Changes

Jump to navigation Jump to search
1,495 bytes removed ,  18:22, January 28, 2013
Line 15: Line 15:  
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.
   −
==Angular momentum==
+
SCIENCE IS USELESS! GOD>SCIENCE!
−
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]
    
[[Category:Physics]]
 
[[Category:Physics]]
21

edits

Navigation menu