WO2012169728A2 - Resonant coil, wireless power transmitter using the same, wireless power receiver using the same - Google Patents
Resonant coil, wireless power transmitter using the same, wireless power receiver using the same Download PDFInfo
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- WO2012169728A2 WO2012169728A2 PCT/KR2012/003152 KR2012003152W WO2012169728A2 WO 2012169728 A2 WO2012169728 A2 WO 2012169728A2 KR 2012003152 W KR2012003152 W KR 2012003152W WO 2012169728 A2 WO2012169728 A2 WO 2012169728A2
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- Prior art keywords
- coil
- wires
- wireless power
- power
- receiving
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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
-
- 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
-
- 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
- H01F27/32—Insulating of coils, windings, or parts thereof
- H01F27/324—Insulation between coil and core, between different winding sections, around the coil; Other insulation structures
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- H—ELECTRICITY
- H02—GENERATION; CONVERSION OR DISTRIBUTION OF ELECTRIC POWER
- H02J—ELECTRIC POWER NETWORKS; 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
-
- H—ELECTRICITY
- H04—ELECTRIC COMMUNICATION TECHNIQUE
- H04B—TRANSMISSION
- H04B5/00—Near-field transmission systems, e.g. inductive or capacitive transmission systems
- H04B5/20—Near-field transmission systems, e.g. inductive or capacitive transmission systems characterised by the transmission technique; characterised by the transmission medium
- H04B5/24—Inductive coupling
- H04B5/26—Inductive coupling using coils
- H04B5/266—One coil at each side, e.g. with primary and secondary coils
-
- 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
- H01F2038/146—Inductive couplings in combination with capacitive coupling
Definitions
- the embodiment relates to a wireless power transmission. More particularly, the embodiment relates to a resonant coil, a wireless power transmitter using the same, and a wireless power receiver using the same used in a wireless power transmission using resonance, in which wires constituting a litz coil used for a wireless power transceiving coil are shorted at a predetermined interval so that the spark can be reduced.
- a wireless power transmission or a wireless energy transfer refers to a technology for wirelessly transferring electric energy to desired devices.
- an electric motor or a transformer employing the principle of electromagnetic induction has been extensively used and then a method for transmitting electric energy by irradiating electromagnetic waves, such as radio waves or lasers, has been suggested.
- electromagnetic waves such as radio waves or lasers
- electric toothbrushes or electric razors which are frequently used in daily life, are charged based on the principle of electromagnetic induction.
- the long-distance transmission using the magnetic induction, the resonance and the short-wavelength radio frequency has been used as the wireless energy transfer scheme.
- a plurality of coils are used for the wireless power transmission.
- litz coils are mainly used for the wireless power transmission.
- the litz coil consists of a plurality of wires and the spark may occur due to potential difference between the wires if one of the wires is open.
- the embodiment is provided to solve the problem of the litz coil and an object of the embodiment is to reduce the spark by shorting the wires of the litz coil at a predetermined interval.
- a coil for wirelessly transmitting or receiving power includes a coil unit formed by winding a plurality of wires insulated from each other; and a capacitor connected to the coil unit, wherein the wires of the coil unit are shorted at a predetermined interval.
- a wireless power transmitter includes a transmission coil for transmitting power supplied from a power source using an electromagnetic induction and a transmission resonant coil coupled with the transmission coil to transmit the power using resonance, wherein at least one of the transmission coil and the transmission resonant coil includes a coil unit formed by winding a plurality of wires which are insulated from each other and shorted at a predetermined interval and a capacitor connected to the coil unit.
- a wireless power receiver for wirelessly receiving power from a wireless power transmitter to transmit the power to a load includes a receiving resonant coil for receiving the power from a transmission resonant coil of the wireless power transmitter by using resonance and a receiving coil for receiving the power from the receiving resonant coil using an electromagnetic induction to transmit the power to the load, wherein at least one of the receiving resonant coil and the receiving coil includes a coil unit formed by winding a plurality of wires which are insulated from each other and shorted at a predetermined interval and a capacitor connected to the coil unit.
- the spark can be reduced even if one of the wires constituting the litz coil used for the wireless power transceiving coil is open.
