In an irregular shaped charged conductor, the electric field inside is always zero in a static situation, as the charges redistribute themselves to cancel any internal electric field. This occurs because, without an external electric field, the net charge at each point within the conductor remains zero, despite local charge displacement. When external fields are present, the charges move to the surface, ensuring that the internal electric field remains null. The distribution of surface charges is specifically arranged to prevent any electric field from penetrating the conductor. This principle holds true only in static conditions.