Vertically polarized light with intensity $I_{0}$ is normally incident on an ideal polarizer. As the polarizer is rotated about a horizontal axis, the intensity $I$ of light transmitted through the polarizer varies with the orientation of the polarizer $(\theta),$ where $\theta=0$ corresponds to a vertical transmission axis. Sketch a graph of $I$ as a function of $\theta$ for one complete rotation of the polarizer $\left(0 \leq \theta \leq 360^{\circ}\right)$.(W) tutorial: polarized light).