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JEE Main 2023
Matrices & Determinants
Matrices and Determinants
Easy

Question

Let λ\lambda be a real number for which the system of linear equations x + y + z = 6, 4x + λ\lambda y – λ\lambda z = λ\lambda – 2, 3x + 2y – 4z = – 5 has infinitely many solutions. Then λ\lambda is a root of the quadratic equation:

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Solution

1. Key Concepts and Formulas

  • System of Linear Equations: A system of nn linear equations with nn variables, 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.
  • Conditions for Infinitely Many Solutions (Cramer's Rule Extension): For a system of three linear equations in three variables to have infinitely many solutions, the following conditions must be met:
    1. The determinant of the coefficient matrix, denoted as Δ\Delta (or det(A)det(A)), must be zero (Δ=0\Delta = 0).
    2. All the determinants obtained by replacing a column of the coefficient matrix with the constant terms (Δx,Δy,Δz\Delta_x, \Delta_y, \Delta_z) must also be zero (Δx=0,Δy=0,Δz=0\Delta_x = 0, \Delta_y = 0, \Delta_z = 0).
  • Determinant Expansion: For a 3×33 \times 3 matrix (abcdefghi)\begin{pmatrix} a & b & c \\ d & e & f \\ g & h & i \end{pmatrix}, its determinant is a(eifh)b(difg)+c(dheg)a(ei - fh) - b(di - fg) + c(dh - eg).

2. Step-by-Step Solution

Step 1: Represent the System in Matrix Form First, we express the given system of linear equations in the standard matrix form AX=BAX=B.

The given system is:

  1. x+y+z=6x + y + z = 6
  2. 4x+λyλz=λ24x + \lambda y - \lambda z = \lambda - 2
  3. 3x+2y4z=53x + 2y - 4z = - 5

From this, we identify the coefficient matrix AA and the constant matrix BB:

A=(1114λλ324)andB=(6λ25)A = \begin{pmatrix} 1 & 1 & 1 \\ 4 & \lambda & -\lambda \\ 3 & 2 & -4 \end{pmatrix} \quad \text{and} \quad B = \begin{pmatrix} 6 \\ \lambda - 2 \\ -5 \end{pmatrix}

Step 2: Calculate Δ\Delta and Find Potential Values of λ\lambda For the system to have infinitely many solutions, the determinant of the coefficient matrix, Δ\Delta, must be zero. We calculate Δ\Delta and set it to zero to find the possible values of λ\lambda.

Δ=1114λλ324\Delta = \begin{vmatrix} 1 & 1 & 1 \\ 4 & \lambda & -\lambda \\ 3 & 2 & -4 \end{vmatrix}

We expand the determinant along the first row (R1R_1):

Δ=1(λ(4)(λ)(2))1(4(4)(λ)(3))+1(4(2)λ(3))\Delta = 1 \cdot (\lambda(-4) - (-\lambda)(2)) - 1 \cdot (4(-4) - (-\lambda)(3)) + 1 \cdot (4(2) - \lambda(3)) Δ=1(4λ+2λ)1(16+3λ)+1(83λ)\Delta = 1 \cdot (-4\lambda + 2\lambda) - 1 \cdot (-16 + 3\lambda) + 1 \cdot (8 - 3\lambda) Δ=2λ+163λ+83λ\Delta = -2\lambda + 16 - 3\lambda + 8 - 3\lambda

Combine like terms:

Δ=(233)λ+(16+8)\Delta = (-2 - 3 - 3)\lambda + (16 + 8) Δ=8λ+24\Delta = -8\lambda + 24

Now, set Δ=0\Delta = 0 to find the value(s) of λ\lambda:

8λ+24=08λ=24λ=3-8\lambda + 24 = 0 \\ -8\lambda = -24 \\ \lambda = 3

This means λ=3\lambda = 3 is the only value for which the system could potentially have infinitely many solutions or no solution.

