Suppose \(\vec {p} : \R \to \R ^3\) is a vector-valued function; its image is a curve in \(\R ^3\).

Let \(\vec {v}(t) = \vec {p}'(t)\) be the derivative, and \(\vec {a}(t) = \vec {p}''(t)\) be the second derivative.

Suppose for all \(t \in \R \) that \(|\vec {v}(t)| = 1\).

Then \(\vec {a}(t) \dotp \vec {v}(t) = \answer {0}\).

We are told that \(\vec {v}(t) \dotp \vec {v}(t) = 1\).
Therefore \(\dd {t} \left ( \vec {v}(t) \dotp \vec {v}(t) \right ) = 0\).
By the product rule, \(\dd {t} \left ( \vec {v}(t) \dotp \vec {v}(t) \right )\) is \(\vec {a}(t) \dotp \vec {v}(t) + \vec {v}(t) \dotp \vec {a}(t)\).
By commutativity of dot product, this means that \(\dd {t} \left ( \vec {v}(t) \dotp \vec {v}(t) \right )\) is \(2 \cdot \vec {a}(t) \dotp \vec {v}(t)\).
Since \(\dd {t} \left ( \vec {v}(t) \dotp \vec {v}(t) \right )\) vanishes, it must be that \(\vec {a}(t) \dotp \vec {v}(t)\) vanishes as well.
Therefore we conclude \(\vec {a}(t) \dotp \vec {v}(t) = 0\).