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History of physics
History of physics
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Physics is a branch of science in which the primary objects of study are matter and energy. These topics were discussed across many cultures in ancient times by philosophers, but they had no means to distinguish causes of natural phenomena from superstitions.

The Scientific Revolution of the 17th century, especially the discovery of the law of gravity, began a process of knowledge accumulation and specialization that gave rise to the field of physics.

Mathematical advances of the 18th century gave rise to classical mechanics, and the increased used of the experimental method led to new understanding of thermodynamics.

In the 19th century, the basic laws of electromagnetism and statistical mechanics were discovered.

At the beginning of the 20th century, physics was transformed by the discoveries of quantum mechanics, relativity, and atomic theory.

Physics today may be divided loosely into classical physics and modern physics.

Ancient history

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Elements of what became physics were drawn primarily from the fields of astronomy, optics, and mechanics, which were methodologically united through the study of geometry. These mathematical disciplines began in antiquity with the Babylonians and with Hellenistic writers such as Archimedes and Ptolemy. Ancient philosophy, meanwhile, included what was called "Physics".

Greek concept

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The move towards a rational understanding of nature began at least since the Archaic period in Greece (650–480 BCE) with the Pre-Socratic philosophers. The philosopher Thales of Miletus (7th and 6th centuries BCE), dubbed "the Father of Science" for refusing to accept various supernatural, religious or mythological explanations for natural phenomena, proclaimed that every event had a natural cause.[1] Thales also made advancements in 580 BCE by suggesting that water is the basic element, experimenting with the attraction between magnets and rubbed amber and formulating the first recorded cosmologies. Anaximander, developer of a proto-evolutionary theory, disputed Thales' ideas and proposed that rather than water, a substance called apeiron was the building block of all matter. Around 500 BCE, Heraclitus proposed that the only basic law governing the Universe was the principle of change and that nothing remains in the same state indefinitely. He, along with his contemporary Parmenides were among the first scholars to contemplate on the role of time in the universe, a key concept that is still an issue in modern physics.

Aristotle (384–322 BCE)

During the classical period in Greece (6th, 5th and 4th centuries BCE) and in Hellenistic times, natural philosophy developed into a field of study. Aristotle (Greek: Ἀριστοτέλης, Aristotélēs) (384–322 BCE), a student of Plato, promoted the concept that observation of physical phenomena could ultimately lead to the discovery of the natural laws governing them.[citation needed] Aristotle's writings cover physics, metaphysics, poetry, theater, music, logic, rhetoric, linguistics, politics, government, ethics, biology and zoology. He wrote the first work which refers to that line of study as "Physics" – in the 4th century BCE, Aristotle founded the system known as Aristotelian physics. He attempted to explain ideas such as motion (and gravity) with the theory of four elements. Aristotle believed that all matter was made of aether, or some combination of four elements: earth, water, air, and fire. According to Aristotle, these four terrestrial elements are capable of inter-transformation and move toward their natural place, so a stone falls downward toward the center of the cosmos, but flames rise upward toward the circumference. Eventually, Aristotelian physics became popular for many centuries in Europe, informing the scientific and scholastic developments of the Middle Ages. It remained the mainstream scientific paradigm in Europe until the time of Galileo Galilei and Isaac Newton.

Early in Classical Greece, knowledge that the Earth is spherical ("round") was common. Around 240 BCE, as the result of a seminal experiment, Eratosthenes (276–194 BCE) accurately estimated its circumference. In contrast to Aristotle's geocentric views, Aristarchus of Samos (Greek: Ἀρίσταρχος; c. 310 – c. 230 BCE) presented an explicit argument for a heliocentric model of the Solar System, i.e. for placing the Sun, not the Earth, at its centre. Seleucus of Seleucia, a follower of Aristarchus' heliocentric theory, stated that the Earth rotated around its own axis, which, in turn, revolved around the Sun. Though the arguments he used were lost, Plutarch stated that Seleucus was the first to prove the heliocentric system through reasoning.

The ancient Greek mathematician Archimedes, developer of ideas regarding fluid mechanics and buoyancy.

In the 3rd century BCE, the Greek mathematician Archimedes of Syracuse Greek: Ἀρχιμήδης (287–212 BCE) – generally considered to be the greatest mathematician of antiquity and one of the greatest of all time – laid the foundations of hydrostatics, statics and calculated the underlying mathematics of the lever. A scientist of classical antiquity, Archimedes also developed elaborate systems of pulleys to move large objects with a minimum of effort. The Archimedes' screw underpins modern hydroengineering, and his machines of war helped to hold back the armies of Rome in the First Punic War. Archimedes even tore apart the arguments of Aristotle and his metaphysics, pointing out that it was impossible to separate mathematics and nature and proved it by converting mathematical theories into practical inventions. Furthermore, in his work On Floating Bodies, around 250 BCE, Archimedes developed the law of buoyancy, also known as Archimedes' principle. In mathematics, Archimedes used the method of exhaustion to calculate the area under the arc of a parabola with the summation of an infinite series, and gave a remarkably accurate approximation of pi. He also defined the spiral bearing his name, formulae for the volumes of surfaces of revolution and an ingenious system for expressing very large numbers. He also developed the principles of equilibrium states and centers of gravity, ideas that would influence future scholars like Galileo, and Newton.

Hipparchus (190–120 BCE), focusing on astronomy and mathematics, used sophisticated geometrical techniques to map the motion of the stars and planets, even predicting the times that Solar eclipses would happen. He added calculations of the distance of the Sun and Moon from the Earth, based upon his improvements to the observational instruments used at that time. Another of the early physicists was Ptolemy (90–168 CE) during the time of the Roman Empire. Ptolemy was the author of several scientific treatises, at least three of which were of continuing importance to later Islamic and European science. The first is the astronomical treatise now known as the Almagest (in Greek, Ἡ Μεγάλη Σύνταξις, "The Great Treatise", originally Μαθηματικὴ Σύνταξις, "Mathematical Treatise"). The second is the Geography, which is a thorough discussion of the geographic knowledge of the Greco-Roman world.

Much of the accumulated knowledge of the ancient world was lost. Even of the works of the many respectable thinkers, few fragments survive. Although he wrote at least fourteen books, almost nothing of Hipparchus' direct work survived. Of the 150 reputed Aristotelian works, only 30 exist, and some of those are "little more than lecture notes".[according to whom?]

India and China

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The Hindu-Arabic numeral system. The inscriptions on the edicts of Ashoka (3rd century BCE) display this number system being used by the Imperial Mauryas.

Important physical and mathematical traditions also existed in ancient Indian and Chinese sciences.

Star maps by the 11th century Chinese polymath Su Song are the oldest known woodblock-printed star maps to have survived to the present day. This example, dated 1092,[note 1] employs the cylindricalequirectangular projection.[2]

In Indian philosophy, Maharishi Kanada was the first to systematically develop a theory of atomism around 200 BCE[3] though some authors have allotted him an earlier era in the 6th century BCE.[4][5] It was further elaborated by the Buddhist atomists Dharmakirti and Dignāga during the 1st millennium CE.[6] Pakudha Kaccayana, a 6th-century BCE Indian philosopher and contemporary of Gautama Buddha, had also propounded ideas about the atomic constitution of the material world. The Vaisheshika school of philosophers believed that an atom was a mere point in space. It was also first to depict relations between motion and force applied. Indian theories about the atom are greatly abstract and enmeshed in philosophy as they were based on logic and not on personal experience or experimentation.

In Indian astronomy, Aryabhata's Aryabhatiya (499 CE) proposed the Earth's rotation, while Nilakantha Somayaji (1444–1544) of the Kerala school of astronomy and mathematics proposed a semi-heliocentric model resembling the Tychonic system.

The study of magnetism in Ancient China dates to the 4th century BCE (in the Book of the Devil Valley Master).[7] A main contributor to this field was Shen Kuo (1031–1095), a polymath and statesman who was the first to describe the magnetic-needle compass used for navigation, as well as establishing the concept of true north. In optics, Shen Kuo independently developed a camera obscura.[8]

Islamic world

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Ibn al-Haytham (c. 965–1040).

In the 7th to 15th centuries, scientific progress occurred in the Muslim world. Many classic works in Indian, Assyrian, Sassanian (Persian) and Greek, including the works of Aristotle, were translated into Arabic.[9] Important contributions were made by Ibn al-Haytham (965–1040), an Arab[10] or Persian[11] scientist, considered to be a founder of modern optics. Ptolemy and Aristotle theorised that light either shone from the eye to illuminate objects or that "forms" emanated from objects themselves, whereas al-Haytham (known by the Latin name "Alhazen") suggested that light travels to the eye in rays from different points on an object. The works of Ibn al-Haytham and al-Biruni (973–1050), a Persian scientist, eventually passed on to Western Europe where they were studied by scholars such as Roger Bacon and Vitello.[12]

Ibn al-Haytham used controlled experiments in his work on optics, although to what extent it differed from Ptolemy is debated.[13][14] Arabic mechanics like Bīrūnī and Al-Khazini developed sophisticated "science of weight", carrying out measurements of specific weights and volumes.[15]

Ibn Sīnā (980–1037), known as "Avicenna", was a polymath from Bukhara (in present-day Uzbekistan) responsible for important contributions to physics, optics, philosophy and medicine. He published his theory of motion in Book of Healing (1020), where he argued that an impetus is imparted to a projectile by the thrower. He viewed it as persistent, requiring external forces such as air resistance to dissipate it.[16][17][18] Ibn Sina made a distinction between 'force' and 'inclination' (called "mayl"), and argued that an object gained mayl when the object is in opposition to its natural motion. He concluded that continuation of motion is attributed to the inclination that is transferred to the object, and that object will be in motion until the mayl is spent. This conception of motion is consistent with Newton's first law of motion, inertia, which states that an object in motion will stay in motion unless it is acted on by an external force.[16] This idea which dissented from the Aristotelian view was later described as "impetus" by John Buridan, who was likely influenced by Ibn Sina's Book of Healing.[19]

A page from al-Khwārizmī's Algebra.

Hibat Allah Abu'l-Barakat al-Baghdaadi (c. 1080 – c. 1165) adopted and modified Ibn Sina's theory on projectile motion. In his Kitab al-Mu'tabar, Abu'l-Barakat stated that the mover imparts a violent inclination (mayl qasri) on the moved and that this diminishes as the moving object distances itself from the mover.[20] He also proposed an explanation of the acceleration of falling bodies by the accumulation of successive increments of power with successive increments of velocity.[21] According to Shlomo Pines, al-Baghdaadi's theory of motion was "the oldest negation of Aristotle's fundamental dynamic law [namely, that a constant force produces a uniform motion], [and is thus an] anticipation in a vague fashion of the fundamental law of classical mechanics [namely, that a force applied continuously produces acceleration]."[22] Jean Buridan and Albert of Saxony later referred to Abu'l-Barakat in explaining that the acceleration of a falling body is a result of its increasing impetus.[20]

Ibn Bajjah (c. 1085–1138), known as "Avempace" in Europe, proposed that for every force there is always a reaction force. Ibn Bajjah was a critic of Ptolemy and he worked on creating a new theory of velocity to replace the one theorized by Aristotle. Two future philosophers supported the theories Avempace created, known as Avempacean dynamics. These philosophers were Thomas Aquinas, a Catholic priest, and John Duns Scotus.[23] Galileo went on to adopt Avempace's formula "that the velocity of a given object is the difference of the motive power of that object and the resistance of the medium of motion".[23]

Nasir al-Din al-Tusi (1201–1274), a Persian astronomer and mathematician who died in Baghdad, introduced the Tusi couple an important mathematical theorem and founded the Maragha School of astronomy. Geocentric (but not heliocentric) astronomical models developed by the Maragha School have many striking parallels with models developed by Nicolaus Copernicus. The possibility that Maragha results may have influenced Copernicus has a been investigated in some detail.[24]

Medieval Europe

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Awareness of ancient works re-entered the West through translations from Arabic to Latin. Their re-introduction, combined with Judeo-Islamic theological commentaries, had a great influence on Medieval philosophers such as Thomas Aquinas. Scholastic European scholars, who sought to reconcile the philosophy of the ancient classical philosophers with Christian theology, proclaimed Aristotle the greatest thinker of the ancient world. In cases where they did not directly contradict the Bible, Aristotelian physics became the foundation for the physical explanations of the European Churches. Quantification became a core element of medieval physics.[25]

Based on Aristotelian physics, Scholastic physics described things as moving according to their essential nature. Celestial objects were described as moving in circles, because perfect circular motion was considered an innate property of objects that existed in the uncorrupted realm of the celestial spheres. Motions below the lunar sphere were seen as imperfect, and thus could not be expected to exhibit consistent motion. More idealized motion in the "sublunary" realm could only be achieved through artifice, and prior to the 17th century, many did not view artificial experiments as a valid means of learning about the natural world. Physical explanations in the sublunary realm revolved around tendencies. Stones contained the element earth, and earthly objects tended to move in a straight line toward the centre of the earth (and the universe in the Aristotelian geocentric view) unless otherwise prevented from doing so.[26]

Aristotle's physics was not scrutinized until John Philoponus, who relied on observation rather than verbal argument like Aristotle.[27] Philoponus' criticism of Aristotelian principles of physics served as an inspiration for Galileo Galilei ten centuries later,[28] during the Scientific Revolution. Galileo cited Philoponus substantially in his works when arguing that Aristotelian physics was flawed.[29][30] In the 1300s Jean Buridan, a teacher in the faculty of arts at the University of Paris, developed the concept of impetus. It was a step toward the modern ideas of inertia and momentum.[31]

Scientific Revolution

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During the 16th and 17th centuries, a large advancement of scientific progress known as the Scientific Revolution took place in Europe. Dissatisfaction with older philosophical approaches had begun earlier and had produced other changes in society, such as the Protestant Reformation, but the revolution in science began when natural philosophers began to mount a sustained attack on the Scholastic philosophical programme and supposed that mathematical descriptive schemes adopted from such fields as mechanics and astronomy could actually yield universally valid characterizations of motion and other concepts.

