Measurement Techniques

Co-Pol Pattern

/koh-pohl pat-urn/
The co-pol pattern shows antenna gain in the intended polarization direction, defined by Ludwig's third definition (1973). A Huygens source reference at each observation point determines co-pol and cross-pol components. Well-designed antennas achieve cross-pol 20 to 40 dB below co-pol peak in the main beam. Specifications require cross-pol < -25 dB within the 3 dB beamwidth for dual-polarized systems using 256-QAM or higher modulation.
Category: Measurement Techniques
Cross-pol ratio: 20 to 40 dB
Standard: Ludwig-3 definition

Understanding Co-Pol Patterns

Every antenna radiates electromagnetic fields with both intended and unintended polarization components. A vertically polarized antenna, for example, radiates a dominant vertical E-field (the co-pol component) along with a smaller horizontal E-field (the cross-pol component) that arises from design imperfections, feed asymmetry, and edge diffraction. The co-pol pattern plots the intended component versus observation angle, revealing the main beam shape, sidelobes, and nulls that determine the antenna's performance in its designated polarization. The cross-pol pattern, measured simultaneously, reveals polarization purity as a function of angle.

Ludwig's third definition provides the standard mathematical framework for separating co-pol and cross-pol in measured data. Unlike simpler definitions that use fixed coordinate axes (Ludwig-1) or spherical unit vectors (Ludwig-2), Ludwig-3 defines co-pol and cross-pol relative to a reference antenna (Huygens source) at each observation point. This matches the physical measurement process where a calibrated probe antenna is rotated to measure each polarization component. The resulting co-pol pattern is smooth and well-defined across the full hemisphere, while cross-pol shows characteristic nulls along the principal planes (E-plane and H-plane) and peaks in the diagonal (45°) planes where the field decomposition is most sensitive to asymmetry.

Co-Pol Pattern Equations

Ludwig-3 Co-Polarization:
Eco = Eθ cosφ - Eφ sinφ

Ludwig-3 Cross-Polarization:
Ecross = Eθ sinφ + Eφ cosφ

Cross-Polar Discrimination:
XPD = 20 log(|Eco| / |Ecross|)   (dB)

Where Eθ, Eφ = spherical field components, φ = azimuthal angle. In E-plane (φ=0): Eco=Eθ, Ecross=Eφ. In H-plane (φ=90°): Eco=-Eφ, Ecross=Eθ. In 45° plane: both components mix.

Co-Pol Specifications by Application

ApplicationCo-Pol SidelobesCross-Pol (main beam)Measurement MethodStandard
SATCOM earth station< -14 dB (29-25logθ)< -25 dBFar-field rangeITU-R S.580
Dual-pol microwave< -20 dB< -30 dBCompact rangeETSI EN 302 217
Weather radar< -25 dB< -35 dB (boresight)Near-field scanWMO No. 8
5G base station< -15 dB< -20 dBOTA chamber3GPP 38.141
Automotive radar< -15 dBNot specifiedCompact rangeETSI EN 301 091
Common Questions

Frequently Asked Questions

What is Ludwig-3 co-polarization?

Ludwig-3 (1973) defines co-pol as the component received by a Huygens source at each observation point maximized for the AUT's polarization. Eco = Eθcosφ - Eφsinφ. In principal planes, co-pol equals Eθ (E-plane) or -Eφ (H-plane). Cross-pol peaks in 45° planes where both components mix.

Why does cross-pol matter?

In CCDP links, antenna cross-pol limits XPD and requires XPIC for >256-QAM. Co-pol to cross-pol must exceed 25 to 30 dB at boresight. In polarimetric radar, cross-pol degrades weather classification. In satellite systems, it couples into orthogonal transponders. Specs require cross-pol < -25 dB within the 3 dB beamwidth.

How is the co-pol pattern measured?

AUT rotates on positioner in anechoic chamber; source transmits known polarization. Power vs angle gives co-pol cut. Source rotated 90° for cross-pol. Near-field scanning (planar/cylindrical/spherical) preferred for large antennas where far-field distance (2D²/λ) is impractical. Accuracy needs: reflections < -40 dB, positioner < 0.1°.

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