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Joseph Fourier - Wikiquote
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class="vector-toc-numb">1</span> <span>Quotes</span> </div> </a> <button aria-controls="toc-Quotes-sublist" class="cdx-button cdx-button--weight-quiet cdx-button--icon-only vector-toc-toggle"> <span class="vector-icon mw-ui-icon-wikimedia-expand"></span> <span>Toggle Quotes subsection</span> </button> <ul id="toc-Quotes-sublist" class="vector-toc-list"> <li id="toc-The_Analytical_Theory_of_Heat_(1822,_Tr._1878)" class="vector-toc-list-item vector-toc-level-2"> <a class="vector-toc-link" href="#The_Analytical_Theory_of_Heat_(1822,_Tr._1878)"> <div class="vector-toc-text"> <span class="vector-toc-numb">1.1</span> <span><i>The Analytical Theory of Heat</i> (1822, Tr. 1878)</span> </div> </a> <ul id="toc-The_Analytical_Theory_of_Heat_(1822,_Tr._1878)-sublist" class="vector-toc-list"> </ul> </li> <li id="toc-"On_the_Temperatures_of_the_Terrestrial_Sphere_and_the_Planetary_Spaces"_(1827,_Tr._1837)" class="vector-toc-list-item vector-toc-level-2"> <a class="vector-toc-link" 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</div> </div> </nav> <h1 id="firstHeading" class="firstHeading mw-first-heading"><span class="mw-page-title-main">Joseph Fourier</span></h1> <div id="p-lang-btn" class="vector-dropdown mw-portlet mw-portlet-lang" > <input type="checkbox" id="p-lang-btn-checkbox" role="button" aria-haspopup="true" data-event-name="ui.dropdown-p-lang-btn" class="vector-dropdown-checkbox mw-interlanguage-selector" aria-label="Go to an article in another language. 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mw-parser-output" lang="en" dir="ltr"><figure class="mw-default-size mw-halign-right" typeof="mw:File/Thumb"><a href="/wiki/File:Grenoble_-_ancien_%C3%A9v%C3%AAch%C3%A9_-_Joseph_Fourier.JPG" class="mw-file-description"><img src="//upload.wikimedia.org/wikipedia/commons/thumb/2/26/Grenoble_-_ancien_%C3%A9v%C3%AAch%C3%A9_-_Joseph_Fourier.JPG/220px-Grenoble_-_ancien_%C3%A9v%C3%AAch%C3%A9_-_Joseph_Fourier.JPG" decoding="async" width="220" height="330" class="mw-file-element" srcset="//upload.wikimedia.org/wikipedia/commons/thumb/2/26/Grenoble_-_ancien_%C3%A9v%C3%AAch%C3%A9_-_Joseph_Fourier.JPG/330px-Grenoble_-_ancien_%C3%A9v%C3%AAch%C3%A9_-_Joseph_Fourier.JPG 1.5x, //upload.wikimedia.org/wikipedia/commons/thumb/2/26/Grenoble_-_ancien_%C3%A9v%C3%AAch%C3%A9_-_Joseph_Fourier.JPG/440px-Grenoble_-_ancien_%C3%A9v%C3%AAch%C3%A9_-_Joseph_Fourier.JPG 2x" data-file-width="2124" data-file-height="3186" /></a><figcaption>Profound study of nature is the most fertile source of mathematical discoveries.</figcaption></figure> <p><b><a href="https://en.wikipedia.org/wiki/Joseph_Fourier" class="extiw" title="w:Joseph Fourier">Jean Baptiste Joseph Fourier</a></b> (<a href="/wiki/March_21" title="March 21">March 21</a>, <a href="/wiki/1768" class="mw-disambig" title="1768">1768</a> – <a href="/wiki/May_16" title="May 16">May 16</a>, <a href="/wiki/1830" class="mw-disambig" title="1830">1830</a>) was a French mathematician and physicist who is best known for initiating the investigation of <a href="https://en.wikipedia.org/wiki/Fourier_series" class="extiw" title="w:Fourier series">Fourier series</a> and their application to problems of <a href="https://en.wikipedia.org/wiki/heat_flow" class="extiw" title="w:heat flow">heat flow</a>. The <a href="https://en.wikipedia.org/wiki/Fourier_transform" class="extiw" title="w:Fourier transform">Fourier transform</a> is also named in his honor. </p> <dl><dd>See also: <i><a href="/wiki/The_Analytic_Theory_of_Heat" title="The Analytic Theory of Heat">The Analytic Theory of Heat</a></i></dd></dl> <meta property="mw:PageProp/toc" /> <div class="mw-heading mw-heading2"><h2 id="Quotes">Quotes</h2><span class="mw-editsection"><span class="mw-editsection-bracket">[</span><a href="/w/index.php?title=Joseph_Fourier&action=edit&section=1" title="Edit section: Quotes"><span>edit</span></a><span class="mw-editsection-bracket">]</span></span></div> <ul><li>I regarded these events as the customary disturbances of a state in which a new usurper tends to pluck the sceptre from his predecessor. ...<b>As the <a href="/wiki/Natural_rights" title="Natural rights">natural</a> ideas of <a href="/wiki/Equality" title="Equality">equality</a> were developed it was possible to conceive the <a href="/wiki/Sublime_(philosophy)" title="Sublime (philosophy)">sublime</a> hope of establishing among us a <a href="/wiki/Freedom" title="Freedom">free</a> <a href="/wiki/Government" title="Government">government</a> exempt from <a href="/wiki/King" title="King">kings</a> and <a href="/wiki/Priest" title="Priest">priests</a> and to free from this double yoke the long usurped soil of Europe. I readily became enamored of this cause... the greatest and most <a href="/wiki/Beauty" title="Beauty">beautiful</a> which any nation has ever undertaken.</b> ...You will judge whether it is I or my adversaries who are terrorists and persecutors. ...<b>I accuse them of having violated ...all the rules of natural justice, of being <a href="/wiki/Ignorance" title="Ignorance">ignorant</a> and <a href="/wiki/Evil" title="Evil">evil</a>, of <a href="/wiki/Profanity" title="Profanity">profaning</a> the words of <a href="/wiki/Humanity" title="Humanity">humanity</a> and <a href="/wiki/Justice" title="Justice">justice</a> in invoking them, just as <a href="/wiki/Tyranny" title="Tyranny">tyranny</a> was organized in the name of <a href="/wiki/Liberty" title="Liberty">liberty</a>. Finally, of having given themselves up to a boundless <a href="/wiki/French_Revolution" title="French Revolution">revolutionary fury</a> which ought to cover then with <a href="/wiki/Disgrace" title="Disgrace">disgrace</a> and <a href="/wiki/Scorn" title="Scorn">scorn</a>.</b> <ul><li>Letter to Edmé Pierre Alexanre Villetard (June/July, 1795) from prison, as quoted by <a href="https://en.wikipedia.org/wiki/John_Herivel" class="extiw" title="wikipedia:John Herivel">John Herivel</a>, <i>Joseph Fourier—The Man and the Physicist</i> (1975) pp. 280-285 (also see p. 27).</li></ul></li></ul> <ul><li>I am sorry not to have known the mathematician who first made use of this method because I would have cited him. Regarding the researches of <a href="/wiki/Jean_le_Rond_d%27Alembert" title="Jean le Rond d'Alembert">d'Alembert</a> and <a href="/wiki/Leonhard_Euler" title="Leonhard Euler">Euler</a> could one not add that if they knew this expansion they made but a very imperfect use of it. They were both persuaded that an arbitrary and discontinuous function could never be resolved in series of this kind, and it does not seem that anyone had developed a constant in cosines of multiple arcs, the first problem which I had to solve in the theory of heat.