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Skaha-Drone
Skaha-Drone
  • Introduction: Digital L-Band (1.4 GHz) Polarimeter for UAVs
  • Microwave Polarimetry
    • Radio Wave Polarization
  • Technical Description
    • Mounting Options
    • Antenna
    • Control Unit
    • RF Signal Chain
    • A/D Converter and Digital Correlator
    • Receiver Noise Temperature
    • Internal Calibration
    • Radio Interference Filter
  • Ground Station and User Interface
    • Ground Station
    • Labels and Tags
    • Status
    • Settings
    • Rawdata
    • Map
    • Internal
  • Online Processing
    • Introduction
    • Sanity Check and Filtering
    • Gain Calibration
    • Conversion to Volumetric Water Content
    • Data Storage in Google Drive
  • Working with the Sensor and Data
    • HDF5 File Structure
    • Python Scripts
    • Test Observations
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On this page
  • Monochromatic Waves
  • Stokes Parameters
  • Partial Polarization
  • Polarization Measurements
  1. Microwave Polarimetry

Radio Wave Polarization

Here is a simplified explanation of polarization and Stokes parameters.

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Last updated 1 year ago

A single electromagnetic wave can be thought of as an oscillating electric and magnetic field. The direction in which the electric field oscillates is the polarization direction. The polarization angle can have values between 0 and 180 degrees.

Monochromatic Waves

The electric field of a harmonic, monochromatic plane wave at a fixed location in space can be described by electric field components in the x- and y-directions:

The electric field vector of arbitrary polarization then reads:

In general, the imaginary part of the analytic signal does not physically exist. Also, whenever nonlinear operations are applied to the electric field vector such as squaring, etc., the real parts must be taken first and the operation is applied to these alone. This, however, is not necessary if the time average of a quadratic expression is required.

Stokes Parameters

Stokes I is the total power signal received through both hands of polarization. Stokes Q and U are the two (x and y) components of the linearly polarized fraction of the signal, and Stokes V represents the circularly polarized component.

The amplitude (polarized intensity PI) of the polarized component can be calculated as follows:

and the polarization angle PA of the linearly polarized component:

The fractional (percentage) polarization PP is given by:

Partial Polarization

A single electromagnetic wave is fully polarized. In nature, however, electromagnetic radiation is produced by a large ensemble of radiators, producing incoherent waves. Incoherent radiation may still show a statistical correlation between the polarization components. This can be interpreted as partial polarization. Stokes parameters are then given by time averages:

Polarization Measurements

A polarimeter does not measure the amplitudes and phase differences of the polarization components directly; it rather detects time-averaged products of the two components, such as, for example, the following product of the x- and y-components:

With

and hence a measure for Stokes U. Using the analytic representation, this equation can be written as:

Time averaging the other possible products gives other Stokes parameters, which leads to the following variant of the definition of Stokes parameters:

In the following text, δ\deltaδ refers to the phases of electric field vectors and ϕ\phiϕ to their polarization angle. EEE denotes an electric field and VVV the voltage of this field.

Ex(t)=A1 eiωtE_x(t) = A_1\,e^{i\omega t}Ex​(t)=A1​eiωt and

Ey(t)=A2 eiωt,E_y(t) = A_2\,e^{i\omega t},Ey​(t)=A2​eiωt,

which are two linearly polarized waves with orthogonal polarization directions and the circular frequency ω\omegaω. The complex amplitudes A1A_1A1​ and A2A_2A2​ are A1=a1eiδ1A_1 = a_1 e^{i\delta_1}A1​=a1​eiδ1​ and A2=a2eiδ2A_2 = a_2 e^{i\delta_2}A2​=a2​eiδ2​, with the real amplitudes a1a_1a1​ and a2a_2a2​ and phases δ1\delta_1δ1​ and δ2\delta_2δ2​. The absolute phases of A1A_1A1​ and A2A_2A2​ are not important; only the relative phase δ=δ2−δ1\delta = \delta_2 − \delta_1δ=δ2​−δ1​ matters so that:

A1=a1A_1 = a_1A1​=a1​ and

A2=a2 eiδA_2 = a_2\,e^{i\delta}A2​=a2​eiδ.

E(t)=(A1A2) eiωt=(a1ex+a2eyeiδ)eiωt\mathbf{E}(t) = \binom{A_1}{A_2}\,e^{i\omega t} = \left(a_1 \mathbf{e}_x + a_2 \mathbf{e}_y e^{i\delta}\right) e^{i\omega t}E(t)=(A2​A1​​)eiωt=(a1​ex​+a2​ey​eiδ)eiωt

in which ex\mathbf{e}_xex​ and ey\mathbf{e}_yey​ are unit vectors of a Cartesian coordinate system.

The electric field vector E(t)\mathbf{E}(t)E(t) is a complex number. It is understood that this is the analytic representation of a plane harmonic wave. To obtain a physically meaningful quantity, for instance the voltage V(t) within the radio receiver, one has to take the real part of the above equation:

V(t)=Re[(Axex+Ayey)eiωt]V(t) = \mathfrak{Re}\left[\left(A_x \mathbf{e}_x + A_y \mathbf{e}_y \right) e^{i\omega t} \right]V(t)=Re[(Ax​ex​+Ay​ey​)eiωt].

