Kirchhoff equations
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In
fluid dynamics In physics, physical chemistry and engineering, fluid dynamics is a subdiscipline of fluid mechanics that describes the flow of fluids – liquids and gases. It has several subdisciplines, including (the study of air and other gases in motion ...
, the Kirchhoff equations, named after
Gustav Kirchhoff Gustav Robert Kirchhoff (; 12 March 1824 – 17 October 1887) was a German chemist, mathematician, physicist, and spectroscopist who contributed to the fundamental understanding of electrical circuits, spectroscopy and the emission of black-body ...
, describe the motion of a
rigid body In physics, a rigid body, also known as a rigid object, is a solid body in which deformation is zero or negligible, when a deforming pressure or deforming force is applied on it. The distance between any two given points on a rigid body rema ...
in an ideal fluid. \begin & = \times \boldsymbol\omega + \times \mathbf v + \mathbf Q_h + \mathbf Q, \\ 0pt & = \times \boldsymbol\omega + \mathbf F_h + \mathbf F, \\ 0ptT & = \left( \boldsymbol\omega^T \tilde I \boldsymbol\omega + m v^2 \right) \\ 0pt\mathbf Q_h & = -\int p \mathbf x \times\hat\mathbf n \, d\sigma, \\ 0pt\mathbf F_h & = -\int p \hat\mathbf n \, d\sigma \end where \boldsymbol\omega and \mathbf v are the angular and linear velocity vectors at the point \mathbf x, respectively; \tilde I is the moment of inertia tensor, m is the body's mass; \hat\mathbf n is a unit normal vector to the surface of the body at the point \mathbf x; p is a pressure at this point; \mathbf Q_h and \mathbf F_h are the hydrodynamic torque and force acting on the body, respectively; \mathbf Q and \mathbf F likewise denote all other torques and forces acting on the body. The integration is performed over the fluid-exposed portion of the body's surface. If the body is completely submerged body in an infinitely large volume of irrotational, incompressible, inviscid fluid, that is at rest at infinity, then the vectors \mathbf Q_h and \mathbf F_h can be found via explicit integration, and the dynamics of the body is described by the KirchhoffClebsch equations: = \times \boldsymbol\omega + \times \mathbf v, \quad = \times \boldsymbol\omega, L(\boldsymbol\omega, \mathbf v) = (A \boldsymbol\omega,\boldsymbol\omega) + (B \boldsymbol\omega,\mathbf v) + (C \mathbf v,\mathbf v) + (\mathbf k,\boldsymbol\omega) + (\mathbf l,\mathbf v). Their first integrals read J_0 = \left(, \boldsymbol\omega \right) + \left(, \mathbf v \right) - L, \quad J_1 = \left(,\right), \quad J_2 = \left(,\right) . Further integration produces explicit expressions for position and velocities.


References

* Kirchhoff G. R. ''Vorlesungen ueber Mathematische Physik, Mechanik''. Lecture 19. Leipzig: Teubner. 1877. * Lamb, H., ''Hydrodynamics''. Sixth Edition Cambridge (UK): Cambridge University Press. 1932. Mechanics Classical mechanics Rigid bodies Gustav Kirchhoff {{fluiddynamics-stub