</li> <li>Letter, quoted by Vladimir Dobrushkin, <a rel="nofollow" class="external text" href="https://www.cfm.brown.edu/people/dobrush/am34/Mathematica/ch5/joseph.html">"Biography of Joseph Fourier"</a> & Elena Presitini, <i>The Evolution of Applied Harmonic Analysis</i> (2004) p. 42.</li></ul> <div class="mw-heading mw-heading3"><h3 id="The_Analytical_Theory_of_Heat_(1822,_Tr._1878)"><span id="The_Analytical_Theory_of_Heat_.281822.2C_Tr._1878.29"></span><i>The Analytical Theory of Heat</i> (1822, Tr. 1878)</h3><span class="mw-editsection"><span class="mw-editsection-bracket">[</span><a href="/w/index.php?title=Joseph_Fourier&action=edit&section=2" title="Edit section: The Analytical Theory of Heat (1822, Tr. 1878)"><span>edit</span></a><span class="mw-editsection-bracket">]</span></span></div> <dl><dd><small>Tr. <a href="https://en.wikipedia.org/wiki/Alexander_Freeman_(mathematician)" class="extiw" title="w:Alexander Freeman (mathematician)">Alexander Freeman</a>, of Fourier's <i>Théorie Analytique de la Chaleur</i> (1822) <a rel="nofollow" class="external text" href="http://www.archive.org/details/analyticaltheory00fourrich">Full text online</a></small></dd></dl> <figure class="mw-default-size mw-halign-right" typeof="mw:File/Thumb"><a href="/wiki/File:Chest_radiograph_2D_Fourier_Spectrum.jpg" class="mw-file-description"><img src="//upload.wikimedia.org/wikipedia/commons/thumb/5/5f/Chest_radiograph_2D_Fourier_Spectrum.jpg/220px-Chest_radiograph_2D_Fourier_Spectrum.jpg" decoding="async" width="220" height="118" class="mw-file-element" srcset="//upload.wikimedia.org/wikipedia/commons/thumb/5/5f/Chest_radiograph_2D_Fourier_Spectrum.jpg/330px-Chest_radiograph_2D_Fourier_Spectrum.jpg 1.5x, //upload.wikimedia.org/wikipedia/commons/thumb/5/5f/Chest_radiograph_2D_Fourier_Spectrum.jpg/440px-Chest_radiograph_2D_Fourier_Spectrum.jpg 2x" data-file-width="599" data-file-height="322" /></a><figcaption>This difficult science is formed slowly, but it preserves every principle which it has once acquired; it grows and strengthens itself incessantly in the midst of the many variations and errors of the human mind.</figcaption></figure> <ul><li>The analytical equations, unknown to the ancient geometers, which <a href="/wiki/Ren%C3%A9_Descartes" title="René Descartes">Descartes</a> was the first to introduce into the study of curves and surfaces, are not restricted to the properties of figures, and to those properties which are the object of rational mechanics; they extend to all general phenomena. There cannot be a language more universal and more simple, more free from errors and from obscurities, that is to say more worthy to express the invariable relations of natural things.<br />Considered from this point of view, <a href="/wiki/Mathematical_analysis" title="Mathematical analysis">mathematical analysis</a> is as extensive as nature itself; it defines all perceptible relations, measures times, spaces, forces, temperatures; this difficult science is formed slowly, but it preserves every principle which it has once acquired; it grows and strengthens itself incessantly in the midst of the many variations and errors of the human mind.<br />Its chief attribute is clearness; it has no marks to express confused notions. It brings together phenomena the most diverse, and discovers the hidden analogies which unite them. <ul><li>Preliminary Discourse, p.7 Note: often quoted as <i>Mathematics [or mathematical analysis] compares the most diverse phenomena and discovers the secret analogies that unite them.</i></li></ul></li></ul> <ul><li>Primary causes are unknown to us; but are subject to simple and constant laws, which may be discovered by observation, the study of them being the object of natural philosophy. <br /> Heat, like gravity, penetrates every substance of the universe, its rays occupy all parts of space. The object of our work is to set forth the mathematical laws which this element obeys. The theory of heat will hereafter form one of the most important branches of general physics. <ul><li>Ch. 1, p. 1</li></ul></li></ul> <ul><li>If we consider further the manifold relations of this mathematical theory to civil uses and the technical arts, we shall recognize completely the extent of its applications. It is evident that it includes an entire series of distinct phenomena, and that the study of it cannot be omitted without losing a notable part of the science of nature. <br /> <b>The principles of the theory are derived, as are those of rational mechanics, from a very small number of primary facts</b>, the causes of which are not considered by geometers, but which they admit as the results of common observations confirmed by all experiment. <ul><li>Ch. 1, p. 6</li></ul></li></ul> <ul><li><b>Profound study of nature is the most fertile source of mathematical discoveries.</b> <ul><li>Ch. 1, p. 7</li></ul></li></ul> <div class="mw-heading mw-heading3"><h3 id=""On_the_Temperatures_of_the_Terrestrial_Sphere_and_the_Planetary_Spaces"_(1827,_Tr._1837)"><span id=".22On_the_Temperatures_of_the_Terrestrial_Sphere_and_the_Planetary_Spaces.22_.281827.2C_Tr._1837.29"></span>"On the Temperatures of the Terrestrial Sphere and the Planetary Spaces" (1827, Tr. 1837)</h3><span class="mw-editsection"><span class="mw-editsection-bracket">[</span><a href="/w/index.php?title=Joseph_Fourier&action=edit&section=3" title="Edit section: "On the Temperatures of the Terrestrial Sphere and the Planetary Spaces" (1827, Tr. 1837)"><span>edit</span></a><span class="mw-editsection-bracket">]</span></span></div> <dl><dd><small><i>American Journal of Science, &c</i>., Vol. 32, No. 1, pp. 1-20. Tr. <a href="https://en.wikipedia.org/wiki/Ebenezer_Burgess" class="extiw" title="wikipedia:Ebenezer Burgess">Ebenezer Burgess</a> of Fourier's paper "M´emoire sur les Temp´eratures du Globe Terrestre et des Espaces Plan´etaires" (1827) <a rel="nofollow" class="external text" href="https://nsdl.library.cornell.edu/websites/wiki/index.php/PALE_ClassicArticles/archives/classic_articles/issue1_global_warming/n1-Fourier_1824corrected.pdf">Full text online.</a></small></dd></dl> <ul><li>The question of <a href="/wiki/Earth" title="Earth">terrestrial</a> temperature, one of the most remarkable and difficult in <a href="/wiki/Natural_philosophy" title="Natural philosophy">natural philosophy</a>... I have... condensed in a single essay... the results of this theory. The analytical details... I have already published. I was specially desirous of presenting... a complete view of the phenomena and the mathematical relations... between them.</li></ul> <ul><li>The heat of the earth is derived from three sources...<br />1. ...[S]olar rays; the unequal distribution of which causes diversities of climate.<br />2. ...[T]he common temperature of the planetary spaces; being exposed to the radiation from the innumerable stars which surround the solar system.<br />3. The earth preserves in its interior that primitive heat which it had at the time of the first formation of the planets. ...We will show ...the principle features of these phenomena.