To find the value of 1 + α + α 2 1 + \alpha + \alpha^2 1 + α + α 2 for which the system of linear equations has infinitely many solutions, we first write the system of equations in algebraic form:
x + α y + α 2 z = 1 — (1) x + \alpha y + \alpha^2 z = 1 \quad \text{--- (1)} x + α y + α 2 z = 1 — (1)
α x + y + α z = − 1 — (2) \alpha x + y + \alpha z = -1 \quad \text{--- (2)} α x + y + α z = − 1 — (2)
α 2 x + α y + z = 1 — (3) \alpha^2 x + \alpha y + z = 1 \quad \text{--- (3)} α 2 x + α y + z = 1 — (3)
The determinant of the coefficient matrix D D D is given by:
D = ∣ 1 α α 2 α 1 α α 2 α 1 ∣ D = \begin{vmatrix} 1 & \alpha & \alpha^2 \\ \alpha & 1 & \alpha \\ \alpha^2 & \alpha & 1 \end{vmatrix} D = 1 α α 2 α 1 α α 2 α 1
Expanding D D D along the first row:
D = 1 ( 1 − α 2 ) − α ( α − α 3 ) + α 2 ( α 2 − α 2 ) D = 1(1 - \alpha^2) - \alpha(\alpha - \alpha^3) + \alpha^2(\alpha^2 - \alpha^2) D = 1 ( 1 − α 2 ) − α ( α − α 3 ) + α 2 ( α 2 − α 2 )
D = 1 − α 2 − α 2 + α 4 = α 4 − 2 α 2 + 1 = ( α 2 − 1 ) 2 D = 1 - \alpha^2 - \alpha^2 + \alpha^4 = \alpha^4 - 2\alpha^2 + 1 = (\alpha^2 - 1)^2 D = 1 − α 2 − α 2 + α 4 = α 4 − 2 α 2 + 1 = ( α 2 − 1 ) 2
For the system of equations to have non-unique solutions (either infinitely many solutions or no solution), the determinant D D D must be equal to zero:
( α 2 − 1 ) 2 = 0 ⟹ α = 1 or α = − 1 (\alpha^2 - 1)^2 = 0 \implies \alpha = 1 \text{ or } \alpha = -1 ( α 2 − 1 ) 2 = 0 ⟹ α = 1 or α = − 1
Now, we analyze the system for both possible values of α \alpha α :
Case 1: α = 1 \alpha = 1 α = 1
Substituting α = 1 \alpha = 1 α = 1 into the system gives:
x + y + z = 1 x + y + z = 1 x + y + z = 1
x + y + z = − 1 x + y + z = -1 x + y + z = − 1
x + y + z = 1 x + y + z = 1 x + y + z = 1
Equations 1 and 2 are inconsistent (1 ≠ − 1 1 \neq -1 1 = − 1 ), which means the system has no solution .
Case 2: α = − 1 \alpha = -1 α = − 1
Substituting α = − 1 \alpha = -1 α = − 1 into the system gives:
x − y + z = 1 x - y + z = 1 x − y + z = 1
− x + y − z = − 1 ⟹ x − y + z = 1 -x + y - z = -1 \implies x - y + z = 1 − x + y − z = − 1 ⟹ x − y + z = 1
x − y + z = 1 x - y + z = 1 x − y + z = 1
All three equations are identical to x − y + z = 1 x - y + z = 1 x − y + z = 1 . This represents a single plane in R 3 \mathbb{R}^3 R 3 , which contains infinitely many solutions .
Thus, the required value of α \alpha α for which the system has infinitely many solutions is α = − 1 \alpha = -1 α = − 1 .
Finally, substituting α = − 1 \alpha = -1 α = − 1 into the given expression:
1 + α + α 2 = 1 + ( − 1 ) + ( − 1 ) 2 = 1 − 1 + 1 = 1 1 + \alpha + \alpha^2 = 1 + (-1) + (-1)^2 = 1 - 1 + 1 = 1 1 + α + α 2 = 1 + ( − 1 ) + ( − 1 ) 2 = 1 − 1 + 1 = 1