organs, whose spatial features are con-
tingent. Therefore Krause rejects Helmholtz’s attempt to draw spatiality out of sensations.
Krause criticizes, in particular, Helmholtz’s argument that a comparison between our space
and its image in a convex mirror should provide us with intuitions we never had. According
to Krause, such intuitions are impossible. He considers plain surfaces, as well as curved
ones, as the boundaries of a three-dimensional body. Straight lines would not correspond to
the geodesics of spherical or pseudospherical geometry. And ‘‘straightest’’ lines between
pairs of points would mean straight lines in the proper sense of the term. For the same
reason, Krause calls into question the extension of the concept of curvature to more than
two-dimensional manifolds: the curvature of space cannot be measured because anything
endowed with direction already lies in space (Krause 1878, 84).
Krause’s further question is: to what extent are the laws of spatial intuition expressed by
the axioms certain? His answer is that, since spatial intuition is necessary for the construction
of every geometric object, the certainty of geometrical axioms cannot be called into question.
The skeptical outcome of the so-called ‘‘Riemann-Helmholtz’s theory’’ is that there would be
no geometrical axiom properly speaking. Krause’s view entails that we should not trust our
measurements, when they contradicted the axioms, because measurements share the
approximate character of natural laws. By contrast, axioms are exact knowledge.
In his reply, Helmholtz makes it clear that the empiricist theory of vision does not entail
that the spatial features of our sense organs determine form and size of the objects.2 More
2 Krause’s description is an oversimplification of the theory of local signs, which would entail, for instance,that a child sees smaller that an adult, for his eyes are smaller. But this assumption is contradicted byempirical facts we are most familiar with (Krause 1878, 39). Krause overlooks that Helmholtz’s explanationof visual perception is psychological rather than physiological (see Hatfield 1990, 182).
F. Biagioli
123
notably, he points out that the Kantian theory of knowledge is not committed to Krause’s
assumptions, which are derived from a nativist theory of vision. So Krause’s argument can
be falsified from a philosophical point of view: once nativist assumptions are rejected,
space can be transcendental without the axioms being so.
Regarding Krause’s objections to nineteenth-century inquiries on the foundations of
geometry, Helmholtz replies that the measure of curvature is a well-defined magnitude and
generally applies to n-dimensional manifolds. This consideration nullifies Krause’s attempt
to show that Euclidean three-dimensional space is a necessary assumption. Helmholtz’s
point is that we must give reasons for our assumptions. Curiously enough, Krause does not
take into account the results of scientific measurements because of their limited accuracy.
But he does not need measurements to be convinced of the correctness of those axioms
which are supposed to be grounded in transcendental intuition. In this case, Krause reas-
sures himself with appraisals by ‘‘visual estimation’’. That is, for Helmholtz, ‘‘measuring
friend and foe by different standards!’’ (1977, 151).
Helmholtz does not say much about the convenience of regarding space as a tran-
scendental concept. Nevertheless, his considerations suffice to exclude Schlick’s later
interpretation. Helmholtz makes it clear that, if the form of intuition is transcendental, it
cannot be given ‘‘by visual estimation’’. Otherwise it could not provide us with conditions
of experience. Furthermore, it should be noticed that Helmholtz does not use Riemann’s
distinction between metrical and extensive properties. In fact Krause overlooks this dis-
tinction. But Helmholtz’s objection to Krause goes deeper: by dismissing well-defined
magnitudes, such as the measure of curvature, and by mistrusting scientific procedures,
Krause fails to explain measurement.
We shall return to this point later on. It may be helpful to notice first that Helmholtz’s
reply was anticipated in many ways by Benno Erdmann in his essay Die Axiome der
Geometrie: Eine philosophische Untersuchung der Riemann-Helmholtz’schen Raumtheo-
rie (1877). Erdmann calls both Helmholtz’s and Riemann’s epistemology a kind of formal
empiricism, according to which our representations are only partial images of the things,
which coincide with them in every quantitative relation (space, time, and natural laws)
while differing from them in every qualitative one. The assumption of a pre-established
harmony between sensations and their causes is called into question because our mental
activities are supposed to originate from our interaction with the world.3 The empirical
occasion does not provide us with spatial determinations; rather, we form spatial concepts
in order to organize our sensations. The form of space must be distinguished from its
empirical content.
Regarding the philosophical meaning of the inquiries on the foundations of geometry,
Erdmann argues that both Riemann’s inquiry on the hypotheses underlying geometry
(1854) and Helmholtz’s mental experiments of 1870 contradict the rationalist opinion that
our spatial intuition is independent of experience. If rationalists were right, space could not
undergo any changes. By contrast, Riemann and Helmholtz show that space admits dif-
ferent geometries. However, they neither answer the question of whether our inference
from our representations to the existence of the things is correct (which is a matter of
controversy between idealism and realism), nor do they exclude other kinds of empiricism.
3 Cf. Krause’s above mentioned misunderstanding of the theory of local signs. Hatfield points out thatHelmholtz considered spiritualist as well as materialist identifications of psychic activities with the materialworld as metaphysical views, lacking explanatory power. By contrast, ‘‘[Helmholtz’s] explanation ascribedthe origin of our spatial abilities to the acquisition of rules for generating spatial representations, theacquisition process being guided by causal commerce with external objects’’ (Hatfield 1990, 191).
Space Can Be Transcendental Without the Axioms
123
Besides formal empiricism, a choice is given between sensism, according to which our
representations are images of the things, and a refined kind of apriorism, which assumes
that our representations, even though they are completely different from the things, may
correspond to them in each and every single part. Erdmann argues for apriorism as follows.
