Shouldn't angular displacement be defined only on $[-\pi,\pi)$?

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I'm used to displacement being a measure which ignores the path taken, like so:

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but when I read about angular displacement, it seems to be more like a distance than a displacement. For instance, in this NASA graphic it's given as $$\phi=\theta_1-\theta_0,\tag{1}$$ so, for instance, if $\theta_1=\frac{3\pi}{2}$ and $\theta_0=0$, we have \begin{align} \phi =\frac{3\pi}{2}-0 =\frac{3\pi}{2}. \end{align}

But the linear distance travelled is $\frac{3\pi}{2}r$ and the linear displacement is $\sqrt{2}r$, so, by analogy, shouldn't we say the angular distance traveled is $\frac{3\pi}{2}$ and the angular displacement is $-\frac{\pi}{2}$?

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But since angular displacements are measured mod $2\pi$ (i.e., we care only about the "principal value"), the values $\frac{3\pi}{2}$ and $-\frac{\pi}{2}$ are equivalent/congruent.

On the other hand, the correct angular analogue of "distance travelled" is "rotation angle" or "angle rotated through", rather.