When a rigid body rotates about a fixed axis, all points experience the same angular acceleration due to the uniform application of torque. The relationship between torque and angular acceleration is expressed through the equation τ = Iα, where I is the moment of inertia and α is the angular acceleration. This uniformity occurs because the body is treated as a single entity in classical mechanics, with properties averaged across its constituent particles. The assumption of no deformation allows for this simplification, leading to a consistent angular acceleration for the entire body. Understanding this concept is crucial for analyzing rotational dynamics in physics.