</li></ul> <ul><li>The solar system is situated in a region of the universe, every point of which has a common and constant temperature, determined by the rays of light and heat which proceed from the surrounding stars. This low temperature is a little below that of the polar regions of the earth.</li></ul> <ul><li>The earth would have only the same temperature as the heavens, were it not for two causes... One is the internal heat... possessed at its formation... only dissipated through the surface; the other is the continued action of the solar rays... which produce at the surface, the diversities of climate.</li></ul> <ul><li>Liquids are very poor conductors of heat; but they have, like <a href="https://en.wiktionary.org/wiki/aeriform#Adjective" class="extiw" title="wikt:aeriform">aeriform</a> media, the property of <a href="https://en.wikipedia.org/wiki/Convection" class="extiw" title="w:Convection">carrying it rapidly in certain directions</a>. This is the same property which, combining with, combining with the centrifugal force, displaces and mingles all parts of the atmosphere... [and] ocean, and maintains in them, regular and immense currents.</li></ul> <ul><li>The interposition of the air very much modifies the effects of the heat upon the surface of the globe. The solar rays traversing the atmospheric strata, which are condensed by their own weight [at decreasing altitudes], heat them very unequally; those which are rarest are likewise coldest, because they... absorb a smaller part of the rays. The heat of the sun... in the form of light, possesses the property of penetrating transparent solids or liquids, and loses this property... when by... terrestrial bodies, it is turned into <a href="https://en.wikipedia.org/wiki/Infrared" class="extiw" title="w:Infrared">heat radiating without light</a>.</li></ul> <ul><li>This distinction of luminous and non-luminous heat, explains the elevation of temperature caused by transparent bodies.</li></ul> <ul><li>We shall describe... the principal results of the prolonged action of the solar rays upon the terrestrial globe. ...[T]he state of the mass has varied continually in proportion to the heat received. This variable... internal temperature... has approached... nearer to a final state... subject to no change. Then each point of the solid sphere has acquired, and preserves... a fixed temperature, which depends only on the situation of the point... <b>The final state of the mass, the heat of which has penetrated all... parts, can... be compared to... a vessel which receives by openings at the top, liquid from some constant source, and permits exactly an equal quantity to escape by orifices</b>.<br />Thus the solar heat has accumulated in the interior of the globe and is... continually renewed.</li></ul> <ul><li>We... now consider the second cause of terrestrial heat, which... resides in the planetary spaces. ...[A]scertain what would be the <a href="https://en.wiktionary.org/wiki/thermometrical" class="extiw" title="wikt:thermometrical">thermometrical</a> state of the terrestrial mass, if it received only the heat of the sun. To facilitate... first leave the atmosphere out of the account. ...[I]f the earth and all the bodies of the solar system, were placed in space deprived of all heat ...The polar regions would be subject to intense cold and the decrease of temperature from... equator to... poles would be incomparably more rapid and extended.<br />In this hypothesis of the absolute cold of space, all the effects of heat... at the surface of the earth, should be attributed to... the sun. The least variance in... [its] distance... from the earth, would occassion... considerable changes in temperature. The interruption of day and night would produce effects sudden... [B]odies, would be exposed... at commencement of night, to a cold of infinite intensity. Animals and vegetables could not resist... the sudden and powerful change... produced at the rising of the sun.</li></ul> <ul><li>The primitive heat... in the interior of the earth would not increase the external temperature of space... for... the effect of this central heat has long since become insensible at the surface, although it may be very great at a moderate depth.</li></ul> <ul><li>We conclude... that there exists a physical cause always present which modifies the temperature at the surface of the earth, and gives this planet a fundamental heat, which is... independent of the action of the sun and that internal heat preserved... It is to be attributed to the radiation from all the bodies in the universe, whose light and heat can reach us... rays which penetrate every part of the planetary regions... [A]ny point of space whatever which contains these bodies acquires a fixed temperature.</li></ul> <ul><li>This temperature of space is not the same in different regions of the universe; but it does not vary in the regions... [of] planetary bodies... [T]he planets of our system... equally participate in the common temperature... augmented for each... by the rays of the sun, according to the distance of the planet from... [it]. ...The intensity and distribution of heat on the surface of these bodies results from the distance from the sun, the inclination of the axes of rotation to the orbit, and the state of the surface...</li></ul> <ul><li>From the constitution of the solar system it is... probable that the temperature of the poles... are a little less than that of space... the same for all... although the distances from the sun may be unequal.</li></ul> <ul><li>It is difficult to know how far the atmosphere influences the mean temperature of the globe... It is to... <a href="https://en.wikipedia.org/wiki/Horace_B%C3%A9n%C3%A9dict_de_Saussure" class="extiw" title="w:Horace Bénédict de Saussure">M. de Saussure</a> that we are indebted for a capital experiment which appears to throw... light on this... The theory of the instrument is... 1st... the acquired heat is concentrated, because it is not dissipated immediately by renewing the air; 2d, that the heat of the sun, has properties different from those of [invisible] heat... The rays... are transmitted in considerable quantity through the glass plates... They heat the air and the partitions which contain it. Their heat thus communicated ceased to be luminous, and preserves only the properties of <a href="https://en.wikipedia.org/wiki/Infrared" class="extiw" title="w:Infrared">non-luminous radiating heat</a>. In this state it cannot pass through the plate of glass covering the vessel. ...It is necessary to consider attentively this order of facts, and the results of the calculus when we would ascertain the influence of the atmosphere and waters upon the thermometrical state of our globe.