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JEE Main 2023
Matrices & Determinants
Matrices and Determinants
Medium

Question

If the system of equations 2x+yz=52 x+y-z=5 2x5y+λz=μ2 x-5 y+\lambda z=\mu x+2y5z=7x+2 y-5 z=7 has infinitely many solutions, then (λ+μ)2+(λμ)2(\lambda+\mu)^{2}+(\lambda-\mu)^{2} is equal to

Options

Solution

1. Key Concepts and Formulas

  • System of Linear Equations: For a system of three linear equations in three variables (x,y,zx, y, z): a1x+b1y+c1z=d1a_1 x + b_1 y + c_1 z = d_1 a2x+b2y+c2z=d2a_2 x + b_2 y + c_2 z = d_2 a3x+b3y+c3z=d3a_3 x + b_3 y + c_3 z = d_3
  • Conditions for Infinitely Many Solutions (Cramer's Rule): A system of linear equations has infinitely many solutions if and only if the determinant of the coefficient matrix (Δ\Delta) is zero, AND all the auxiliary determinants (Δx,Δy,Δz\Delta_x, \Delta_y, \Delta_z) are also zero.
    • Δ=a1b1c1a2b2c2a3b3c3=0\Delta = \left|\begin{array}{ccc} a_1 & b_1 & c_1 \\ a_2 & b_2 & c_2 \\ a_3 & b_3 & c_3 \end{array}\right| = 0
    • Δx=d1b1c1d2b2c2d3b3c3=0\Delta_x = \left|\begin{array}{ccc} d_1 & b_1 & c_1 \\ d_2 & b_2 & c_2 \\ d_3 & b_3 & c_3 \end{array}\right| = 0
    • Δy=a1d1c1a2d2c2a3d3c3=0\Delta_y = \left|\begin{array}{ccc} a_1 & d_1 & c_1 \\ a_2 & d_2 & c_2 \\ a_3 & d_3 & c_3 \end{array}\right| = 0
    • Δz=a1b1d1a2b2d2a3b3d3=0\Delta_z = \left|\begin{array}{ccc} a_1 & b_1 & d_1 \\ a_2 & b_2 & d_2 \\ a_3 & b_3 & d_3 \end{array}\right| = 0
  • Determinant of a 3×33 \times 3 Matrix: The determinant of abcdefghi\left|\begin{smallmatrix} a & b & c \\ d & e & f \\ g & h & i \end{smallmatrix}\right| is a(eifh)b(difg)+c(dheg)a(ei-fh) - b(di-fg) + c(dh-eg).
  • Algebraic Identity: (A+B)2+(AB)2=2(A2+B2)(A+B)^2 + (A-B)^2 = 2(A^2+B^2).

2. Step-by-Step Solution

We are given the system of equations:

  1. 2x+yz=52 x+y-z=5
  2. 2x5y+λz=μ2 x-5 y+\lambda z=\mu
  3. x+2y5z=7x+2 y-5 z=7

Step 1: Calculate the coefficient determinant (Δ\Delta) and find λ\lambda.

For the system to have infinitely many solutions, the determinant of the coefficient matrix must be zero (Δ=0\Delta = 0). First, let's form the coefficient matrix and calculate its determinant. The coefficients are: a1=2,b1=1,c1=1a_1=2, b_1=1, c_1=-1 a2=2,b2=5,c2=λa_2=2, b_2=-5, c_2=\lambda a3=1,b3=2,c3=5a_3=1, b_3=2, c_3=-5

Δ=21125λ125\Delta = \left|\begin{array}{ccc} 2 & 1 & -1 \\ 2 & -5 & \lambda \\ 1 & 2 & -5 \end{array}\right| Expanding along the first row: Δ=25λ2512λ15+(1)2512\Delta = 2 \cdot \left| \begin{array}{cc} -5 & \lambda \\ 2 & -5 \end{array} \right| - 1 \cdot \left| \begin{array}{cc} 2 & \lambda \\ 1 & -5 \end{array} \right| + (-1) \cdot \left| \begin{array}{cc} 2 & -5 \\ 1 & 2 \end{array} \right| Δ=2((5)(5)(λ)(2))1((2)(5)(λ)(1))1((2)(2)(5)(1))\Delta = 2((-5)(-5) - (\lambda)(2)) - 1((2)(-5) - (\lambda)(1)) - 1((2)(2) - (-5)(1)) Δ=2(252λ)1(10λ)1(4+5)\Delta = 2(25 - 2\lambda) - 1(-10 - \lambda) - 1(4 + 5) Δ=504λ+10+λ9\Delta = 50 - 4\lambda + 10 + \lambda - 9 Δ=(50+109)+(4λ+λ)\Delta = (50 + 10 - 9) + (-4\lambda + \lambda) Δ=513λ\Delta = 51 - 3\lambda

Now, apply the condition Δ=0\Delta = 0: 513λ=051 - 3\lambda = 0 3λ=513\lambda = 51 λ=513\lambda = \frac{51}{3} λ=17\lambda = 17

Step 2: Calculate an auxiliary determinant (Δz\Delta_z) and find μ\mu.

