Analyzing the Setup
The integral provided is:
I=∫−π/2π/2sin4x(1+log(2−sinx2+sinx))dx
When you encounter limits of the form [−2π,2π], your mathematical intuition should immediately signal to check for symmetry. This is the key to unlocking the problem efficiently.
The Divide and Conquer Strategy
We start by splitting this intimidating integral into two manageable pieces. Let I=I1+I2, where:
I2=∫−π/2π/2sin4xlog(2−sinx2+sinx)dx
By separating the terms, we have effectively isolated the complex logarithmic component from the simpler trigonometric power.
The Parity Investigation
Now, let us focus on I2. We define the integrand as f2(x)=sin4xlog(2−sinx2+sinx).
To check for parity, we evaluate
f2(−x):
f2(−x)=sin4(−x)log(2−sin(−x)2+sin(−x))
Since
sin(−x)=−sinx and the power of four makes the sine term positive, we obtain:
f2(−x)=sin4xlog(2+sinx2−sinx)
Notice that 2+sinx2−sinx is the reciprocal of 2−sinx2+sinx. Using the property log(ba)=−log(ab), we find that f2(−x)=−f2(x).
This confirms that f2(x) is an odd function. The integral of an odd function over a symmetric interval [−a,a] is always zero, as the area above the x-axis perfectly cancels the area below it. Thus, I2=0.
The Wallis Formula
We are left with I=I1=∫−π/2π/2sin4xdx. Since sin4x is an even function, we apply the property ∫−aaf(x)dx=2∫0af(x)dx:
Now, we apply the
Wallis Formula for
∫0π/2sinnxdx with
n=4:
∫0π/2sin4xdx=43⋅21⋅2π=163π
Final Calculation
Finally, multiplying by the factor of two we extracted earlier:
I=2⋅163π=83π
The final result is 83π. A seemingly impossible integral has been solved with elegance and symmetry.