Next: 1752: D'Alembert's Paradox Up: Contents
D'ALEMBERT'S PARADOX
And Lagrangian Coordinates

Leon L. Van Dommelen
FAMU-FSU College of Engineering

Our theoretical understanding of fluid mechanical drag is traced back in history. After Newton first defined force, it still took centuries to understand why there is a significant drag on simple bodies moving through liquids or gasses. Even now, our understanding is very limited.


 
1752: D'Alembert's Paradox
1752: D'Alembert's Paradox
1760: Lagrangian Coordinates
1777: Newton is Wrong
1841: Vorticity
1841: continued
1869: Kirchhoff Flows
1869: continued
1904: Boundary Layers
1904: Small Times
1904: Separation
1904: Zero Wall Shear
1904: continued
1948: Singularities
1958: Unsteady Separation
1958: continued
1958: continued
1962: Rear Stagnation Point
1972: Steady Separation
1975: Definition of Separation
1977: Numerical Discovery
1977: continued
1977: continued
1977: continued
1977: continued
1982: Analytical Description
1982: continued
1995: Vortex Computations
1995: continued
1995: continued
1995: continued
1995: continued
1995: A New Division of Drag
Summary

Next: 1752: D'Alembert's Paradox Up: Contents