|
|
You can navigate through this E-Book using the menu to the left. For E-Books that have a Chapter/Section organization each option in the menu to the left indicates a chapter and will open a menu showing the sections in that chapter. Alternatively, you can navigate to the next/previous section or chapter by clicking the links in the boxes at the very top and bottom of the material.
Also, depending upon the E-Book, it will be possible to download the complete E-Book, the chapter containing the current section and/or the current section. You can do this be clicking on the E-Book, Chapter, and/or the Section link provided below.
For those pages with mathematics on them you can, in most cases, enlarge the mathematics portion by clicking on the equation. Click the enlarged version to hide it.
If you go back to the Euclidean n-space chapter where we first introduced the concept of vectors
you’ll notice that we also introduced something called a dot product. However, in this chapter, where we’re dealing
with the general vector space, we have yet to introduce anything even remotely
like the dot product. It is now time to
do that. However, just as this chapter
is about vector spaces in general, we are going to introduce a more general
idea and it will turn out that a dot product will fit into this more general
idea. Here is the definition of this
more general idea.
Note that we are assuming here that the scalars are real
numbers in this definition. In fact we
probably should have been using the terms “real vector space” and “real inner
product space” in this definition to make it clear. If we were to allow the scalars to be complex
numbers (i.e. dealing with a complex
vector space) the axioms would change slightly.
Also, in the rest of this section if we say that V is an inner product space we are
implicitly assuming that it is a vector space and that some inner product has
been defined on it. If we do not
explicitly give the inner product then the exact inner product that we are
using is not important. It will only be
important in these cases that there has been an inner product defined on the
vector space.
Here are some more examples of inner products.
|
Example 2 Suppose
that  and  are two vectors in  and that  ,
 ,
… ,  are positive
real numbers (called weights) then
the weighted Euclidean inner product is defined to be,

It is fairly simple to show that this is in fact an inner
product. All we need to do is show
that it satisfies all the axioms from Definition 1.
So, suppose that u,
v, and a are all vectors in  and that c
is a scalar.
First note that because we know that real numbers commute
with multiplication we have,

So, the first
axiom is satisfied.
To show the
second axiom is satisfied we just need to run through the definition as
follows,

and the second
axiom is satisfied.
Here’s the work
for the third axiom.

Finally, for
the fourth axiom there are two things we need to check. Here’s the first,

Note that this
is greater than or equal to zero because the weights  ,
 ,
… ,  are positive numbers. If we hadn’t made that assumption there
would be no way to guarantee that this would be positive.
Now suppose
that  .
Because each of the terms above is greater than or equal to zero the only way
this can be zero is if each of the terms is zero itself. Again, however, the weights are positive
numbers and so this means that

We therefore
must have  if  .
Likewise if  then by plugging in we can see that we must
also have  and so the fourth axiom is also satisfied.
|
                                         
The next two examples require that you’ve had Calculus and
so if you haven’t had Calculus you can skip these examples. Both of these however are very important
inner products in some areas of mathematics, although we’re not going to be
looking at them much here because of the Calculus requirement.
|
Example 4 Suppose
that  and  are two continuous functions on the interval
 . In other words, they are in the vector
space  . An inner product on  can be defined as,

Provided you
remember your Calculus, showing this is an inner product is fairly simple. Suppose that f, g, and h are continuous functions in  and that c
is any scalar.
Here is the
work showing the first axiom is satisfied.

The second
axiom is just as simple,

Here’s the
third axiom.

Finally, the
fourth axiom. This is the only one
that really requires something that you may not remember from a Calculus
class. The previous examples all used
properties of integrals that you should remember.
First, we’ll
start with the following,

Now, recall
that if you integrate a continuous function that is greater than or equal to
zero then the integral must also be greater than or equal to zero. Hence,

Next, if  then clearly we’ll have  . Likewise, if we have  then we must also have  .
|
| |