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In this section we’re going to take a look at an important
idea in the study of vector spaces. We
will also be drawing heavily on the ideas from the previous two sections and so
make sure that you are comfortable with the ideas of span and linear
independence.
We’ll start this section off with the following definition.
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Definition 1 Suppose
 is a set of vectors from the vector space V.
Then S is called a basis (plural is bases) for V if both of
the following conditions hold.
(a)  ,
i.e. S spans the vector space V.
(b) S is a linearly independent set of
vectors.
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Let’s take a look at some examples.
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Example 1 Determine
if each of the sets of vectors will be a basis for  .
(a)  ,
 and  . [Solution]
(b)  ,
 and  . [Solution]
(c)  and  . [Solution]
(d)  ,
 and  . [Solution]
Solution
(a)  ,
 and  .
Now, let’s see what we’ve got to do here to determine
whether or not this set of vectors will be a basis for  . First, we’ll need to show that these
vectors span  and from the section on Span
we know that to do this we need to determine if we can find scalars  ,
 ,
and  so that a general vector  from  can be expressed as a linear combination of
these three vectors or,

As we saw in
the section on Span all we need to do is convert this to a system of
equations, in matrix form, and then determine if the coefficient matrix has a
non-zero determinant or not. If the
determinant of the coefficient matrix is non-zero then the set will span the
given vector space and if the determinant of the coefficient matrix is zero
then it will not span the given vector space.
Recall as well that if the determinant of the coefficient matrix is
non-zero then there will be exactly one solution to this system for each u.
The matrix form
of the system is,

Before we get
the determinant of the coefficient matrix let’s also take a look at the other
condition that must be met in order for this set to be a basis for  . In order for these vectors to be a basis
for  then they must be linearly independent. From the section on Linear Independence we know that to
determine this we need to solve the following equation,

If this system
has only the trivial solution the vectors will be linearly independent and if
it has solutions other than the trivial solution then the vectors will be
linearly dependent.
Note however,
that this is really just a specific case of the system that we need to solve
for the span question. Namely here we
need to solve,

Also, as noted
above, if these vectors will span  then there will be exactly one solution to
the system for each u. In this case we know that the trivial
solution will be a solution, our only question is whether or not it is the
only solution.
So, all that we
need to do here is compute the determinant of the coefficient matrix and if
it is non-zero then the vectors will both span  and be linearly independent and hence the
vectors will be a basis for  . On the other hand, if the determinant is
zero then the vectors will not span  and will not be linearly independent and so
they won’t be a basis for  .
So, here is the
determinant of the coefficient matrix for this problem.

So, these
vectors will form a basis for  .
[Return to Problems]
(b)  ,
 and  .
Now, we could
use a similar path for this one as we did earlier. However, in this case, we’ve done all the
work for this one in previous sections.
In Example 4(a) of the section on
Span we determined that the standard basis vectors (Interesting name isn’t
it? We’ll come back to this in a bit)  ,
 and  will span  . Notice that while we’ve changed the
notation a little just for this problem we are working with the standard
basis vectors here and so we know that they will span  .
Likewise, in Example 1(c) from the section on
Linear Independence we saw that these vectors are linearly independent.
Hence based on
all this previous work we know that these three vectors will form a basis for
 .
[Return to Problems]
(c)  and  .
We can’t use
the method from part (a) here because the coefficient matrix wouldn’t be
square and so we can’t take the determinant of it. So, let’s just start this out be checking
to see if these two vectors will span  . If these two vectors will span  then for each  in  there must be scalars  and  so that,

However, we can
see right away that there will be problems here. The third component of the each of these
vectors is zero and hence the linear combination will never have any non-zero
third component. Therefore, if we
choose  to be any vector in  with  we will not be able to find scalars  and  to satisfy the equation above.
Therefore,
these two vectors do not span  and hence cannot be a basis for  .
Note however,
that these two vectors are linearly independent (you should verify
that). Despite this however, the
vectors are still not a basis for  since they do not span  .
(d)  ,
 and 
[Return to Problems]
In this case
we’ve got three vectors with three components and so we can use the same
method that we did in the first part.
The general equation that needs solved here is,

and the matrix
form of this is,

We’ll leave it to you to verify that  and so these three vectors do not span  and are not linearly independent. Either of which will mean that these three
vectors are not a basis for  .
[Return to Problems]
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Before we move on let’s go back and address something we
pointed out in Example 1(b). As we
pointed out at the time the three vectors we were looking at were the standard
basis vectors for 
. We should discuss the name a little more at
this point and we’ll do it a little more generally than in 
.
The vectors

