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Introduction to main parameters of antenna
2022-07-28 18:23:00 【Welcome pine 88】
One 、 Input impedance and matching
The input impedance of the antenna refers to the impedance of the antenna at the feed port . Generally, the input impedance of the antenna is designed as 50 o . When the feeder and antenna impedance match , The reflection of the feed port is minimum , The energy on the feeder can be effectively transmitted to the antenna . therefore , The feeder needs to match the impedance of the antenna , That is, the feeder characteristic impedance value is designed as 50 o . therefore , Hardware PCB The characteristic impedance of the microstrip line connecting the antenna on the should be 50 o . To facilitate the adjustment of impedance matching , The built-in antenna model generally needs to reserve one near the feeding point π The location of the shape matching network . The input impedance of the external antenna is generally close 50 o , Reserve matching network according to actual needs .
Two 、 Return loss 、 Reflection coefficient and standing wave ratio
Return loss calculation formula : return wave damage Consumption = Enter into shoot work rate back shoot work rate = ( work rate back shoot rate ) − 1 Return loss =\frac{ Incident power }{ Reflected power }=( Power reflectivity )^{-1} return wave damage Consumption = back shoot work rate Enter into shoot work rate =( work rate back shoot rate )−1
When the feeder and antenna conjugate match , All the energy is absorbed by the load , There is only incident wave on the feeder , No reflected wave .
When the antenna and feeder do not match , That is, when the input impedance of the antenna is not equal to the characteristic impedance of the feeder , The load can only absorb part of the energy .
Part of the energy of the incident wave is reflected back to form a reflected wave .
chart 2.1 Energy conversion of antenna
As shown in the figure above , When the feeder is mismatched with the antenna , Assume that the antenna has no loss , Input 10W The power of 9.5W Radiate through the antenna ,0.5W The power is reflected back . Return loss here RL=-10log(0.5/10)=13dB .
In case of mismatch , There are both incident waves and reflected waves on the feeder . The ratio of the voltage amplitude of the reflected wave to the incident wave is called the reflection coefficient .
back shoot system Count Γ = back shoot electric Pressure Enter into shoot electric Pressure Reflection coefficient \Gamma =\frac{ Reflected voltage }{ Incident voltage } back shoot system Count Γ= Enter into shoot electric Pressure back shoot electric Pressure
Where the phase of the incident wave and the reflected wave is the same, the sum of the amplitudes is the largest , Form antinodes ; Where the phase of the incident wave and the reflected wave is opposite, the amplitude subtraction is the smallest , Form nodes . The ratio of antinode voltage to nodal voltage amplitude is called standing wave coefficient , Also called voltage standing wave ratio (VSWR).
Stationed wave Than V S W R = wave abdomen electric Pressure wave section electric Pressure In Bobbie VSWR=\frac{ Antinode voltage }{ Nodal voltage } Stationed wave Than VSWR= wave section electric Pressure wave abdomen electric Pressure
The closer the terminal load impedance is to the feeder characteristic impedance , The smaller the reflection coefficient , The closer the standing wave coefficient is to 1, The better the match .
Basic requirements of antenna : In Bobbie VSWR ≤2; namely : Return loss RL ≥9.6dB .( notes :VSWR=2 when ,RL=9.54dB
Approximate 9.6 dB, Reflected power / Incident power =11.11%)
3、 ... and 、 efficiency
Antenna efficiency refers to the ratio of antenna radiation power to input power , Calculation formula :
God Line effect rate η = Spoke shoot work rate transport Enter into work rate Antenna efficiency \eta =\frac{ Radiation power }{ Input power } God Line effect rate η= transport Enter into work rate Spoke shoot work rate
The efficiency of the external antenna is generally 70%-85%, The efficiency of the built-in antenna is generally 50-80% .
Part of the energy not radiated is reflected back , Part is the loss of the antenna itself . As shown in the figure below , Radiation efficiency =9W/10W=90% .