</li></ul> <ul><li>[I]f all the strata of air of... the atmosphere... preserved their density with their transparency, and lost only the mobility... peculiar to them, this mass of air, thus become solid, on being exposed to the rays of the sun, would produce an effect the same in kind... [as] just described.</li></ul> <ul><li>The mobility of the air, which is rapidly displaced... and... rises when heated... diminish the intensity of the effects... [of] a transparent and solid atmosphere, but do not entirely change their character.</li></ul> <ul><li>We shall now consider that peculiar heat which our globe had at the time of the formation of the planets, and which continues to be dissipated at the surface under the influence of the low temperature of the planetary space.</li></ul> <div class="mw-heading mw-heading2"><h2 id="Quotes_about_Fourier">Quotes about Fourier</h2><span class="mw-editsection"><span class="mw-editsection-bracket">[</span><a href="/w/index.php?title=Joseph_Fourier&action=edit&section=4" title="Edit section: Quotes about Fourier"><span>edit</span></a><span class="mw-editsection-bracket">]</span></span></div> <figure class="mw-default-size" typeof="mw:File/Thumb"><a href="/wiki/File:Fourier2_-_restoration1.jpg" class="mw-file-description"><img src="//upload.wikimedia.org/wikipedia/commons/thumb/d/df/Fourier2_-_restoration1.jpg/220px-Fourier2_-_restoration1.jpg" decoding="async" width="220" height="278" class="mw-file-element" srcset="//upload.wikimedia.org/wikipedia/commons/thumb/d/df/Fourier2_-_restoration1.jpg/330px-Fourier2_-_restoration1.jpg 1.5x, //upload.wikimedia.org/wikipedia/commons/thumb/d/df/Fourier2_-_restoration1.jpg/440px-Fourier2_-_restoration1.jpg 2x" data-file-width="1619" data-file-height="2048" /></a><figcaption><center>Joseph Fourier<br />early 19th c. engraving by<br /><a href="https://en.wikipedia.org/wiki/Julien-L%C3%A9opold_Boilly" class="extiw" title="wikipedia:Julien-Léopold Boilly">Julien-Léopold Boilly</a></center></figcaption></figure> <ul><li>In a military school directed by monks, the minds of the pupils necessarily waver only between two careers in life—the church and the sword. Like <a href="/wiki/Ren%C3%A9_Descartes" title="René Descartes">Descartes</a>, Fourier wished to be a soldier; like that philosopher he would doubtless have found the life of a garrison very wearisome. But he was not permitted to make the experiment. His demand to undergo the examination for the artillery, although strongly supported by our illustrious colleague <a href="https://en.wikipedia.org/wiki/Adrien-Marie_Legendre" class="extiw" title="w:Adrien-Marie Legendre">Legendre</a>, was rejected with a severity of expression of which you may judge yourselves: "Fourier," replied the minister, "not being noble, could not enter the artillery, although he were a second Newton." <ul><li><a href="/wiki/Fran%C3%A7ois_Arago" title="François Arago">François Arago</a>, <i><a rel="nofollow" class="external text" href="https://books.google.com/books?id=m7pcAAAAcAAJ">Biographies of Distinguished Scientific Men</a></i> (1857) Tr. William Henry Smyth, Baden Powell & Robert Grant</li></ul></li></ul> <ul><li>Fourier's analytical theory of heat (final form, 1822), devised in the Galileo-Newton tradition of controlled observation plus mathematics, is the ultimate source of much modern work in the theory of functions of a real variable and in the critical examination of the foundation of mathematics. <ul><li><a href="/wiki/Eric_Temple_Bell" title="Eric Temple Bell">Eric Temple Bell</a>, <i>The Development of Mathematics</i> (1940) p. 165</li></ul></li></ul> <ul><li>At the age of twenty-one he went to Paris to read before the Academy of Sciences a memoir on the resolution of numerical equations, which was an improvement on <a href="https://en.wikipedia.org/wiki/Newton%27s_method#History" class="extiw" title="w:Newton's method">Newton's method of approximation</a>. This investigation of his early youth he never lost sight of. He lectured upon it... he developed it... it constituted a part of a work entitled <i>Analyse des equations determines</i> (1831), which was in press when death overtook him. This work contained "<a href="https://en.wikipedia.org/wiki/Budan%27s_theorem#Fourier's_theorem" class="extiw" title="w:Budan's theorem">Fourier's theorem</a>" on the number of real roots between two chosen limits. <a href="https://en.wikipedia.org/wiki/Fran%C3%A7ois_Budan_de_Boislaurent" class="extiw" title="w:François Budan de Boislaurent">Budan</a> had published <a href="https://en.wikipedia.org/wiki/Budan%27s_theorem" class="extiw" title="w:Budan's theorem">this result</a> as early as 1807, but there is evidence to show that Fourier had established it before Budan's publication. These brilliant results were eclipsed by <a href="https://en.wikipedia.org/wiki/Sturm%27s_theorem" class="extiw" title="w:Sturm's theorem">the theorem</a> of <a href="https://en.wikipedia.org/wiki/Jacques_Charles_Fran%C3%A7ois_Sturm" class="extiw" title="w:Jacques Charles François Sturm">Sturm</a>, published in 1835. <ul><li><a href="/wiki/Florian_Cajori" title="Florian Cajori">Florian Cajori</a>, <i><a href="/wiki/A_History_of_Mathematics" title="A History of Mathematics">A History of Mathematics</a></i> (1893)</li></ul></li></ul> <ul><li>Fourier took a prominent part at his home in promoting the Revolution. Under the <a href="/wiki/French_Revolution" title="French Revolution">French Revolution</a> the arts and sciences seemed for a time to flourish. ...The <a href="https://en.wikipedia.org/wiki/%C3%89cole_normale_sup%C3%A9rieure" class="extiw" title="w:École normale supérieure">Normal School</a> was created in 1795, of which Fourier became at first pupil, then lecturer. His brilliant success secured him a chair in the <a href="https://en.wikipedia.org/wiki/%C3%89cole_Polytechnique" class="extiw" title="w:École Polytechnique">Polytechnic School</a>, the duties of which he afterwards quitted, along with <a href="https://en.wikipedia.org/wiki/Gaspard_Monge" class="extiw" title="w:Gaspard Monge">Monge</a> and <a href="https://en.wikipedia.org/wiki/Claude_Louis_Berthollet" class="extiw" title="w:Claude Louis Berthollet">Berthollet</a>, to accompany <a href="/wiki/Napoleon" title="Napoleon">Napoleon</a> on his campaign to Egypt. Napoleon founded the <a href="https://en.wikipedia.org/wiki/Institut_d%27%C3%89gypte" class="extiw" title="w:Institut d'Égypte">Institute of Egypt</a>, of which Fourier became secretary. In Egypt he engaged not only in scientific work, but discharged important political functions. ...In 1827 Fourier succeeded <a href="/wiki/Pierre-Simon_Laplace" title="Pierre-Simon Laplace">Laplace</a> as president of the council of the Polytechnic School. <ul><li>Florian Cajori, <i>A History of Mathematics</i> (1893)</li></ul></li></ul> <ul><li>He carried on his elaborate investigations on the propagation of heat in solid bodies, published in 1822 in his work entitled <i>La Theorie Analytique de la Chaleur</i>. This work marks an epoch in the history of mathematical physics. "<a href="https://en.wikipedia.org/wiki/Fourier_series" class="extiw" title="w:Fourier series">Fourier's series</a>" constitutes its gem. By this research a long controversy was brought to a close, and the fact established that any arbitrary function can be represented by a <a href="https://en.wikipedia.org/wiki/Trigonometric_series" class="extiw" title="w:Trigonometric series">trigonometric series</a>. The first announcement of this great discovery was made by Fourier in 1807 before the French Academy. The trigonometric series <span class="mwe-math-element"><span class="mwe-math-mathml-inline mwe-math-mathml-a11y" style="display: none;"><math xmlns="http://www.w3.org/1998/Math/MathML" alttext="{\displaystyle \sum _{n=0}^{n=\infty }(a_{n}\sin nx+b_{n}\cos nx)}"> <semantics> <mrow class="MJX-TeXAtom-ORD"> <mstyle displaystyle="true" scriptlevel="0"> <munderover> <mo>∑<!