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  1. Jean-Baptiste Joseph Fourier (/ ˈ f ʊr i eɪ,-i ər /; French:; 21 March 1768 – 16 May 1830) was a French mathematician and physicist born in Auxerre and best known for initiating the investigation of Fourier series, which eventually developed into Fourier analysis and harmonic analysis, and their applications to problems of heat transfer ...

  2. May 12, 2024 · Joseph Fourier (born March 21, 1768, Auxerre, France—died May 16, 1830, Paris) was a French mathematician, known also as an Egyptologist and administrator, who exerted strong influence on mathematical physics through his Théorie analytique de la chaleur (1822; The Analytical Theory of Heat).

    • Dirk Jan Struik
  3. Joseph Fourier studied the mathematical theory of heat conduction. He established the partial differential equation governing heat diffusion and solved it by using infinite series of trigonometric functions.

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  5. Jean Baptiste Joseph Fourier (March 21, 1768 – May 16, 1830) was a French mathematician, physicist and government administrator during the reign of Napoleon who is best known for his study of heat conduction, and for using series of trigonometric functions, now called Fourier series, to solve difficult mathematical problems.

  6. Joseph, Baron Fourier, (born March 21, 1768, Auxerre, France—died May 16, 1830, Paris), French mathematician and Egyptologist. While an engineer on Napoleon’s Egyptian expedition, he conducted (1798–1801) anthropological investigations and wrote the preface to the monumental Description de l’Égypte , whose publication he oversaw (1809 ...

  7. Mar 20, 2018 · Learn how the French mathematician and physicist Joseph Fourier developed the transform that bears his name and how it is used in modern medicine, climate science and physics. The article celebrates his 250th birthday and his legacy in mathematics.

  8. lpsa.swarthmore.edu › Fourier › SeriesBiography of Fourier

    Baron Jean-Baptiste-Joseph Fourier (March 21 1768-May 16, 1830), born in poor circumstances in Auxerre, introduced the idea that an arbitrary function, even one defined by different analytic expressions in adjacent segments of its range (such as a staircase waveform), could nevertheless be represented by a single analytic expression.

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