Difference between revisions of "Forest UCM RBM"
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Consider a rigid body that rotates about a fixed z-axis with the origin at point O. | Consider a rigid body that rotates about a fixed z-axis with the origin at point O. | ||
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+ | INSERT PICTURE HERE | ||
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let | let | ||
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:<math>\vec{r}_k^{\prime}</math> points from the center of mass to the mass element <math>m_k</math> | :<math>\vec{r}_k^{\prime}</math> points from the center of mass to the mass element <math>m_k</math> | ||
− | + | the angular momentum of mass element <math>m_k</math> about the point O is given as | |
+ | :<math>\ell_k = \vec {r}_k \times \vec {p}_k = \vec {r}_k \times m \vec {\dot r}_k</math> | ||
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Let | Let |
Revision as of 01:58, 19 November 2014
Rigid Body Motion
Rigid Body
- Rigidy Body
- A Rigid Body is a system involving a large number of point masses, called particles, whose distances between pairs of point particles remains constant even when the body is in motion or being acted upon by external force.
- Forces of Constraint
- The internal forces that maintain the constant distances between the different pairs of point masses.
Consider a rigid body that rotates about a fixed z-axis with the origin at point O.
INSERT PICTURE HERE
let
- point to the center of mass of the object
- points to a mass element
- points from the center of mass to the mass element
the angular momentum of mass element
about the point O is given as
Let
- the kth mass of a particle located at the distance , from the origin, and moving with the velocity and angular velocity . \psi represents the angle the point mass makes with the line OA used as a reference point for the rotation angle of the rigid body.
The particle moves about the rotation axis in a circle of radius