CN108448743B - Consumer Electronics Wireless Power Receiving Devices - Google Patents
- ️Fri Mar 26 2021
CN108448743B - Consumer Electronics Wireless Power Receiving Devices - Google Patents
Consumer Electronics Wireless Power Receiving Devices Download PDFInfo
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Publication number
- CN108448743B CN108448743B CN201810220336.7A CN201810220336A CN108448743B CN 108448743 B CN108448743 B CN 108448743B CN 201810220336 A CN201810220336 A CN 201810220336A CN 108448743 B CN108448743 B CN 108448743B Authority
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- receiving coil
- iron core
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- 2018-03-16 Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
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- H—ELECTRICITY
- H02—GENERATION; CONVERSION OR DISTRIBUTION OF ELECTRIC POWER
- H02J—CIRCUIT ARRANGEMENTS OR SYSTEMS FOR SUPPLYING OR DISTRIBUTING ELECTRIC POWER; SYSTEMS FOR STORING ELECTRIC ENERGY
- H02J50/00—Circuit arrangements or systems for wireless supply or distribution of electric power
- H02J50/10—Circuit arrangements or systems for wireless supply or distribution of electric power using inductive coupling
- H02J50/12—Circuit arrangements or systems for wireless supply or distribution of electric power using inductive coupling of the resonant type
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- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01F—MAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
- H01F27/00—Details of transformers or inductances, in general
- H01F27/24—Magnetic cores
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- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01F—MAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
- H01F27/00—Details of transformers or inductances, in general
- H01F27/28—Coils; Windings; Conductive connections
- H01F27/2823—Wires
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- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01F—MAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
- H01F38/00—Adaptations of transformers or inductances for specific applications or functions
- H01F38/14—Inductive couplings
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- Engineering & Computer Science (AREA)
- Power Engineering (AREA)
- Computer Networks & Wireless Communication (AREA)
- Near-Field Transmission Systems (AREA)
- Coils Of Transformers For General Uses (AREA)
Abstract
本发明涉及一种消费类电子产品无线电能接收装置,采用磁耦合谐振式无线电能收发方式,其电磁接收部分包括接收线圈、接收线圈铁芯,接收线圈铁芯包括铁芯细轴圆柱和位于其两端的铁芯两端圆台;接收线圈的高度与接收线圈铁芯细轴圆柱的长度L相等;所述的接收线圈铁芯细轴圆柱的横截面半径R与接收线圈的半径R2相同;所述的接收线圈铁芯两端圆台的上底面均靠近铁芯细轴圆柱,下底面半径r2与发射线圈1的半径R1相同;上底面半径r1与接收线圈铁芯细轴圆柱的横截面半径R相同。本发明增大了接收线圈铁芯两端的表面曲率,增大了退磁磁力线的路径,减小了接收线圈铁芯细轴圆柱轴线上各点的轴向损耗参数。
The invention relates to a wireless power receiving device for consumer electronic products, which adopts a magnetic coupling resonance wireless power sending and receiving method. Its electromagnetic receiving part includes a receiving coil and a receiving coil iron core. Both ends of the iron core are circular truncated; the height of the receiving coil is equal to the length L of the thin-axis cylinder of the receiving coil iron core; the cross-sectional radius R of the thin-axis cylinder of the receiving coil iron core is the same as the radius R2 of the receiving coil; the The upper bottom surface of the circular table at both ends of the receiving coil iron core is close to the iron core thin axis cylinder, the lower bottom surface radius r2 is the same as the radius R1 of the transmitting coil 1; . The invention increases the surface curvature of the two ends of the iron core of the receiving coil, increases the path of the demagnetizing magnetic force line, and reduces the axial loss parameter of each point on the axis of the thin shaft cylinder of the iron core of the receiving coil.
Description
Technical Field
The invention belongs to the technical field of wireless power transmission, and relates to a wireless power receiving device for consumer electronic products.
Background
The wireless power transmission technology is a novel power supply mode for transmitting electric energy from a power supply end to electric equipment by means of a space intangible soft medium. Compared with the traditional wire power supply mode, the wire power supply device has the advantages of safety, reliability, convenience and the like, is particularly suitable for some special occasions, and therefore receives more and more extensive attention.
