[v]B means "the list of numbers you multiply the basis vectors of B by to build v."
If B={b1,b2} and v=3b1−2b2, then [v]B=(−23).
[T]CB means "the table that converts B-coordinates of an input into C-coordinates
of the output." Read it right-to-left: bottom label B is what goes in, top label C
is what comes out.
e1,e2,… are the standard basis arrows: e1=(1,0,…), e2=(0,1,0,…), and so on.
WHAT we do: hit each standard basis arrow with T, read off coordinates.
T(e1)=2(1,0)=(2,0) → first column (02).
T(e2)=2(0,1)=(0,2) → second column (20).
WHY: each column catches where a basis vector goes (the mnemonic "Columns Catch
Outputs in C"). Here C is the standard basis, so the output already is its coordinates.
[T]=(2002).
Recall Solution 1.2
Size: 3×3 (three-dimensional in, three-dimensional out).
T(e1)=(1,0,0) → column (1,0,0)⊤.
T(e2)=(0,1,0) → column (0,1,0)⊤.
T(e3)=(0,0,0) → column (0,0,0)⊤. Why zero? the z-axis is flattened away.
[T]=100010000.
The all-zero third column is the fingerprint of a degenerate direction — see
Kernel and image: that column being zero means e3 lives in the kernel.
Recall Solution 1.3
Read the columns back out — they tell you where the basis arrows land.
Column 1 = (10): so T(e1)=(0,1). The arrow pointing right now points up.
Column 2 = (01): so T(e2)=(1,0). The arrow pointing up now points right.
Right ↔ up swap means every point (x,y) goes to (y,x): this is the ==reflection across
the line y=x==. ✓
A 180° turn sends every arrow to its exact opposite: (x,y)↦(−x,−y).
T(e1)=(−1,0) → column (−1,0)⊤.
T(e2)=(0,−1) → column (0,−1)⊤.
[T]=(−100−1).Verify:[T](−34)=(3−4), and indeed (4,−3) flipped through the origin
is (−4,3). ✓
Recall Solution 2.2
Now the output basis is the full {1,x,x2}, so every column has three entries.
T(1)=0 → (0,0,0)⊤.
T(x)=1=1⋅1 → (1,0,0)⊤.
T(x2)=2x=2⋅x → (0,2,0)⊤.
[T]=000100020.Apply:[p]B=(7,2,5)⊤, so [T][p]B=(2,10,0)⊤, meaning 2+10x. And
p′=2+10x. ✓ Note the bottom row is all zeros: the derivative can never produce an x2
term, so it can't hit that basis direction — a preview of Rank and nullity.
Recall Solution 2.3
Size forecast: 3×2 (three out, two in).
T(e1)=T(1,0)=(1,1,0) → column (1,1,0)⊤.
T(e2)=T(0,1)=(−1,1,2) → column (−1,1,2)⊤.
[T]=110−112.Test:[T](13)=(3−1,3+1,0+2)⊤=(2,4,2)⊤, and
T(3,1)=(3−1,3+1,2)=(2,4,2). ✓
WHAT: apply T to each new basis arrow, then express the answer back in B′.
First, in standard coordinates the map is T(x,y)=(x+2y,y).
T(1,0)=(1,0). Write (1,0)=a(1,0)+b(1,1): from the second slot b=0, then a=1.
→ column (1,0)⊤.
T(1,1)=(1+2,1)=(3,1). Write (3,1)=a(1,0)+b(1,1): second slot gives b=1, then
a+1=3⇒a=2. → column (2,1)⊤.
[T]B′=(1021).Surprise: it's the same matrix! WHY:b1′=(1,0)=e1 lies along the shear's
fixed direction, and the shear moves b2′ by exactly one copy of b1′ — the geometry
the new basis measures happens to match the old. This is the Change of basis formula
P−1AP landing on the same matrix because P commutes with this particular A.
Recall Solution 3.2
T(e2)=3e2. In B′={e2,e1} this is 3⋅(first B′ vector) →
column (3,0)⊤.
T(e1)=2e1. In B′ this is 2⋅(second B′ vector) →
column (0,2)⊤.
[T]B′=(3002).
Reordering the basis just swaps the diagonal entries. This is exactly what
Eigenvalues and diagonalization uses: when the basis is made of eigenvectors, the
matrix is diagonal and the entries are the stretch factors (eigenvalues).
