In a perfect conductor, both electric and magnetic fields vanish due to the movement of surface charges in response to time-varying fields, as outlined in John David Jackson's "Classical Electrodynamics." This principle is foundational in waveguide theory, where the magnetic field must be parallel to the boundary, preventing a normal component. While superconductors exhibit the Meissner effect, expelling magnetic fields entirely, this behavior requires additional conditions on Maxwell's Equations that do not apply to theoretical perfect conductors. In static conditions, a magnetic field can exist in a perfect conductor, but this scenario is considered ill-posed in practical terms. The discussion highlights the complexities of electromagnetic fields in both ideal and real-world scenarios, emphasizing the differences between perfect conductors and superconductors.