Nicolaus Copernicus

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Heliocentric model proposed in 1543 by Nicolaus Copernicus

A breakthrough in astronomy was made by Renaissance astronomer Nicolaus Copernicus (1473–1543) when, in 1543, he gave strong arguments for the heliocentric model of the Solar System, ostensibly as a means to render tables charting planetary motion more accurate and to simplify their production. In heliocentric models of the Solar system, the Earth orbits the Sun along with other bodies in Earth's galaxy, a contradiction according to the Greek-Egyptian astronomer Ptolemy (2nd century CE; see above), whose system placed the Earth at the center of the Universe and had been accepted for over 1,400 years. The Greek astronomer Aristarchus of Samos (c. 310 – c. 230 BCE) had suggested that the Earth revolves around the Sun, but Copernicus's reasoning led to lasting general acceptance of this "revolutionary" idea. Copernicus's book presenting the theory (De revolutionibus orbium coelestium, "On the Revolutions of the Celestial Spheres") was published just before his death in 1543 and, as it is now generally considered to mark the beginning of modern astronomy, is also considered to mark the beginning of the Scientific Revolution.[citation needed] Copernicus's new perspective, along with the accurate observations made by Tycho Brahe, enabled German astronomer Johannes Kepler (1571–1630) to formulate his laws regarding planetary motion that remain in use today.

Galileo Galilei

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Galileo Galilei (1564–1642), early proponent of the modern scientific worldview and method

The Italian mathematician, astronomer, and physicist Galileo Galilei (1564–1642) was a supporter of Copernicanism who made numerous astronomical discoveries, carried out empirical experiments and improved the telescope. As a mathematician, Galileo's role in the university culture of his era was subordinated to the three major topics of study: law, medicine, and theology (which was closely allied to philosophy). Galileo, however, felt that the descriptive content of the technical disciplines warranted philosophical interest, particularly because mathematical analysis of astronomical observations – notably, Copernicus's analysis of the relative motions of the Sun, Earth, Moon, and planets – indicated that philosophers' statements about the nature of the universe could be shown to be in error. Galileo also performed mechanical experiments, insisting that motion itself – regardless of whether it was produced "naturally" or "artificially" (i.e. deliberately) – had universally consistent characteristics that could be described mathematically.

Galileo's early studies at the University of Pisa were in medicine, but he was soon drawn to mathematics and physics. At age 19, he discovered (and, subsequently, verified) the isochronal nature of the pendulum when, using his pulse, he timed the oscillations of a swinging lamp in Pisa's cathedral and found that it remained the same for each swing regardless of the swing's amplitude. He soon became known through his invention of a hydrostatic balance and for his treatise on the center of gravity of solid bodies. While teaching at the University of Pisa (1589–1592), he initiated his experiments concerning the laws of bodies in motion that brought results so contradictory to the accepted teachings of Aristotle that strong antagonism was aroused. He found that bodies do not fall with velocities proportional to their weights. The story in which Galileo is said to have dropped weights from the Leaning Tower of Pisa is apocryphal, but he did find that the path of a projectile is a parabola and is credited with conclusions that anticipated Newton's laws of motion (e.g. the notion of inertia). Among these is what is now called Galilean relativity, the first precisely formulated statement about properties of space and time outside three-dimensional geometry.[citation needed]

Composite montage comparing Jupiter (left) and its four Galilean moons (from top: Io, Europa, Ganymede, Callisto)

Galileo has been called the "father of modern observational astronomy",[32] the "father of modern physics", the "father of science",[33] and "the father of modern science".[34] According to Stephen Hawking, "Galileo, perhaps more than any other single person, was responsible for the birth of modern science."[35] As religious orthodoxy decreed a geocentric or Tychonic understanding of the Solar system, Galileo's support for heliocentrism provoked controversy and he was tried by the Inquisition. Found "vehemently suspect of heresy", he was forced to recant and spent the rest of his life under house arrest.

The contributions that Galileo made to observational astronomy include the telescopic confirmation of the phases of Venus; his discovery, in 1609, of Jupiter's four largest moons (subsequently given the collective name of the "Galilean moons"); and the observation and analysis of sunspots. Galileo also pursued applied science and technology, inventing, among other instruments, a military compass. His discovery of the Jovian moons was published in 1610, enabling him to obtain the position of mathematician and philosopher to the Medici court. As such, he was expected to engage in debates with philosophers in the Aristotelian tradition and received a large audience for his own publications such as the Discourses and Mathematical Demonstrations Concerning Two New Sciences (published abroad following his arrest for the publication of Dialogue Concerning the Two Chief World Systems) and The Assayer.[36][37] Galileo's interest in experimenting with and formulating mathematical descriptions of motion established experimentation as an integral part of natural philosophy. This tradition, combining with the non-mathematical emphasis on the collection of "experimental histories" by philosophical reformists such as William Gilbert and Francis Bacon, drew a significant following in the years leading to and following Galileo's death, including Evangelista Torricelli and the participants in the Accademia del Cimento in Italy; Marin Mersenne and Blaise Pascal in France; Christiaan Huygens in the Netherlands; and Robert Hooke and Robert Boyle in England.

Johannes Kepler

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Johannes Kepler's first law of planetary motion states that planets move in elliptical orbits about the Sun.

Johannes Kepler (1571–1630) was a German astronomer, mathematician, astrologer, natural philosopher and a key figure in the 17th century Scientific Revolution, best known for his laws of planetary motion, and his books Astronomia nova, Harmonice Mundi, and Epitome Astronomiae Copernicanae, influencing among others Isaac Newton, providing one of the foundations for his theory of universal gravitation.[38] The variety and impact of his work made Kepler one of the founders of modern astronomy, the scientific method, natural and modern science.[39][40][41]

Kepler was partly driven by his belief that there is an intelligible plan that is accessible through reason.[42] Kepler described his new astronomy as "celestial physics",[43] as "an excursion into Aristotle's Metaphysics",[44] and as "a supplement to Aristotle's On the Heavens",[45] treating astronomy as part of a universal mathematical physics.[46]

René Descartes

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Cartesian coordinate system was introduced by René Descartes

The French philosopher René Descartes (1596–1650) was well-connected to, and influential within, experimental philosophy networks. Descartes had an agenda, however, which was geared toward replacing the Scholastic philosophical tradition. Questioning the reality interpreted through the senses, Descartes sought to re-establish philosophical explanations by reducing all phenomena to the motion of an invisible sea of "corpuscles". (Notably, he reserved human thought and God from his scheme, holding these to be separate from the physical universe). In proposing this philosophical framework, Descartes supposed that different kinds of motion, such as that of planets versus that of terrestrial objects, were not fundamentally different, but were manifestations of an endless chain of corpuscular motions obeying universal principles. Particularly influential were his explanations for circular astronomical motions in terms of the vortex motion of corpuscles in space (Descartes argued, in accord with the beliefs, if not the methods, of the Scholastics, that a vacuum could not exist), and his explanation of gravity in terms of corpuscles pushing objects downward.[47][48][49]

Descartes, like Galileo, was convinced of the importance of mathematical explanation, and he and his followers were key figures in the development of mathematics and geometry in the 17th century. Cartesian mathematical descriptions of motion held that all mathematical formulations had to be justifiable in terms of direct physical action, a position held by Christiaan Huygens and the German philosopher Gottfried Leibniz, who, while following in the Cartesian tradition, developed his own philosophical alternative to Scholasticism, which he outlined in his 1714 work, the Monadology. Descartes has been dubbed the "Father of Modern Philosophy", and much subsequent Western philosophy is a response to his writings, which are studied closely to this day. In particular, his Meditations on First Philosophy continues to be a standard text at most university philosophy departments. Descartes' influence in mathematics is equally apparent; the Cartesian coordinate system – allowing algebraic equations to be expressed as geometric shapes in a two-dimensional coordinate system – was named after him. He is credited as the father of analytical geometry, the bridge between algebra and geometry, important to the discovery of calculus and analysis.

Christiaan Huygens

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Christiaan Huygens (1629–1695)

The Dutch physicist, mathematician, astronomer and inventor Christiaan Huygens (1629–1695) was the leading scientist in Europe between Galileo and Newton. Huygens came from a family of nobility that had an important position in the Dutch society of the 17th century; a time in which the Dutch Republic flourished economically and culturally. This period – roughly between 1588 and 1702 – of the history of the Netherlands is also referred to as the Dutch Golden Age, an era during the Scientific Revolution when Dutch science was among the most acclaimed in Europe. At this time, intellectuals and scientists like René Descartes, Baruch Spinoza, Pierre Bayle, Antonie van Leeuwenhoek, John Locke and Hugo Grotius resided in the Netherlands. It was in this intellectual environment that Christiaan Huygens grew up. Christiaan's father, Constantijn Huygens, was, apart from an important poet, the secretary and diplomat for the Princes of Orange. He knew many scientists of his time because of his contacts and intellectual interests, including René Descartes and Marin Mersenne, and it was because of these contacts that Christiaan Huygens became aware of their work, especially Descartes, whose mechanistic philosophy was going to have a huge influence on Huygens' own work. Descartes was later impressed by the skills Huygens showed in geometry, as was Mersenne, who christened him "the new Archimedes" (which led Constantijn to refer to his son as "my little Archimedes").

A child prodigy, Huygens began his correspondence with Marin Mersenne when he was 17 years old. Huygens became interested in games of chance when he encountered the work of Fermat, Blaise Pascal and Girard Desargues. It was Pascal who encouraged him to write Van Rekeningh in Spelen van Gluck, which Frans van Schooten translated and published as De Ratiociniis in Ludo Aleae in 1657. The book is the earliest known scientific treatment of the subject, and at the time the most coherent presentation of a mathematical approach to games of chance. Two years later Huygens derived geometrically the now standard formulae in classical mechanics for the centripetal- and centrifugal force in his work De vi Centrifuga (1659). Around the same time Huygens' research in horology resulted in the invention of the pendulum clock; a breakthrough in timekeeping and the most accurate timekeeper for almost 300 years. The theoretical research of the way the pendulum works eventually led to the publication of one of his most important achievements: the Horologium Oscillatorium. This work was published in 1673 and became one of the three most important 17th century works on mechanics (the other two being Galileo's Discourses and Mathematical Demonstrations Relating to Two New Sciences (1638) and Newton's Philosophiæ Naturalis Principia Mathematica (1687)[50]). The Horologium Oscillatorium is the first modern treatise in which a physical problem (the accelerated motion of a falling body) is idealized by a set of parameters then analyzed mathematically and constitutes one of the seminal works of applied mathematics.[51][52] It is for this reason, Huygens has been called the first theoretical physicist and one of the founders of modern mathematical physics.[53][54] Huygens' Horologium Oscillatorium influenced the work of Isaac Newton, who admired the work. For instance, the laws Huygens described in the Horologium Oscillatorium are structurally the same as Newton's first two laws of motion.[55]

Five years after the publication of his Horologium Oscillatorium, Huygens described his wave theory of light. Though proposed in 1678, it was not published until 1690 in his Traité de la Lumière. His mathematical theory of light was initially rejected in favour of Newton's corpuscular theory of light, until Augustin-Jean Fresnel adopted Huygens' principle to give a complete explanation of the rectilinear propagation and diffraction effects of light in 1821. Today this principle is known as the Huygens–Fresnel principle.

As an astronomer, Huygens began grinding lenses with his brother Constantijn Jr. to build telescopes for astronomical research. He was the first to identify the rings of Saturn as "a thin, flat ring, nowhere touching, and inclined to the ecliptic," and discovered the first of Saturn's moons, Titan, using a refracting telescope.

Huygens was also the first who brought mathematical rigor to the description of physical phenomena. Because of this, and the fact that he developed institutional frameworks for scientific research on the continent, he has been referred to as "the leading actor in 'the making of science in Europe'"[56]

Isaac Newton

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Sir Isaac Newton (1642–1727)

Cambridge University physicist and mathematician Sir Isaac Newton (1642–1727) was a fellow of the Royal Society of England, who created a single system for describing the workings of the universe. Newton formulated three laws of motion which formulated the relationship between motion and objects and also the law of universal gravitation, the latter of which could be used to explain the behavior not only of falling bodies on the earth but also planets and other celestial bodies. To arrive at his results, Newton invented one form of an entirely new branch of mathematics: calculus (also invented independently by Gottfried Leibniz), which was to become an essential tool in much of the later development in most branches of physics. Newton's findings were set forth in his Philosophiæ Naturalis Principia Mathematica ("Mathematical Principles of Natural Philosophy"), the publication of which in 1687 marked the beginning of the modern period of mechanics and astronomy.