Four 、 Directivity and gain
Directivity of antenna refers to the ability of antenna to radiate electromagnetic waves in a certain direction . For the receiving antenna , Directivity indicates whether the antenna is aligned
The radio waves transmitted in the same direction have different receiving capabilities . The directivity of an antenna is usually represented by a pattern . The direction map can be used to say tomorrow
The ability of a line to transmit or receive electromagnetic waves in all directions of space . A single symmetric oscillator has “ Doughnuts ” Shaped
Directions :
chart 4.1 Symmetrical dipole pattern
Gain refers to the condition that the input power is equal , Actual antenna and ideal radiation unit ( Point source antenna ) At the same point in space
The square ratio of the generated field strength , That is, the ratio of power .
The commonly used omni-directional antenna generally refers to the horizontal plane ( The plane perpendicular to the antenna axis ) Omnidirectional antenna . Its pattern is a circle in the horizontal plane , It means that the gain of each direction is equal . Directional antenna refers to the antenna whose energy is concentrated in a certain direction .
Upper figure : Omnidirectional antenna ( Left ) And directional antenna ( Right ) Directions
The antenna gain reflects the concentration of the energy radiated by the antenna . The greater the gain , The more concentrated the energy . According to the conservation of energy , The more energy distributed in one direction , Naturally, the less energy distributed in other directions . The maximum gain of directional antenna is large , But its vertical plane covers a smaller area .
Upper figure : Comparison of antenna patterns with different gains
5、 ... and 、 bandwidth
Antenna bandwidth refers to the working frequency range in which one or some electrical properties of the antenna meet the requirements . Usually , When working at the center frequency, the antenna can transmit the maximum power , When it deviates from the center frequency, the power it transmits will be reduced . Simply speaking : Standing wave less than 2 For the working band width is the bandwidth .
6、 ... and 、 Polarization
When radio waves travel in space , Its electric field direction changes according to a certain law , This phenomenon is called the pole of radio waves
turn . The electric field direction of radio waves is called the polarization direction of radio waves .
Usually , If the electric field direction of the electric wave is perpendicular to the ground , We call it vertically polarized wave . If the electric field direction of the radio wave is the same as the ground
parallel , It is called horizontally polarized wave . The corresponding antennas are called vertical polarization antenna and horizontal polarization antenna .
Besides vertical polarization and horizontal polarization , And circular polarization 、 Elliptical polarization and other polarization methods . According to different rotation directions, circular polarization can be divided into left
Rotating circular polarization and right rotating circular polarization .
As shown in the figure below , If the electric field intensity on the section perpendicular to the transmission direction is decomposed into x Weight and y component , namely :
E x = E 1 s i n ( w t − β z ) E_{x}=E_{1}sin(wt-\beta z) Ex=E1sin(wt−βz)
E x = E 1 s i n ( w t − β z + δ ) E_{x}=E_{1}sin(wt-\beta z+\delta ) Ex=E1sin(wt−βz+δ)
Upper figure : Polarization diagram
When Ex And Ey Phase difference by 0 or 180 When the degree of , The polarization mode is linear polarization .
When E1=E2, And Ex And Ey Phase difference by 90 When the degree of , The polarization mode is circular polarization .
When E1≠E2, And Ex And Ey Phase difference Not for 0 Degree or 180 When the degree of , The polarization mode is elliptical polarization .
When the polarization direction of the incoming wave is inconsistent with that of the receiving antenna , Polarization loss usually occurs in the receiving process , for example : When receiving any linearly polarized wave with a circularly polarized antenna , Or when receiving any circularly polarized wave with a linearly polarized antenna , Will produce 3 DB polarization loss , That is, it can only receive half the energy of the incoming wave .
When the polarization direction of the receiving antenna ( For example, horizontal or right-handed circular polarization ) And the polarization direction of the incoming wave ( Corresponding to vertical or left-handed circular polarization ) When completely orthogonal , The receiving antenna will not receive the energy of the incoming wave at all , At this time, it is said that the transmitting antenna and the receiving antenna are polarization isolated .
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