Solving Ax=b via Inverses - Linear Algebra

  1. Consider the system of equations 3x+2y=73x + 2y = 7 and 4x+3y=94x + 3y = 9. If this system is represented as Ax⃗=b⃗A\vec{x}=\vec{b}, and the solution is found using x⃗=A−1b⃗\vec{x}=A^{-1}\vec{b}, what is the matrix A−1A^{-1}?
    Answer: (3−2−43)\begin{pmatrix} 3 & -2 \\ -4 & 3 \end{pmatrix} The matrix for the system is A=(3243)A = \begin{pmatrix} 3 & 2 \\ 4 & 3 \end{pmatrix}. To find the inverse, first calculate the determinant: det⁡(A)=(3)(3)−(2)(4)=9−8=1\det(A) = (3)(3) - (2)(4) = 9 - 8 = 1. The formula for the inverse of a 2x2 matrix (abcd)\begin{pmatrix} a & b \\ c & d \end{pmatrix} is 1ad−bc(d−b−ca)\frac{1}{ad-bc}\begin{pmatrix} d & -b \\ -c & a \end{pmatrix}. Applying this, A−1=11(3−2−43)=(3−2−43)A^{-1} = \frac{1}{1}\begin{pmatrix} 3 & -2 \\ -4 & 3 \end{pmatrix} = \begin{pmatrix} 3 & -2 \\ -4 & 3 \end{pmatrix}.
  2. For an invertible matrix A=(abcd)A = \begin{pmatrix} a & b \\ c & d \end{pmatrix}, the solution to Ax⃗=(pq)A\vec{x} = \begin{pmatrix} p \\ q \end{pmatrix} is x⃗=(x1x2)\vec{x} = \begin{pmatrix} x_1 \\ x_2 \end{pmatrix}. Which expression represents x1x_1?
    Answer: x1=dp−bqad−bcx_1 = \frac{dp - bq}{ad-bc} First, find the inverse of AA. The determinant is det⁡(A)=ad−bc\det(A)=ad-bc. The inverse is A−1=1ad−bc(d−b−ca)A^{-1} = \frac{1}{ad-bc} \begin{pmatrix} d & -b \\ -c & a \end{pmatrix}. The solution is x⃗=A−1b⃗\vec{x} = A^{-1}\vec{b}. So, (x1x2)=1ad−bc(d−b−ca)(pq)=1ad−bc(dp−bq−cp+aq)\begin{pmatrix} x_1 \\ x_2 \end{pmatrix} = \frac{1}{ad-bc} \begin{pmatrix} d & -b \\ -c & a \end{pmatrix} \begin{pmatrix} p \\ q \end{pmatrix} = \frac{1}{ad-bc} \begin{pmatrix} dp - bq \\ -cp + aq \end{pmatrix}. The first component of the solution vector is x1=dp−bqad−bcx_1 = \frac{dp - bq}{ad-bc}.
  3. For the system Ax=bAx = b where A=(cos⁡θ−sin⁡θsin⁡θcos⁡θ)A = \begin{pmatrix} \cos\theta & -\sin\theta \\ \sin\theta & \cos\theta \end{pmatrix} and b=(10)b = \begin{pmatrix} 1 \\ 0 \end{pmatrix}, the solution using x=A−1bx = A^{-1}b is x=(cos⁡θsin⁡θ)x = \begin{pmatrix} \cos\theta \\ \sin\theta \end{pmatrix}. What does this solution represent geometrically?
    Answer: Rotating the vector bb clockwise by angle θ\theta to obtain the solution vector xx Matrix AA is a rotation matrix that rotates vectors counterclockwise by θ\theta. Since x=A−1bx = A^{-1}b, we have Ax=bAx = b, meaning rotating xx counterclockwise by θ\theta gives b=(10)b = \begin{pmatrix} 1 \\ 0 \end{pmatrix}. Therefore, xx is obtained by rotating bb clockwise by θ\theta. Indeed, A−1=AT=(cos⁡θsin⁡θ−sin⁡θcos⁡θ)A^{-1} = A^T = \begin{pmatrix} \cos\theta & \sin\theta \\ -\sin\theta & \cos\theta \end{pmatrix} rotates clockwise by θ\theta. Choice A incorrectly states counterclockwise rotation. Choice C describes projection, not rotation. Choice D describes reflection, which is incorrect.
