Analyzing the Setup
Welcome, fellow traveler on the road to JEE excellence. Today, we aren't just solving a matrix problem; we are uncovering the hidden symmetry of linear transformations.
You are presented with a matrix A=[1λ510] and a mysterious relationship A−1=αA+βI.
At first glance, you might be tempted to dive into the standard formula for the inverse, calculating the determinant and the adjoint. But stop—take a breath. In the world of JEE Advanced, we look for the path of least resistance, the path that reveals the soul of the matrix.
The Characteristic Soul
Every square matrix carries a 'DNA' known as its characteristic equation. This equation, defined by det(A−kI)=0, tells us how the matrix behaves under transformation.
Let us compute this for our matrix A:
Expanding this, we get (1−k)(10−k)−5λ=0, which simplifies beautifully to k2−11k+(10−5λ)=0. This is the heartbeat of our matrix.
The Power of Cayley-Hamilton
Here is where the magic happens. The Cayley-Hamilton Theorem tells us that a matrix satisfies its own characteristic equation. So, we replace k with A:
This equation is a bridge. We need to reach the form A−1=αA+βI. We simply multiply the entire equation by A−1:
Distributing A−1, we get A−11I+(10−5λ)A−1=0. Now, watch as we isolate A−1 with the precision of a surgeon:
The Final Unveiling
By comparing this to our given relation A−1=αA+βI, we identify our coefficients: α=10−5λ−1 and β=10−5λ11.
We are given the constraint α+β=−2. Substituting our expressions, we find:
10−5λ−1+11=−2⟹10−5λ10=−2
Solving this simple linear equation, we find 10=−20+10λ, which leads us to λ=3.
With λ in hand, the rest is a victory lap. We calculate α=51 and β=−511. Finally, we evaluate the expression 4α2+β2+λ2:
4(51)2+(−511)2+32=4(251)+25121+9=25125+9=5+9=14
And there it is—14. The complexity dissolves into simplicity when you understand the underlying structure. Keep this perspective, and no matrix will ever intimidate you again. Onward!