Analyzing the Setup
Imagine you are standing in a vast, three-dimensional space. You have three flat, infinite sheets of glass—these are your planes, defined by the equations x+y+z=6, x+2y+5z=9, and x+5y+λz=μ.
In a perfect world, these three planes would meet at a single, beautiful point, representing the unique solution (x,y,z). But today, we are looking for the chaos—the moment when these planes refuse to meet. We are looking for the condition of no solution.
The Gatekeeper
The Determinant D
To understand why a system fails, we must look at the coefficient matrix D. Think of D as the 'DNA' of the system; it tells us whether the equations are linearly independent.
If $D
eq 0$, the planes are oriented such that they must intersect at exactly one point. If D=0, the planes are 'linearly dependent'—they are either parallel or they intersect in a way that does not provide a single point of convergence.
We calculate the determinant:
Expanding this along the first row, we get:
As we simplify this, the tension builds. We find D=2λ−25−λ+5+3, which collapses beautifully into D=λ−17.
For the system to have any chance of being inconsistent, we must have D=0. Thus, the first piece of our puzzle falls into place: λ=17. If λ were anything else, the system would have a unique solution, and our search for 'no solution' would be over before it began.
The Trap
Distinguishing Inconsistency from Infinity
Now, here is where most students stumble. They find λ=17 and stop. But wait! If D=0, the system could either have no solution or infinitely many solutions.
To tell the difference, we look at the 'replacement' determinants, specifically Dz. Think of Dz as the 'test of consistency'. We replace the third column of our matrix with the constants from the right-hand side of our equations:
Expanding this, we get:
Dz=1(2μ−45)−1(μ−9)+6(5−2)
Simplifying this expression, we arrive at Dz=2μ−45−μ+9+18, which simplifies to Dz=μ−18.
The Final Revelation
If Dz were zero, the planes would be perfectly aligned to intersect along a line, giving us infinitely many solutions. But we want no solution. We want the planes to be parallel or shifted such that they never touch.
Therefore, we demand that $D_z
eq 0$. This leads us to the final condition: $\mu - 18
eq 0$, or simply $\mu
eq 18$.
When you look at the final result—λ=17 and $\mu
eq 18$—you aren't just looking at numbers. You are looking at the geometric configuration where the planes are forced into a state of perpetual disagreement.
You have mastered the logic of the system, navigated the trap of infinite solutions, and arrived at the truth. Every time you face a system of equations, remember: you are not just solving for x,y, and z; you are orchestrating the geometry of space itself.