The Mystery of the Integral Equation
Welcome, my dear student. Today, we are going to peel back the layers of a problem that often intimidates students at first glance: the Fredholm integral equation. It looks like a loop, doesn't it?
We have f(x) defined by an integral that contains f(y). It feels like a snake eating its own tail. But I want you to take a deep breath. In the world of JEE Advanced, these problems are not designed to trap you; they are designed to test your ability to see the hidden structure beneath the complexity.
Phase 1
The Constant Insight
Let us look at the equation:
f(x)=x+∫0π/2sinx⋅cosyf(y)dy
The first thing we must do is observe the variable of integration. We are integrating with respect to y. This is the key to the entire kingdom.
Because the integral is strictly about y, the term sinx is completely oblivious to the integration process. To the integral, sinx is just a constant, like the number 5 or π.
So, let us pull it out! We rewrite the equation as:
f(x)=x+sinx∫0π/2cosyf(y)dy
Suddenly, the equation looks much less intimidating, doesn't it?
Phase 2
The Power of Substitution
Now, look at that integral: ∫0π/2cosyf(y)dy. Since the limits are 0 and π/2, this integral is not a function of x; it is a fixed, numerical value.
Let us call this value K. By defining K=∫0π/2cosyf(y)dy, we have transformed our complex integral equation into a simple algebraic one:
This is the 'soul' of our function. We now know that f(x) must be of the form x plus some constant times sinx. Our only mission now is to find that constant K.
Phase 3
The Recursive Loop
How do we find K? We use the definition we just created! We know K=∫0π/2cosyf(y)dy.
Since we now know that f(y)=y+Ksiny, we can substitute this directly into our integral. This gives us:
By distributing the cosy, we get:
K=∫0π/2(ycosy+Ksinycosy)dy
Using the linearity of integrals, we split this into two parts:
K=∫0π/2ycosydy+K∫0π/2sinycosydy
Phase 4
The Calculus Journey
Let us solve these two integrals one by one. For the first part, I1=∫0π/2ycosydy, we use integration by parts.
Let u=y and dv=cosydy. Then du=dy and v=siny. The formula ∫udv=uv−∫vdu gives us:
[ysiny]0π/2−∫0π/2sinydy
Evaluating this, we get (2π⋅1−0)−[−cosy]0π/2=2π−(0−(−1))=2π−1. Beautiful, isn't it?
Now for the second part, I2=K∫0π/2sinycosydy. We know that sinycosy=21sin(2y).
Integrating this, we get:
K[2sin2y]0π/2=K(21−0)=2K
Phase 5
The Final Victory
We are almost there. Putting it all together, we have:
Subtracting 2K from both sides, we get 2K=2π−1. Multiplying by 2, we find K=π−2.
We have conquered the constant! Now, we simply substitute K back into our structural equation:
You have successfully navigated the integral equation. Take a moment to appreciate the elegance of the result. You didn't just solve a problem; you decoded a mathematical structure. Keep this confidence with you for the next one!