FinalKey
- Page ID
- 218480
\( \newcommand{\vecs}[1]{\overset { \scriptstyle \rightharpoonup} {\mathbf{#1}} } \)
\( \newcommand{\vecd}[1]{\overset{-\!-\!\rightharpoonup}{\vphantom{a}\smash {#1}}} \)
\( \newcommand{\dsum}{\displaystyle\sum\limits} \)
\( \newcommand{\dint}{\displaystyle\int\limits} \)
\( \newcommand{\dlim}{\displaystyle\lim\limits} \)
\( \newcommand{\id}{\mathrm{id}}\) \( \newcommand{\Span}{\mathrm{span}}\)
( \newcommand{\kernel}{\mathrm{null}\,}\) \( \newcommand{\range}{\mathrm{range}\,}\)
\( \newcommand{\RealPart}{\mathrm{Re}}\) \( \newcommand{\ImaginaryPart}{\mathrm{Im}}\)
\( \newcommand{\Argument}{\mathrm{Arg}}\) \( \newcommand{\norm}[1]{\| #1 \|}\)
\( \newcommand{\inner}[2]{\langle #1, #2 \rangle}\)
\( \newcommand{\Span}{\mathrm{span}}\)
\( \newcommand{\id}{\mathrm{id}}\)
\( \newcommand{\Span}{\mathrm{span}}\)
\( \newcommand{\kernel}{\mathrm{null}\,}\)
\( \newcommand{\range}{\mathrm{range}\,}\)
\( \newcommand{\RealPart}{\mathrm{Re}}\)
\( \newcommand{\ImaginaryPart}{\mathrm{Im}}\)
\( \newcommand{\Argument}{\mathrm{Arg}}\)
\( \newcommand{\norm}[1]{\| #1 \|}\)
\( \newcommand{\inner}[2]{\langle #1, #2 \rangle}\)
\( \newcommand{\Span}{\mathrm{span}}\) \( \newcommand{\AA}{\unicode[.8,0]{x212B}}\)
\( \newcommand{\vectorA}[1]{\vec{#1}} % arrow\)
\( \newcommand{\vectorAt}[1]{\vec{\text{#1}}} % arrow\)
\( \newcommand{\vectorB}[1]{\overset { \scriptstyle \rightharpoonup} {\mathbf{#1}} } \)
\( \newcommand{\vectorC}[1]{\textbf{#1}} \)
\( \newcommand{\vectorD}[1]{\overrightarrow{#1}} \)
\( \newcommand{\vectorDt}[1]{\overrightarrow{\text{#1}}} \)
\( \newcommand{\vectE}[1]{\overset{-\!-\!\rightharpoonup}{\vphantom{a}\smash{\mathbf {#1}}}} \)
\( \newcommand{\vecs}[1]{\overset { \scriptstyle \rightharpoonup} {\mathbf{#1}} } \)
\(\newcommand{\longvect}{\overrightarrow}\)
\( \newcommand{\vecd}[1]{\overset{-\!-\!\rightharpoonup}{\vphantom{a}\smash {#1}}} \)
\(\newcommand{\avec}{\mathbf a}\) \(\newcommand{\bvec}{\mathbf b}\) \(\newcommand{\cvec}{\mathbf c}\) \(\newcommand{\dvec}{\mathbf d}\) \(\newcommand{\dtil}{\widetilde{\mathbf d}}\) \(\newcommand{\evec}{\mathbf e}\) \(\newcommand{\fvec}{\mathbf f}\) \(\newcommand{\nvec}{\mathbf n}\) \(\newcommand{\pvec}{\mathbf p}\) \(\newcommand{\qvec}{\mathbf q}\) \(\newcommand{\svec}{\mathbf s}\) \(\newcommand{\tvec}{\mathbf t}\) \(\newcommand{\uvec}{\mathbf u}\) \(\newcommand{\vvec}{\mathbf v}\) \(\newcommand{\wvec}{\mathbf