He maintains that the concept of space can be specified both geometrically and analyti-
cally. On the one hand, a system of metric relations can be derived from our spatial
intuition, which is supposed to be singular and directly given, and yet capable of infinitely
many variations. On the other hand, Riemann shows that a generalized metric form can be
developed also analytically, so that our original system becomes a special case. Now, this
prompts the question of how the geometrical and analytical interpretations of geometric
concepts are related. In order to answer this question, Erdmann uses the whole-part
opposition, which is characteristic of his apriorism. He writes:
The fact that our spatial intuition is single is not contradicted: we can only con-
ceptualize the general intuition of a pseudospherical or spherical space of a certain
measure of curvature. Such uniqueness, however, is not absolute anymore, because
we can fix homogeneous parts of those spaces intuitively and compare them with the
metrical relations between partial representations of our space. But the concepts of
such spaces show in their development all the clearness and distinction enabled by
the discursive nature of conceptual knowledge. Therefore we may also speak about a
concept of space. At the same time, however, we clearly cannot form it directly
without a diversion into the concept of quantity. (Erdmann 1877, 135)
This passage refers to Helmholtz’s mental experiments. Helmholtz’s world in the convex
mirror shows that an intuitive comparison between different metrics is possible, though
only locally: in order to make such a comparison, one should not start from space itself but
from its parts. Helmholtz adopts Riemann’s approach: the concept of space presupposes
that of quantity, not vice versa. At the same time, Erdmann does not reject the Kantian
hypothesis that space as a whole is a singular intuition, not a concept.
Helmholtz rejects Kant’s supposition. As Helmholtz puts it, the resolution of the con-
cept of intuition into the elementary processes of thought is the most essential advance in
the recent period (1977, 143). Nevertheless, he appreciates Erdmann’s work on the axioms
of geometry as a reliable discussion of that subject-matter in philosophical terms (Helm-
holtz 1977, 149). In my opinion, Helmholtz’s appreciation is due to the fact that Erdmann,
unlike Land and Krause, seeks to explain how space and quantity are related to each other.
Similarly, in order to construct the concept of space, Helmholtz begins with the most basic
relationship between spatial magnitudes—namely, their congruence. The broader specifi-
cations of space, especially constant curvature, are supposed to be determined by the free
mobility of rigid bodies, which is required for spatial magnitudes to be congruent. Since
manifolds of constant curvature admit different geometries, narrower specifications, such
as the axioms of congruence, must be distinguished from the general principles of
measurement.
To summarize, Helmholtz’s distinction between space and axioms follows from his
analysis of measurement. This distinction does not provide an argument for Helmholtz’s
connection with Kant. Helmholtz’s argument goes from the parts to the whole, and is not
compatible with Kant’s conclusion that space is an intuition, not a concept. Nevertheless,
Helmholtz’s formal-empiricist attempt to prove that quantitative relations are common to
subjective and objective experience might require a transcendental argument. As we shall
see, such argument is explicit in Helmholtz’s paper ‘‘Zahlen und Messen, er-
kenntnistheoretisch betrachtet’’ (1887). I suggest that a reconstruction of his argument may
F. Biagioli
123
help us to explain his use of the notion of ‘‘transcendental’’. Firstly, the same expression is
used here with regard to time. Secondly, and more notably, in 1887 Helmholtz develops a
general theory of measurement or composition of physical magnitudes, so that congruence
can be treated as a special case. In the dispute with Krause, the issue at stake is the same. I
shall then add some remarks on Helmholtz’s conception of space and its reception after
presenting his full analysis of measurement.
4 Transcendental Intuition in Counting and Measuring
At the beginning of ‘‘Zahlen und Messen’’, Helmholtz summarizes his remarks on tran-
scendental intuition as follows. Geometrical axioms cannot be derived from an innate
intuition independently of experience. Helmholtz does not reject Kant’s view of space as a
transcendental form of intuition, but rather that particular specification of his view which
was influenced by the metaphysical endeavors of his successors.4 We already noticed that a
legitimate idealistic interpretation of the transcendental role of space in Helmholtz’s sense
should take into account an inner-outer opposition, which is reflected in the opposition
between physical and pure geometry. Helmholtz’s point in 1887 is that such interpretation
must be completed by an inquiry on the foundations of arithmetic, for several reasons.
Firstly, physical equivalence between spatial magnitudes is supposed to admit a numerical
expression. Secondly, Helmholtz’s goal is to use his theory of knowledge to account for the
origin and meaning of the axioms of arithmetic. He writes:
[…] if the empiricist theory—which I besides others advocate—regards the axioms
of geometry no longer as propositions unprovable and without need of proof, it must
also justify itself regarding the origin of the axioms of arithmetic, which are cor-
respondingly related to the form of intuition of time. (Helmholtz 1977, 72)
The parallelism with space suggests that time can be deemed transcendental in the same
sense: a transcendental argument is necessary for the axioms of arithmetic to be valid for
the empirical manifold. They are the following propositions:
AI. If two magnitudes are both alike with a third, they are alike amongst themselves.
AII. The associative law of addition: (a ? b) ? c = a ? (b ? c).
AIII. The commutative law of addition: a ? b = b ? a.
AIV. Like added to like gives like.
AV. Like added to unlike gives unlike.
Helmholtz’s argument proceeds as follows. First of all, he notices that arithmetic tea-
ches the logical application of a system of signs (i.e., numbers) and explores which dif-
ferent combinations (i.e., calculative operations) lead to the same results. Such a system,
however, neither warrants the inner coherence of our thought nor sets out rules of play for
fictitious objects. The axioms of arithmetic are laws of addition. And additive principles of
the same kind are required for physical magnitudes to be compared. Helmholtz’s purpose is
to provide us with a natural basis for our use of symbols and a proof of their applicability.
Therefore he deems arithmetic ‘‘a method constructed upon purely psychological facts’’
4 Recall that already in 1855, in a celebrated lecture entitled ‘‘Uber das Sehen des Menschen’’, Helmholtzcontrasts Kant with later attempts to solve nature into a system of subjective forms, as pursued by nine-teenth-century philosophers of identity such as Hegel. Helmholtz’s conception of the interaction betweensubjective and objective factors of knowledge has its roots in his interpretation of Kant as well as in hisreception of the philosophy of Fichte (see Kohnke 1986, 151–153; Heidelberger 1994, 170–175).