- FIG. 1 is a view showing the structure of a wireless power transmission system according to one embodiment
- FIG. 2 is a view showing an equivalent circuit of a transmission coil 21 according to one embodiment
- FIG. 3 is a view showing an equivalent circuit of a power source 10 and a transmitter 20 according to one embodiment
- FIG. 4 is a view showing an equivalent circuit of a receiving resonant coil 31, a receiving coil 32, a smoothing circuit 40 and a load 50;
- FIG. 5 is a view showing a wire of the related art and a litz coil according to one embodiment
- FIG. 6 is a view showing the structure of a litz coil according to one embodiment.
- FIG. 7 is a view showing equivalent circuits corresponding to the status of a litz coil according to one embodiment.
- FIG. 1 is a view showing the structure of a wireless power transmission system according to one embodiment.
- Power generated from a power source 10 is transmitted to a transmitter 20 and then transmitted to a receiver 30 that forms a resonant circuit with the transmitter 20 using resonance, that is, has a resonant frequency value equal to that of the transmitter 20.
- the power transmitted to the receiver 30 is transmitted to a load 50 through a rectifier circuit 40.
- the load 50 may be a battery or a device requiring the power.
- the power source 10 is an AC power source to provide AC power having a predetermined frequency.
- the transmitter 20 includes a transmission coil 21 and a transmission resonant coil 22.
- the transmission coil 21 is connected to the power source 10 and AC current is applied to the transmission coil 21.
- the AC current is applied to the transmission coil 21, the AC current is induced to the transmission resonant coil 22, which is physically spaced apart from the transmission coil 21, using the electromagnetic induction.
- the power transmitted to the transmission resonant coil 22 is transmitted to the power receiver 30, which forms a resonant circuit together with the power transmitter 10 using resonance.
- the power can be transmitted between two LC circuits which are impedance-matched.
- the power transmission using the resonance can transmit the power farther than the power transmission using the electromagnetic induction with the high power transmission efficiency.
- the power receiver 30 includes a receiving resonant coil 31 and a receiving coil 32.
- the power transmitted through the transmission resonant coil 22 is received in the receiving resonant coil 31 so that the AC current is applied to the receiving resonant coil 31.
- the power transmitted to the receiving resonant coil 31 is transmitted to the receiving coil 32 using the electromagnetic induction.
- the power transmitted to the receiving coil 32 is rectified through the rectifier circuit 40 and then transmitted to the load 50.
- the transmitting resonant coil of the power transmitter 20 transmits power to the receiving resonant coil of the power receiver 30 using magnetic field.
- the transmitting resonant coil and the receiving resonant coil are magnetically coupled and each of them can operate at resonant frequency. Resonant coupling of the transmitting resonant coil and the receiving resonant coil significantly improves power transmission efficiency between the power transmitter 20 and the power receiver 30.
- FIG. 2 shows the equivalent circuit of the transmission coil 21 according to one embodiment.
- the transmission coil 21 may include an inductor L1 and a capacitor C1 and a circuit having predetermined inductance and capacitance values can be formed by using the inductor L1 and the capacitor C1.
- the capacitor C1 may be a variable capacitor and the impedance matching can be performed by controlling the variable capacitor.
- the equivalent circuit of the transmission resonant coil 22, the receiving resonant coil 31 and the receiving coil 22 may be equal to the equivalent circuit shown in FIG. 2.
- FIG. 3 is a view showing an equivalent circuit of the power source 10 and the transmitter 20 according to one embodiment.
- the transmission coil 21 and the transmission resonant coil 22 may consist of inductors L1 and L2 having predetermined inductance values and capacitors C1 and C2 having predetermined capacitance values, respectively.
- FIG. 4 is a view showing an equivalent circuit of the receiving resonant coil 31, the receiving coil 32, the smoothing circuit 40 and the load 50.
- the receiving resonant coil 31 and the receiving coil 32 may consist of inductors L3 and L4 having predetermined inductance values and capacitors C3 and C4 having predetermined capacitance values, respectively.
- the smoothing circuit 40 may consist of a diode D1 and a smoothing capacitor C5 and can output DC power by converting AC power to the DC power.
- the load 50 is shown as a DC power source of 1.3V, the load 50 may be a battery or a device requiring the DC power.
- a plurality of wires as shown in FIG. 5(b) can be used for the coils 21, 22, 31 and 32.
- the wires are litz wires insulated from each other.
- the litz wires shown in FIG. 5(b) can be obtained by combining a plurality of wires insulated from each other.
- the litz wires can be preferably used because the litz wires can reduce the skin effect.
