| Euclid's parallel postulate, in its modern reformulation, | | | | (corresponding to spacetime) but geodesics in plane |
| holds that, on a plane, given a line and a point not on | | | | space (corresponding to space). |
| the line, only one line can be drawn through the point | | | | Intrinsic curvature, which was introduced by Riemann |
| parallel to the line. Gerolamo Saccheri (1667-1733) | | | | to explain how straight lines could have the |
| brilliantly attempted to prove this through a reductio | | | | properties associated with curvature without being |
| ad absurdum argument. There were two ways to | | | | curved in the ordinary sense, is now used to explain |
| contradict the postulate: space could have 1) no | | | | how something which is obviously curved, e.g. the |
| parallel lines (straight lines in a plane will always meet | | | | orbit of a planet, is really straight. Something has |
| if extended far enough), or 2) multiple straight lines | | | | gotten turned around. If the curvature of spacetime |
| through a given point parallel to a given line in the | | | | is evident to us in extrinsically curved lines in three |
| plane. These become non-Euclidean axioms. Saccheri | | | | dimensional space, then the form of the analogy |
| convincingly achieved his reductio for the first | | | | forces us to posit the "higher" or extrinsic dimension, |
| possibility with the innocent assumption that straight | | | | into which the straight lines are curved, as a spatial |
| lines are infinite [cf. Jeremy Gray, Ideas of Space | | | | one, not the temporal one. If three dimensional space |
| Euclidean, Non-Euclidean, and Relativistic, Oxford, | | | | is not extrinsically curved into time according to the |
| 1989; p. 64]. Later David Hilbert (1862-1953) would | | | | axiom of open ortho-curvature, then it must be time |
| point out that the same reductio proof could be | | | | that is extrinsically curved into the dimensions of |
| achieved by assuming that given three points on a | | | | space. In the model, where before the surface of |
| line only one can be between the other two [David | | | | the sphere was analogous to solid space, now the |
| Hilbert and S. Cohn-Vossen Geometry and the | | | | surface must be analogous to two dimensions of |
| Imagination (Anschauliche Geometrie--better | | | | space plus time, with the third dimension of space as |
| translated Intuitive Geometry), Chelsea Publishing | | | | that into which the geodesics of spacetime are |
| Company, 1952; p. 240]. For the second possibility, | | | | extrinsically curved. Switching the role of time |
| however, Saccheri did not achieve a good proof. And | | | | suddenly makes the model very non-intuitive, but it is |
| it was using just such an axiom that the first | | | | compelled by the feature of the model that the |
| complete non-Euclidean geometries were achieved by | | | | geodesic is on the surface of the sphere. It does not |
| Bolyai (1802-1860) and Lobachevskii (1792-1856). | | | | help the philosophical issue to eject the complications |
| If by "flat" we mean a plane of straight lines as | | | | of the axiom of open ortho-curvature and simply |
| understood by Euclid, then true non-Euclidean | | | | take the four dimensions of spacetime as satisfying |
| manifolds (i.e. areas, volumes, spacetimes, etc.), in | | | | hetero-curvature; for this loses sight of Kant's |
| order to really contradict Euclid, who was talking | | | | Antinomy of Space, which we hope to answer, and |
| about straight lines, would have to be flat. They could | | | | of the circumstance that even in Relativity the |
| not be curved. Straight lines would be Euclidean | | | | dimension of time is not exactly the same as the |
| straight, but the properties specified by non-Euclidean | | | | dimensions of space. That is the most intuitively |
| axioms would be satisfied. Nevertheless, since | | | | obvious in the "separation" formula: s2 = t2 - (x2 + |
| Bernhard Riemann (1826-1866), non-Euclidean | | | | y2 + z2)/c2. Here the Pythagorean formula for |
| manifolds are said to be "curved," and only Euclidean | | | | changes in spatial location, divided by the velocity of |
| space itself is called "flat." Contradiction #1 above | | | | light squared, is subtracted from the change in time |
| produces "positively" curved space ("spherical" or | | | | squared, to give the spacetime "separation" in units |
| "elliptical" geometry, first described by Riemann | | | | of time. Thus time is not treated as simply another |
