Systematic Approach
Every rotation has two characteristics. The first one is the axis of rotation and the second one is the angle of rotation. Suppose that you have a given vector $\bf{r}$. Then, we want to find the rotation of this vector around the axis $L$ with the director $\bf{l}$ by the angle $\Phi$. If we call the vector after rotation $\bf{r'}$, then it can be proved that the following formula will hold
$$\boxed{
{\bf{r'}} = \cos \Phi {\bf{r}} + \sin \Phi {\bf{l}} \times {\bf{r}} + \left( {1 - \cos \Phi } \right)\left( {{\bf{r}}.{\bf{l}}} \right){\bf{l}}
}$$
you can find the proof on the net. Now, in your question we have
$$\eqalign{
& {\bf{r}} = \left( {1,2,2} \right) \cr
& \Phi = \frac{\pi }{2} \cr
& {\bf{l}} = \frac{{{\bf{r}} \times {\bf{i}}}}{{\left\| {{\bf{r}} \times {\bf{i}}} \right\|}}\,\,\,\,\,\, \to \,\,\,\,\,{\bf{r}}.{\bf{l}} = 0 \cr} $$
put it into the formula and do the computations. In this case, the formula reduces to
$${\bf{r'}} = {\bf{l}} \times {\bf{r}}$$
Your Approach
If you want to solve the problem by writing down equations and solving for the three unknown components of ${{\bf{r'}}}$ there is some other ways. In your problem ${\bf{r'}}.{\bf{l}} = 0$ and $\Phi = \frac{\pi }{2}$ hold. We can take advantage of these. So the system that you should solve is
$$\eqalign{
& {\bf{r'}}.{\bf{r}} = 0 \cr
& r' = r \cr
& {\bf{r'}}.{\bf{l}} = 0 \cr} $$
where the first one states that the rotated vector is perpendicular to the original one. The second one says that the length of the rotated vector and the original vector are equal. The third one emphasize this fact that the rotated vector is in the plane perpendicular to the rotation axis.