- the skin effect refers to the phenomenon, in which current flows toward a surface of a wire when time-variable current flows along the wire. If the current flows toward the surface of the wire, the current rarely reach to the center of the wire, so a section area of the wire through which the current flows may be reduced, resulting in the increase of resistance.
- the sectional area of the wire can be enlarged so that the skin effect can be prevented and the sectional area of the total wires can be widened. Thus, it is possible to prevent the resistance components of the coil from being increased.
- the current may flow through each litz wire having a thin thickness. If one of the litz wires is open, potential difference may occur between the litz wire having the open section and other litz wires and between the open section and a non-open section of the litz wire. In the case of high power transmission, the potential difference may generate the spark through the insulating material (cladding) of each litz wire.
- a litz coil consisting of a plurality of wires is shorted at a predetermined interval.
- the short of the litz coil can be achieved by removing an insulating material from each wire at a predetermined interval and then connecting the wires with each other using a conductor.
- the possibility of the spark can be reduced.
- the interval of the short in the litz coil is too narrow, the resistance value may be increased due to the skin effect.
- the wires are shorted at a predetermined interval such that the resistance value caused by the skin effect can be reduced while lowering the possibility of the spark.
- the interval of the short capable reducing the resistance value caused by the skin effect while lowering the possibility of the spark is in the range of about 0.01m to about 100m.
- the above range of about 0.01m to about 100m is illustrative purpose only.
- FIG. 7 is a view showing equivalent circuits corresponding to the status of the litz coil according to one embodiment.
- inductors L1, L2 and L3 represent the inductance components of wires constituting the litz coil and have the same inductance value.
- the potential difference may occur about the open section, so the spark may be generated due to the potential difference between the wires.
- the wires are shorted at a predetermined interval as shown in FIG. 7(c), for instance, if the wires are shorted at the interval of “m” by equally dividing the length of the wire, the potential difference about the open section of the wire may be reduced to 1/m. This is because the shorted region has the same voltage and the same voltage is applied to each inductor.
- the spark caused by the open of the wire can be prevented.
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- Engineering & Computer Science (AREA)
- Power Engineering (AREA)
- Computer Networks & Wireless Communication (AREA)
- Signal Processing (AREA)
- Charge And Discharge Circuits For Batteries Or The Like (AREA)
- Current-Collector Devices For Electrically Propelled Vehicles (AREA)
- Near-Field Transmission Systems (AREA)
Abstract
Disclosed is a coil for wirelessly transmitting or receiving power. The coil includes a coil unit formed by winding a plurality of wires insulated from each other; and a capacitor connected to the coil unit. The wires of the coil unit are shorted at a predetermined interval.
Description
The embodiment relates to a wireless power transmission. More particularly, the embodiment relates to a resonant coil, a wireless power transmitter using the same, and a wireless power receiver using the same used in a wireless power transmission using resonance, in which wires constituting a litz coil used for a wireless power transceiving coil are shorted at a predetermined interval so that the spark can be reduced.
A wireless power transmission or a wireless energy transfer refers to a technology for wirelessly transferring electric energy to desired devices. In the 1800’s, an electric motor or a transformer employing the principle of electromagnetic induction has been extensively used and then a method for transmitting electric energy by irradiating electromagnetic waves, such as radio waves or lasers, has been suggested. Actually, electric toothbrushes or electric razors, which are frequently used in daily life, are charged based on the principle of electromagnetic induction. Until now, the long-distance transmission using the magnetic induction, the resonance and the short-wavelength radio frequency has been used as the wireless energy transfer scheme.
A plurality of coils are used for the wireless power transmission. For instance, litz coils are mainly used for the wireless power transmission. The litz coil consists of a plurality of wires and the spark may occur due to potential difference between the wires if one of the wires is open.
The embodiment is provided to solve the problem of the litz coil and an object of the embodiment is to reduce the spark by shorting the wires of the litz coil at a predetermined interval.
A coil for wirelessly transmitting or receiving power according to the embodiment includes a coil unit formed by winding a plurality of wires insulated from each other; and a capacitor connected to the coil unit, wherein the wires of the coil unit are shorted at a predetermined interval.
A wireless power transmitter according to the embodiment includes a transmission coil for transmitting power supplied from a power source using an electromagnetic induction and a transmission resonant coil coupled with the transmission coil to transmit the power using resonance, wherein at least one of the transmission coil and the transmission resonant coil includes a coil unit formed by winding a plurality of wires which are insulated from each other and shorted at a predetermined interval and a capacitor connected to the coil unit.