| himself), and contradiction #2 "negatively" curved | | | | spatial dimension. Thus we must consider the |
| space ("hyperbolic" or Lobachevskian geometry). To | | | | differences between space and time, and the axiom |
| Euclid, this doubtlessly would seem to prove his point: | | | | of open ortho-curvature alone allows for this. |
| the parallel postulate is about straight lines, so using | | | | The result of attributing extrinsic curvature to time is |
| curved lines hardly produces an honest non-Euclidean | | | | also suggested by the peculiarity of using "curved |
| geometry. "Curvature" in this respect, however, is | | | | space" alone to explain gravity, as is common in |
| used in an unusual sense. Euclidean geodesics | | | | museums and textbooks around the world; for |
| "straight" and generalized straight lines "geodesics". | | | | curved space conjures up images of hills and valleys |
| "Flat" spaces of more than three dimensions may be | | | | through which moving objects describe curved paths. |
| called "Euclidean" because of their lack of curvature; | | | | However, those images presuppose motion, and |
| but this is an extension of geometry that would have | | | | motion is the very thing to be explained. Gravity |
| very much been news to Euclid, and I wish to retain | | | | does not just direct motion; it causes it. An object |
| the historical connection between "Euclidean" and | | | | passing by the earth is accelerated towards the |
| Euclid]. What "curvature" would have meant to Euclid | | | | earth and thereby acquires a velocity along a vector |
| is now "extrinsic" curvature: that for a line or a plane | | | | where it previously may have had no velocity at all. |
| or a space to be "curved" it must occupy a space of | | | | An object placed at rest with respect to the earth, |
| higher dimension, i.e. that a curved line requires a | | | | with no initial velocity in any direction, will be |
| plane, a curved plane requires a volume, a curved | | | | accelerated with a velocity towards the earth. If |
| volume requires some fourth dimension, etc. Now | | | | there are no "forces" acting on the body, as Einstein |
| "intrinsic" curvature has nothing to do with any higher | | | | says, then the only change that takes place is the |
| dimension. But how did this happen? Why did | | | | body's movement along the temporal axis; and if the |
| "curvature" come to have this unusual meaning? Why | | | | body is thereby displaced in space, it must be |
| should we confuse ourselves by saying that "intrinsic" | | | | displaced by its movement along that axis. The |
| straight lines, geodesics, in non-Euclidean spaces have | | | | temporal axis can displace the object if the axis is |
| curvature? This happened because non-Euclidean | | | | itself curved; so the curvature of spacetime in a |
| planes can be modeled as extrinsically curved | | | | gravitational field must result from the curvature of |
| surfaces within Euclidean space. Thus the surface of | | | | time, not of space. The extrinsic dimension of |
| a sphere is the classic model of a two-dimensional, | | | | ortho-curvature, into which the straight lines curve, is |
| positively curved Riemannian space; but while great | | | | a dimension of ordinary Euclidean space. This can be |
| circles are the straight lines (geodesics) according to | | | | intuitively shown, not so much in our non-Euclidean |
| the intrinsic properties of that surface, we see the | | | | models, but simply in a graph plotting time (t) against |
| surface as itself curved into the third dimension of | | | | one dimension of space (r). An accelerating body will |
| Euclidean space. A sphere is such a good | | | | describe a curved line that changes its coordinate in |
| representation of a non-Euclidean surface, and | | | | the r axis as its coordinate in the t axis changes. If |
| spherical trigonometry was so well developed at the | | | | the acceleration comes from spacetime itself, then |
| time, that it now is a little surprising that it was not | | | | the coordinate grid will itself be curved: the t axis |
| the basis of the first non-Euclidean geometry | | | | lines will curve, displacing themselves against the r |
| developed [cf. Gray ibid. p.171]. However, as noted, | | | | axis (spatial location), while the r axis lines will not |
| such a geometry does contradict other axioms that | | | | curve. The curvature of time itself is hidden from us |
| can easily be posited for geometry. Accepting | | | | because, indeed, we intersect only one point on the |
