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Antenna Gain Calculator

Estimate antenna gain in dBi from E-plane and H-plane half-power beamwidths using the beam-area approximation - for dish, horn, and Yagi antenna design.

Frequently Asked Questions

Can I increase range by adding antenna gain?

Yes, but with an important caveat: gain comes from narrowing the beam, so you must aim the antenna carefully. Replacing a 2 dBi omnidirectional antenna with a 12 dBi Yagi gives you 10 dB of extra signal - equivalent to a 10x increase in transmitter power or roughly tripling the range in free space. However, the Yagi has a beam only 30-40 degrees wide, so both ends of the link must point at each other. For fixed point-to-point links this is straightforward. For mobile or broadcast applications where coverage area matters, a high-gain antenna can actually hurt performance by leaving gaps in coverage.

Why is my measured gain lower than the datasheet?

Several real-world factors subtract from the rated figure. Impedance mismatch between the antenna and feedline causes some power to reflect rather than radiate, reducing effective gain. Cable losses between the transmitter and antenna consume power before it even reaches the radiating element. Polarization mismatch between transmit and receive antennas (for example, vertical vs. horizontal) can cost 3-20 dB. Nearby structures detune the antenna and alter its pattern. And many datasheets are measured in an anechoic chamber with an ideal feed, conditions that rarely exist in a real installation.

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Estimates for informational purposes only.

Important Disclaimer: Estimates for informational purposes only.

This calculator provides estimates for informational purposes only. Results are based on assumptions and may not reflect actual outcomes. Consult qualified professionals in relevant fields before making important decisions based on these results.

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How This Calculator Works

This calculator estimates the directive gain of an antenna from its half-power beamwidths in the two principal planes. A narrower beam concentrates radiated energy into a smaller solid angle, which raises the gain. The approximation divides the number of square degrees on a sphere by the area of the main beam and converts the ratio to decibels relative to an isotropic radiator.

Why It Is An Estimate

The real gain of an antenna is always lower than this beamwidth estimate because the formula ignores ohmic losses, side lobe radiation, and impedance mismatch. Treat the result as an upper bound that is useful for quick comparisons rather than a calibrated measurement. The constant in the formula already accounts for the full sphere expressed in square degrees.

Tips

Measure beamwidths at the points where the radiated power falls to half of its peak.
Subtract one to three decibels from this estimate to allow for typical real world losses.
Smaller beamwidths give higher gain but a narrower coverage area.

dBi vs. dBd - Choosing the Right Reference

Antenna gain is always a ratio, and the choice of reference antenna changes the number. dBi references a hypothetical isotropic radiator that radiates equally in all directions, a theoretical construct that cannot be physically built. Because it is the most conservative reference, dBi is the standard in most technical and regulatory contexts. dBd references a real half-wave dipole in free space, which itself has a gain of 2.15 dBi over isotropic. The practical conversion is simple: dBi = dBd + 2.15. Datasheets sometimes list both figures because marketing materials favor dBd (a larger-sounding number) while engineers and regulators expect dBi. When comparing antennas, always check which reference is being used - a 5 dBd antenna and a 5 dBi antenna are not equally capable.

Effective Radiated Power (ERP) and EIRP

Regulatory bodies and link budget engineers express transmitter output in terms of the power that would need to be fed into a reference antenna to produce the same signal at the receiver. EIRP (Equivalent Isotropic Radiated Power) is referenced to an isotropic radiator: EIRP = P_tx + G_tx - L_cable, where all terms are in dBm and dB respectively. ERP uses the half-wave dipole as the reference and is therefore 2.15 dB lower than EIRP for the same setup. The FCC uses EIRP for most Part 15 and Part 97 regulatory limits because it is unambiguous. If your transmitter puts out 23 dBm, your cable has 2 dB of loss, and your antenna has 5 dBi of gain, your EIRP is 23 - 2 + 5 = 26 dBm.

Antenna Types and Typical Gains

Different antenna technologies occupy very different regions of the gain spectrum, with a fundamental trade-off between gain and beamwidth: concentrating energy into a narrower beam raises gain but shrinks coverage area.

Isotropic radiator: 0 dBi by definition. Theoretical only - used as the reference point.
Half-wave dipole: 2.15 dBi. The workhorse antenna for HF, VHF, and UHF. Omnidirectional in the broadside plane.
Yagi-Uda: 6-20 dBi depending on the number of elements. A 3-element Yagi is around 7-8 dBi; a 15-element long-boom Yagi reaches 16-18 dBi. Widely used for TV reception and amateur radio.
Patch/microstrip: 5-8 dBi. Low profile, easy to integrate into PCBs and consumer devices. GPS and WiFi devices commonly use patch antennas.
Parabolic dish: 20-45 dBi. Gain scales with the square of the dish diameter relative to wavelength. Satellite TV dishes are around 33-37 dBi; large radio telescope dishes exceed 60 dBi.
Horn antenna: 10-25 dBi. Excellent reference standard, low side lobes, commonly used as a feed for parabolic dishes.
Phased array: Gain scales with the number of elements - doubling elements adds 3 dB. Modern 5G base stations use 32-256 element arrays for beamforming.
Collinear array: 3-9 dBi. Stacked dipoles for higher gain while maintaining omnidirectional pattern. Common on VHF/UHF repeater masts.

The key trade-off is inescapable: a narrow beam means high gain but you must point the antenna accurately. A parabolic dish with 1-degree beamwidth and 40 dBi of gain will lose most of that gain if it is off-axis by even a fraction of a degree.

Gain in System Link Budgets

Antenna gain directly impacts system performance in two ways. On the transmit side, each decibel of antenna gain is equivalent to doubling the transmitter power - a 3 dBi increase in antenna gain saves as much power as doubling the transmitter. On the receive side, gain adds directly to the signal-to-noise ratio because the antenna collects more signal without changing the receiver noise floor. This is why large parabolic dishes are used for satellite downlinks even with powerful satellites - the link budget demands it.

The Friis transmission equation ties it all together: P_r = P_t + G_t + G_r - FSPL, all in dB. The received power equals the transmitted power, plus transmit antenna gain, plus receive antenna gain, minus free-space path loss. Adding 3 dB of receive antenna gain is equivalent to halving the path loss distance in terms of received signal level.

For receive-only systems like satellite TV dishes and radio telescopes, the figure of merit is G/T (gain-to-noise-temperature ratio), where T is the system noise temperature in Kelvin. A higher G/T means the system can detect weaker signals. Pointing a dish at a warmer part of the sky raises T and degrades G/T even without changing G.

Regulatory Limits

The FCC and other regulatory bodies cap EIRP rather than transmitter power alone, which means that a high-gain antenna can force you to reduce transmitter power to stay legal. FCC Part 15 ISM band devices (2.4 GHz WiFi point-to-point) allow EIRP of up to 4 W (36 dBm) for point-to-point links but only 1 W for point-to-multipoint. For licensed amateur radio operators, there is no specific power limit in most bands, but the rule is to use the minimum power necessary. Military and aerospace applications often specify maximum EIRP to prevent interference with other systems operating in the same band.