Low-frequency loading antenna
An antenna and low-frequency technology, applied in the field of radio transceivers, can solve the problems of large loss, deterioration of antenna performance, and low antenna radiation efficiency.
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Example Embodiment
[0027] Example 1
[0028] A low-frequency loading antenna, including:
[0029] Monopole antenna, the monopole antenna is connected with a feeder, the length of the monopole antenna is 360mm, the radius is 7.5mm, and the distance between the radiation boundary and the antenna is 375mm;
[0030] Lumped loading part, which is connected in series with the monopole antenna;
[0031] Impedance converter, used to realize that the impedance of the feed end of the monopole antenna is equal to the characteristic impedance of the feeder. In this embodiment, an AT&T (pin-type) impedance converter is selected;
[0032] Among them, the lumped loading part includes inductance and resistance. The inductance and resistance are connected in series with the monopole antenna. The parameters of inductance and resistance are 1.73uH inductance and 2.12kΩ in resistance.
[0033] The reactance of the monopole antenna is capacitive, so if the inductance L and the resistance R are connected in series at the input ...
Example Embodiment
[0040] Example 2
[0041] Compared with embodiment 1, the difference is that the parameters of inductance and resistance are 102.70nH inductance and 420Ω resistance, and also includes a sleeve, which is sheathed on the top of the monopole antenna, and the top of the monopole antenna Connect with the inside of the sleeve.
[0042] According to transmission line theory, a terminal short-circuit line with a total length of no more than a quarter of a wavelength can be used as an inductive load, and its equivalent reactance value can be calculated by the following formula:
[0043] jX in =jZ 0 tanβl
[0044] The sleeve can be regarded as a terminal short circuit, which is equivalent to an inductive load loaded on the top of the antenna. Also, because the monopole antenna is an antenna with capacitive impedance, the loading of the sleeve can just offset a certain capacitive reactance, thereby reducing the resonant frequency of the antenna and improving the impedance characteristics of th...
Example Embodiment
[0045] Example 3
[0046] Compared with Embodiment 1, the difference is that the inductor is a tunable inductor, and the resistor is a sliding rheostat. In this way, when the monopole antenna undergoes deformation within a certain range (such as being hit or broken), the present invention can still work normally by adjusting the parameters of the inductance and resistance.
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