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Knowledge Hubantenna and propagation1. Antenna Basics: From Current to Coverage

antenna and propagation learning note

1. Antenna Basics: From Current to Coverage

Start with wavelength, matching, radiation pattern, gain, efficiency, and polarization; learn what each quantity tells you before evaluating an antenna.

Incident power splits into reflected and accepted power; accepted power splits into heat loss and radiated power, which forms a directional pattern
Original figure: feed matching and radiation efficiency answer different questions. The directional pattern then determines where the radiated power is useful.

What to Know First

An antenna turns a signal at its feed into a radiated field, or receives a field at that feed.

  • Frequency: sets wavelength and electrical size.
  • Direction: tells where the radiated power goes.
  • Polarization: tells how the electric field is oriented.
  • Why all three: one peak gain value cannot describe every frequency, direction, and polarization.

In free space:

λ=cf\lambda=\frac{c}{f}
  • λ\lambda: wavelength in metres.
  • cc: speed of light, approximately 3×1083\times10^8 m/s.
  • ff: frequency in hertz.

Higher frequency means shorter wavelength. Always state frequency when comparing antenna dimensions or patterns.

  • 3 GHz: wavelength about 10 cm; half-wavelength element spacing about 5 cm.
  • 30 GHz: wavelength about 1 cm; half-wavelength spacing about 5 mm.
  • Trade-off: compact mmWave arrays are possible, but feed loss, fabrication tolerance, and blockage become harder.
References for this section3

Follow the Power

Follow the power in the figure: some reflects at the port, some becomes heat, and the remainder radiates in different directions.

  • Directivity: how strongly the pattern concentrates power compared with an isotropic reference.
  • Gain: directivity with radiation efficiency included.
  • Realized gain: gain with feed mismatch included as well.
  • Practical check: a data sheet must say which gain it reports.
QuantityPhysical meaningWhen it matters
S11S_{11} / return lossHow much incident feed power reflects back at the portChecking matching over the operating band
Radiation efficiencyRadiated power divided by accepted powerDistinguishing a lossy antenna from a useful radiator
Realized gainDirectional gain after mismatch lossComparing installed link-budget inputs on a consistent basis
Radiation pattern and HPBWWhere energy goes and the main-lobe half-power widthPlanning coverage, pointing, and interference
PolarizationOrientation or trajectory of the electric fieldMatching Tx/Rx antennas and interpreting cross-polarized ports
  • ∣S11∣2|S_{11}|^2: reflected power fraction for the stated one-port reference impedance.
  • Why matching is not enough: a matched resistor can absorb power without radiating it.

For a reference impedance Z0Z_0 and antenna input impedance ZinZ_{\mathrm{in}}, the reflection coefficient is

Γ=Zin−Z0Zin+Z0,S11,dB=20log⁡10∣Γ∣\Gamma=\frac{Z_{\mathrm{in}}-Z_0}{Z_{\mathrm{in}}+Z_0}, \qquad S_{11,\mathrm{dB}}=20\log_{10}|\Gamma|
  • Γ\Gamma: feed-port reflection coefficient; ∣Γ∣2|\Gamma|^2 is the reflected power fraction.
  • ZinZ_{\mathrm{in}}: antenna input impedance; Z0Z_0: stated reference impedance.
  • S11,dBS_{11,\mathrm{dB}}: reflection expressed in dB, assuming the same reference.

The accepted and radiated powers can then be separated:

Paccepted=Pincident(1−∣Γ∣2),Pradiated=ηradPacceptedP_{\mathrm{accepted}}=P_{\mathrm{incident}}(1-|\Gamma|^2), \qquad P_{\mathrm{radiated}}=\eta_{\mathrm{rad}}P_{\mathrm{accepted}}
  • PincidentP_{\mathrm{incident}}, PacceptedP_{\mathrm{accepted}}, PradiatedP_{\mathrm{radiated}}: power reaching the port, entering the antenna, and actually radiated.
  • Γ\Gamma: feed-port reflection coefficient from the preceding equation.
  • ηrad\eta_{\mathrm{rad}}: radiation efficiency, between 0 and 1.
References for this section3

S-Parameters: Follow the RF Waves

Scattering parameters describe what happens to RF waves at the ports of a device. They are complex values, so both magnitude and phase can be measured over frequency.

Incident waves a1 and a2 enter a two-port network; outgoing waves b1 and b2 distinguish input reflection S11, forward transfer S21, reverse transfer S12, and output reflection S22
Original signal-flow diagram. Measure one excited port at a time while the other port is terminated in the stated reference impedance.
  • Port: a defined RF connection or antenna feed with a reference impedance, commonly but not necessarily 50 Ω50\ \Omega.
  • Incident wave aia_i: the wave entering port ii.
  • Outgoing wave bib_i: the wave leaving port ii.
  • Index rule: in SijS_{ij}, jj is the excited input port and ii is the observed output port.

