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Pierre Henri Hugoniot : ウィキペディア英語版
Pierre Henri Hugoniot

Pierre-Henri Hugoniot (born in Allenjoie, Doubs, France on June 5, 1851 - died in Nantes, France in February 1887)〔Encyclopedia.com: Complete Dictionary of Scientific Biography (2008): (Hugoniot, Pierre Henri ).〕 who mostly lived in Montbéliard, (Franche-Comté). He was an inventor, mathematician, and physicist who worked on fluid mechanics, especially on issues related to material shock.
After going into the marine artillery upon his graduation from the École Polytechnique in 1872,〔Roger Chéret, "The life and work of Pierre Henri Hugoniot" in ''Shock Compression of Condensed Matter - 1989: Proceedings of the American Physical Society Topical Conference held in Albuquerque, New Mexico, August 14-17, 1989'', S.C. Schmidt, J.N. Johnson, and L.W. Davison, ed.s (Amsterdam, Netherlands: North-Holland, 1990), pages 12-19. Reprinted in:
* R. Chéret (1992) "The life and work of Pierre-Henri Hugoniot," ''Shock Waves'', vol. 2, no. 1, pages 1-4.
* Roger Chéret, ("The life and work of Pierre Henri Hugoniot" ) in ''Classic Papers in Shock Compression Science'', J.N. Johnson and R. Chéret, ed.s (New York, New York: Springer,1998), pages 149-160.〕 Hugoniot became professor of mechanics and ballistics at the School of Artillery Lorient (1879-1882) and Deputy Director of the Central Laboratory of the artillery Navy (1882-1884). He was promoted to captain in January 1884, and in April was appointed assistant professor of mechanical engineering at the École polytechnique. He conducted, along with his colleague Hippolyte Sebert (1839-1930), research on the trigger gas accompanying the detonation of a cannon.
He invented the theory based on conservation of mass, momentum, and energy, which allowed for improvements in fluid flow studies (with applications to aerospace). The Rankine-Hugoniot equation (or adiabatic dynamics of gas) has been named in his honor.
==References==


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