Recall Solution 3.3
Matrices.[S]=(01−10), [T]=(100−1).
Way 1 — multiply (composition rule [T∘S]=[T][S]):
=\begin{pmatrix}0&-1\\-1&0\end{pmatrix}.$$
**Way 2 — track basis vectors** (apply $S$ then $T$):
- $e_1=(1,0)\xrightarrow{S}(0,1)\xrightarrow{T}(0,-1)$ → column $(0,-1)^\top$.
- $e_2=(0,1)\xrightarrow{S}(-1,0)\xrightarrow{T}(-1,0)$ → column $(-1,0)^\top$.
$$[T\circ S]=\begin{pmatrix}0&-1\\-1&0\end{pmatrix}. \checkmark$$
Both agree — this is [[Composition of linear maps]]: matrix multiplication is *defined* to
make these two routes match.
Apply the derivative, then express each answer in C by solving.
T(1)=0=0⋅1+0⋅(1+x) → column (0,0)⊤.
T(1+x)=1. Write 1=a⋅1+b⋅(1+x): match x-term b=0, then constant a=1.
→ column (1,0)⊤.
T(1+x+x2)=1+2x. Write 1+2x=a⋅1+b(1+x): match x-term b=2, then constant
a+b=1⇒a=−1. → column (−1,2)⊤.
[T]CB=(0010−12).Sanity test. Take p=1+x+x2; its B-coords are (0,0,1)⊤ (it's the third basis
vector). Then [T]CB(0,0,1)⊤=(−1,2)⊤, meaning −1⋅1+2⋅(1+x)=1+2x. And
directly p′=(1+x+x2)′=1+2x. ✓
Recall Solution 4.2
The given vectors {(1,2),(0,1)} form a basis, so this data determines T. But we want
the matrix in the standard basis, so we need T(e1) and T(e2).
e2=(0,1) is already given: T(e2)=(1,1).
e1=(1,0): write e1=1⋅(1,2)−2⋅(0,1). By linearity
T(e1)=1⋅T(1,2)−2⋅T(0,1)=(3,0)−2(1,1)=(1,−2).
[T]=(1−211).Check both conditions:[T](21)=(−2+21+2)=(03) ✓ and
[T](10)=(11) ✓.
The plane's unit normal is n=31(1,1,1). Projection onto the plane removes
the component along n:
T(v)=v−(v⋅n)n=v−3(v⋅(1,1,1))(1,1,1).Why subtract the normal part? whatever sticks out of the plane along n is exactly the
shadow being removed; the rest lies flat in the plane.
T(e1)=(1,0,0)−31(1,1,1)=(32,−31,−31).
T(e2)=(0,1,0)−31(1,1,1)=(−31,32,−31).
T(e3)=(0,0,1)−31(1,1,1)=(−31,−31,32).
[T]=312−1−1−12−1−1−12.(b) The image is the whole plane (2-dimensional) so rank =2. Everything along the
normal (1,1,1) collapses to 0, so the kernel is the line spanned by (1,1,1),
nullity =1. Check: [T](1,1,1)⊤=31(0,0,0)⊤=0 ✓, and rank + nullity
=2+1=3=dimR3, the Rank and nullity theorem. See Kernel and image.
Recall Solution 5.2
(a) Apply T to each basis vector.
T(1)=1+0=1 → column (1,0,0)⊤.
T(x)=x+1=1+x → column (1,1,0)⊤.
T(x2)=x2+2x → column (0,2,1)⊤.
[T]=100110021.(b) It's upper-triangular with all diagonal entries 1, so det=1=0: invertible.
Invert (back-substitute the triangular system):
[T]−1=100−1102−21.Check:[T][T]−1=I. As a map, T−1(p)=p−p′+p′′ (a finite version of
∑(−1)kp(k), which terminates because third and higher derivatives vanish on
P2). Quick test: T−1(x2) has coords [T]−1(0,0,1)⊤=(2,−2,1)⊤, i.e.
2−2x+x2; apply T: (2−2x+x2)+(−2+2x)=x2 ✓.
Recall Self-check: the one-line recipe behind every problem
To build [T]CB ::: apply T to each vector of B, write each output in the basis C, and make those coordinate lists the columns.
Matrix size for T:V→W ::: dimW rows by dimV columns.
When is [T] not invertible ::: exactly when T has a nonzero kernel (some direction maps to 0), equivalently det=0.