The polarization or position angle ϕ\phiϕ of the electric field vector is defined by:

tan⁡ϕ=ExEy=a2a1\tan\phi = \frac{E_x}{E_y} = \frac{a_2}{a_1}tanϕ=Ey​Ex​​=a1​a2​​.

With the amplitudes a1a_1a1​ and a2a_2a2​ expressed by the amplitude a0a_0a0​ of the initial wave and the polarization angle ϕ\phiϕ:

a1=a0cos⁡ϕa_1 = a_0\cos\phia1​=a0​cosϕ and

a2=a0sin⁡ϕa_2 = a_0\sin\phia2​=a0​sinϕ,

the polarization state of a linearly polarized wave is completely described by a0a_0a0​ and ϕ\phiϕ in terms of two linear polarization components.

Three independent parameters are needed to describe the polarization state of the initial vector wave. In the case of linear polarization components, these are the amplitudes axa_xax​ , aya_yay​ and the relative phase ϕ\phiϕ. A practical way of expressing these parameters is by the use of the so-called Stokes parameters. The following relation exists-by definition-between Stokes parameters and the amplitude and phase of the polarization components:

I=ax2+ay2I = a_x^2 + a_y^2I=ax2​+ay2​

Q=ax2−ay2Q = a_x^2 - a_y^2Q=ax2​−ay2​

U=2axaycos⁡δU = 2 a_x a_y \cos \deltaU=2ax​ay​cosδ

V=2axaysin⁡δV = 2 a_x a_y \sin \deltaV=2ax​ay​sinδ.

PI=U2+Q2\mathrm{PI} = \sqrt{U^2 + Q^2}PI=U2+Q2​

PA=arctan⁡(QU)\mathrm{PA} = \arctan\left(\dfrac{Q}{U}\right)PA=arctan(UQ​)

PP=PI/I\mathrm{PP} = \mathrm{PI} / IPP=PI/I

I=<ax2>+<ay2>I = \left<a_x^2\right> + \left<a_y^2\right>I=⟨ax2​⟩+⟨ay2​⟩

Q=<ax2>−<ay2>Q = \left<a_x^2\right> - \left<a_y^2\right>Q=⟨ax2​⟩−⟨ay2​⟩

U=2<axaycos⁡δ>U = 2 \left<a_x a_y \cos \delta\right>U=2⟨ax​ay​cosδ⟩

V=2<axaysin⁡δ>V = 2 \left<a_x a_y \sin \delta\right>V=2⟨ax​ay​sinδ⟩.

<VxVy>=lim⁡T′→∞14T′∫−T′T′(Ex+Ex∗)(Ey+Ey∗)dt\left<V_x V_y\right> = \lim\limits_{T'\to\infty} \frac{1}{4T'} \int_{-T'}^{T'} \left(E_x + E_x^*\right) \left(E_y + E_y^*\right) dt⟨Vx​Vy​⟩=T′→∞lim​4T′1​∫−T′T′​(Ex​+Ex∗​)(Ey​+Ey∗​)dt.

12T′∫−T′T′e2iωtdt=T4πT′sin⁡2ωT′≈0\frac{1}{2T'} \int_{-T'}^{T'} e^{2i\omega t} dt = \frac{T}{4\pi T'}\sin 2\omega T' \approx 02T′1​∫−T′T′​e2iωtdt=4πT′T​sin2ωT′≈0

for T′≫TT' \gg TT′≫T the time-averaged product becomes:

<VxVy>∝AxAy∗+Ax∗Ay=axaycos⁡δ\left< V_x V_y \right> \propto A_x A_y^* + A_x^* A_y = a_x a_y \cos \delta⟨Vx​Vy​⟩∝Ax​Ay∗​+Ax∗​Ay​=ax​ay​cosδ

<VxVy>=Re(ExEy∗)=axaycos⁡δ\left< V_x V_y \right> = \mathfrak{Re} \left(E_x E_y^*\right) = a_x a_y \cos\delta⟨Vx​Vy​⟩=Re(Ex​Ey∗​)=ax​ay​cosδ.

I=<ExEx∗>+<EyEy∗>I = \left< E_x E_x^* \right> + \left< E_y E_y^* \right>I=⟨Ex​Ex∗​⟩+⟨Ey​Ey∗​⟩

Q=<ExEx∗>−<EyEy∗>Q = \left< E_x E_x^* \right> - \left< E_y E_y^* \right>Q=⟨Ex​Ex∗​⟩−⟨Ey​Ey∗​⟩

U=2 Re<ExEy∗>U = 2 \, \mathfrak{Re} \left< E_x E_y^* \right>U=2Re⟨Ex​Ey∗​⟩

V=2 Im<ExEy∗>V = 2 \, \mathfrak{Im} \left< E_x E_y^* \right>V=2Im⟨Ex​Ey∗​⟩.

Source:
https://en.wikipedia.org/wiki/Polarization_(waves)