will span 
as we saw in the section on Span and it is fairly
simple to show that these vectors are linearly independent (you should verify
this) and so they form a basis for 
. In some way this set of vectors is the
simplest (we’ll see this in a bit) and so we call them the standard basis vectors for 
.
We also have a set of standard basis vectors for a couple of
the other vector spaces we’ve been looking at occasionally. Let’s take a look at each of them.
Note that we only looked at the standard basis vectors for 
,
but you should be able to modify this appropriately to arrive at a set of
standard basis vector for 
in general.
Next let’s take a look at the following theorem that gives
us one of the reasons for being interested in a set of basis vectors.
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Theorem 1 Suppose
that the set  is a basis for the vector space V then every vector u from V can be expressed as a linear combination of the vectors from S in exactly one way.
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Proof : First,
since we know that the vectors in S
are a basis for V then for any vector
u in V we can write it as a linear combination as follows,
Now, let’s suppose that it is also possible to write it as
the following linear combination,
If we take the difference of these two linear combinations
we get,
However, because the vectors in S are a basis they are linearly independent. That means that this equation can only have
the trivial solution. Or, in other words,
we must have,
But this means that,
and so the two linear combinations were in fact the same
linear combination.

We also have the following fact. It probably doesn’t really rise to the level
of a theorem, but we’ll call it that anyway.
The proof here is so simple that we’re not really going to
give it. By assumption the set is
linearly independent and by definition V
is the span of S and so the set must
be a basis for V.
We now need to take a look at the following definition.
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Definition 2 Suppose
that V is a non-zero vector space
and that S is a set of vectors from
V that form a basis for V.
If S contains a finite
number of vectors, say  ,
then we call V a finite dimensional vector space and
we say that the dimension of V, denoted by  ,
is n (i.e. the number of basis elements in S). If V is not a finite dimensional vector space (so S does not have a finite number of
vectors) then we call it an infinite
dimensional vector space.
By definition the dimension of the zero vector space (i.e. the vector space consisting
solely of the zero vector) is zero.
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Here are the dimensions of some of the vector spaces we’ve
been dealing with to this point.
























We now need to take a look at several important theorems
about vector spaces. The first couple of
theorems will give us some nice ideas about linearly independent/dependent sets
and spans. One of the more important
uses of these two theorems is constructing a set of basis vectors as we’ll see
eventually.
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Theorem 3 Suppose
that V is a vector space and that  is any basis for V.
(a) If
a set has more than n vectors then
it is linearly dependent.
(b) If
a set has fewer than n vectors then
it does not span V.
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Proof :
(a) Let 
and suppose that 
. Since S
is a basis of V every vector in R can be written as a linear combination
of vectors from S as follows,
Now, we want to show that the vectors in R are linearly dependent. So, we’ll need to show that there are more
solutions than just the trivial solution to the following equation.
If we plug in the set of linear combinations above for the 
’s in this equation and collect all the
coefficients of the 
’s we arrive at.
Now, the 
’s are linearly independent and so we
know that the coefficients of each of the 
in this equation must be zero. This gives the following system of equations.
Now, in this system the 
’s are known scalars from the linear
combinations above and the 
’s are unknowns. So we can see that there are n equations and m unknowns. However, because

there are more unknowns than equations and so
by Theorem 2 in the
solving systems of equations section we know that if there are more unknowns
than equations in a homogeneous system, as we have here, there will be
infinitely many solutions.
Therefore the equation,
will have more solutions than the trivial solution and so
the vectors in R must be linearly
dependent.
(b) The proof of
this part is very similar to the previous part.
Let’s start with the set 
and this time we’re going to assume that 
. It’s not so easy to show directly that R will not span V, but if we assume for a second that R does span V we’ll see
that we’ll run into some problems with our basis set S. This is called a proof by
contradiction. We’ll assume the opposite
of what we want to prove and show that this will lead to a contradiction of
something that we know is true (in this case that S is a basis for V).
So, we’ll assume that R
will span V. This means that all the vectors in S can be written as a linear combination
of the vectors in R or,
Let’s now look at the equation,
Now, because S is
a basis we know that the 
’s must be linearly independent and so
the only solution to this must be the trivial solution. However, if we substitute the linear
combinations of the 
’s into this, rearrange as we did in
part (a) and then setting all the
coefficients equal to zero gives the following system of equations.
Again, there are more unknowns than equations here and so
there are infinitely many solutions.
This contradicts the fact that we know the only solution to the equation

is the trivial solution.
So, our original assumption that R spans V must be
wrong. Therefore R will not span V.

Proof :
(a) If 
we need to show that the set 
is linearly independent. So, let’s form the equation,
Now, if 
is not zero we will be able to write u as a linear combination of the 
’s but this contradicts the fact that u is not in 
. Therefore we must have 
and our equation is now,
But the vectors in S
are linearly dependent and so the only solution to this is the trivial
solution,
So, we’ve shown that the only solution to
is
Therefore, the vectors in R are linearly independent.
(b) Let’s suppose
that our set is 
and so we have 
. First, by assumption u is a linear combination of the remaining vectors in S or,
Next let w be any
vector in 
. So, w
can be written as a linear combination of all the vectors in S or,
Now plug in the expression for u above to get,
So, w is a linear
combination of vectors only in R and
so at the least every vector that is in 
must also be in 
.
Finally, if w is
any vector in 
then it can be written as a linear combination
of vectors from R, but since these
are also vectors in S we see that w can also, by default, be written as a
linear combination of vectors from S
and so is also in 
. We’ve just shown that every vector in 
must also be in 
.
Since we’ve shown that 
must be contained in 
and that every vector in 
must also be contained in 
this can only be true if 
.

