Write the general term using lnn+2n=lnn−ln(n+2), so
an=(−1)n(lnn−ln(n+2)).
The series is alternating, lnn+2n→0 monotonically, so by the Leibniz test it converges. To find the sum, compute the partial sum SN for even N by tracking the coefficient of each lnk.
The lnn part gives ∑n=1N(−1)nlnn, and the −ln(n+2) part gives
−∑n=1N(−1)nln(n+2)=−∑m=3N+2(−1)mlnm.
The shared range m=3,…,N cancels (interior terms telescope), leaving only the boundary:
For even N the boundary term is ln(N+1)−ln(N+2)=lnN+2N+1, hence
SN=ln2+lnN+2N+1.
Letting N→∞, lnN+2N+1→ln1=0, so
∑n=1∞(−1)nlnn+2n=ln2.
The answer is option 4.
Exam trick: Split lnn+2n into lnn−ln(n+2) and note every interior lnk cancels — only the first two and last two terms of the partial sum survive, so the limit is read off the boundary alone.