The wireless power transmission technology can be classified into an inductive coupling type, a microwave radiation type and a magnetic coupling resonance type. Inductively coupled wireless power transfer utilizes an alternating magnetic field generated by a transmitting coil to couple power to a receiving coil. The transmission distance is very limited, generally within the range of 1cm, and the method is suitable for the application occasions with small power and short distance. The radiation type wireless power transmission utilizes a far field to transmit, the transmission distance is far greater than the geometric dimension of the transmission device, but the transmission power is smaller, the energy transmission direction is greatly limited, the human body and other organisms are seriously injured, and the technology is generally applied to special occasions. The magnetic coupling resonance type wireless power transmission transmits energy through near-field magnetic coupling between 2 inductance coils which resonate at the same frequency, and compared with inductive coupling type energy transmission, the transmission distance is greatly expanded; compared with microwave radiation type energy transmission, the microwave radiation type energy transmission device has small influence on an electromagnetic environment and large transmission power, and therefore receives more and more extensive attention and research.
Although the magnetic coupling resonant wireless energy transmission technology improves the transmission distance, particularly the axial distance, the practicability is greatly improved. However, this technique has an optimum working condition called critical coupling, and the distance corresponding to this condition is the optimum transmission distance. If the magnetic coupling is beyond this range, the magnetic coupling is rapidly weakened, resulting in a rapid drop in the power transmission efficiency and a great deterioration in the transmission performance. In order to increase the transmission distance, a coil structure with an iron core can be adopted, and the magnetic coupling effect between the coils is increased. In the prior art, a receiving coil is wound around a cylindrical iron core, and the magnetic coupling effect is enhanced by a magnetic field generated when the iron core is magnetized. However, the core with such a shape generates a large loss of magnetization, resulting in a reduction in the energy obtained by the receiver coil and a reduction in the transmission efficiency. The defect can be compensated to a certain extent by increasing the core area and the coil length, but the iron core with larger volume and heavier mass brings great inconvenience to the installation and use of the system.
Disclosure of Invention
The invention aims to provide a wireless power receiving device of a consumer electronic product, aiming at the problem that the transmission efficiency of a wireless power transmission system is reduced due to the fact that the magnetic coupling effect is weakened when the wireless power transmission system transmits energy in a long distance. The invention is realized by the following technical scheme:
a wireless electric energy receiving arrangement of consumer electronic product, adopt the magnetic coupling resonant mode wireless electric energy to receive and dispatch the way, its electromagnetic receiving part includes receiving coil, receiving coil iron core, characterized by that, the said receiving coil iron core includes the thin axle cylinder of iron core and iron core both ends round platform located at its both ends; the described connectionThe receiving coil is tightly wound on the thin shaft cylinder of the receiving coil iron core; the height of the receiving coil is equal to the length L of the thin-axis cylinder of the iron core of the receiving coil; the radius R of the cross section of the thin-axis cylinder of the iron core of the receiving coil and the radius R of the receiving coil2The same; the cone angles of the circular truncated cones at the two ends of the receiving coil iron core are defined as alpha; the height h of the circular truncated cones at the two ends of the receiving coil iron core is 1/4 of the length L of the thin-axis cylinder of the receiving coil iron core; the upper bottom surfaces of the round tables at the two ends of the iron core of the receiving coil are close to the thin shaft cylinder of the iron core, and the radius r of the lower bottom surface2Radius R of the transmitter coil 11The same; radius of upper bottom surface r1The radius of the cross section of the thin shaft cylinder is the same as that of the thin shaft cylinder of the coil core; the radius r of the lower bottom surface of the circular truncated cones at two ends of the receiving coil iron core2Radius r of upper bottom surface of circular truncated cone at two ends of iron core of receiving coil1,r1The slope corresponding to half of the cone angle alpha of the truncated cones at the two ends of the iron core of the receiving coil, namely alpha/2, is linearly and uniformly changed to r2(ii) a Setting the axial minimum loss parameter of each point on the thin-axis cylindrical axis of the iron core of the receiving coil as Fzmin(0<Fzmin<1) The number of turns of the receiving coil is N and the wire diameter of the receiving coil is dwireLet z1The length L of the receive coil core bobbin cylinder is calculated using the following equation:
the cone angles of the circular truncated cones at the two ends of the iron core of the receiving coil can be calculated according to the following formula:
number of layers K of receiving coillayer=NdwireL, bus length of receiving coil Lwire=2πNR+πN2dwire/L。
Compared with the existing coil core structure, the invention has the advantages that: the invention utilizes the structures of the round tables at the two ends of the iron core of the receiving coil, increases the surface curvature of the two ends of the iron core of the receiving coil, increases the path of demagnetizing magnetic lines, reduces the axial loss parameters of each point on the axis of the thin-axis cylinder of the iron core of the receiving coil, and simultaneously realizes the aggregation of the magnetic field by the thin-axis cylinder of the iron core of the receiving coil, thereby increasing the magnetic field intensity passing through the receiving coil, enhancing the magnetic coupling effect between the two coils, greatly improving the transmission distance and simultaneously improving the transmission efficiency.
