Q.Evaluate
The integral is solved by using the identity , then integrating term by term. The result is .
This problem is a classic example of evaluating a definite integral of a squared trigonometric function. The direct approach — integrating as is — is messy because the antiderivative isn't immediately obvious. Instead, we use a power-reduction identity to rewrite the integrand into a sum of simpler terms.
The key insight: oscillates between 0 and 1, and its average value over a full period is . The identity converts the squared sine into a constant plus a cosine wave with double frequency. Integrating a constant is trivial, and integrating is straightforward. The limits are symmetric about zero, which also simplifies things slightly, but the method works for any limits.
Let’s work through it step by step.
- Apply the power-reduction identity. We rewrite the integrand using the standard identity:
This is derived from the double-angle formula .
The integral becomes:
- Split the integral into two simpler ones. The constant factor can be pulled out, and the difference inside the integral splits:
- Evaluate the first integral. The integral of over an interval is just the length of the interval:
So the first term is:
- Evaluate the second integral. The antiderivative of is . Thus:
Compute at the upper limit: .
At the lower limit: .
So:
Therefore:
Because is an even function? Actually, is even, but the integral from to of an even function is . Here, that would give , same result. But note: the antiderivative method is foolproof.
- Combine the results. The second term in step 2 is . Adding the first term:
A common mistake is forgetting the factor from the identity, or mis-evaluating at the limits — especially the sign at the lower limit. Always double-check: , so .
The value of the integral is .
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