0 0 votes The vector $\mathrm{H}$ in the far field of an antenna satisfies $\nabla \cdot \overrightarrow{\mathrm{H}}=0$ and $\nabla \times \overrightarrow{\mathrm{H}}=0$ $\nabla \cdot \overrightarrow{\mathrm{H}} \neq 0$ and $\nabla \times \overrightarrow{\mathrm{H}} \neq 0$ $\nabla \cdot \vec{\text{H}}=0$ and $\nabla \times \vec{\text{H}} \neq 0$ $\nabla \cdot \overrightarrow{\mathrm{H}} \neq 0$ and $\nabla \times \overrightarrow{\mathrm{H}}=0$ Maxwell's Equations gate1998-ec electromagnetics vector-analysis plane-waves-and-properties + – admin 229 views answer comment Share Follow Add Sync Questions Print 0 reply Please log in or register to add a comment.
