The de-Broglie wavelength \( \lambda \) for an electron in an orbit of radius \( r_n \) is given by:
\[
\lambda = \frac{h}{mv}
\]
For the electron in the second orbit of hydrogen, the radius \( r_n \) is proportional to \( n^2 \), and using Bohr's model, the wavelength for the second orbit \( n = 2 \) is given by:
\[
\lambda = \frac{4 \pi a_0}{n}
\]
Thus, the correct answer is \( \frac{4 \pi a_0}{n} \).