|  |    The problem is that a straight line tangent to a circular arc
   has only first order geometric continuity.  That is, the curvature
   undergoes a discontinuous jump, and this is felt as a sudden
   force.
   Any curve which joins the circular arc and the straight line which
   has 3-rd order geometric continuity could smooth out the jump
   in acceleration.  A cubic curve in the shape of a spiral is the
   minimum order polynomial curve which would accomplish this.
   You could also think of it in terms of Fourier analysis - the idea
   would be to have no harmonics below a certain order in the path
   by "low pass filtering" the path.
   Here's a possible way.  Suppose you approach a circle of radius
   1 from below at a speed of w units per second, meeting it at (1,0)
   at t = 0, and thereafter follow the circle with velocity w radians per
   second.
   then
	x(t) = 1,		y(t) = wt		t < 0
	x(t) = cos(wt),		y(t) = sin(wt)		t >= 0
	x'(t) = 0,		y'(t) = w		t < 0
	x'(t) = -w*sin(wt),	y'(t) = w*cos(wt)	t >= 0
	x''(t) = 0,		y''(t) = 0		t < 0
	x''(t) = -w^2*cos(wt),	y''(t) = -w^2*sin(wt)	t >= 0
    You can see a jump in the second x derivative at t = 0; simply
    specify an acceleration that smoothly joins the discontinuity
    over some time interval [-tau,0] so that the path still meets the circle.
    It could even be a simple linear ramp in x acceleration...  upon
    integration this would give a cubic curve.
    - Jim
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