2011 Lectures for Antennas I 1. Far-field approximation 2. Antenna radiation characteristics: Pattern, dimensions, directivity, gain, and resistance 1. Far-field approximation: Since we are always interested in E and H fields in great distance while r>>, we can simply the E and H fields by considering: kr=2r/>>1 so 1/kr>>1/(kr)2, and jI 0 lk 0 e jkr E 4 r E H 0 sin V / m A / m 2. Antenna radiation characteristics: Pattern, dimensions, directivity, gain, and resistance Power Density: The power density can be expressed by the time-average Poynting vector. 1 2011 1 S ave Re E H * 2 0 k 2 I 02 l 2 S r , 2 2 32 r S max 2 sin S max sin 2 15I 02 r2 F , 1 2 S r , S max Total Radiation Power: 2 S r , , sin dd r 0 0 Prad r 2 d sin dd 2 2 S max F , d 4 2011 Beam dimensions: For an antenna with a single main lobe, the pattern solid angle describes the equivalent width of the main lobe. p F , d 4 3 2011 For an isotropic antenna with F(,)=1, p=4 (sr) In practical, the beam width can be also described using halfpower beam width (3-dB width) or null beam width. Antenna Directivity: Directivity characterizes the ratio of the antenna’s maximum radiation intensity to its average intensity. D S max Fmax 1 S ave Fave 4 1 F , d 4 p 4 Radiation efficiency: If the total power supplied to the antenna is Pt, a part, Prad, is radiated out into space, and the remainder, Ploss, is dissipated as heat. The radiation efficiency is defined as: Radiation gain: 4 Prad Pt 2011 The gain of an antenna has similar definition as the directivity D, but also account for Ohmic loss. G S max Pt 4r 2 Radiation gain: The total power supplied to the antenna is Pt and the radiated power Prad, can also be characterized using impedance concepts as loss resistance and radiation resistance: Prad 1 2 I 0 Rrad 2 5 Prad 1 2 I 0 Rrad Rloss 2 Rrad Rrad Rloss