MATH SOLUTIONS TO PRACTICE PROBLEMS - MIDTERM I. 1. We carry out row reduction. We begin with the row operations

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MATH 2 - SOLUTIONS TO PRACTICE PROBLEMS - MIDTERM I. We carry out row reduction. We begin with the row operations yielding the matrix This is already upper triangular hence The lower triangular matrix equals R 2 R 2 2R, R 3 R 3 R 3. 2 U = 3. 2 L = 2. 2. For further reference, we begin by row-reducing the augumented matrix 2 3 4 b 2 3 5 7 b 2 2 3 4 b b 2 2b 2 2b 2 3b b 2 + 2b. 2 b 3 2 2 2 b + b 3 2b 2 + b 3 3b (i) The null space of A is also the null space of the row-reduced matrix rref(a) = 2. The first two variables x, y are pivots, the last two variables z, w are free. We obtain the system We conclude x + z + 2w = = x = z 2w y + z + w = = y = z w. x 2 y z = z + w w Therefore N(A) has the basis 2 N(A) = span, The nullity of A equals 2.

(ii) Each vector in the null space gives a relation between the columns of A. For instance, the vector and N(A) = c c 2 + c 3 = 2 N(A) = 2c c 2 + c 4 =. (iii) The last row of zeros in the row-reduced augumented matrix gives the equation 2b 2 + b 3 3b = that must be satisfied by all vectors b in the column space. b 2 b 3 (iv) The pivot columns, namely the first and second columns of A, give a basis for C(A): C(A) = span 2, 2 3. The rank of A equals 2. (v) The pivots are in the first and second row, so a basis for the row space of A is span, 2 (vi) The dimension of the left-null space of A is the number of rows minus the rank which is 3 2 =. (vii) We can easily find a particular solution x p =. The general solution is x = x p + x h hence 2 x = + z + w (viii) The rank of A equals 2 which not equal to the number of rows or columns of A. Hence A does not admit a left inverse nor a right inverse.

3. Assume first that the vectors {u, v w, u + v 2w} are linearly dependent. There exist constants a, b, c not all zero such that Rearranging, we obtain au + b(v w) + c(u + v 2w) =. (a + c)u + (b + c)v + (b 2c)w =. Since {u, v, w} is a basis, the vectors {u, v, w} must be independent. This implies that Solving for a, b, c we find a + c =, b + c =, b 2c =. a = b = c = which is impossible by assumption that not all (a, b, c) are zero. It follows that {u, v w, u + v 2w} are three linearly independent vectors in R 3 hence they must form a basis of R 3. 4. (i) Not a vector space. For instance (,,..., ) is in the set, but twice the vector 2(,,..., ) is not in the set. (ii) Vector space. This is the null space of the matrix [ ] 2 3 4. Null spaces are always vector spaces. (iii) Vector space. This is a bit harder to see. First, we determine the set a bit more explicitly. The square of the distance to (3, 4,, ) equals (x 3) 2 + (y + 4) 2 + z 2 + w 2 while the square distance to (, 3, 4, ) equals x 2 + (y + 3) 2 + (z 4) 2 + w 2. Since the two distances must be equal, we have (x 3) 2 + (y + 4) 2 + z 2 + w 2 = x 2 + (y + 3) 2 + (z 4) 2 + w 2. Expanding out and canceling, we obtain the linear equation 3x + y + 4z =. The requirement that the distances from (, 3, 4, ) and (, 4, 3, ) be equal can be worked out in a similar fashion. We obtain the equation 7y + z =.

Thus the set in question can be described by the two linear equations 3x + y + 4z =, 7y + z =. This is a null space of the matrix [ 3 ] 4 7 hence it is a subspace. (iv) Vector space. Indeed, if P and Q are two polynomials with P () = P () = P () =, Q() = Q () = Q () = then their sum P + Q also satisfies (P + Q)() = (P + Q) () = (P + Q) () =. Similarly, scalar multiplication is preserved since cp satisfies (v) Vector space. This is the set of matrices (cp )() = (cp ) () = (cp ) () =. A T = A. This is a subspace since if A is skew symmetric so is ca since (ca) T = ca T = ca. Similarly, if A, B are skew symmetric so is their sum A + B since (A + B) T = A T + B T = A B = (A + B). (vi) Not a vector space. If y is a solution of the equation, then y + 4y = sin t. But 2y is not a solution since (2y) + 4(2y) = 2 sin t. Since the equation changes, the solution set is not a vector space. 5. We calculate the null space of rref (A). This is the space spanned by. Elements in the null space of A give relations between the columns of A. Writing v, v 2, v 3, v 4 for the columns of A we must have 6. Note that 3 v 2 = v 4 v v 3 = 2. 2 = 2 2 + 2.

Therefore, 7. T 2 = 2T T 2 + T 2 = 2 (i) Clearly, {, x, x 2 } is a basis of P 2 hence dim P 2 = 3. [ [ 2 3 + ] 2] [ ] [ =. 2 2] To show that {, x, x 2 } is also a basis, it suffices to prove that the three vectors are linearly dependent. Assume otherwise, so that a + b(x ) + cx 2 = for some constants a, b, c. This rewrites as (a b) + bx + cx 2 = = a b =, b =, c = = a = b = c = proving the independence. (ii) We calculate T () =, T (x ) = (x ), T (x 2 ) = 2x + x 2 = x 2 + 2(x ) + 2. For the last equality, we needed to express T (x 2 ) = 2x + x 2 in terms of the basis elements, x, x 2. The matrix of T in this basis is given by collecting the coefficients of the basis elements, x, x 2, yielding the matrix 2 2. 8. True. To explain this fact, note that C has fewer rows than columns. Then C must have free variables. This in turn means that the null space N(C) contains a non-zero vector x: Cx =. We claim that x is also in the null space of A. Indeed, Ax = BCx = B =. This shows that N(A) contains a nonzero vector. 9. Consider Mat 2 the space of 2 2 matrices. This is a 4-dimensional vector space. The 5 matrices I, A, A 2, A 3, A 4 are vectors in Mat 2. Since 5 vectors in a 4-dimensional vector space must be linearly dependent, we can therefore find constants c, c, c 2, c 3, c 4 not all zero such that c I + c A + c 2 A 2 + c 3 A 3 + c 4 A 4 =.