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| | An interesting case of a sideways force is a weight on the end of a string (like the Biblical slingshot used by [[David]] against [[Goliath]]). When you twirl the weight around above your head, the string is pulling the weight toward you - but it never gets any closer! This kind of force is called a [[centripetal force|centripetal]], or center seeking, force. | | An interesting case of a sideways force is a weight on the end of a string (like the Biblical slingshot used by [[David]] against [[Goliath]]). When you twirl the weight around above your head, the string is pulling the weight toward you - but it never gets any closer! This kind of force is called a [[centripetal force|centripetal]], or center seeking, force. |
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| − | SCIENCE IS USELESS! GOD>SCIENCE!
| + | ==Angular momentum== |
| | + | A rotating or orbiting body possesses angular momentum. Like linear momentum, angular momentum is a vector quantity and is conserved. An object's angular momentum changes only when a [[torque]] is applied to it. |
| | | | |
| | + | The magnitude of the angular momentum of a particle orbiting some origin (such as the [[earth]] orbiting the [[sun]]) is given by |
| | + | |
| | + | :<math>L=mvr</math> |
| | + | |
| | + | where |
| | + | |
| | + | *'''L''' is angular momentum |
| | + | *'''m''' is the mass of the particle |
| | + | *'''v''' is the linear velocity of the particle |
| | + | *'''r''' is the distance from the particle to the origin |
| | + | |
| | + | The direction of the angular momentum vector points perpendicularly to the plane formed by the object's orbit, in accordance with the [[right hand rule]]. |
| | + | |
| | + | In addition to orbital angular momentum, the earth has rotational angular momentum due to its spin. The equations for calculating rotational angular momentum depend on the object's [[moment of inertia]], and therefore the shape and density of the object. |
| | + | |
| | + | === Generalized momentum === |
| | + | The definition of momentum can be generalized in [[Lagrangian Dynamics|Lagrangian]] and [[Hamiltonian Dynamics|Hamiltonian]] dynamics, to |
| | + | |
| | + | <math> |
| | + | p=\frac{\partial L}{\partial \dot x} |
| | + | </math> |
| | + | |
| | + | where L is the [[Lagrangian]] and <math>\dot x</math> is the velocity. In some cases the generalized momentum is the same as the momentum defined above. For example, for a free particle the Lagrangian equals the [[kinetic energy]] and so |
| | + | |
| | + | <math> |
| | + | p=\frac{\partial (m\dot x^2/2)}{\partial \dot x}=m\dot x |
| | + | </math> |
| | + | |
| | + | as above. |
| | ==External Links== | | ==External Links== |
| | *[http://id.mind.net/~zona/mstm/physics/mechanics/momentum/momentum.html Momemtum] | | *[http://id.mind.net/~zona/mstm/physics/mechanics/momentum/momentum.html Momemtum] |
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| | [[Category:Physics]] | | [[Category:Physics]] |