Drawings
FIG. 1 is a schematic diagram of the calculation of loss parameters of a cylindrical iron core;
FIG. 2 is a graph of axial loss parameter distribution at each point on a cylindrical iron core axis;
FIG. 3 is a schematic diagram of an overall consumer electronics wireless power transmission and reception system configuration;
FIG. 4 is a perspective view of a thin-axis cylinder of a receiver coil core according to the present invention;
FIG. 5 is a perspective view of the magnetic focusing low loss receiving coil core with truncated cones at both ends;
FIG. 6 is a schematic diagram of the core structure of the magnetic focusing low loss receiver coil of the present invention;
FIG. 7 is a graph of mutual inductance simulation data analysis in an embodiment of the present invention;
fig. 8 is a graph illustrating an analysis of power transmission efficiency data according to an embodiment of the present invention.
Wherein:
1: the transmitting coil 2: receiving coil
3: magnetic focusing low loss receiving coil core 4: magnetic gathering low-loss receiving coil iron core thin-axis cylinder
5: magnetic gathering low-loss receiving coil iron core two-end round table
Detailed Description
The present invention will be described in further detail with reference to the accompanying drawings and examples.
In order to solve the problems in the prior art, the applicant has conducted various research, when the iron core is subjected to the action of an external magnetic field, the iron core can be remarkably magnetized, two magnetic poles of south and north are formed at two ends, and a demagnetizing magnetic field is generated. Demagnetizing field HinThe relation to the magnetization M can be determined by lossesParameter F, i.e.
Hin=F×M (1)
Effective magnetic field inside the core is
Heff=Hex-Hin (2)
In the formula: hexIs the external magnetic field acting on the core.
L, R shows the length and cross section radius of the
thin axis cylinder4 of the magnetic concentration low loss receiving coil iron core, ρ is the calculation bin on the circular surface with radius R, and θ is the positive included angle between the bin ρ and the x axis. To calculate without loss of generality, P is selected as a calculation field point, and due to the symmetry of the iron core structure, the P point is located on a yz plane and has coordinates of P (0, y)1,z1). To facilitate analysis of the characteristics of the loss parameters, let
Then the axial loss parameter and the radial loss parameter of the
thin shaft cylinder4 of the iron core of the magnetic aggregation low-loss receiving coil are respectively as follows:
wherein
Order to
The following can be obtained: the loss parameter perpendicular to the axial direction of each point on the middle cross section and the axis of the thin-
axis cylinder4 of the iron core of the magnetic gathering low-loss receiving coil is zero, namely
The axial loss parameters of each point on the axis of the
thin shaft cylinder4 of the magnetic gathering low-loss receiving coil iron core are as follows:
the length L of the thin-
axis cylinder4 of the iron core of the magnetic aggregation low-loss receiving coil is as follows:
as shown in FIG. 2, in order to minimize the axial loss parameters of all points on the axis of the thin-
axis cylinder4 of the iron core of the magnetic concentration low-loss receiving coil, z is satisfied1When the number is equal to L,
Fzminthe length L of the magnetic concentration low-loss receiving coil iron core
thin shaft cylinder4 can be obtained by the above formula (7) as the axial minimum loss parameter of each point on the axis of the magnetic concentration low-loss receiving coil iron core
thin shaft cylinder4.