Step 3: Verify Conditions for Infinitely Many Solutions (Check Δx,Δy,Δz\Delta_x, \Delta_y, \Delta_z for λ=3\lambda=3) For infinitely many solutions, not only must Δ=0\Delta=0, but also Δx=0\Delta_x=0, Δy=0\Delta_y=0, and Δz=0\Delta_z=0. We substitute λ=3\lambda=3 into the expressions for Δx,Δy,Δz\Delta_x, \Delta_y, \Delta_z and verify they are all zero.

  • Calculate Δx\Delta_x for λ=3\lambda=3: Replace the first column of AA with BB:

    Δx=611λ2λλ524\Delta_x = \begin{vmatrix} 6 & 1 & 1 \\ \lambda - 2 & \lambda & -\lambda \\ -5 & 2 & -4 \end{vmatrix}

    Substitute λ=3\lambda = 3:

    Δx=6113233524=611133524\Delta_x = \begin{vmatrix} 6 & 1 & 1 \\ 3 - 2 & 3 & -3 \\ -5 & 2 & -4 \end{vmatrix} = \begin{vmatrix} 6 & 1 & 1 \\ 1 & 3 & -3 \\ -5 & 2 & -4 \end{vmatrix}

    Expand Δx\Delta_x along the first row:

    Δx=6(3(4)(3)(2))1(1(4)(3)(5))+1(1(2)3(5))Δx=6(12+6)1(415)+1(2+15)Δx=6(6)1(19)+1(17)Δx=36+19+17Δx=36+36=0\Delta_x = 6(3(-4) - (-3)(2)) - 1(1(-4) - (-3)(-5)) + 1(1(2) - 3(-5)) \\ \Delta_x = 6(-12 + 6) - 1(-4 - 15) + 1(2 + 15) \\ \Delta_x = 6(-6) - 1(-19) + 1(17) \\ \Delta_x = -36 + 19 + 17 \\ \Delta_x = -36 + 36 = 0

    This condition is met.

  • Calculate Δy\Delta_y for λ=3\lambda=3: Replace the second column of AA with BB:

    Δy=1614λ2λ354\Delta_y = \begin{vmatrix} 1 & 6 & 1 \\ 4 & \lambda - 2 & -\lambda \\ 3 & -5 & -4 \end{vmatrix}

    Substitute λ=3\lambda = 3:

    Δy=1614323354=161413354\Delta_y = \begin{vmatrix} 1 & 6 & 1 \\ 4 & 3 - 2 & -3 \\ 3 & -5 & -4 \end{vmatrix} = \begin{vmatrix} 1 & 6 & 1 \\ 4 & 1 & -3 \\ 3 & -5 & -4 \end{vmatrix}

    Expand Δy\Delta_y along the first row:

    Δy=1(1(4)(3)(5))6(4(4)(3)(3))+1(4(5)1(3))Δy=1(415)6(16+9)+1(203)Δy=196(7)+(23)Δy=19+4223Δy=4242=0\Delta_y = 1(1(-4) - (-3)(-5)) - 6(4(-4) - (-3)(3)) + 1(4(-5) - 1(3)) \\ \Delta_y = 1(-4 - 15) - 6(-16 + 9) + 1(-20 - 3) \\ \Delta_y = -19 - 6(-7) + (-23) \\ \Delta_y = -19 + 42 - 23 \\ \Delta_y = 42 - 42 = 0

    This condition is also met.

  • Calculate Δz\Delta_z for λ=3\lambda=3 (Optional, but good for completeness): Replace the third column of AA with BB:

    Δz=1164λλ2325\Delta_z = \begin{vmatrix} 1 & 1 & 6 \\ 4 & \lambda & \lambda - 2 \\ 3 & 2 & -5 \end{vmatrix}

    Substitute λ=3\lambda = 3:

    Δz=1164332325=116431325\Delta_z = \begin{vmatrix} 1 & 1 & 6 \\ 4 & 3 & 3 - 2 \\ 3 & 2 & -5 \end{vmatrix} = \begin{vmatrix} 1 & 1 & 6 \\ 4 & 3 & 1 \\ 3 & 2 & -5 \end{vmatrix}