  4. The solution to the system Ax⃗=b⃗A\vec{x}=\vec{b} is x⃗=(5−2)\vec{x}=\begin{pmatrix} 5 \\ -2 \end{pmatrix}. If the same matrix AA is used in a new system Ay⃗=c⃗A\vec{y}=\vec{c}, where c⃗=3b⃗\vec{c} = 3\vec{b}, what is the solution vector y⃗\vec{y}?
    Answer: (15−6)\begin{pmatrix} 15 \\ -6 \end{pmatrix} From the first system, we know that x⃗=A−1b⃗\vec{x} = A^{-1}\vec{b}. The solution to the new system is y⃗=A−1c⃗\vec{y} = A^{-1}\vec{c}. Since we are given that c⃗=3b⃗\vec{c} = 3\vec{b}, we can substitute this into the equation for y⃗\vec{y}: y⃗=A−1(3b⃗)\vec{y} = A^{-1}(3\vec{b}). By the properties of matrix multiplication, the scalar can be factored out: y⃗=3(A−1b⃗)\vec{y} = 3(A^{-1}\vec{b}). Since A−1b⃗=x⃗A^{-1}\vec{b}=\vec{x}, we have y⃗=3x⃗\vec{y} = 3\vec{x}. Therefore, y⃗=3(5−2)=(15−6)\vec{y} = 3\begin{pmatrix} 5 \\ -2 \end{pmatrix} = \begin{pmatrix} 15 \\ -6 \end{pmatrix}.
  5. A system of linear equations Ax⃗=b⃗A\vec{x}=\vec{b} is solved using the inverse matrix A−1A^{-1}. Given A−1=(2513)A^{-1} = \begin{pmatrix} 2 & 5 \\ 1 & 3 \end{pmatrix} and b⃗=(−12)\vec{b} = \begin{pmatrix} -1 \\ 2 \end{pmatrix}, what is the solution vector x⃗\vec{x}?
    Answer: (85)\begin{pmatrix} 8 \\ 5 \end{pmatrix} The solution is given by the formula x⃗=A−1b⃗\vec{x} = A^{-1}\vec{b}. We compute the matrix-vector product: x⃗=(2513)(−12)=((2)(−1)+(5)(2)(1)(−1)+(3)(2))=(−2+10−1+6)=(85)\vec{x} = \begin{pmatrix} 2 & 5 \\ 1 & 3 \end{pmatrix} \begin{pmatrix} -1 \\ 2 \end{pmatrix} = \begin{pmatrix} (2)(-1) + (5)(2) \\ (1)(-1) + (3)(2) \end{pmatrix} = \begin{pmatrix} -2 + 10 \\ -1 + 6 \end{pmatrix} = \begin{pmatrix} 8 \\ 5 \end{pmatrix}
  6. The matrix equation AXB=CAXB = C can be solved for XX when AA and BB are invertible. If this equation is rewritten as a system of the form Mx=cMx = c where xx contains the entries of XX, which matrix MM allows solution via x=M−1cx = M^{-1}c?
    Answer: M=BT⊗AM = B^T \otimes A where ⊗\otimes denotes the Kronecker product When you encounter matrix equations like AXB=CAXB = C, the key is understanding how to vectorize them using the Kronecker product. This transformation allows you to convert a matrix equation into a standard linear system that can be solved using matrix inversion. The vectorization of AXB=CAXB = C follows a specific rule: vec(AXB)=(BT⊗A)vec(X)\text{vec}(AXB) = (B^T \otimes A)\text{vec}(X). This identity comes from the fundamental property that vec(PQR)=(RT⊗P)vec(Q)\text{vec}(PQR) = (R^T \otimes P)\text{vec}(Q). Applying this to our equation, we get (BT⊗A)vec(X)=vec(C)(B^T \otimes A)\text{vec}(X) = \text{vec}(C), which gives us the system Mx=cMx = c where M=BT⊗AM = B^T \otimes A. Answer D is correct because it provides the matrix M=BT⊗AM = B^T \otimes A that emerges from proper vectorization of the original equation. Answer A is wrong because A⊗BA \otimes B doesn't account for the transpose needed in the vectorization formula. Answer B is incorrect because ABAB uses standard multiplication, which doesn't preserve the structure needed for vectorization—the dimensions won't even match in most cases. Answer C is close but has the Kronecker product terms reversed; A⊗BTA \otimes B^T doesn't follow the correct vectorization rule. Remember this pattern: when vectorizing AXB=CAXB = C, the coefficient matrix is always (BT⊗A)(B^T \otimes A)—the rightmost matrix gets transposed and appears first in the Kronecker product. This reversal and transpose rule is essential for solving matrix equations via vectorization.
