The Beauty of Symmetry
Unlocking the Integral
Welcome, future engineer. Today, we are going to dismantle a problem that, at first glance, looks like a nightmare of transcendental functions. We are tasked with evaluating the integral I=∫1/22xtan−1xdx.
If you try to find an antiderivative for xtan−1x using standard methods, you will quickly find yourself in a labyrinth with no exit. But in the JEE Advanced arena, when a problem seems impossible to solve directly, it is usually a sign that there is a hidden symmetry waiting to be exploited.
Phase 1
The Reciprocal Insight
Look closely at the limits of integration: 1/2 and 2. They are reciprocals. This is not a coincidence; it is a deliberate invitation.
Whenever you encounter limits that are reciprocals, the substitution x=t1 is your golden key. Let us apply this transformation. If x=t1, then dx=−t21dt.
Now, let us transform the limits: when x=1/2, t=2, and when x=2, t=1/2. Our integral I transforms into:
I=∫21/21/ttan−1(1/t)(−t21)dt
Notice the negative sign from the differential dx. We can use that negative sign to flip the limits back to their original order, from 1/2 to 2. After simplifying the algebra, we get:
Phase 2
The Identity Magic
Here is where the elegance of mathematics shines. We know that for t>0, the inverse trigonometric identity tan−1(1/t)=cot−1(t) holds true. Our integral now looks like this:
Since t is just a dummy variable, we can rename it back to x without changing the value of the integral. We now have two different expressions for the same value I: the original one and this new one involving cot−1x.
This is the moment of truth. Let us add them together:
2I=∫1/22xtan−1xdx+∫1/22xcot−1xdx
Phase 3
The Grand Simplification
Because the limits and the denominators are identical, we can merge these integrals into one:
2I=∫1/22xtan−1x+cot−1xdx
Recall the fundamental identity: tan−1x+cot−1x=2π. The entire numerator collapses into a simple constant!
Our terrifying integral has suddenly become trivial:
2I=∫1/22xπ/2dx=2π∫1/22x1dx
Phase 4
The Final Stretch
The integral of 1/x is simply ln∣x∣. Evaluating this from 1/2 to 2, we get:
2I=2π[lnx]1/22=2π(ln2−ln(1/2))
Since ln(1/2)=−ln2, the expression becomes 2π(ln2−(−ln2))=2π(2ln2). Therefore, 2I=πln2, which leads us to our final answer:
This problem is a masterclass in why we study properties of definite integrals. We didn't need to find a complex antiderivative; we simply needed to see the symmetry, apply the right substitution, and let the identities do the heavy lifting. Keep this strategy in your arsenal—it is a weapon that will serve you well in the exam hall.