| positively curved spaces means that those axioms | | | | temporal axis. Consequently, how do we know we |
| must be rejected. Also, and more importantly, these | | | | are being accelerated by gravity? In free fall we are |
| models in Euclidean space are not always | | | | being displaced with space itself, and so we move |
| successful.with Lobachevskian space. A saddle shaped | | | | with our entire frame of reference and would not be |
| surface is a Lobachevskian space at the center of | | | | able to detect that locally. Indeed, we cannot. It is |
| the saddle, but a true Lobachevskian space does not | | | | Einstein's own "equivalence" principle of General |
| have a center. Other Lobachevskian models distort | | | | Relativity that we cannot tell the difference between |
| shapes and sizes. There is no representation of a | | | | free fall in a gravitational field and free floating in the |
| Lobachevskian surface that shares the virtues of a | | | | absence of a gravitational field. The motion induced in |
| sphere in having no center, no singularities (i.e. points | | | | us by the curvature of time is evident only because |
| that do not belong to the space), and in allowing | | | | we can observe distant objects that are not subject |
| figures to be moved around without distortion in | | | | to our local acceleration. When we are not in free fall, |
| shape or size. Three dimensional non-Euclidean spaces | | | | e.g. standing on the surface of the earth, we feel |
| of course cannot be modeled at all using Euclidean | | | | weight, just as according to the equivalence principle |
| space. | | | | when we are being accelerated by a force (e.g. a |
| This raises two questions: 1) what can we spatially | | | | rocket engine) in the absence of a gravitational field. |
| visualize? (a question of psychology) And 2) what | | | | These are indeed equivalent because in each case |
| can exist in reality? (a question of ontology). We | | | | we are moving relative to space according to our |
| cannot visualize any true Lobachevskian spaces or | | | | own frame of reference. When we are accelerated |
| any non-Euclidean spaces at all with more than two | | | | by a rocket we say that we move in the stationary |
| dimensions--or any spaces at all with more than three | | | | reference of external space; but when we are |
| dimensions. Also we can only visualize a positively | | | | accelerated standing on the surface of the earth, it is |
| curved surface if this is embedded in a Euclidean | | | | space itself that is displaced (by time) relative to us. |
| volume with an explicit extrinsic curvature. | | | | Either we move through space, or space moves |
| "Curvature" was thus a natural term for intrinsic | | | | through us. That is the experience of weight. |
| properties because there always was extrinsic | | | | A question remains about the global character of |
| curvature for any model that could be visualized. | | | | spacetime. Gravitational fields are locally positively |
| Why are there these limits on what we can visualize? | | | | curved, but Einstein and his philosophical successors |
| Why is our visual imagination confined to three | | | | evidently expected that spacetime as a whole would |
| Euclidean dimensions? It is now common to say that | | | | be positively curved, since a finite but unbounded |
| computer graphics are breaking through these | | | | universe is aesthetically more satisfying--and it |
| limitations, but such references are always to | | | | answers Kant's Antinomy of Space. Now, however, |
| projections of non-Euclidean or multi-dimensional | | | | the geometry of cosmological spacetime is usually |
| spaces onto two dimensional computer screens. Such | | | | tied to the dynamical fate of the expanding universe. |
| projections could be done, laboriously, long before | | | | Open, ever expanding universes, are regarded as |
| computers; but they never produced more, and can | | | | having Lobachevskian or even Euclidean geometry |
| produce no more, than flat Euclidean drawings of | | | | and only closed universes, headed for ultimate |
| curves. If such graphics are expected to alter our | | | | collapse, positive Riemannian curvature. The |
| minds so that we can see things differently, this is no | | | | observational evidence at the moment is for an open |
| more than a prediction, or a hope, not a fact. And | | | | universe, and "inflationary" models even have reasons |