  7. Matrix AA satisfies A2=I+2AA^2 = I + 2A. To solve Ax=bAx = b using the inverse method, what is the correct expression for A−1A^{-1}?
    Answer: A−1=A−2IA^{-1} = A - 2I When you encounter a matrix equation like A2=I+2AA^2 = I + 2A, you're dealing with finding a matrix inverse through algebraic manipulation. The key insight is to rearrange this equation to isolate terms that will help you express A−1A^{-1}. Starting with A2=I+2AA^2 = I + 2A, subtract 2A2A from both sides: A2−2A=IA^2 - 2A = I. Now factor the left side: A(A−2I)=IA(A - 2I) = I. This is the crucial step—you've found that AA multiplied by (A−2I)(A - 2I) equals the identity matrix II. By definition of matrix inverses, if AB=IAB = I, then B=A−1B = A^{-1}. Therefore, A−1=A−2IA^{-1} = A - 2I. Choice A (A−1=I+2AA^{-1} = I + 2A) comes from incorrectly assuming you can just move terms around without proper algebraic manipulation. If this were correct, then A(I+2A)=IA(I + 2A) = I, which would mean A+2A2=IA + 2A^2 = I—but substituting our original equation shows this doesn't work. Choice B (A−1=12(A−I)A^{-1} = \frac{1}{2}(A - I)) likely results from incorrect factoring or arithmetic errors in the algebraic manipulation. Choice D (A−1=2I−AA^{-1} = 2I - A) is close to the correct answer but has the wrong sign. This might come from incorrectly rearranging A(A−2I)=IA(A - 2I) = I as (2I−A)A=I(2I - A)A = I. Study tip: When finding matrix inverses from polynomial equations, always factor to get the form A⋅(expression)=IA \cdot (\text{expression}) = I. The expression in parentheses is your inverse. Double-check by verifying that your candidate inverse actually satisfies AA−1=IAA^{-1} = I.
  8. The system Ax=bAx = b has solution x∗x^*. A student claims that if ∥A−1∥\|A^{-1}\| is large, then small changes in bb will cause large changes in the solution x∗x^*. To test this claim using the inverse method x=A−1bx = A^{-1}b, which approach is most appropriate?
    Answer: Compute ∥A−1(b+δb)−A−1b∥\|A^{-1}(b + \delta b) - A^{-1}b\| for small perturbations δb\delta b and compare to ∥A−1∥∥δb∥\|A^{-1}\|\|\delta b\| The change in solution is Δx=A−1(b+δb)−A−1b=A−1δb\Delta x = A^{-1}(b + \delta b) - A^{-1}b = A^{-1}\delta b. So ∥Δx∥=∥A−1δb∥≤∥A−1∥∥δb∥\|\Delta x\| = \|A^{-1}\delta b\| \leq \|A^{-1}\|\|\delta b\|. Testing this relationship directly validates the student's claim about sensitivity. Choice A looks at changes in norms rather than changes in vectors. Choice C incorrectly relates determinant to matrix norm and sensitivity. Choice D confuses existence of solution with stability of solution.
  9. Let AA be an invertible 3×33 \times 3 matrix. If one were to solve the system Ax⃗=e2⃗A\vec{x} = \vec{e_2}, where e2⃗=(010)\vec{e_2} = \begin{pmatrix} 0 \\ 1 \\ 0 \end{pmatrix} is the second standard basis vector, what would the solution vector x⃗\vec{x} represent?
    Answer: The second column of A−1A^{-1}. The solution to the system is given by x⃗=A−1b⃗\vec{x} = A^{-1}\vec{b}. In this case, b⃗=e2⃗\vec{b} = \vec{e_2}. So, x⃗=A−1e2⃗\vec{x} = A^{-1}\vec{e_2}. The product of a matrix and the jj-th standard basis vector, ej⃗\vec{e_j}, results in the jj-th column of that matrix. Therefore, A−1e2⃗A^{-1}\vec{e_2} is precisely the second column of the matrix A−1A^{-1}.
  10. Consider two systems: Ax=b1Ax = b_1 with solution x1=A−1b1x_1 = A^{-1}b_1 and Ax=b2Ax = b_2 with solution x2=A−1b2x_2 = A^{-1}b_2. If b2=b1+αAx1b_2 = b_1 + \alpha Ax_1 for some scalar α\alpha, what is x2x_2 in terms of x1x_1?
    Answer: x2=x1+αx1=(1+α)x1x_2 = x_1 + \alpha x_1 = (1 + \alpha)x_1 When you encounter linear systems with related right-hand sides, the key insight is recognizing how changes in the input vector affect the solution. This question tests your understanding of how matrix inverses distribute over vector addition. Let's work through this systematically. We know that x2=A−1b2x_2 = A^{-1}b_2, and we're given that b2=b1+αAx1b_2 = b_1 + \alpha Ax_1. Substituting this expression: x2=A−1(b1+αAx1)=A−1b1+A−1(αAx1)=A−1b1+αA−1Ax1x_2 = A^{-1}(b_1 + \alpha Ax_1) = A^{-1}b_1 + A^{-1}(\alpha Ax_1) = A^{-1}b_1 + \alpha A^{-1}Ax_1 Since A−1A=IA^{-1}A = I (the identity matrix), we have A−1Ax1=x1A^{-1}Ax_1 = x_1. Also, since x1=A−1b1x_1 = A^{-1}b_1, our expression becomes: x2=x1+αx1=(1+α)x1x_2 = x_1 + \alpha x_1 = (1 + \alpha)x_1 This confirms answer C is correct. Looking at the wrong answers: A) x2=(1+α)A−1x1x_2 = (1 + \alpha)A^{-1}x_1 incorrectly applies the inverse to x1x_1 instead of recognizing that A−1b1=x1A^{-1}b_1 = x_1. B) x2=x1+αA−1x1x_2 = x_1 + \alpha A^{-1}x_1 stops one step short of the simplification, failing to recognize that A−1Ax1=x1A^{-1}Ax_1 = x_1. D) x2=x1+αA−2x1x_2 = x_1 + \alpha A^{-2}x_1 incorrectly squares the inverse, showing a fundamental misunderstanding of matrix multiplication. Study tip: When working with linear systems and matrix inverses, always look for opportunities to use the fact that A−1A=IA^{-1}A = I. This identity is your key to simplifying expressions involving both a matrix and its inverse.
  11. A system Ax=bAx = b has a unique solution that can be expressed as x=A−1bx = A^{-1}b. If matrix AA is replaced by 2A2A, what expression gives the solution to the new system (2A)y=b(2A)y = b?
    Answer: y=12A−1by = \frac{1}{2}A^{-1}b For the system (2A)y=b(2A)y = b, we need (2A)−1(2A)^{-1}. Since (2A)−1=12A−1(2A)^{-1} = \frac{1}{2}A^{-1}, the solution is y=(2A)−1b=12A−1by = (2A)^{-1}b = \frac{1}{2}A^{-1}b. Choice B incorrectly multiplies by 2 instead of 12\frac{1}{2}. Choice C ignores the scalar multiplication entirely. Choice D is technically correct notation but doesn't simplify the expression as requested.
  12. Consider the block matrix M=(A00B)M = \begin{pmatrix} A & 0 \\ 0 & B \end{pmatrix} where AA and BB are invertible 2×22 \times 2 matrices. To solve M(xy)=(uv)M\begin{pmatrix} x \\ y \end{pmatrix} = \begin{pmatrix} u \\ v \end{pmatrix} using M−1M^{-1}, which statement is correct?
    Answer: M−1=(A−100B−1)M^{-1} = \begin{pmatrix} A^{-1} & 0 \\ 0 & B^{-1} \end{pmatrix} and the system decouples into Ax=uAx = u and By=vBy = v For a block diagonal matrix M=(A00B)M = \begin{pmatrix} A & 0 \\ 0 & B \end{pmatrix}, the inverse is M−1=(A−100B−1)M^{-1} = \begin{pmatrix} A^{-1} & 0 \\ 0 & B^{-1} \end{pmatrix}. The system M(xy)=(uv)M\begin{pmatrix} x \\ y \end{pmatrix} = \begin{pmatrix} u \\ v \end{pmatrix} decouples into two independent systems: Ax=uAx = u and By=vBy = v. Choice B gives wrong form for block diagonal inverse. Choice C confuses block diagonal with general 2×22 \times 2 matrix inverse formula. Choice D correctly identifies M−1M^{-1} but incorrectly claims the system cannot decouple.
  13. Let A=(1224)A = \begin{pmatrix} 1 & 2 \\ 2 & 4 \end{pmatrix}. An attempt to solve the system Ax⃗=b⃗A\vec{x}=\vec{b} using the inverse method fails. What is the fundamental reason for this failure?
