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Mathematical Expression Editor
Matrices of Linear Transformations with Respect to Arbitrary Bases
We know that every linear transformation from \(\RR ^n\) into \(\RR ^m\) is a matrix transformation
(Theorem th:matlin of Standard Matrix of a Linear Transformation from \(\RR ^n\) to \(\RR ^m\)). What about
linear transformations between vector spaces other than \(\RR ^n\)? In this section we will
learn to represent linear transformations between arbitrary finite-dimensional vector
spaces using matrices. To do so, we will use the fact that every \(n\)-dimensional vector
space is isomorphic to \(\RR ^n\) (Corollary cor:ndimisotorn of Isomorphic Vector Spaces). What we do
here will serve as yet another example of how isomorphisms can be used to
translate problems in one vector space to another, more convenient, vector
space.
You should verify that \(\tau _2\) is linear. (See Practice Problem prob:taulinear.)
We will examine \(\tau _2\) in an effort to find a way to represent it with a matrix. (In the
process, we will also end up proving that \(\tau _2\) is an isomorphism, which is what you were
challenged to do in Isomorphic Vector Spaces.)
We will start by selecting a basis for each of \(\mathbb {M}_{2,2}\) and \(\mathbb {P}^3\). We can choose any basis for either
space, but we will choose bases that will make computations easier.
be our ordered bases or choice for \(\mathbb {M}_{2,2}\) and \(\mathbb {P}^3\), respectively.
Recall that a coordinate vector isomorphism maps a vector to its coordinate vector
with respect to the given ordered basis (Theorem ex:coordmapiso of Isomorphic Vector Spaces). In
the diagram below, let \(R\) and \(S\) be coordinate vector isomorphisms with respect to \(\mathcal {B}\) and
\(\mathcal {C}\).
Observe that \(T=S\circ \tau _2\circ R^{-1}\). Because \(T\) is a composition of linear transformations, \(T\) itself is linear
(Theorem th:complinear of Composition and Inverses of Linear Transformations). Thus, we
should be able to find the standard matrix for \(T\). To do this, find the images of
the standard unit vectors and use them to create the standard matrix \(A\) for
\(T\).
We say that \(A\) is the matrix of \(\tau _2\) with respect to ordered bases \(\mathcal {B}\) and \(\mathcal {C}\).
As a side-note, observe that \(\tau _2=S^{-1}\circ T\circ R\). Observe also that \(T\) is invertible because \(A\) is invertible.
So, \(T\) is an isomorphism. As a composition of isomorphisms, \(\tau _2\) is an isomorphism
(Theorem th:isocompisiso of Isomorphic Vector Spaces). While we could have proved this result
directly, as you were challenged to do in Isomorphic Vector Spaces, this approach is
much less tedious.
Our goal now is to find a matrix for \(T\) with respect to \(\mathcal {B}\) and \(\mathcal {C}\).
The information given in this problem is slightly different from the information in
Exploration init:taumatrix. Instead of being given an expression for the image of a generic vector of
\(V\), we are only given the images of the two basis vectors of \(V\). But this information is
sufficient to determine the linear transformation.
As before, we will map vectors of \(V\) and \(W\) to their coordinate vectors. Where are the
coordinate vectors located?
(a)
\([\vec {v}_1]_{\mathcal {B}}\) and \([\vec {v}_2]_{\mathcal {B}}\) are elements of \(\RR \), \(\RR ^2\), \(\RR ^3\)
(b)
\([\vec {w}_1]_{\mathcal {C}}\) and \([\vec {w}_2]_{\mathcal {C}}\) are elements of \(\RR \), \(\RR ^2\), \(\RR ^3\)
Here is a diagram that summarizes this information. (Press the arrow on the right to
expand.)
Define \(F:\RR ^2\rightarrow \RR ^2\) by \(F=S\circ T\circ R^{-1}\). \(F\) is a linear transformation that maps \(\begin{bmatrix}1\\0\end{bmatrix}\) and \(\begin{bmatrix}0\\1\end{bmatrix}\) to \(\begin{bmatrix}2\\-3\end{bmatrix}\) and \(\begin{bmatrix}-1\\4\end{bmatrix}\), respectively. Thus,
the standard matrix for \(F\) is:
\[A=\begin{bmatrix}2&-1\\-3&4\end{bmatrix}\]
We say that \(A\) is a matrix for \(T\) with respect to \(\mathcal {B}\) and \(\mathcal {C}\).
Let’s take a look at what this matrix can do for us. Recall that in Example ex:subtosub1 we found
that the image of \(\vec {v}=2\vec {v}_1+\vec {v}_2\) is
Let \(V\) and \(W\) be vector spaces with ordered bases \(\mathcal {B}=\{\vec {v}_1, \vec {v}_2, \vec {v}_3\}\) and \(\mathcal {C}=\{\vec {w}_1, \vec {w}_2\}\), respectively. Define a linear
transformation \(T:V\rightarrow W\) by
Find the matrix of \(T\) with respect to \(\mathcal {B}\) and \(\mathcal {C}\), and use it to find \(T(2\vec {v}_1-\vec {v}_2+3\vec {v}_3)\). Verify your answer by
computing \(T(2\vec {v}_1-\vec {v}_2+3\vec {v}_3)\) directly.
We start with a diagram:
Looking at the images of the standard unit vectors in \(\RR ^3\), we can construct the standard
matrix \(A\) of \(T\) with respect to \(\mathcal {B}\) and \(\mathcal {C}\).
\[A=\begin{bmatrix}2&-1&1\\-1&0&3\end{bmatrix}\]
Applying this matrix to the coordinate vector of \(2\vec {v}_1-\vec {v}_2+3\vec {v}_3\) we get
In this section we will formalize the process for finding the matrix of a linear
transformation with respect to arbitrary bases that we established through earlier
examples.
