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There are two directions: the r direction is the direction of a vector 
  from the origin to the point in question;
  a unit  vector in this direction has representation:
ur = i cos
+ 
  j sin
 
the
direction 
    is normal to this:
u
 
  = -i sin
 
  + j cos
 
The vector r is represented in this coordinate system by r 
    = rur , where r = (x2+y2)1/2;
    since we have
r(t) = x(t) i + y(t) j
we obtain
x = rcos
 
    , y = rsin![]()
Taking derivatives we find
![]()
verify by differentiating yourself that
 
which gives:
 
![]()

The second and fourth terms here are sometimes referred to in physics as the centrifugal and Coriolis forces. Thus if an object is subject to no external force, so that
![]()
you will find that it obeys
,
and
![]()
The former causes the radial velocity to grow if there is angular motion: the latter slows down the angular motion if the object is moving away from the origin.