7.1.a Suppose that f and g are in the set. Then f (0) = f (1) and g(0) = g(1), therefore f (0) + g(0) = f (1) + g(1), so f + g is also in the set. If c is an arbitrary scalar, then cf (0) = cf (1), hence cf is also in the set. The set is non-empty, since, for example, the constant zero function is in the set. Consequently, the set is a subspace 7.1.b No, since if we multiply an increasing function by −1, we get a decreasing function. 7.2. Reducing the matrix 1 −1 1 2 1 7 2 2 10 to the row echelon form, we get 1 −1 1 1 −1 1 1 0 3 5 → 0 3 5 → 0 0 4 8 0 1 3 0 −1 1 1 1 3 → 0 3 5 0 −1 1 1 3 , 0 −4 we see that the vectors are independent, hence the dimension is 3. (The row operations also show that the determinant of the matrix is non-zero.) 7.3. 1 2 2 3 1 4 2 1 2 2 3 1 4 2 1 2 3 2 3 5 1 4 → 6 → 0 0 1 −1 2 0 0 1 −1 2 −3 4 3 6 7 8 5 9 10 1 2 2 3 1 4 2 1 2 2 3 1 4 2 0 0 1 −1 2 1 4 → 0 0 1 −1 2 1 4 → 0 0 0 0 0 1 0 0 0 0 0 0 −4 0 1 2 0 5 −3 0 −6 1 2 2 3 1 0 2 0 0 1 −1 2 0 4 → 0 0 1 −1 2 0 4 . 0 0 0 0 0 1 0 0 0 0 0 0 1 0 We see that the first, third, and sixth columns form a basis, hence a basis of the columns space is 2 4 1 1 , 3 , 5 . 3 7 9 A basis of the row space is 1 2 0 5 −3 0 −6 , 0 0 1 1 −1 2 0 4 , 0 0 0 0 0 1 0 . The solution of the homogeneous system is 6 3 −5 −2 −2x2 − 5x4 + 3x5 + 6x7 0 0 0 1 x2 −4 −2 1 0 x4 − 2x5 − 4x7 = x2 0 +x4 1 +x5 0 +x7 0 , x4 0 1 0 0 x5 0 0 0 0 0 1 0 0 0 x7 therefore a basis of the nullspaces is −5 −2 1 0 0 1 0 , 1 0 0 0 0 0 0 , 3 0 −2 0 1 0 0 , 6 0 −4 0 0 0 1 7.4. a) For any two 4 × 4 matrices A, B, we have L(A + B) = (A + B) + 2(A + B)> = A + B + 2A> + 2B > = A + 2A> + B + 2B > = L(A) + L(B). For every scalar c we have L(cA) = (cA) + 2(cA)> = cA + c2A> = cL(A), hence L is a linear transformation (operator). b) L(cA) = (cA)2 = c2 A2 6= cA2 = cL(A), hence L is not a linear operator. 7.5. It is 1 2 0 1 1 1 . 2 2 2 It is just the coefficients in the formula. 7.6. Let us diagonalize the matrix. Its characteristic polynomial is 1−x 1 1 −1 −1 − x −1 = (1−x)(−1−x)(1−x)−1−1+1+x+1−x+1−x = 1 1 1−x x2 − x3 = x2 (1 − x), hence the eigenvalues are 0 (double) and 1. For λ = 0 the eigenvectors are found solving the system 1 1 1 −1 −1 −1 → 1 1 1 , 1 1 1 solution: −x2 − x3 −1 −1 = x2 1 + x3 0 , x2 x3 0 1 2 −1 −1 hence a basis of the eigenspace is 1 , 0 . 0 1 For λ = 1 we have 0 1 1 1 1 0 1 1 0 1 0 −1 −1 −2 −1 → 0 1 1 → → , 0 1 1 0 1 1 1 1 0 0 −1 −1 1 and an eigenvector is −1 . 1 −1 −1 1 0 0 0 0 −1 and D = 0 0 0 . We get A = SDS −1 for S = 1 0 1 1 0 0 1 Let us find S −1 : −1 1 0 −1 1 1 0 −1 0 1 1 0 1 1 0 1 0 1 −1 0 1 1 0 0 −1 −1 0 1 1 0 0 −1 −1 1 1 0 0 → 0 −1 0 1 1 1 0 1 1 0 0 1 1 −1 −1 0 0 −1 0 → 0 1 0 −1 0 1 0 0 1 1 0 1 0 0 0 1 1 0 −1 −1 0 → 0 1 0 1 1 1 1 0 0 1 0 1 0 1 2 1 so S −1 = −1 −1 0 . 1 1 1 It follows that −1 −1 1 0 −1 eA = SeD S −1 = 1 0 1 1 −1 −1 1 1 2 1 0 −1 −1 −1 0 1 1 e e e0 0 0 0 0 → 1 0 0 −1 0 → 1 1 1 −1 1 2 1 −1 0 , 1 1 1 2 1 0 0 −1 −1 0 = 1 1 1 e1 1 e e−1 e−1 0 = 1 − e 2 − e 1 − e . e e−1 e−1 e 0 0 7.7. The eigenvalues of A are 0, 1, hence A = S S −1 for some S. 0 1 Then √ √ √ 0 √0 0 0 −1 −1 A = S DS = S S =S S −1 = A. 0 1 0 1 3 0 e0 0