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The electric field changes when crossing a boundary between two different media because the field components above and below the surface differ. Using a Gaussian pillbox at the boundary and applying Gauss's law, the normal component of the electric field exhibits a discontinuity proportional to the surface charge density. This discontinuity arises from the change in the medium's properties affecting how the field propagates.

The normal component of the electric field is discontinuous across a boundary. By applying Gauss's law to a thin pillbox positioned at the surface, the surface integral contributions from only the top and bottom faces remain as thickness approaches zero. This yields the discontinuity of the normal component, which depends on the surface charge density at the boundary.

Yes, the tangential component of the electric field is always continuous across any boundary. Using a thin loop on the boundary surface, the line integral of the electric field around the closed path equals zero. When loop thickness approaches zero, contributions from the sides vanish, leaving only the tangential components, which must be equal on both sides of the boundary.

Electric potential is continuous across any boundary between two media. Since the electric field is the negative gradient of potential, the line integral of the field from below to above the boundary tends to zero. This mathematical relationship ensures that potential values remain the same on both sides of the surface boundary, maintaining continuity despite field discontinuities.

The normal component of the electric field is discontinuous at a boundary, while the tangential component remains continuous. Together, these conditions define the complete field behavior at the interface. By combining both component equations and defining a unit vector perpendicular to the surface, the total electric field at the boundary can be fully characterized, describing how the field transitions between two media.

Gauss's law in integral form relates the surface integral of the electric field to enclosed charge. Applying this law to a Gaussian pillbox positioned at a boundary shows that as thickness approaches zero, only the faces parallel to the boundary contribute. This geometric approach directly yields the discontinuity of the normal component, quantifying how much the field changes across the surface.

The tangential component remains unchanged because the line integral of the electric field around any closed loop equals zero. Applying this principle to a thin rectangular loop at the boundary and taking the limit as thickness approaches zero eliminates contributions from the loop sides. Only the tangential components along the boundary remain, and they must be equal on both sides to satisfy this fundamental electrostatic condition.