Since the system has 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 can use any one of these to find μ\mu. Let's use Δz=0\Delta_z = 0. The constant terms are: d1=5,d2=μ,d3=7d_1=5, d_2=\mu, d_3=7. The auxiliary determinant Δz\Delta_z is formed by replacing the third column (coefficients of zz) in Δ\Delta with the constant terms: Δz=21525μ127\Delta_z = \left|\begin{array}{ccc} 2 & 1 & 5 \\ 2 & -5 & \mu \\ 1 & 2 & 7 \end{array}\right| Expanding Δz\Delta_z along the first row: Δz=25μ2712μ17+52512\Delta_z = 2 \cdot \left| \begin{array}{cc} -5 & \mu \\ 2 & 7 \end{array} \right| - 1 \cdot \left| \begin{array}{cc} 2 & \mu \\ 1 & 7 \end{array} \right| + 5 \cdot \left| \begin{array}{cc} 2 & -5 \\ 1 & 2 \end{array} \right| Δz=2((5)(7)(μ)(2))1((2)(7)(μ)(1))+5((2)(2)(5)(1))\Delta_z = 2((-5)(7) - (\mu)(2)) - 1((2)(7) - (\mu)(1)) + 5((2)(2) - (-5)(1)) Δz=2(352μ)1(14μ)+5(4+5)\Delta_z = 2(-35 - 2\mu) - 1(14 - \mu) + 5(4 + 5) Δz=704μ14+μ+5(9)\Delta_z = -70 - 4\mu - 14 + \mu + 5(9) Δz=704μ14+μ+45\Delta_z = -70 - 4\mu - 14 + \mu + 45 Δz=(7014+45)+(4μ+μ)\Delta_z = (-70 - 14 + 45) + (-4\mu + \mu) Δz=(84+45)3μ\Delta_z = (-84 + 45) - 3\mu Δz=393μ\Delta_z = -39 - 3\mu

Now, apply the condition Δz=0\Delta_z = 0: 393μ=0-39 - 3\mu = 0 3μ=39-3\mu = 39 μ=393\mu = \frac{39}{-3} μ=13\mu = -13

Step 3: Calculate the required expression (λ+μ)2+(λμ)2(\lambda+\mu)^{2}+(\lambda-\mu)^{2}.

We have found λ=17\lambda = 17 and μ=13\mu = -13. The expression to evaluate is (λ+μ)2+(λμ)2(\lambda+\mu)^{2}+(\lambda-\mu)^{2}.

Substitute the values: (17+(13))2+(17(13))2(17 + (-13))^{2} + (17 - (-13))^{2} =(1713)2+(17+13)2= (17 - 13)^{2} + (17 + 13)^{2} =(4)2+(30)2= (4)^{2} + (30)^{2} =16+900= 16 + 900 =916= 916

Alternatively, using the algebraic identity (A+B)2+(AB)2=2(A2+B2)(A+B)^2 + (A-B)^2 = 2(A^2+B^2): (λ+μ)2+(λμ)2=2(λ2+μ2)(\lambda+\mu)^{2}+(\lambda-\mu)^{2} = 2(\lambda^2 + \mu^2) =2(172+(13)2)= 2(17^2 + (-13)^2) =2(289+169)= 2(289 + 169) =2(458)= 2(458) =916= 916


3. Common Mistakes & Tips

  • Sign Errors in Determinant Expansion: Be extremely careful with the alternating signs and arithmetic when calculating 3×33 \times 3 and 2×22 \times 2 determinants. This is a frequent source of error.
  • Misapplication of Cramer's Rule Conditions: Remember that for infinitely many solutions, all determinants (Δ,Δx,Δy,Δz\Delta, \Delta_x, \Delta_y, \Delta_z) must be zero. If Δ=0\Delta=0 but any Δi0\Delta_i \neq 0, there is no solution.
  • Leverage Algebraic Identities: Using identities like (a+b)2+(ab)2=2(a2+b2)(a+b)^2+(a-b)^2 = 2(a^2+b^2) can simplify calculations and save time in the final step.

4. Summary

This problem required a thorough understanding and application of Cramer's Rule for systems of linear equations. By correctly identifying the conditions for infinitely many solutions (Δ=0\Delta=0 and all auxiliary determinants also zero), we systematically calculated the determinant of the coefficient matrix to find λ\lambda, and then used one of the auxiliary determinants to find μ\mu. Finally, we substituted these values into the given expression, using an algebraic identity for efficiency, to arrive at the solution.

The final answer is 916\boxed{\text{916}}, which corresponds to option (A).

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