Space Can Be Transcendental Without the Axioms
123
(Helmholtz 1977, 75). For Helmholtz the clarification of this point requires a complete
analysis of the concept of number. In a certain sense, it is clear that the ‘‘naturalness’’ of
the number series is merely an appearance: the choice of number signs is a matter of
stipulation and the so-called ‘‘natural’’ numbers are but arbitrarily chosen signs. All the
same, their series is impressed on our memory much more firmly than any other series of
objects as a consequence of its frequent repetition. Ordinal numbers acquire a paradigmatic
role in the recollection of all other sequences in our memory, and their series shows the
characteristics of inner intuition: each representation entering our consciousness is nec-
essarily subject to an irreversible relationship with the preceding and the following rep-
resentations in the series and it is uniquely singled out by its position in time. This requires
us to designate each step in the series by means of a system of signs that allows neither
interruptions nor repetitions, as in the decimal system. Helmholtz maintains that the
complete disjunction thereby obtained is ‘‘founded in the essence of the time sequence’’
(1977, 77). He expresses this fact as follows:
AVI. If two numbers are different, one of them must be higher than another.
AVI entails that ordinal relations are asymmetric and transitive. From AI it follows that
equality is transitive and symmetric instead. From transitivity (i.e., if a = b and b = c,
then a = c) the validity of AI for the series of integer numbers follows. And a generalized
form of the remaining axioms can be derived from:
aþ bð Þ þ 1 ¼ aþ bþ 1ð Þ:
This is Grassmann’s axiom, which provides us with a definition of addition. For example,
the associative law of addition is generalized as follows:
Rþ aþ bþ S ¼ Rþ aþ bð Þ þ S;
where capital letters denote the sum of arbitrarily many numbers.
Once addition has been defined, Helmholtz introduces the following axiom:
AVII. If a number c is higher than another one a, then I can portray c as the sum of a and
a positive integer number b to be found.
In the following, Helmholtz extends the laws of addition, especially AVII, to cardinal
numbers. He describes the method of numbering off for the purpose of addition as coor-
dinating an ordered sequence (n ? 1), (n ? 2)… to the series of integer numbers. He then
combines a first series preserving a certain sequence with a second series having variable
sequences. Given two numbers n and (n ? 1), on the one side, and two symbols e and f, on
the other, there are two possible manners of coordination:
aÞ n! e; nþ 1ð Þ ! f
or bÞ n! f; nþ 1ð Þ ! e:
If a) is substituted for b), the second series a, b, c, etc. can be put into one-to-one
correspondence with the series (n ? 1), (n ? 2), etc. By continued exchange of neigh-
boring members of a group, we bring about any possible sequence of its members without
gaps or repetitions. According to Helmholtz’s theorem:
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123
Attributes of a series of elements which do not alter when arbitrarily neighbouring
elements are exchanged in order with each other, are not altered by any possible
alteration of the order of the elements. (1977, 85)
As a consequence of this theorem, cardinal numbers can be defined as follows: if the
complete number series from 1 to n is needed in order to coordinate a number with each
element of the group, then n is called the cardinal number of the members of the group.
The corresponding proposition for AVII is that the total number of the members of two
groups that have no member in common equals the sum of the cardinal numbers of the
members of the two single groups. Another consequence is that the commutative law of
addition can be generalized as follows. Given the associative law of addition, by AIII, and
by his theorem, Helmholtz infers that:
Rþ aþ bþ S ¼ Rþ aþ bð Þ þ S ¼ Rþ bþ aþ S:
Summing up, Helmholtz develops a theory of ordinal number: the laws of addition
apply, first of all, to ordinal numbers, but he needs a theorem in order to prove that the
same laws apply to cardinal numbers as well. It might seem that this technicality does not
provide us with a justification of Helmholtz’s empiricist theory. Note, however, that
Helmholtz’s conception of addition is not arithmetical strictly speaking. Arithmetical
addition is but a (possibly paradigmatic) case. But there are different kinds of numbering
also within the theory of numbers, and we do not know from the start whether the laws of
addition apply to the specific case of numbering that ascertains the cardinality of a set of
things. If Helmholtz’s theory of knowledge is to be justified, the same principles must be
extended to empirical domains. So it is not surprising that Helmholtz resumes his con-
siderations on transcendental intuition after presenting his theory of number. He writes:
The concept of addition described above […] coincides with the concept of it which
proceeds from determining the total cardinal number of several groups of numerable
objects, but has the advantage of being obtainable without reference to external
experience. One has thereby proved, for the concepts of number and of a sum—taken
only from inner intuition—from which we started out, the series of axioms of
addition which are necessary for the foundation of arithmetic; and also proved, at the
same time, that the outcome of this kind of addition coincides with the kind which
can be derived from the numbering of external numerable objects. (Helmholtz 1977,
87)
The concepts of number and of a sum, which are fist taken from inner intuition, show a
constitutive function, insofar as they provide us with the general conditions of the
numbering of external objects. In this sense, Helmholtz’s argument can be taken as a
transcendental one.