| considering that non-Euclidean geometries have been | | | | to prefer a Euclidean over a Lobachevskian |
| conceived for almost two centuries, the | | | | geometry. These possibilities, however, introduce |
| transformation of our imagination seems a bit tardy, | | | | considerable trouble; for Euclidean and Lobachevskian |
| however much help computers can now give to it. | | | | spaces are both infinite, and it is a much different |
| Mathematicians don't have to worry about these | | | | proposition to say that an infinitely dense Big Bang |
| questions of visualization because visualization is not | | | | starts at a finite singularity, into which a finite |
| necessary for the analytic formulas that describe the | | | | positively curved space can be packed, than it is to |
| spaces. The formulas gave meaningfulness to | | | | say that an infinite homogeneous and isotropic |
| non-Euclidean geometry as common sense never | | | | universe, which must have begun infinite, starts from |
| could. | | | | an infinitely dense Big Bang. An infinitely dense |
| The Euclidean nature of our imagination led Kant to | | | | singularity can have a finite mass, but an extended |
| say that although the denial of the axioms of Euclid | | | | infinite density, even in a small finite region of space, |
| could be conceived without contradiction, our intuition | | | | cannot. |
| is limited by the form of space imposed by our own | | | | In a recent cosmological article in Scientific American, |
| minds on the world. While it is not uncommon to find | | | | "Textures and Cosmic Structure" (March 1992), the |
| claims that the very existence of non-Euclidean | | | | authors, Spergel and Turok, speak of the universe |
| geometry refutes Kant's theory, such a view fails to | | | | (they do not say "the observable universe") starting |
| take into account the meaning of the term | | | | from an "infinitesimally small point" or of the universe |
| "synthetic," which is that a synthetic proposition can | | | | being at one time the size of a "grapefruit," as |
| be denied without contradiction. Leonard Nelson | | | | though that would hold true for all model universes. |
| realized that Kant's theory implies a prediction of | | | | The infinite universes are not even considered, and |
| non-Euclidean geometry, not a denial of it, and that | | | | so the questions about density can be happily |
| the existence of non-Euclidean geometry vindicates | | | | ignored. The problem is compounded here because |
| Kant's claim that the axioms of geometry are | | | | there are actually two infinities competing with each |
| synthetic. The intelligibility of non-Euclidean geometry | | | | other: there is the infinite volume of space, and there |
| for Kantian theory is neither a psychological nor an | | | | is the infinite shrinkage, or compression, represented |
| ontological question, but simply a logical one--using | | | | by the big bang singularity. However much you shrink |
| Hume's criterion of possibility as logically consistent | | | | an infinite space, it is still infinite. On the other hand, |
| conceivability. Kant does not say non-Euclidean | | | | any finite region within infinite space, however large, |
| geometry is logically impossible, but that is only | | | | can be compressed to a single point at the big bang. |
| because he does not claim that any geometry is | | | | There is no conflict between the two infinities so |
| logically true; geometry in his view is synthetic, not | | | | long as you specify just what it is that you are |
| analytic. And Kant's belief that Euclidean geometry | | | | talking about. |
| was true, because our intuitions tell us so, seems to | | | | The problem here, however, is not visualization, it is |
| me to be either unintelligible or wrong. | | | | the hard logical truth that an infinite space remains |
| If we are unable to visualize non-Euclidean geometries | | | | infinite and that the big bang for an infinite space, |
| without using extrinsically curved lines, however, the | | | | although it can be described as a singularity in relation |
| intelligibility of Kant's theory is not hard to find. The | | | | to any finite region of space, cannot be a finite |
| sense of the truth of Euclidean geometry for Kant is | | | | singularity. |
| no more or less than the confidence that centuries | | | | Einstein himself introduced his Cosmological Constant |
| of geometers had in the parallel postulate, a | | | | to preserve a static universe, before Hubble's |