A wireless power receiver for wirelessly receiving power from a wireless power transmitter to transmit the power to a load includes a receiving resonant coil for receiving the power from a transmission resonant coil of the wireless power transmitter by using resonance and a receiving coil for receiving the power from the receiving resonant coil using an electromagnetic induction to transmit the power to the load, wherein at least one of the receiving resonant coil and the receiving coil includes a coil unit formed by winding a plurality of wires which are insulated from each other and shorted at a predetermined interval and a capacitor connected to the coil unit.
According to the embodiment, the spark can be reduced even if one of the wires constituting the litz coil used for the wireless power transceiving coil is open.
FIG. 1 is a view showing the structure of a wireless power transmission system according to one embodiment;
FIG. 2 is a view showing an equivalent circuit of a transmission coil 21 according to one embodiment;
FIG. 3 is a view showing an equivalent circuit of a power source 10 and a transmitter 20 according to one embodiment;
FIG. 4 is a view showing an equivalent circuit of a receiving resonant coil 31, a receiving coil 32, a smoothing circuit 40 and a load 50;
FIG. 5 is a view showing a wire of the related art and a litz coil according to one embodiment;
FIG. 6 is a view showing the structure of a litz coil according to one embodiment; and
FIG. 7 is a view showing equivalent circuits corresponding to the status of a litz coil according to one embodiment.
Hereinafter, embodiments will be described in more detail with reference to accompanying drawings.
FIG. 1 is a view showing the structure of a wireless power transmission system according to one embodiment.
Power generated from a power source 10 is transmitted to a transmitter 20 and then transmitted to a receiver 30 that forms a resonant circuit with the transmitter 20 using resonance, that is, has a resonant frequency value equal to that of the transmitter 20. The power transmitted to the receiver 30 is transmitted to a load 50 through a rectifier circuit 40. The load 50 may be a battery or a device requiring the power.
In detail, the power source 10 is an AC power source to provide AC power having a predetermined frequency.
The transmitter 20 includes a transmission coil 21 and a transmission resonant coil 22. The transmission coil 21 is connected to the power source 10 and AC current is applied to the transmission coil 21. As the AC current is applied to the transmission coil 21, the AC current is induced to the transmission resonant coil 22, which is physically spaced apart from the transmission coil 21, using the electromagnetic induction. The power transmitted to the transmission resonant coil 22 is transmitted to the power receiver 30, which forms a resonant circuit together with the power transmitter 10 using resonance.
According to the power transmission using the resonance, the power can be transmitted between two LC circuits which are impedance-matched. The power transmission using the resonance can transmit the power farther than the power transmission using the electromagnetic induction with the high power transmission efficiency.
The power receiver 30 includes a receiving resonant coil 31 and a receiving coil 32. The power transmitted through the transmission resonant coil 22 is received in the receiving resonant coil 31 so that the AC current is applied to the receiving resonant coil 31. The power transmitted to the receiving resonant coil 31 is transmitted to the receiving coil 32 using the electromagnetic induction. The power transmitted to the receiving coil 32 is rectified through the rectifier circuit 40 and then transmitted to the load 50.
The transmitting resonant coil of the power transmitter 20 transmits power to the receiving resonant coil of the power receiver 30 using magnetic field. The transmitting resonant coil and the receiving resonant coil are magnetically coupled and each of them can operate at resonant frequency. Resonant coupling of the transmitting resonant coil and the receiving resonant coil significantly improves power transmission efficiency between the power transmitter 20 and the power receiver 30.
FIG. 2 shows the equivalent circuit of the transmission coil 21 according to one embodiment. As shown in FIG. 2, the transmission coil 21 may include an inductor L1 and a capacitor C1 and a circuit having predetermined inductance and capacitance values can be formed by using the inductor L1 and the capacitor C1. The capacitor C1 may be a variable capacitor and the impedance matching can be performed by controlling the variable capacitor. The equivalent circuit of the transmission resonant coil 22, the receiving resonant coil 31 and the receiving coil 22 may be equal to the equivalent circuit shown in FIG. 2.
FIG. 3 is a view showing an equivalent circuit of the power source 10 and the transmitter 20 according to one embodiment. As shown in FIG. 3, the transmission coil 21 and the transmission resonant coil 22 may consist of inductors L1 and L2 having predetermined inductance values and capacitors C1 and C2 having predetermined capacitance values, respectively.
