In an inertial frame of reference S, a body can accelerate with constant acceleration a, but there cannot exist another inertial frame S' moving at speed u relative to S where the body does not accelerate. If the body does not accelerate in S', it must move with constant velocity, which contradicts the initial condition of acceleration. This principle holds true in both special relativity and Newtonian mechanics. Additionally, if acceleration is constant in frame S, it will not remain constant in frame S' due to the changing velocity of the moving object. Thus, the transformation of acceleration between frames reveals fundamental differences in how motion is perceived in relativity.