Antenna Polarization

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.

Theory & Mathematical Formulation

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:

\[ E_x(t,z) = a \cos(\omega t - \beta z) \quad \text{(Horizontal axis)} \] \[ E_y(t,z) = b \cos(\omega t - \beta z + \phi) \quad \text{(Vertical axis)} \]

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:

\[ \left(\frac{E_x}{a}\right)^2 + \left(\frac{E_y}{b}\right)^2 - 2 \frac{E_x E_y}{ab} \cos \phi = \sin^2 \phi \]

This general formula classifies polarization types into:

Interactive Polarization Simulator

Varying amplitudes \(a\), \(b\), and phase difference \(\phi\) changes the polarization trace dynamically.

Value: 1
Value: 1
Value: 0
0π/2π3π/2
The canvas displays the tip of vector \(\mathbf{E}\) evolving over time. The horizontal axis represents \(E_x\) and the vertical axis represents \(E_y\).

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