Dual-frequency bidirectional rectification antenna with wide power range
By etching a specific structure on the rectifier antenna and designing a rectifier circuit with a dual rectifier branch, high conversion efficiency in a wide power range is achieved, and the problem that existing antennas are difficult to have both high gain directional radiation and omnidirectional radiation is solved. It is suitable for Ambient RF energy harvesting and wireless energy transmission.
Patent Information
- Application Number
- CN202411610371.1
- Authority / Receiving Office
- CN · China
- Patent Type
- Applications(China)
- Current Assignee / Owner
- Filing Date
- 2024-11-12
- Publication Date
- 2025-01-07
- Estimated Expiration
- 2044-11-12
AI Technical Summary
Existing rectified antennas are difficult to have both high gain directional radiation characteristics and omnidirectional radiation characteristics, and are difficult to achieve high conversion efficiency over a wide power range, limiting their application in two application environments: RF energy collection and wireless energy transmission.
A bi-frequency bidirectional rectifier antenna is designed to achieve directional radiation in the high frequency band and omnidirectional radiation in the low frequency band by etching specific grooves and grooves on a rectangular metal patch, combining L-shaped metal patches and coaxial probes. , and adopts a rectifier circuit with dual rectifier branches to automatically switch the rectifier branches according to the input power to achieve high conversion efficiency in a wide power range.
It achieves high conversion efficiency over a wide power range, meets the dual application requirements of radio frequency energy harvesting and wireless energy transmission systems, and can have high gain directional radiation and omnidirectional radiation characteristics at different frequency bands.
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Figure CN119275556A_ABST
Abstract
Description
Technical Field
[0001] The present invention relates to the field of communication technology, and in particular to a dual-frequency bidirectional rectifying antenna with a wide power range. Background Art
[0002] With the development of information technology, the Internet of Things, Internet of Vehicles, smart homes, environmental monitoring and medical testing are becoming more and more widely used. Sensors are indispensable to them. However, due to the limitations of the working scenarios of sensors, the battery capacity is generally small. Therefore, how to solve the power supply problem has become an important topic. In order to solve the power supply problem of small and low-power devices, wireless power supply methods have emerged. General wireless power supply methods, such as wind power generation, solar power generation, and mechanical power generation, are greatly affected by the environment and the implementation process is relatively complicated. They are not suitable for stable and continuous supply of electricity to small and low-power devices. Radio frequency energy harvesting technology has received widespread attention due to its advantages such as simple conversion process and easy compatibility with wireless communication systems.
[0003] RF energy harvesting is a way of powering electronic devices by collecting electromagnetic waves in space and converting them into direct current. In the RF energy harvesting system, the rectifying antenna is its main component, which consists of a receiving antenna and a rectifying circuit. The receiving antenna is the front-end part of the RF energy harvesting system and is used to capture electromagnetic wave energy in the environment. The rectifying circuit converts the received electromagnetic wave energy into direct current energy and outputs it to the back-end equipment for use.
[0004] RF energy collection can be divided into ambient RF energy collection and wireless energy transmission according to the collection method; in ambient RF linear energy collection technology, the RF energy in free space comes from all directions, so the antenna is required to have omnidirectional radiation characteristics; in directional wireless energy transmission, since the transmitted RF energy comes from a fixed direction, the Friis equation requires the antenna to have high-gain directional radiation characteristics; therefore, in order to be used for both ambient wireless energy collection and directional wireless energy transmission, the antenna is required to have both omnidirectional and high-gain directional radiation characteristics. When performing ambient RF energy collection, the output power of the antenna can be as low as microwatts, while the output power of the antenna can reach more than 20dBm when performing directional wireless energy transmission. Therefore, the rectifier circuit is required to be able to rectify the RF energy output by the antenna within a wide input power range.
[0005] Traditional rectennas are mostly directional antennas and omnidirectional antennas. It is difficult for them to have both high-gain directional radiation characteristics and omnidirectional radiation characteristics. At the same time, it is difficult to achieve high conversion efficiency within a wide power range. As a result, the current rectennas are difficult to be used in both ambient RF energy collection and wireless energy transmission applications, which limits their widespread application. Summary of the invention
[0006] The embodiment of the present invention provides a dual-frequency bidirectional rectenna with a wide power range, which can solve the problem in the prior art that the current rectenna is difficult to have both high-gain directional radiation characteristics and omnidirectional radiation characteristics, and at the same time it is difficult to achieve high conversion efficiency within a wide power range, so that the current rectenna is difficult to be used in both environmental RF energy collection and wireless energy transmission application environments.
