If we recognize a symmetry of sorts around 1, we can try the substitution x = 1/u. This gives us that dx = -1/u2 du:
∫tan-1(x)/x dx = ∫tan-1(1/u)/(1/u) (-1/u2) du = -∫(π/2 - tan-1(u))/u du
Now, if we consider the limits of integration, the last integral is from 2014 to 1/2014, which means we can swap the limits and change the sign. Apologize that this format doesn't give me a clear way of expressing that, but with both definite integrals evaluated over 1/2014 to 2014, we get:
∫tan-1(x)/x dx = ∫(π/2 - tan-1(u))/u du = ∫(π/2u)du - ∫tan-1(u)/u du
∫tan-1(x)/x dx + ∫tan-1(u)/u du = ∫(π/2u)du = π/2 [ln(2014) - ln(1/2014)] = π/2 [2 ln(2014)]
Since the definite integrals on the left are equal, we can add them and divide by 2 to get:
∫tan-1(x)/x dx = π/2 ln(2014) ≈ 11.95
Akasapu K.
01/09/17