The complex line generated by v is
\{r[(\cos(\theta) v_r -\sin(\theta) v_i) + i(\sin(\theta) v_r +\cos(\theta) v_i)]:\\ r\ge 0, \theta\in[0, 2\pi]\}
So, essentially, it is a set of concentric ellipses. We consider one of them:
\{(\cos(\theta) v_r -\sin(\theta) v_i) + i(\sin(\theta) v_r +\cos(\theta) v_i): \theta\in[0, 2\pi]\}
As \theta increases, both (\cos(\theta) v_r -\sin(\theta) v_i) and (\sin(\theta) v_r +\cos(\theta) v_i) rotate in the ellipse, always being conjugate to each other.