    Expand Δz\Delta_z along the first row:

    Δz=1(3(5)1(2))1(4(5)1(3))+6(4(2)3(3))Δz=1(152)1(203)+6(89)Δz=171(23)+6(1)Δz=17+236Δz=66=0\Delta_z = 1(3(-5) - 1(2)) - 1(4(-5) - 1(3)) + 6(4(2) - 3(3)) \\ \Delta_z = 1(-15 - 2) - 1(-20 - 3) + 6(8 - 9) \\ \Delta_z = -17 - 1(-23) + 6(-1) \\ \Delta_z = -17 + 23 - 6 \\ \Delta_z = 6 - 6 = 0

    All conditions (Δ=0,Δx=0,Δy=0,Δz=0\Delta = 0, \Delta_x = 0, \Delta_y = 0, \Delta_z = 0) are met for λ=3\lambda = 3. Therefore, the system has infinitely many solutions when λ=3\lambda = 3.

Step 4: Identify the Quadratic Equation Now, we need to find which of the given quadratic equations has λ=3\lambda = 3 as a root. We substitute λ=3\lambda=3 into each option:

  • (A) λ2+λ6=0\lambda^2 + \lambda - 6 = 0 (3)2+(3)6=9+36=126=60(3)^2 + (3) - 6 = 9 + 3 - 6 = 12 - 6 = 6 \neq 0. So, (A) is not the answer.

  • (B) λ2λ6=0\lambda^2 - \lambda - 6 = 0 (3)2(3)6=936=66=0(3)^2 - (3) - 6 = 9 - 3 - 6 = 6 - 6 = 0. This equation is satisfied by λ=3\lambda=3.

  • (C) λ23λ4=0\lambda^2 - 3\lambda - 4 = 0 (3)23(3)4=994=40(3)^2 - 3(3) - 4 = 9 - 9 - 4 = -4 \neq 0. So, (C) is not the answer.

  • (D) λ2+3λ4=0\lambda^2 + 3\lambda - 4 = 0 (3)2+3(3)4=9+94=184=140(3)^2 + 3(3) - 4 = 9 + 9 - 4 = 18 - 4 = 14 \neq 0. So, (D) is not the answer.

Thus, λ=3\lambda=3 is a root of the quadratic equation λ2λ6=0\lambda^2 - \lambda - 6 = 0.

3. Common Mistakes & Tips

  • Determinant Calculation Errors: Carefully expand determinants, paying close attention to signs, especially when terms involve negative λ\lambda or subtraction of negative products. A small arithmetic error can lead to an incorrect value of λ\lambda.
  • Incomplete Conditions: Remember that Δ=0\Delta=0 alone is not sufficient for infinitely many solutions; it could also lead to no solution. All Δx,Δy,Δz\Delta_x, \Delta_y, \Delta_z must also be zero. If Δ=0\Delta=0 but any Δi0\Delta_i \neq 0, the system has no solution.
  • Alternative Method (Gaussian Elimination): For verification or if determinants are complex, converting the system into an augmented matrix and performing row operations (Gaussian elimination) can also determine the nature of solutions. For infinitely many solutions, this method will result in at least one row of zeros (e.g., 0 0 0  00 \ 0 \ 0 \ | \ 0).

4. Summary

To find the value of λ\lambda for which the system of linear equations has infinitely many solutions, we first calculated the determinant of the coefficient matrix (Δ\Delta) and set it to zero. This yielded λ=3\lambda=3. Next, we verified that for λ=3\lambda=3, the determinants Δx,Δy,Δz\Delta_x, \Delta_y, \Delta_z were also all zero, confirming that λ=3\lambda=3 leads to infinitely many solutions. Finally, we checked which of the given quadratic equations has λ=3\lambda=3 as a root, finding that λ2λ6=0\lambda^2 - \lambda - 6 = 0 is the correct equation.

The final answer is (B)λ2λ6=0\boxed{\text{(B)} \lambda^2 - \lambda - 6 = 0}.

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