An electron projected perpendicular to a uniform magnetic field \( B \) moves in a circle. If Bohr's quantization is applicable, then the radius of the electronic orbit in the first excited state is:
\( \displaystyle\sqrt{\frac{h}{\pi e B}} \)
\( \displaystyle\sqrt{\frac{h}{2\pi e B}} \)
\( \displaystyle\sqrt{\frac{4h}{\pi e B}} \)
\(\displaystyle \sqrt{\frac{2h}{\pi e B}} \)