To Letters Editor Physics Today. Re: Did Newton Need Hooke's Program to Divine Planetary Motions? Physics Today, Sept. 2003 This year marks the anniversary of the death of Robert Hooke one of the greatest scientist of the 17th century, who is currently being rehabilitated from three centuries of oblivion. It might be expected that by now his seminal influence on Newton's development of the theory of planetary motion would be well understood, if not by physicists then at least by historians and philosophers of science, who have argued about this subject during the past century. But this is not the case as one finds, for example, in reading the recent book by Ofer Gal, subtitled "Hooke, Newton and the 'Compounding of the Celestiall Motions of the Planetts'", which was reviewed in this journal by George E. Smith. In order to appreciate the importance of Hooke's contribution, to planetary motion, which he communicated to Newton during a correspondence in the Fall of 1679, it is necessary to understand not only Hooke's views, described at length in Gal's book, but also Newton's own understanding of this subject at the time of this correspondence. Smith repeats the usual comment by historians of science that " before his correspondence with Hooke, Newton (along with many others) thought of the planetary orbits as an equilibrium between 'an endeavor to recede from the center' associated with circular motion and some other mechanism". But this explanation is inadequate and, moreover, it is not the one offered by Gal, who makes the bizarre claim that before Hooke's intervention, Newton represented "force-driven motion by straight lines or open curves, while reserving the closed orbits to represent force-free motion" [1]. Newton's Dec. 13, 1679 letter to Hooke shows that this claim is incorrect [2]. Unlike his contemporaries, Newton had developed by that time a sophisticated mathematical theory of orbital motion, as is evident in his description of orbital curves under the action of various central forces. In this letter, Newton included even the special case of a $1/r^3$ force (usually not treated in physics textbooks) which leads to an orbit that rotates towards the center " by an infinite number of spiral revolutions" [2], but this remarkable result has been universally ignored by historians of science. There is considerable evidence that Newton's theory of orbital motion was based on the mathematical description of curvature which he, and independently Huygens, had developed earlier [3]. However, an essential ingredient was missing in Newton's approach, which was based on a decomposition of motion along the tangent and the normal to the orbital curve. Newton was not yet aware that for central forces, angular momentum is conserved, justifying Kepler's second law (area law). Newton later admitted that "in the year 1679, in answer to a letter to Dr. Hook..I found now that whatsoever was the law of the forces which kept the Planets in their Orbs, the areas described by the Radius drawn from them to the Sun would be proportional to the times in which they were described..." [4]. What Hooke had suggested in 1679 to Newton is that orbital motion could be decomposed into "a direct [inertial] motion by the tangent, and an attractive motion [radial] towards the central body" For a central impulsive force acting at periodic intervals, this decomposition of motion makes the conservation of angular momentum manifest, as Newton subsequently showed in De Motu, his first draft of the Principia. This proof became a cornerstone of the Principia, as Proposition 1 in Book 1, because it permitted him to completely geometrize orbital dynamics by replacing the time variable by the area swept by the radius drawn to the center of force [5]. Contrary to the argument by Gal, that Hooke "had a scientific style radically different from Newton's", and Smith's assertion that there exists a "monumental contrast" between their approaches to science, in fact both Hooke and Newton had a very similar and quite modern approach to the understanding of natural phenomena based on observations and experiments. For example, Hooke reached his views of planetary motion by an analysis of the motion of a conical pendulum, as he explained in considerable detail in a lecture given at the Royal Society on May 23, 1666 [4][6]. The essential difference is that Newton was able to translate physical concepts into mathematical form and solve the resulting equations, while Hooke lacked far behind Newton in this ability. The physical basis for planetary motion was not "divined" (coming from God) by Newton, but should be recognized as a remarkable joint scientific achievement of Newton and Hooke [7]. References: [1] O. Gal, "Meanest Foundations and Nobler Superstructures, Hooke, Newton and the 'Compounding of the Celestiall Motions of the Planetts'" (Kluwer Academic Publishers 2003) p. 184. Gal also makes the unprecedent claim that the "novelty of {\it De Motu} [Newton's first draft of the Principia written 5 years after his correspondence with Hooke] thus encapsulated the willingness [of Newton] to represent forced motions by closed curves" p. 188, {2} M. Nauenberg, "Newton's Early Computational Method for Dynamics" Archives for History of Exact Sciences, 46, (1994) 221-251 [3] J.B. Brackenridge and M. Nauenberg, "Curvature in Newton's Dynamics" in The Cambridge Companion to Newton, edited by I.B. Cohen and G.E. Smith (Cambridge Univ. Press 2003) pp. 85-137 [4] M. Nauenberg, "Hooke, orbital motion, and Newton's Principia" American Journal of Physics 62, (1994) 331-350 [5] M. Nauenberg, "Kepler's area law in the Principia: Filling in some details in Newton's proof of Proposition 1" Historia Mathematica v. 30 (to be published) [6] In his review, Smith states "that the great value of Gal's book lies in his analysis of how Hooke arrived at this conception through his research in optics". But in his Royal Society lecture Hooke explicitly rejected the optical analogy that the "bending" of the orbital motion of planets into a curve is caused by the "unequal density of the medium". [7] M. Nauenberg, " Robert Hooke's seminal contribution to orbital dynamics" Invited paper presented at a conference at the Royal Society in London, July 7-8,2003, to mark the tercentenary of the death of Robert Hooke (1635-1703) (to be published)