| confidence based on our very real spatial imagination. | | | | evidence of the red shift. He thus seems to have |
| If Kant's claim is "unintelligible," then Gray has not | | | | been thinking that a global positively curved |
| reflected on why everyone in history until the 19th | | | | geometry for spacetime was not necessarily tied to |
| century believed that the parallel postulate was true. | | | | some dynamical evolution of the universe. This is still |
| That is the psychological question, not the logical or | | | | a possibility. Three dimensional space can still be |
| ontological one. The sense of ancient confidence can | | | | conceived as having an inherent hetero-curvature |
| be recovered at any time today simply by trying to | | | | apart from the gravitational fate of the universe: |
| explain non-Euclidean geometry to undergraduate | | | | non-Euclidean without the need to regard time or |
| students who have never heard of it before. We | | | | anything else as a fourth dimension into which space |
| might say that attempts to prove the postulate | | | | needs to be extrinsically curved. This makes for a |
| show that people were uneasy about it; but the | | | | finite Big Bang regardless of the dynamical fate of |
| universal expectation was that the postulate was | | | | the universe, where that fate is tied to the effect of |
| really a theorem, and no one cashed in their unease | | | | the curvature of time, locally positively curved but |
| by trying to construct geometry with a denial of it. | | | | globally possibly Lobachevskian or Euclidean. However, |
| Saccheri denied it, but only because he was | | | | a theory of global hetero-curvature then stands |
| constructing reductio ad absurdum proofs. | | | | separate from the mathematical Relativistic theory of |
| Non-Euclidean geometry did not change our spatial | | | | gravity and becomes a theory in metaphysical |
| imagination, it only proved what Kant had already | | | | cosmology more than a theory in physical cosmology. |
| implicitly claimed: the synthetic and axiomatically | | | | A positively hetero-curved universe happens to suit |
| independent character of the first principles of | | | | the most commonly used cosmological model of all: |
| geometry. It could well be the case that Kant is right | | | | the inflating balloon, where motion is added to our |
| and that we will never be able to imagine the | | | | spherical model of non-Euclidean geometry. The |
| appearance of Lobachevskian or multi-dimensional | | | | surface of the balloon remains spherical regardless of |
| non-Euclidean spaces, or to model them without | | | | whether the balloon is blown up forever or whether |
| extrinsic curvature, however well we understand the | | | | it eventually is allowed to deflate. As a model the |
| analytic equations. This is purely a question of | | | | balloon therefore actually posits five dimensions, with |
| psychology and not at all one of logic, mathematics, | | | | the surface representing the three dimensions of |
| physics, or ontology. Mathematicians are free to | | | | space, time as the fourth, but as a fifth the third |
| ignore the limitations of our imagination, although they | | | | spatial dimension into which the surface is curved and |
| then run the risk of wandering so far from common | | | | through which the surface moves in time. A positively |
| sense that the frontiers of mathematics will never be | | | | hetero-curved universe, however, does not need |
| intelligible to even well-informed persons of general | | | | that fifth dimension. Space would be non-Euclidean |
| knowledge. Furthermore, since Kant believed that | | | | without higher dimensions, even while it moves along |
| space was a form imposed by our minds on the | | | | a temporal axis that is locally ortho-curved into an |
| world, he did not believe that space actually existed | | | | apparently hetero-curved spacetime because of the |
| apart from our experience. This leads us to the | | | | curvature of time. The balloon model therefore can |
| ontological question: what can exist in reality? | | | | represent a different kind of theory than it was |
| Non-Euclidean geometry was no more than a | | | | intended to, but a most suggestive one, where the |
| mathematical curiosity until Einstein applied it to | | | | global structure of the isotropic and homogeneous |
| physics. Now the whole issue seems much deeper | | | | universe may allow us to avoid an infinite Big Bang |
