General Relativity (GR) is compatible with the SO(3) symmetry in the context of its local structure, as vielbeins transform under SO(3,1), which includes SO(3) as a subalgebra. However, solutions to Einstein's equations do not necessarily require global rotational symmetry, indicating that GR can accommodate a variety of geometries. The discussion highlights that while local symmetries are maintained, global solutions may not reflect these symmetries. The compatibility with SO(3) symmetry within the Lorentz group follows a similar reasoning. Overall, GR's flexibility allows for diverse solutions beyond strict rotational symmetry.