A metallic rod of length ‘L’ is rotated with an angular speed of \( '\omega' \) normal to a uniform magnetic field ‘B’ about an axis passing through one end of rod as shown in figure. The induced emf will be:
\( \tfrac{1}{4} B^{2}L\omega \)
\( \tfrac{1}{4} BL^{2}\omega \)
\( \tfrac{1}{2} B^{2}L^{2}\omega \)
\( \tfrac{1}{2} BL^{2}\omega \)