Animated Solution for Mathematics - Indefinite Integration: For x∈(−2π,2π), if y(x)=∫cscxsecx+tanxsin2xcscx+sinxdx and limx→(2π)−y(x)=0 then y(4π) is equal to
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Visualized Solution
Analyze the Given Integral
Given function: y(x)=∫cscxsecx+tanxsin2xcscx+sinxdx
The Sigma Insight: Evaluation of Special Integral Forms
Analyzing the Setup
My dear student, welcome to the arena. Today, we face a problem that looks like a tangled mess of trigonometric functions. You see cscx, secx, tanx, and sinx all fighting for space in a single fraction.
It is designed to intimidate. But remember, in the world of JEE Advanced, complexity is often just a mask for elegance. Let us peel back that mask together.
The Art of Simplification
We begin with our integrand:
y(x)=∫cscxsecx+tanxsin2xcscx+sinxdx
The first rule of combat is to simplify your terrain. Let us convert everything into the fundamental language of sine and cosine. The numerator, cscx+sinx, becomes sinx1+sinx, which simplifies beautifully to sinx1+sin2x.
Now, look at the denominator: cscxsecx+tanxsin2x. This is sinxcosx1+cosxsinx⋅sin2x, which is sinxcosx1+cosxsin3x.
By taking a common denominator of sinxcosx, we get sinxcosx1+sin4x. When we divide the numerator by the denominator, the sinx terms vanish, and the cosx flips to the top. We are left with the much cleaner integral:
y(x)=∫1+sin4x(1+sin2x)cosxdx
The Power of Substitution
Now, look at that cosxdx sitting there. It is a beacon of hope, as it is the derivative of sinx. This is our cue to perform the substitution t=sinx, which gives us dt=cosxdx.
The integral transforms into:
y=∫1+t41+t2dt
This is a classic form that every JEE aspirant must recognize. To solve it, we divide the numerator and denominator by t2, yielding:
∫t2+1/t21+1/t2dt
The Final Transformation
We are almost there. We need a substitution for the denominator. Let u=t−1/t. Then du=(1+1/t2)dt.
The denominator t2+1/t2 can be rewritten as (t−1/t)2+2, which is u2+2. Our integral is now the standard form:
∫u2+2du
Using the formula ∫x2+a2dx=a1tan−1(ax)+C, we get:
y=21tan−1(2u)+C
Substituting back u=t−1/t and t=sinx, we find:
y(x)=21tan−1(2sinx−1/sinx)+C
The Final Act
We are given that limx→(2π)−y(x)=0. As x→2π, sinx→1, so the argument of the tan−1 becomes zero, forcing C=0.
Finally, we evaluate at x=4π. Since sin(4π)=21, the argument becomes: