II On Relativity Theory
6 ON THE ORIGINS OF THE SPECIAL THEORY OF RELATIVITY
Continuity or Revolution?
INSTEINâS WORK in relativity is both typical and special. The rise of relativity theory shares many features with the rise of other important scientific theories in our time. But it is of course very much more. To find another work that illuminates as richly the relationship among physics, mathematics, and epistemology or between experiment and theory, or a work with the same range of scientific, philosophical, and general intellectual implications, one would have to go back to Newtonâs P
RINCIPIA. The theory of relativity was a key development both in physical science itself and in the philosophy of science. The reason for its dual significance is that Einsteinâs work provided not only a new principle of physics, but, as A. N. Whitehead said, âa principle, a procedure, and an explanation.â Accordingly, the commentaries on the historical origins of the theory of relativity have tended to fall into two classes, each having distinguished proponents: the one views it as a mutant, a sharp break with respect to the work of Einsteinâs immediate predecessors; the other regards it as an elaboration of then current work, for example, by H. A. Lorentz and Henri PoincarĂ©.
As we shall see, Einsteinâs innovation is understood best by superposing the two views, by seeing the discontinuity of his methodological orientation within a historically continuous scientific development.1 His own comments repeatedly stressed the aspect of continuity. Thus he wrote to Carl Seelig on March 11, 1952: âBetween the conception of the idea of this special relativity theory and the completion of the corresponding publication, there elapsed five or six weeks. But [he added rather cryptically] it would be hardly correct to consider this as a birth date, because earlier the arguments and building blocks were being prepared over a period of years, although without bringing about the fundamental decision.â2 One of our tasks in this chapter will be to get some idea of what happened during those years and whatâ or whoâhelped to bring about the âfundamental decision.â How large or small was the effect of the work of earlier physicists? Is there some strong influence that has so far been overlooked? Indeed, what are the sources for a study of the origins of the special theory of relativity?3 What was the state of science around 1905, what were the contributions which prepared the field for the RT, and what did Einstein know about them? To what extent was this work consciously based on that of Lorentz and PoincarĂ©? What was the early reception of the RT among scientists? What may we say about the style of Einsteinâs work? What, if anything, in the origins and content of the RT is typical of other theories that have had great impact on science? And even, what methodological principles for research in the history of science emerge from this case?
Continuity in Einsteinâs Work
When one studies Einsteinâs early relativity papers and correspondence in the larger contextual setting of his other scientific papers, particularly those on the quantum theory of light and on Brownian motion, which also were written and published in 1905, one is struck by two crucial points. Although the three epochal papers of 1905â sent to the ANNALEN DER PHYSIK at intervals of less than eight weeksâ seem to be in entirely different fields, closer study shows that they arose in fact from the same general problem, namely, the fluctuations in the pressure of radiation. In 1905, as Einstein later wrote to von Laue,4 he had already known that Maxwellâs theory leads to the wrong prediction of the motion of a delicately suspended mirror âin a Planckian radiation cavity.â This connects on the one hand with the consideration of Brownian motion as well as with the quantum structure of radiation, and on the other hand with Einsteinâs more general reconsideration of âthe electromagnetic foundations of physicsâ itself.5
One also finds that the style of the three papers is essentially the same and reveals what is typical of Einsteinâs work at that time. Each begins with a statement of formal asymmetries or other incongruities of a predominantly aesthetic nature (rather than, for example, a puzzle posed by unexplained experimental facts), then proposes a principleâpreferably one of the generality of, say, the Second Law of Thermodynamics, to cite Einsteinâs repeated analogyâwhich removes the asymmetries as one of the deduced consequences, and at the end produces one or more experimentally verifiable predictions.
Einsteinâs first paper on the quantum theory of light opens in a typical manner: âThere exists a radical formal difference between the theoretical representations which physicists have constructed for themselves concerning gases and other ponderable bodies on the one hand, and Maxwellâs theory of electromagnetic processes in so-called empty space on the other hand.â6 The significant starting point is a formalistic difference between theoretical representations in two fields of physics which, to most physicists, were so widely separated that no such comparison would have invited itself and therefore no such discrepancy would be noted. The discrepancy Einstein points out is between the discontinuous or discrete character of particles and of their energy on one hand, and the continuous nature of functions referring to electromagnetic events and of the energy per unit area in an expanding wave front on the other hand. The discussion of the photoelectric effect, for which this paper is mostly remembered, occurs toward the end, in a little over two pages out of the total sixteen. The prescription for obtaining an experimental verification of his point of view is given in a single, typically succinct Einsteinian sentence (straight-line relation with constant slope between frequency of light and stopping potential for all electrode materials).
