Let's analyze the given position vector of the particle: \overrightarrow{r} = (a \cos \, \omega t) \widehat{i} + (a \sin \omega t) \widehat{j} .
This position vector indicates that the particle is moving in a circular path, where \(a\) is the radius of the circle, and \( \omega t \) is the angular position of the particle.
- First, we calculate the velocity of the particle by differentiating the position vector with respect to time \(t\):
\begin{align*}
\overrightarrow{v} &= \frac{d\overrightarrow{r}}{dt} \\
&= \frac{d}{dt} \left( (a \cos \omega t) \widehat{i} + (a \sin \omega t) \widehat{j} \right) \\
&= \left( -a \omega \sin \omega t \right) \widehat{i} + \left( a \omega \cos \omega t \right) \widehat{j}.
\end{align*}
- The velocity vector is \overrightarrow{v} = (-a \omega \sin \omega t) \widehat{i} + (a \omega \cos \omega t) \widehat{j} .
- Now, check if the velocity vector is perpendicular to the position vector. For two vectors to be perpendicular, their dot product should be zero.
- Calculate the dot product of the position vector \overrightarrow{r} and velocity vector \overrightarrow{v} :
\begin{align*}
\overrightarrow{r} \cdot \overrightarrow{v} &= ((a \cos \omega t) \widehat{i} + (a \sin \omega t) \widehat{j}) \cdot ((-a \omega \sin \omega t) \widehat{i} + (a \omega \cos \omega t) \widehat{j}) \\
&= (a \cos \omega t) (-a \omega \sin \omega t) + (a \sin \omega t) (a \omega \cos \omega t) \\
&= -a^2 \omega \cos \omega t \sin \omega t + a^2 \omega \sin \omega t \cos \omega t \\
&= 0.
\end{align*}
Since the dot product is zero, the velocity vector is indeed perpendicular to the position vector.
Conclusion: The correct answer is that the velocity of the particle is perpendicular to the position vector.