[0007] An embodiment of the present invention provides a dual-frequency bidirectional rectifying antenna with a wide power range, comprising a dual-frequency bidirectional receiving antenna and a rectifying circuit;
[0008] The dual-frequency bidirectional receiving antenna comprises a rectangular metal patch arranged on the top surface of the first dielectric substrate, the inner side of the rectangular metal patch is etched with two first rectangular grooves symmetrically about the longitudinal axis of the rectangular metal patch, and the side of the rectangular metal patch is etched with two second rectangular grooves symmetrically about the transverse axis of the rectangular metal patch;
[0009] L-shaped metal patches are respectively arranged on both sides of the rectangular metal patch, and a coaxial probe is passed through the inner side of the rectangular metal patch;
[0010] The rectifier circuit includes a single-branch matching network arranged on the top surface of the second dielectric substrate and connected to the coaxial probe, the single-branch matching network is respectively connected to a first rectifier branch and a second rectifier branch, and the various parts of the rectifier circuit are connected via a microstrip transmission line;
[0011] A first rectangular groove and a second rectangular groove are etched on the rectangular metal patch, so as to make the antenna resonate at a high frequency band and be in a directional radiation mode; L-shaped metal patches are respectively arranged on both sides of the rectangular metal patch, so as to make the antenna resonate at a low frequency band and be in an omnidirectional radiation mode;
[0012] The high-frequency and low-frequency electromagnetic waves received by the antenna in the directional radiation mode and the omnidirectional radiation mode are input into the rectification circuit through the coaxial probe; when the single-branch matching network detects that the electromagnetic wave is a low-power electromagnetic wave, the electromagnetic wave enters the first rectification branch for rectification; when the single-branch matching network detects that the electromagnetic wave is a high-power electromagnetic wave, the electromagnetic wave enters the second rectification branch for rectification.
[0013] Preferably, a defective ground plate is provided on the bottom surface of the first dielectric substrate, and the coaxial probe penetrates the defective ground plate.
[0014] Preferably, the first rectifying branch is composed of a plurality of open branches, a capacitor C1 and a diode D1 are connected between a branch of the first rectifying branch and a branch of the branch matching network, and a terminal branch of the first rectifying branch is connected to a load RL1;
[0015] The diode D1 is a HSMS285B diode.
[0016] Preferably, the second rectifying branch is composed of a plurality of open branches, a capacitor C2 and a diode D2 are connected between a branch of the second rectifying branch and a branch of the single-branch matching network, and a terminal branch of the second rectifying branch is connected to a load RL2;
[0017] The diode D2 is a HSMS286B diode.
[0018] Preferably, the branches contained in the first rectifying branch and the second rectifying branch can form an output pass filter, and the output pass filter is composed of four open branches, and the lengths of the four open branches correspond to a quarter wavelength of 2.45GHz, 4.9GHz, 5.8GHz and 11.6GHz respectively.
[0019] Preferably, the first dielectric substrate is a polytetrafluoroethylene F4B dielectric substrate, the dielectric constant of the dielectric substrate is 2.55, the loss tangent is 0.0017, and the thickness is 2 mm;
[0020] The second dielectric substrate is a Rogers 4350B dielectric substrate, the dielectric constant of the dielectric substrate is 3.66, the loss tangent is 0.0037, and the thickness is 0.762 mm.
[0021] Preferably, the resonant frequency of the dual-frequency bidirectional receiving antenna in the directional radiation mode is 5.8 GHz, and the resonant frequency of the dual-frequency bidirectional receiving antenna in the omnidirectional radiation mode is 2.45 GHz.
[0022] The embodiment of the present invention provides a dual-frequency bidirectional rectifying antenna with a wide power range. Compared with the prior art, the beneficial effects thereof are as follows:
[0023] The present invention etches two first rectangular grooves and a second rectangular groove on a rectangular metal patch respectively, so that the antenna resonates only in a high frequency band and is in a directional radiation mode, and L-shaped metal patches are respectively arranged on both sides of the rectangular metal patch, so that the antenna resonates simultaneously in the high frequency band and the low frequency band, and is in an omnidirectional radiation mode in the low frequency band; and a rectifier circuit combining a rectifier branch working at a low input power and a rectifier branch working at a high input power is designed, and the two rectifier branches switch and rectify the electromagnetic waves collected by the antenna in the high frequency band and the low frequency band through the directional radiation mode and the omnidirectional radiation mode, so as to achieve high conversion efficiency in a wide power range.
