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Rolling cone motion
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Rolling cone motion : ウィキペディア英語版
Rolling cone motion
Rolling cone motion is the rolling motion generated by a cone rolling over another cone. In rolling cone motion, at least one of the cones is convex, while the other cone may be either convex, or concave, or a flat surface (a flat surface can be regarded as a special case of a cone whose apex angle equals \pi). The distinguishing characteristic of a rolling cone, in relation to other axially symmetrical rollers (cylinder, sphere, round disk), is that while rolling on a flat surface, the cone's center of gravity performs a circular motion rather than a linear one. Another unique characteristic is that one of its points (its apex) is at rest throughout the entire motion.
==Kinematics==
:
The motion of a rolling cone can be described as a combination of a rotational motion of the cone around its axis of symmetry, and a rotary motion of its axis around the axis of symmetry of the stationary cone. The ratio between the angular velocities of these two motions is given by:
:\frac =,
where \alpha and \beta are the half apex angles of the stationary cone and the rolling cone, respectively, \omega_1 is the angular velocity of the rolling cone's axis of symmetry around the axis of symmetry of the stationary cone, and \omega_2 is the angular velocity of the rolling cone around its own axis of symmetry. In the special case of a cone rolling on a flat surface, this ratio becomes \sin \alpha, where \alpha is the cone's half apex angle. For example, a cone having an apex angle of 120 degrees, while being rolled on a flat surface, will perform exactly two full rotations around its axis of symmetry before returning to its original position.

抄文引用元・出典: フリー百科事典『 ウィキペディア(Wikipedia)
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