Analyzing the Setup
Imagine you are standing before a mirror, looking at your own reflection. In the world of mathematics, functional equations often present us with a similar scenario. When you see a problem involving f(x) and f(x1), you are essentially looking at a mathematical mirror.
The function is reflecting itself across the transformation x→x1. This is not just a coincidence; it is a structural hint. Our journey begins with the given equation:
By replacing every instance of x with x1, we generate a second, perfectly complementary equation:
Now, we have a system. Think of f(x) and f(x1) as two unknown variables. This is the moment where the complexity collapses into simplicity.
The Art of Elimination
We want to isolate f(x). To do this, we need to eliminate f(x1). We multiply our first equation by 3 and our second equation by 2:
When we subtract the second equation from the first, the terms involving f(x1) vanish entirely. We are left with:
We have successfully isolated our function. It is no longer a mystery; it is an explicit expression:
The Calculus of Change
Now that we have the explicit form of f(x), we are ready to tackle the second part of our challenge: finding f′(41). We differentiate our expression with respect to x:
With this derivative in hand, we substitute x=41:
5f′(41)=−3(4)2−2=−48−2=−50
This yields the result f′(41)=−10.
Final Calculation
Finally, we return to our original goal: ∣f(3)+f′(41)∣. First, we find f(3) by substituting x=3 into our isolated function:
f(3)=51(33−2(3)−10)=51(1−6−10)=5−15=−3
Adding these together, we get:
The elegance of this solution lies in how the symmetry allowed us to break down a complex functional relationship into a simple algebraic system, and then into a straightforward calculus problem.