Let us see how this argument leads to a general theory of measurement. Helmholtz
defines magnitudes as those objects, or attributes of objects, which allow a distinction into
greater, equal or smaller when compared with similar ones. This requires us to give a
physical interpretation of AI and AVII. Note that Helmholtz already analyzed physical
equality between spatial magnitudes in his reply to Land. This analysis is completed in
1887: if two such magnitudes are to be measured, it must be possible to assign a cardinal
number to them. Helmholtz makes it clear that AI provides us with a definition of equality:
as a definition, it does not have objective meaning itself. Measurement presupposes, in
addition, that two like objects, when interacting under suitable circumstances, allow the
observation of a particular outcome which does not occur as a rule between other pairs of
Space Can Be Transcendental Without the Axioms
123
similar objects. Helmholtz calls a procedure which enables us to accomplish such obser-
vation method of comparison. For example, the simplest geometrical structure for which a
magnitude is specifiable is the distance between a pair of points. The condition for
assigning a numerical value is that the points remain fixedly linked for at least the time of
our measurement. The method of comparison, in that case, is to verify whether pairs of
points can be brought into congruent coincidence. It may seem that metrical properties are
thereby induced from our experiences with solid bodies. Indeed, the ‘‘well-known’’ method
of coincidence admittedly requires time (Helmholtz 1977, 92). This reading would be
correct with regard to Helmholtz’s theory of local signs. However, his argument in the
context of the theory of measurement is a different one: the dynamic factor is mentioned
because measurement requires us to assign numerical coordinates to the points within a
system of reference which needs to remain identifiable in motion.
Note also that Helmholtz’s argument would be incomplete without a second step. Once
we have found a suitable method of comparison, the particular outcome of the interaction
between two like objects is supposed to remain unaltered if the two objects are interchanged.
Furthermore, if two such objects a and b are proved to be equal, and we know by previous
observation that a equals c, then b must also equal c. This procedure must be generalized, so
that objects which have proved to be equal are also mutually substitutable in any further
cases. To clarify this point, let us return to Helmholtz’s example. The concept of length
gives something more than that of distance. Whereas distance allows only a distinction of
equal and unequal, length also entails an opposition of greater and smaller. If two pairs of
points a, b and a, c, of differing distance, coincide at a and are placed in a straight line, so
that a portion of this line is common to both, then either b falls upon the line ac or c upon the
line ab. This fact leads to a more general consideration: once we know whether two
magnitudes are equal or unequal, in order to measure them in the second case, the greater
must be calculable as the sum of the smaller and their difference. That is to say, if AI is to
acquire objective meaning, it must be also given a physical interpretation of AVII or the
principle of homogeneity of the sum and the summands. Equality (Gleichheit) can be
attributed to two or more objects only if they are compared from some point of view. Their
comparison with regard to magnitude requires that equal or possibly unequal magnitudes be
homogeneous. This consideration is purely logical and shows that homogeneity (Gle-
ichartigkeit) is a more fundamental property than equality. In addition, Helmholtz gives the
following physical interpretation: it does not suffice to have a method of comparison
whatsoever; the issue of whether the result of connection remains the same, when parts are
exchanged, must be decided by the same method of comparison with which we ascertained
the equality of the parts to be exchanged. Given the homogeneity of the sum and the
summands, the remaining laws of addition can be applied to the composition of physical
magnitudes. Helmholtz’s theorem corresponds to the following proposition:
A physical method of connecting magnitudes alike in kind can be regarded as
addition, if the result of the connection—when likened as a magnitude of the same
kind—is not altered either by exchanging individual elements with each other, or by
exchanging terms of the connection with alike magnitudes of like kind. (Helmholtz
1977, 96)
In the following, Helmholtz shows that magnitudes which can be added are also
divisible. Every occurring magnitude can be regarded as a sum of a cardinal number of
equal parts to be chosen as units. This choice is conventional, and it might happen that the
magnitudes under consideration are not expressible without remainder. Nevertheless, also
in that case, the unit can be divided again in the usual manner, so that any degree of
F. Biagioli
123
precision can be attained. Complete precision is attainable only for rational proportions,
and the value of irrational ones can be enclosed between arbitrarily reducible limits. So we
can calculate all continuous differentiable functions of irrational magnitudes occurring in
geometry and physics, where Weierstrass’ everywhere continuous but nowhere differen-
tiable functions have not yet been encountered.
We already mentioned that Helmholtz overturns Kant’s part-whole opposition. Now his
analysis of measurement gives a specific reason to begin with the parts and their rela-
tionships to each other. In a well-known passage of the Transcendental Aesthetic, Kant
maintains that parts of space always belong to one and the same space (1787, 39–40). Their
homogeneity seems to be derived a priori from the infinite divisibility of space: there
would be no need to prove that the composition of spatial magnitudes follows the laws or
arithmetic. If Helmholtz’s problem is a real one, the Kantian theory provides no solution.
Helmholtz does not only require divisibility in its metrical aspect or into equal parts, but,
contrary to Kant’s argument, homogeneity implies infinite divisibility, and not vice versa
(see Darrigol 2003, 548–549; Hyder 2006, 33–36).
To conclude, the parallelism between space and time may help us to clarify Helmholtz’s
claim that space can be transcendental. In both cases, it is clear that the form of intuition is
not directly given. Such a form depends on an interaction between inner and outer
experience: on the one hand, the structure of time is described as a fact, whose origin
should be explained psychologically; on the other hand, this fact provides us with concepts,
such as that of number and of sum, which can be proved to determine our conception of
nature. Similarly, space entails the concept of fixed geometric structure. The axioms of
arithmetic, as well as those of geometry, presuppose a transcendental intuition. The axioms
are not transcendental because they provide us with definitions which, in order to be
applied to empirical objects, require a physical interpretation.
There is evidence that Helmholtz might have understood his parallelism in this way.