w}\) \(\newcommand{\xvec}{\mathbf x}\) \(\newcommand{\yvec}{\mathbf y}\) \(\newcommand{\zvec}{\mathbf z}\) \(\newcommand{\rvec}{\mathbf r}\) \(\newcommand{\mvec}{\mathbf m}\) \(\newcommand{\zerovec}{\mathbf 0}\) \(\newcommand{\onevec}{\mathbf 1}\) \(\newcommand{\real}{\mathbb R}\) \(\newcommand{\twovec}[2]{\left[\begin{array}{r}#1 \\ #2 \end{array}\right]}\) \(\newcommand{\ctwovec}[2]{\left[\begin{array}{c}#1 \\ #2 \end{array}\right]}\) \(\newcommand{\threevec}[3]{\left[\begin{array}{r}#1 \\ #2 \\ #3 \end{array}\right]}\) \(\newcommand{\cthreevec}[3]{\left[\begin{array}{c}#1 \\ #2 \\ #3 \end{array}\right]}\) \(\newcommand{\fourvec}[4]{\left[\begin{array}{r}#1 \\ #2 \\ #3 \\ #4 \end{array}\right]}\) \(\newcommand{\cfourvec}[4]{\left[\begin{array}{c}#1 \\ #2 \\ #3 \\ #4 \end{array}\right]}\) \(\newcommand{\fivevec}[5]{\left[\begin{array}{r}#1 \\ #2 \\ #3 \\ #4 \\ #5 \\ \end{array}\right]}\) \(\newcommand{\cfivevec}[5]{\left[\begin{array}{c}#1 \\ #2 \\ #3 \\ #4 \\ #5 \\ \end{array}\right]}\) \(\newcommand{\mattwo}[4]{\left[\begin{array}{rr}#1 \amp #2 \\ #3 \amp #4 \\ \end{array}\right]}\) \(\newcommand{\laspan}[1]{\text{Span}\{#1\}}\) \(\newcommand{\bcal}{\cal B}\) \(\newcommand{\ccal}{\cal C}\) \(\newcommand{\scal}{\cal S}\) \(\newcommand{\wcal}{\cal W}\) \(\newcommand{\ecal}{\cal E}\) \(\newcommand{\coords}[2]{\left\{#1\right\}_{#2}}\) \(\newcommand{\gray}[1]{\color{gray}{#1}}\) \(\newcommand{\lgray}[1]{\color{lightgray}{#1}}\) \(\newcommand{\rank}{\operatorname{rank}}\) \(\newcommand{\row}{\text{Row}}\) \(\newcommand{\col}{\text{Col}}\) \(\renewcommand{\row}{\text{Row}}\) \(\newcommand{\nul}{\text{Nul}}\) \(\newcommand{\var}{\text{Var}}\) \(\newcommand{\corr}{\text{corr}}\) \(\newcommand{\len}[1]{\left|#1\right|}\) \(\newcommand{\bbar}{\overline{\bvec}}\) \(\newcommand{\bhat}{\widehat{\bvec}}\) \(\newcommand{\bperp}{\bvec^\perp}\) \(\newcommand{\xhat}{\widehat{\xvec}}\) \(\newcommand{\vhat}{\widehat{\vvec}}\) \(\newcommand{\uhat}{\widehat{\uvec}}\) \(\newcommand{\what}{\widehat{\wvec}}\) \(\newcommand{\Sighat}{\widehat{\Sigma}}\) \(\newcommand{\lt}{<}\) \(\newcommand{\gt}{>}\) \(\newcommand{\amp}{&}\) \(\definecolor{fillinmathshade}{gray}{0.9}\)|
Math 203 Practice Final Exam Printable Key
Please work out all of the following problems. Credit will be given based on the progress that you make towards the final solution. Show your work. No calculators allowed for this page.
