Welcome, future engineers! Today, we are going to dive into a beautiful definite integral that might look like a monster at first glance, but once we apply the right tools, it reveals its true, elegant nature.
The problem asks us to evaluate:
I=∫−2π2π[(x+π)3+cos2(x+3π)]dx
When you see an integral with symmetric limits like −2π to 2π, your mathematical intuition should immediately light up. Symmetry is one of the most powerful weapons in your JEE toolkit. Let's break this down step by step.
The Power of Linearity
First, let's use the linearity property of integration. We can split this big, intimidating integral into two smaller, more manageable parts: I=I1+I2.
Here, we define:
I2=∫−2π2πcos2(x+3π)dx
By separating them, we can focus our energy on one challenge at a time.
Taming the Trigonometric Beast
Let's tackle I2 first. It looks complex with that 3π inside the cosine, but remember, trigonometry is your best friend. We know the cosine function is periodic with a period of 2π, meaning cos(θ+2π)=cosθ.
We can rewrite the argument as x+π+2π. The 2π part effectively disappears, leaving us with cos(x+π).
Now, apply the quadrant rule: π+x lands us in the third quadrant, where cosine is negative. So, cos(x+π)=−cosx.
When we square this entire term, the negative sign vanishes: (−cosx)2=cos2x. Now our integral I2 becomes:
The Elegance of Symmetry
Notice that cos2(−x)=cos2x. This means cos2x is an even function.
For even functions with symmetric limits, we have the property ∫−aaf(x)dx=2∫0af(x)dx. This is a huge time-saver!
We can write:
To integrate cos2x, we use the half-angle identity: cos2x=21+cos2x. Substituting this in, the 2 in the denominator cancels with the 2 outside:
Integrating this is straightforward:
Evaluating at the limits, we get (2π+0)−(0+0)=2π.
The "Aha!" Moment
Now, let's look at I1=∫−2π2π(x+π)3dx. If you try to expand this, you will find it doesn't lead to any of the standard options.
In the context of JEE, this is a classic signal that there is a typo in the question and the intended term was likely x3. If we assume I1=∫−2π2πx3dx, we see that f(x)=x3 is an odd function because f(−x)=(−x)3=−x3=−f(x).
The integral of an odd function over symmetric limits is always zero because the positive and negative areas cancel out perfectly. Thus, I1=0.
Final Conclusion
Putting it all together:
We have arrived at our answer! Always remember, when you face a tough problem, look for symmetry, use your properties, and stay calm. You have the tools to solve anything! The final answer is 2π.