Indeed, in a celebrated passage of his lecture of 1870 he already noticed that the concept of
fixed geometric structure might be regarded as a transcendental one and the axioms of
geometry as propositions given a priori in transcendental intuition. He also noticed that, in
that case, the axioms of geometry would not be synthetic propositions in Kant’s sense: they
would only assert something which followed analytically from the definition of fixed
geometrical structures (Helmholtz 1977, 24–25). However, there is an important differ-
ence: in the case of time, Helmholtz does not distinguish between broader and narrower
specifications. Nevertheless, he distinguishes between time and arithmetical axioms
because, if the constitutive function of fundamental structures is to be proved, their laws
must be generalized progressively. Even though Helmholtz admits that irrational propor-
tions lack a numerical expression, he rejects the view that continuity is an intrinsic property
of some magnitudes. His point is that the extension of additive principles proceeds inde-
pendently of the supposition that there might be a difference in nature between extensive
and intensive magnitudes (Helmholtz 1977, 99). For the same reason, he does not treat
from the outset physical magnitudes as ones only composed out of units. Firstly, quantities
other than measurable magnitudes (e.g., coefficients) are used in physics. Secondly, and
more notably, the domain of validity of the laws of arithmetic should not be unnecessarily
restricted (Helmholtz 1977, 73).
These considerations may help us to explain Helmholtz’s distinction between tran-
scendental intuition and axioms also in the case of space. More precisely, since the
composition of spatial magnitudes is treated as a special case of measurement, Helmholtz’s
parallelism between space and time is better understood as an attempt to show how these
two concepts are related to each other. The claim that space can be transcendental without
Space Can Be Transcendental Without the Axioms
123
the axioms being so follows from a more general argument: Helmholtz deems transcen-
dental those structures which make measurement possible independently of the specific
nature of the objects to be measured. On the other hand, measurement requires principles
which are formulated for each measuring situation presently under consideration, and
which are coherently generalized to all known physical processes. These are not a priori
given because such extension depends on the advancement of empirical science.
My emphasis lies on the formal aspect of Helmholtz’s analysis of measurement, rather
than on the psychological one. I do not deny that there is such an aspect, but it seems to me
to be more problematic. In order to support my view, I shall benefit from the discussion of
Helmholtz’s theory of ordinal number in Ernst Cassirer’s Substanzbegriff und Funk-
tionsbegriff: Untersuchungen uber die Grundfragen der Erkenntniskritik (1910). For
Cassirer’s interpretation of the claim that space is transcendental, I shall refer to the fourth
volume of his Das Erkenntnisproblem in der Philosophie und Wissenschaft der neueren
Zeit (1957).
5 Cassirer’s Remarks on Helmholtz’s Transcendental Forms of Intuition
Let us first consider Cassirer’s remarks of 1910 on Helmholtz’s conception of number.
According to Cassirer, Helmholtz supports a kind of refined ‘‘copy’’ theory of knowledge
(Abbildtheorie): the numerical relations that we do not find directly in comparing external
objects acquire an objective meaning because we have previously developed a system of
signs which works as a substitute for them. Cassirer’s objection is that Helmholtz is not
able to explain how different signs could represent different things. From a psychological
point of view, signs would differ from each other because of their size and arrangement.
They were judged merely according to what they sensuously are, and not according to
what they intellectually mean. Judgments about numbers would be derived from judgments
about numerals. Cassirer writes:
It is only the ambiguity in the concept of symbol, only the circumstance that under it
can be understood, now the bare existence of a sensuous content, and now the ideal
object symbolized by the latter, which makes possible this reduction to the nomi-
nalistic schema. Leibniz, whose entire thought was concentrated upon the idea of a
‘‘universal characteristic,’’ clearly pointed out in opposition to the formalistic the-
ories of his time, the fact that is essential here. The ‘‘basis’’ of the truth lies, as he
says, never in the symbols but in the objective relations between ideas. If it were
otherwise, we would have to distinguish as many forms of truth as there are ways of
symbolizing. (Cassirer 1923, 43)
The nominalistic schema is untenable, because a meaningful use of symbolism
presupposes a logical basis or, as Leibniz puts it, objective relations between ideas. In
deeming such relations ‘‘objective’’, Cassirer overcomes Helmholtz’s opposition between
inner and outer experience. Cassirer reformulates Helmholtz’s Kant-oriented argument as
follows:
The consideration of the ‘‘cardinal numbers’’ […] occasions the discovery of no new
property and no new relation, which could not have been previously deduced from
the bare element of order. The only advantage is that the formulae developed by the
ordinal theory gain a wider application, since they can henceforth be read in two
different languages. (Cassirer 1923, 42)
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123
What is right in Helmholtz’s argument is that the theory of cardinal numbers does not
produce new objects, but rather realizes a new logical function: a finite sequence of unities
earlier regarded as a series can be regarded also as a whole—namely, a system, along with
the operations acting on it. This consideration must be completed by a logical analysis of
the system of natural numbers. Therefore, Cassirer uses Dedekind’s definition of number of
1888. Dedekind requires that the system of natural numbers be an infinite one, namely a set
which can be put into one-to-one correspondence with a proper subset of itself (e.g., the
even numbers). Given a fundamental element 1, a relation \, and an injective function ufrom any element to its successor, the series of natural numbers N can be generated by uN,
and their system can be defined as: {1 [ uN}.
Note that there is a specific assumption in Helmholtz’s axiomatization which is
unnecessary, namely AVI. And it is precisely the one which is supposed to be grounded in
the essence of the time sequence. The system of natural numbers can be treated inde-
pendently of the time sequence, because the structure analyzed by Dedekind is the more
general concept of a progression whatsoever. Dedekind shows that it suffices to introduce
‘‘\’’ as a transitive and asymmetric relation. Numbers are generated as those elements
which are in such a relation to each other. But Helmholtz’s connection with Kant is
misleading for another reason as well. Kant does not provide the foundations of arithmetic
in the Transcendental Aesthetic, and in the chapter on Schematism he writes:
The pure image of all magnitudes (quantorum) for outer sense is space; for all
objects of the senses in general, it is time. The pure schema of magnitude (quanti-
tatis), however, as a concept of the understanding, is number, which is a represen-
tation that summarizes the successive addition of one (homogeneous) unit to another.
Thus number is nothing other than the unity of the synthesis of the manifold of a
homogeneous intuition in general, because I generate time itself in the apprehension
of the intuition. (Kant 1787, 182)
Cassirer maintains that Dedekind’s conception of number is Kantian in spirit, because
every singular quantity is produced by addition of the preceding one in the series with the
unit. Helmholtz is right to point out that the cardinal aspect presupposes the ordinal one.