| and complex than it did in Kant's day, or Riemann's. If | | | | independent of the dynamical fate of the universe |
| our imagination is necessarily Euclidean, hard-wired into | | | | and fulfill the hope of the philosophers that Einstein |
| the brain as we might now think by analogy with | | | | answered Kant's Antinomy of Space. |
| computers, but Einstein found a way to apply | | | | §4. Conclusion |
| non-Euclidean geometry to the world, then we might | | | | Just because the math works doesn't mean that we |
| think that space does have a reality and a genuine | | | | understand what is happening in nature. Every |
| structure in the world however we are able to | | | | physical theory has a mathematical component and a |
| visually imagine it. | | | | conceptual component, but these two are often |
| In light of the distinction between intrinsic and | | | | confused. Many speak as though the mathematical |
| extrinsic curvature, we must consider all the kinds of | | | | component confers understanding, this even after |
| ontological axioms that will cover all the possible | | | | decades of the beautiful mathematics of quantum |
| spaces that Euclidean and non-Euclidean geometries | | | | mechanics obviously conferring little understanding. |
| can describe. If the limitations imposed by our | | | | The mathematics of Newton's theory of gravity |
| imaginations present us with features of real space, | | | | were beautiful and successful for two centuries, but |
| we would have to say that intrinsic curvature, | | | | it conferred no understanding about what gravity |
| despite being analytically independent of extrinsic | | | | was. Now we actually have two competing ways of |
| curvature, can only exist in conjunction with extrinsic | | | | understanding gravity, either through Einstein's |
| curvature and so with an embedding in higher | | | | geometrical method or through the interaction of |
| dimensions. This could be called the axiom of | | | | virtual particles in quantum mechanics. |
| ortho-curvature, according to which there would | | | | Nevertheless, there is often still a kind of deliberate |
| actually be no true non-Euclidean geometry, for | | | | know-nothing-ism that the mathematics is the |
| non-Euclidean geodesics would necessarily have | | | | explanation. It isn't. Instead, each theory contains a |
| extrinsic curvature and so would never be the actual | | | | conceptual interpretation that assigns meaning to its |
| straight lines that we need ex hypothese to | | | | mathematical expressions. In non-Euclidean geometry |
| contradict Euclid. The geometry of the surface of a | | | | and its application by Einstein, the most important |
| sphere would thus involve ortho-curvature because | | | | conceptual question is over the meaning of |
| its intrinsic straight lines, the great circles, must be | | | | "curvature" and the ontological status of the |
| simultaneously visualized and understood to be | | | | dimensions of space, time, or whatever. The most |
| curved lines in three dimensional Euclidean space. On | | | | important point is that the ontological status of the |
| the other hand, it may be that intrinsically curved | | | | dimensions involved with the distinction between |
| spaces can exist in reality without extrinsic curvature | | | | intrinsic and extrinsic curvature is a question entirely |
| and so without being embedded in a higher dimension. | | | | separate from the mathematics. It is also, to an |
| This could be called the axiom of hetero-curvature, | | | | extent, a question that is separate from |
| and it would make true non-Euclidean geometry | | | | science--since a scientific theory may work quite well |
| possible, since lines with non-Euclidean relations to | | | | without out needing to decide what all is going on |
| each other would be straight in the common meaning | | | | ontologically. Some realization of this, unfortunately, |
| of the term understood by Euclid or Kant. | | | | leads people more easily to the conclusion that |
| A further ontological distinction can be made. Even if | | | | science is conventionalistic or a social construction |
| the ortho-curvature axiom is true, a functionally | | | | than to the more difficult truth that much remains to |
| non-Euclidean geometry would be possible if a higher | | | | be understood about reality and that philosophical |
| dimension that allows for extrinsic curvature exists | | | | questions and perspectives are not always useless or |
| but is hidden from us. We must consider whether | | | | without meaning. Philosophy usually does a poor job |