Newton refuted the Cartesian mechanical tradition that all motions should be explained with respect to the immediate force exerted by corpuscles. Using his three laws of motion and law of universal gravitation, Newton removed the idea that objects followed paths determined by natural shapes and instead demonstrated that all the future motions of any body could be deduced mathematically based on knowledge of their existing motion, their mass, and the forces acting upon them. However, observed celestial motions did not precisely conform to a Newtonian treatment, and Newton, who was also deeply interested in theology, imagined that God intervened to ensure the continued stability of the solar system.

Newton's cannonball, a though experiment by Newton relating the motion of a projectile and orbiting of planets.

Newton's principles (but not his mathematical treatments) proved controversial with Continental philosophers, who found his lack of metaphysical explanation for movement and gravitation philosophically unacceptable. Beginning around 1700, a bitter rift opened between the Continental and British philosophical traditions, which were stoked by heated, ongoing, and viciously personal disputes between the followers of Newton and Leibniz concerning priority over the analytical techniques of calculus, which each had developed independently. Initially, the Cartesian and Leibnizian traditions prevailed on the Continent (leading to the dominance of the Leibnizian calculus notation everywhere except Britain). Newton himself remained privately disturbed at the lack of a philosophical understanding of gravitation while insisting in his writings that none was necessary to infer its reality. As the 18th century progressed, Continental natural philosophers increasingly accepted the Newtonians' willingness to forgo ontological metaphysical explanations for mathematically described motions.[57][58][59]

Newton built the first functioning reflecting telescope[60] and developed a theory of color, published in Opticks, based on the observation that a prism decomposes white light into the many colours forming the visible spectrum. While Newton explained light as being composed of tiny particles, a rival theory of light which explained its behavior in terms of waves was presented in 1690 by Christiaan Huygens. However, the belief in the mechanistic philosophy coupled with Newton's reputation meant that the wave theory saw relatively little support until the 19th century. Newton also formulated an empirical law of cooling, studied the speed of sound, investigated power series, demonstrated the generalised binomial theorem and developed a method for approximating the roots of a function. His work on infinite series was inspired by Simon Stevin's decimals.[61] Most importantly, Newton showed that the motions of objects on Earth and of celestial bodies are governed by the same set of natural laws, which were neither capricious nor malevolent. By demonstrating the consistency between Kepler's laws of planetary motion and his own theory of gravitation, Newton also removed the last doubts about heliocentrism. By bringing together all the ideas set forth during the Scientific Revolution, Newton effectively established the foundation for modern society in mathematics and science.

Other achievements

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Other branches of physics also received attention during the period of the Scientific Revolution. William Gilbert, court physician to Queen Elizabeth I, described how the earth itself behaves like a giant magnet. Robert Boyle (1627–1691) studied the behavior of gases enclosed in a chamber and formulated the gas law named for him; he also contributed to physiology and to the founding of modern chemistry.

Another factor in the Scientific Revolution was the rise of learned societies and academies in various countries. The earliest of these were in Italy and Germany and were short-lived. More influential were the Royal Society of England (1660) and the Academy of Sciences in France (1666). The former was a private institution in London and included John Wallis, William Brouncker, Thomas Sydenham, John Mayow, and Christopher Wren (who contributed not only to architecture but also to astronomy and anatomy); the latter, in Paris, was a government institution and included as a foreign member the Dutchman Huygens. In the 18th century, important royal academies were established at Berlin (1700) and at St. Petersburg (1724). The societies and academies provided the principal opportunities for the publication and discussion of scientific results during and after the scientific revolution. In 1690, James Bernoulli showed that the cycloid is the solution to the tautochrone problem; and the following year, in 1691, Johann Bernoulli showed that a chain freely suspended from two points will form a catenary, the curve with the lowest possible center of gravity available to any chain hung between two fixed points. He then showed, in 1696, that the cycloid is the solution to the brachistochrone problem.

Early thermodynamics

[edit]
Magdeburg hemispheres, an experiment by Otto von Guericke where two metal hemispheres are held together by vacuum and cannot be separated even if large forces are applied.


A precursor of the engine was designed by the German scientist Otto von Guericke who, in 1650, designed and built the world's first vacuum pump to create a vacuum as demonstrated in the Magdeburg hemispheres experiment. He was driven to make a vacuum to disprove Aristotle's long-held supposition that 'Nature abhors a vacuum'. Shortly thereafter, Irish physicist and chemist Boyle had learned of Guericke's designs and in 1656, in coordination with English scientist Robert Hooke, built an air pump. Using this pump, Boyle and Hooke noticed the pressure-volume correlation for a gas: PV = k, where P is pressure, V is volume and k is a constant: this relationship is known as Boyle's law. In that time, air was assumed to be a system of motionless particles, and not interpreted as a system of moving molecules. The concept of thermal motion came two centuries later. Therefore, Boyle's publication in 1660 speaks about a mechanical concept: the air spring.[62] Later, after the invention of the thermometer, the property temperature could be quantified. This tool gave Joseph Louis Gay-Lussac the opportunity to derive his law, which led shortly later to the ideal gas law. But, already before the establishment of the ideal gas law, an associate of Boyle's named Denis Papin built in 1679 a bone digester, which is a closed vessel with a tightly fitting lid that confines steam until a high pressure is generated.

Later designs implemented a steam release valve to keep the machine from exploding. By watching the valve rhythmically move up and down, Papin conceived of the idea of a piston and cylinder engine. He did not however follow through with his design. Nevertheless, in 1697, based on Papin's designs, engineer Thomas Savery built the first engine. Although these early engines were crude and inefficient, they attracted the attention of the leading scientists of the time. Hence, prior to 1698 and the invention of the Savery Engine, horses were used to power pulleys, attached to buckets, which lifted water out of flooded salt mines in England. In the years to follow, more variations of steam engines were built, such as the Newcomen Engine, and later the Watt Engine. In time, these early engines would replace horses. Thus, each engine began to be associated with a certain amount of "horse power" depending upon how many horses it had replaced. The main problem with these first engines was that they were slow and clumsy, converting less than 2% of the input fuel into useful work. In other words, large quantities of coal (or wood) had to be burned to yield a small fraction of work output; the need for a new science of engine dynamics was born.

18th-century developments

[edit]

During the 18th century, the mechanics founded by Newton was developed by several scientists as more mathematicians learned calculus and elaborated upon its initial formulation. The application of mathematical analysis to problems of motion was known as rational mechanics, or mixed mathematics (and was later termed classical mechanics).

Mechanics

[edit]
Replica of William Herschel's telescope used to discover Uranus

In 1714, Brook Taylor derived the fundamental frequency of a stretched vibrating string in terms of its tension and mass per unit length by solving a differential equation. The Swiss mathematician Daniel Bernoulli (1700–1782) made important mathematical studies of the behavior of gases, anticipating the kinetic theory of gases developed more than a century later, and has been referred to as the first mathematical physicist.[63] In 1733, Daniel Bernoulli derived the fundamental frequency and harmonics of a hanging chain by solving a differential equation. In 1734, Bernoulli solved the differential equation for the vibrations of an elastic bar clamped at one end. Bernoulli's treatment of fluid dynamics and his examination of fluid flow was introduced in his 1738 work Hydrodynamica.

Rational mechanics dealt primarily with the development of elaborate mathematical treatments of observed motions, using Newtonian principles as a basis, and emphasized improving the tractability of complex calculations and developing of legitimate means of analytical approximation. A representative contemporary textbook was published by Johann Baptiste Horvath. By the end of the century analytical treatments were rigorous enough to verify the stability of the Solar System solely on the basis of Newton's laws without reference to divine intervention – even as deterministic treatments of systems as simple as the three body problem in gravitation remained intractable.[64] In 1705, Edmond Halley predicted the periodicity of Halley's Comet, William Herschel discovered Uranus in 1781, and Henry Cavendish measured the gravitational constant and determined the mass of the Earth in 1798. In 1783, John Michell suggested that some objects might be so massive that not even light could escape from them.

In 1739, Leonhard Euler solved the ordinary differential equation for a forced harmonic oscillator and noticed the resonance phenomenon. In 1742, Colin Maclaurin discovered his uniformly rotating self-gravitating spheroids. In 1742, Benjamin Robins published his New Principles in Gunnery, establishing the science of aerodynamics. British work, carried on by mathematicians such as Taylor and Maclaurin, fell behind Continental developments as the century progressed. Meanwhile, work flourished at scientific academies on the Continent, led by such mathematicians as Bernoulli and Euler, as well as Joseph-Louis Lagrange, Pierre-Simon Laplace, and Adrien-Marie Legendre. In 1743, Jean le Rond d'Alembert published his Traité de dynamique, in which he introduced the concept of generalized forces for accelerating systems and systems with constraints, and applied the new idea of virtual work to solve dynamical problem, now known as D'Alembert's principle, as a rival to Newton's second law of motion. In 1747, Pierre Louis Maupertuis applied minimum principles to mechanics. In 1759, Euler solved the partial differential equation for the vibration of a rectangular drum. In 1764, Euler examined the partial differential equation for the vibration of a circular drum and found one of the Bessel function solutions. In 1776, John Smeaton published a paper on experiments relating power, work, momentum and kinetic energy, and supporting the conservation of energy. In 1788, Lagrange presented his equations of motion in Mécanique analytique, in which the whole of mechanics was organized around the principle of virtual work. In 1789, Antoine Lavoisier stated the law of conservation of mass. The rational mechanics developed in the 18th century received expositions in both Lagrange's Mécanique analytique and Laplace's Traité de mécanique céleste (1799–1825).

Thermodynamics and static electricity

[edit]
An engraving of Benjamin Franklin's kite experiment used to study lightning.


During the 18th century, thermodynamics was developed through the theories of weightless "imponderable fluids", such as heat ("caloric"), electricity, and phlogiston (which was rapidly overthrown as a concept following Antoine Lavoisier's identification of oxygen gas late in the century). Assuming that these concepts were real fluids, their flow could be traced through a mechanical apparatus or chemical reactions. This tradition of experimentation led to the development of new kinds of experimental apparatus, such as the Leyden jar; and new kinds of measuring instruments, such as the calorimeter, and improved versions of old ones, such as the thermometer. Experiments also produced new concepts, such as the University of Glasgow experimenter Joseph Black's notion of latent heat and Philadelphia intellectual Benjamin Franklin's characterization of electrical fluid as flowing between places of excess and deficit (a concept later reinterpreted in terms of positive and negative charges). Franklin also showed that lightning is electricity in 1752.

The accepted theory of heat in the 18th century viewed it as a kind of fluid, called caloric; although this theory was later shown to be erroneous, a number of scientists adhering to it nevertheless made important discoveries useful in developing the modern theory, including Joseph Black (1728–1799) and Henry Cavendish (1731–1810). Opposed to this caloric theory, which had been developed mainly by the chemists, was the less accepted theory dating from Newton's time that heat is due to the motions of the particles of a substance. This mechanical theory gained support in 1798 from the cannon-boring experiments of Count Rumford (Benjamin Thompson), who found a direct relationship between heat and mechanical energy.

While it was recognized early in the 18th century that finding absolute theories of electrostatic and magnetic force akin to Newton's principles of motion would be an important achievement, none were forthcoming. This impossibility only slowly disappeared as experimental practice became more widespread and more refined in the early years of the 19th century in places such as the newly established Royal Institution in London. Meanwhile, the analytical methods of rational mechanics began to be applied to experimental phenomena, most influentially with the French mathematician Joseph Fourier's analytical treatment of the flow of heat, as published in 1822.[65][66][67] Joseph Priestley proposed an electrical inverse-square law in 1767, and Charles-Augustin de Coulomb introduced the inverse-square law of electrostatics in 1798.

At the end of the century, the members of the French Academy of Sciences had attained clear dominance in the field.[59][68][69][70] At the same time, the experimental tradition established by Galileo and his followers persisted. The Royal Society and the French Academy of Sciences were major centers for the performance and reporting of experimental work. Experiments in mechanics, optics, magnetism, static electricity, chemistry, and physiology were not clearly distinguished from each other during the 18th century, but significant differences in explanatory schemes and, thus, experiment design were emerging. Chemical experimenters, for instance, defied attempts to enforce a scheme of abstract Newtonian forces onto chemical affiliations, and instead focused on the isolation and classification of chemical substances and reactions.[71]

19th century

[edit]

Mechanics

[edit]

In 1821, William Hamilton began his analysis of Hamilton's characteristic function. In 1835, he stated Hamilton's canonical equations of motion.

In 1813, Peter Ewart supported the idea of the conservation of energy in his paper On the measure of moving force. In 1829, Gaspard Coriolis introduced the terms of work (force times distance) and kinetic energy with the meanings they have today. In 1841, Julius Robert von Mayer, an amateur scientist, wrote a paper on the conservation of energy, although his lack of academic training led to its rejection. In 1847, Hermann von Helmholtz formally stated the law of conservation of energy.

Electromagnetism

[edit]
The Voltaic pile, the first battery was invented by Alessandro Volta in 1800

In 1800, Alessandro Volta invented the electric battery (known as the voltaic pile) and thus improved the way electric currents could also be studied. A year later, Thomas Young demonstrated the wave nature of light – which received strong experimental support from the work of Augustin-Jean Fresnel – and the principle of interference. In 1820, Hans Christian Ørsted found that a current-carrying conductor gives rise to a magnetic force surrounding it, and within a week after Ørsted's discovery reached France, André-Marie Ampère discovered that two parallel electric currents will exert forces on each other. In 1821, Michael Faraday built an electricity-powered motor, while Georg Ohm stated his law of electrical resistance in 1826, expressing the relationship between voltage, current, and resistance in an electric circuit.