Let \( A = \begin{pmatrix} 2 & 1 \\ 1 & 2 \end{pmatrix} \) Find an orthogonal matrix P and a diagonal matrix D with A = PDP-1. Solution We find \( | \lambda I - A| = \begin{vmatrix} \lambda I - 2 & -1 \\ -1 & \lambda I - 2 \end{vmatrix} \) \( (\lambda - 2) (\lambda - 2) = \lambda ^2 - 4 \lambda + 3 = (\lambda - 1) (\lambda - 3) \) Hence the eigenvalues are 1 and 3. Now we find the eigenvectors by finding the null space of \( A - 1I \) . We have \( | 1I - A| = \begin{vmatrix} \lambda -1 & -1 \\ -1 & -1 \end{vmatrix} \)
since the determinant is zero, we can use the first row which corresponds with the equation -x - y = 0. Which has eigenvector (1,-1) Normalizing gives \( ( \frac{1}{\sqrt{2}} , - \frac{1}{\sqrt{2}} ) \) For the eigenvector corresponding with the eigenvalue of 3, we have \( | 3I - A| = \begin{vmatrix} \lambda 1 & -1 \\ -1 & 1 \end{vmatrix} \) again, since the determinant is zero, we can use the first row which corresponds with the equation x - y = 0. Which has eigenvector (1,1) Normalizing gives \( ( \frac{1}{\sqrt{2}} , \frac{1}{\sqrt{2}} ) \) Putting this all together, gives \( D = \begin{pmatrix} \lambda 1 & 0 \\ 0 & 3 \end{pmatrix} \) \( P = \begin{pmatrix} \lambda \frac{1}{\sqrt{2}} & \frac{1}{\sqrt{2}} \\ - \frac{1}{\sqrt{2}} & \frac{1}{\sqrt{2}} \end{pmatrix} \)
Use the permutation definition of the determinant to find the determinant of
\( \begin{pmatrix} 4 & 2 & 3 \\ 0 & 0 & -2 \\ 1 & 6 & 5 \end{pmatrix} \) Solution The permutations on three elements and their corresponding products are even odd odd even even odd
(4)(0)(5) - (4)(-2)(6) - (2)(0)(5) + (2)(-2)(1) + (3)(0)(6) - (3)(0)(1)
= 48 - 4 = 44
Find the inverse of A if \( A = \begin{pmatrix} 1 & 1 & 0 \\ -1 & 0 & 1 \\ 3 & -1 & 5 \end{pmatrix} \)Solution We augment this matrix with the identity matrix and rref it. \( \left( \begin{array}{ccc|ccc} 1 & 1 & 0 & 1 & 0 & 0 \\ -1 & 0 & 1 & 0 & 1 & 0\\ 3 & -1 & 5 & 0 & 0 & 1 \end{array} \right) \begin{array}{ccc|lcr} R_2 & \rightarrow & R_2 + R_1 \\ \rightarrow & \rightarrow & \rightarrow \\ R_3 & \rightarrow & R_3 + -3 R_1 \end{array} \left( \begin{array}{ccc|ccc} 1 & 1 & 0 & 0 & 0 & 0 \\ 0 & 1 & 1 & 1 & 1 & 0\\ 0 & 0 & -1 & -3 & 0 & 1 \end{array} \right)\) \(\begin{array}{ccc|lcr} R_1 & \rightarrow & R_1 + (-1)R_2 \\ \rightarrow & \rightarrow & \rightarrow \end{array} \left( \begin{array}{ccc|ccc} 1 & 0 & -1 & 0 & -1 & 0 \\ 0 & 1 & 1 & 1 & 1 & 0\\ 0 & 0 & -1 & -3 & 0 & 1 \end{array} \right) \begin{array}{ccc|lcr} R_3 & \rightarrow & (-1)R_3 \\ \rightarrow & \rightarrow & \rightarrow \end{array} \left( \begin{array}{ccc|ccc} 1 & 0 & -1 & 0 & -1 & 0 \\ 0 & 1 & 1 & 1 & 1 & 0\\ 0 & 0 & 1 & 3 & 0 & -1 \end{array} \right)\)
\( \begin{array}{ccc|lcr} R_1 & \rightarrow & R_1 + R_3 \\ \rightarrow & \rightarrow & \rightarrow \\ R_2 & \rightarrow & R_2 + (-1)R_3 \end{array} \left( \begin{array}{ccc|ccc} 1 & 0 & 0 & 3 & -1 & -1 \\ 0 & 1 & 0 & -2 & 1 & 1\\ 0 & 0 & 1 & 3 & 0 & -1 \end{array} \right)\) We conclude that \( A^{-1} = \begin{pmatrix} 3 & -1 & -1 \\ -2 & 1 & 1 \\ 3 & 0 & 01 \end{pmatrix} \)
Calculators are permitted on this part
Problem 4 Consider the matrix
\( A = \begin{pmatrix} 5 & 10 & 0 & 3 \\ 3 & 6 & 1 & 1 \\ 2 & 4 & 0 & 1 \\ 1 & 2 & 0 & -1 \end{pmatrix} \)
A. Determine the rank of A. Solution We find
\( rref(A) \begin{pmatrix} 1 & 2 & 0 & 0 \\0 & 0 & 1 & 0 \\ 0 & 0 & 0 & 1 \\ 0 & 0 & 0 & 0 \end{pmatrix} \) Since there are three pivots, the rank is 3.
