This page explores the concept of antenna polarization, describing how the orientation of the electric field vector of a radiated wave behaves over time. Review foundational equations and use the interactive simulator below to test linear, circular, and elliptical polarizations in real-time.
The polarization of an antenna describes the orientation of the electric field of the wave it radiates. For a given position along the propagation axis \(z\), the electric field vector \(\mathbf{E}\) has components along the axes of the diagram:
Here \(a\) and \(b\) represent amplitudes, \(\phi\) is the phase difference between components, \(\omega\) is the angular frequency, and \(\beta = \dfrac{2\pi}{\lambda}\) is the propagation constant.
The tip of the electric field vector \(\mathbf{E}(t) = (E_x, E_y)\) traces a curve in the \(xy\)-plane. Trigonometric derivation yields the standard curve equation:
This general formula classifies polarization types into:
Varying amplitudes \(a\), \(b\), and phase difference \(\phi\) changes the polarization trace dynamically.