Given a smooth vector-valued function r(t). Any vector parallel to r′(t0) is tangent to the graph of r(t) at t=t0. It is often useful to consider just the direction of r′(t) and not its magnitude.
Therefore we are interested in the unit vector in the direction of r′(t)
This leads to a definition.
Let r(t) be a smooth function on an open interval I. The unit tangent vector T(t) is
T(t)=∣∣r′(t)∣∣1r′(t),∣∣r′(t)∣∣=0
Let v(t)=r′(t) denote the velocity vector. Then we define the unit tangent vectorby as the unit vector in the direction of the velocity vector.
T(t)=∣∣v(t)∣∣1v(t),∣∣v(t)∣∣=0
The tangential component of acceleration is in the direction of the unit tangent vector
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