B. Find a basis for the null space of A. Solution The equation form of rref(A) is
x1 = -2x2 Since the rank of A is 3 and n = 4, the nullity is 1. A basis for the null space is {(-2, 1,0,0)} C. Find a basis for the column space of A using columns of A. Solution We see that the corners are in columns 1, 3, and 4. Hence the first, second, and third columns of A are a basis for the column space of A. {(5,3,2,1), (0,1,0,0), (3,1,1,-1)}
Problem 5 Let \( L: P_2 \rightarrow R^2 \) be defined by \( L(f(t)) = ( f'(1), \int_0^1 f(x) dx \)
A. Prove that L is a linear transformation. Solution
Let f(t) = a1 + b1t + c1t2 and g(t) = a2 + b2t + c2t2 Then 1. L(f(t) + g(t)) = (b1 + 2c1 + b2 + 2c2, a1 + 1/2 b1 + 1/3 c1 + a2 + 1/2 b2 + 1/3 c2) and L(f(t)) + L(g(t)) = (b1 + 2c1, a1 + 1/2 b1 + 1/3 c1) + (b2 + 2c2, a2 + 1/2 b2 + 1/3 c2) = (b1 + 2c1 + b2 + 2c2, a1 + 1/2 b1 + 1/3 c1 + a2 + 1/2 b2 + 1/3 c2) 2. L(cf(t)) = (cb1 + 2cc1, ca1 + 1/2 cb1 + 1/3 cc1) = c(b1 + 2c1, a1 + 1/2 b1 + 1/3 c1) = cL(f(t)) hence L is a linear transformation B. Let S = {x2 + x, x2 + 1, x} and T = {(1,1), (1,2)} be bases for P2 and R2. Find the matrix for L with the bases S and T. Solution \( P_{E \leftarrow S} \begin{pmatrix} 0 & 1 & 0 \\ 1 & 0 & 1 \\ 1 & 1 & 0 \end{pmatrix} \) \( P_{E \leftarrow T} \begin{pmatrix} 1 & 1 \\ 1 & 2 \end{pmatrix} \) and L(1,0,0) = L(1) = (0,1) L(0,1,0) = L(t) = (1,1/2) L(0,0,1) = L(t2) = (2,1/3) Hence \( A_L = \begin{pmatrix} 0 & 1 & 2 \\ 1 & \frac{1}{2} & \frac{1}{3} \end{pmatrix} \) Now consider the diagram \(S \begin{array}{lr} \longrightarrow \\ P_{ E \leftarrow S} \end{array} E_{P_2} \begin{array}{lr} \longrightarrow \\ A_L \end{array} E_{R^2} \begin{array}{lr} \longrightarrow \\ P^{-1}_{E \leftarrow T} \end{array} T \) We the matrix we want is \( P_{ E \leftarrow S}A_L P^{-1}_{E \leftarrow T} = \begin{pmatrix} 1 & 1 \\ 1 & 2 \end{pmatrix} \begin{pmatrix} 0 & 1 & 2 \\ 1 & \frac{1}{2} & \frac{1}{3} \end{pmatrix} \begin{pmatrix} 0 & 1 & 0 \\ 1 & 0 & 1 \\ 1 & 1 & 0 \end{pmatrix}^{-1} = \begin{pmatrix} 0 & 1 & 2 \\ 1 & \frac{1}{2} & \frac{1}{3} \end{pmatrix} \begin{pmatrix} \frac{17}{6} & \frac{7}{3} & - \frac{4}{3} \\ \frac{8}{3} & \frac{8}{3} & - \frac{2}{3} \end{pmatrix} \)
Show that the set \( S = \{ \begin{pmatrix} 1 & 2 \\ 0 & 0 \end{pmatrix} \) , \( \begin{pmatrix} 0 & 0 \\ 2 & 1 \end{pmatrix} \) , \( \begin{pmatrix} 0 & 2 \\ 0 & 1 \end{pmatrix} \) , \( \begin{pmatrix} 2 & 0 \\ 1 & 0 \end{pmatrix} \) , is a basis for M2x 2.
