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Pendulum (mathematics) : ウィキペディア英語版
Pendulum (mathematics)

The mathematics of pendulums are in general quite complicated. Simplifying assumptions can be made, which in the case of a simple pendulum allows the equations of motion to be solved analytically for small-angle oscillations.
== Simple gravity pendulum ==

A so-called "simple pendulum" is an idealization of a "real pendulum" but in an isolated system using the following assumptions:
* The rod or cord on which the bob swings is massless, inextensible and always remains taut;
* The bob is a point mass;
* Motion occurs only in two dimensions, i.e. the bob does not trace an ellipse but an arc.
* The motion does not lose energy to friction or air resistance.
* The gravitational field is uniform.
* The support does not move.
The differential equation which represents the motion of a simple pendulum is
where g is acceleration due to gravity, \ell is the length of the pendulum, and \theta is the angular displacement.
,
where \mathbf is the length vector of the pendulum and \mathbf is the force due to gravity.
For now just consider the magnitude of the torque on the pendulum.
:\mathbf = -mg l \sin\theta,
where m is the mass of the pendulum, g is the acceleration due to gravity, l is the length of the pendulum
and \theta is the angle between the length vector and the force due to gravity.
Next rewrite the angular momentum.
:\mathbf = \mathbf = m\mathbf.
Again just consider the magnitude of the angular momentum.
: \mathbf = mr^2 \omega = m l^2 .
and its time derivative
: \mathbf = m l^2 ,
According to \over dt} }, we can get by comparing the magnitudes
:-mgl \sin\theta = m l^2 ,
thus:
: + \sin\theta = 0,
which is the same result as obtained through force analysis.
}}
|}
= \sqrt \\
& =

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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