Let the given integral be I.
I = \int_\limits0^\pi \frac{x^2 \sin x \cos x}{\sin ^4 x+\cos ^4 x} d x
Step 1: Apply the King's Property.
We use the property ∫0af(x)dx=∫0af(a−x)dx. Here, a=π.
Let f(x)=sin4x+cos4xx2sinxcosx.
Then f(π−x)=sin4(π−x)+cos4(π−x)(π−x)2sin(π−x)cos(π−x).
We know that sin(π−x)=sinx and cos(π−x)=−cosx.
So, sin(π−x)cos(π−x)=(sinx)(−cosx)=−sinxcosx.
And sin4(π−x)=(sinx)4=sin4x, and cos4(π−x)=(−cosx)4=cos4x.
Therefore, f(π−x)=sin4x+cos4x(π−x)2(−sinxcosx).
Applying the King's property:
I=∫0πsin4(π−x)+cos4(π−x)(π−x)2sin(π−x)cos(π−x)dx=∫0πsin4x+cos4x(π−x)2(−sinxcosx)dx
So, we have two expressions for I:
I=∫0πsin4x+cos4xx2sinxcosxdx(∗)I=∫0πsin4x+cos4x(π−x)2(−sinxcosx)dx(∗∗)
Step 2: Add the two expressions for I.
Adding (**) to (*):
2I=∫0πsin4x+cos4xx2sinxcosxdx+∫0πsin4x+cos4x(π−x)2(−sinxcosx)dx2I=∫0πsin4x+cos4x[x2−(π−x)2]sinxcosxdx
Simplify the term x2−(π−x)2:
x2−(π−x)2=x2−(π2−2πx+x2)=x2−π2+2πx−x2=2πx−π2=π(2x−π).
So,
2I=∫0πsin4x+cos4xπ(2x−π)sinxcosxdx2I=π∫0πsin4x+cos4x(2x−π)sinxcosxdx
Step 3: Consider the integral ∫0πg(x)dx where g(x)=sin4x+cos4x(2x−π)sinxcosx.
Let's check the property g(π−x)=−g(x).
We already found that sin(π−x)cos(π−x)=−sinxcosx.
And sin4(π−x)+cos4(π−x)=sin4x+cos4x.
The term (2x−π) becomes (2(π−x)−π)=(2π−2x−π)=π−2x=−(2x−π).
So, g(π−x)=sin4(π−x)+cos4(π−x)(2(π−x)−π)sin(π−x)cos(π−x)g(π−x)=sin4x+cos4x−(2x−π)(−sinxcosx)=sin4x+cos4x(2x−π)sinxcosx=g(x).
This is not −g(x). Let's re-examine the addition of I and the modified I.
Let's go back to 2I=∫0πsin4x+cos4x[x2−(π−x)2]sinxcosxdx.
2I=∫0πsin4x+cos4x(2πx−π2)sinxcosxdx2I=∫0πsin4x+cos4x2πxsinxcosxdx−∫0πsin4x+cos4xπ2sinxcosxdx
Let I1=∫0πsin4x+cos4x2πxsinxcosxdx and I2=∫0πsin4x+cos4xπ2sinxcosxdx.
So, 2I=I1−I2.
For I1: Let h(x)=sin4x+cos4x2πxsinxcosx.
h(π−x)=sin4(π−x)+cos4(π−x)2π(π−x)sin(π−x)cos(π−x)h(π−x)=sin4x+cos4x2π(π−x)(−sinxcosx)=sin4x+cos4x−2π(π−x)sinxcosx.
So, I1=∫0πh(x)dx.
Also, I1=∫0πh(π−x)dx=∫0πsin4x+cos4x−2π(π−x)sinxcosxdx.
Adding the two forms of I1:
2I1=∫0πsin4x+cos4x2πxsinxcosxdx+∫0πsin4x+cos4x−2π(π−x)sinxcosxdx2I1=∫0πsin4x+cos4x[2πx−2π(π−x)]sinxcosxdx2I1=∫0πsin4x+cos4x(2πx−2π2+2πx)sinxcosxdx2I1=∫0πsin4x+cos4x(4πx−2π2)sinxcosxdx. This is not simplifying as expected.
Let's use a different approach for the integral I = \int_\limits0^\pi \frac{x^2 \sin x \cos x}{\sin ^4 x+\cos ^4 x} d x.
We can rewrite the denominator:
sin4x+cos4x=(sin2x+cos2x)2−2sin2xcos2x=1−21(2sinxcosx)2=1−21sin2(2x).
The numerator is x2sinxcosx=x22sin(2x).
So, I=∫0π1−21sin2(2x)x22sin(2x)dx=∫0π2−sin2(2x)x2sin(2x)dx.
Now, let's use the property ∫02af(x)dx=∫02af(2a−x)dx.
Here, the integral is from 0 to π. Let's consider the interval [0,2π] and then use symmetry.
However, the integrand is defined on [0,π].
Let's go back to the property ∫0af(x)dx=∫0af(a−x)dx.
I=∫0πsin4x+cos4xx2sinxcosxdx.