The cone angle of the
truncated cone5 at the two ends of the iron core of the magnetic aggregation low-loss receiving coil
Number of layers of the
receiving coil2
Klayer=Ndwire/L (9)
The total length of the
receiving coil2
lwire=2πNR+πN2dwire/L (10)
In the formula: r is2The radius of the lower bottom surface of the circular
truncated cones5 at the two ends of the iron core of the magnetic gathering low-loss receiving coil is equal to the radius of the lower bottom surface of the circular
truncated cones5 at the two ends of the iron core of the magnetic gathering low-loss receiving coil; r, L are the cross section radius and length of the magnetic gathering low loss receiving coil iron core
thin axis cylinder4; n, dwireThe number of turns and the wire diameter of the
receiving coil2, respectively.
Examples
As shown in fig. 3, the present embodiment includes a function signal generator, a dc regulated power supply, a high frequency power amplifier, a transmitting coil compensating capacitor, a receiving coil compensating capacitor, an external load, a transmitting coil 1, a receiving
coil2, and a magnetic focusing low loss receiving
coil iron core3. The signal generator, the direct current stabilized voltage power supply and the high-frequency power amplifier form an external power supply part; the transmitting coil 1 and the transmitting coil compensation capacitor form an electromagnetic transmitting part, and the resonant frequency of the transmitting coil 1 is matched with the central frequency of a power supply through the transmitting coil compensation capacitor; the magnetic focusing low-loss receiving
coil iron core3, the receiving
coil2 and the receiving coil compensation capacitor form an electromagnetic receiving part, and the resonance frequency of the receiving
coil2 is matched with the central frequency of a power supply through the receiving coil compensation capacitor. The sine model emitted by the function signal generator is sent to a high-frequency power amplifier for amplification, the power amplifier signal output is connected with an electromagnetic transmitting part, an electromagnetic receiving part receives the energy in the transmitting coil 1 through coupling resonance, a
receiving coil2 is connected with an external load, and the external load is connected with an oscilloscope. The DC stabilized voltage power supply provides bias voltage for the power amplifier.
The design method of the invention is shown in fig. 4 and 5, and takes a certain resonant coupling type wireless energy transfer system as an embodiment, and the design given values are as follows:
transmitting coil 1 radius R1Radius R of the receiving
coil2 of 5cm2Axial minimum loss parameter F of each point on the axis of the 2cm magnetic concentration low-loss receiving coil iron core
thin shaft cylinder4zmin0.5, 20 turns N of the receiving
coil2, and the wire diameter d of the receiving
coil2wire=0.2cm。
The design method of the novel wireless power receiving device of the consumer electronic product comprises the following steps:
(1) according to the radius R of the transmitting coil 11And determining the radius r of the lower bottom surfaces of the circular
truncated cones5 at the two ends of the iron core of the magnetic concentration low-loss receiving coil according to the Gauss law of the magnetic field2I.e. r2=R1=5cm;
(2) According to the radius R of a given receiving
coil22Determining the radius R of the cross section of a
thin shaft cylinder4 of the iron core of the magnetic aggregation low-loss receiving coil and the radius R of the upper bottom surface of circular
truncated cones5 at two ends of the iron core of the magnetic aggregation low-loss receiving coil1I.e. R ═ R1=R2=2cm;
(3) According to the cross section radius R of the magnetic aggregation low-loss receiving coil iron core
thin shaft cylinder4 and the axial minimum loss parameter F of each point on the axis of the magnetic aggregation low-loss receiving coil iron core
thin shaft cylinder4zminLet z1L is calculated as: length L of core thin-
axis cylinder4 of magnetic focusing low-loss receiver coil, i.e.
Then L is 4 cm.
