We need to find the value of dxdy specifically at x=π.
Let's evaluate the two massive terms one by one.
Remember the trigonometric values: sinπ=0 and cosπ=−1.
Evaluating the First Term
Look at the first term: −sinπ⋅∫…
Since sinπ=0, the entire first term becomes zero!
We don't even need to evaluate the integral.
Calculating the Second Term
Now for the second term: cosπ(1+sin2πcosπ⋅2π)
Substitute the values: (−1)⋅(1+02−1⋅2π)
Final Simplification
Simplify the expression: (−1)⋅(−1)⋅2π
dxdyx=π=2π
Key Takeaway: Always pull out constants before differentiating, and check for zero terms before doing hard calculations!
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The Sigma Insight: Newton-Leibniz & Reduction Formulas
Solution Diagram
The Arena of Calculus
Welcome, student. Today, we stand before a problem that looks like a daunting fortress. At first glance, you see an integral, a trigonometric function, and a variable x lurking in both the limits and the integrand.
It is designed to intimidate. But I want you to take a deep breath. In the world of JEE Advanced, we do not fight monsters with brute force; we dismantle them with elegance.
The Art of Observation
Our function is defined as:
y(x)=∫16π2x21+sin2θcosxcosθdθ
The first thing to notice is the variable of integration: θ. Everything else is just scenery. Look at that cosx in the numerator; it does not depend on θ.
It is completely independent. This is our 'Aha!' moment. We can treat cosx as a constant relative to θ and pull it outside the integral sign.
Suddenly, our function becomes:
y(x)=cosx⋅∫16π2x21+sin2θcosθdθ
We have turned a complex integral into a simple product of two functions, u(x)=cosx and v(x)=∫16π2x21+sin2θcosθdθ.
The Toolbox
Product Rule and Leibniz
Now that we have a product, the path forward is clear. We need the derivative dxdy. We reach for our trusty Product Rule:
dxd[u⋅v]=dxdu⋅v+u⋅dxdv
The first part, dxdu, is easy: the derivative of cosx is −sinx. The second part, dxdv, requires the Newton-Leibniz Rule.
This rule is the secret weapon for differentiating integrals with variable limits. It states:
dxd∫ag(x)f(θ)dθ=f(g(x))⋅g′(x)
We substitute our upper limit g(x)=x2 into the integrand, replacing θ with x2, and then multiply by the derivative of the limit, which is 2x.
Now, we evaluate this at x=π. Here is the beauty of the problem: we know that sinπ=0. The entire first term, which contains that 'scary' integral, vanishes into thin air!
We are left with only the second term:
cosπ(1+sin2πcosπ⋅2π)
Since cosπ=−1 and sinπ=0, this simplifies to (−1)⋅(1+0−1⋅2π).
The final result is 2π. We have conquered the fortress. Remember, in mathematics, the most complex problems often collapse under the weight of a single, elegant observation.