In 1831, Faraday (and independently Joseph Henry) discovered the reverse effect, the production of an electric potential or current through magnetism – known as electromagnetic induction; these two discoveries are the basis of the electric motor and the electric generator, respectively.

In 1873, James Clerk Maxwell published A Treatise on Electricity and Magnetism, which described the transmission of energy in wave form through a "luminiferous ether", and suggested that light was such a wave. This was confirmed in 1888 when Helmholtz student Heinrich Hertz generated and detected electromagnetic radiation in the laboratory.[72][73][74][75]

Laws of thermodynamics

[edit]
James Prescott Joule's apparatus for measuring the mechanical equivalent of heat which the "work" of the falling weight is converted into the "heat" of agitation in the water.

In the 19th century, the connection between heat and mechanical energy was established quantitatively by Julius Robert von Mayer and James Prescott Joule, who measured the mechanical equivalent of heat in the 1840s. In 1849, Joule published results from his series of experiments (including the paddlewheel experiment) which show that heat is a form of energy, a fact that was accepted in the 1850s. The relation between heat and energy was important for the development of steam engines, and in 1824 the experimental and theoretical work of Sadi Carnot was published. Carnot captured some of the ideas of thermodynamics in his discussion of the efficiency of an idealized engine. Sadi Carnot's work provided a basis for the formulation of the first law of thermodynamics – a restatement of the law of conservation of energy – which was stated around 1850 by William Thomson, later known as Lord Kelvin, and Rudolf Clausius. Lord Kelvin, who had extended the concept of absolute zero from gases to all substances in 1848, drew upon the engineering theory of Lazare Carnot, Sadi Carnot, and Émile Clapeyron as well as the experimentation of James Prescott Joule on the interchangeability of mechanical, chemical, thermal, and electrical forms of work to formulate the first law.

Kelvin and Clausius also stated the second law of thermodynamics, which was originally formulated in terms of the fact that heat does not spontaneously flow from a colder body to a warmer one. Other formulations followed quickly (for example, the second law was expounded in Thomson and Peter Guthrie Tait's influential work Treatise on Natural Philosophy) and Kelvin in particular understood some of the law's general implications. The second Law – the idea that gases consist of molecules in motion – had been discussed in some detail by Daniel Bernoulli in 1738, but had fallen out of favor, and was revived by Clausius in 1857. In 1850, Hippolyte Fizeau and Léon Foucault measured the speed of light in water and found that it is slower than in air, in support of the wave model of light. In 1852, Joule and Thomson demonstrated that a rapidly expanding gas cools, later named the Joule–Thomson effect or Joule–Kelvin effect. Hermann von Helmholtz put forward the idea of the heat death of the universe in 1854, the same year that Clausius established the importance of dQ/T (Clausius's theorem) (though he did not yet name the quantity).

Statistical mechanics

[edit]
Maxwell's demon, thought experiment by James Clerk Maxwell to describe the kinetic theory of gases and describe how a microscopic creature could lead to violations of the second law of thermodynamics.

In 1860, James Clerk Maxwell worked out the mathematics of the distribution of velocities of the molecules of a gas, known today as the Maxwell–Boltzmann distribution.

The atomic theory of matter had been proposed again in the early 19th century by the chemist John Dalton and became one of the hypotheses of the kinetic-molecular theory of gases developed by Clausius and James Clerk Maxwell to explain the laws of thermodynamics.

The kinetic theory in turn led to a revolutionary approach to science, the statistical mechanics of Ludwig Boltzmann (1844–1906) and Josiah Willard Gibbs (1839–1903), which studies the statistics of microstates of a system and uses statistics to determine the state of a physical system. Interrelating the statistical likelihood of certain states of organization of these particles with the energy of those states, Clausius reinterpreted the dissipation of energy to be the statistical tendency of molecular configurations to pass toward increasingly likely, increasingly disorganized states (coining the term "entropy" to describe the disorganization of a state). The statistical versus absolute interpretations of the second law of thermodynamics set up a dispute that would last for several decades (producing arguments such as "Maxwell's demon"), and that would not be held to be definitively resolved until the behavior of atoms was firmly established in the early 20th century.[76][77] In 1902, James Jeans found the length scale required for gravitational perturbations to grow in a static nearly homogeneous medium.

Other developments

[edit]

In 1822, botanist Robert Brown discovered Brownian motion: pollen grains in water undergoing movement resulting from their bombardment by the fast-moving atoms or molecules in the liquid.

In 1834, Carl Jacobi discovered his uniformly rotating self-gravitating ellipsoids (the Jacobi ellipsoid).

In 1834, John Russell observed a nondecaying solitary water wave (soliton) in the Union Canal near Edinburgh, Scotland, and used a water tank to study the dependence of solitary water wave velocities on wave amplitude and water depth. In 1835, Gaspard Coriolis examined theoretically the mechanical efficiency of waterwheels, and deduced the Coriolis effect. In 1842, Christian Doppler proposed the Doppler effect.

In 1851, Léon Foucault showed the Earth's rotation with a huge pendulum (Foucault pendulum).

There were important advances in continuum mechanics in the first half of the century, namely formulation of laws of elasticity for solids and discovery of Navier–Stokes equations for fluids.

20th century: birth of modern physics

[edit]
Marie Skłodowska-Curie
(1867–1934) received Nobel prizes in physics (1903) and chemistry (1911).

At the end of the 19th century, physics had evolved to the point at which classical mechanics could cope with highly complex problems involving macroscopic situations; thermodynamics and kinetic theory were well established; geometrical and physical optics could be understood in terms of electromagnetic waves; and the conservation laws for energy and momentum (and mass) were widely accepted. So profound were these and other developments that it was generally accepted that all the important laws of physics had been discovered and that, henceforth, research would be concerned with clearing up minor problems and particularly with improvements of method and measurement.

However, around 1900 serious doubts arose about the completeness of the classical theories – the triumph of Maxwell's theories, for example, was undermined by inadequacies that had already begun to appear – and their inability to explain certain physical phenomena, such as the energy distribution in blackbody radiation and the photoelectric effect, while some of the theoretical formulations led to paradoxes when pushed to the limit. Prominent physicists such as Hendrik Lorentz, Emil Cohn, Ernst Wiechert and Wilhelm Wien believed that some modification of Maxwell's equations might provide the basis for all physical laws. These shortcomings of classical physics were never to be resolved and new ideas were required. At the beginning of the 20th century, a major revolution shook the world of physics, which led to a new era, generally referred to as modern physics.[78]

Radiation experiments

[edit]
Crookes tube used to study cathode rays. It led to the discovery of the electron by J. J. Thomson.

In the 19th century, experimenters began to detect unexpected forms of radiation: Wilhelm Röntgen caused a sensation with his discovery of X-rays in 1895; in 1896, Henri Becquerel discovered that certain kinds of matter emit radiation on their own accord. In 1897, J. J. Thomson discovered the electron, and new radioactive elements found by Marie and Pierre Curie raised questions about the supposedly indestructible atom and the nature of matter. Marie and Pierre coined the term "radioactivity" to describe this property of matter, and isolated the radioactive elements radium and polonium. Ernest Rutherford and Frederick Soddy identified two of Becquerel's forms of radiation with electrons and the element helium. Rutherford identified and named two types of radioactivity and in 1911 interpreted experimental evidence as showing that the atom consists of a dense, positively charged nucleus surrounded by negatively charged electrons. Classical theory, however, predicted that this structure should be unstable. Classical theory had also failed to explain successfully two other experimental results that appeared in the late 19th century. One of these was the demonstration by Albert A. Michelson and Edward W. Morley – known as the Michelson–Morley experiment – which showed there did not seem to be a preferred frame of reference, at rest with respect to the hypothetical luminiferous ether, for describing electromagnetic phenomena. Studies of radiation and radioactive decay continued to be a preeminent focus for physical and chemical research through the 1930s, when the discovery of nuclear fission by Lise Meitner and Otto Frisch opened the way to the practical exploitation of what came to be called "atomic" energy.

Albert Einstein's theory of relativity

[edit]
Albert Einstein (1879–1955), ca. 1905

In 1905, a 26-year-old German physicist named Albert Einstein (then a patent clerk in Bern, Switzerland) showed how measurements of time and space are affected by motion between an observer and what is being observed. Einstein's radical theory of relativity revolutionized science. Although Einstein made many other important contributions to science, the theory of relativity alone is one of the greatest intellectual achievements of all time. Although the concept of relativity was not introduced by Einstein, he recognised that the speed of light in vacuum is constant, i.e., the same for all observers, and an absolute upper limit to speed. This does not impact a person's day-to-day life since most objects travel at speeds much slower than light speed. For objects travelling near light speed, however, the theory of relativity shows that clocks associated with those objects will run more slowly and that the objects shorten in length according to measurements of an observer on Earth. Einstein also derived the equation, E = mc2, which expresses the equivalence of mass and energy.

Special relativity

[edit]

Einstein argued that the speed of light was a constant in all inertial reference frames and that electromagnetic laws should remain valid independent of reference frame – assertions which rendered the ether "superfluous" to physical theory, and that held that observations of time and length varied relative to how the observer was moving with respect to the object being measured (what came to be called the "special theory of relativity"). It also followed that mass and energy were interchangeable quantities according to the equation E=mc2. In another paper published the same year, Einstein asserted that electromagnetic radiation was transmitted in discrete quantities ("quanta"), according to a constant that the theoretical physicist Max Planck had posited in 1900 to arrive at an accurate theory for the distribution of blackbody radiation – an assumption that explained the strange properties of the photoelectric effect.

The special theory of relativity is a formulation of the relationship between physical observations and the concepts of space and time. The theory arose out of contradictions between electromagnetism and Newtonian mechanics and had great impact on both those areas. The original historical issue was whether it was meaningful to discuss the electromagnetic wave-carrying "ether" and motion relative to it and also whether one could detect such motion, as was unsuccessfully attempted in the Michelson–Morley experiment. Einstein demolished these questions and the ether concept in his special theory of relativity. However, his basic formulation does not involve detailed electromagnetic theory. It arises out of the question: "What is time?" Newton, in the Principia (1686), had given an unambiguous answer: "Absolute, true, and mathematical time, of itself, and from its own nature, flows equably without relation to anything external, and by another name is called duration." This definition is basic to all classical physics.

Einstein had the genius to question it, and found that it was incomplete. Instead, each "observer" necessarily makes use of his or her own scale of time, and for two observers in relative motion, their time-scales will differ. This induces a related effect on position measurements. Space and time become intertwined concepts, fundamentally dependent on the observer. Each observer presides over his or her own space-time framework or coordinate system. There being no absolute frame of reference, all observers of given events make different but equally valid (and reconcilable) measurements. What remains absolute is stated in Einstein's relativity postulate: "The basic laws of physics are identical for two observers who have a constant relative velocity with respect to each other."

Special relativity had a profound effect on physics: started as a rethinking of the theory of electromagnetism, it found a new symmetry law of nature, now called Poincaré symmetry, that replaced Galilean symmetry.

Special relativity exerted another long-lasting effect on dynamics. Although initially it was credited with the "unification of mass and energy", it became evident that relativistic dynamics established a distinction between rest mass, which is an invariant (observer independent) property of a particle or system of particles, and the energy and momentum of a system. The latter two are separately conserved in all situations but not invariant with respect to different observers. The term mass in particle physics underwent a semantic change, and since the late 20th century it almost exclusively denotes the rest (or invariant) mass.

General relativity

[edit]
Einstein proposed that gravitation results from masses (or their equivalent energies) curving ("bending") the spacetime in which they exist, altering the paths they follow within it.

By 1916, Einstein was able to generalize this further, to deal with all states of motion including non-uniform acceleration, which became the general theory of relativity. In this theory, Einstein also specified a new concept, the curvature of space-time, which described the gravitational effect at every point in space. The curvature of space-time replaced Newton's universal law of gravitation. According to Einstein, gravitational force in the normal sense is an illusion caused by the geometry of space. The presence of a mass causes a curvature of space-time in the vicinity of the mass, and this curvature dictates the space-time path that all freely-moving objects follow. It was also predicted from this theory that light should be subject to gravity – all of which was verified experimentally. This aspect of relativity explained the phenomena of light bending around the sun, predicted black holes as well as properties of the Cosmic microwave background radiation – a discovery rendering fundamental anomalies in the classic Steady-State hypothesis. For his work on relativity, the photoelectric effect and blackbody radiation, Einstein received the Nobel Prize in 1921.

The gradual acceptance of Einstein's theories of relativity and the quantized nature of light transmission, and of Niels Bohr's model of the atom created as many problems as they solved, leading to a full-scale effort to reestablish physics on new fundamental principles. Expanding relativity to cases of accelerating reference frames (the "general theory of relativity") in the 1910s, Einstein posited an equivalence between the inertial force of acceleration and the force of gravity, leading to the conclusion that space is curved and finite in size, and the prediction of such phenomena as gravitational lensing and the distortion of time in gravitational fields.

Quantum mechanics

[edit]
Hydrogen emission spectrum is discrete (here in log scale). The lines can only be explained with quantum mechanics.

Although relativity resolved the electromagnetic phenomena conflict demonstrated by Michelson and Morley, a second theoretical problem was the explanation of the distribution of electromagnetic radiation emitted by a black body; experiment showed that at shorter wavelengths, toward the ultraviolet end of the spectrum, the energy approached zero, but classical theory predicted it should become infinite. This glaring discrepancy, known as the ultraviolet catastrophe, was solved by the new theory of quantum mechanics. Quantum mechanics is the theory of atoms and subatomic systems. Approximately the first 30 years of the 20th century represent the time of the conception and evolution of the theory. The basic ideas of quantum theory were introduced in 1900 by Max Planck (1858–1947), who was awarded the Nobel Prize for Physics in 1918 for his discovery of the quantified nature of energy. The quantum theory (which previously relied in the "correspondence" at large scales between the quantized world of the atom and the continuities of the "classical" world) was accepted when the Compton Effect established that light carries momentum and can scatter off particles, and when Louis de Broglie asserted that matter can be seen as behaving as a wave in much the same way as electromagnetic waves behave like particles (wave–particle duality).

In 1905, Einstein used the quantum theory to explain the photoelectric effect, and in 1913 the Danish physicist Niels Bohr used the same constant to explain the stability of Rutherford's atom as well as the frequencies of light emitted by hydrogen gas. The quantized theory of the atom gave way to a full-scale quantum mechanics in the 1920s. New principles of a "quantum" rather than a "classical" mechanics, formulated in matrix-form by Werner Heisenberg, Max Born, and Pascual Jordan in 1925, were based on the probabilistic relationship between discrete "states" and denied the possibility of causality. Quantum mechanics was extensively developed by Heisenberg, Wolfgang Pauli, Paul Dirac, and Erwin Schrödinger, who established an equivalent theory based on waves in 1926; but Heisenberg's 1927 "uncertainty principle" (indicating the impossibility of precisely and simultaneously measuring position and momentum) and the "Copenhagen interpretation" of quantum mechanics (named after Bohr's home city) continued to deny the possibility of fundamental causality, though opponents such as Einstein would metaphorically assert that "God does not play dice with the universe".[79] The new quantum mechanics became an indispensable tool in the investigation and explanation of phenomena at the atomic level. Also in the 1920s, the Indian scientist Satyendra Nath Bose's work on photons and quantum mechanics provided the foundation for Bose–Einstein statistics, the theory of the Bose–Einstein condensate.

The spin–statistics theorem established that any particle in quantum mechanics may be either a boson (statistically Bose–Einstein) or a fermion (statistically Fermi–Dirac). It was later found that all fundamental bosons transmit forces, such as the photon that transmits electromagnetism.

Fermions are particles "like electrons and nucleons" and are the usual constituents of matter. Fermi–Dirac statistics later found numerous other uses, from astrophysics (see Degenerate matter) to semiconductor design.

Division into classical and modern

[edit]
1927 Solvay Conference included prominent physicists Albert Einstein, Werner Heisenberg, Max Planck, Hendrik Lorentz, Niels Bohr, Marie Curie, Erwin Schrödinger, Paul Dirac

The conceptual differences between physics theories discussed in the 19th century and those that were most historically prominent in the first decades of the 20th century lead to a characterization of the earlier sciences as "classical physics" while the work based on quantum and relativity theories became known as "modern physics". Initially applied to mechanics, as in "classical mechanics", the divide eventually came to characterize quantum and relativistic effects.[80]: 411 This characterization was driven initially by physicists like Max Planck and Hendrik Lorentz, established scientists who nevertheless saw issues that established theories could not explain. Their involvement and contributions to the 1911 Solvay Conference lead to the introduction of this split as a concept.[81]: 558

This division is reflected in the titles of many physics textbooks. For example, the preface of Goldstein's Classical mechanics explains why the topic is still relevant for physics students.[82] In Concepts of Modern Physics Arthur Beiser starts with a definition of modern physics:[83]

Modern physics began in 1900 with Max Planck’s discovery of the role of energy quantization in blackbody radiation, a revolutionary idea soon followed by Albert Einstein’s equally revolutionary theory of relativity and quantum theory of light.

Kenneth Krane's Modern physics begins a text on quantum and relativity theories with a few pages on deficiencies of classical physics.[84]: 3 E.T. Whittaker's two-volume History of the Theories of Aether and Electricity subtitles volume one The Classical Theories and volume two The Modern Theories (1900–1926).[85]

Contemporary physics

[edit]

Quantum field theory

[edit]
A Feynman diagram representing (left to right) the production of a photon (blue sine wave) from the annihilation of an electron and its complementary antiparticle, the positron. The photon becomes a quarkantiquark pair and a gluon (green spiral) is released.
Richard Feynman's Los Alamos ID badge

As the philosophically inclined continued to debate the fundamental nature of the universe, quantum theories continued to be produced, beginning with Paul Dirac's formulation of a relativistic quantum theory in 1928. However, attempts to quantize electromagnetic theory entirely were stymied throughout the 1930s by theoretical formulations yielding infinite energies. This situation was not considered adequately resolved until after World War II, when Julian Schwinger, Richard Feynman and Sin-Itiro Tomonaga independently posited the technique of renormalization, which allowed for an establishment of a robust quantum electrodynamics (QED).[86]

Meanwhile, new theories of fundamental particles proliferated with the rise of the idea of the quantization of fields through "exchange forces" regulated by an exchange of short-lived "virtual" particles, which were allowed to exist according to the laws governing the uncertainties inherent in the quantum world. Notably, Hideki Yukawa proposed that the positive charges of the nucleus were kept together courtesy of a powerful but short-range force mediated by a particle with a mass between that of the electron and proton. This particle, the "pion", was identified in 1947 as part of what became a slew of particles discovered after World War II. Initially, such particles were found as ionizing radiation left by cosmic rays, but increasingly came to be produced in newer and more powerful particle accelerators.[87]

Outside particle physics, significant advances of the time were:

Unified field theories

[edit]

Einstein deemed that all fundamental interactions in nature can be explained in a single theory. Unified field theories were numerous attempts to "merge" several interactions. One of many formulations of such theories (as well as field theories in general) is a gauge theory, a generalization of the idea of symmetry. Eventually the Standard Model (see below) succeeded in unification of strong, weak, and electromagnetic interactions. All attempts to unify gravitation with something else failed.

Particle physics and the Standard Model

[edit]
The Standard Model
Chien-Shiung Wu worked on parity violation in 1956 and announced her results in January 1957.[88]

When parity was broken in weak interactions by Chien-Shiung Wu in her experiment, a series of discoveries were created thereafter.[89] The interaction of these particles by scattering and decay provided a key to new fundamental quantum theories. Murray Gell-Mann and Yuval Ne'eman brought some order to these new particles by classifying them according to certain qualities, beginning with what Gell-Mann referred to as the "Eightfold Way". While its further development, the quark model, at first seemed inadequate to describe strong nuclear forces, allowing the temporary rise of competing theories such as the S-Matrix, the establishment of quantum chromodynamics in the 1970s finalized a set of fundamental and exchange particles, which allowed for the establishment of a "standard model" based on the mathematics of gauge invariance, which successfully described all forces except for gravitation, and which remains generally accepted within its domain of application.[79]

The Standard Model, based on the Yang–Mills theory[90] groups the electroweak interaction theory and quantum chromodynamics into a structure denoted by the gauge group SU(3)×SU(2)×U(1). The formulation of the unification of the electromagnetic and weak interactions in the standard model is due to Abdus Salam, Steven Weinberg and, subsequently, Sheldon Glashow. Electroweak theory was later confirmed experimentally (by observation of neutral weak currents),[91][92][93][94] and distinguished by the 1979 Nobel Prize in Physics.[95]

Since the 1970s, fundamental particle physics has provided insights into early universe cosmology, particularly the Big Bang theory proposed as a consequence of Einstein's general theory of relativity. However, starting in the 1990s, astronomical observations have also provided new challenges, such as the need for new explanations of galactic stability ("dark matter") and the apparent acceleration in the expansion of the universe ("dark energy").

While accelerators have confirmed most aspects of the Standard Model by detecting expected particle interactions at various collision energies, no theory reconciling general relativity with the Standard Model has yet been found, although supersymmetry and string theory were believed by many theorists to be a promising avenue forward. The Large Hadron Collider, however, which began operating in 2008, has failed to find any evidence that is supportive of supersymmetry and string theory.[96]

Cosmology

[edit]

Cosmology may be said to have become a serious research question with the publication of Einstein's General Theory of Relativity in 1915 although it did not enter the scientific mainstream until the period known as the "Golden age of general relativity".

About a decade later, in the midst of what was dubbed the "Great Debate", Edwin Hubble and Vesto Slipher discovered the expansion of universe in the 1920s measuring the redshifts of Doppler spectra from galactic nebulae. Using Einstein's general relativity, Georges Lemaître and George Gamow formulated what would become known as the Big Bang theory. A rival, called the steady state theory, was devised by Fred Hoyle, Thomas Gold, Jayant Narlikar and Hermann Bondi.

Cosmic microwave background radiation was verified in the 1960s by Arno Allan Penzias and Robert Woodrow Wilson, and this discovery favoured the big bang at the expense of the steady state scenario. Later work was by George Smoot et al. (1989), among other contributors, using data from the Cosmic Background explorer (CoBE) and the Wilkinson Microwave Anisotropy Probe (WMAP) satellites refined these observations. The 1980s (the same decade of the COBE measurements) also saw the proposal of inflation theory by Alan Guth.

Recently the problems of dark matter and dark energy have risen to the top of the cosmology agenda.

Higgs boson

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One possible signature of a Higgs boson from a simulated proton–proton collision. It decays almost immediately into two jets of hadrons and two electrons, visible as lines.

On July 4, 2012, physicists working at CERN's Large Hadron Collider announced that they had discovered a new subatomic particle greatly resembling the Higgs boson, a potential key to an understanding of why elementary particles have mass and indeed to the existence of diversity and life in the universe.[97] For now, some physicists are calling it a "Higgslike" particle.[97] Joe Incandela, of the University of California, Santa Barbara, said, "It's something that may, in the end, be one of the biggest observations of any new phenomena in our field in the last 30 or 40 years, going way back to the discovery of quarks, for example."[97] Michael Turner, a cosmologist at the University of Chicago and the chairman of the physics center board, said:

"This is a big moment for particle physics and a crossroads – will this be the high water mark or will it be the first of many discoveries that point us toward solving the really big questions that we have posed?"

— Michael Turner, University of Chicago[97]

Peter Higgs was one of six physicists, working in three independent groups, who, in 1964, invented the notion of the Higgs field ("cosmic molasses"). The others were Tom Kibble of Imperial College, London; Carl Hagen of the University of Rochester; Gerald Guralnik of Brown University; and François Englert and Robert Brout, both of Université libre de Bruxelles.[97]

Although they have never been seen, Higgslike fields play an important role in theories of the universe and in string theory. Under certain conditions, according to the strange accounting of Einsteinian physics, they can become suffused with energy that exerts an antigravitational force. Such fields have been proposed as the source of an enormous burst of expansion, known as inflation, early in the universe and, possibly, as the secret of the dark energy that now seems to be accelerating the expansion of the universe.[97]

Physical sciences

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With increased accessibility to and elaboration upon advanced analytical techniques in the 19th century, physics was defined as much, if not more, by those techniques than by the search for universal principles of motion and energy, and the fundamental nature of matter. Fields such as acoustics, geophysics, astrophysics, aerodynamics, plasma physics, low-temperature physics, and solid-state physics joined optics, fluid dynamics, electromagnetism, and mechanics as areas of physical research. In the 20th century, physics also became closely allied with such fields as electrical, aerospace and materials engineering, and physicists began to work in government and industrial laboratories as much as in academic settings. Following World War II, the population of physicists increased dramatically, and came to be centered on the United States, while, in more recent decades, physics has become a more international pursuit than at any time in its previous history.

Articles on the history of physics

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On branches of physics

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On specific discoveries

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Historical periods

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See also

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Notes

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References

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Further reading

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Revisions and contributorsEdit on WikipediaRead on Wikipedia
from Grokipedia
The history of physics encompasses the progressive evolution of scientific inquiry into the fundamental principles of , , motion, and the , beginning with ancient philosophical explanations of natural phenomena and advancing through empirical experimentation, mathematical formulation, and revolutionary theoretical paradigms in the . This discipline, one of the oldest academic fields, initially intertwined with astronomy and , transitioned into a distinct during the , and continues to drive discoveries in areas such as and cosmology. In ancient times, from around 650 BCE to 200 CE, early contributions laid foundational concepts across various civilizations, with parallel developments in Near Eastern, Egyptian, Indian, and Chinese traditions alongside Greek natural philosophy. Presocratic philosophers like proposed natural rather than supernatural causes for events, earning him recognition as the "Father of Physics." (384–322 BCE) systematized physics through his theory of four elements (earth, air, fire, water) plus aether, influencing geocentric models and natural motion ideas for centuries. (287–212 BCE) advanced and , formulating the principle of buoyancy, while emerged from and in the 5th–4th centuries BCE, positing indivisible particles as the basis of matter. (ca. 90–168 CE) refined the geocentric system. During the medieval period (5th–15th centuries), Islamic scholars preserved and expanded Greek works, with (965–1040) pioneering experimental and emphasizing reproducibility, bridging ancient ideas to modern methods. (973–1050) contributed to scientific methodology through precise measurements, while other Islamic scholars like integrated spiritual and empirical approaches. These efforts critiqued and refined earlier models, such as Ptolemy's geocentric framework, setting the stage for the . The (16th–18th centuries) marked physics' emergence as an experimental science, with (1473–1543) reviving in 1543, challenging geocentric views. (1571–1630) formulated laws of planetary motion in 1609 and 1619, while (1564–1642) introduced inertial frames and the through observations and falling-body experiments, earning him the title "Father of Modern Physics." (1643–1727) unified these ideas in his 1687 , establishing , universal gravitation, and as core tools. The 19th century expanded into and , with inventing the battery in 1800 and discovering in 1831. James Clerk Maxwell (1831–1879) unified and in his 1864 equations, predicting the as constant. advanced with the first law of energy conservation (1840s) and the second law (1850s) by figures like and William Thomson (Lord Kelvin). Discoveries like X-rays by Wilhelm Röntgen (1895) and the by J.J. Thomson (1897) hinted at subatomic realms. In the 20th century, physics underwent profound transformations with modern theories, as Max Planck (1900) introduced the quantum hypothesis to explain blackbody radiation, and Albert Einstein's 1905 special relativity revealed E=mc2E = mc^2 and time dilation. General relativity (1915) described gravity as spacetime curvature, while nuclear fission was discovered by Lise Meitner and Otto Frisch in 1938. The Standard Model of particle physics emerged by 1975, unifying quantum fields, with milestones like the Higgs boson confirmation at CERN in 2012. Today, physics integrates quantum field theory, cosmology, and experimental tools like the Large Hadron Collider to probe unresolved questions in unification and dark matter.

