An electric dipole of moment \[p\]is placed at the origin along the \[x\]-axis. The electric field at a point \[P\], whose position vector makes an angle\[\theta \]with the \[x\]-axis, will make an angle ..... with the \[x\]-axis, where \[\tan \alpha =\frac{1}{2}\tan \theta \] [MP PMT 1994]

• A.                    \[\alpha \]
• B.                                      \[\theta \]
• C.                    \[\theta +\alpha \]
• D.                                      \[\theta +2\alpha \]