[0024] In addition, the antenna can collect electromagnetic waves in dual frequency bands through directional radiation mode and omnidirectional radiation mode, and can be used for environmental RF energy collection and wireless energy transmission systems at the same time. BRIEF DESCRIPTION OF THE DRAWINGS
[0025] Figure 1 A schematic diagram of the front structure of a receiving antenna of a dual-frequency bidirectional rectifying antenna with a wide power range provided by an embodiment of the present invention;
[0026] Figure 2 A schematic diagram of the back structure of a receiving antenna of a dual-frequency bidirectional rectifying antenna with a wide power range provided by an embodiment of the present invention;
[0027] Figure 3 A front structural schematic diagram of a rectifier circuit of a dual-frequency bidirectional rectifier antenna with a wide power range provided by an embodiment of the present invention;
[0028] Figure 4 A schematic diagram of a first rectifying branch of a rectifying circuit of a dual-frequency bidirectional rectifying antenna with a wide power range provided by an embodiment of the present invention;
[0029] Figure 5 A schematic diagram of simulation and test results of the return loss of a receiving antenna of a dual-frequency bidirectional rectifying antenna with a wide power range provided by an embodiment of the present invention;
[0030] Figure 6 A schematic diagram of simulation and test results of a radiation pattern of a receiving antenna at 2.45 GHz of a dual-frequency bidirectional rectenna with a wide power range provided by an embodiment of the present invention;
[0031] Figure 7 A schematic diagram of simulation and test results of a 5.8 GHz radiation pattern of a receiving antenna of a dual-frequency bidirectional rectenna with a wide power range provided by an embodiment of the present invention;
[0032] Figure 8 A schematic diagram of simulation and test results of the conversion efficiency of a rectifier circuit of a dual-frequency bidirectional rectifier antenna with a wide power range at 2.45 GHz varying with input power provided by an embodiment of the present invention;
[0033] Fig. 9 A schematic diagram of simulation and test results of the conversion efficiency of a rectifier circuit of a dual-frequency bidirectional rectenna with a wide power range at 5.8 GHz varying with input power provided by an embodiment of the present invention.
[0034] Wherein: 1. rectangular metal patch, 2. L-shaped metal patch, 3. first rectangular groove, 4. second rectangular groove, 5. defective ground plate, 6. first dielectric substrate, 7. second dielectric substrate, 8. single-branch matching network, 9. diode D1, 10. diode D2, 11. first rectifying branch, 12. second rectifying branch, 13. capacitor C1, 14. capacitor C2, 15. load RL1, 16. load RL2. DETAILED DESCRIPTION
[0035] In order to make the above-mentioned objects, features and advantages of the present invention more obvious and easy to understand, the specific embodiments of the present invention are described in detail below in conjunction with the accompanying drawings. In the following description, many specific details are set forth to facilitate a full understanding of the present invention. However, the present invention can be implemented in many other ways different from those described herein, and those skilled in the art can make similar improvements without violating the connotation of the present invention, so the present invention is not limited by the specific embodiments disclosed below.
[0036] In the description of the present invention, it is to be understood that the terms “center”, “longitudinal”, “lateral”, “length”, “width”, “thickness”, “up”, “down”, “front”, “back”, “left”, “right”, “vertical”, “horizontal”, “top”, “bottom”, “inside”, “outside”, “clockwise”, “counterclockwise”, “axial”, “radial”, “circumferential”, etc., indicating orientations or positional relationships based on the orientations or positional relationships shown in the accompanying drawings, are only for the convenience of describing the present invention and simplifying the description, and do not indicate or imply that the device or element referred to must have a specific orientation, be constructed and operated in a specific orientation, and therefore should not be understood as limiting the present invention.
[0037] In addition, the terms "first" and "second" are used for descriptive purposes only and should not be understood as indicating or implying relative importance or implicitly indicating the number of the indicated technical features. Therefore, the features defined as "first" and "second" may explicitly or implicitly include at least one of the features. In the description of the present invention, the meaning of "plurality" is at least two, such as two, three, etc., unless otherwise clearly and specifically defined.
