Oscillations of hinged rigid body are described by the model of physical pendulum.
For mathematical pendulum "\\displaystyle T = 2 \\pi \\sqrt{\\frac{L}{g}}" where L is a length of pendulum.
For physical pendulum we can introduce equivalent length L - the distance from the pivot to the centre of oscillation.
"\\displaystyle L = \\frac{I}{mR}"
where where I is the moment of inertia of the pendulum about the pivot point, m is the mass of the pendulum, and R is the distance between the pivot point and the centre of the mass.
So, "\\displaystyle T = 2\\pi \\sqrt{\\frac{I}{mgR}}" .
Angular frequency "\\displaystyle \\omega = \\frac{2\\pi}{T} =\\sqrt{ \\frac{mgR}{I}}" .
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