Solution Since there are four vectors in a four dimensional space, we only need to show that the vectors are linearly independent. We let
\( c_1 \begin{pmatrix} 1 & 2 \\ 0 & 0 \end{pmatrix} + c_2 \begin{pmatrix} 0 & 0 \\ 2 & 1 \end{pmatrix} + c_3 \begin{pmatrix} 0 & 2 \\ 0 & 1 \end{pmatrix} + c_4 \begin{pmatrix} 2 & 0 \\ 1 & 0 \end{pmatrix} = \begin{pmatrix} 0 & 0 \\ 0 & 0 \end{pmatrix} \)
This gives us the four equations c1 + 2c4 = 0 Putting this into the matrix form Ac = 0 gives \( \begin{pmatrix} 1 & 0 & 0 & 2 \\ 2 & 0 & 2 & 0 \\ 0 & 2 & 0 & 1 \\ 0 & 1 & 1 & 0 \end{pmatrix} \begin{pmatrix} c_1 \\ c_2 \\ c_3 \\ c_4 \end{pmatrix} = \begin{pmatrix} 0 \\ 0 \\ 0 \\ 0 \end{pmatrix} \) We calculate |A| = -6 Since the determinant is nonzero, the above equation has only the trivial solution. Hence the four vectors are linearly independent. We can conclude that they form a basis for M2x2. Problem 7 Use matrices to find the unknown currents in the given circuit.
Solution First we find the loop equations. a --> b --> d --> a : -I1 - 60 - 2I2 + 10 = 0 b --> c --> d --> b : -4I3 - 50 + 2I2 + 60 = 0
The node equations are
b: I1 - I2 - I3 = 0 d: -I1 + I2 + I3 = 0 Notice that the second node equation is redundant, so we can discard this one. The three equations together give
-I1 - 2I2 = 50 2I2 - 4I3 = -10 I1 - I2 - I3 = 0
The corresponding matrix equation AI = b is \( \begin{pmatrix} -1 & 2 & 0 \\ 0 & 2 & -4 \\ 1 & -1 & -1 \end{pmatrix} \begin{pmatrix} I_1 \\ I_2 \\ I_3 \end{pmatrix} = \begin{pmatrix} 50 \\ -10 \\ 0 \end{pmatrix} \) Hence, the solution is I = A-1b. We have \( A^{-1}b \begin{pmatrix} -\frac{3}{7} & -\frac{1}{7} & \frac{4}{7} \\ -\frac{2}{7} & \frac{1}{7} & -\frac{2}{7} \\ -\frac{1}{7} & -\frac{3}{7} & -\frac{1}{7} \end{pmatrix} \begin{pmatrix} 50 \\ -10 \\ 0 \end{pmatrix} = \begin{pmatrix} -20 \\ -15 \\ -5 \end{pmatrix} \) so that I1 = -20 I2 = -15 I3 = -5 Notice that the minus signs means that the currents are traveling in the opposite direction as the arrows indicate.
Problem 8 Graph the equation and write the equation in standard form.
