Difference between revisions of "Forest UCM RBM"
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:<math> \vec L = \sum \ell_k = \sum \vec {r}_k \times m \vec {\dot r}_k</math> | :<math> \vec L = \sum \ell_k = \sum \vec {r}_k \times m \vec {\dot r}_k</math> | ||
+ | This can be cast in term of the angular momentum about the center of mass and the angular momentum of the motion | ||
− | + | :<math>\vec {r}_k = \vec R + \vec{r}_k^{\prime}</math> | |
− | : | ||
− | |||
− | |||
[[Forest_Ugrad_ClassicalMechanics#Rigid_Body_Motion]] | [[Forest_Ugrad_ClassicalMechanics#Rigid_Body_Motion]] |
Revision as of 02:02, 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 asThe total angular momentum about the point O is given as
This can be cast in term of the angular momentum about the center of mass and the angular momentum of the motion