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Matrices & Determinants
Matrices and Determinants
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The system of linear equations \matrixx+λyz=0\crλxyz=0\crx+yλz=0\cr\matrix{ {x + \lambda y - z = 0} \cr {\lambda x - y - z = 0} \cr {x + y - \lambda z = 0} \cr } has a non-trivial solution for :

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Solution

1. Key Concept: Non-Trivial Solutions for Homogeneous Systems

A system of linear equations is called a homogeneous system if all the constant terms are zero. For the given system: x+λyz=0λxyz=0x+yλz=0\begin{aligned} x + \lambda y - z &= 0 \\ \lambda x - y - z &= 0 \\ x + y - \lambda z &= 0 \end{aligned} Notice that all equations are set to zero. Such a system always has at least one solution, which is the trivial solution: x=0,y=0,z=0x=0, y=0, z=0.

For a homogeneous system to have non-trivial solutions (i.e., solutions where at least one of x,y,zx, y, z is non-zero), a specific condition must be met. This condition is that the determinant of the coefficient matrix must be equal to zero. If we represent the system in matrix form as AX=0AX = 0, where AA is the coefficient matrix and XX is the column vector of variables, then non-trivial solutions exist if and only if det(A)=0\det(A) = 0.

2. Setting Up the Problem

First, let's write down the coefficient matrix AA for the given system of equations: A=(1λ1λ1111λ)A = \begin{pmatrix} 1 & \lambda & -1 \\ \lambda & -1 & -1 \\ 1 & 1 & -\lambda \end{pmatrix}

3. Applying the Condition for Non-Trivial Solutions

As established, for the system to have a non-trivial solution, the determinant of the coefficient matrix AA must be zero. det(A)=1λ1λ1111λ=0\det(A) = \begin{vmatrix} 1 & \lambda & -1 \\ \lambda & -1 & -1 \\ 1 & 1 & -\lambda \end{vmatrix} = 0

4. Step-by-Step Calculation of the Determinant

We will expand the 3×33 \times 3 determinant along the first row. The formula for expanding a 3×33 \times 3 determinant abcdefghi\begin{vmatrix} a & b & c \\ d & e & f \\ g & h & i \end{vmatrix} is a(eifh)b(difg)+c(dheg)a(ei - fh) - b(di - fg) + c(dh - eg).

Applying this to our determinant: 1λ1λ1111λ=1((1)(λ)(1)(1))λ((λ)(λ)(1)(1))+(1)((λ)(1)(1)(1))\begin{vmatrix} 1 & \lambda & -1 \\ \lambda & -1 & -1 \\ 1 & 1 & -\lambda \end{vmatrix} = 1 \cdot \left( (-1)(-\lambda) - (-1)(1) \right) - \lambda \cdot \left( (\lambda)(-\lambda) - (-1)(1) \right) + (-1) \cdot \left( (\lambda)(1) - (-1)(1) \right)

Now, let's simplify each term:

  • First term: 1(λ+1)1 \cdot (\lambda + 1)
    • Here, (1)(λ)=λ(-1)(-\lambda) = \lambda and (1)(1)=1(-1)(1) = -1. So, λ(1)=λ+1\lambda - (-1) = \lambda + 1.
  • Second term: λ(λ2+1)-\lambda \cdot (-\lambda^2 + 1)
    • Here, (λ)(λ)=λ2(\lambda)(-\lambda) = -\lambda^2 and (1)(1)=1(-1)(1) = -1. So, λ2(1)=λ2+1-\lambda^2 - (-1) = -\lambda^2 + 1.
  • Third term: 1(λ+1)-1 \cdot (\lambda + 1)
    • Here, (λ)(1)=λ(\lambda)(1) = \lambda and (1)(1)=1(-1)(1) = -1. So, λ(1)=λ+1\lambda - (-1) = \lambda + 1.

Substitute these simplified terms back into the determinant equation: 1(λ+1)λ(λ2+1)1(λ+1)=01(\lambda + 1) - \lambda(-\lambda^2 + 1) - 1(\lambda + 1) = 0

5. Solving the Resulting Equation for λ\lambda

Now, we simplify the equation further: (λ+1)λ(λ2+1)(λ+1)=0(\lambda + 1) - \lambda(-\lambda^2 + 1) - (\lambda + 1) = 0 Notice that the first term (λ+1)(\lambda+1) and the third term (λ+1)-(\lambda+1) cancel each other out. λ(λ2+1)=0-\lambda(-\lambda^2 + 1) = 0 We can multiply both sides by 1-1 to make it easier to work with: λ(λ2+1)=0\lambda(-\lambda^2 + 1) = 0 Rearrange the term inside the parenthesis: λ(1λ2)=0\lambda(1 - \lambda^2) = 0 Now, factorize the term (1λ2)(1 - \lambda^2) using the difference of squares formula (a2b2=(ab)(a+b)a^2 - b^2 = (a-b)(a+b)): λ(1λ)(1+λ)=0\lambda(1 - \lambda)(1 + \lambda) = 0 For this product to be zero, at least one of the factors must be zero. This gives us the possible values for λ\lambda: λ=0or1λ=0or1+λ=0\lambda = 0 \quad \text{or} \quad 1 - \lambda = 0 \quad \text{or} \quad 1 + \lambda = 0 Solving each of these simple equations: λ=0,λ=1,λ=1\lambda = 0, \quad \lambda = 1, \quad \lambda = -1

6. Interpreting the Results and Conclusion

We have found three distinct values of λ\lambda for which the system of linear equations has a non-trivial solution: λ=1,0,1\lambda = -1, 0, 1. Therefore, there are exactly three values of λ\lambda.

Comparing this with the given options: (A) infinitely many values of λ\lambda. (B) exactly one value of λ\lambda. (C) exactly two values of λ\lambda. (D) exactly three values of λ\lambda.

The correct option is (D).

Tips for Success and Common Mistakes:

  • Understand the Condition: Always remember that for a homogeneous system, det(A)=0\det(A) = 0 is the necessary and sufficient condition for non-trivial solutions. If det(A)0\det(A) \ne 0, only the trivial solution (x=y=z=0x=y=z=0) exists.
  • Determinant Expansion Accuracy: Be very careful with signs when expanding determinants, especially for 3×33 \times 3 matrices. A common mistake is forgetting the alternating signs (+++ - +) for the terms in the expansion.
  • Algebraic Simplification: Take your time with the algebraic simplification of the polynomial equation. Look for opportunities to factor or cancel terms, as shown in step 5 where (λ+1)(\lambda+1) terms cancelled out. This can significantly simplify the process of finding roots.
  • Don't Miss λ=0\lambda=0: It's easy to overlook λ=0\lambda=0 if you jump straight to λ21=0\lambda^2 - 1 = 0 after seeing λ(λ21)=0\lambda(\lambda^2 - 1) = 0. Always factor out common terms completely.

Summary / Key Takeaway:

For a homogeneous system of linear equations (AX=0AX=0), non-trivial solutions exist if and only if the determinant of the coefficient matrix AA is zero. The process involves forming the determinant, setting it equal to zero, and then solving the resulting algebraic equation for the unknown parameter(s). In this problem, solving the determinant equation λ(1λ2)=0\lambda(1-\lambda^2)=0 led to three distinct values for λ\lambda.

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