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Commented solutions for selected problems of test 3 in linear algebra. It covers topics such as forming matrices, transition matrices, matrix representations of linear transformations, and finding the wronskian matrix. The document also includes a bonus section on consistent and inconsistent equations and the rank of compositions.
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1.a. Form the matrix S = (A|B|F ) whose columns are A, B and F. Since rref(S) = I 3 , β is linearly independent. And because |β| = 3, β also spans R^3 , i.e. β is a basis for R^3. (MATLAB: A=[1 1 1]’,B=[-1 1 1]’,F=[-1 1 -1]’,E=[1 1 -1]’,ABF=[A B F], rref(ABF)) b. Note that S = (^) ε[id]β is the transition matrix that transforms coordinates w.r.t. β into coord.’s w.r.t. the standard basis (e.g. [A]β = (1, 0 , 0)T^ , and S · (1, 0 , 0)T^ = A = [A]ε, i.e. S · [A]β = [A]ε). Hence [E]β = S−^1 E = (1, − 1 , 1)T^. (MATLAB: ABF\E. Geometrically note: A + F = B + E) c. Form the matrix Y whose columns are (the coord.’s w.r.t. the standard basis ε of) the images of the vectors in β under the map L, i.e., Y = (L(A)|L(B)|L(F )) = (B|E|E) [LONG SENTENCE!]. Note that this is the matrix representation for L w.r.t. the basis β for the input and w.r.t. the standard basis ε for the output, e.g. B = Y · (1, 0 , 0)T and [A]β = (1, 0 , 0)T^ , or [B]ε = (^) ε[L]β · [A]β. Hence ε[L]ε =^ ε[L]β ·^ β [id]ε =^ ε[L]β ·^ (ε[id]β )
− (^1) = Y S− (^1) , and
β [L]β =^ β [id]ε ·^ ε[L]β = (ε[id]β )−^1 ·^ ε[L]β =^ S−^1 Y. d. L(C) = [L(C)]ε = (^) ε[L]ε · [C]ε = (1, − 1 , −1)T^ = H.
ε[L]ε =^ Y^ ·^ S−^1 =
β [L]β =^ S−^1 ·^ Y^ =
(In MATLAB: eLb=[B,E,E], eLe=eLb/ABF, bLb=ABF\eLb, LC=eLe*C) Bonus: Because {A, D, F } are linearly dependent (compare a.) the given equations are overdeter- mined. These may be consistent or inconsistent. Geometrically, since F = −D, T (F ) must equal T (−D) = −T (D) = −E = C. Algebraically, with the usual abuse of notation, we want a matrix X such that X · (A|D|F ) = (A|E|F ), i.e. (A|D|F )T^ · XT^ = (A|E|F )T^. Thus (in)consistency and possible solutions can be read off of the rref(
( (A|D|F )T^ | (A|E|F )T^
) . If e.g. T (F ) = C was specified, we may pick any vector v that is linearly independent from {A, D}, and completely freely specify T (v) ∈ R^3. Then (^) ε[T ]γ = (A|E|T (v)) is the matrix representation for the desired map T w.r.t. the basis γ = {A, D, v} for the input and ε for the output.
4.a. The Wronskian matrix of the functions {e−^3 x, xe−^3 x, x^2 e−^3 x} evaluated at x = 0 is lower tri- angular with nonzero entries along the diagonal. Hence the Wronskian has full rank. Thus β is linearly independent. Since β spans by defn., it is a basis for V. b. [(2 − 5 x^2 )e−^3 x]β = (2, 0 , −5)T c. Suppose c ∈ R and y 1 , y 2 ∈ V. Then L(cy 1 + y 2 ) = (cy 1 + y 2 )′^ = cy 1 ′ + y′ 2 = cL(y 1 ) + L(y 2 ).
d. For vi ∈ β calculate the coordinates of L(vi) w.r.t. β. They are the columns of the desired matrix. e. Since (^) β [L]β has full rank, ker(L) = { 0 } and a basis is the empty set { }. f. Calculate (^) β [L]− β 1 [f (x)]β = (−^89 , 109 , 53 )T^. Hence
( −^89 + 109 x + 53 x^2
) e−^3 x^ is the desired antiderivative.
Bonus. Compare 4.d. This interesting pair of linear maps whose commutator (^) ε[X ◦ D − D ◦ X]ε = I 3 is the identity is useful e.g. as a mathematical model in quantum mechanics.
β [L]β =
ε[D^ ◦^ X]ε =
ε[X^ ◦^ D]ε =
.