| only the three dimensions of space exist or whether | | | | of preparing the way for science, but it never hurts |
| there may be additional dimensions which somehow | | | | to ask questions. The worst thing that can ever |
| we do not experience but which can produce an | | | | happen for philosophy, and for science, is that people |
| intrinsic curvature whose extrinsic properties cannot | | | | are so overawed by the conventional wisdom in |
| be visualized or imaginatively inspected by us. Thus | | | | areas where they feel inadequate (like math) that |
| we should distinguish between an axiom of closed | | | | they are actually afraid to ask questions that may |
| ortho-curvature, which says that three dimensional | | | | imply criticism, skepticism, or, heaven help them, |
| space is all there is, and an axiom of open | | | | ignorance. |
| ortho-curvature, which says that higher dimensions | | | | These observations about Einstein's Relativity are not |
| can exist. This gives us three possibilities: | | | | definitive answers to any questions; they are just an |
| That, with the axiom of closed ortho-curvature, | | | | attempt to ask the questions which have not been |
| there are no true non-Euclidean geometries (and no | | | | asked. Those questions become possible with a |
| spatial dimensions beyond three), but only | | | | clearer understanding of the separate logical, |
| pseudo-geometries consisting of curves in Euclidean | | | | mathematical, psychological, and ontological |
| space; | | | | components of the theory of non-Euclidean |
| That, with the axiom of open ortho-curvature, there | | | | geometry. The purpose, then, is to break ground, to |
| are no true non-Euclidean geometries but we may be | | | | open up the issues, and to stir up the complacency |
| faced with a functional non-Euclidean geometry in | | | | that is all too easy for philosophers when they think |
| Euclidean space whose external curvature is | | | | that somebody else is the expert and understands |
| concealed from us in dimensions (more than the | | | | things quite adequately. It is the philosopher's job to |
| three familiar spatial dimensions) not available to our | | | | question and inquire, not to accept somebody else's |
| inspection--this is an apparent hetero-curvature; | | | | word for somebody else's understanding. |
| And that, with the axiom of hetero-curvature, there | | | | Grappling with the causes of inertia, Newton imagined |
| are real non-Euclidean geometries whose intrinsic | | | | two buckets partially filled with water. The first |
| properties do not ontologically presuppose higher | | | | bucket is left still, and the surface of the water is |
| dimensions (whether or not there are more than | | | | flat. The second bucket is spun rapidly, and the |
| three spatial dimensions). | | | | surface of the water is concave. Why? |
| It is necessary to keep in mind that these axioms | | | | The naive answer is centrifugal force. But how does |
| are answers to questions concerning reality that | | | | the second bucket know it is spinning? In particular, |
| would be asked in physics or metaphysics and are | | | | what defines the inertial reference frame relative to |
| logically entirely separate from the status of | | | | which the second bucket spins and the first does |
| geometry in logic or mathematics or from our | | | | not? Berkeley [!] and Mach's answer was that all the |
| psychological powers of visual imagination. The | | | | matter [which Berkeley didn't believe in] in the |
| second axiom leaves open the question whether | | | | universe collectively provides the reference frame. |
| "hidden" dimensions are just hidden from our | | | | The first bucket is at rest relative to distance |
| perception or actually separate from our own | | | | galaxies, so its surface remains flat. The second |
| dimensional existence. With these ontological | | | | bucket spins relative to those galaxies, so its surface |
| alternatives in mind, we can now examine the | | | | is concave. If there were no distant galaxies, there |
| philosophical implications of Einstein's use of | | | | would be no reason to prefer one reference frame |
| non-Euclidean geometry. | | | | over the other. The surface in both buckets would |
| §3. Geometry in Einstein's Theory of Relativity | | | | have to remain flat, and therefore the water would |
| Einstein's general theory of relativity proposes that | | | | require no centripetal force to keep it rotating. In |
