Analyzing the Setup
We begin by defining our integral as:
I=∫−2π2π1+πsinx1+sin2xdx
The moment you see symmetric limits from −2π to 2π, your mathematical spider-sense should tingle. This is the hallmark of the King's Property, one of the most powerful tools in your arsenal.
The property states that:
∫abf(x)dx=∫abf(a+b−x)dx
In our case, a=−2π and b=2π, so a+b=0. This means we are simply replacing x with −x.
The Transformation
When we substitute x→−x, our integral becomes:
I=∫−2π2π1+πsin(−x)1+sin2(−x)dx
Recall your trigonometry: sin(−x)=−sinx, and because of the square, sin2(−x)=sin2x. The numerator remains unchanged, but the denominator becomes 1+π−sinx.
Since π−sinx=πsinx1, we can simplify the denominator to πsinxπsinx+1. Flipping the fraction, our new integral becomes:
I=∫−2π2ππsinx+1πsinx(1+sin2x)dx
The Master Equation
Now, we add our two expressions for I together:
2I=∫−2π2π(1+πsinx1+sin2x+1+πsinxπsinx(1+sin2x))dx
Notice that both terms share the same denominator. Combining the numerators and factoring out (1+sin2x), we get:
2I=∫−2π2π1+πsinx(1+sin2x)(1+πsinx)dx
The exponential terms cancel out perfectly, leaving us with:
Final Calculation
Since 1+sin2x is an even function, we use the symmetry property ∫−aaf(x)dx=2∫0af(x)dx:
2I=2∫02π(1+sin2x)dx⇒I=∫02π(1+sin2x)dx
Using the identity sin2x=21−cos2x, we substitute:
I=∫02π(1+21−cos2x)dx=∫02π(23−21cos2x)dx
Integrating term by term, we evaluate:
Plugging in the limits, the upper limit yields 23(2π)−41sin(π)=43π−0. The lower limit is 0.
The final answer is 43π.