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JEE Main 2020
Matrices & Determinants
Matrices and Determinants
Medium

Question

If the system of equations 11x+y+λz=52x+3y+5z=38x19y39z=μ\begin{array}{r} 11 x+y+\lambda z=-5 \\ 2 x+3 y+5 z=3 \\ 8 x-19 y-39 z=\mu \end{array} has infinitely many solutions, then λ4μ\lambda^4-\mu is equal to :

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Solution

1. Understanding the Condition for Infinitely Many Solutions

For a system of linear equations in three variables: a1x+b1y+c1z=d1a2x+b2y+c2z=d2a3x+b3y+c3z=d3\begin{array}{l} a_1 x+b_1 y+c_1 z=d_1 \\ a_2 x+b_2 y+c_2 z=d_2 \\ a_3 x+b_3 y+c_3 z=d_3 \end{array} This system can be represented in matrix form as AX=BAX = B, where AA is the coefficient matrix, XX is the variable matrix, and BB is the constant matrix. A=(a1b1c1a2b2c2a3b3c3),X=(xyz),B=(d1d2d3)A = \begin{pmatrix} a_1 & b_1 & c_1 \\ a_2 & b_2 & c_2 \\ a_3 & b_3 & c_3 \end{pmatrix}, \quad X = \begin{pmatrix} x \\ y \\ z \end{pmatrix}, \quad B = \begin{pmatrix} d_1 \\ d_2 \\ d_3 \end{pmatrix} According to Cramer's Rule, for this system to have infinitely many solutions, two crucial conditions must be met simultaneously:

  1. The determinant of the coefficient matrix, denoted as Δ=det(A)\Delta = \det(A), must be zero.
  2. All the determinants obtained by replacing a column of AA with the constant terms from BB, denoted as Δ1,Δ2,Δ3\Delta_1, \Delta_2, \Delta_3, must also be zero.

Let's define these determinants explicitly: Δ=a1b1c1a2b2c2a3b3c3\Delta = \begin{vmatrix} a_1 & b_1 & c_1 \\ a_2 & b_2 & c_2 \\ a_3 & b_3 & c_3 \end{vmatrix} Δ1=d1b1c1d2b2c2d3b3c3,Δ2=a1d1c1a2d2c2a3d3c3,Δ3=a1b1d1a2b2d2a3b3d3\Delta_1 = \begin{vmatrix} d_1 & b_1 & c_1 \\ d_2 & b_2 & c_2 \\ d_3 & b_3 & c_3 \end{vmatrix}, \quad \Delta_2 = \begin{vmatrix} a_1 & d_1 & c_1 \\ a_2 & d_2 & c_2 \\ a_3 & d_3 & c_3 \end{vmatrix}, \quad \Delta_3 = \begin{vmatrix} a_1 & b_1 & d_1 \\ a_2 & b_2 & d_2 \\ a_3 & b_3 & d_3 \end{vmatrix} The condition for infinitely many solutions is: Δ=0ANDΔ1=0ANDΔ2=0ANDΔ3=0\Delta = 0 \quad \text{AND} \quad \Delta_1 = 0 \quad \text{AND} \quad \Delta_2 = 0 \quad \text{AND} \quad \Delta_3 = 0 Why this condition? If Δ0\Delta \neq 0, the system has a unique solution. If Δ=0\Delta = 0, the system is either inconsistent (no solution) or has infinitely many solutions. The additional condition that all Δi\Delta_i must also be zero distinguishes the case of infinitely many solutions from the case of no solution. If Δ=0\Delta=0 but at least one Δi0\Delta_i \neq 0, then the system has no solution.

2. Setting Up the System

The given system of linear equations is:

  1. 11x+y+λz=511 x+y+\lambda z=-5
  2. 2x+3y+5z=32 x+3 y+5 z=3
  3. 8x19y39z=μ8 x-19 y-39 z=\mu

From these equations, we can identify the coefficient matrix AA and the constant vector BB: A=(111λ23581939),B=(53μ)A = \begin{pmatrix} 11 & 1 & \lambda \\ 2 & 3 & 5 \\ 8 & -19 & -39 \end{pmatrix}, \quad B = \begin{pmatrix} -5 \\ 3 \\ \mu \end{pmatrix}

3. Finding the Value of λ\lambda

To find the value of λ\lambda, we must apply the first necessary condition for infinitely many solutions: Δ=0\Delta = 0. This condition will allow us to determine λ\lambda.

Let's calculate the determinant of the coefficient matrix AA: Δ=111λ23581939\Delta = \begin{vmatrix} 11 & 1 & \lambda \\ 2 & 3 & 5 \\ 8 & -19 & -39 \end{vmatrix} To simplify the calculation of the determinant, we can use row operations to create zeros in a column or row. Let's perform R3R3+19R2R_3 \to R_3 + 19R_2 to simplify the second column: Δ=111λ2358+19(2)19+19(3)39+19(5)\Delta = \begin{vmatrix} 11 & 1 & \lambda \\ 2 & 3 & 5 \\ 8+19(2) & -19+19(3) & -39+19(5) \end{vmatrix} Δ=111λ235463856\Delta = \begin{vmatrix} 11 & 1 & \lambda \\ 2 & 3 & 5 \\ 46 & 38 & 56 \end{vmatrix} Now, we expand the determinant along the first row: Δ=113538561254656+λ234638\Delta = 11 \begin{vmatrix} 3 & 5 \\ 38 & 56 \end{vmatrix} - 1 \begin{vmatrix} 2 & 5 \\ 46 & 56 \end{vmatrix} + \lambda \begin{vmatrix} 2 & 3 \\ 46 & 38 \end{vmatrix} Δ=11((3)(56)(5)(38))1((2)(56)(5)(46))+λ((2)(38)(3)(46))\Delta = 11((3)(56) - (5)(38)) - 1((2)(56) - (5)(46)) + \lambda((2)(38) - (3)(46)) Δ=11(168190)1(112230)+λ(76138)\Delta = 11(168 - 190) - 1(112 - 230) + \lambda(76 - 138) Δ=11(22)1(118)+λ(62)\Delta = 11(-22) - 1(-118) + \lambda(-62) Δ=242+11862λ\Delta = -242 + 118 - 62\lambda Δ=12462λ\Delta = -124 - 62\lambda For the system to have infinitely many solutions, we must have Δ=0\Delta = 0: 12462λ=0-124 - 62\lambda = 0 62λ=124-62\lambda = 124 λ=12462\lambda = \frac{124}{-62} λ=2\lambda = -2 Thus, we have found the value of λ=2\lambda = -2.

