Blasius theorem
In fluid dynamics, Blasius theorem states that Lamb, H. (1993). Hydrodynamics. Cambridge university press. pp. 91Milne-Thomson, L. M. (1949). Theoretical hydrodynamics (Vol. 8, No. 00). London: Macmillan.Acheson, D. J. (1991). Elementary fluid dynamics. the force experienced by a two-dimensional fixed body in a steady irrotational flow is given by
:
and the moment about the origin experienced by the body is given by
:
Here,
- is the force acting on the body,
- is the density of the fluid,
- is the contour flush around the body,
- is the complex potential ( is the velocity potential, is the stream function),
- is the complex velocity ( is the velocity vector),
- is the complex variable ( is the position vector),
- is the real part of the complex number, and
- is the moment about the coordinate origin acting on the body.
The first formula is sometimes called Blasius–Chaplygin formula.{{cite web|last1=Eremenko|first1=Alexandre (2013)|title=Why airplanes fly, and ships sail|url=https://www.math.purdue.edu/~eremenko/dvi/airplanes.pdf|publisher=Purdue University}}
The theorem is named after Paul Richard Heinrich Blasius, who derived it in 1911.Blasius, H. (1911). Mitteilung zur Abhandlung über: Funktionstheoretische Methoden in der Hydrodynamik. Zeitschrift für Mathematik und Physik, 59, 43-44. The Kutta–Joukowski theorem directly follows from this theorem.
References
{{reflist|30em}}