Let us mark the horizontal diameter AB = 2r of the log at the moment it passes through the equilibrium position.
Let us now consider the log at the instant when the ropes on which it is suspended are deflected from the vertical by a small angle α (Fig. 187).
In the absence of slippage of the ropes, we can easily find from geometrical considerations that the diameter AB always remains horizontal in the process of oscillations. Indeed, if EF ⊥ DK, FK = 2r tan α ≈ 2rα. But BD ≈ FK/2 ≈ rα. Consequently, ∠BOD, α as was indicated above. Since the diameter AB remains horizontal all the time, the log performs translatory motion, i.e. the velocities of all its points are the same at each instant. Therefore, the motion of the log is synchronous to the oscillation of a simple pendulum of length I. Therefore, the period of small oscillations of the log is