Analyzing the Setup
Welcome, fellow traveler on the JEE journey! Today, we are going to peel back the curtain on one of the most elegant topics in linear algebra: the manipulation of matrix inverses.
When you first look at a problem involving G=(I−EF)−1, it is easy to feel overwhelmed by the abstract symbols. See this not as a wall of algebra, but as a dance of structures.
The Bedrock
Defining the Inverse
We are given that G is the inverse of (I−EF). By the very definition of an inverse matrix, if we multiply a matrix by its inverse, we must get the identity matrix I.
This gives us two powerful, symmetric equations:
G(I−EF)=I⟹G−GEF=I⟹GEF=G−I
(I−EF)G=I⟹G−EFG=I⟹EFG=G−I
Both GEF and EFG are equal to the same expression, G−I. This immediately proves that EFG=GEF, confirming that Statement (C) is true.
Even though matrix multiplication is non-commutative, the inverse relationship forces a specific symmetry upon these products.
The Algebraic Dance
Proving Statement (B)
Now, let us tackle Statement (B). We need to evaluate the product (I−FE)(I+FGE).
Expand it just like binomials, being careful to maintain the order of multiplication:
(I−FE)(I+FGE)=I(I)+I(FGE)−FE(I)−FE(FGE)=I+FGE−FE−FEFGE
Focus on the last term: FEFGE. We can use the associativity of matrix multiplication to group it as F(EFG)E.
Since we already know EFG=G−I, we can substitute that in:
FEFGE=F(EFG)E=F(G−I)E=FGE−FE
Now, substitute this back into our expanded expression:
I+FGE−FE−(FGE−FE)=I+FGE−FE−FGE+FE=I
Everything cancels out perfectly. It is like a choreographed dance where every step leads to the identity matrix; thus, Statement (B) is proven true.
The Determinant Bridge
Proving Statement (A)
Finally, let us look at Statement (A). We need to connect ∣FE∣ and ∣FGE∣.
We know from Statement (B) that (I−FE) and (I+FGE) are inverses. Taking the determinant of both sides, we get ∣I−FE∣∣I+FGE∣=∣I∣=1.
To bridge the gap, evaluate the product FE(I+FGE):
FE(I+FGE)=FE+FEFGE=FE+(FGE−FE)=FGE
Taking the determinant of both sides, we get ∣FE∣∣I+FGE∣=∣FGE∣.
Since ∣I+FGE∣=∣I−FE∣1, we substitute this to get:
∣FE∣⋅∣I−FE∣1=∣FGE∣⟹∣FE∣=∣I−FE∣∣FGE∣
Therefore, Statement (A) is also true.
The Takeaway
We have navigated the abstract world of matrices and found that even in the absence of commutativity, there is a deep, underlying order.
The key is to trust the definitions, use associativity to your advantage, and look for the symmetry in the expressions. Keep practicing, and soon, these algebraic dances will become second nature to you!