Fisica

Chapter 2 Kinematics in One Dimension
2.1 Displacement
There are two aspects to any motion. In a purely descriptive sense, there is the movement itself. Is it rapid or slow, for instance? Then, there is the issue of what causes the motion or what changes it, which requires that forces be considered. Kinematics deals with the concepts that are needed to describe motion. without any reference to forces. The present chapter discusses these concepts as they apply to motion in one dimension, and the next chapter treats two-dimensional motion. Dynamics deals with the effect that forces have on motion, a topic that is considered in Chapter 4. Together, kinematics and dynamics form the branch of physics known as mechanics. We turn now to the first of the kinematics concepts to be discussed, which is displacement. To describe the motion of an object, we must be able to specify the location of the object at all times, and Figure 2.1 shows how to do this for one-dimensional motion. In this drawing, the initial position of a car is indicated by the vector labeled x 0 . The length of x 0 is the distance of the car from an arbitrarily chosen origin. At a later time the car has moved to a new position, which is indicated by the vector x. The displacement of the car x (read as “delta x” or “the change in x”) is a vector drawn from the initial position to the final position. Displacement is a vector quantity in the sense discussed in Section 1.5, for it conveys both a magnitude (the distance between the initial and final positions) and a direction. The displacement can be related to x 0 and x by noting from the drawing that x0 x x or x x x0

Origin t0

t

x0

Displacement = ∆x x

Figure 2.1 The displacement

x is a

vector that points from the initial position x0 to the final position x.

Thus, the displacement x is the difference between x and x 0 , and the Greek letter delta ( ) is used to signify this difference. It is important to note that the change in any