[0038] In the present invention, unless otherwise clearly specified and limited, the terms "installed", "connected", "connected", "fixed" and the like should be understood in a broad sense, for example, it can be a fixed connection, a detachable connection, or an integral connection; it can be a mechanical connection or an electrical connection; it can be a direct connection or an indirect connection through an intermediate medium, it can be the internal connection of two elements or the interaction relationship between two elements, unless otherwise clearly defined. For ordinary technicians in this field, the specific meanings of the above terms in the present invention can be understood according to specific circumstances.
[0039] In the present invention, unless otherwise clearly specified and limited, a first feature being "above" or "below" a second feature may mean that the first and second features are in direct contact, or the first and second features are in indirect contact through an intermediate medium. Moreover, a first feature being "above", "above" or "above" a second feature may mean that the first feature is directly above or obliquely above the second feature, or simply means that the first feature is higher in level than the second feature. A first feature being "below", "below" or "below" a second feature may mean that the first feature is directly below or obliquely below the second feature, or simply means that the first feature is lower in level than the second feature.
[0040] It should be noted that when an element is referred to as being "fixed to" or "disposed on" another element, it may be directly on the other element or there may be a central element. When an element is considered to be "connected to" another element, it may be directly connected to the other element or there may be a central element at the same time. The terms "vertical", "horizontal", "upper", "lower", "left", "right" and similar expressions used herein are for illustrative purposes only and do not represent the only implementation method.
[0041] See also Figures 1 to 3 An embodiment of the present invention provides a dual-frequency bidirectional rectifying antenna with a wide power range, including a dual-frequency bidirectional receiving antenna and a rectifying circuit.
[0042] The dual-frequency bidirectional rectifying antenna is composed of a rectangular metal patch 1, an L-shaped metal patch 2, a first rectangular groove 3, a second rectangular groove 4, a defect ground plate 5, a first dielectric substrate 6 and a coaxial probe. The rectangular metal patch 1 and the L-shaped metal patch 2 constitute a radiation patch; the radiation patch is arranged on the top surface of the first dielectric substrate 6, four symmetrical rectangular grooves are etched on the rectangular metal patch 1, two first rectangular grooves 3 are arranged on the left and right sides of the inner side of the rectangular metal patch 1, and two second rectangular grooves 4 are opened on the upper and lower sides of the rectangular metal patch 1.
[0043] Among them, the first dielectric substrate 6 is F4B material with a dielectric constant of 2.55, a loss tangent of 0.0017, and a thickness of 2mm; the length of the rectangular metal patch 1 is 61mm and the width is 24mm; the short side length of the L-shaped metal patch 2 is 32mm, the short side width is 2.5mm, the long side length is 34mm, and the long side width is 3mm; the length of the first rectangular groove 3 is 17.8mm and the width is 2.5mm; the length of the second rectangular groove 4 is 4.5mm and the width is 2mm.
[0044] The rectifier circuit includes a single-branch matching network 8, a diode D1, a diode D2, a first rectifier branch 11, a second rectifier branch 12, a capacitor C1, a capacitor C2, a load RL1 and a load RL2; the output end of the dual-frequency bidirectional receiving antenna is connected to the input end of the rectifier circuit, wherein the various parts of the rectifier circuit are connected through a microstrip transmission line; the single-branch matching network 8 is a matching circuit of the rectifier circuit; the diode D1 and the diode D2 are rectifier diodes of the rectifier circuit, the diode D1 is HSMS285B, and the diode D2 is HSMS28 6B; the first rectifying branch 11 and the second rectifying branch 12 both include output pass filters, which are specifically composed of four microstrip open branches and three microstrip transmission lines, and the lengths of the four open branches correspond to a quarter wavelength of 2.45 GHz, 4.9 GHz, 5.8 GHz and 11.6 GHz, respectively; and the rectifying circuit is arranged on the second dielectric substrate 7, the second dielectric substrate 7 is a Rogers 4350B dielectric substrate with a dielectric constant of 3.66, the thickness of the substrate is 0.762 mm, and the loss tangent is 0.0037.
