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Spatial acceleration
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Spatial acceleration : ウィキペディア英語版
Spatial acceleration
In physics the study of rigid body motion provides for several ways of defining the acceleration state of a rigid body. The classical definition of acceleration entails following a single particle/point along the rigid body and observing its changes of velocity. In this article the notion of spatial acceleration is explored, which entails looking at a fixed (unmoving) point in space and observing the changes of velocity of whatever particle/point happens to coincide with the observation point. This is similar to the acceleration definition fluid dynamics where typically one can measure velocity and/or accelerations on a fixed locate inside a testing apparatus.
== Definition ==
Consider a moving rigid body and the velocity of a particle/point ''P'' along the body being a function of the position and velocity of a center particle/point ''C'' and the angular velocity \vec \omega.
The linear velocity vector \vec v_P at ''P'' is expressed in terms of the velocity vector \vec v_C at ''C'' as:
\vec v_P = \vec v_C + \vec \omega \times (\vec r_P-\vec r_C)
where \vec \omega is the angular velocity vector.
The material acceleration at ''P'' is:
\vec a_P = \frac \vec v_P} t}
\vec a_P = \vec a_C + \vec \alpha \times (\vec r_P-\vec r_C) + \vec \omega \times (\vec v_P-\vec v_C)
where \vec \alpha is the angular acceleration vector.
The spatial acceleration \vec \psi_P at ''P'' is expressed in terms of the spatial acceleration \vec \psi_C at ''C'' as:
\vec \psi_P = \frac
\vec_ = \vec_+\vec\times(\vec_-\vec_)
which is similar to the velocity transformation above.
In general the spatial acceleration \vec \psi_P of a particle point ''P'' that is moving with linear velocity \vec v_P is derived from the material acceleration \vec a_P at ''P'' as:
\vec_=\vec_-\vec\times\vec_
}

抄文引用元・出典: フリー百科事典『 ウィキペディア(Wikipedia)
ウィキペディアで「Spatial acceleration」の詳細全文を読む



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