- Let
I=∫−π/2π/21+exx2cosxdx.
We use the standard symmetry trick by replacing x with −x.
- Define
I=∫−π/2π/21+exx2cosxdx.
Now under x↦−x,
- x2 remains x2,
- cos(−x)=cosx,
- e−x appears in the denominator.
So,
I=∫−π/2π/21+e−xx2cosxdx.
- Add the two expressions for I:
2I=∫−π/2π/2x2cosx(1+ex1+1+e−x1)dx.
Now simplify the bracket:
1+ex1+1+e−x1=1+ex1+1+exex=1.
Hence,
2I=∫−π/2π/2x2cosxdx.
Therefore,
I=21∫−π/2π/2x2cosxdx.
- Since x2cosx is an even function,
I=21⋅2∫0π/2x2cosxdx=∫0π/2x2cosxdx.
So we now evaluate
∫0π/2x2cosxdx.
- Use integration by parts.
Let
u=x2,dv=cosxdx.
Then
du=2xdx,v=sinx.
Thus,
∫x2cosxdx=x2sinx−∫2xsinxdx.
Again apply integration by parts to ∫2xsinxdx:
Let
u=2x,dv=sinxdx,
so
du=2dx,v=−cosx.
Hence,
∫2xsinxdx=−2xcosx+2∫cosxdx=−2xcosx+2sinx.
Therefore,
∫x2cosxdx=x2sinx+2xcosx−2sinx.
- Evaluate from 0 to π/2:
∫0π/2x2cosxdx=[x2sinx+2xcosx−2sinx]0π/2.
At x=π/2,
sin2π=1,cos2π=0,
so value is
4π2(1)+2⋅2π⋅0−2(1)=4π2−2.
At x=0,
02sin0+2⋅0cos0−2sin0=0.
Thus,
I=4π2−2.
- Compare with options:
- A: 4π2−2 ✔
- B: 4π2+2 ✘
- C: π2−eπ/2 ✘
- D: π2+eπ/2 ✘
So the correct option is A.