[0045] The two branches work at high and low input powers respectively, and together achieve high conversion efficiency under a wide input power range. At low input power, most of the RF power is transmitted to the first rectifier branch, while at high input power, most of the RF power is transmitted to the second rectifier branch. At the same time, the first rectifier branch and the second rectifier branch have good impedance matching with the input end at the base frequency, that is, P in =P in1 +P in2 , then the power distribution of the two branches is P in1 / P in2 =|Z in2 | / |Z in1 |. Among them, |Z in1 | represents the input impedance Z of the first rectifier branch in1 The modulus value, |Z in2 | represents the input impedance Z of the second rectifier branch in2 The modulus of the input impedance between the two branches is inversely proportional to the modulus of the input impedance between the two branches. In order to automatically distribute the input power, |Z in1 | needs to increase with the increase of input power, thereby gradually reducing the allocation ratio of RF energy; while |Z in2|It needs to gradually decrease with the increase of input power, so as to gradually increase the distribution ratio of RF energy. Within the entire input power range, the states of the rectifier circuit can be divided into three types: (1) When the input power is low, the input impedance amplitude of the first rectifier branch 11 is much smaller than that of the second rectifier branch 12, most of the power enters the first rectifier branch 11 and is rectified by the diode D1, and the diode D2 of the second rectifier branch 12 is basically in the cut-off state. The conversion efficiency of the rectifier circuit is determined by the rectification efficiency of the first rectifier branch 11; (2) When the input power is medium, the input impedance amplitudes of the first rectifier branch 11 and the second rectifier branch 12 are close, and the power is almost evenly distributed to the two branches. At this time, the diodes D1 and D2 are rectified at the same time; (3) When the input power is high, most of the input power enters the second rectifier branch 12 and is rectified by the diode D2. The diode D1 in the first rectifier branch 11 is basically in the cut-off state. The diode D2 rectifies the RF signal at a higher conversion efficiency than the diode D1 at high input power.
[0046] The input impedance of the diode is shown in formula (1), Z D is the input impedance of the diode, θ on is half of the conduction angle (0<θ on <π / 2), the input admittance of the diode is as shown in formulas (2)-(4):
[0047]
[0048] Y D =1 / Z D =Re(Y D )+jIm(Y D ) (2)
[0049]
[0050] As shown in formula (4), the imaginary part of the diode input admittance Im(Y D ) is a positive inductive reactance, so the imaginary part of the input impedance Im(Z D ) is a negative capacitive reactance. Let the input conductance Re(Y D ) and input susceptance Im(Y D ) for θ on Taking the derivative, the result is as follows:
[0051]
[0052] For the convenience of analysis, the above formula is simplified as follows:
[0053] α=1-cos2θ on (7)
[0054] β=(π-θ on )sinθ on +cos 3 θ on -cosθ on (8)
[0055] The simplified formulas (5) and (6) are:
[0056]
[0057] Formulas (9) and (10) are represented by α and β respectively. When θ on When α and β vary from 0 to π / 2, they are always positive, that is, Re(Y D ) and Im(Y D ) for θ on The derivative of Re(Y D ) and Im(Y D ) is an increasing function, Re(Z D ) and Im(Z D ) is a decreasing function, indicating that the modulus of the real and imaginary parts of the diode input impedance increases with θ on By adding a T-type short-circuit structure after the diode in each branch, the input impedance of the two rectifier branches can be increased and decreased respectively. Taking the first rectifier branch as an example, Figure 4 , short-circuit lines TL3 and TL4 are connected in parallel after microstrip line TL1, and the length of TL4 is λ / 2 corresponding to 2.45GHz. When the input signal is 2.45GHz, TL3 is short-circuited by TL4, and TL1 is adjusted so that the input impedance of the first rectifier branch is an increasing function of the input power; when the input signal is 5.8GHz, the electrical length of TL3 is adjusted to change the overall input impedance of TL1, TL3 and TL4, so that the input impedance of the first rectifier branch at 5.8GHz is also an increasing function of the input power. The second rectifier branch is similar.
[0058] The present invention is based on the high-order mode theory and combines the bidirectional radiation mechanism and the principle of the adaptive power distribution rectifier circuit to design the dual-frequency bidirectional rectifier antenna of the present invention, including:
[0059] Step 1: Simulate and analyze the initial patch antenna. Two first rectangular grooves 3 are etched in the upper rectangular metal patch 1, and the length of the rectangular metal patch 1 is set to 61 mm and the width is set to 24 mm to obtain dual-band high-gain characteristics.