-- ∑ --></mo> <mrow class="MJX-TeXAtom-ORD"> <mi>n</mi> <mo>=</mo> <mn>0</mn> </mrow> <mrow class="MJX-TeXAtom-ORD"> <mi>n</mi> <mo>=</mo> <mi mathvariant="normal">∞<!-- ∞ --></mi> </mrow> </munderover> <mo stretchy="false">(</mo> <msub> <mi>a</mi> <mrow class="MJX-TeXAtom-ORD"> <mi>n</mi> </mrow> </msub> <mi>sin</mi> <mo>⁡<!-- --></mo> <mi>n</mi> <mi>x</mi> <mo>+</mo> <msub> <mi>b</mi> <mrow class="MJX-TeXAtom-ORD"> <mi>n</mi> </mrow> </msub> <mi>cos</mi> <mo>⁡<!-- --></mo> <mi>n</mi> <mi>x</mi> <mo stretchy="false">)</mo> </mstyle> </mrow> <annotation encoding="application/x-tex">{\displaystyle \sum _{n=0}^{n=\infty }(a_{n}\sin nx+b_{n}\cos nx)}</annotation> </semantics> </math></span><img src="https://wikimedia.org/api/rest_v1/media/math/render/svg/0bd99e6c16dc74eb42b52e98b085d588e699194e" class="mwe-math-fallback-image-inline mw-invert skin-invert" aria-hidden="true" style="vertical-align: -3.005ex; width:26.186ex; height:6.843ex;" alt="{\displaystyle \sum _{n=0}^{n=\infty }(a_{n}\sin nx+b_{n}\cos nx)}"></span> represents the function <span class="mwe-math-element"><span class="mwe-math-mathml-inline mwe-math-mathml-a11y" style="display: none;"><math xmlns="http://www.w3.org/1998/Math/MathML" alttext="{\displaystyle \phi (x)}"> <semantics> <mrow class="MJX-TeXAtom-ORD"> <mstyle displaystyle="true" scriptlevel="0"> <mi>ϕ<!-- ϕ --></mi> <mo stretchy="false">(</mo> <mi>x</mi> <mo stretchy="false">)</mo> </mstyle> </mrow> <annotation encoding="application/x-tex">{\displaystyle \phi (x)}</annotation> </semantics> </math></span><img src="https://wikimedia.org/api/rest_v1/media/math/render/svg/546b660b2f3cfb5f34be7b3ed8371d54f5c74227" class="mwe-math-fallback-image-inline mw-invert skin-invert" aria-hidden="true" style="vertical-align: -0.838ex; width:4.524ex; height:2.843ex;" alt="{\displaystyle \phi (x)}"></span> for every value of <span class="mwe-math-element"><span class="mwe-math-mathml-inline mwe-math-mathml-a11y" style="display: none;"><math xmlns="http://www.w3.org/1998/Math/MathML" alttext="{\displaystyle x}"> <semantics> <mrow class="MJX-TeXAtom-ORD"> <mstyle displaystyle="true" scriptlevel="0"> <mi>x</mi> </mstyle> </mrow> <annotation encoding="application/x-tex">{\displaystyle x}</annotation> </semantics> </math></span><img src="https://wikimedia.org/api/rest_v1/media/math/render/svg/87f9e315fd7e2ba406057a97300593c4802b53e4" class="mwe-math-fallback-image-inline mw-invert skin-invert" aria-hidden="true" style="vertical-align: -0.338ex; width:1.33ex; height:1.676ex;" alt="{\displaystyle x}"></span> if the coefficients <span class="mwe-math-element"><span class="mwe-math-mathml-inline mwe-math-mathml-a11y" style="display: none;"><math xmlns="http://www.w3.org/1998/Math/MathML" alttext="{\displaystyle a_{n}={\frac {1}{\pi }}\int _{-\pi }^{\pi }\phi (x)\sin nx\,dx}"> <semantics> <mrow class="MJX-TeXAtom-ORD"> <mstyle displaystyle="true" scriptlevel="0"> <msub> <mi>a</mi> <mrow class="MJX-TeXAtom-ORD"> <mi>n</mi> </mrow> </msub> <mo>=</mo> <mrow class="MJX-TeXAtom-ORD"> <mfrac> <mn>1</mn> <mi>π<!-- π --></mi> </mfrac> </mrow> <msubsup> <mo>∫<!-- ∫ --></mo> <mrow class="MJX-TeXAtom-ORD"> <mo>−<!-- − --></mo> <mi>π<!-- π --></mi> </mrow> <mrow class="MJX-TeXAtom-ORD"> <mi>π<!-- π --></mi> </mrow> </msubsup> <mi>ϕ<!-- ϕ --></mi> <mo stretchy="false">(</mo> <mi>x</mi> <mo stretchy="false">)</mo> <mi>sin</mi> <mo>⁡<!-- --></mo> <mi>n</mi> <mi>x</mi> <mspace width="thinmathspace" /> <mi>d</mi> <mi>x</mi> </mstyle> </mrow> <annotation encoding="application/x-tex">{\displaystyle a_{n}={\frac {1}{\pi }}\int _{-\pi }^{\pi }\phi (x)\sin nx\,dx}</annotation> </semantics> </math></span><img src="https://wikimedia.org/api/rest_v1/media/math/render/svg/ba87715b75c8cd4f0b9b84fe20190f543b6c2e58" class="mwe-math-fallback-image-inline mw-invert skin-invert" aria-hidden="true" style="vertical-align: -2.505ex; width:26.046ex; height:6.009ex;" alt="{\displaystyle a_{n}={\frac {1}{\pi }}\int _{-\pi }^{\pi }\phi (x)\sin nx\,dx}"></span>, and <span class="mwe-math-element"><span class="mwe-math-mathml-inline mwe-math-mathml-a11y" style="display: none;"><math xmlns="http://www.w3.org/1998/Math/MathML" alttext="{\displaystyle b_{n}}"> <semantics> <mrow class="MJX-TeXAtom-ORD"> <mstyle displaystyle="true" scriptlevel="0"> <msub> <mi>b</mi> <mrow class="MJX-TeXAtom-ORD"> <mi>n</mi> </mrow> </msub> </mstyle> </mrow> <annotation encoding="application/x-tex">{\displaystyle b_{n}}</annotation> </semantics> </math></span><img src="https://wikimedia.org/api/rest_v1/media/math/render/svg/28e2d72f6dd9375c8f1f59f1effd9b4e5492ac97" class="mwe-math-fallback-image-inline mw-invert skin-invert" aria-hidden="true" style="vertical-align: -0.671ex; width:2.216ex; height:2.509ex;" alt="{\displaystyle b_{n}}"></span> be equal to a similar integral. The weak point in Fourier's analysis lies in his failure to prove generally that the trigonometric series actually converges to the value of the function. <ul><li><a href="/wiki/Florian_Cajori" title="Florian Cajori">Florian Cajori</a>, <i><a href="/wiki/A_History_of_Mathematics" title="A History of Mathematics">A History of Mathematics</a></i> (1893)</li></ul></li></ul> <ul><li>It is true that M. Fourier had the opinion that the principal end of mathematics was the public utility and the explanation of natural phenomena; but such a philosopher as he is should have known that the unique end of science is the honor of the human mind, and that from this point of view a question of number is as important as a question of the system of the world. <ul><li><a href="/wiki/Carl_Gustav_Jacob_Jacobi" title="Carl Gustav Jacob Jacobi">Carl Gustav Jacob Jacobi</a>, Letter to <a href="https://en.wikipedia.org/wiki/Adrien-Marie_Legendre" class="extiw" title="w:Adrien-Marie Legendre">Legendre</a> (July 2, 1830) in response to Fourier's report to the Paris Academy Science that mathematics should be applied to the natural sciences, as quoted in <i>Science</i> (March 10, 1911) <a rel="nofollow" class="external text" href="https://books.google.com/books?id=4LU7AQAAMAAJ&pg=PA359">Vol. 33</a>, p.359, with additional citations and dates from H. Pieper, "Carl Gustav Jacob Jacobi," <i>Mathematics in Berlin</i> (2012) p.46</li></ul></li></ul> <div class="mw-heading mw-heading3"><h3 id="The_Evolution_of_Applied_Harmonic_Analysis_(2004)"><span id="The_Evolution_of_Applied_Harmonic_Analysis_.282004.29"></span><i>The Evolution of Applied Harmonic Analysis</i> (2004)</h3><span class="mw-editsection"><span class="mw-editsection-bracket">[</span><a href="/w/index.php?title=Joseph_Fourier&action=edit&section=5" title="Edit section: The Evolution of Applied Harmonic Analysis (2004)"><span>edit</span></a><span class="mw-editsection-bracket">]</span></span></div> <dl><dd><small>by Elena Presitini</small></dd></dl> <ul><li>He started as a convinced <a href="https://en.wikipedia.org/wiki/Jacobins" class="extiw" title="w:Jacobins">Jacobin</a>... and ended up a cautious liberal.