Let \(V\) and \(W\) be vector spaces with ordered bases \(\mathcal {B}=\{\vec {v}_1, \vec {v}_2,\ldots ,\vec {v}_n\}\) and \(\mathcal {C}=\{\vec {w}_1, \vec {w}_2,\ldots ,\vec {w}_m\}\), respectively. Suppose \(T:V\rightarrow W\) is a
linear transformation. Our goal is to find a matrix for \(T\) with respect to \(\mathcal {B}\) and
\(\mathcal {C}\).
Observe that \(\text {dim}(V)=n=\text {dim}(\RR ^n)\) and \(\text {dim}(W)=m=\text {dim}(\RR ^m)\). Let \(R:V\rightarrow \RR ^n\) and \(S:W\rightarrow \RR ^m\) be coordinate vector isomorphisms defined
by
We know that \(R\) is an isomorphism and \(R^{-1}\) exists. Consider the transformation
\[S\circ T\circ R^{-1}:\RR ^n\rightarrow \RR ^m\]
As a composition of linear transformation, \(S\circ T\circ R^{-1}\) is linear and thus has a standard matrix.
To find it, we need to determine the images of standard unit vectors \(\vec {e}_i\) under \(S\circ T\circ R^{-1}\). We have
the following:
Vectors \([T(\vec {v}_i)]_{\mathcal {C}}\) will become the columns of the standard matrix. We summarize this
discussion as a theorem.
Let \(V\) and \(W\) be finite-dimensional vector spaces with ordered bases \(\mathcal {B}=\{\vec {v}_1,\vec {v}_2,\ldots ,\vec {v}_n\}\) and \(\mathcal {C}\), respectively.
Suppose \(T:V\rightarrow W\) is a linear transformation.
Then \(A[\vec {v}]_{\mathcal {B}}=[T(\vec {v})]_{\mathcal {C}}\) for all vectors \(\vec {v}\) in \(V\).
Matrix \(A\) of Theorem 5 is called the matrix of \(T\) with respect to ordered bases \(\mathcal {B}\) and \(\mathcal {C}\).
In conclusion, observe how isomorphisms helped us solve the matrix of a linear
transformation problem. The coordinate mappings \(R\) and \(S\) are isomorphisms. This
means that \(V\) and \(\RR ^n\) are isomorphic and have the same structural properties. The same
is true for \(W\) and \(\RR ^m\). In this abstract discussion, we do not know anything about the
elements of \(V\) and \(W\), but isomorphisms allow us to take a problem that we do not
know much about and transform it to a familiar problem involving familiar
spaces.
The Inverse of a Linear Transformation and its Matrix
Let \(V\) and \(W\) be vector spaces. Suppose \(T:V\rightarrow W\) is an invertible linear transformation. This, of
course, means that \(T\) is an isomorphism, which means that
\[\mbox {dim}(V)=\mbox {dim}(W)\]
Let \(\mathcal {B}=\{\vec {v}_1, \vec {v}_2,\ldots ,\vec {v}_n\}\) and \(\mathcal {C}=\{\vec {w}_1, \vec {w}_2,\ldots ,\vec {w}_n\}\) be ordered bases of \(V\) and \(W\), respectively. We can find the matrix of \(T^{-1}\) with
respect to \(\mathcal {C}\) and \(\mathcal {B}\) by finding the standard matrix of the linear transformation
\(R\circ T^{-1}\circ S^{-1}:\RR ^n\rightarrow \RR ^n\).
Observe that \(R\circ T^{-1}\circ S^{-1}\) is the inverse of \(S\circ T\circ R^{-1}\). So, if \(A\) is the standard matrix of \(S\circ T\circ R^{-1}\), then \(A^{-1}\)
is the standard matrix of \(R\circ T^{-1}\circ S^{-1}\). Thus, \(A^{-1}\) is the matrix of \(T^{-1}\) with respect to \(\mathcal {C}\) and
\(\mathcal {B}\).
Find the matrix of \(T^{-1}\) with respect to ordered bases \(\mathcal {C}=\left \{\begin{bmatrix}1\\0\end{bmatrix},\begin{bmatrix}0\\1\end{bmatrix}\right \}\) and \(\mathcal {B}=\left \{\begin{bmatrix}1\\0\\0\end{bmatrix}, \begin{bmatrix}1\\1\\1\end{bmatrix}\right \}\)
Consider the diagram:
This gives us the matrix of \(T\) with respect to \(\mathcal {B}\) and \(\mathcal {C}\):
Let \(V\) and \(W\) be vector spaces with ordered bases \(\mathcal {B}=\{\vec {v}_1, \vec {v}_2\}\) and \(\mathcal {C}=\{\vec {w}_1, \vec {w}_2, \vec {w}_3\}\), respectively. Define a linear
transformation \(T:V\rightarrow W\) by
Find the matrix \(A\) of \(T\) with respect to \(\mathcal {B}\) and \(\mathcal {C}\), and use it to find \(T(-\vec {v}_1-3\vec {v}_2)\). Verify your answer by
computing \(T(-\vec {v}_1-3\vec {v}_2)\) directly.
Show that \(\begin{bmatrix}-1\\3\\2\end{bmatrix}, \begin{bmatrix}2\\4\\1\end{bmatrix}\) lie in \(W\) by expressing them as linear combinations of \(\vec {w}_1\) and \(\vec {w}_2\).