For uniform (constant speed) circular motion, the speed, $v$ is the circumference divided by the period. The circumference is 10$\pi$ (in the same length units as $x$ and $y$) and the period is 1000 (seconds). The direction of the velocity vector is perpendicular to the radius vector from the center of the circle to point $(x,y)$, so $\vec{v}$ is parallel to $(y-5)\hat{i}-(x-5)\hat{j}$. Therefore
$$\vec{v} = \pm \frac{10\pi}{1000}\frac{(y-5)\hat{i}-(x-5)\hat{j}}{\sqrt{(x-5)^2+(y-5)^2}} = \frac{\pm \pi}{500}[(y-5)\hat{i}-(x-5)\hat{j}]$$
The $\pm$ sign indicates the velocity could be either clockwise (+) or counter-clockwise (-).
The acceleration has magnitude $v^2/r$ and its direction is opposite to the radius vector. Therefore
$$\vec{a} = \frac{-\pi^2}{5(500)^2}\frac{(x-5)\hat{i}+(y-5)\hat{j}}{\sqrt{(x-5)^2+(y-5)^2}} = \frac{-\pi^2}{5^2(500)^2}[(x-5)\hat{i}+(y-5)\hat{j}]$$