For a two-port network:

[b1b2]=[S11S12S21S22][a1a2]\begin{bmatrix}b_1\\b_2\end{bmatrix} =\begin{bmatrix}S_{11}&S_{12}\\S_{21}&S_{22}\end{bmatrix} \begin{bmatrix}a_1\\a_2\end{bmatrix}
  • a1,a2a_1,a_2: incident waves at ports 1 and 2; b1,b2b_1,b_2: outgoing waves.

  • S11S_{11}: reflection back into port 1 when port 2 is matched.

  • S22S_{22}: reflection back into port 2 when port 1 is matched.

  • S21S_{21}: forward transfer from port 1 to 2; S12S_{12}: reverse transfer from port 2 to 1.

  • One antenna port: S11S_{11} checks feed matching, not radiation efficiency.

  • Two antenna ports: S21S_{21} or S12S_{12} indicate coupling under stated terminations; neither alone proves independent MIMO channels.

References for this section3

Return Loss, Mismatch, and VSWR

Three views of the same one-port reflection are useful:

Preflected/Pincident=∣S11∣2,RL=−20log⁡10∣S11∣P_{\mathrm{reflected}}/P_{\mathrm{incident}}=|S_{11}|^2, \qquad RL=-20\log_{10}|S_{11}|
  • Preflected/PincidentP_{\mathrm{reflected}}/P_{\mathrm{incident}}: reflected power fraction at the stated port reference.
  • S11S_{11}: complex reflection coefficient for this one-port measurement; ∣S11∣|S_{11}| is its wave-amplitude ratio.
  • RLRL: positive return loss in dB. By contrast, S11,dB=20log⁡10∣S11∣S_{11,\mathrm{dB}}=20\log_{10}|S_{11}| is usually negative; RL=−S11,dBRL=-S_{11,\mathrm{dB}}.
VSWR=1+∣S11∣1−∣S11∣\mathrm{VSWR}=\frac{1+|S_{11}|}{1-|S_{11}|}
  • VSWR\mathrm{VSWR}: voltage standing-wave ratio on a line referenced to the same impedance.
  • ∣S11∣|S_{11}|: reflection magnitude, from 0 (perfect match) toward 1 (complete reflection).

Example: S11=−10S_{11}=-10 dB means ∣S11∣≈0.316|S_{11}|\approx0.316, about 10% reflected power, 90% accepted power, RL=10RL=10 dB, and VSWR about 1.92. This does not mean 90% radiates: internal loss must still be checked.

References for this section3

Transmission and Isolation

S21=b2a1∣a2=0,S12=b1a2∣a1=0S_{21}=\left.\frac{b_2}{a_1}\right|_{a_2=0}, \qquad S_{12}=\left.\frac{b_1}{a_2}\right|_{a_1=0}
  • S21S_{21}: complex forward wave ratio with port 2 matched.
  • S12S_{12}: complex reverse wave ratio with port 1 matched.
  • ai,bia_i,b_i: incident and outgoing waves shown in the diagram; the zero subscript condition means the other port has no incident wave from its matched termination.
  • For a passive two-port device: 20log⁡10∣S21∣20\log_{10}|S_{21}| reports transfer in dB; a more negative number can mean more insertion loss.
  • For antenna ports: a more negative coupling value can indicate better port isolation, but pattern, efficiency, correlation, and over-the-air channel still matter.

Under matched, equal-reference port conditions, a useful positive loss convention is:

IL21=−20log⁡10∣S21∣,I21=−20log⁡10∣S21∣IL_{21}=-20\log_{10}|S_{21}|, \qquad I_{21}=-20\log_{10}|S_{21}|
  • IL21IL_{21}: insertion loss in dB when port 2 is the intended output of a passive path.
  • I21I_{21}: isolation in dB when transfer from port 1 to port 2 is unwanted coupling.
  • ∣S21∣|S_{21}|: forward wave-amplitude ratio with the other port matched; the arithmetic is the same, but the engineering question differs.
  • Example: S21=−20S_{21}=-20 dB corresponds to about 1% transferred power under these matched-reference conditions, or 20 dB isolation between ports.

Measurement order: calibrate the vector network analyser at the chosen reference plane, state port impedance and cable/de-embedding treatment, sweep the intended band, then compare SS-parameters at the same frequency and setup.