(4) Determining the height of the circular
truncated cones5 at two ends of the iron core of the magnetic aggregation low-loss receiving coil according to the length L of the
thin shaft cylinder4 of the iron core of the magnetic aggregation low-loss receiving coil
(5) According to the radius r of the lower bottom surface of the circular
truncated cones5 at two ends of the iron core of the magnetic gathering low-loss receiving coil2The cross section radius R of the
thin shaft cylinder4 of the iron core of the magnetic gathering low-loss receiving coil and the length L of the
thin shaft cylinder4 of the iron core of the magnetic gathering low-loss receiving coil, and the cone angles alpha of the circular
truncated cones5 at the two ends of the iron core of the magnetic gathering low-loss receiving coil are calculated according to the following formula, namely
(6) According to the cross section radius R of the magnetic concentration low-loss receiving coil iron core
thin shaft cylinder4, the length L of the magnetic concentration low-loss receiving coil iron core
thin shaft cylinder4, the number of turns N of the receiving
coil2 and the wire diameter d of the receiving
coil2wireThe following are calculated respectively:
number of layers K of receiving
coil2layer=Ndwire/L=20×0.2/4=1,
The bus length l of the receiving
coil2wire=2πNR+πN2dwire/L=2π×20×2+π×202×0.2/4=314cm。
According to the technical scheme of the invention, the device structure and parameters are as follows:
the sinusoidal signal sent by the function signal generator is sent to a high-frequency power amplifier for amplification, the center frequency of the amplified sinusoidal signal is 8MHz, the amplitude is 14V, the power amplifier signal output is connected with an electromagnetic transmitting part, an electromagnetic receiving part receives energy in a transmitting coil 1 through coupling resonance, the resonance frequency of the transmitting coil 1 and the resonance frequency of a receiving
coil2 are 8MHz through tuning, the receiving
coil2 is connected with an external load, and the external load is connected with an oscilloscope. The DC stabilized voltage power supply provides bias voltage for the power amplifier.
As shown in fig. 3, the transmitting coil 1 and the receiving
coil2 are solenoid coils formed by winding copper wires with a wire diameter of 0.2 cm. The transmitting coil 1 has 10 turns, a radius R of 5cm and a turn pitch of 0.5 mm.
As shown in fig. 6, the radius r of the lower bottom surface of the
truncated cones5 at the two ends of the magnetic concentration low-loss receiving coil core is2The length L and the cross section radius R of a
thin shaft cylinder4 of the magnetic gathering low-loss receiving coil iron core are respectively 4cm and 2cm, the height h of circular
truncated cones5 at two ends of the magnetic gathering low-loss receiving coil iron core is 1cm, and the degree of half of the cone angle alpha, namely alpha/2, of the circular
truncated cones5 at two ends of the magnetic gathering low-loss receiving coil iron core is 71.5 degrees.
And obtaining related simulation data based on the set system platform. Data analysis as shown in fig. 7 and 8, it can be seen that the present invention greatly increases the transmission distance and also improves the transmission efficiency.
The device designed by the invention reduces the axial loss parameters of each point on the axis when the existing coil iron core structure is magnetized, enhances the magnetic field intensity passing through the receiving coil, reduces the volume, the weight and the length of the iron core and has wide market application prospect.
The above description is only exemplary of the present invention and should not be taken as limiting the invention, as any modification, equivalent replacement, or improvement made within the spirit and principle of the present invention should be included in the protection scope of the present invention.
