Animated Solution for Mathematics - Indefinite Integration: Let I(x)=∫(xtanx+1)2x2(xsec2x+tanx)dx. If I(0)=0, then I(4π) is equal to
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Visualized Solution
Introduction to the Problem
Given Integral:I(x)=∫(xtanx+1)2x2(xsec2x+tanx)dx
Condition:I(0)=0
Goal: Find I(4π)
Identifying the Derivative Pattern
Let u=xtanx+1
Differentiating with respect to x:
dxdu=dxd(xtanx)+dxd(1)
dxdu=(xsec2x+tanx⋅1)+0
∴du=(xsec2x+tanx)dx
Setting up Integration by Parts
Integration by Parts Formula:∫f⋅gdx=f∫gdx−∫(f′∫gdx)dx
Let f(x)=x2
Let g(x)=(xtanx+1)2xsec2x+tanx
Integrating the Second Function g(x)
∫g(x)dx=∫(xtanx+1)2xsec2x+tanxdx
Using substitution u=xtanx+1, du=(xsec2x+tanx)dx:
∫u2du=−u1=−xtanx+11
Applying the IBP Formula
I(x)=x2(−xtanx+11)−∫2x(−xtanx+11)dx
Simplifying:
I(x)=−xtanx+1x2+2∫xtanx+1xdx
Simplifying the Second Integral
Consider I1=∫xtanx+1xdx
Convert to sine and cosine:
I1=∫xcosxsinx+1xdx=∫xsinx+cosxxcosxdx
Substitution for the Second Integral
Let t=xsinx+cosx
Differentiating:
dt=(xcosx+sinx⋅1−sinx)dx
∴dt=xcosxdx
Integrating the Second Part
I1=∫tdt=ln∣t∣=ln∣xsinx+cosx∣
From Step 4, the second term was 2I1:
2I1=2ln∣xsinx+cosx∣
The Complete Expression for I(x)
I(x)=−xtanx+1x2+2ln∣xsinx+cosx∣+C
Finding the Constant C
Given I(0)=0
0=−0tan0+102+2ln∣0sin0+cos0∣+C
0=0+2ln(1)+C
0=0+0+C⟹C=0
Evaluating at x=4π
I(4π)=−4πtan4π+1(4π)2+2ln∣4πsin4π+cos4π∣
Substitute tan4π=1, sin4π=21, cos4π=21
Simplifying the Algebraic Term
First Term:−4π+116π2=−4π+416π2
=−16π2⋅π+44=−4(π+4)π2
Simplifying the Logarithmic Term
Second Term:2ln∣4π⋅21+21∣
=2ln∣42π+4∣
Using nlnA=lnA2:
=ln∣(42π+4)2∣=ln∣16⋅2(π+4)2∣=ln32(π+4)2
Final Answer and Conclusion
Final Result:I(4π)=ln32(π+4)2−4(π+4)π2
Correct Option: 2
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The Sigma Insight: Integration by Parts
Solution Diagram
The Beauty of the Hidden Pattern
Welcome, fellow explorer of the mathematical universe! Today, we are standing before an integral that, at first glance, looks like a chaotic mess of trigonometric functions and algebraic terms.
We have the following integral:
I(x)=∫(xtanx+1)2x2(xsec2x+tanx)dx
It is easy to feel intimidated by such an expression, but remember: in the world of JEE Advanced, complexity is often just a mask for elegance. Our mission is to peel back that mask.
The Detective Work
Finding the Substitution
Whenever you encounter a complex fraction in an integral, your first instinct should be to investigate the denominator. Let us look at the expression inside the square: u=xtanx+1.
What happens if we differentiate this with respect to x? Using the product rule on xtanx, we get:
dxd(xtanx)=xsec2x+tanx
The derivative of the constant 1 is simply 0. Therefore, dxdu=xsec2x+tanx.
Look at that! The derivative is exactly the term sitting in our numerator. This is not a coincidence; it is the key to the entire problem.
The Strategy
Integration by Parts
With this discovery, we can employ the powerful tool of Integration by Parts. We need to split our integrand into two functions.
We choose f(x)=x2 because it is a polynomial that simplifies beautifully when differentiated. The remaining part, g(x)=(xtanx+1)2xsec2x+tanx, becomes our second function.
We already know how to integrate g(x) because we just found that its numerator is the derivative of the base of its denominator. The integral of u2du is −u1.
Thus, we have:
∫g(x)dx=−xtanx+11
The Transformation
Applying the Integration by Parts formula, ∫f⋅gdx=f∫gdx−∫(f′∫gdx)dx, we get:
I(x)=x2(−xtanx+11)−∫2x(−xtanx+11)dx
The two negative signs cancel out, leaving us with:
I(x)=−xtanx+1x2+2∫xtanx+1xdx
Now, we are left with a new, simpler integral. Let us call it I1=∫xtanx+1xdx.
By converting tanx to cosxsinx and multiplying the numerator and denominator by cosx, we get:
I1=∫xsinx+cosxxcosxdx
If we set t=xsinx+cosx, then dt=(xcosx+sinx−sinx)dx=xcosxdx. The numerator is once again the derivative of the denominator!
This gives us I1=ln∣xsinx+cosx∣.
The Grand Finale
Putting it all together, our indefinite integral is:
I(x)=−xtanx+1x2+2ln∣xsinx+cosx∣+C
We are given I(0)=0. Plugging in x=0, we find that C=0.
Finally, we evaluate at x=4π. Using the values tan4π=1, sin4π=21, and cos4π=21, the expression simplifies to:
ln32(π+4)2−4(π+4)π2
You have successfully navigated the complexity and arrived at the solution. Keep practicing, and remember that every difficult integral is just a puzzle waiting for your insight!