    Answer: The matrix AA is singular because its columns are linearly dependent. The inverse method requires the matrix AA to be invertible. A matrix is invertible if and only if its determinant is non-zero. The determinant of AA is det⁡(A)=(1)(4)−(2)(2)=4−4=0\det(A) = (1)(4) - (2)(2) = 4 - 4 = 0. Since the determinant is zero, AA is singular and not invertible. This singularity is a result of the columns being linearly dependent (the second column is twice the first column). This is the fundamental reason the inverse method fails.
  14. To solve the matrix equation XA=BXA = B for the matrix XX, where AA and BB are known n×nn \times n matrices and AA is invertible, one must perform a matrix multiplication involving A−1A^{-1} and BB. Which expression correctly calculates XX?
    Answer: X=BA−1X = BA^{-1} To isolate the matrix XX in the equation XA=BXA = B, we need to multiply by A−1A^{-1}. Since matrix multiplication is not commutative, the side on which we multiply matters. To cancel AA, we must multiply by A−1A^{-1} on the right side of both sides of the equation: XAA−1=BA−1XAA^{-1} = BA^{-1}. This simplifies to XI=BA−1XI = BA^{-1}, so X=BA−1X = BA^{-1}. Choice A is the solution to AX=BAX=B.
  15. A 3×33 \times 3 matrix AA has the property that A−1=12ATA^{-1} = \frac{1}{2}A^T. If the system Ax=e1Ax = e_1 (where e1=(100)e_1 = \begin{pmatrix} 1 \\ 0 \\ 0 \end{pmatrix}) has solution x=(abc)x = \begin{pmatrix} a \\ b \\ c \end{pmatrix}, what constraint must hold?
    Answer: a2+b2+c2=12a^2 + b^2 + c^2 = \frac{1}{2} This question tests your understanding of orthogonal matrices and their properties. When you see that A−1=12ATA^{-1} = \frac{1}{2}A^T, you're dealing with a scaled orthogonal matrix, which means the columns (and rows) of AA have special geometric relationships. To find the constraint, start with the given relationship A−1=12ATA^{-1} = \frac{1}{2}A^T. Since AA−1=IAA^{-1} = I, we have: A⋅12AT=IA \cdot \frac{1}{2}A^T = I 12AAT=I\frac{1}{2}AA^T = I AAT=2IAA^T = 2I Now, since Ax=e1Ax = e_1 where x=(abc)x = \begin{pmatrix} a \\ b \\ c \end{pmatrix}, we can use the relationship AAT=2IAA^T = 2I. The first column of AATAA^T equals AA times the first column of ATA^T (which is the first row of AA). But we also know that the first column of AATAA^T is the first column of 2I2I, which is (200)\begin{pmatrix} 2 \\ 0 \\ 0 \end{pmatrix}. Since Ax=e1Ax = e_1, we have x=A−1e1=12ATe1x = A^{-1}e_1 = \frac{1}{2}A^T e_1, which means xx is half the first column of ATA^T (or half the first row of AA). The constraint AAT=2IAA^T = 2I tells us that the dot product of the first row of AA with itself equals 2. Since xx is half this row, we get a2+b2+c2=12a^2 + b^2 + c^2 = \frac{1}{2}. Choice A gives 14\frac{1}{4} (dividing by 4 instead of 2), choice B gives 2 (forgetting the scaling), and choice C gives 1 (assuming standard orthogonal matrix). Choice D correctly accounts for the 12\frac{1}{2} scaling factor. Study tip: When working with scaled orthogonal matrices, always track how the scaling affects inner products and norms throughout your calculations.
  16. Consider the system of equations defined by Ax⃗=b⃗A\vec{x}=\vec{b} where A=(k49k)A = \begin{pmatrix} k & 4 \\ 9 & k \end{pmatrix}. For which value(s) of kk is it NOT possible to find a unique solution using the formula x⃗=A−1b⃗\vec{x}=A^{-1}\vec{b}?
    Answer: k=6k=6 and k=−6k=-6 The inverse method is not possible when the matrix AA is singular, which occurs when its determinant is zero. The determinant of AA is det⁡(A)=(k)(k)−(4)(9)=k2−36\det(A) = (k)(k) - (4)(9) = k^2 - 36. Setting the determinant to zero gives the equation k2−36=0k^2 - 36 = 0. This factors as (k−6)(k+6)=0(k-6)(k+6)=0, which has solutions k=6k=6 and k=−6k=-6. For these values of kk, the matrix AA is not invertible.
