Acceleration is the time derivative of velocity, equivalently the second derivative of position:It is a vector with SI unit . A change in direction produces acceleration even if speed stays constant. For example, a car rounding a bend at steady speed needs an inward resultant force by Newton's second law. Thus acceleration does not mean only speeding up. When , the dot product gives : a perpendicular acceleration changes direction without changing speed at that instant.
Take counterclockwise circular motion about the origin with radius and constant angular speed . The position, velocity and acceleration areThe speed is throughout, while the inward centripetal acceleration has magnitude . At the four cardinal points, reached at , the velocities in are ; the accelerations in are . The vectors turn together, remaining perpendicular. [ref]
https://openstax.org/books/university-physics-volume-1/pages/4-4-uniform-and-nonuniform-circular-motion. Ling, Sanny and Moebs, section 4.4: uniform circular motion
The proof outline is just two applications of the chain rule to ; then fixes both magnitudes. The usefulness is geometric: turning requires a force even when a speed reading remains steady, and doubling speed at fixed radius quadruples the required centripetal acceleration. The same mechanism appears in a circular orbit.
Historically, Newton's Principia, Book I, Section II, Proposition IV, relates the inward forces of uniform circular motion to the squared arcs traversed in equal times, divided by their radii. In modern notation, its dependence on speed and radius is ; Newton presents a geometric argument rather than the coordinate derivatives above. [ref]
https://en.wikisource.org/wiki/The_Mathematical_Principles_of_Natural_Philosophy_(1729)/Book_1/Section_2. Newton, Principia, Book I, Proposition IV; Motte's 1729 translation
New to topics? Read the docs here!
