A dipole with charges +/- q near a neutral metallic sheet induces opposite charges on the sheet, resulting in an electric field that has no tangential components and normal components influenced by both the dipole and image charges. The strength of the electric field is strong and directed towards the sheet when the dipole is close, but it diminishes with increasing distance, eventually becoming negligible. The orientation of the dipole affects the direction of the electric field; if parallel to the sheet, the field points towards it, while if perpendicular, it points away. The interaction between the dipole's charges and the induced charges on the sheet is crucial in determining the electric field's behavior. Ultimately, the electric field's characteristics are contingent on both distance and dipole orientation.