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  2. Kater's pendulum - Wikipedia

    en.wikipedia.org/wiki/Kater's_pendulum

    A Kater's pendulum is a reversible free swinging pendulum invented by British physicist and army captain Henry Kater in 1817 (made public on 29 January 1818), [1] for use as a gravimeter instrument to measure the local acceleration of gravity.

  3. Moment of inertia - Wikipedia

    en.wikipedia.org/wiki/Moment_of_inertia

    For a simple pendulum, this definition yields a formula for the moment of inertia I in terms of the mass m of the pendulum and its distance r from the pivot point as, =. Thus, the moment of inertia of the pendulum depends on both the mass m of a body and its geometry, or shape, as defined by the distance r to the axis of rotation.

  4. Category:Pendulums - Wikipedia

    en.wikipedia.org/wiki/Category:Pendulums

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  5. Henry Kater - Wikipedia

    en.wikipedia.org/wiki/Henry_Kater

    His first major contribution to science was the comparison of the merits of the Cassegrainian and Gregorian telescopes; Kater determined the latter to be an inferior design. [ 1 ] His most substantial work was the invention of Kater's pendulum , enabling the strength of gravity to be determined, first at London [ 2 ] and subsequently at various ...

  6. Pendulum (mechanics) - Wikipedia

    en.wikipedia.org/wiki/Pendulum_(mechanics)

    A pendulum is a body suspended from a fixed support such that it freely swings back and forth under the influence of gravity. When a pendulum is displaced sideways from its resting, equilibrium position, it is subject to a restoring force due to gravity that will accelerate it back towards the equilibrium position.

  7. Kater pendulum - Wikipedia

    en.wikipedia.org/?title=Kater_pendulum&redirect=no

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  8. Index of physics articles (K) - Wikipedia

    en.wikipedia.org/wiki/Index_of_physics_articles_(K)

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  9. Center of percussion - Wikipedia

    en.wikipedia.org/wiki/Center_of_percussion

    For a free, rigid beam, an impulse is applied at right angle at a point of impact, defined as a distance from the center of mass (CM). The force results in the change in velocity of the CM, i.e. d v c m {\displaystyle dv_{cm}} :

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