Ancient physics

Near Eastern and Egyptian foundations

The earliest foundations of physics in the and emerged from practical observations and empirical techniques aimed at understanding and harnessing natural phenomena, particularly in astronomy, , and . In , particularly among the Babylonians, astronomy developed as a tool for timekeeping and prediction, rooted in systematic observations recorded on clay tablets dating back to around 2000 BCE. These tablets, such as those from the city of , document celestial events including planetary positions and lunar phases, enabling the creation of predictive models. Babylonian astronomers employed a (base-60) numerical system, inherited from the Sumerians around 3000 BCE, which facilitated precise calculations for angles and time divisions still used today in degrees and minutes. A key achievement was the development of lunar calendars, which reconciled the of approximately 29.5 days with the solar year through intercalary months added periodically to maintain seasonal alignment. This lunisolar system supported agricultural planning and religious festivals. By the 8th century BCE, Babylonians identified the Saros cycle, a period of about 18 years (223 synodic months) during which lunar and solar s recur in a predictable pattern, with systematic records beginning around 747 BCE. These predictive models, derived from centuries of observations, allowed forecasts of timings with accuracies of 1-2 hours by the 3rd century BCE. Mesopotamian cosmology envisioned a flat disk floating on primordial waters, enclosed by a solid dome-like supported by pillars or mountains, where celestial bodies moved along fixed paths. Early concepts of balance and motion appeared in practical applications, such as standardized weights and measures for , where equilibrium in scales reflected notions of proportional forces and stability in weighing systems established by the BCE. In , physical knowledge advanced through engineering feats and hydraulic management, driven by the 's annual floods. , serving around 2650 BCE, is credited as the first named architect and engineer, designing the at using stacked mastabas of limestone blocks, innovating stone construction techniques like ramps and levers to achieve heights over 200 feet. Pyramid building later evolved with precise alignment to cardinal directions, employing basic surveying tools for leveling and orientation. For flood prediction, Egyptians used nilometers—graduated stone markers or wells along the —to measure rising water levels, correlating them with historical data to anticipate inundation heights and durations from as early as (ca. 2686–2181 BCE). This empirical ensured agricultural fertility by guiding basin designs. Mathematical texts like the Rhind (ca. 1650 BCE) demonstrate practical for land measurement, including methods to calculate areas of triangles and circles using approximations (e.g., circle area as (8/9 )^2), applied to re-survey fields after floods. These techniques emphasized utility over abstraction, laying groundwork for later scientific traditions including Greek astronomy.

Greek natural philosophy

Greek natural philosophy marked a pivotal transition from mythological explanations of the natural world to rational inquiry, influenced briefly by Near Eastern astronomical observations that encouraged systematic speculation about cosmic order. This shift began with the Pre-Socratic philosophers in the 6th century BCE, who sought underlying principles (archai) to explain the origins and transformations of all things without invoking divine intervention. Thales of Miletus (ca. 585 BCE) proposed water as the primary substance from which all matter arises and to which it returns, viewing it as the . Anaximander, his successor, introduced the —an indefinite, eternal, and boundless substance—as the origin of opposites like hot and cold, generating the ordered universe through processes of separation and return governed by justice. Heraclitus emphasized flux and constant change, positing fire as the fundamental element symbolizing transformation, with the (rational principle) underlying the in a dynamic . Philosophical debates intensified around the nature of reality and change, exemplified by ' argument for immutability, where true being is eternal, indivisible, and unchanging, rendering sensory perceptions of motion and alteration illusory. In contrast, the Pythagoreans integrated into , discovering that musical harmonics arise from simple whole-number ratios—such as 2:1 for the and 3:2 for the fifth—revealing numbers as the essence of cosmic harmony and order. Addressing ' denial of change, emerged with and (ca. 400 BCE), who theorized that the universe consists of indivisible atoms moving in a void, differing only in shape, size, and arrangement; this discrete model explained multiplicity and motion without , distinguishing it from continuous substances like those in earlier elemental theories. Aristotle (ca. 350 BCE) synthesized these ideas into a comprehensive system, positing four elements—earth, water, air, and fire—each seeking its natural place (earth at the center, fire at the periphery) due to inherent tendencies toward rest and order. His physics incorporated teleology, where natural motions and changes serve purposeful ends, and explained projectile motion through antiperistasis, the medium's circular displacement sustaining the object's path after the initial impetus. Archimedes (ca. 250 BCE) advanced practical applications, formulating the buoyancy principle in hydrostatics—that a submerged body experiences an upward force equal to the weight of displaced fluid—and the law of the lever, stating equilibrium when moments (force times distance from fulcrum) balance, laying foundations for statics and mechanics.

Indian and Chinese traditions

The school of , founded by Kanada around 600 BCE, developed an early form of positing that the universe consists of indivisible particles called paramāṇu (atoms), which combine to form larger substances through motion and inherent qualities. This system categorized reality into six padārthas (categories), including dravya (substance, such as the four elements and atoms) and karma (motion or action), explaining physical phenomena like combination and separation without invoking a void, in contrast to parallel developments in Greek thought. These ideas integrated with metaphysics, viewing atoms as eternal and motion as a fundamental attribute driving cosmic processes. In the 5th century CE, astronomer advanced cosmological models in his (499 CE), incorporating elements suggestive of by treating planetary motions relative to the Sun while asserting the Earth's axial rotation to account for the apparent daily motion of celestial bodies. This rotation model, where the Earth spins like a , challenged prevailing geocentric views and enabled precise calculations of eclipses and planetary positions, laying groundwork for later . The Sulba Sutras, Vedic texts dating to around 800 BCE, applied geometric principles to construct sacrificial altars, employing base-10 () numbering for measurements and approximations like the to ensure precise proportions, such as √2 ≈ 1.4142135 for diagonal calculations. These works marked early advancements in , using decimal systems for scaling altar designs from squares to circles without explicit zero notation, though zero as a placeholder emerged later in Indian numeral systems. Indian cosmology emphasized vast cyclical time scales, with yugas (epochs) forming a mahayuga of 4.32 million years and a kalpa (day of Brahma) spanning 4.32 billion years, integrating notions of creation, preservation, and dissolution influenced by atomic combinations and motions. This framework viewed physical changes as recurring patterns tied to ethical and cosmic order, contrasting linear Western timelines. The Surya Siddhanta, an influential astronomical treatise from around the 4th–5th century CE, provided detailed calculations for solar, lunar, and planetary positions, including sine tables and eclipse predictions based on epicycle models, serving as a practical handbook for centuries. In ancient , the Mohist school, led by around 400 BCE, explored through experiments on light reflection in mirrors and the principle, while also analyzing levers and pulleys in the Mozi text to explain and distribution. These investigations linked sensory with practical , emphasizing empirical observation in philosophy. Chinese correlative cosmology revolved around wuxing (five phases or elements)—wood, fire, earth, metal, and water—which interacted through cycles of generation and conquest to explain natural transformations, including seasonal changes and material properties. This system influenced early understandings of motion and balance in the physical world, viewing as interdependent rather than isolated. By around 200 BCE, Chinese scholars utilized () devices for , marking the earliest known magnetic compasses that aligned with Earth's field, predating navigational uses. The yin-yang duality, formalized in texts like the by the Warring States period (ca. 400 BCE), conceptualized cosmic balance as complementary opposites driving change, with implications for motion (yang as active ) and stability (yin as receptive), shaping views of forces. In 1088 CE, polymath documented in his , noting that compass needles deviated from by about 4 degrees, providing the first recorded observation of this geomagnetic variation and advancing navigational . Zhang Heng's seismoscope, invented in 132 CE, detected distant earthquakes up to 500 km away using a vessel with dragon heads and toad mouths to indicate direction via dropped balls, relying on inertial mechanics.

Islamic synthesis

During the , scholars synthesized Greek and Indian mathematical traditions, advancing physics through empirical observation, mathematical rigor, and innovative instrumentation. This period, spanning roughly the 8th to 13th centuries, saw the preservation of ancient knowledge alongside original contributions that emphasized experimentation and precise measurement. (c. 780–850 CE) developed systematic algebraic methods in his treatise Al-Kitab al-Mukhtasar fi Hisab al-Jabr wal-Muqabala (c. 820 CE), which provided tools for solving equations applicable to mechanical problems, such as those in and . His work laid foundational techniques for later applications in physics, including calculations of forces and motions in practical devices. Building on Indian arithmetic, al-Khwarizmi promoted the adoption of Hindu-Arabic numerals (0–9) across the Islamic world, facilitating complex computations essential for astronomical and physical analyses. In optics, Ibn al-Haytham (Alhazen, 965–1040 CE) revolutionized the field with his (Book of Optics, 1021 CE), where he experimentally demonstrated the to explain and formulated early laws of through controlled tests on passing between media. His emphasis on testing and quantitative verification marked a shift toward modern scientific methodology in physics. Commentaries on Aristotle's natural philosophy further refined concepts of motion and the soul-body relation. (Ibn Sina, 980–1037 CE) critiqued Aristotelian views in his Al-Shifa (), introducing the "" to argue for the soul's independence from sensory input and bodily perception, influencing later discussions on self-motion and . (Ibn Rushd, 1126–1198 CE), in his extensive commentaries on Aristotle's Physics, challenged aspects of by questioning the role of the medium as a continuous mover, proposing instead that an impressed sustains the object's path, prefiguring impetus theory. Astronomical advancements included refinements to the by (973–1055 CE), who around 1000 CE enhanced its design for precise angular measurements, enabling him to calculate at approximately 39,375 km using and observations from a mountain peak. His work integrated geometry and empirical data to determine planetary positions and geodetic properties. Early emerged in , as seen in Ismail al-Jazari's (1136–1206 CE) The Book of Knowledge of Ingenious Mechanical Devices (1206 CE), which detailed automata and water clocks using crankshafts, cams, and floats to demonstrate principles of force, balance, and periodic motion. Concepts of impetus—an internal force propelling objects—were explored by philosophers like (Ibn Bajjah, d. 1138 CE) and , serving as precursors to Jean Buridan's later formulation in . Specific advances extended to , where hospitals (bimaristans) incorporated precise balances and scales for weighing pharmaceuticals, applying principles of equilibrium and leverage to ensure accurate dosing in treatments. These institutions, such as the 9th-century hospital, integrated physical instrumentation with clinical practice, enhancing empirical .

Medieval and Renaissance transitions

European scholasticism

European scholasticism emerged as a dominant intellectual framework in medieval universities, integrating Aristotelian with Christian doctrine to explain the physical world within a theological context. The scholastic method, characterized by dialectical reasoning and quaestiones disputatae, sought to reconcile pagan with revealed truth, emphasizing qualitative descriptions over quantitative analysis. This approach framed physics—understood as —as a branch of divine wisdom, where natural causes operated under God's ultimate governance. Influences from translated Islamic texts, such as those by and , facilitated the adoption of Aristotelian concepts in during the 12th and 13th centuries. Thomas Aquinas (c. 1225–1274) exemplified this synthesis in his , where he harmonized Aristotle's physics with around 1270. Aquinas argued that could demonstrate God's existence through observable motions and causes in the physical universe, positing an as the prime cause of all change. In his treatment of , he adapted Aristotelian notions of motion, elements, and celestial incorruptibility to affirm creation's order as evidence of , rejecting any conflict between and reason. This framework dominated university curricula, positioning physics as a tool for understanding God's rational design rather than empirical experimentation. A key advancement in scholastic mechanics was the , refined by Jean Buridan (c. 1295–1363) around 1340 at the . Buridan proposed that a continues moving due to an "impetus" impressed upon it by the initial force, rather than requiring continuous propulsion from the air or another agent, as had suggested. This qualitative explanation addressed by attributing sustained velocity to an internal motive quality that gradually diminishes due to resistance and , marking a shift toward internalized causes of motion while remaining compatible with theological views of divine conservation. Buridan's ideas influenced later thinkers, bridging Aristotelian dynamics with emerging kinematic insights. At Oxford's Merton College, the "" in the mid-14th century advanced quantitative reasoning in , building on nominalist principles associated with (c. 1287–1347). Ockham's emphasized observable particulars over universal essences, encouraging precise analysis of motion without metaphysical excess. Around 1330, scholars like William Heytesbury formulated the mean speed theorem, stating that for uniformly accelerated motion, the distance traveled equals that of uniform motion at the average of initial and final velocities. This theorem, derived through logical and geometric arguments, provided a rule for calculating distances in accelerated fall—such as a body reaching the midpoint speed covering the same distance as constant motion at half the final speed—laying groundwork for later while adhering to scholastic qualitative constraints. Scholastic cosmology retained the geocentric Ptolemaic model, adapted to Christian doctrine, envisioning the as a series of concentric carrying planets and stars in uniform circular motion. , composed of the four elements, occupied the immutable , surrounded by ethereal spheres driven by intelligences or God's will, ensuring the heavens' perfection and incorruptibility. This hierarchical structure, detailed in commentaries on Aristotle's De Caelo, underscored divine order, with sublunary changes contrasting celestial eternity, and was taught as integral to . The served as a central hub for scholastic from the early , where curricula mandated Aristotelian texts like Physics and De Caelo alongside theological integration. Faculties structured teaching around lectures, disputations, and quaestiones on topics such as motion, elements, and cosmology, fostering debates that refined impetus and concepts. Paris's arts faculty emphasized logical analysis over observation, training generations in a physics subordinated to , which spread across European universities.