References for this section3

Worked Example: Matching Is Not Efficiency

Suppose 1 W is incident on an antenna with S11=−10S_{11}=-10 dB and radiation efficiency of 80%:

  1. At the port: ∣S11∣2=0.1|S_{11}|^2=0.1; 0.1 W reflects and 0.9 W is accepted.
  2. Inside the antenna: 0.8×0.9=0.720.8\times0.9=0.72 W is radiated; 0.18 W is lost internally.
  3. In the useful direction: if directivity is 12 dBi, gain is 12+10log⁡10(0.8)≈11.012+10\log_{10}(0.8)\approx11.0 dBi. Including mismatch gives realized gain of about 10.6 dBi.

A second antenna with the same matching could radiate less if its efficiency is lower. These values assume efficiency and directivity at the same frequency and direction.

References for this section3

Radiation Pattern and Beamwidth

Radiation pattern shows how radiated strength changes with direction. It may be a power/intensity pattern or a field-amplitude pattern; check the plotted quantity and normalization.

Conceptual azimuth radiation pattern with main lobe, sidelobes, and half-power beamwidth alongside incident, accepted, and radiated power stages
Original conceptual figure: an azimuth slice identifies beam features; it is not a complete 3D pattern or a measured antenna.
  • Main lobe: strongest radiation direction; a narrower lobe often raises peak gain but covers less angle.
  • Sidelobes: smaller peaks that can illuminate unintended users or interferers.
  • Back radiation: power sent behind the intended direction.
  • Read a pattern with: frequency, polarization, cut plane, and normalization. An azimuth slice is not the full 3D pattern.

Half-power beamwidth (HPBW) measures the angle between the two main-lobe directions at half the peak power:

U(θ1,ϕ0)=U(θ2,ϕ0)=Umax⁡2,HPBW=∣θ2−θ1∣U(\theta_1,\phi_0)=U(\theta_2,\phi_0)=\frac{U_{\max}}{2}, \qquad \mathrm{HPBW}=|\theta_2-\theta_1|
  • U(θ,ϕ)U(\theta,\phi): radiation intensity in direction (θ,ϕ)(\theta,\phi), in W/sr.
  • Umax⁡U_{\max}: peak intensity on the stated cut; ϕ0\phi_0: fixed plane of that cut.
  • θ1,θ2\theta_1,\theta_2: the two half-power angles around the main lobe.
  • HPBW\mathrm{HPBW}: angular width, usually in degrees. Half power is −3.01-3.01 dB relative to peak.
References for this section3

Directivity, Gain, and EIRP

Radiation intensity turns the far-field power density at a range into a direction-dependent power per solid angle:

U(θ,ϕ)=r2Srad(r,θ,ϕ),Prad=∫4πU(θ,ϕ) dΩU(\theta,\phi)=r^2S_{\mathrm{rad}}(r,\theta,\phi), \qquad P_{\mathrm{rad}}=\int_{4\pi}U(\theta,\phi)\,d\Omega
  • U(θ,ϕ)U(\theta,\phi): radiation intensity in W/sr at direction (θ,ϕ)(\theta,\phi).
  • SradS_{\mathrm{rad}}: far-field power density in W/m² at distance rr in metres.
  • PradP_{\mathrm{rad}}: total power radiated over all directions, in watts.
  • dΩd\Omega: small solid angle in steradians; 4π4\pi denotes the entire sphere.

Directivity compares one direction with an ideal isotropic radiator that radiates the same total power:

D(θ,ϕ)=4πU(θ,ϕ)PradD(\theta,\phi)=\frac{4\pi U(\theta,\phi)}{P_{\mathrm{rad}}}
  • D(θ,ϕ)D(\theta,\phi): dimensionless directional concentration; 10log⁡10D10\log_{10}D gives dBi.
  • U(θ,ϕ)U(\theta,\phi): radiation intensity in that direction.
  • PradP_{\mathrm{rad}}: total radiated power; 4π4\pi is the full-sphere solid angle in sr.
  • Physical point: directivity describes shape, not conductor/dielectric loss or feed mismatch.

Radiation efficiency and gain include the antenna's internal loss:

ηrad=PradPaccepted,G(θ,ϕ)=ηradD(θ,ϕ)\eta_{\mathrm{rad}}=\frac{P_{\mathrm{rad}}}{P_{\mathrm{accepted}}}, \qquad G(\theta,\phi)=\eta_{\mathrm{rad}}D(\theta,\phi)
  • ηrad\eta_{\mathrm{rad}}: fraction of accepted power radiated, between 0 and 1.
  • PacceptedP_{\mathrm{accepted}}: power entering the antenna after feed reflection.
  • PradP_{\mathrm{rad}}: power actually radiated; DD: directivity; GG: directional power gain relative to isotropic.
  • In dB: GdBi=DdBi+10log⁡10ηradG_{\mathrm{dBi}}=D_{\mathrm{dBi}}+10\log_{10}\eta_{\mathrm{rad}}.

