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Question 84 of 118

Q.Discuss the solutions of the following system of equations for all values of λ\lambda. x+y+z=2x + y + z = 2, 2x+y−2z=22x + y - 2z = 2, λx+y+4z=2\lambda x + y + 4z = 2

Puducherry TnboardTamil Nadu HSC (DGE) Board 2018Subjective· 10mImportance★★★★★
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Compute the coefficient determinant Δ (a multiple of λ) and the three numerator determinants to classify the system by Cramer's rule, then solve explicitly in each case.

  1. System: x+y+z=2x+y+z=2, 2x+y−2z=22x+y-2z=2, λx+y+4z=2\lambda x+y+4z=2.
  2. Coefficient determinant: Δ=∣11121−2λ14∣\Delta=\begin{vmatrix}1&1&1\\2&1&-2\\\lambda&1&4\end{vmatrix}.
  3. Expand along column 1: Δ=1[(1)(4)−(−2)(1)]−2[(1)(4)−(1)(1)]+λ[(1)(−2)−(1)(1)]=1(6)−2(3)+λ(−3)=6−6−3λ=−3λ\Delta=1[(1)(4)-(-2)(1)]-2[(1)(4)-(1)(1)]+\lambda[(1)(-2)-(1)(1)]=1(6)-2(3)+\lambda(-3)=6-6-3\lambda=-3\lambda.
  4. So Δ=−3λ\Delta=-3\lambda, which vanishes exactly when λ=0\lambda=0.
  5. Case λ≠0\lambda\neq0: Δ≠0\Delta\neq0, so by Cramer's rule the system has a unique solution.
  6. Δx\Delta_x (replace the xx-column, which contains 1,2,λ1,2,\lambda, by the constants 2,2,22,2,2): Δx=∣21121−2214∣=2[(1)(4)−(−2)(1)]−1[(2)(4)−(−2)(2)]+1[(2)(1)−(1)(2)]=2(6)−1(12)+1(0)=12−12+0=0\Delta_x=\begin{vmatrix}2&1&1\\2&1&-2\\2&1&4\end{vmatrix}=2[(1)(4)-(-2)(1)]-1[(2)(4)-(-2)(2)]+1[(2)(1)-(1)(2)]=2(6)-1(12)+1(0)=12-12+0=0. This determinant never contains λ\lambda (that column was replaced), so Δx=0\Delta_x=0 for every λ\lambda.
  7. Δy\Delta_y (replace the yy-column by constants): Δy=∣12122−2λ24∣=1[(2)(4)−(−2)(2)]−2[(2)(4)−(−2)λ]+1[(2)(2)−(2)λ]=1(12)−2(8+2λ)+1(4−2λ)=12−16−4λ+4−2λ=−6λ\Delta_y=\begin{vmatrix}1&2&1\\2&2&-2\\\lambda&2&4\end{vmatrix}=1[(2)(4)-(-2)(2)]-2[(2)(4)-(-2)\lambda]+1[(2)(2)-(2)\lambda]=1(12)-2(8+2\lambda)+1(4-2\lambda)=12-16-4\lambda+4-2\lambda=-6\lambda.
  8. Δz\Delta_z (replace the zz-column by constants): Δz=∣112212λ12∣=1[(1)(2)−(2)(1)]−1[(2)(2)−(2)λ]+2[(2)(1)−(1)λ]=1(0)−1(4−2λ)+2(2−λ)=−4+2λ+4−2λ=0\Delta_z=\begin{vmatrix}1&1&2\\2&1&2\\\lambda&1&2\end{vmatrix}=1[(1)(2)-(2)(1)]-1[(2)(2)-(2)\lambda]+2[(2)(1)-(1)\lambda]=1(0)-1(4-2\lambda)+2(2-\lambda)=-4+2\lambda+4-2\lambda=0; this also never survives with λ\lambda, so Δz=0\Delta_z=0 for every λ\lambda.
  9. For λ≠0\lambda\neq0: x=ΔxΔ=0−3λ=0x=\dfrac{\Delta_x}{\Delta}=\dfrac{0}{-3\lambda}=0, y=ΔyΔ=−6λ−3λ=2y=\dfrac{\Delta_y}{\Delta}=\dfrac{-6\lambda}{-3\lambda}=2, z=ΔzΔ=0−3λ=0z=\dfrac{\Delta_z}{\Delta}=\dfrac{0}{-3\lambda}=0. So the unique solution is (x,y,z)=(0,2,0)(x,y,z)=(0,2,0) — independent of the particular nonzero λ\lambda (it satisfies all three equations for any λ\lambda). …

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