In the moment of force, we see the direction of $\vec{r}$ is taken from the center to the point (radially outwards).
A similar approach for Electric Dipole moment $\vec{p}$ shows us that, only if the direction is taken from -q to +q, the direction of the torque will go into the paper, which is the correct direction of rotation for the forces shown.
\(\vec{\tau}=\vec{r}\times\vec{F}\)
\(\hspace{1cm}=\vec{r}q\times\frac{\vec{F}}{q}\)
\(\hspace{1cm}=2\vec{a}q\times\vec{E}\)
\(\)
\(\vec{\tau}=\vec{p}\times\vec{E}\)
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