However, Cassirer prefers Dedekind’s definition of number because it makes it clear that
order is not intuitively given, but follows from the use of ‘‘u’’, which is an operation of the
thought. This way of thinking enables us to study the structural properties of numbers
independently of their specific nature. The set of numbers is determined and arguably
extended by the specification of the operations acting on it.
Cassirer maintains that the objects of geometry can be classified in a similar way. In
order to prove, in Euclidean geometry, that two figures are equal, we presuppose that they
can be brought into congruent coincidence without changes in shape and size during their
displacement. But this kind of congruence can also be defined as that relation between
spatial magnitudes that is invariant under a specific group of transformations, which is
called ‘‘the Euclidean group’’. This idea goes back to Sophus Lie and Felix Klein. The
general issue at stake in Klein’s Erlanger Programm of 1872 is, given a manifold and a
transformation group acting on it, to investigate those properties of figures on that manifold
that are invariant under all transformations of that group. The broader the group is, the
fewer properties are left unvaried. For example, the affine group is broader than the
Euclidean one, and does not make a difference between a circle and an ellipse, but only
between finite and infinite conic sections. From the point of view of the projective group,
all conic sections are classified as the same figure. And the group of continuous trans-
formations makes no difference between a cone-shaped figure and a cube.
Space Can Be Transcendental Without the Axioms
123
In the fourth volume of the Erkenntnisproblem, Cassirer maintains that Helmholtz
presupposes such a classification. The claim that space can be transcendental without the
axioms being so is interpreted by Cassirer as follows. On the one hand, the general
characteristics of space provide us with conditions of experience. In Cassirer’s interpre-
tation, they are three-dimensionality and constant curvature, and correspond to the pro-
jective group. Since we know by the above-mentioned classification that such group is
broader than the Euclidean group, Helmholtz is right to point out that the specific axi-
omatic structure of our space is not a priori determined and might be Euclidean or non-
Euclidean. On the other hand, he maintains that measurement also presupposes our
experiences with rigid bodies and the supposition of their free mobility, which is necessary
for spatial magnitudes to be compared by superposition. The problem with this specific
method of comparison is that it cannot prove that two such magnitudes are equal, unless
the Euclidean group is presupposed from the outset. As pointed out by the French math-
ematician Henri Poincare in La Science et l’Hypothese (1902), Helmholtz deems ‘‘rigid’’
those bodies whose properties are invariant under the transformations of the said group.
Then how are these transformations to be defined? If their definition presupposes the
existence of rigid bodies, Helmholtz’s reasoning is circular (Poincare 1902, 60).
Cassirer agrees with Poincare. Nevertheless, Cassirer emphasizes that Helmholtz, as in
the case of arithmetic, foreshadows a formal treatment of that subject-matter: the concept
he implicitly uses to define geometric objects and their properties is not that of space, but
that of group (Cassirer 1957, 50). This treatment shows that geometries are hypothetic-
deductive systems, whose application is a matter of empirical science. The issue of a
complete classification of hypotheses can be solved a priori, and must be distinguished
from that of a search for methodological criteria for choosing among them. Cassirer’s point
here is important. However, it might be objected that his characterization of Helmholtz’s
issue is wide enough to admit solutions which might be incompatible, such as Kantianism,
empiricism or conventionalism. In this regard, the parallelism with the philosophy of
arithmetic may help us because, in that case, Cassirer has a more specific argument for a
Kantian interpretation of Helmholtz’s theory of ordinal number: if singular quantities are to
be constructed, the structural properties of a numerical domain must be proved to have a
constitutive function. A similar consideration can be made with regard to Helmholtz’s
theory of measurement: the aspect in which his analysis admits a Kantian interpretation is
the formal one. In this regard, it is worth noting Helmholtz’s influence on the German
mathematician Otto Holder (1859–1937), who developed a formal analysis of measure-
ment and, at the same time, a synthetic conception of mathematics and geometry.
6 Helmholtz’s Influence on Holder
Let us first notice that Holder’s classification of the sciences differs from Helmholtz’s
classification because Holder maintains that arithmetic concepts admit a purely logical
construction. Arithmetic for Holder begins with definitions such as Grassmann’s formula,
which means that the sum of a number a and the successor b ? 1 of a number b is the
successor of the number a ? b in the series of integer numbers. By contrast, some geo-
metric objects must be given in intuition or experience. Their relations with each other can
be extended to all similar cases according to general principles to be postulated (i.e., the
axioms). Whereas geometric inferences are hypothetic-deductive, arithmetic inferences are
purely deductive and need no axioms.
F. Biagioli
123
Helmholtz’s parallelism between space and time, and their relationship to the axioms of
geometry and arithmetic, respectively, does not play any role here. Nevertheless, in a paper
of 1901, ‘‘Die Axiome der Quantitat und die Lehre vom Mass’’, Holder faces the same
issue as Helmholtz (1887)—namely, how to formulate general conditions for a numerical
representation of magnitudes. This inquiry does need axioms. And, at the beginning of the
paper, Holder appeals to Helmholtz on this point, in support of his own conception of the
axioms of quantity (Holder 1901, 1, note). These are the following propositions:
QI. Given any two quantities a and b, one and only one of the following is true: (1) a is
identical with b (a = b and b = a); (2) a is greater than b and b is smaller than
a (a [ b and b \ a); (3) b is greater than a and a is smaller than b (b [ a and a \ b).
QII. For every quantity there exist one that is smaller.
QIII. Any two quantities a and b, also in case that a = b, when added in a definite order,
give a univocally determined sum a ? b.
QIV. a ? b is greater than a and greater than b.
QV. If a [ b, then there exist two quantities, x and y, such that a ? x = b and
y ? a = b.