Let f(x)=sin4x+cos4xx2sinxcosx.
f(π−x)=sin4(π−x)+cos4(π−x)(π−x)2sin(π−x)cos(π−x)=sin4x+cos4x(π−x)2(−sinxcosx).
I=∫0πf(π−x)dx=∫0πsin4x+cos4x(π−x)2(−sinxcosx)dx.
2I=∫0πsin4x+cos4xx2sinxcosx−(π−x)2sinxcosxdx2I=∫0πsin4x+cos4x(x2−(π−x)2)sinxcosxdx2I=∫0πsin4x+cos4x(2πx−π2)sinxcosxdx2I=∫0πsin4x+cos4x2πxsinxcosxdx−π2∫0πsin4x+cos4xsinxcosxdx.
Let J=∫0πsin4x+cos4xsinxcosxdx.
Let's consider the integrand g(x)=sin4x+cos4xsinxcosx.
g(π−x)=sin4(π−x)+cos4(π−x)sin(π−x)cos(π−x)=sin4x+cos4x(sinx)(−cosx)=−g(x).
For an integral ∫02af(x)dx, if f(2a−x)=−f(x), then the integral is 0.
Here, the integral is from 0 to π. Let's consider 2a=π, so a=π/2.
Let's consider the integral from 0 to π.
The property is: if f(π−x)=−f(x), then ∫0πf(x)dx=0.
Here, g(π−x)=−g(x), so J=∫0πsin4x+cos4xsinxcosxdx=0.
Now consider the first part of 2I: ∫0πsin4x+cos4x2πxsinxcosxdx.
Let k(x)=sin4x+cos4x2πxsinxcosx.
k(π−x)=sin4(π−x)+cos4(π−x)2π(π−x)sin(π−x)cos(π−x)=sin4x+cos4x2π(π−x)(−sinxcosx).
Let I′=∫0πsin4x+cos4x2πxsinxcosxdx.
I′=∫0πk(π−x)dx=∫0πsin4x+cos4x2π(π−x)(−sinxcosx)dx.
2I′=∫0πsin4x+cos4x2πxsinxcosxdx+∫0πsin4x+cos4x−2π(π−x)sinxcosxdx2I′=∫0πsin4x+cos4x[2πx−2π(π−x)]sinxcosxdx2I′=∫0πsin4x+cos4x(2πx−2π2+2πx)sinxcosxdx2I′=∫0πsin4x+cos4x(4πx−2π2)sinxcosxdx. This is still not simplifying to zero easily.
Let's use the property ∫02af(x)dx=a∫02f(x)dx if f(2a−x)=f(x).
And ∫02af(x)dx=0 if f(2a−x)=−f(x).
Let's go back to 2I=∫0πsin4x+cos4x(2πx−π2)sinxcosxdx.
Let h(x)=sin4x+cos4x(2πx−π2)sinxcosx.
We found that h(π−x)=sin4x+cos4x(2π(π−x)−π2)(−sinxcosx)=sin4x+cos4x(2π2−2πx−π2)(−sinxcosx)=sin4x+cos4x(π2−2πx)(−sinxcosx)=sin4x+cos4x−(2πx−π2)(−sinxcosx)=sin4x+cos4x(2πx−π2)sinxcosx=h(x).
So, for the integral ∫0πh(x)dx, we have h(π−x)=h(x).
This means ∫0πh(x)dx=2∫0π/2h(x)dx.
This does not directly lead to zero.
Let's reconsider the initial integral I = \int_\limits0^\pi \frac{x^2 \sin x \cos x}{\sin ^4 x+\cos ^4 x} d x.
Let u=sin2x. Then du=2sinxcosxdx.
When x=0, u=0. When x=π, u=0. This substitution won't work directly because the limits become the same.
Let's use the property ∫02af(x)dx=∫02af(2a−x)dx.
Let's consider the integrand F(x)=sin4x+cos4xx2sinxcosx.
We need to evaluate π3120I.
Let's consider the integral ∫0πxsin4x+cos4xsinxcosxdx.
Let g(x)=sin4x+cos4xsinxcosx. We know g(π−x)=−g(x).
So, ∫0πxg(x)dx.
Let Ix=∫0πxg(x)dx.
Ix=∫0π(π−x)g(π−x)dx=∫0π(π−x)(−g(x))dx=−∫0π(π−x)g(x)dx.
Ix=−π∫0πg(x)dx+∫0πxg(x)dx.
Since ∫0πg(x)dx=0, we have Ix=Ix. This doesn't help.
Let's go back to 2I=∫0πsin4x+cos4x(2πx−π2)sinxcosxdx.
Let u=tanx. Then du=sec2xdx. This is not suitable.
Consider the substitution t=tanx.
sin2x=1+t2t2, cos2x=1+t21.
sin4x+cos4x=(1+t2t2)2+(1+t21)2=(1+t2)2t4+1.
sinxcosx=1+t2t.
When x goes from 0 to π, t goes from 0 to ∞ and then from −∞ to 0. This is problematic.
