Article ID: CBB001211054

“Continuity and Change”: Representing Mass Conservation in Fluid Mechanics (2013)

unapi

The evolution of the equation of mass conservation in fluid mechanics is studied. Following early hydraulic approximations, and progress by Daniel and Johann Bernoulli, its first expression as a partial differential equation was achieved by d'Alembert, and soon given definitive form by Euler. Later reworkings by Lagrange, Laplace, Poisson and others advanced the subject, but all based their derivations on the conserved mass of a moving fluid particle. Later, Duhamel and Thomson gave a simpler derivation, by considering mass flow into and out of a fixed portion of space. The later propagation of these derivations in nineteenth-century British textbooks and treatises is also examined, including Maxwell's on the kinetic theory of gases.

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Description On work from the 17th to the 19th centuries.


Citation URI
https://data.isiscb.org/isis/citation/CBB001211054/

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Authors & Contributors
Caneva, Kenneth L.
Cahan, David L.
Villone, Barbara
Frisch, Uriel
Underwood, Ted
Strien, Marij van
Journals
Science and Education
Notes and Records: The Royal Society Journal of the History of Science
Archive for History of Exact Sciences
Studies in History and Philosophy of Science
Revue d'Histoire des Sciences
Historia Scientiarum: International Journal of the History of Science Society of Japan
Publishers
Città del Silenzio
World Scientific
Science History Publications
Omniscience
MIT Press
Concepts
Physics
Conservation of energy (physical concept)
Mathematics
Fluid mechanics
Continuity
Energy (physics)
People
Helmholtz, Hermann Ludwig Ferdinand von
Mayer, Julius Robert von
Joule, James Prescott
Euler, Leonhard
Taylor, Brook
Seki, Takakazu
Time Periods
19th century
17th century
18th century
Renaissance
Medieval
Enlightenment
Places
Great Britain
Japan
Italy
Germany
France
China
Institutions
Royal Society (Great Britain). European Science Exchange Programme
Académie des Sciences, Paris
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