Tip for Determinant Calculation: Using row/column operations to introduce zeros before expanding can significantly simplify calculations and reduce the chance of arithmetic errors, especially for larger matrices. Remember that operations of the form RiRi+kRjR_i \to R_i + k R_j (or CiCi+kCjC_i \to C_i + k C_j) do not change the determinant value.

4. Finding the Value of μ\mu

Now that we have λ=2\lambda = -2, we need to use the other conditions, Δ1=0\Delta_1=0, Δ2=0\Delta_2=0, or Δ3=0\Delta_3=0, to find μ\mu. Since the problem states that the system has infinitely many solutions, all these determinants must be zero. We only need to set one of them to zero to find μ\mu. Let's choose Δ3=0\Delta_3 = 0.

First, we form Δ3\Delta_3 by replacing the third column of the coefficient matrix AA with the constant vector BB. We also substitute the value of λ=2\lambda=-2 into the matrix: Δ3=1115233819μ\Delta_3 = \begin{vmatrix} 11 & 1 & -5 \\ 2 & 3 & 3 \\ 8 & -19 & \mu \end{vmatrix} Now, we set Δ3=0\Delta_3 = 0 and solve for μ\mu. Let's expand along the third column to directly involve μ\mu: Δ3=(5)cofactor(1,3)+(3)cofactor(2,3)+(μ)cofactor(3,3)\Delta_3 = (-5) \cdot \text{cofactor}(1,3) + (3) \cdot \text{cofactor}(2,3) + (\mu) \cdot \text{cofactor}(3,3) Δ3=5238193111819+μ11123\Delta_3 = -5 \begin{vmatrix} 2 & 3 \\ 8 & -19 \end{vmatrix} - 3 \begin{vmatrix} 11 & 1 \\ 8 & -19 \end{vmatrix} + \mu \begin{vmatrix} 11 & 1 \\ 2 & 3 \end{vmatrix} Δ3=5((2)(19)(3)(8))3((11)(19)(1)(8))+μ((11)(3)(1)(2))\Delta_3 = -5((2)(-19) - (3)(8)) - 3((11)(-19) - (1)(8)) + \mu((11)(3) - (1)(2)) Δ3=5(3824)3(2098)+μ(332)\Delta_3 = -5(-38 - 24) - 3(-209 - 8) + \mu(33 - 2) Δ3=5(62)3(217)+μ(31)\Delta_3 = -5(-62) - 3(-217) + \mu(31) Δ3=310+651+31μ\Delta_3 = 310 + 651 + 31\mu Δ3=961+31μ\Delta_3 = 961 + 31\mu For infinitely many solutions, we must have Δ3=0\Delta_3 = 0: 961+31μ=0961 + 31\mu = 0 31μ=96131\mu = -961 μ=96131\mu = \frac{-961}{31} μ=31\mu = -31 So, we have found the value of μ=31\mu = -31.

Common Mistake to Avoid: When calculating Δi\Delta_i, ensure that you substitute the value of λ\lambda (if λ\lambda is part of the determinant Δi\Delta_i) before setting Δi=0\Delta_i=0 to solve for μ\mu. Also, be extremely careful with arithmetic, especially managing negative signs in determinant expansions.

5. Calculating the Final Expression

We have found λ=2\lambda = -2 and μ=31\mu = -31. The question asks for the value of λ4μ\lambda^4 - \mu. λ4μ=(2)4(31)\lambda^4 - \mu = (-2)^4 - (-31) =16(31)= 16 - (-31) =16+31= 16 + 31 =47= 47 Therefore, λ4μ=47\lambda^4 - \mu = 47.

6. Summary and Key Takeaways

This problem is a direct application of the conditions for a system of linear equations to have infinitely many solutions, based on Cramer's Rule. Key Takeaways:

  • A system AX=BAX=B has infinitely many solutions if and only if Δ=0\Delta = 0 AND Δ1=0\Delta_1 = 0 AND Δ2=0\Delta_2 = 0 AND Δ3=0\Delta_3 = 0.
  • The condition Δ=0\Delta=0 is typically used first to find parameters within the coefficient matrix (like λ\lambda in this case).
  • Subsequently, any of the Δi=0\Delta_i=0 conditions can be used to find parameters in the constant vector (like μ\mu here), after substituting the values found from Δ=0\Delta=0.
  • Leverage determinant properties like row/column operations to simplify calculations and reduce potential errors.
  • Meticulous arithmetic and sign management are crucial when evaluating determinants.

The final answer is 47\boxed{\text{47}}.

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