</li></ul> <ul><li>He ranks among the most important scientists of the 19the century for his studies in the <a href="https://en.wikipedia.org/wiki/Heat_transfer" class="extiw" title="w:Heat transfer">propagation of heat</a>... and the paternity of the expression "<a href="https://en.wikipedia.org/wiki/greenhouse_effect" class="extiw" title="wikipedia:greenhouse effect">greenhouse effect</a>"—<i>effet de serre</i>—is attributed to Fourier.</li></ul> <ul><li>The novelty of his method... initially perplexed... mathematicians... from <a href="/wiki/Joseph_Louis_Lagrange" title="Joseph Louis Lagrange">Lagrange</a> to <a href="/wiki/Pierre-Simon_Laplace" title="Pierre-Simon Laplace">Laplace</a> and <a href="/wiki/Sim%C3%A9on_Denis_Poisson" title="Siméon Denis Poisson">Poisson</a>. ...[P]ublication ...was ...delayed as many as fifteen years during which he ...defended, explained and extended [his work].</li></ul> <ul><li>The formula and even the method was... used by <a href="/wiki/Leonhard_Euler" title="Leonhard Euler">Euler</a> in... 1777, published... 1798. (Fourier... having failed to refer to earlier works...) ...[A]s with <a href="/wiki/Daniel_Bernoulli" title="Daniel Bernoulli">Bernoulli</a>, Fourier had acquired an intimate understanding of the <a href="/wiki/Physics" title="Physics">physical</a> meaning of the problem. Over... two years... Fourier repeated all important experiments... carried out in England, France, and Germany and added experiments of his own. ...[S]triking ...confirmations of <a href="https://en.wikipedia.org/wiki/Thermal_conduction#Fourier's_law" class="extiw" title="w:Thermal conduction">his new theory</a> ...together with his overcoming ...difficulties advanced by the old masters. Fourier mentioned the motion of fluids... propagation of sounds and...vibrations of elastic bodies, as other applications ...fully aware of having opened up a new era for the solution or <a href="/wiki/Partial_differential_equation" title="Partial differential equation">partial differential equations</a>... It was the era of linearization that would dominate mathematics for the first half of the nineteenth century and... has remained important... The <a href="/wiki/Heat_equation" title="Heat equation">diffusion equation</a> is a <a href="https://en.wikipedia.org/wiki/linear_equation" class="extiw" title="wikipedia:linear equation">linear equation</a>: Linear combinations of solutions are still solutions. It was not the first such equation... in history... but the method opened up enormous... possibilities. <ul><li><small><b>Ref: 1)</b> <a href="/wiki/Leonhard_Euler" title="Leonhard Euler">Leonhard Euler</a>, "Remarques sur les mémoires précédens de M. Bernoulli," <i>Mémoires de l’Académie Royale de Berlin</i>, 9 (1753: publ. 1755), pp. 196-222. <b>2) </b><a href="/wiki/Daniel_Bernoulli" title="Daniel Bernoulli">Daniel Bernoulli</a>, "Réflexions et éclaircissemens sur les nouvelles vibrations des cordes exposées dans les mémoires de l'Académie de 1747 et 1748," <i>Mémoires de l'Académie Royale de Berlin</i>, 9 (1753: publ. 1755), pp. 147-172.</small></li></ul></li></ul> <ul><li><a href="/wiki/Galileo_Galilei" title="Galileo Galilei">Galileo</a> and <a href="/wiki/Robert_Hooke" title="Robert Hooke">Hooke</a> demonstrated that every sound is characterized by a precise number of vibrations per second, but the full understanding of even the simplest... vibrators requires... <a href="/wiki/Calculus" title="Calculus">calculus</a>. ...<a href="/wiki/Leonhard_Euler" title="Leonhard Euler">Leonard Euler</a>, <a href="/wiki/Daniel_Bernoulli" title="Daniel Bernoulli">Daniel Bernoulli</a>, <a href="/wiki/Jean_le_Rond_d%27Alembert" title="Jean le Rond d'Alembert">Jean le Rond d'Alembert</a>, and <a href="/wiki/Joseph_Louis_Lagrange" title="Joseph Louis Lagrange">Joseph Louis Lagrange</a> all studied the vibrating string.... In 1747 d'Alembert found... the <a href="/wiki/Wave_equation" title="Wave equation">wave equation</a> and in 1753 Bernoulli stated the... decomposition of every motion of a string as a sum of elementary sinusoidal motions. Then at the beginning of the following century Fourier developed "<a href="/wiki/Harmonic_analysis" title="Harmonic analysis">harmonic analysis</a>."</li></ul> <div class="mw-heading mw-heading2"><h2 id="External_links">External links</h2><span class="mw-editsection"><span class="mw-editsection-bracket">[</span><a href="/w/index.php?title=Joseph_Fourier&action=edit&section=6" title="Edit section: External links"><span>edit</span></a><span class="mw-editsection-bracket">]</span></span></div> <div class="noprint" style="clear: right; border: solid #aaa 1px; margin: 0 0 1em 1em; font-size: 90%; background: #f9f9f9; width: 250px; padding: 4px; spacing: 0px; text-align: left; float: right;"> <div style="float: left;"><figure class="mw-halign-none" typeof="mw:File"><a href="/wiki/File:Wikipedia-logo-v2.svg" class="mw-file-description" title="Wikipedia"><img alt="Wikipedia" src="//upload.wikimedia.org/wikipedia/commons/thumb/8/80/Wikipedia-logo-v2.svg/50px-Wikipedia-logo-v2.svg.png" decoding="async" width="50" height="46" class="mw-file-element" srcset="//upload.wikimedia.org/wikipedia/commons/thumb/8/80/Wikipedia-logo-v2.svg/75px-Wikipedia-logo-v2.svg.png 1.5x, //upload.wikimedia.org/wikipedia/commons/thumb/8/80/Wikipedia-logo-v2.svg/100px-Wikipedia-logo-v2.svg.png 2x" data-file-width="103" data-file-height="94" /></a><figcaption>Wikipedia</figcaption></figure></div> <div style="margin-left: 60px;"><a href="/wiki/Wikipedia" title="Wikipedia">Wikipedia</a> has an article about: <div style="margin-left: 10px;"><i><b><a href="https://en.wikipedia.org/wiki/Joseph_Fourier" class="extiw" title="wikipedia:Joseph Fourier">Joseph Fourier</a></b></i></div> </div> </div> <ul><li><a rel="nofollow" class="external text" href="http://www-history.mcs.st-andrews.ac.uk/Biographies/Fourier.html">"Jean Baptiste Joseph Fourier" profile at the University of St. Andrews</a></li> <li><a rel="nofollow" class="external