This preview shows pages 1–3. Sign up to view the full content.
This preview has intentionally blurred sections. Sign up to view the full version.View Full Document
Unformatted text preview: 2 Traditional Vector Theory The earliest definition of a vector usually encountered is that a vector is a thing possessing length and direction. This is the arrow in space view with length naturally being the length of the arrow and direction being the direction the arrow is pointing. We will denote vectors by writing their name in boldface (e.g., v and a ) or by drawing a little arrow above their name (e.g., v and a ). Some examples of such vectors include the velocity of an object at a particular time and the acceleration of an object at a particular time. (For now, we are not considering vector fields; that is, our vectors will not be functions of time or position.) Perhaps the most fundamental of vectors are those describing relative position or dis- placement: If A and B are two points in space (i.e., positions in space), then the vector from A to B , denoted AB , is simply the arrow 1 starting at point A and ending at point B . AB gives you the direction and distance to move from position A to position B (hence the term relative position). We will use displacement vectors as the basic model for traditional vectors. Almost all other traditional vectors in physics velocities, accelerations, forces, etc. are derived from displacement vectors. For example, the velocity v of an object at a given position p is the limit v = lim Delta1 t pq Delta1 t where q is the position of the object Delta1 t time units after being at p . It is through these derivations that the properties we derive for displacement (relative position) vectors can be shown to hold for all the traditional vectors in physics. By the way, throughout this discussion, we are assuming that the points in space are points in a Euclidean space. We will discuss exactly what this means later (in another chapter). For now, assume high school geometry. In particular: 1. Any two points can be connected by a straight line segment (totally contained in the space) whose length is the distance between the two points. 2. The angles of each triangle add up to (or 180 degrees). 3. The laws of similar triangles hold. 4. Parallelograms are well defined. 1 officially, AB is a directed line segment . 8/25/2011 Traditional Vector Theory Chapter & Page: 22 Keep in mind that there are different Euclidean spaces. Two different flat planes, for example, are two different Euclidean spaces. ? Exercise 2.1: Give several reasons why a sphere is not a Euclidean space. 2 2.1 Fundamental Defining Concepts Fundamental Geometrically Defined Concepts The Two Fundamental Measurable Quantities Our goal is to develop the fundamental theory of vectors as things that are completely defined by length and direction, using the set of vectors describing relative position in some Euclidean space as a basic model. Keep in mind the requirement that length and direction completelyspace as a basic model....
View Full Document
This note was uploaded on 11/07/2011 for the course MA 607 taught by Professor Staff during the Summer '11 term at University of Alabama in Huntsville.
- Summer '11