
What Is Antenna Gain and Why Calculate It?
Antenna gain quantifies how effectively an antenna concentrates radiated power in a particular direction compared to an isotropic radiator. It is expressed in dBi (decibels relative to isotropic). A patch antenna with 6 dBi gain, for example, delivers four times the power density on boresight versus an ideal isotrope radiating the same total power. Knowing gain is essential for closing any wireless link budget—whether you are designing a 5.8 GHz Wi-Fi feed, a 24 GHz radar front-end, or a 77 GHz automotive sensor on a PCB-integrated antenna.
Core Formulas Behind the Antenna Gain Calculator

Gain From Half-Power Beamwidths
The most common quick estimate relates gain to the 3 dB beamwidths in the two principal planes (E-plane and H-plane). The classical approximation is:
G ≈ k / (θE × θH)
where θE and θH are the half-power beamwidths in degrees and k is a constant that depends on the sidelobe structure. For a uniform aperture distribution k ≈ 26,000; for a typical tapered distribution with −13 dB first sidelobes, k ≈ 30,000 is more accurate. In decibels:
G (dBi) ≈ 10 log10(k / (θE × θH))
A horn antenna with 10° × 12° beamwidths and k = 26,000 yields G ≈ 10 log(26000/120) ≈ 23.4 dBi. Switching to k = 30,000 gives 24.0 dBi—illustrating how sidelobe assumptions shift the result by roughly half a dB.
Gain From Physical Aperture
For aperture-type antennas (horns, reflectors, slot arrays, lens antennas), gain relates directly to the physical aperture area A:
G = η × (4π A / λ²)
where η is the aperture efficiency (typically 0.5–0.7 for a parabolic dish, 0.8–0.9 for a well-designed horn) and λ is the free-space wavelength. A 30 cm diameter dish at 10 GHz (λ = 30 mm) with η = 0.55 produces G ≈ 0.55 × 4π × 0.0707 / 0.0009 ≈ 27.1 dBi.
Gain vs. Directivity
Directivity is the theoretical maximum, assuming zero ohmic and mismatch loss. Gain = ηrad × Directivity, where ηrad is the radiation efficiency. On a PCB antenna with lossy FR-4 substrate at 5.8 GHz, ηrad can drop below 0.7, costing you more than 1.5 dB versus the same geometry on low-loss Rogers RO4350B (Df = 0.0037 at 10 GHz). Material choice matters—especially above 10 GHz.
Antenna Gain and Beamwidth Calculator
Enter your beamwidths in degrees or your aperture dimensions and frequency below. The tool returns gain in dBi and the corresponding linear gain factor, so you can drop the number straight into a Friis link budget calculator or a radar range equation.
If the calculator returns 20 dBi from 15° × 18° beamwidths (k = 26,000), that means roughly 100× power concentration on boresight. For a 77 GHz automotive radar transmitting +12 dBm, those 20 dBi of antenna gain yield +32 dBm EIRP—enough to detect a 1 m² target beyond 100 m when paired with a receiver of adequate sensitivity. To refine the link, feed this gain value into a radar link budget tool along with your noise figure and integration parameters.
Factors That Change Real-World Gain
Aperture Efficiency (η)
Aperture efficiency bundles several sub-efficiencies: illumination taper, spillover, phase error, polarization mismatch, and surface roughness. A corporate-fed microstrip patch array on low-loss laminate can achieve η ≈ 0.65–0.75. A series-fed array trades some bandwidth for simpler feed routing but may see η drop to 0.50–0.60 due to amplitude taper across the array.
Substrate and Feed Losses
Every millimeter of microstrip feed line between the connector and the radiating element adds loss. At 24 GHz on RO3003 (Df = 0.0013), a 20 mm feed run costs roughly 0.3 dB. The same run on standard FR-4 (Df ≈ 0.020) would cost over 2 dB—wiping out the gain advantage of adding extra elements to the array. Use the interactive Smith chart tool to check the impedance match at the feed point and quantify mismatch loss.
Mismatch Loss
An antenna with S11 = −10 dB reflects 10 % of incident power, costing 0.46 dB. At −15 dB return loss the penalty shrinks to 0.14 dB. Always subtract mismatch loss from the calculated gain to get realized gain—the figure that actually matters in a link budget.
