The boundary condition \(\frac{\partial H_z}{\partial n}=0\) indicates that the magnetic field component \(H_z\) is constant at the waveguide's boundary, meaning there is no magnetic field leakage. This condition arises from the requirement that the magnetic field normal to the surface must be zero, derived from the equation \(n \cdot B = 0\). The discussion references Jackson's equations, specifically Eq. (8.24) and Eq. (8.30), to clarify the derivation of this boundary condition. The resulting magnetic field distribution in a rectangular waveguide is expressed as \(H_z(x,y) \sim \cos(m\pi x/A)\cos(n\pi y/B)\). Understanding these equations is crucial for analyzing wave propagation in cylindrical and rectangular waveguides.