Revival of ancient texts

The fall of in marked a pivotal event in the revival of texts, as Byzantine scholars fled to with invaluable manuscripts preserved in their libraries. This exodus accelerated the flow of classical knowledge into , introducing works on , astronomy, and that had been largely inaccessible during the medieval period. Scholars such as Cardinal Bessarion and settled in Italian cities like and , where they taught Greek and facilitated translations, bridging the gap between Byzantine scholarship and . Building on the foundations of medieval , this influx enriched European intellectual life by providing direct access to original sources rather than Latin translations filtered through intermediaries. A key figure in this translation movement was , who in 1484 published the first complete Latin translation of Plato's extant works, including dialogues that explored and cosmology. Sponsored by the Medici family in , Ficino's efforts at the emphasized the harmony between Platonic thought and , inspiring a broader humanist engagement with ancient ideas. This work not only revived interest in Plato's concepts of the but also encouraged the study of related scientific texts, laying groundwork for empirical inquiries into nature. The invention of Johannes Gutenberg's printing press around 1455 further amplified this revival by enabling the rapid and widespread dissemination of translated and edited ancient texts. While initially used for the , the press soon produced editions of scientific works, such as those by —whose mathematical treatises on levers and were printed in Latin in 1544—and , whose astronomical systems appeared in printed forms like Regiomontanus's 1496 of the . This technological innovation reduced costs and errors in copying, allowing scholars across to access reliable versions of these foundational texts, which spurred advancements in and celestial modeling. Among the key figures benefiting from this environment was Johannes , whose 1474 publication of Ephemerides provided astronomical tables calculated using advanced , drawing on rediscovered Greek methods. 's earlier De Triangulis (1464) systematized plane and , treating it as an independent discipline essential for astronomy, and his printed works exemplified how revived texts fueled mathematical progress. Similarly, the rediscovery of Hero of Alexandria's Pneumatica in Italy, through Byzantine manuscripts translated and printed in the late , reintroduced pneumatic devices and automata, inspiring engineers to explore principles of and described in the original Greek. These recoveries highlighted the shift toward studying ancient empirical descriptions as precursors to modern experimentation.

Pre-revolutionary experiments

The late period marked a shift toward empirical investigation in physics, as scholars and artisans increasingly relied on hands-on experimentation to explore natural phenomena, laying groundwork for the . These efforts, often conducted outside formal academic institutions, emphasized practical mechanics, instrumentation, and observations that challenged Aristotelian traditions. Inspired briefly by the revival of ancient texts such as those of , experimenters focused on tangible demonstrations rather than abstract philosophy. Leonardo da Vinci (1452–1519) exemplified early mechanical studies through his detailed notebooks, where he analyzed as a opposing motion, noting its dependence on load but independence from the apparent contact area in sketches of sliding blocks and wheels around 1500 CE. He also examined gears and levers in designs for machines like cranes and mills, applying principles of to optimize transmission. Da Vinci's investigations into flight involved aerodynamic concepts, such as the role of air resistance in bird wings and mechanisms, based on observations of natural motion. Additionally, his anatomical dissections integrated physics with , exploring levers in muscle-skeleton systems to understand human movement as a mechanical process. In the realm of magnetism and related forces, English physician William Gilbert published in 1600, presenting systematic experiments that established as a distinct natural property of the , which he modeled as a giant . Gilbert's —a spherical —allowed him to replicate behavior and demonstrate magnetic poles, distinguishing it from electrical attraction observed in (which he termed "electric" from the Greek elektron). His work rejected alchemical , emphasizing quantitative observations like dip angles to argue for terrestrial magnetism's role in . Optical innovations emerged with the telescope's invention in 1608 by Dutch spectacle-maker Hans Lippershey, who patented a refracting device using convex and concave lenses to magnify distant objects up to three times. Initial observations with this instrument, conducted by Lippershey and contemporaries like Jacob Metius, revealed enhanced views of landscapes and ships at sea, prompting further refinements in lens grinding among artisan opticians. These early uses demonstrated the potential for , influencing subsequent astronomical applications without immediate theoretical frameworks. Galileo Galilei contributed key devices in the late , including the around 1593, an open-tube apparatus filled with water and air that expanded or contracted with changes, providing qualitative indications of variations. His studies, initiated after observing chandeliers in around 1581 and refined by 1602, revealed the isochronous property—where swing periods remain nearly constant regardless of amplitude for small angles—through timed experiments with bobs of varying lengths. These investigations highlighted periodicity in oscillatory motion, applicable to timekeeping and . Artisan contributions extended empirical physics into practical domains like and warfare. In , Italian metallurgist Vannoccio Biringuccio's De la pirotechnia (1540) detailed advancements in ore extraction, including blasting and water-powered pumps, which improved efficiency in deep shafts and addressed hydrostatic pressures. These techniques, developed by guild craftsmen in regions like , integrated mechanical principles to manage subterranean forces. In , Florentine artisans and engineers produced cannons and studied trajectories during conflicts, employing empirical trials to calibrate ranges and elevations, as seen in the production of munitions that transformed siege warfare. Such hands-on innovations by non-academic practitioners underscored the interplay between technology and physical observation.

Scientific Revolution

Heliocentric astronomy

The heliocentric model marked a pivotal shift in astronomical thought during the early , proposing the Sun as the center of the rather than . In 1543, published , articulating a heliocentric where and other planets orbit the Sun, thereby simplifying by eliminating the Ptolemaic equant—a device that allowed non-uniform motion in epicycle models. This approach explained retrograde motion not as actual planetary reversals but as an arising from 's faster orbital speed overtaking slower outer planets. Copernicus retained circular orbits with epicycles, yet his system reduced the complexity of geocentric frameworks and aligned planetary periods with their distances from the Sun. Building on Copernicus's ideas, , a Lutheran , played a crucial role in disseminating the theory through his Narratio prima (1540), an introductory abstract that outlined the heliocentric framework and urged publication of Copernicus's full work. However, the model faced significant opposition from the and , who viewed it as conflicting with literal interpretations of Scripture, such as passages in and implying a stationary and moving Sun. Figures like criticized the theory in 1539 as contrary to biblical accounts, while expressed reservations in sermons, though evidence of direct condemnation remains debated. This resistance delayed widespread acceptance, framing heliocentrism initially as a mathematical rather than physical reality. Tycho Brahe's meticulous observations from the 1570s to 1590s provided the empirical foundation needed to refine heliocentric models, conducted at his observatory on the island of Hven without telescopes, achieving unprecedented precision through large, fixed instruments like mural quadrants and sextants. These naked-eye measurements, accurate to within arcminutes, cataloged planetary positions—particularly Mars—over two decades, surpassing prior data in detail and reliability. Brahe's work, though adhering to a geo-heliocentric system, supplied the high-quality dataset essential for subsequent advancements. Johannes Kepler, utilizing Brahe's observations, formulated three laws of planetary motion that solidified the heliocentric paradigm. In 1609, Kepler's first law stated that planets orbit the Sun in ellipses with the Sun at one focus, departing from circular assumptions and fitting Mars's path precisely. His second law, also published in 1609, asserted that a line connecting a planet to the Sun sweeps out equal areas in equal times, implying variable orbital speeds—faster near the Sun and slower farther away. By 1619, in Harmonices Mundi, Kepler introduced the third law: the square of a planet's orbital period TT is proportional to the cube of its semi-major axis aa, expressed as T2a3,T^2 \propto a^3, revealing a harmonic relation among planetary orbits independent of mass. These laws, derived mathematically from observational data, provided a quantitative framework for heliocentric astronomy, influencing future celestial mechanics.

Experimental mechanics

The experimental mechanics of the Scientific Revolution marked a pivotal departure from Aristotelian qualitative descriptions of motion, emphasizing precise measurements and mathematical quantification to investigate forces and terrestrial dynamics. Pioneered by figures like , this approach involved controlled experiments to test hypotheses about and periodicity, replacing appeals to natural places or teleological causes with empirical data. This methodological shift facilitated the development of as a quantitative , grounded in repeatable observations rather than philosophical deduction. Galileo conducted experiments around 1604 to study the motion of falling bodies, using bronze balls rolling down grooved wooden ramps to slow the descent and measure distances with a for timing. These trials revealed that the distance traveled by a uniformly accelerating body is proportional to the square of the time elapsed, expressed in modern notation as s=12gt2s = \frac{1}{2} g t^2, where ss is distance, tt is time, and gg is . Complementing this, Galileo's studies from 1603–1609 demonstrated isochronism—the property that the period of oscillation depends only on the length of the pendulum, not its or bob mass—providing a reliable method for timing experiments and challenging Aristotelian views on natural . In his seminal work Discorsi e Dimostrazioni Matematiche intorno a Due Nuove Scienze (1638), Galileo synthesized these findings into the foundations of and the , detailing theorems on , uniform , and structural resistance derived from his terrestrial experiments. The text's dialogues illustrate how empirical data from inclined planes and pendula underpin mathematical models of and resistance, establishing as an experimental discipline. Galileo's , refined in 1609, further advanced experimental precision through observations like the 1610 discovery of Jupiter's four moons and the , which, while primarily astronomical, informed mechanical understandings of orbital dynamics by supporting heliocentric models through quantifiable positional data. Evangelista Torricelli extended this experimental ethos in 1643 by inventing the mercury , a device that measured by observing the height of a mercury column in a sealed tube inverted in a dish of mercury. This innovation not only quantified the "weight" of air—demonstrating it supported the column up to about 76 cm at —but also created a measurable above the mercury, refuting Aristotelian horror vacui and advancing as a branch of experimental . Torricelli's work, building on Galileo's legacy, underscored the role of in revealing invisible forces acting on .

Newtonian synthesis

Isaac Newton's Philosophiæ Naturalis Principia Mathematica, published in 1687, marked a pivotal unification of terrestrial and celestial mechanics, laying the groundwork for classical physics. In this seminal work, Newton formulated three laws of motion that describe the fundamental principles governing physical interactions. The first law states that an object remains at rest or in uniform motion unless acted upon by an external force, establishing the concept of inertia. The second law quantifies the relationship between force, mass, and acceleration as F=maF = ma, where force is the product of mass and acceleration. The third law asserts that for every action, there is an equal and opposite reaction, ensuring conservation in interactions. Complementing these, Newton proposed the law of universal gravitation, which posits that every particle attracts every other with a force proportional to the product of their masses and inversely proportional to the square of the distance between them, expressed as F=Gm1m2r2F = G \frac{m_1 m_2}{r^2}, where GG is the gravitational constant. This synthesis extended gravitational attraction from apples to planets, unifying diverse phenomena under a single mathematical framework. To derive the trajectories of celestial bodies, Newton developed the , an early form of , during the 1660s, which he applied extensively in the Principia for calculating orbits and perturbations. His fluxional notation facilitated the of instantaneous rates of change, essential for modeling continuous motion in gravitational fields. This innovation sparked a bitter priority dispute with , who independently developed a differential and integral with superior notation; the controversy, fueled by national rivalries, persisted into the early and divided European mathematical communities. Beyond mechanics, Newton's contributions extended to optics, detailed in his Opticks published in 1704. Through experiments with prisms, he demonstrated that white light decomposes into a spectrum of colors, refuting the prevailing view that color arises from modification of white light and instead showing it as an inherent property of rays. Newton advocated a , proposing that light consists of small particles traveling in straight lines, which explained phenomena like and dispersion based on varying particle velocities in media. These findings not only advanced understanding of vision and color but also influenced instrument design, such as his . Newton applied his gravitational theory to specific astronomical problems, notably developing a that accounted for the Moon's irregular orbit due to perturbations from the Sun and Earth's . In Book III of the Principia, he analyzed trajectories, treating them as elliptical orbits under inverse-square gravitation, which enabled predictions of their paths and return periods; this work inspired Edmund Halley's later successful forecast of the named after him. Such applications demonstrated the of Newton's framework, bridging observation and theory in astronomy. Philosophically, Newton's approach emphasized empirical rigor and mathematical deduction, encapsulated in his famous query from the 1713 edition of the Principia: hypotheses non fingo ("I frame no hypotheses"), rejecting speculative causes in favor of deriving laws directly from phenomena. This stance promoted methodological naturalism, insisting that natural philosophy explain the universe through observable, quantifiable mechanisms without invoking supernatural agents, profoundly shaping scientific inquiry by prioritizing evidence over conjecture. Newton's synthesis built upon the empirical foundations of Galileo and Kepler, integrating kinematics and planetary laws into a cohesive system.