Beamwidth-to-Gain Quick Reference

| θE (°) | θH (°) | G (dBi), k = 26 000 | Typical Antenna Type |
|---|---|---|---|
| 90 | 90 | 5.1 | Single patch, dipole + reflector |
| 60 | 60 | 8.6 | 2 × 2 patch array |
| 30 | 30 | 14.6 | 4 × 4 patch array |
| 15 | 15 | 20.6 | 8 × 8 array, small dish |
| 5 | 5 | 30.2 | Large reflector, phased array |
| 1 | 1 | 44.1 | High-gain parabolic dish |
These values assume uniform illumination. Real antennas with tapered distributions will show 0.5–1.5 dB higher gain for the same beamwidths because sidelobe power is redistributed into the main lobe.
Connecting Gain to System Performance
Communication Links
The Friis transmission equation ties transmit gain, receive gain, path loss, and wavelength together. Doubling the antenna gain at one end adds 3 dB to the received power—equivalent to doubling the transmitter output power, but at zero extra DC current. That makes high-gain PCB antennas attractive for battery-powered IoT devices operating at 868 MHz or 2.4 GHz.
Radar Systems
In the radar range equation, antenna gain appears squared (once for transmit, once for receive in a monostatic system). A 3 dB gain improvement therefore adds 6 dB to the signal-to-noise ratio, extending detection range by roughly 41 %. When designing an FMCW radar chirp, pair the gain calculation with range-resolution analysis to ensure the antenna beamwidth and the radar’s angular resolution are consistent.
Unit Conversions in the RF Chain
Once you have gain in dBi, you will add it to transmit power (in dBm) and subtract path loss (in dB) to find received power. Keep units straight by using a dBm-to-watt and VSWR converter alongside this antenna gain calculator so every number in the cascade is in the same domain.
Common Pitfalls
- Using the wrong k constant. k = 41,253 applies only to the theoretical case of 100 % efficiency with no sidelobes—an impossible antenna. Use 26,000–33,000 depending on sidelobe level.
- Ignoring scan loss in arrays. A phased array scanned 60° off boresight loses roughly 6 dB of projected aperture gain. The calculator gives boresight gain; derate for your scan volume.
- Confusing dBi with dBd. dBd is gain relative to a half-wave dipole, which itself has 2.15 dBi. So 6 dBd = 8.15 dBi. Always confirm the reference in your datasheet.
- Neglecting radome loss. A plastic housing or conformal coating adds 0.2–1.0 dB of loss at millimeter-wave frequencies, reducing realized gain below the bare-antenna value.
FAQ
How do I convert beamwidth to gain in dBi?
Divide the constant k (typically 26,000 for uniform illumination) by the product of the E-plane and H-plane 3 dB beamwidths in degrees, then take 10 log10 of the result. The answer is gain in dBi.
What aperture efficiency should I assume?
For a parabolic reflector, 0.55 is a safe starting point. For a well-matched horn, use 0.7–0.8. For a PCB patch array with corporate feed on low-loss laminate, 0.65 is typical. Measure or simulate to refine.
Can I use this calculator for phased arrays?
Yes, for boresight gain. Enter the full array’s 3 dB beamwidths or total aperture area. For off-boresight gain, multiply the result by cos(θ) (or cosn(θ) for element-pattern roll-off) and subtract any additional scan-related phase-error losses.
Does antenna gain change with frequency?
For a fixed physical aperture, gain increases with frequency because λ decreases and G ∝ A/λ². For a fixed electrical size (like a half-wave dipole), gain stays roughly constant. PCB patch antennas are fixed-physical-size, so their gain rises if you scale frequency up—but bandwidth narrows and losses increase, so realized gain may peak and then fall.
Where does gain appear in the radar equation?
In the monostatic radar equation, gain appears squared: Pr ∝ G² λ² σ / R⁴. A 3 dB increase in antenna gain yields a 6 dB improvement in received power, equivalent to extending range by about 41 %. See the radar link budget calculator for a full worked example.
For a deeper treatment of antenna gain theory and measurement methods, the Wikipedia article on antenna gain provides a solid, peer-reviewed overview with references to the IEEE standard definitions in IEEE Std 145-2013 (Definitions of Terms for Antennas).
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