[0060] Step 2: Based on the required resonant frequency of the antenna and without changing the antenna radiation mode, two second rectangular grooves 4 are etched in the upper rectangular metal patch 1. The length of the second rectangular groove 4 is 4.5 mm and the width is 2 mm to achieve an antenna design with single-frequency directional radiation.
[0061] Step 3: Based on the result of step 2, add a new resonant frequency to the antenna and design it to achieve bidirectional radiation; add two L-shaped metal patches 2 at the zero point of the electric field generated by the antenna at 5.8 GHz, achieving omnidirectional radiation at 2.45 GHz and high-gain directional radiation at 5.8 GHz.
[0062] Step 4: The rectifier circuit is a radio frequency rectifier circuit, including a matching circuit, a rectifier diode and a pass-through filter; the matching circuit uses a microstrip single-branch matching network 8; at the same time, based on the principle of adaptive power allocation, the rectifier circuit is composed of two different rectifier branches, the first rectifier branch 11 uses a HSMS285B diode working at a lower power, and the second rectifier branch 12 uses a HSMS286B diode working at a higher power; the pass-through filter is designed with four open branches, and the power distribution of the two rectifier branches is changed to avoid the input impedance of the pass-through filter at the fundamental frequency affecting the input impedance of the rectifier branch; and while suppressing the fundamental frequency and the second harmonic, the input impedance of the pass-through filter is adjusted to a higher value close to the open circuit.
[0063] like Figure 5 The simulation and test results of the return loss of the antenna of the present invention are shown in FIG. Figure 6 The figure shows the simulation and test results of the radiation pattern of the antenna of the present invention at 2.45 GHz. Figure 7 The figure shows the simulation and test results of the radiation pattern of the antenna of the present invention at 5.8 GHz. Figure 8 The figure shows the simulation and test results of the conversion efficiency of the rectifier circuit of the antenna of the present invention at 2.45 GHz as a function of input power. Fig. 9 The figure shows the simulation and test results of the conversion efficiency of the rectifier circuit of the antenna of the present invention at 5.8 GHz as the input power changes. It can be seen from the figure that the antenna operates at 2.45 GHz and 5.8 GHz, and is omnidirectional radiation at 2.45 GHz and high-gain directional radiation at 5.8 GHz. The antenna of the present invention can achieve high conversion efficiency within a wide input power range, which meets the different requirements of the RF energy harvesting system for the antenna radiation pattern in different application scenarios and the requirement that the rectifier circuit maintains high conversion efficiency within a wide input power range.
[0064] The antenna designed by the present invention can be used for environmental radio frequency energy collection and directional wireless energy transmission at the same time; firstly, by slotting the electric field zero point of the high-gain directional antenna to suppress the undesired resonant frequency band, the antenna is made to resonate only at 5.8 GHz and is in a high-gain directional radiation mode; secondly, by adding a pair of bent L-shaped metal patches at the electric field zero points on both sides of the rectangular antenna and reducing the size of the ground plate on both sides, resonance is generated at 2.45 GHz and an omnidirectional radiation mode is achieved without affecting the performance of the antenna at 5.8 GHz, and power is fed through an eccentric coaxial probe; at the same time, the rectifier circuit is composed of two rectifier branches operating at low input power and high input power respectively, and by loading a T-type short-circuit structure after the parallel diode of each branch, the input impedance of the two rectifier branches can be made to show an increasing and decreasing trend respectively, and the input radio frequency power is automatically distributed according to the change of the impedance ratio under different input powers, so that the rectifier branches can be automatically switched under high and low input powers, and finally high conversion efficiency can be achieved in a wide power range.
[0065] When the input signal is 2.45GHz, the conversion efficiency of the rectifier circuit is greater than 50% in the input power range of 9-26dBm; when the input signal is 5.8GHz, the conversion efficiency is greater than 30% in the ranges of 2-11.5dBm and 23.5-27dBm, and greater than 20% in the range of -2-27dBm, which fully proves that the dual-frequency bidirectional rectifying antenna designed by the present invention can achieve high conversion efficiency in a wide input power range.
[0066] The above-mentioned embodiments only express several implementation methods of the present invention, and the descriptions thereof are relatively specific and detailed, but they cannot be understood as limiting the scope of the invention patent. It should be pointed out that, for ordinary technicians in this field, several variations and improvements can be made without departing from the concept of the present invention, and these all belong to the protection scope of the present invention. Therefore, the protection scope of the patent of the present invention shall be subject to the attached claims.