text" href="http://www.wmconnolley.org.uk/sci/fourier_1827/fourier_1827.html"><i>Memoir on the temperature of the earth and planetary spaces</i> (1827)</a></li> <li><a rel="nofollow" class="external text" href="http://www.ujf-grenoble.fr/22046314/1/fiche___pagelibre/">Brief Profile at Université Joseph Fourier, Grenoble, France</a></li> <li>YouTube videos <ul><li><a rel="nofollow" class="external text" href="https://www.youtube.com/watch?v=4VYbXp9k-%20Q">The Revolutionary Genius Of Joseph Fourier</a> Fourier's derivation of the <a href="/wiki/Heat_equation" title="Heat equation">Heat equation</a> from <a href="https://en.wikipedia.org/wiki/Newton%27s_law_of_cooling" class="extiw" title="wikipedia:Newton's law of cooling">Newton's law of cooling</a> and <a href="https://en.wikipedia.org/wiki/specific_heat_capacity" class="extiw" title="wikipedia:specific heat capacity">specific heat capacity</a> research of <a href="/wiki/Antoine_Lavoisier" title="Antoine Lavoisier">Lavoisier</a> and <a href="/wiki/Pierre-Simon_Laplace" title="Pierre-Simon Laplace">Laplace</a>, plus more @Dr. Will Wood channel.</li></ul></li></ul> <div style="clear:both; width:100%; border-top:1px solid #A88"><br /></div> <table class="wikitable mw-collapsible"> <tbody><tr> <td style="background:#9F9F9F" align="center" colspan="3"><b><a href="/wiki/Mathematics" title="Mathematics">Mathematics</a></b> </td></tr> <tr> <td><a href="/wiki/Mathematicians" title="Mathematicians">Mathematicians</a><br /><small>(<a href="/wiki/Category:Mathematicians_by_country" title="Category:Mathematicians by country">by country</a>)</small> </td> <td style="font-size:0.8em"> <p><a href="/wiki/Niels_Henrik_Abel" title="Niels Henrik Abel">Abel</a> • <a href="/wiki/Anaxagoras" title="Anaxagoras">Anaxagoras</a> • <a href="/wiki/Archimedes" title="Archimedes">Archimedes</a> • <a href="/wiki/Aristarchus_of_Samos" title="Aristarchus of Samos">Aristarchus of Samos</a> • <a href="/wiki/Averroes" title="Averroes">Averroes</a> • <a href="/wiki/Vladimir_Arnold" title="Vladimir Arnold">Arnold</a> • <a href="/wiki/Stefan_Banach" title="Stefan Banach">Banach</a> • <a href="/wiki/Georg_Cantor" title="Georg Cantor">Cantor</a> • <a href="/wiki/Henri_Cartan" title="Henri Cartan">Cartan</a> • <a href="/wiki/Shiing-Shen_Chern" title="Shiing-Shen Chern">Chern</a> • <a href="/wiki/Paul_Cohen" title="Paul Cohen">Cohen</a> • <a href="/wiki/Ren%C3%A9_Descartes" title="René Descartes">Descartes</a> • <a href="/wiki/Diophantus" title="Diophantus">Diophantus</a> • <a href="/wiki/Paul_Erd%C5%91s" title="Paul Erdős">Erdős</a> • <a href="/wiki/Euclid" title="Euclid">Euclid</a> • <a href="/wiki/Leonhard_Euler" title="Leonhard Euler">Euler</a> • <a class="mw-selflink selflink">Fourier</a> • <a href="/wiki/Carl_Friedrich_Gauss" title="Carl Friedrich Gauss">Gauss</a> • <a href="/wiki/Kurt_G%C3%B6del" title="Kurt Gödel">Gödel</a> • <a href="/wiki/Hermann_Grassmann" title="Hermann Grassmann">Grassmann</a> • <a href="/wiki/Alexander_Grothendieck" title="Alexander Grothendieck">Grothendieck</a> • <a href="/wiki/William_Rowan_Hamilton" title="William Rowan Hamilton">Hamilton</a> • <a href="/wiki/David_Hilbert" title="David Hilbert">Hilbert</a> • <a href="/wiki/Hypatia" title="Hypatia">Hypatia</a> • <a href="/wiki/Joseph_Louis_Lagrange" title="Joseph Louis Lagrange">Lagrange</a> • <a href="/wiki/Pierre-Simon_Laplace" title="Pierre-Simon Laplace">Laplace</a> • <a href="/wiki/Gottfried_Leibniz" title="Gottfried Leibniz">Leibniz</a> • <a href="/wiki/John_Milnor" title="John Milnor">Milnor</a> • <a href="/wiki/Isaac_Newton" title="Isaac Newton">Newton</a> • <a href="/wiki/John_von_Neumann" title="John von Neumann">von Neumann</a> • <a href="/wiki/Emmy_Noether" title="Emmy Noether">Noether</a> • <a href="/wiki/Roger_Penrose" title="Roger Penrose">Penrose</a> • <a href="/wiki/Grigori_Perelman" title="Grigori Perelman">Perelman</a> • <a href="/wiki/Henri_Poincar%C3%A9" title="Henri Poincaré">Poincaré</a> • <a href="/wiki/George_P%C3%B3lya" title="George Pólya">Pólya</a> • <a href="/wiki/Pythagoras" title="Pythagoras">Pythagoras</a> • <a href="/wiki/Bernhard_Riemann" title="Bernhard Riemann">Riemann</a> • <a href="/wiki/Bertrand_Russell" title="Bertrand Russell">Russell</a> • <a href="/wiki/Laurent_Schwartz" title="Laurent Schwartz">Schwartz</a> • <a href="/wiki/Jean-Pierre_Serre" title="Jean-Pierre Serre">Serre</a> • <a href="/wiki/Terence_Tao" title="Terence Tao">Tao</a> • <a href="/wiki/Alfred_Tarski" title="Alfred Tarski">Tarski</a> • <a href="/wiki/Thales" title="Thales">Thales</a> • <a href="/wiki/Alan_Turing" title="Alan Turing">Turing</a> • <a href="/wiki/Andr%C3%A9_Weil" title="André Weil">Weil</a> • <a href="/wiki/Hermann_Weyl" title="Hermann Weyl">Weyl</a> • <a href="/wiki/Andrew_Wiles" title="Andrew Wiles">Wiles</a> • <a href="/wiki/Edward_Witten" title="Edward Witten">Witten</a> </p> </td></tr> <tr> <td><a href="/wiki/Number" title="Number">Numbers</a> </td> <td style="font-size:0.8em"> <p><a href="/wiki/1_(number)" title="1 (number)">1</a> • <a href="/wiki/23" title="23">23</a> • <a href="/wiki/360_(number)" title="360 (number)">360</a> • <a href="/wiki/E_(mathematical_constant)" title="E (mathematical constant)"><i>e</i></a> • <a href="/wiki/%CE%A0" title="Π"><i>π</i></a> • <a href="/wiki/Fibonacci_numbers" title="Fibonacci numbers">Fibonacci numbers</a> • <a href="/wiki/Irrational_number" title="Irrational number">Irrational number</a> • <a href="/wiki/Negative_number" title="Negative number">Negative number</a> • <a href="/wiki/Number" title="Number">Number</a> • <a href="/wiki/Prime_number" title="Prime number">Prime number</a> • <a href="/wiki/Quaternion" title="Quaternion">Quaternion</a> • <a href="/wiki/Octonion" title="Octonion">Octonion</a> </p> </td></tr> <tr> <td>Concepts </td> <td style="font-size:0.8em"> <p><a href="/wiki/Abstraction_(mathematics)" title="Abstraction (mathematics)">Abstraction</a> • <a href="/wiki/Algorithms" title="Algorithms">Algorithms</a> • <a href="/wiki/Axiomatic_system" title="Axiomatic system">Axiomatic system</a> • <a href="/wiki/Completeness" title="Completeness">Completeness</a> • <a href="/wiki/Deductive_reasoning" title="Deductive reasoning">Deductive reasoning</a> • <a href="/wiki/Differential_equation" title="Differential equation">Differential equation</a> • <a href="/wiki/Dimension" title="Dimension">Dimension</a> • <a href="/wiki/Ellipse" title="Ellipse">Ellipse</a> • <a href="/wiki/Elliptic_curve" title="Elliptic curve">Elliptic curve</a> • <a href="/wiki/Exponential_growth" title="Exponential growth">Exponential growth</a> • <a href="/wiki/Infinity" title="Infinity">Infinity</a> • <a href="/wiki/Integration" title="Integration">Integration</a> • <a href="/wiki/Geodesic" title="Geodesic">Geodesic</a> • <a href="/wiki/Mathematical_induction" title="Mathematical induction">Induction</a> • <a href="/wiki/Mathematical_proof" title="Mathematical proof">Proof</a> • <a