Answer: Integral of ln(1+x)/(1+x²) via Feynman Self-Reference
Key Idea / Intuition
The integrand mixes ln(1+x) with 1/(1+x2) in a way that resists direct antidifferentiation. The Feynman trick introduces a parameter t to "scale" the argument of the logarithm, turning the integral into a function of t whose derivative is a rational integral you can evaluate exactly. The final answer combines π and ln2 in a pleasing way — a hallmark of integrals sitting at the intersection of logarithmic and trigonometric worlds.
Formal Proof / Solution
Step 1: Introduce the parameter.
Define
I(t)=∫011+x2ln(1+tx)dx,t∈[0,1].
We want I(1), and clearly I(0)=0.
Step 2: Differentiate under the integral sign.
I′(t)=∫01(1+tx)(1+x2)xdx.
Step 3: Partial fractions.
Decompose:
(1+tx)(1+x2)x=1+txA+1+x2Bx+C.
Multiply through by (1+tx)(1+x2):
x=A(1+x2)+(Bx+C)(1+tx).
Setting x=−1/t: −1/t=A(1+1/t2), so A=1+t2−t.
Comparing x2 terms: 0=A+Bt, so B=1+t21.
Comparing constant terms: 0=A+C, so C=1+t2t.
Thus:
I′(t)=1+t2−t∫011+txdx+1+t21∫011+x2xdx+1+t2t∫011+x2dx.
Step 4: Evaluate each sub-integral.
∫011+txdx=tln(1+t),(t>0)
∫011+x2xdx=2ln2,
∫011+x2dx=4π.
So:
I′(t)=1+t2−t⋅tln(1+t)+1+t21⋅2ln2+1+t2t⋅4π.
=1+t2−ln(1+t)+2(1+t2)ln2+4(1+t2)πt.
Step 5: Integrate from 0 to 1.
I(1)=∫01I′(t)dt=−I(1)+2ln2⋅4π+4π⋅2ln2.
Wait — let's be careful:
∫011+t2−ln(1+t)dt=−I(1)(that’s exactly our original integral!)
∫012(1+t2)ln2dt=2ln2⋅4π=8πln2.
∫014(1+t2)πtdt=4π⋅2ln2=8πln2.
So:
I(1)=−I(1)+8πln2+8πln2.
2I(1)=4πln2.
I=8πln2.
Sanity check: The answer πln2/8≈0.2722 is in (0,1), which matches the integrand being bounded above by ln2≈0.693 on [0,1].