Q.
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Start your 14-day free trial to unlock the full solution →Using the symmetry property , the integrand simplifies to after combining and . The integral then becomes , which evaluates to .
The key insight here is that the limits are symmetric about zero, from to . When you see symmetric limits, your first instinct should be to check if the integrand has any symmetry — even, odd, or something that simplifies when you replace with . Here, the integrand is , which is neither even nor odd. But the symmetry trick still works: we can rewrite the integral as half the sum of the function and its reflection.
Let’s walk through it.
- Apply the symmetry property for definite integrals. For any function integrated over , we have:
This is because the integral from to can be transformed by substituting , and then adding it to the integral from to .
Here, and . So:
- Simplify . Since and , we get:
So the sum inside the integral becomes:
- Use the identity . This is a standard double-angle identity. So:
Notice how the symmetry turned a sum of two logs into a single log of a product, and that product collapsed into a simple trigonometric function. This is the power of the trick — it often reveals hidden simplifications.
- Substitute to simplify further. Let . Then , and when , ; when , . So:
- Recall the standard result for . This is a well-known integral. One way to derive it is to use the identity (by substituting ), and then note that:
But the left side, with , becomes , and using symmetry, that equals . Solving gives:
›Proof
Derivation of : …
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