0 0 votes The electric field component of a uniform plane electromagnetic wave propagating in the $Y$-direction in a lossless medium will satisfy the equation. $\frac{\partial^2 E_y}{\partial y^2}=\mu \in \frac{\partial^2 E_y}{\partial t^2}$ $\frac{\partial^2 E_y}{\partial x^2}=\mu \in \frac{\partial^2 E_y}{\partial t^2}$ $\frac{\partial^2 E_x}{\partial y^2}=\mu \in \frac{\partial^2 E_x}{\partial t^2}$ $\frac{\sqrt{E_x^2+E_z^2}}{\sqrt{H_x^2+H_z^2}}=\sqrt{\frac{\mu}{\epsilon}}$ Maxwell's Equations gate1991-ec plane-waves-and-properties electromagnetics + – admin 399 views answer comment Share Follow Add Sync Questions Print 0 reply Please log in or register to add a comment.
