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Tennis racket theorem information


Principal axes of a tennis racket.
Composite video of a tennis racquet rotated around the three axes – the intermediate one flips from the light edge to the dark edge (note that the numbering is off-set by 1 from the diagram above)
Title page of "Théorie Nouvelle de la Rotation des Corps", 1852 printing

The tennis racket theorem or intermediate axis theorem, is a kinetic phenomenon of classical mechanics which describes the movement of a rigid body with three distinct principal moments of inertia. It has also dubbed the Dzhanibekov effect, after Soviet cosmonaut Vladimir Dzhanibekov, who noticed one of the theorem's logical consequences whilst in space in 1985.[1] Formally the effect had been known for at least 150 years, having been described by Louis Poinsot in 1834.[2][3]

The theorem describes the following effect: rotation of an object around its first and third principal axes is stable, whereas rotation around its second principal axis (or intermediate axis) is not.

This can be demonstrated by the following experiment: hold a tennis racket at its handle, with its face being horizontal, and throw it in the air such that it performs a full rotation around its horizontal axis perpendicular to the handle (ê2 in the diagram, ê1 in the video), and then catch the handle. In almost all cases, during that rotation the face will also have completed a half rotation, so that the other face is now up. By contrast, it is easy to throw the racket so that it will rotate around the handle axis (ê1 in the diagram) without accompanying half-rotation around another axis; it is also possible to make it rotate around the vertical axis perpendicular to the handle (ê3 in the diagram) without any accompanying half-rotation.

The experiment can be performed with any object that has three different moments of inertia, for instance with a book, remote control, or smartphone. The effect occurs whenever the axis of rotation differs only slightly from the object's second principal axis; air resistance or gravity are not necessary.[4]

  1. ^ Эффект Джанибекова (гайка Джанибекова), 23 July 2009 (in Russian). The software can be downloaded from here
  2. ^ Poinsot (1834) Theorie Nouvelle de la Rotation des Corps, Bachelier, Paris
  3. ^ Derek Muller (September 19, 2019). The Bizarre Behavior of Rotating Bodies, Explained. Veritasium. Retrieved February 16, 2020.
  4. ^ Levi, Mark (2014). Classical Mechanics with Calculus of Variations and Optimal Control: An Intuitive Introduction. American Mathematical Society. pp. 151–152. ISBN 9781470414443.

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