Realized gain also includes mismatch at the stated feed:

Grealized(θ,ϕ)=(1−∣S11∣2)G(θ,ϕ)G_{\mathrm{realized}}(\theta,\phi)=(1-|S_{11}|^2)G(\theta,\phi)
  • GrealizedG_{\mathrm{realized}}: gain including feed mismatch, for this single-port reference.
  • ∣S11∣2|S_{11}|^2: reflected power fraction; 1−∣S11∣21-|S_{11}|^2 is accepted power fraction.
  • GG: gain after internal radiation loss but before mismatch loss.

EIRP is the isotropic power that would produce the same far-field strength in a chosen direction:

EIRPdBm(θ,ϕ)=Ptx,dBm−Lfeed,dB+GdBi(θ,ϕ)\mathrm{EIRP}_{\mathrm{dBm}}(\theta,\phi)=P_{\mathrm{tx,dBm}}-L_{\mathrm{feed,dB}}+G_{\mathrm{dBi}}(\theta,\phi)
  • Ptx,dBmP_{\mathrm{tx,dBm}}: power at the point before the stated feed loss.
  • Lfeed,dBL_{\mathrm{feed,dB}}: loss between that point and the antenna's accepted-power reference.
  • GdBi(θ,ϕ)G_{\mathrm{dBi}}(\theta,\phi): directional gain at the antenna input in dBi.
  • EIRPdBm\mathrm{EIRP}_{\mathrm{dBm}}: equivalent isotropic radiated power in that direction. If using realized gain at an incident-port reference, do not subtract mismatch again.

Worked comparison: take 1 W (30 dBm) at the incident port, 12 dBi directivity, 80% radiation efficiency, and S11=−10S_{11}=-10 dB.

  1. Gain: about 11.0 dBi after radiation loss.
  2. Realized gain: about 10.6 dBi after reflection at the feed.
  3. Peak EIRP: about 40.6 dBm from this incident-port reference.
References for this section3

What a Pattern Can and Cannot Say

Polarization mismatch means the transmitting and receiving electric-field orientations do not line up, even when their beams do.

ηpol=cos⁡2ψ\eta_{\mathrm{pol}}=\cos^2\psi
  • ηpol\eta_{\mathrm{pol}}: ideal linear-polarization power-coupling fraction.

  • ψ\psi: angle between the two linear polarizations.

  • 45∘45^\circ mismatch: half the ideal power couples, a 3 dB loss.

  • 90∘90^\circ mismatch: zero coupling in the ideal linear model.

  • Link lesson: matching and peak gain do not fix wrong pointing or polarization.

References for this section3

Gain, Aperture, and Beamwidth

  • Peak gain: concentration of existing radiation, not extra generated power.

  • Electrical aperture: antenna size measured relative to wavelength; a larger one can usually make a narrower beam.

  • HPBW: angle between the two main-lobe directions at half peak power (−3-3 dB).

  • Coverage check: report azimuth and elevation cuts; a beam can be narrow in one plane and broad in the other.

  • Data sheet: inspect patterns across the band, not only one peak dBi number.

  • Sidelobes/back radiation: check unintended illumination and interference.

  • Array: element pattern and array factor combine; element gain alone cannot predict the steered beam.

References for this section3

Where This Is Used

  • Coverage planning: select a pattern and downtilt that illuminate the intended area.

  • Link budgets: use the appropriate directional gain, feed loss, and pointing loss.

  • MIMO and arrays: inspect port isolation and correlation as well as the element pattern.

  • Measurement: check S11S_{11} with a calibrated network analyser, then measure radiation pattern and gain with an appropriate antenna setup; one test does not replace the other.

  • Rooftop sector: pattern and downtilt decide whether power reaches the street or overshoots it.

  • Point-to-point backhaul: a narrow beam adds directional gain but requires precise alignment.

  • Handset: efficiency and hand detuning can matter more than laboratory peak gain.

  • Dual-polarized MIMO: cross-polar discrimination and port isolation join gain and pattern checks.

Practical checklist:

  1. State the band and reference impedance; plot S11S_{11} across the band.
  2. Measure efficiency and realized gain; inspect co- and cross-polar patterns.
  3. Repeat at representative steering angles or installation positions.
  4. Judge values against the required link margin and coverage region.
References for this section3

Complete references and further reading