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

:F_x-iF_y = \frac{i\rho}{2} \oint_C \left(\frac{\mathrm{d}w}{\mathrm{d}z}\right)^2\mathrm{d}z

and the moment about the origin experienced by the body is given by

:M=\Re\left\{-\frac{\rho}{2}\oint_C z \left(\frac{\mathrm{d}w}{\mathrm{d}z}\right)^2\mathrm{d}z\right\}.

Here,

  • (F_x,F_y) is the force acting on the body,
  • \rho is the density of the fluid,
  • C is the contour flush around the body,
  • w=\phi+ i\psi is the complex potential (\phi is the velocity potential, \psi is the stream function),
  • {\mathrm{d}w}/{\mathrm{d}z} = u_x-i u_y is the complex velocity ((u_x,u_y) is the velocity vector),
  • z=x+iy is the complex variable ((x,y) is the position vector),
  • \Re is the real part of the complex number, and
  • M 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

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Category:Fluid dynamics