Читать книгу Introduction To Modern Planar Transmission Lines - Anand K. Verma - Страница 208

If medium #2 is a perfect conductor, . The medium #1 supports the wave with interference, and the fields are written from equation (5.2.17) as follows:

(5.2.19)

In equation (5.2.19), time‐harmonic dependence e^jωt is suppressed. At the surface of the perfect conductor x = 0, the field component forms the standing wave. However, the standing wave pattern travels along the interface in the y‐direction.