href="/wiki/Partial_differential_equation" title="Partial differential equation">Partial differential equation</a> • <a href="/wiki/Principle_of_least_action" title="Principle of least action">Principle of least action</a> • <a href="/wiki/Prisoner%27s_dilemma" title="Prisoner's dilemma">Prisoner's dilemma</a> • <a href="/wiki/Probability" title="Probability">Probability</a> • <a href="/wiki/Randomness" title="Randomness">Randomness</a> • <a href="/wiki/Theorem" title="Theorem">Theorem</a> • <a href="/wiki/Topological_space" title="Topological space">Topological space</a> • <a href="/wiki/Wave_equation" title="Wave equation">Wave equation</a> </p> </td></tr> <tr> <td>Results </td> <td style="font-size:0.8em"> <p><a href="/wiki/Euler%27s_identity" title="Euler's identity">Euler's identity</a> • <a href="/wiki/Fermat%27s_Last_Theorem" title="Fermat's Last Theorem">Fermat's Last Theorem</a> </p> </td></tr> <tr> <td><a href="/wiki/Pure_mathematics" title="Pure mathematics">Pure math</a> </td> <td style="font-size:0.8em"> <p><a href="/wiki/Abstract_algebra" title="Abstract algebra">Abstract algebra</a> • <a href="/wiki/Algebra" title="Algebra">Algebra</a> • <a href="/wiki/Mathematical_analysis" title="Mathematical analysis">Analysis</a> • <a href="/wiki/Algebraic_geometry" title="Algebraic geometry">Algebraic geometry</a> (<a href="/wiki/Sheaf_theory" title="Sheaf theory">Sheaf theory</a>) • <a href="/wiki/Algebraic_topology" title="Algebraic topology">Algebraic topology</a> • <a href="/wiki/Arithmetic" title="Arithmetic">Arithmetic</a> • <a href="/wiki/Calculus" title="Calculus">Calculus</a> • <a href="/wiki/Category_theory" title="Category theory">Category theory</a> • <a href="/wiki/Combinatorics" title="Combinatorics">Combinatorics</a> • <a href="/wiki/Commutative_algebra" title="Commutative algebra">Commutative algebra</a> • <a href="/wiki/Complex_analysis" title="Complex analysis">Complex analysis</a> • <a href="/wiki/Differential_calculus" title="Differential calculus">Differential calculus</a> • <a href="/wiki/Differential_geometry" title="Differential geometry">Differential geometry</a> • <a href="/wiki/Differential_topology" title="Differential topology">Differential topology</a> • <a href="/wiki/Ergodic_theory" title="Ergodic theory">Ergodic theory</a> • <a href="/wiki/Foundations_of_mathematics" title="Foundations of mathematics">Foundations of mathematics</a> • <a href="/wiki/Functional_analysis" title="Functional analysis">Functional analysis</a> • <a href="/wiki/Game_theory" title="Game theory">Game theory</a> • <a href="/wiki/Geometry" title="Geometry">Geometry</a> • <a href="/wiki/Global_analysis" title="Global analysis">Global analysis</a> • <a href="/wiki/Graph_theory" title="Graph theory">Graph theory</a> • <a href="/wiki/Group_theory" title="Group theory">Group theory</a> • <a href="/wiki/Harmonic_analysis" title="Harmonic analysis">Harmonic analysis</a> • <a href="/wiki/Homological_algebra" title="Homological algebra">Homological algebra</a> • <a href="/wiki/Invariant_theory" title="Invariant theory">Invariant theory</a> • <a href="/wiki/Mathematical_logic" title="Mathematical logic">Logic</a> • <a href="/wiki/Non-Euclidean_geometry" title="Non-Euclidean geometry">Non-Euclidean geometry</a> • <a href="/wiki/Nonstandard_analysis" title="Nonstandard analysis">Nonstandard analysis</a> • <a href="/wiki/Number_theory" title="Number theory">Number theory</a> • <a href="/wiki/Numerical_analysis" title="Numerical analysis">Numerical analysis</a> • <a href="/wiki/Operations_research" title="Operations research">Operations research</a> • <a href="/wiki/Representation_theory" title="Representation theory">Representation theory</a> • <a href="/wiki/Ring_theory" title="Ring theory">Ring theory</a> • <a href="/wiki/Set_theory" title="Set theory">Set theory</a> • <a href="/wiki/Sheaf_theory" title="Sheaf theory">Sheaf theory</a> • <a href="/wiki/Statistics" title="Statistics">Statistics</a> • <a href="/wiki/Symplectic_geometry" title="Symplectic geometry">Symplectic geometry</a> • <a href="/wiki/Topology" title="Topology">Topology</a> </p> </td></tr> <tr> <td><a href="/wiki/Applied_mathematics" title="Applied mathematics">Applied math</a> </td> <td style="font-size:0.8em"> <p><a href="/wiki/Computational_fluid_dynamics" title="Computational fluid dynamics">Computational fluid dynamics</a> • <a href="/wiki/Econometrics" title="Econometrics">Econometrics</a> • <a href="/wiki/Fluid_mechanics" title="Fluid mechanics">Fluid mechanics</a> • <a href="/wiki/Mathematical_physics" title="Mathematical physics">Mathematical physics</a> • <a href="/wiki/Science" title="Science">Science</a> </p> </td></tr> <tr> <td><a href="/wiki/History_of_mathematics" title="History of mathematics">History of math</a> </td> <td style="font-size:0.8em"> <p><a href="/wiki/Ancient_Greek_mathematics" title="Ancient Greek mathematics">Ancient Greek mathematics</a> • <a href="/wiki/Euclid%E2%80%99s_Elements" title="Euclid’s Elements">Euclid's <i>Elements</i></a> • <a href="/wiki/History_of_algebra" title="History of algebra">History of algebra</a> • <a href="/wiki/History_of_calculus" title="History of calculus">History of calculus</a> • <a href="/wiki/History_of_logarithms" title="History of logarithms">History of logarithms</a> • <a href="/wiki/Indian_mathematics" title="Indian mathematics">Indian mathematics</a> • <a href="/wiki/Principia_Mathematica" title="Principia Mathematica"><i>Principia Mathematica</i></a> </p> </td></tr> <tr> <td>Other </td> <td style="font-size:0.8em"> <p><a href="/wiki/Mathematics_and_mysticism" title="Mathematics and mysticism">Mathematics and mysticism</a> • <a href="/wiki/Mathematics_education" title="Mathematics education">Mathematics education</a> • <a href="/wiki/Mathematics,_from_the_points_of_view_of_the_Mathematician_and_of_the_Physicist" title="Mathematics, from the points of view of the Mathematician and of the Physicist">Mathematics, from the points of view of the Mathematician and of the Physicist</a> • <a href="/wiki/Philosophy_of_mathematics" title="Philosophy of mathematics">Philosophy of mathematics</a> • <a href="/wiki/Unification_in_science_and_mathematics" title="Unification in science and mathematics">Unification in science and mathematics</a> </p> </td></tr></tbody></table> <p><br clear="all" /> </p> <!-- NewPP limit report Parsed by mw‐web.codfw.main‐7d9797f5d‐vrrzq Cached time: 20241119224305 Cache expiry: 2592000 Reduced expiry: false Complications: [show‐toc] CPU time usage: 0.086 seconds Real time usage: 0.275 seconds Preprocessor visited node count: 300/1000000 Post‐expand include size: 6366/2097152 bytes Template argument size: 356/2097152 bytes Highest expansion depth: 5/100 Expensive parser function count: 0/500 Unstrip recursion depth: 0/20 Unstrip post‐expand size: 180/5000000 bytes Number of Wikibase entities loaded: 0/400 --> <!-- Transclusion 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