Antenna gain
The dimensionless ratio G = 4π · (maximum radiation intensity)/(total radiated power) that quantifies how much an antenna concentrates its radiation in its peak direction relative to an isotropic radiator. Usually expressed in dBi (decibels over isotropic).
Definition
Antenna gain is the dimensionless ratio G = 4π U_max/P_rad, where U_max is the maximum radiation intensity (power per unit solid angle) and P_rad is the total power radiated by the antenna. It quantifies the extent to which an antenna concentrates its radiated power in its peak direction compared with a hypothetical isotropic radiator that would spread the same total power uniformly over 4π steradians. Gain is usually expressed in decibels relative to isotropic (dBi): G_dBi = 10 log₁₀(G).
Representative values: an isotropic radiator has G = 1 (0 dBi) by definition. A Hertzian dipole has G = 1.5 (1.76 dBi). A centre-fed half-wave dipole has G ≈ 1.64 (2.15 dBi). A three-element Yagi for VHF television has about 7 dBi. A large parabolic dish for satellite downlink has G up to 40–60 dBi, with its gain-aperture relation G = 4π A_eff/λ². The reciprocity theorem guarantees that an antenna's gain is the same for transmission and reception — a high-gain dish that concentrates outgoing power into a narrow beam equally collects incoming power from that same narrow beam and rejects signals from elsewhere. The gain enters the Friis transmission formula P_r = P_t G_t G_r (λ/4πr)² that governs radio link budgets, and the effective aperture A_eff = G λ²/(4π) gives the equivalent collecting area for reception. Gain above isotropic is always paid for by pattern narrowness: no antenna can have G > 1 in every direction; high gain in one direction requires nulls elsewhere.