There were major transformations worth calling revolutionary, but not one event that created a single modern method everywhere at once. The term Scientific Revolution is useful if it identifies a connected set of changes in problems, instruments, explanations and intellectual authority. It becomes misleading when it substitutes a sudden victory of reason over an undifferentiated earlier ignorance for an explanation of those changes.
One substantial transformation concerned the relation between mathematics and physical explanation. Newton's laws of motion and Newton's law of universal gravitation connected terrestrial and celestial motion within the same quantitative framework. The importance of this achievement was not simply a more accurate table of planetary positions. Kepler's laws of planetary motion could become consequences of a dynamical account, while deviations from simple planetary paths became problems of interacting bodies. A theory could now generate further quantitative questions about the Moon, comets and the figure of the Earth. This was a change in what an adequate physical explanation might accomplish.[ref]
The Mathematical Principles of Natural Philosophy by Isaac Newton (1846 edition). Laws of Motion and Book III, propositions 1–8; distinguish the later English edition from the original 1687 publication
A second transformation concerned evidence. In 1610 Galileo Galilei presented a telescope as a means of investigating objects that ordinary unaided observation could not resolve. The changing appearances of bodies near Jupiter supported the existence of satellites accompanying that planet; the disposition of light and shadow on the Moon supported an irregular surface. These observations challenged the claim that all celestial bodies displayed a uniquely perfect constitution. They also required arguments about the reliability of the instrument and the interpretation of what appeared through it.[ref]
Sidereus Nuncius by Galileo Galilei. lunar observations and the successive observations of Jupiter's companions
They did not, by themselves, uniquely establish the Earth's motion: a system in which planets circled the Sun while the Sun circled the Earth could accommodate satellites of Jupiter. Distinguishing a result from the stronger worldview later associated with it prevents a misleading account of instant conversion.Programmes for producing knowledge also changed. Francis Bacon criticized premature generalization and proposed organized movement between observations, experiments and increasingly general claims. His comparison of the ant, spider and bee rejected both the mere accumulation of facts and reasoning spun entirely from the mind. The ambition was a cooperative, productive investigation of nature, with procedures for correcting habitual intellectual mistakes.[ref] This programme is evidence for a methodological reform movement, not proof that every successful seventeenth-century investigator followed one Baconian algorithm.
The discontinuities were nevertheless built from inherited resources. Aristotelian natural philosophy already asked about causes and systematic knowledge; astronomy had long depended on demanding mathematical and observational practices. Instrument making depended on craft skills. Galileo Galilei's discovery claims also depended on patronage: his dedication and naming of the newly observed bodies in Sidereus Nuncius by Galileo Galilei explicitly linked celestial investigation to the Medici court. A socially situated discovery need not be scientifically false, but its circulation cannot be explained solely by the logical content of a theory.[ref]
Nor did change imply a uniform retreat of religion. The General Scholium by Isaac Newton coupled the rejection of Cartesian vortices with an argument about divine government. That addition first appeared in 1713, so it should not be silently placed in the 1687 first edition. Its combination of physical argument and theology nevertheless rules out a simple narrative in which successful mathematical physics necessarily became religiously indifferent.[ref]
General Scholium by Isaac Newton. opening discussion of vortices and subsequent discussion of divine dominion; linked English translation published in 1729
Steven Shapin's challenge to a single, self-evident Scientific Revolution is therefore a useful warning about the historian's category, rather than a reason to deny every substantial change.[ref]
The Scientific Revolution by Steven Shapin. Introduction: the problem of treating diverse historical transformations as one event
The strongest qualified verdict is that a revolutionary reorganization occurred in several influential European traditions, especially mathematical natural philosophy and instrumental observation. Its chronology, geographical reach and relation to other disciplines must be demonstrated separately. The category explains something only when those differences remain visible.Kepler's laws of planetary motion state that, in the relative two-body description, bound trajectories are ellipses with the attracting body at a focus, the radius vector sweeps equal areas in equal times, and the square of the period is proportional to the cube of the semimajor axis for a fixed total mass. Their Newtonian derivation is especially informative. With relative coordinate and , the inverse-square acceleration is . Its zero torque conserves , fixing a plane and the areal velocity .
For , the orbit equation is as a function of polar angle. ThereforeBound negative-energy motion has and semilatus rectum . Dividing ellipse area by areal velocity givesFor a planet much lighter than its star, replace by . Zero-energy and positive-energy encounters are parabolic and hyperbolic rather than periodic ellipses. Perturbations from other bodies and departures from point-mass Newtonian gravity can precess or otherwise modify the orbit; Kepler's laws are a two-body approximation, not an exact rule for every observed planetary path.
- Kepler's first law: a bound planetary orbit is an ellipse with the central attracting body at one focus.
- Kepler's second law: the line from that focus to the planet sweeps equal areas in equal times, equivalent to constant areal velocity.
- Kepler's third law: the squared orbital period is proportional to the cube of the semi-major axis, when the orbiting mass is negligible.
The first law includes a circular Kepler orbit as a special case. The third-law constant is the same for bodies orbiting the same dominant mass.
For two isolated point masses, introduce total mass , reduced mass and relative separation . The relative acceleration is . Conserved specific angular momentum fixes a plane and a constant areal velocity . The specific orbital energy isFor , the trajectory is a conic:Negative energy gives an ellipse, including the circular limit ; zero energy gives a parabola; positive energy gives a hyperbola. Bound ellipses obey andThus Kepler's laws of planetary motion follow from angular momentum conservation and the inverse-square force. For a circular orbit of radius , , while escape from that radius requires . Energy determines whether the orbit is bound; angular momentum also determines its shape. These ideal results neglect extended-body perturbations, drag and relativistic corrections.