Another good example:
Let's repulse a long cylinder inside Isolated System. The repulse should hit the
cylinder away from object center mass. This hit energy splits for two object
movements. This cylinder starts rotation with translation movement. The Isolated
System starts move to opposite cylinder translation movement direction. During
this object movement let transform this cylinder to a sphere. This sphere is
rotating faster than cylinder because this object moment of inertia less than
cylinder moment of inertia. However this rotation does not make any sense for
translation momentum transfer. The sphere translation momentum is equal to
cylinder translation momentum. However from cylinder repulse action the system
takes higher translation momentum than sphere has. The sphere translation
momentum won't be enough to stop the Isolated System.
http://knol.google.com/k/alex-belov/paradox-of-classical-mechanics-2/1xmqm1l0s4y\
s/9#


--- In gravitationalpropulsionstevenson@yahoogroups.com, "abelov0927"
<abelov0927@...> wrote:
This is a good example is shown transfer between angular and linear momentums.
Unfortunately the simulator does not allow giving different angular velocities
for squares.
Anyway, on this model easy to understand these squares with different angular
velocities will take a different linear velocities on the end of action.
Base on my theory about frame of reference conversion for complicated movement,
the law of momentum conservation works, however for correct calculation need use
imaginary part of velocity.
The momentum is conserve. The frame of reference is changing. This frame of
reference exchange gives the system ability to move.