Given a smooth vector-valued function "\\overrightarrow{r}(t)". Any vector parallel to "\\overrightarrow{r}'(t_0)" is tangent to the graph of "\\overrightarrow{r}(t)" at "t=t_0." It is often useful to consider just the direction of "\\overrightarrow{r}'(t)" and not its magnitude.
Therefore we are interested in the unit vector in the direction of "\\overrightarrow{r}'(t)"
This leads to a definition.
Let "\\overrightarrow{r}(t)" be a smooth function on an open interval "I." The unit tangent vector "\\overrightarrow{T}(t)" is
Let "\\overrightarrow{v}(t)=\\overrightarrow{r}'(t)" denote the velocity vector. Then we define the unit tangent vector by as the unit vector in the direction of the velocity vector.
The tangential component of acceleration is in the direction of the unit tangent vector
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