Substitute u=lnx. As x→+∞ we have u→+∞, so the limit becomes
L=limu→+∞u(tan−1u−2π).
This is an ∞⋅0 indeterminate form, since tan−1u→2π.
Use the complementary-angle identity. For u>0,
tan−1u+tan−1u1=2π⟹tan−1u−2π=−tan−1u1.
Therefore
L=limu→+∞u(−tan−1u1)=−limu→+∞1/utan−1(1/u).
Put t=u1→0+. Using the standard limit ttan−1t→1,
L=−limt→0+ttan−1t=−1.
Cross-check via L'Hôpital. Writing L=limu→∞1/utan−1u−π/2 (form 00) and differentiating,
L=limu→∞−u211+u21=limu→∞1+u2−u2=−1.
So the value is −1, which is option 3.
Exam trick: For u>0, tan−1u−2π=−tan−1(1/u)≈−u1 as u→∞; multiplying by u instantly gives −1 without any differentiation.