Claims (3)
1. A wireless electric energy receiving arrangement of consumer electronic product, adopt the magnetic coupling resonant mode wireless electric energy to receive and dispatch the way, its electromagnetic receiving part includes receiving coil, receiving coil iron core, characterized by that, the said receiving coil iron core includes the thin axle cylinder of iron core and iron core both ends round platform located at its both ends; the receiving coil is tightly wound on the thin shaft cylinder of the receiving coil iron core; the height of the receiving coil is equal to the length L of the thin-axis cylinder of the iron core of the receiving coil; the radius R of the cross section of the thin-axis cylinder of the iron core of the receiving coil and the radius R of the receiving coil2The same; the cone angles of the circular truncated cones at the two ends of the receiving coil iron core are defined as alpha; the height h of the circular truncated cones at the two ends of the receiving coil iron core is 1/4 of the length L of the thin-axis cylinder of the receiving coil iron core; the upper bottom surfaces of the round tables at the two ends of the iron core of the receiving coil are close to the thin shaft cylinder of the iron core, and the radius r of the lower bottom surface2Radius R of the transmitter coil 11The same; radius of upper bottom surface r1The radius of the cross section of the thin shaft cylinder is the same as that of the thin shaft cylinder of the coil core; the radius r of the lower bottom surface of the circular truncated cones at two ends of the receiving coil iron core2Radius r of upper bottom surface of circular truncated cone at two ends of iron core of receiving coil1,r1The slope corresponding to half of the cone angle alpha of the truncated cones at the two ends of the iron core of the receiving coil, namely alpha/2, is linearly and uniformly changed to r2(ii) a Setting the axial minimum loss parameter of each point on the thin-axis cylindrical axis of the iron core of the receiving coil as Fzmin,<Fzmin<1. The number of turns of the receiving coil is N and the wire diameter of the receiving coil is dwireThe loss parameter of the thin-axis cylinder of the iron core of the magnetic gathering low-loss receiving coil can be measuredCalculating the length L of the thin-axis cylinder of the iron core of the receiving coil, wherein the derivation process is as follows:
for the magnetic gathering low-loss receiving coil iron core thin-axis cylinder, rho is a calculation surface element on a circular surface with the radius of R, and theta is a positive included angle between the surface element rho and an x axis; to calculate without loss of generality, one point P in the yz plane is selected as the calculation field point, and due to the symmetry of the iron core structure, the P coordinate is (0, y)1,z1) (ii) a To facilitate analysis of the characteristics of the loss parameters, let
Then the axial loss parameter and the radial loss parameter of the thin-axis cylinder of the iron core of the magnetic aggregation low-loss receiving coil are respectively as follows:
wherein
Order to
Then the loss parameter perpendicular to the axial direction of each point on the central cross section and the axis of the thin-axis cylinder of the magnetic gathering low-loss receiving coil iron core is zero, namely:
the axial loss parameters of each point on the thin-axis cylindrical axis of the magnetic aggregation low-loss receiving coil iron core are as follows:
the length L of the thin-axis cylinder of the iron core of the magnetic aggregation low-loss receiving coil is as follows:
let z1When L is equal to L, the axial loss parameters of all points on the thin-axis cylindrical axis of the magnetic gathering low-loss receiving coil iron core are all minimum, and at the moment
FzminThe length L of the thin-axis cylinder of the iron core of the receiving coil can be calculated by the following formula:
2. the radio energy receiving device of claim 1, wherein the cone angles of the truncated cones at the two ends of the core of the receiver coil are calculated as follows:
3. the device of claim 1, wherein the number of layers of receiving coils is Klayer=NdwireL, bus length of receiving coil Lwire=2πNR+πN2dwire/L。
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Citations (4)
* Cited by examiner, † Cited by third partyPublication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN101026033A (en) * | 2005-12-01 | 2007-08-29 | 通用电气公司 | Contactless power transfer system |
CN103872800A (en) * | 2014-04-08 | 2014-06-18 | 武汉大学 | Transmitting terminal applied to magnetic resonance wireless power transmission device |
JP2015195256A (en) * | 2014-03-31 | 2015-11-05 | ユニパルス株式会社 | Rotary type non-contact power supply transformer |
CN106024345A (en) * | 2016-07-05 | 2016-10-12 | 湖北第二师范学院 | Adjustable induction device, and wireless energy transmission system and control method thereof |
-
2018
- 2018-03-16 CN CN201810220336.7A patent/CN108448743B/en not_active Expired - Fee Related
Patent Citations (4)
* Cited by examiner, † Cited by third partyPublication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN101026033A (en) * | 2005-12-01 | 2007-08-29 | 通用电气公司 | Contactless power transfer system |
JP2015195256A (en) * | 2014-03-31 | 2015-11-05 | ユニパルス株式会社 | Rotary type non-contact power supply transformer |
CN103872800A (en) * | 2014-04-08 | 2014-06-18 | 武汉大学 | Transmitting terminal applied to magnetic resonance wireless power transmission device |
CN106024345A (en) * | 2016-07-05 | 2016-10-12 | 湖北第二师范学院 | Adjustable induction device, and wireless energy transmission system and control method thereof |
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2023-03-03 | CF01 | Termination of patent right due to non-payment of annual fee |