Let's split the integral: I=∫0π/2sin4x+cos4xx2sinxcosxdx+∫π/2πsin4x+cos4xx2sinxcosxdx.
In the second integral, let x=π−y. Then dx=−dy.
When x=π/2, y=π/2. When x=π, y=0.
∫π/2πsin4x+cos4xx2sinxcosxdx=∫π/20sin4(π−y)+cos4(π−y)(π−y)2sin(π−y)cos(π−y)(−dy)=∫0π/2sin4y+cos4y(π−y)2(−sinycosy)dy=−∫0π/2sin4y+cos4y(π−y)2sinycosydy.
So, I=∫0π/2sin4x+cos4xx2sinxcosxdx−∫0π/2sin4x+cos4x(π−x)2sinxcosxdx.
I=∫0π/2sin4x+cos4x[x2−(π−x)2]sinxcosxdx.
I=∫0π/2sin4x+cos4x(2πx−π2)sinxcosxdx.
Let u=tanx. Then du=sec2xdx.
sinxcosx=sec2xtanx=1+u2u.
sin4x+cos4x=(1+u2)2u4+1.
sinxcosxdx=1+u2usec2xdu=1+u2u1+u2du=(1+u2)2udu.
When x=0, u=0. When x=π/2, u→∞.
I=∫0∞(1+u2)2u4+1(2πarctanu−π2)(1+u2)2uduI=∫0∞(2πarctanu−π2)u4+1udu.
I=2π∫0∞u4+1uarctanudu−π2∫0∞u4+1udu.
Consider the integral ∫0∞u4+1udu.
Let v=u2, dv=2udu.
∫0∞v2+112dv=21[arctanv]0∞=21(2π−0)=4π.
So, π2∫0∞u4+1udu=π24π=4π3.
Now consider 2π∫0∞u4+1uarctanudu.
Let's examine the original integral.
If we consider the integrand F(x)=sin4x+cos4xx2sinxcosx.
Let's check the property F(π−x)=−F(x) for the entire interval [0,π].
F(π−x)=sin4(π−x)+cos4(π−x)(π−x)2sin(π−x)cos(π−x)=sin4x+cos4x(π−x)2(−sinxcosx).
This is not −F(x).
Let's consider the integral I=∫0πsin4x+cos4xx2sinxcosxdx.
Let's observe the symmetry around x=π/2.
Let x=π/2+t. Then dx=dt.
When x=0, t=−π/2. When x=π, t=π/2.
I=∫−π/2π/2sin4(π/2+t)+cos4(π/2+t)(π/2+t)2sin(π/2+t)cos(π/2+t)dt.
sin(π/2+t)=cost.
cos(π/2+t)=−sint.
sin4(π/2+t)=cos4t.
cos4(π/2+t)=sin4t.
So, the integral becomes:
I=∫−π/2π/2cos4t+sin4t(π/2+t)2(cost)(−sint)dt.
I=−∫−π/2π/2cos4t+sin4t(π/2+t)2sintcostdt.
Let g(t)=cos4t+sin4tsintcost. This is an odd function of t because sin(−t)cos(−t)=(−sint)(cost)=−sintcost, and cos4(−t)+sin4(−t)=cos4t+sin4t.
So, ∫−π/2π/2g(t)dt=0.
The second integral ∫−π/2π/2cos4t+sin4tπtsintcostdt=0 because the integrand is an odd function of t.
The first integral ∫−π/2π/2cos4t+sin4t(π/2)2sintcostdt. Let G(t)=cos4t+sin4tsintcost. G(−t)=−G(t), so G(t) is odd.
Thus, ∫−π/2π/2G(t)dt=0.
Therefore, the first integral is 0.
Now consider the third integral: −∫−π/2π/2cos4t+sin4tt2sintcostdt.
Let H(t)=cos4t+sin4tt2sintcost.
H(−t)=cos4(−t)+sin4(−t)(−t)2sin(−t)cos(−t)=cos4t+sin4tt2(−sint)(cost)=−cos4t+sin4tt2sintcost=−H(t).
So, the third integral is also 0.
Thus, I=0.
The expression we need to evaluate is π3120I.
Since I=0, the value is π3120×0=0.
Common Mistakes & Tips
Be careful when applying the King's property ∫0af(x)dx=∫0af(a−x)dx and the property ∫02af(x)dx=0 if f(2a−x)=−f(x). Ensure the conditions are met for the correct integral limits.
Symmetry arguments are powerful. Splitting the integral interval or using substitutions like x=a+t can reveal useful symmetries.
When dealing with trigonometric integrands, simplifying the denominator using identities like sin4x+cos4x=1−21sin2(2x) can be helpful.
Summary
The problem involves evaluating a definite integral with trigonometric functions. We used the property of definite integrals related to symmetry around the midpoint of the integration interval. By substituting x=π/2+t, we transformed the integral from [0,π] to [−π/2,π/2]. The resulting integrand was analyzed for its symmetry properties. We found that the integral could be broken down into components, each of which evaluated to zero due to the integrand being an odd function over a symmetric interval. Consequently, the value of the integral I is 0, making the final expression also 0.