I read this from "The Sagnac effect and its interpretation by Paul Langevin", in cylindrical coordinates $$ ds^2=c^2t^2-dr^2-r^2d\theta^2 $$
...This transformation means that the observer O (inertial) now uses a coordinate system that accompanies the disk in its rotation. From the inertial observer O point of view, the source, the detector and the non-inertial observer (assumed to be at the same place) are located on a radius with a fixed orientation, for instance $\theta=0$ . Neglecting a small second-order term in $ R \omega\over c $, the $ ds^2$ (relativistic invariant) takes the form $$ ds^2=c^2t^2-dr^2-r^2d\theta^2 -2r^2\omega\ d\theta\ dt $$ Following Langevin, this expression is called the metric of the rotating disk. It will be noted the presence of a cross term in $d\theta\ dt $, source of the impossibility of synchronizing clocks, uniformly distributed around the periphery of the disk and connected thereto (a relativistic phenomenon which is the essence of the Sagnac effect).
Could anyone clarify why the term $d\theta\ dt $ makes the clocks synchronization impossible?