answer
To show that A" role="presentation">A and Q" role="presentation">Q have the same column space, we'll use the given hints:
### Step 1: Show that Col A⊆Col Q" role="presentation">Col A⊆Col Q
Given y∈Col A" role="presentation">y∈Col A, we can write y=Ax" role="presentation">y=Ax for some vector x" role="presentation">x.
Since A=QR" role="presentation">A=QR and R" role="presentation">R is invertible, we have:
y=Ax=QRx" role="presentation">y=Ax=QRx
Let x′=Rx" role="presentation">x′=Rx. Since R" role="presentation">R is invertible, x′" role="presentation">x′ can be any vector in Rn" role="presentation">Rn. Thus:
y=Qx′" role="presentation">y=Qx′
This shows that y" role="presentation">y is also in the column space of Q" role="presentation">Q, i.e., Col A⊆Col Q" role="presentation">Col A⊆Col Q.
### Step 2: Show that Col Q⊆Col A" role="presentation">Col Q⊆Col A
Given y∈Col Q" role="presentation">y∈Col Q, we can write y=Qx" role="presentation">y=Qx for some vector x" role="presentation">x.
Since A=QR" role="presentation">A=QR and R" role="presentation">R is invertible, we can multiply both sides by R−1" role="presentation">R−1:
\[ Q = AR^{-1} \]
Thus:
y=Qx=AR−1x" role="presentation">y=Qx=AR−1x
Let x′=R−1x" role="presentation">x′=R−1x. Since R" role="presentation">R is invertible, x′" role="presentation">x′ can be any vector in Rn" role="presentation">Rn. Thus:
y=Ax′" role="presentation">y=Ax′
This shows that y" role="presentation">y is also in the column space of A" role="presentation">A, i.e., Col Q⊆Col A" role="presentation">Col Q⊆Col A.
### Conclusion
Since we've shown that Col A⊆Col Q" role="presentation">Col A⊆Col Q and Col Q⊆Col A" role="presentation">Col Q⊆Col A, we conclude that Col A=Col Q" role="presentation">Col A=Col Q.
Therefore, A" role="presentation">A and Q" role="presentation">Q have the same column space.
details
To understand why x′" role="presentation">x′ can be any vector in Rn" role="presentation">Rn, let's break it down step by step.
### Understanding the Concept
Given that R" role="presentation">R is an invertible matrix:
1. **Invertibility of R" role="presentation">R**: Since R" role="presentation">R is invertible, there exists a matrix R−1" role="presentation">R−1 such that:
RR−1=I" role="presentation">RR−1=I
where
I" role="presentation">I is the identity matrix.
2. **Transformation by R" role="presentation">R**: Any vector x∈Rn" role="presentation">x∈Rn can be transformed by multiplying it by R" role="presentation">R, resulting in a new vector x′" role="presentation">x′. We write:
x′=Rx" role="presentation">x′=Rx
3. **Invertible Transformation**: Because R" role="presentation">R is invertible, we can always find x" role="presentation">x given x′" role="presentation">x′ by multiplying x′" role="presentation">x′ by R−1" role="presentation">R−1:
x=R−1x′" role="presentation">x=R−1x′
### Why x′" role="presentation">x′ Can Be Any Vector in Rn" role="presentation">Rn
Let's see why x′" role="presentation">x′ can be any vector in Rn" role="presentation">Rn:
1. **Surjectivity**: The function f:Rn→Rn" role="presentation">f:Rn→Rn defined by f(x)=Rx" role="presentation">f(x)=Rx is surjective because for any vector x′" role="presentation">x′ in the output space (the codomain), there exists an x" role="presentation">x in the input space (the domain) such that Rx=x′" role="presentation">Rx=x′. This is because R" role="presentation">R has full rank (since it's invertible).
2. **Vector Space Mapping**: Since R" role="presentation">R maps Rn" role="presentation">Rn to itself in a bijective manner (one-to-one and onto), for every vector x′∈Rn" role="presentation">x′∈Rn, there exists a vector x∈Rn" role="presentation">x∈Rn such that x′=Rx" role="presentation">x′=Rx.
3. **Existence of x" role="presentation">x**: Given any vector x′∈Rn" role="presentation">x′∈Rn, we can always find a corresponding vector x" role="presentation">x using x=R−1x′" role="presentation">x=R−1x′. Therefore, x′" role="presentation">x′ can be any vector in Rn" role="presentation">Rn.
### Example
Let's consider a concrete example with R" role="presentation">R:
1. Suppose R" role="presentation">R is a 2x2 invertible matrix:
R=(2113)" role="presentation">R=(2113)
2. We can find R−1" role="presentation">R−1:
R−1=15(3−1−12)" role="presentation">R−1=15(3−1−12)
3. Now, given any vector x′∈R2" role="presentation">x′∈R2, say x′=(45)" role="presentation">x′=(45):
x=R−1x′=15(3−1−12)(45)=15(3⋅4+(−1)⋅5(−1)⋅4+2⋅5)=15(12−5−4+10)=(1.41.2)" role="presentation">x=R−1x′=15(3−1−12)(45)=15(3⋅4+(−1)⋅5(−1)⋅4+2⋅5)=15(12−5−4+10)=(1.41.2)
This shows that for any x′" role="presentation">x′, we can find an x" role="presentation">x such that x′=Rx" role="presentation">x′=Rx, thus demonstrating that x′" role="presentation">x′ can indeed be any vector in Rn" role="presentation">Rn.
By understanding this property of invertible matrices, we can see why x′" role="presentation">x′ can be any vector in Rn" role="presentation">Rn.