Next let's think about the velocity vector when t = (pi)/2 .
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First look at three POINTS:
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(1) the "position" POINT P when t=(pi)/2, which is the head/end-point of the path (vector) when t = (pi)/2 ... think of this POINT P as the POINT on the curve when t = (pi)/2
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(2) the point that is the head/end of the velocity VECTOR when t = (pi)/2
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(3) the origin
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Now let's graph the VECTOR for the origin O to the point V
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Now let's "move" the vector OV as so it's initial/start point is P (rather than the origin O).
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So we are attaching the tail/start point of the velocity vector (when t=(pi)/2) to the point on the curve when t=(pi)/2.
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Prof. G: do the "magnetic" explaination !
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All done .
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