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We can consider a given coordinate system as a reference frame within which we can describe the kinematics of an object. By the kinematics, I mean the position, the velocity, and the acceleration as a function of time, basically a geometric description of the motion. Some aspects of these kinematics will look different in different reference frames and Id like to examine that now. First, I want to define what I mean by an inertial reference frame. An inertial reference frame is one in which an isolated body, one with no net force acting on it, moves at constant velocity, where that constant velocity might be zero. Another way of saying this is that an inertial reference frame is one in which Newtons laws of motion apply. Recall that Newtons first law of motion states that an isolated object with no forces acting on it moves at constant velocity. So lets begin by considering an observer in a particular reference frame. Well call that reference frame S and denote it by coordina