Angular velocity for a two-dimensional laminar object, such as a rod, remains consistent across all axes of rotation perpendicular to its plane due to the uniform distribution of angular acceleration. For a point at distance x from the rotation axis, the tangential velocity is proportional to the distance and angular acceleration, expressed as vx = xα. This relationship holds true for points at distances 2x and 3x, where v2x = 2xα and v3x = 3xα, respectively. Consequently, the relative angular acceleration remains constant across these points. This principle illustrates the uniformity of angular velocity in two-dimensional objects regardless of the axis of rotation.