Vectors in Rn

Definition and Properties

We assume that you are already familiar with vectors in R2 and R3, so that you will see that the definition extends naturally. 

A vector in Rn is a n x 1 matrix.

        

The set of all vectors in Rn is called n-space.

We define the sum and difference of two vectors and the product of a scalar and a vector by just realizing that vectors are matrices. 

 

Example

Let

                then             


Properties of Vectors

Vectors enjoy the following properties. 

If u, v, and w are vectors and c and d are scalars, then

 

  1. u + v  =  v + u

  2. u + (v + w)  =  (u + v) + w 

  3. There is a 0 with u + = 0 + u  =  u for all vectors u.

  4. For any u there is a -u with u + (-u)  =  0.

  5. cu is a vector in Rn.

  6. c(u + v)  =  cu + cv

  7. (c + d)u  =  cu + du

  8. c(du)  =  (cd)u

  9. 1u  =  u 

The proofs of all of these come from the properties of real numbers since the definition of addition subtraction and scalar multiplication is given componentwise.  For example to prove number 6, we have

        [(c + d)u]i  =  (c + d)[u]i  =  c[u]i + d[u]i  =  [cu]i + [du]i 


Dot Product and Length

Just as we defined the dot product for vectors in R2 and R3, we similarly define the dot product for two vectors in the more general Rn.  

Definition

Let

       

then the dot product (or scalar product) of u and v is defined by

        u . v  =  S uivi

We define the length or magnitude of a vector as 

       

A vector is a unit vector if it has length one.  The unit vector in the direction of u is given by

          u
                   
         ||u||

and the distance between u and v by

        Distance  =  ||u - v||

The angle q between two vectors is defined by

                            u . v
        cos q  =                      
                           ||u|| ||v||

u  and v are orthogonal if

        u . =  0

        

Example

Let

       

as in the first example, then

        u . v  =  (1)(-4) + (4)(2) + (3)(0) + (2)(4)  =  12

and the distance between u and v is

       

The unit vector in the direction of u is 

       

The angle between u and v is defined by

       

and 

       


Properties of the Dot Product

Next we give some basic properties of the dot product.

Let u, v, and w be vectors and c be a scalar, then

  1. u . u  > 0;  u . u  =  0  if and only if u  =  0.

  2. u .=  v . u.

  3. (u + v) . w  =  u . w v . w.

  4. (cu) . v  =  u . (cv)  =  c(u . v).

 

We will prove property 2 and leave the rest of the proofs for you.  

Proof of 2

        u .S uivi  =  S viui  =  v . u


Another important property called the Cauchy-Schwartz inequality is important enough to stand by itself.  

Cauchy-Schwartz Inequality

If u and v are vectors then 

        |u . v|   <  ||u|| ||v||

If equality holds, we say that u and v are parallel.  This will occur only if u is a multiple of v.

 

Proof

The proof is this is quite tricky.  We let x be a scalar and note from property 1 that 

        0 < (xu + v) . (xu + v)

        =   u . u x2 +  2 u . v x + v . v

Since the dot product produces a scalar, the above equation is a quadratic in x.  A quadratic that is always positive has nonpositive discriminant.  Hence

        (2 u . v)2 - 4(u . u)(v . v<  0

dividing by 4 gives

        (u . v)2 - (u . u)(v . v<  0

or 

                (u . v)2  <   (u . u)(v . v)  

Taking the square root of both sides produces the result.


The final property of the dot product that we will discuss comes from geometry.  We all know that the shortest distance between two points is a straight line.  If we want to travel from the origin to a point P, it is quicker to go along the straight path then to go to a point Q first and then to P.  If we choose the point P to be the tip of the vector u + v, and Q to be the tip of the vector u, then we have a following diagram.

       

This leads us the the triangle inequality.

 

The Triangle Inequality

If u and v are vectors then 

        ||u + v||  <  ||u|| + ||v||

 

Proof

  We take the square of the left hand side

        ||u + v||2  =  (u + v) . (u + v)  =  u . u + 2 u . v + v . v

        =  ||u||2 + 2(u . v) + ||v||2   <   ||u||2 + 2||u|| ||v|| + ||v||2         by Cauchy-Schwartz

        =  (||u|| + ||v||)2 



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