We can use the previous two theorems to get some nice ideas
about the basis of a vector space.
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Theorem 5 Suppose
that V is a vector space then all
the bases for V contain the same
number of vectors.
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Proof : Suppose
that 
is a basis for V. Now, let R be any other basis for V.
Then by Theorem 3 above if R
contains more than n elements it
can’t be a linearly independent set and so can’t be a basis. So, we know that, at the least R can’t contain more than n elements. However, Theorem 3 also tells us that if R contains less than n elements then it won’t span V and hence can’t be a basis for V.
Therefore the only possibility is that R must contain exactly n
elements.

Proof : First
suppose that 
. If S
is linearly dependent then there must be some vector u in S that can be
written as a linear combination of other vectors in S and so by Theorem 4(b) we can remove u from S and our new set
of 
vectors will still span V. However, Theorem 3(b)
tells us that any set with fewer vectors than a basis (i.e. less than n in this
case) can’t span V. Therefore, S must be linearly independent and hence S is a basis for V.
Now, let’s suppose that S
is linearly independent. If S does not span V then there must be a vector u
that is not in 
. If we add u to S the resulting set
with 
vectors must be linearly independent by
Theorem 4(a). On the other hand, Theorem
3(a) tells us that any set with more vectors than the basis (i.e. greater than n) can’t be linearly independent.
Therefore, S must span V and hence S is a basis for V.

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Theorem 7 Suppose
that V is a finite dimensional
vector space with  and that S
is any finite set of vectors from V.
(a) If
S spans V but is not a basis for V
then it can be reduced to a basis for V
by removing certain vectors from S.
(b) If
S is linearly independent but is
not a basis for V then it can be
enlarged to a basis for V by adding
in certain vectors from V.
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Proof :
(a) If S spans V but is not a basis for V
then it must be a linearly dependent set.
So, there is some vector u in
S that can be written as a linear
combination of the other vectors in S. Let R
be the set that results from removing u
from S. Then by Theorem 4(b) R will still span V. If R
is linearly independent then we have a basis for V and if it is still linearly dependent we can remove another
element to form a new set 
that will still span V. We continue in this way
until we’ve reduced S down to a set
of linearly independent vectors and at that point we will have a basis of V.


(b) If S is linearly independent but not a
basis then it must not span V. Therefore, there is a vector u that is not in 
. So, add u
to S to form the new set R.
Then by Theorem 4(a) the set R
is still linearly independent. If R now spans V we’ve got a basis for V
and if not add another element to form the new linearly independent set 
. Continue in this fashion until we reach a set
with n vectors and then by Theorem 6
this set must be a basis for V.

Okay we should probably see some examples of some of these
theorems in action.
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Example 5 Reduce
each of the following sets of vectors to obtain a basis for the given vector
space.
(a)  ,
 ,
 and  for  . [Solution]
(b)  ,
 ,
 ,
 and  for  . [Solution]
Solution
First, notice that provided each of these sets of vectors
spans the given vector space Theorem 7(a) tells us that this can in fact be
done.
(a)  ,
 ,
 and  for  .
We will leave it to you to verify that this set of vectors
does indeed span  and since we know that  we can see that we’ll need to remove one
vector from the list in order to get down to a basis. However, we can’t just remove any of the
vectors. For instance if we removed  the set would no longer span  . You should verify this, but you can also
quickly see that only  has a non-zero first component and so will
be required for the vectors to span  .
Theorem 4(b) tells us that if we remove a vector that is a
linear combination of some of the other vectors we won’t change the span of
the set. So, that is what we need to
look for. Now, it looks like the last
three vectors are probably linearly dependent so if we set up the following
equation

and solve it,

we can see that
these in fact are linearly dependent vectors.
This means that we can remove any of these since we could write any
one of them as a linear combination of the other two. So, let’s remove  for no other reason that the entries in this
vector are larger than the others.
The following
set the still spans  and has exactly 3 vectors and so by Theorem
6 it must be a basis for  .

For the
practice you should verify that this set does span  and is linearly independent.
[Return to Problems]
(b)  ,
 ,
 ,
 and  for  .
We’ll go through this one a little faster. First, you should verify that the set of
vectors does indeed span  . Also, because  we know that we’ll need to remove two of the
vectors. Again, remember that each
vector we remove must be a linear combination of some of the other vectors.
First, it looks like  is a linear combination of  and  (you should verify this) and so we can
remove  and the set will still span  . This leaves us with the following set of
vectors.

Now, it looks
like  can easily be written as a linear
combination of the remaining vectors (again, please verify this) and so we
can remove that one as well.
We now have the
following set,

which has 3 vectors and will span  and so it must be a basis for  by Theorem 6.
[Return to Problems]
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