Difference between revisions of "Forest UCM RBM"
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::<math> = \sum (\vec R + \vec{r}_k^{\;\; \prime}) \times m_k (\vec \dot R + \vec{\dot r}_k^{\;\; \prime})</math> | ::<math> = \sum (\vec R + \vec{r}_k^{\;\; \prime}) \times m_k (\vec \dot R + \vec{\dot r}_k^{\;\; \prime})</math> | ||
::<math> = \sum \vec R \times m_k \vec \dot R + \sum \vec R \times m_k \vec{\dot r}_k^{\;\; \prime} + \sum \vec{r}_k^{\;\; \prime} \times m_k \vec \dot R +\sum \vec{r}_k^{\;\; \prime} \times m_k \vec{\dot r}_k^{\;\; \prime} </math> | ::<math> = \sum \vec R \times m_k \vec \dot R + \sum \vec R \times m_k \vec{\dot r}_k^{\;\; \prime} + \sum \vec{r}_k^{\;\; \prime} \times m_k \vec \dot R +\sum \vec{r}_k^{\;\; \prime} \times m_k \vec{\dot r}_k^{\;\; \prime} </math> | ||
+ | |||
+ | |||
+ | : <math>\sum \vec R \times m_k \vec \dot R = \vec R \times \sum m_k \vec \dot R = \vec R \times M \vec \dot R = \vec R \times \vec P</math> | ||
+ | |||
+ | ::<math>\vec P =</math> momentum of the center of Mass | ||
+ | |||
+ | :<math>\sum \vec R \times m_k \vec{\dot r}_k^{\;\; \prime} =</math> | ||
+ | : <math>\sum \vec{r}_k^{\;\; \prime} \times m_k \vec \dot R =</math> | ||
+ | :<math>\sum \vec{r}_k^{\;\; \prime} \times m_k \vec{\dot r}_k^{\;\; \prime} =</math> | ||
[[Forest_Ugrad_ClassicalMechanics#Rigid_Body_Motion]] | [[Forest_Ugrad_ClassicalMechanics#Rigid_Body_Motion]] |
Revision as of 13:19, 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
- momentum of the center of Mass