Question:
A rigid, uniform rod of length $L$ and mass $M$ is pivoted to the origin $O$ at one end, and is then left to swing freely in a vertical plane.
If the angle the rod makes with the vertical is $\theta$, show that the kinetic energy of the rod is $$T = \frac 16 ML^2{\dot \theta} ^2$$
Attempt:
In terms of $\theta$, the position of the center of mass is
$$(x,y) = \bigg(\frac L2 \sin \theta, -\frac L2 \cos \theta \bigg)$$
In a previous part of the question, I have shown that the moment of inertia of the rod about one of its endpoints is $$I = \frac 13 ML^2$$
Thus, the total kinetic energy of the rod should be
\begin{align} T & = \frac 12 M(\dot x^2 + \dot y^2) + \frac 12 I \omega ^2 \\ & = \frac 12 M\bigg[\bigg(\frac L2 \dot \theta\cos \theta \bigg)^2 + \bigg(\frac L2 \dot \theta \sin \theta\bigg)^2 \bigg] + \frac 12\bigg(\frac 13 ML^2 \bigg) \dot \theta ^2 \\ & = \frac 18 ML^2 \dot \theta ^2 + \frac 16 ML^2 \dot \theta ^2 \\ & \neq \frac 16 ML^2 \dot \theta ^2 \end{align}
Is this perhaps not the right way to do this question?