| the "force" of gravity actually results from an intrinsic | | | | short, there would be no inertia. Mach inferred that |
| curvature of spacetime, not from Newtonian | | | | the amount of inertia a body experiences is |
| action-at-a-distance or from a quantum mechanical | | | | proportional to the total amount of matter in the |
| exchange of virtual particles. If we view Einstein's | | | | universe. An infinite universe would cause infinite |
| philosophical project as an answer to Kant's Antinomy | | | | inertia. Nothing would ever move. [p. 92, comments |
| of Space--to explain how straight lines in space can | | | | added] |
| be finite but unbounded--the introduction of time | | | | Whatever the "naive" explanation may be, it is not |
| reckoned as the fourth dimension suggests that we | | | | the one used by Newton. The argument made by |
| may separate the intrinsic curvature of spacetime | | | | Luminet et al., Berkeley, and Mach is actually the |
| into curvature based on the relationship between | | | | argument originally made by Leibniz (and just recycled |
| space and time: we can think of Einstein's theory as | | | | by Berkeley, who believed in space less than in |
| one that satisfies the axiom of open ortho-curvature, | | | | matter) against Newton's idea that space was real. |
| with the peculiarity that it is indeed time, rather than | | | | For Newton, the rotating bucket was rotating in |
| a higher dimension of space, that is posited beyond | | | | relation to space itself. Evidently, it is now such |
| our familiar three spatial dimensions. This is a | | | | "conventional wisdom" that space itself provides no |
| metaphysically elegant theory, since is gives us the | | | | inertial frame of reference, since Einstein, that it |
| mathematical use of a higher dimension without the | | | | doesn't occur to anyone that the kind of reference it |
| need to postulate a real spatial dimension beyond our | | | | provides vis à vis rotation is rather different from |
| experience or our existence. Time is a dimension that | | | | what it fails to provide to establish absolute linear |
| is present to us only one spatial slice at a time, just | | | | motion. The argument that, in empty space, with no |
| as the third dimension is only intersected at one | | | | "distant galaxies," there would be no centrifugal force |
| (radial) point by the curved surface of a sphere in | | | | in the bucket and the water in one would be just as |
| our previous model of a positively curved space. | | | | flat as in the other is not a necessary conclusion, but |
| Our spherical model for non-Euclidean spacetime, | | | | only a theory. And not a theory easily tested without |
| however, is not quite right; for on the analogy, the | | | | an empty universe available. |
| intrinsic lines in space should be the geodesics and so | | | | On the other hand, the question can still be asked |
| should appear straight to us. They should appear | | | | how the bucket can "know" that the "distant |
| curved only from the perspective of the higher | | | | galaxies" are out there. There must be a physical |
| dimension, as the great circles on the sphere appear | | | | interaction for that (the range of gravity is infinite); |
| curved from our three dimensional perspective. That | | | | yet Einstein, again, said that no physical interaction |
| is not true in terms of astronomical space, where the | | | | can travel faster than the velocity of light, and in an |
| lines drawn by freefalling bodies in gravitational fields | | | | "inflationary" universe (which Mach didn't know about) |
| are most evidently curved to our three dimensional | | | | light can have reached us from only a finite part of |
| imaginations, even while they are understood to be | | | | the universe, even in an infinite universe. Thus the |
| geodesics only in terms of their form in the higher | | | | argument of Luminet et al. fails, for a infinite universe |
| dimension of spacetime. That is exactly the opposite | | | | would make for infinite inertia only if the whole |
| of the case in the model: Freefalling paths ("world | | | | universe could physically affect a location. If only a |
| lines") are geodesics in spacetime but extrinsically | | | | finite part of the universe, infinite or otherwise, |
| curved lines in space, while in the model great circles | | | | affects a location, then there will still only be finite |
| are extrinsically curved lines in solid space | | | | inertia. |