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Antennas. Hertzian dipole antenna. Heinrich Hertz (1857-1894). Schematic diagram of Hertz’ experiment. Propagation of electromagnetic wave. Electric field : red Magnetic field : blue. Reception of EM wave. current. V. Transmitting antenna. Receiving antenna.
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Hertziandipole antenna Heinrich Hertz (1857-1894)
Propagation of electromagnetic wave Electric field : red Magnetic field : blue
Reception of EM wave current V Transmitting antenna Receiving antenna The charges on the receiving antenna move toward the antenna terminal, which causes voltage drop across them.
Advantage of a resonant circuit Generate higher voltage than input voltage. At resonance Maximum current level depends on internal resistance.
How to generate time varying currents Alternating currents accelerate electrons which emit electromagnetic waves propagating in perpendicular direction Electronic circuit generate oscillating voltages Output voltage
Radiation from an infinitesimally small current segment Exact solution :
Far field approximation Near field approximation Electrostatic solution Biot-Savart’s law Coulomb’s law
Gain and directivityof an antenna Isotropic pattern Omnidirectional pattern Directional pattern Directivity 정의 : (Efficiency) : Gain takes into account losses and reflections of the antenna.
Friis equation transmitter receiver
Array factor Array factor : z-directed array
x-directed array Array factor Top view
How to change currents on elementary antennas? Magnitudes and phases of currents on elementary antennas can be changed by amplifiers and phase shifters.
Pattern synthesis Equi-phase surface Equi-phase surface
Examples (1) Two element array (2) Two element array
(3) Five element array 3dB Beamwidth Beam direction (4) Five element array (5) Five element array
Sample MATLAB codes phi=0:0.01:2*pi; %0<phi<2*pi k=2*pi; d=0.5;% 0.5 lambda spacing. shi=k*d*cos(phi); alpha = pi*0.0; beta = exp(i*alpha); %Currents=[1,2*beta, 3*beta^2,2*beta^3,1*beta^4]; %Current excitations Currents=[1, 1*beta, 1*beta^2, 1*beta^3,1*beta^4]; %Current excitations E=freqz(Currents,1,shi); %E for different shi values E = DB(E)+30; % 최대값에서 30dB 범위까지 그림. E = (E>0.).*E; polar(phi,E); %Generating the radiation pattern
N-element linear array antenna Uniform Array : Magnitudes of all currents are equal. Phases increase monotonically.
Difference : • Universal Pattern is symmetric about y= p. • Width of main lobe decrease with N • Number of sidelobes = (N-2) • Widths of sidelobes = (2π/N) • Side lobe levels decrease with increasing N.
Visible and invisible regions 1 visible region Array Factor의 특성 • Array factor has a period of 2p with respect to ψ. • Of universal pattern, the range covered by a circle with radius “kd” become visible range. • The rest region become invisible range Visible range of the linear array
Grating Lobes Phenomenon 1 grating lobes major lobe They have the same strength ! visible region • If the visible range includes more than one peak levels of universal pattern, unwanted peaks are called grating lobes. • To avoid grating lobes, the following condition should be met. Example : , no grating lobe occurs , no grating lobe occurs
Example : array antenna (77GHz) 표면 전류 분포 두께 0.127mm 비유전율 2.2 17mm 10mm 77GHz에서 array element들이 모두 동위상을 갖도록 설계함.
Radiation pattern (77GHz) elementarypattern Radiation pattern of 8-element array
Beamforming Approaches : Digital Beamformer (DBF) Interference or multipath signal direction Digital Signal Processing (Amplitude & Phase) LPF A/D LPF A/D LPF A/D Desired signal direction LPF A/D ~