In his second paper published in 1905,7 Einstein points out in the second paragraph that the range of application of classical thermodynamics may be discontinuous even in volumes large enough to be microscopically observable. He ends with the equation giving Avogadroâs number in terms of observables in the study of particle motion, and with the one-sentence exhortation: âMay some investigator soon succeed in deciding the question which has been raised here, and which is important for the theory of heat!â Significantly, Einstein reported the following year8 that only after the publication of this paper was his attention drawn to the experimental identification, as long ago as 1888, of Brownian motion with the effect whose existence he had deduced as a necessity from the kinetic-molecular theory. In his Autobiographical Notes he repeats that he did the work of 1905 âwithout knowing that observations concerning Brownian motion were already long familiar.â9
The third paper of 190510 is, of course, Einsteinâs first paper on the RT. He begins again by drawing attention to a formal asymmetry, that is, in the description of currents generated during relative motion between magnets and conductors. The paper does not invoke by name any of the several well-known experimental difficultiesâand the Michelson and Michelson-Morley experiments are not even mentioned when the opportunity arises to show in what manner the RT accounts for them. At the end, Einstein briefly mentions here, too, specific predictions of possible experiments (giving the equation âaccording to which the electron must move in conformity with the theory presented hereâ).11
âRevolutionâ as Return to Classical Purity
The study of the three papers together reveals the extent to which Einsteinâs RT represents an attempt to solve problems by the postulation of appropriate fundamental hypotheses and to restrict those hypotheses to the most general kind and the smallest number possibleâa goal on which Einstein often insisted.12 In the 1905 paper on the RT, he makes, in addition to the two âconjecturesâ raised to âpostulatesâ (that is, of relativity and of the constancy of light velocity) only four other assumptions: one of the isotropy and homogeneity of space, the others concerning three logical properties of the definition of synchronization of watches. In contrast, H. A. Lorentzâs great paper13 that appeared a year before Einsteinâs publication and typified the best work in physics of its timeâa paper which Lorentz declared to be based on âfundamental assumptionsâ rather than on âspecial hypothesesââcontained in fact eleven ad hoc hypotheses: restriction to small ratios of velocities v to light velocity c, postulation a priori of the transformation equations (rather than their derivation from other postulates), assumption of a stationary ether, assumption that the stationary electron is round, that its charge is uniformly distributed, that all mass is electromagnetic, that the moving electron changes one of its dimensions precisely in the ratio of (1âv2/c2)1/2 to 1, that forces between uncharged particles and between a charged and uncharged particle have the same transformation properties as electrostatic forces in the electrostatic system, that all charges in atoms are in a certain number of separate âelectrons,â that each of these is acted on only by others in the same atom, and that atoms in motion as a whole deform as electrons themselves do. It is for these reasons that Einstein later maintained that the RT grew out of the Maxwell-Lorentz theory of electrodynamics âas an amazingly simple summary and generalization of hypotheses which previously have been independent of one another.â14
If one has studied the development of scientific theories, one notes here a familiar theme: the so-called revolution which Einstein is commonly said to have introduced into the physics in 1905 turns out to be at bottom an effort to return to a classical purity. Not only is this a key to a new evaluation of Einsteinâs contribution, it indicates a fairly general characteristic of great scientific ârevolutions.â Indeed, although it is usually stressed that Einstein challenged Newtonian physics in fundamental ways, the equally correct but neglected point is the number of methodological correspondences with earlier classics, for example, with the PRINCIPIA.
Here a listing of some main parallels between the two works must suffice: the early postulation of general principles which in themselves do not spring directly from experience; the limitation to a few basic hypotheses;15 the exceptional attention to epistemological rules in the body of a scientific work; the philosophical eclecticism of the author; his ability to dispense with mechanistic models in a science which in each case was dominated at the time by such models;16 the small number of specific experimental predictions; and the fact that the most gripping effect of the work is its exhibition of a new point of view.
The central problem, moreover, is the same in both works: the nature of space and time and what follows from it for physics. Here, the basic attitudes have in both cases more in common than appears at first reading. That Newtonâs absolute space and absolute time were not meaningful concepts in the sense of laboratory operations was, of course, not the original discovery of Mach; rather, it was freely acknowledged by Newton himself. But Einstein was also quite explicit that in replacing absolute Newtonian space and time with an infinite ensemble of rigid meter sticks and ideal clocks he was not proposing a laboratory-operational definition. He stated that it could be realized only to some degree, ânot even with arbitrary approximation,â and that the fundamental role of the whole conception, both on factual and on logical grounds, âcan be attacked with a certain right.â17 Thus the RT merely shifted the locus of space time from the sensorium of Newtonâs God to the sensorium of Einsteinâs abstract Gedanken-experimenterâas it were, the final secularization of physics. We shall return to this point below.18
Whittakerâs Accounts of the Origins of Einsteinâs Work
Not all scholars agree with this view of Einsteinâs originality within an old tradition. Some exaggerate its discontinuity and insist on a ârevolution.â Someâfor ideological and other reasonsâgo the opposite way. To illustrate this last point concretely, I turn to a question on which a dispute has been active: namely, to what extent Einsteinâs work was not only anticipated by but even specifically based on published work by other contemporary physicists. Particularly revealing is an essay published in 1955 by Sir Edmund Whittaker.19 Whittakerâs commitment to the nineteenth-century tradition of physics and to the ether theory was illustrated earlier in his well-known book, A HISTORY OF THE THEORIES OF AETHER AND ELECTRICITY,20and also by his excellent contributions in the field of classical mechanics. Moreover, in the second volume of the HISTORY, completed in 1953, which carr...