4x2 + 2xy + 4y2 = 15
Solution
We first write this as a matrix equation xTAx = 15. \( \begin{pmatrix} x & y \end{pmatrix} \begin{pmatrix} 4 & 1 \\ 1 & 4 \end{pmatrix} \begin{pmatrix} x \\ y \end{pmatrix} = 15 \)
Next we find the eigenvalues of this matrix. They are 3 and 5. We used a calculator for this, but we could have done this by hand. We have \( 3I - A = \begin{pmatrix} -1 & -1 \\ -1 & -1 \end{pmatrix} \) \( 5I - A = \begin{pmatrix} 1 & -1 \\ -1 & 1 \end{pmatrix} \) \) The eigenvectors are \( v_3 = \begin{pmatrix} \frac{1}{\sqrt{2}} & -\frac{1}{\sqrt{2}} \end{pmatrix} \) \( v_5 = \begin{pmatrix} \frac{1}{\sqrt{2}} & \frac{1}{\sqrt{2}} \end{pmatrix} \) The equation can be written in the form xTPDPTx = 15 \( \begin{pmatrix} x & y \end{pmatrix} \begin{pmatrix} \frac{1}{\sqrt{2}} & \frac{1}{\sqrt{2}} \\ -\frac{1}{\sqrt{2}} & \frac{1}{\sqrt{2}} \end{pmatrix} \begin{pmatrix} 3 & 0 \\ 0 & 5 \end{pmatrix} \begin{pmatrix} \frac{1}{\sqrt{2}} & \frac{1}{\sqrt{2}} \\ -\frac{1}{\sqrt{2}} & \frac{1}{\sqrt{2}} \end{pmatrix}^T \begin{pmatrix} x \\ y \end{pmatrix} = 15\) Let x' = PTx Then the equation of the conic becomes x'TDx' = 15 or 3x'2 + 5y'2 = 15 or x'2 y'2 We see that the graph is rotated from the (x,y) plane by an angle of arctan(-1) = -p/4 The graph is shown below.
Problem 9 One of the following is a subspace of the space of differentiable functions.
I. {f | f(0) – f '(0) = 1} II. {f | f(1) = f '(1)}
A. Determine which is not a subspace and explain why. Solution The first one is not a subspace. For example f(x) = -x is in the set, but 2f(x) = -2x is not.
B. Prove that the other one is a subspace.
Solution
If f(1) = f '(1) and g(1) = g '(1) then (f + g)(1) = f(1) + g(1) = f '(1) + g'(1) = (f + g)'(1) proving closure under "+". Also (cf)(1) = c(f(1)) = c(f '(1)) = (cf)'(1) proving closure under " . " Hence set II is a subspace of the space of differentiable functions.
Problem 10 Prove that if A is a matrix such that A2 = 0 then 0 is an eigenvalue for A.
Solution
We need to show that there is a nonzero v with Av = 0v = 0 This is true if and only if det(A) = 0 but (det A)2 = det(A2) = det(0) = 0 hence det A = 0, and we can conclude that 0 is an eigenvalue for A. Problem 11 Answer the following true or false. If it is true, explain why. If it is false explain why or provide a counter example.
A. If S = {v1, v2} is a linear independent set of vectors in R3 and v3 is not in the span of S, then {v1, v2, v3} is a basis for R3.
Solution True, since then dim(Span{v1, v2, v3}) > dim(Span(S)) = 2. Hence dim(Span{{v1, v2, v3}} = 3. Since any 3 vectors in R3 is a basis for R3.
B. Every orthonormal set of five vectors in R5 is a basis for R5. Solution True, since orthonormal vectors are always linearly independent and five linearly independent vectors in R5 always form a basis for R5. C. Let A and B be matrices such that A2v = a, B2v = b, and ABv = c. Then (A + B)2 v = a + b + 2c Solution False, (A + B)2v = (A2 + AB + BA + B2)v = A2v + ABv + BAv + B2v = a + b + c + BAv So as long as ABv is not equal to BAv, the statement is false. Remember that matrix multiplication does not enjoy the commutative property. |