18th-century classical foundations

Celestial mechanics

Celestial mechanics in the 18th century advanced the application of Newtonian gravity to the intricate motions within the solar system, focusing on perturbations and multi-body interactions to predict planetary and lunar paths with greater precision. Leonhard Euler made significant early contributions to tackling the , particularly in the 1740s, by developing approximations for the gravitational interactions among the Sun, , and , which laid groundwork for more accurate orbital calculations. His , first detailed in the 1753 publication Theoria motus lunae, provided formulas for lunar tables that supported navigation for over a century, while his 1772 second refined these approximations using successive iterations and dual coordinate systems to model the Moon's irregular orbit under solar perturbations. Joseph-Louis Lagrange further refined celestial mechanics through his analytical approach, introducing generalized coordinates that reformulated Newtonian dynamics in terms of variational principles, enabling more flexible treatments of complex systems without relying on Cartesian frameworks. In 1772, Lagrange analyzed the restricted three-body problem and identified stable equilibrium points, now known as Lagrange points, which demonstrated the potential for long-term orbital stability in perturbed systems; this work directly explained the positioning and stability of Trojan asteroids sharing Jupiter's orbit at the L4 and L5 points. Pierre-Simon Laplace's multi-volume Mécanique Céleste (1799–1825) synthesized these efforts into a comprehensive framework, employing to quantify small deviations in planetary orbits caused by mutual gravitational influences, thereby confirming the long-term . Within this work, Laplace also elaborated on the , positing that the solar system formed from a rotating cloud of gas that contracted and cooled, ejecting rings of material that coalesced into planets, providing a dynamical explanation for the system's architecture. These theoretical advancements coincided with key observational discoveries that expanded the known solar system and tested the models. In 1781, identified as a while surveying the constellation Gemini with a homemade , marking the first planetary discovery since antiquity and doubling the known extent of the system at a distance twice that of Saturn. Central to these developments were analytical tools like series expansions, which Euler, Lagrange, and Laplace employed to approximate solutions for perturbed orbits by expanding gravitational potentials into infinite series of periodic terms, allowing computation of secular variations and close approaches without exact integration of the nonlinear equations.

Fluid dynamics and waves

In the , the study of emerged as a key extension of Newtonian , treating as continuous media to analyze motion under , , and velocity. Building on Newton's early ideas in Principia about fluid resistance, scientists developed mathematical frameworks for steady and unsteady flows, laying groundwork for applications like and . This period marked a shift from empirical observations to predictive equations, emphasizing conservation principles without invoking initially. Daniel Bernoulli's Hydrodynamica (1738) introduced a foundational principle of energy conservation for incompressible fluids along streamlines, stating that the sum of pressure, gravitational potential, and kinetic energy remains constant: p+ρgh+12ρv2=constant,p + \rho g h + \frac{1}{2} \rho v^2 = \text{constant}, where pp is pressure, ρ\rho is density, gg is gravity, hh is height, and vv is velocity. This equation, derived from integrating Newton's laws along fluid paths, explained phenomena like fluid acceleration under pressure gradients and found early use in ship hydrodynamics to optimize hull shapes for reduced drag. For instance, Bernoulli's work influenced designs for faster vessels by predicting how velocity increases lower pressure around curved surfaces, aiding propulsion efficiency. Leonhard Euler advanced this continuum approach in 1757 with his equations for , formalizing the balance for fluids as a set of partial differential equations: ρ(vt+(v)v)=p+ρg,\rho \left( \frac{\partial \mathbf{v}}{\partial t} + (\mathbf{v} \cdot \nabla) \mathbf{v} \right) = -\nabla p + \rho \mathbf{g}, neglecting viscous terms to model ideal fluids. These equations generalized to unsteady, three-dimensional flows and were applied to problems like water flow in channels and ship resistance, where Euler calculated wave-making drag for . Parallel developments in wave theory addressed vibrations and propagation, starting with Brook Taylor's 1714 analysis of musical string vibrations. Taylor derived the transverse displacement of a taut string under tension, showing that oscillation frequency depends on tension and linear density, providing a mathematical basis for harmonic motion in continuous media. This work paved the way for Jean le Rond d'Alembert's 1747 , which governs one-dimensional propagation: 2ut2=c22ux2,\frac{\partial^2 u}{\partial t^2} = c^2 \frac{\partial^2 u}{\partial x^2}, where uu is displacement, tt is time, xx is position, and cc is wave speed. D'Alembert solved it using characteristic methods, revealing waves as superpositions of forward and backward traveling components, applicable to sound in air columns. These theories found practical application in acoustics, particularly organ pipe design, where Euler extended Bernoulli's ideas to model and in cylindrical pipes. Euler's Dissertation De Sono (1727, expanded later) analyzed end corrections and harmonic overtones in open and closed pipes, explaining why organ tones produce rich spectra from at the pipe mouth. This informed 18th-century organ builders in tuning pipes for church instruments, balancing fundamental frequencies with partials for tonal clarity. In atmospheric studies, George Hadley's 1735 paper proposed a meridional circulation cell to explain , attributing their easterly direction to deflecting equatorward surface flow. This model, now known as the , described rising air at the , poleward drift aloft, and sinking at about 30° latitude, with return flow as —integrating with Coriolis effects for global wind patterns. Such insights briefly informed celestial perturbation models by analogy to fluid drag in .

Early heat theories

In the early 18th century, advancements in thermometry laid the groundwork for quantitative studies of . developed the in 1714, introducing a standardized scale that marked 32°F as the freezing point of and 212°F as its under standard conditions, enabling more precise measurements than previous alcohol-based devices. This instrument facilitated experiments distinguishing as a measurable , separate from mere sensation. Joseph Black's investigations in the 1760s advanced the understanding of by differentiating between , which causes perceptible changes, and , which is absorbed or released during phase transitions without altering . In 1762, Black demonstrated that melting ice requires a significant quantity of —later quantified as 334 J/g—without raising its , a discovery made through careful using mixtures of substances at different temperatures. He also introduced the concept of specific heats, showing that different materials require varying amounts of to achieve the same increase; for instance, water has a specific heat of 1 cal/g·°C, higher than metals like lead at 0.031 cal/g·°C. These distinctions were pivotal in shifting from a vague quality to a quantifiable entity in chemical and physical processes. The decline of the in the late further integrated into chemical frameworks. Proposed earlier by , phlogiston was imagined as a fire-like substance released during , but Antoine Lavoisier's experiments from the onward revealed conservation and the role of oxygen, disproving the theory by 1780 as combustion involved gain rather than loss of weight. This paved the way for , where Lavoisier in the 1780s conceptualized as an indestructible, weightless fluid called "caloric" that flows between bodies to equalize s, analogous to fluids in . Lavoisier and used ice calorimeters to measure heat capacities, confirming that caloric's quantity in a body determines its and enabling precise assessments of in reactions. Challenges to caloric theory emerged through mechanical experiments. In 1798, Benjamin Thompson, Count Rumford, observed during cannon boring in Munich that friction between a blunt steel borer and brass produced enough heat to boil approximately 19 pounds of water, with no evident limit to the heat generated despite minimal material removal—contradicting the idea of caloric being stored or released from matter. Rumford argued that heat arises from motion, not a fluid, as the process converted mechanical work indefinitely into thermal effects without caloric depletion. These instruments and concepts marked the transition from heat as a subtle substance to a form of , influencing early thermodynamic principles.

19th-century unification

Lagrangian and Hamiltonian mechanics

In the late , developed a reformulation of that shifted emphasis from forces to principles, culminating in his seminal work Mécanique Analytique published in 1788. This approach generalized Newtonian mechanics by employing variational principles, which posit that the path of a system minimizes or extremizes a quantity known as the action, defined as the integral of the Lagrangian over time. Central to this framework is , extended by Lagrange to handle constraints through , allowing for the derivation of without resolving individual forces. The Lagrangian function itself is expressed as L=TVL = T - V, where TT represents the and VV the of the system. Building on this foundation, introduced a complementary in 1834, transforming into a symplectic structure suited for analytical solutions and later quantum developments. similarly relies on the action integral but employs and momenta, leading to the Hamilton-Jacobi and the : qi˙=Hpi\dot{q_i} = \frac{\partial H}{\partial p_i} and pi˙=Hqi\dot{p_i} = -\frac{\partial H}{\partial q_i}, where H=T+VH = T + V is the Hamiltonian, representing the total energy in —a multidimensional space of positions and momenta. This perspective enabled a deeper understanding of dynamical systems' evolution and conserved quantities. Lagrangian and Hamiltonian methods found immediate applications in , where they simplified the treatment of rotations and precessions, as seen in Lagrange's analysis of the for top motion. In , these tools revisited planetary perturbations, offering more efficient computational paths than direct Newtonian integrations, thus aiding 19th-century calculations. A key advance came in the 1840s through , who extended Hamilton's approach by introducing —now known as the Jacobi determinant—for evaluating integrals of motion, facilitating the in complex systems and uncovering additional conserved quantities. Philosophically, these developments reinforced in by highlighting conservation laws—such as , , and —as Noether-like symmetries inherent to the Lagrangian, emphasizing the predictability of physical systems from initial conditions.

Electromagnetic theory

The development of electromagnetic theory in the marked a pivotal unification of , , and , transforming physics from disparate phenomena into a coherent field theory. This era began with experimental discoveries linking electric currents to magnetic effects, progressed through quantitative laws governing induction and electrochemical processes, and culminated in a mathematical framework that predicted electromagnetic waves traveling at the . In 1800, invented the , the first device to produce a steady from chemical reactions involving alternating and discs separated by brine-soaked cardboard, providing a reliable source for subsequent electromagnetic experiments. Building on this, Danish physicist discovered in 1820 that an flowing through a wire deflects a nearby needle, demonstrating that generates ; specifically, during a lecture, Ørsted observed the needle's perpendicular alignment to the current-carrying wire, with the deflection circling the wire in a manner dependent on current direction. This breakthrough, detailed in Ørsted's pamphlet Experimenta circa effectum conflictus electrici in acum magneticam, established the fundamental connection between the two forces, overturning prior assumptions of their independence. Inspired by Ørsted's finding, rapidly formulated a mathematical description of the magnetic forces between current-carrying wires in 1820–1826. In his seminal work Mémoire sur la théorie mathématique des phénomènes électrodynamiques uniquement déduite de l'expérience, derived the force law between two current elements, showing that parallel currents attract and antiparallel ones repel, with the force proportional to the product of the currents and inversely proportional to the square of their separation distance, modulated by angular factors. 's electrodynamics treated currents as flows of an incompressible fluid, laying the groundwork for vectorial field descriptions and influencing later theoretical syntheses. Michael Faraday advanced these ideas through experiments on , announced in 1831. In his Experimental Researches in Electricity (first series, 1832), Faraday demonstrated that a changing induces an in a nearby circuit, as shown by a galvanometer deflection when he moved a relative to a coil or varied current in a primary circuit linked to a secondary one via an ; the induced current's direction opposed the change in , per Lenz's later rule. Faraday conceptualized these effects using "lines of force," invisible curves representing and intensities, where field strength is proportional to line density, providing an intuitive, non-mathematical precursor to vector fields. Faraday also established the laws of electrolysis in 1833–1834, quantifying the relationship between and . His first law states that the of a substance altered at an is directly proportional to the quantity of passed; the second law asserts that for a given quantity of , the deposited is proportional to the substance's . These principles introduced the , approximately 96,485 coulombs per mole of electrons, linking to atomic-scale chemical changes and supporting the electrochemical equivalence of elements. The theoretical pinnacle arrived with James Clerk Maxwell's 1865 paper A Dynamical Theory of the , which synthesized prior work into four partial differential equations governing . are: [E](/page/E!)=ρε0\nabla \cdot \mathbf{[E](/page/E!)} = \frac{\rho}{\varepsilon_0} [B](/page/Listofpunkrapartists)=0\nabla \cdot \mathbf{[B](/page/List_of_punk_rap_artists)} = 0 ×[E](/page/E!)=[B](/page/Listofpunkrapartists)t\nabla \times \mathbf{[E](/page/E!)} = -\frac{\partial \mathbf{[B](/page/List_of_punk_rap_artists)}}{\partial t} ×[B](/page/Listofpunkrapartists)=μ0J+μ0ε0[E](/page/E!)t\nabla \times \mathbf{[B](/page/List_of_punk_rap_artists)} = \mu_0 \mathbf{J} + \mu_0 \varepsilon_0 \frac{\partial \mathbf{[E](/page/E!)}}{\partial t} The first describes electric field divergence from charge density ρ\rho, with ε0\varepsilon_0 as the permittivity of free space; the second indicates no magnetic monopoles, as magnetic flux B\mathbf{B} has zero divergence; the third captures Faraday's induction law via curl of electric field E\mathbf{E}; and the fourth extends Ampère's law with the displacement current term μ0ε0Et\mu_0 \varepsilon_0 \frac{\partial \mathbf{E}}{\partial t}, where μ0\mu_0 is vacuum permeability and J\mathbf{J} is current density, ensuring consistency in non-steady states. From these equations, Maxwell derived the wave equation for electromagnetic disturbances, propagating at speed c=1μ0ε0c = \frac{1}{\sqrt{\mu_0 \varepsilon_0}}
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