Claims
1. A dual-frequency bidirectional rectifying antenna with a wide power range, characterized in that: include: Dual-frequency two-way receiving antenna and rectifier circuit; The dual-frequency bidirectional receiving antenna comprises a rectangular metal patch (1) arranged on the top surface of a first dielectric substrate (6), the inner side of the rectangular metal patch (1) being symmetrically etched with two first rectangular grooves (3) about the longitudinal axis of the rectangular metal patch (1), and the side of the rectangular metal patch (1) being symmetrically etched with two second rectangular grooves (4) about the transverse axis of the rectangular metal patch (1); L-shaped metal patches (2) are respectively arranged on both sides of the rectangular metal patch (1), and a coaxial probe is passed through the inner side of the rectangular metal patch (1); The rectifier circuit comprises a single-branch matching network (8) arranged on the top surface of a second dielectric substrate (7) and connected to a coaxial probe, the single-branch matching network (8) being respectively connected to a first rectifier branch (11) and a second rectifier branch (12), and various parts of the rectifier circuit being connected via a microstrip transmission line; A first rectangular groove (3) and a second rectangular groove (4) are etched on the rectangular metal patch (1) to make the antenna resonate in a high frequency band and in a directional radiation mode; L-shaped metal patches (2) are respectively arranged on both sides of the rectangular metal patch (1) to make the antenna resonate in a low frequency band and in an omnidirectional radiation mode; The high-frequency band and low-frequency band electromagnetic waves received by the antenna in the directional radiation mode and the omnidirectional radiation mode are input into the rectification circuit through the coaxial probe; when the single-branch matching network (8) detects that the electromagnetic wave is a low-power electromagnetic wave, the electromagnetic wave enters the first rectification branch (11) for rectification; when the single-branch matching network (8) detects that the electromagnetic wave is a high-power electromagnetic wave, the electromagnetic wave enters the second rectification branch (12) for rectification.
2. A dual-frequency bidirectional rectifying antenna with a wide power range according to claim 1, characterized in that: A defective grounding plate (5) is provided on the bottom surface of the first dielectric substrate (6), and the coaxial probe penetrates the defective grounding plate (5).
3. A dual-frequency bidirectional rectifying antenna with a wide power range according to claim 1, characterized in that: The first rectifying branch (11) is composed of a plurality of open branches, a capacitor C1 (13) and a diode D1 (9) are connected between a branch of the first rectifying branch (11) and a branch of the branch matching network (8), and a load RL1 (15) is connected to a terminal branch of the first rectifying branch (11); The diode D1 (9) is a HSMS285B diode.
4. A dual-frequency bidirectional rectifying antenna with a wide power range according to claim 1, characterized in that: The second rectifying branch (12) is composed of a plurality of open branches, a capacitor C2 (14) and a diode D2 (10) are connected between a branch of the second rectifying branch (12) and a branch of the single-branch matching network (8), and a load RL2 (16) is connected to an end branch of the second rectifying branch (12); The diode D2 (10) is a HSMS286B diode.
5. A dual-frequency bidirectional rectifying antenna with a wide power range according to claim 1, characterized in that: The branches contained in the first rectifying branch (11) and the second rectifying branch (12) can form an output straight-through filter, and the output straight-through filter is composed of four open-circuit branches, and the lengths of the four open-circuit branches correspond to a quarter wavelength of 2.45 GHz, 4.9 GHz, 5.8 GHz and 11.6 GHz respectively.
6. A dual-frequency bidirectional rectifying antenna with a wide power range according to claim 1, characterized in that: The first dielectric substrate (6) is a polytetrafluoroethylene F4B dielectric substrate, the dielectric constant of the dielectric substrate is 2.55, the loss tangent is 0.0017, and the thickness is 2 mm; The second dielectric substrate (7) is a Rogers 4350B dielectric substrate, the dielectric constant of the dielectric substrate is 3.66, the loss tangent is 0.0037, and the thickness is 0.762 mm.
7. A dual-frequency bidirectional rectifying antenna with a wide power range according to claim 1, characterized in that: The resonant frequency of the dual-frequency bidirectional receiving antenna in the directional radiation mode is 5.8 GHz, and the resonant frequency of the dual-frequency bidirectional receiving antenna in the omnidirectional radiation mode is 2.45 GHz.
Citation Information
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