QVI. (a ? b) ? c = a ? (b ? c).
QVII. If all quantities are divided into two classes such that (1) each quantity belongs to
exactly one class, and (2) each quantity of the first class is smaller than any quantity of
the second class, then there exist a quantity n, such that every quantity n0\ n belongs to
the first class and every quantity n00[ n belongs to the second class (n may belong to
either, depending upon the case).
QVII is an equivalent formulation of Dedekind’s axiom of continuity, which is not
deducible from Helmholtz’s axioms. Dedekind calls cuts all partitions of rational numbers
in two such classes, and proves that each rational number corresponds to one and only one
cut. He introduces irrational numbers by requiring that each cut correspond to one and only
one number (Dedekind 1872, 13). It is noteworthy that, except for QVI (i.e., the associative
law of addition), Holder’s axiomatization is completely different from Helmholtz’s. So it is
not easy to see the connection with Helmholtz. It may be helpful to illustrate Holder’s
theorem first. Holder uses QVII to prove a theorem which is equivalent to the Archimedean
axiom:
Given two quantities a and b, and a \ b, then there exist an integer number n, such that
na [ b.
This theorem, along with the theory of irrational numbers, enables Holder to develop a
complete theory of proportions. Suppose that a and b are magnitudes of the same kind and
that lm is called a lower fraction in relation to their ratio a:b, if ma [lb; and an upper
fraction, if ma B lb. By the Archimedean principle, there exist both a positive integer m,
such that ma [ b, and a positive integer l, such that a \lb. Thus, in relation to the ratio
a:b, there exist both lower and upper fractions, and in every case the lower fractions are
less than the upper ones. It follows from Dedekind’s continuity that:
For every ratio of quantities a:b, i.e., for each two quantities which are given in a
determined order, there exist a well-determined cut, i.e., a determined number in the
general sense of the word. (Holder 1901, 23)
Holder’s theorem justifies Newton’s requirement that the ratio of quantities of the same
kind be expressed by positive real numbers: since order and operations with cuts can be
developed arithmetically, the laws of addition apply to all quantities that satisfy the axiom
of continuity and the remaining axioms of quantity.
Space Can Be Transcendental Without the Axioms
123
In the second part of the paper, Holder presents a model of a non-Archimedean con-
tinuum. This is the most original part of the paper. So it is surprising that Holder
emphasizes the importance of the said theorem above all. Nevertheless, his emphasis is
interesting in the present context because it shows Helmholtz’s influence (see also Michell
1993). Holder notices that Newton’s requirement entails a more specific one, which cor-
responds to Helmholtz’s requirement that the composition of physical magnitudes be
expressed by the arithmetical sum of equal parts of the same. Therefore, Holder uses
Dedekind’s (Archimedean) continuity, which is necessary for physical measurements.
Holder’s proof that divisibility can be derived as a consequence of continuity entails
Helmholtz’s proof that magnitudes that can be added can also be divided into equal parts.
But there is also a methodological aspect of Holder’s approach that shows Helmholtz’s
influence. Though Holder’s theory of quantity provides us only with formal conditions of
measurement, he agrees with Helmholtz that arithmetic should be related to the theory of
quantity. Therefore, Holder adopts a non-formalistic approach (1901, 2, note). This point is
strictly related to Holder’s considerations on geometry in the inaugural lecture he gave in
Leipzig in 1899, ‘‘Anschauung und Denken in der Geometrie’’. The text of the lecture was
published in 1900 with Holder’s additional notes. His proof that both divisibility and the
Archimedean property can be derived from the axiom of continuity is first presented in this
essay, for the following reason. We already mentioned that geometry, according to Holder,
presupposes some given concepts. One of such concepts is that of a spatial magnitude.
Holder’s proof shows that given concepts can be constructed so that arithmetical reasoning
plays a role in geometry and arguably in physics. His approach corresponds to Helmholtz’s
Kant-oriented argument that the laws of arithmetic can be progressively extended to non-
numerical domains. The structure of inner experience is thereby proved to have a con-
stitutive function.
There is evidence that Holder might have seen his argument as a development con-
sistent with the Kantian philosophy of mathematics. This point is made explicit in his book
on mathematical method (1924). There Holder adopts Kant’s terminology and calls those
concepts whose development does not require assumptions other than the operations of our
thought, such as the concept of coordination, series, number, and group, purely synthetic.
Those concepts of geometry and mechanics which require special assumptions in order to
be constructed are called hypothetically synthetic. Holder rejects formalism because, if
those thoughts which may lead to the introduction of new symbols were represented
through another symbolic computation, there would be an infinite regress. Holder’s view is
that symbols represent concepts, and these can be constructed (1924, 5–6). Holder’s
argument is drawn from Paul Natorp, Kantian philosopher and master of Cassirer in
Marburg (see Natorp 1910, 5). This common reference to Natorp might explain why
Cassirer developed an argument similar to Holder’s in 1910 already. However, Holder does
not mention Cassirer, and, arguably, was not aware of his argument.