  17. In which step did the student first make an error?
    Answer: Step 3 The formula for the inverse matrix is A−1=1det⁡(A)adj(A)A^{-1} = \frac{1}{\det(A)}\text{adj}(A). The student correctly calculated the determinant in Step 1 and the adjugate matrix in Step 2. However, in Step 3, the student failed to divide the adjugate matrix by the determinant (which is 2). The correct inverse should be A−1=12(3−2−54)A^{-1} = \frac{1}{2}\begin{pmatrix} 3 & -2 \\ -5 & 4 \end{pmatrix}. This is the first error in the process.
  18. The system of linear equations Ax⃗=b⃗A\vec{x}=\vec{b} is to be solved using the matrix inverse method, yielding the unique solution x⃗=A−1b⃗\vec{x}=A^{-1}\vec{b}. Which of the following conditions is necessary for this method to be applicable?
    Answer: The determinant of matrix AA must be non-zero. The formula x⃗=A−1b⃗\vec{x}=A^{-1}\vec{b} requires the existence of the inverse matrix A−1A^{-1}. A square matrix AA has an inverse if and only if it is non-singular, which is equivalent to its determinant being non-zero. The other conditions are not necessary. Symmetry is not required for invertibility. The method works for b⃗=0⃗\vec{b}=\vec{0} (giving x⃗=0⃗\vec{x}=\vec{0}). For a unique solution via matrix inversion, AA must be a square matrix (number of equations equals number of variables).
  19. Let AA and BB be invertible n×nn \times n matrices. To solve the matrix equation ABx⃗=c⃗AB\vec{x} = \vec{c} for the vector x⃗\vec{x}, which of the following computations is correct?
    Answer: x⃗=B−1A−1c⃗\vec{x} = B^{-1}A^{-1}\vec{c} To isolate x⃗\vec{x}, we need to multiply both sides by the inverse of the matrix product ABAB. The inverse of a product of matrices is the product of their inverses in reverse order: (AB)−1=B−1A−1(AB)^{-1} = B^{-1}A^{-1}. We must left-multiply both sides of the equation by this inverse: (AB)−1(AB)x⃗=(AB)−1c⃗(AB)^{-1}(AB)\vec{x} = (AB)^{-1}\vec{c}, which simplifies to Ix⃗=B−1A−1c⃗I\vec{x} = B^{-1}A^{-1}\vec{c}, so x⃗=B−1A−1c⃗\vec{x} = B^{-1}A^{-1}\vec{c}.
  20. A bakery sells two types of boxes: a pastry box with 3 croissants and 4 muffins, and a breakfast box with 5 croissants and 2 muffins. On a given day, they use a total of 160 croissants and 100 muffins to fill an order. Let pp be the number of pastry boxes and bb be the number of breakfast boxes. The situation is modeled by the matrix equation A(pb)=(160100)A\begin{pmatrix} p \\ b \end{pmatrix} = \begin{pmatrix} 160 \\ 100 \end{pmatrix}. Which of the following expressions correctly solves for the number of boxes?
    Answer: 1−14(2−5−43)(160100)\frac{1}{-14} \begin{pmatrix} 2 & -5 \\ -4 & 3 \end{pmatrix} \begin{pmatrix} 160 \\ 100 \end{pmatrix} The system of equations is 3p+5b=1603p + 5b = 160 (croissants) and 4p+2b=1004p + 2b = 100 (muffins). The coefficient matrix is A=(3542)A = \begin{pmatrix} 3 & 5 \\ 4 & 2 \end{pmatrix}. The solution is given by (pb)=A−1(160100)\begin{pmatrix} p \\ b \end{pmatrix} = A^{-1}\begin{pmatrix} 160 \\ 100 \end{pmatrix}. We must calculate A−1A^{-1}. The determinant is det⁡(A)=(3)(2)−(5)(4)=6−20=−14\det(A) = (3)(2) - (5)(4) = 6 - 20 = -14. The inverse is A−1=1−14(2−5−43)A^{-1} = \frac{1}{-14}\begin{pmatrix} 2 & -5 \\ -4 & 3 \end{pmatrix}. Therefore, the correct expression for the solution is 1−14(2−5−43)(160100)\frac{1}{-14} \begin{pmatrix} 2 & -5 \\ -4 & 3 \end{pmatrix} \begin{pmatrix} 160 \\ 100 \end{pmatrix}.

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