As in Helmholtz, the use of Kant’s terminology and Kantian arguments does not prevent
Holder from supporting geometrical empiricism. In 1899 he summarizes the different
views on geometrical intuition as follows. Kant’s view is that a pure intuition endowed
with subjective laws makes experience possible. By contrast, according to nineteenth-
century views, such as those developed by Julius Baumann and Wilhelm Wundt, geo-
metrical intuition can be induced by experience. Both views look at intuition as a source of
geometry and as an indispensable tool for proof. Since an indispensable role of intuition in
geometrical proof is excluded by the deductive character of geometrical inferences, it
might seem that intuition is necessary at least to provide us with specific objects. However,
it can be replaced by purely deductive inferences. We have already seen Holder’s example:
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the concept of magnitude can be constructed. Holder uses his methodological analysis to
defend Helmholtz’s philosophy of geometry. Helmholtz is said to avoid any commitment
to a supposedly intuitive character of geometry: he explains basic geometric concepts ‘‘in a
more physical way’’ (Holder 2013, 16). In order to avoid a vicious circle, such explanation
should be based on observations that do not presuppose geometry. For example, approx-
imately rigid bodies should be distinguished from non-rigid ones because only the former
can be easily brought back to their initial position after displacements.5 Helmholtz’s free
mobility can be derived from the fact that parts of two such bodies can be brought to
coincidence and that such experience can be repeated at any time. So Helmholtz’s ‘‘facts’’
underlying geometry are better understood as ‘‘rules’’ for inferring facts in any further
cases. For Holder the formulation of such rules requires a kind of ‘‘complicated induction’’
preceding both deduction and induction properly speaking (2013, 31). In this regard there
is no disagreement with Kant. Holder writes: ‘‘any single fact of experience, if expressed
by means of concepts—and how could one want to express it otherwise—is the result of a
mental elaboration of experience’’ (2013, 28). He argues against Kant’s philosophy of
geometry as follows:
It will no longer appear contradictory that, though we use [the concept of space] in
some cases in order to interpret experience, we nevertheless consider it possible to
check this concept—whose adequateness is hypothetical—for correspondence with
experience in order to reshape the concept, if necessary, as we do with physical
concepts. (Holder 2013, 46)
This argument entails that the use of the concept of space presupposes a physical theory.
The empiricist theory requires that assumptions about the geometrical part of the theory
have the same degree of probability as other (optical or mechanical) parts of it.
Holder does not discuss Helmholtz’s claim that space can be transcendental without the
axioms being so. Nevertheless, his methodological considerations suggest the following
interpretation. In the context of pre-relativistic physics, space can be supposed to have a
curvature that approximately equals zero. At the same time, the conjecture that space is
generally flat must be rejected: since geometrical inferences are deductive, it would nec-
essarily follow from this conjecture that Euclidean axioms are true. But these axioms are
only hypothetically true, and non-Euclidean hypotheses might also be considered. So there
must be a broader characterization of space that includes Euclidean geometry as a special
case. Helmholtz’s inquiry on the foundations of geometry provides us with such a char-
acteristic—namely, constant curvature. This follows from free mobility, which is Helm-
holtz’s rule for the interpretation of spatial measurements.
7 Concluding Remarks
Helmholtz argues that space is a three-fold extended manifold of constant curvature in his
inquiries on the foundations of geometry of 1868 and 1870, and there is no evidence that he
changes his mind in 1878: he only emphasizes that these characteristics are broader than
the specific axiomatic structures that distinguish the three classical cases of such manifolds
from one another. I do not think that there can be any doubt about which characteristics are
5 Holder 1924, 371; 2013, 17. In 1924 Holder recalls that Poincare proposes a similar explanation: ‘‘Parmiles objets qui nous entourent, il y en a qui eprouvent frequemment des deplacements susceptibles d’etre […]corriges par un mouvement correlatif de notre propre corps, ce sont le corps solides’’ (Poincare 1902, 79).
Space Can Be Transcendental Without the Axioms
123
said to be general. So I addressed another question: does Helmholtz’s claim that space can
be transcendental without the axioms being so admit a Kantian interpretation? If this claim
means that the Kantian theory is valid only for intuitive space, then the general charac-
teristics of space might differ considerably from those established by Helmholtz, because
they might be indescribable qualities or qualities describable only as topological properties.
I argued against this reading because it overlooks the fact that Helmholtz’s considerations
in his discussion with Krause and Land are about spatial magnitudes and physical space in
the first place. One might object that Helmholtz does not distinguish between intuitive and
physical space. Nevertheless, my reconstruction of that discussion shows that Helmholtz’s
purpose is to defend the reliability of scientific measurements. The required argument for
the Kantian theory of space is that its characteristics can be proved to have a constitutive
function—namely, to provide us with general conditions of measurement. My interpreta-
tion is that Helmholtz deems space ‘‘transcendental’’ because such proof corresponds to a
transcendental argument in Kant’s sense, and I interpret Helmholtz’s proof that topogenous
factors influence the course of real processes as one such argument.
Helmholtz’s analysis of measurement is completed in his paper of 1887. So it is no
accident that, in that paper, Helmholtz resumes his considerations on transcendental intu-
itions and reformulates his argument as follows: the objectivity of measurements presup-
poses an interaction between inner and outer experience. This is because, on the one hand,
mathematical structures can only be defined independently of the objects we experience; on
the other hand, generally valid judgments about magnitudes presuppose a physical inter-
pretation of the same structures. Helmholtz apparently believes that his attempt to explain the
psychological origin of these structures is part of his argument. In this sense, he maintains that
geometrical axioms are related to space as arithmetical axioms are related to the form of
intuition of time. My point is that these considerations are not necessary for Helmholtz’s
argument, which can be interpreted as a Kantian one. The argument is that some structures
provide us with general conditions of experience. In addition to my own interpretation, I
considered two alternative formulations. The first is provided by Cassirer: Helmholtz’s
argument presupposes not so much his psychological explanation of the ordinal conception
of number, as the logical development of arithmetic. Similarly, congruence and other rela-
tions between spatial magnitudes should be analyzed group-theoretically. Following a
similar line of thought, Holder develops a more precise version of the argument—namely,
that magnitudes can be constructed as hypothetic-synthetic concepts. Holder’s argument
entails both the Kantian view that mathematics is synthetic and an empiricist conception of its
(arguably progressive) applicability, which is characteristic of Helmholtz’s approach.
Acknowledgments An earlier version of the paper was presented at the Max Planck Institute for theHistory of Science. I thank Vincenzo De Risi and his research team for their feedback on that occasion. Ialso wish to thank my colleague and friend Giovanni Gellera for stylistic suggestions. I am grateful to twoanonymous referees for their constructive criticisms.
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