FIG. 4 is a view showing an equivalent circuit of the receiving resonant coil 31, the receiving coil 32, the smoothing circuit 40 and the load 50.
As shown in FIG. 4, the receiving resonant coil 31 and the receiving coil 32 may consist of inductors L3 and L4 having predetermined inductance values and capacitors C3 and C4 having predetermined capacitance values, respectively. The smoothing circuit 40 may consist of a diode D1 and a smoothing capacitor C5 and can output DC power by converting AC power to the DC power. Although the load 50 is shown as a DC power source of 1.3V, the load 50 may be a battery or a device requiring the DC power.
Meanwhile, a plurality of wires as shown in FIG. 5(b) can be used for the coils 21, 22, 31 and 32. Preferably, the wires are litz wires insulated from each other. Different from the single wire shown in FIG. 5(a), the litz wires shown in FIG. 5(b) can be obtained by combining a plurality of wires insulated from each other.
The litz wires can be preferably used because the litz wires can reduce the skin effect. The skin effect refers to the phenomenon, in which current flows toward a surface of a wire when time-variable current flows along the wire. If the current flows toward the surface of the wire, the current rarely reach to the center of the wire, so a section area of the wire through which the current flows may be reduced, resulting in the increase of resistance.
If the litz wires are employed, the sectional area of the wire can be enlarged so that the skin effect can be prevented and the sectional area of the total wires can be widened. Thus, it is possible to prevent the resistance components of the coil from being increased.
At this time, the current may flow through each litz wire having a thin thickness. If one of the litz wires is open, potential difference may occur between the litz wire having the open section and other litz wires and between the open section and a non-open section of the litz wire. In the case of high power transmission, the potential difference may generate the spark through the insulating material (cladding) of each litz wire.
However, as shown in FIG. 6, according to the embodiment, a litz coil consisting of a plurality of wires is shorted at a predetermined interval. The short of the litz coil can be achieved by removing an insulating material from each wire at a predetermined interval and then connecting the wires with each other using a conductor.
As the number of shorts in the litz coil increases, the possibility of the spark can be reduced. However, if the interval of the short in the litz coil is too narrow, the resistance value may be increased due to the skin effect. Thus, the wires are shorted at a predetermined interval such that the resistance value caused by the skin effect can be reduced while lowering the possibility of the spark.
The interval of the short capable reducing the resistance value caused by the skin effect while lowering the possibility of the spark is in the range of about 0.01m to about 100m. However, the above range of about 0.01m to about 100m is illustrative purpose only.
FIG. 7 is a view showing equivalent circuits corresponding to the status of the litz coil according to one embodiment.
Referring to FIG. 7, inductors L1, L2 and L3 represent the inductance components of wires constituting the litz coil and have the same inductance value.
If there is no open wire as shown in FIG. 7(a), the spark may not occur because the same voltage is generated at the same position of each wire.
If there is one open wire as shown in FIG. 7(b), the potential difference may occur about the open section, so the spark may be generated due to the potential difference between the wires.
If the wires are shorted at a predetermined interval as shown in FIG. 7(c), for instance, if the wires are shorted at the interval of “m” by equally dividing the length of the wire, the potential difference about the open section of the wire may be reduced to 1/m. This is because the shorted region has the same voltage and the same voltage is applied to each inductor.
According to the above construction, the spark caused by the open of the wire can be prevented.
Although embodiments have been described with reference to a number of illustrative embodiments thereof, it should be understood that numerous other modifications and embodiments can be devised by those skilled in the art that will fall within the spirit and scope of the principles of this disclosure. More particularly, various variations and modifications are possible in the component parts and/or arrangements of the subject combination arrangement within the scope of the disclosure, the drawings and the appended claims. In addition to variations and modifications in the component parts and/or arrangements, alternative uses will also be apparent to those skilled in the art.
Claims (13)
- A coil for wirelessly transmitting or receiving power, the coil comprising:a coil unit formed by winding a plurality of wires insulated from each other; anda capacitor connected to the coil unit,wherein the wires of the coil unit are shorted at a predetermined interval.
- The coil of claim 1, wherein the wires are shorted at a predetermined interval in a range of 0.01m to 100m.
- The coil of claim 1, wherein the wires insulated from each other include litz wires.
- The coil of claim 1, wherein the coil unit is a solenoid type coil unit.
- The coil of claim 1, wherein the coil unit is a spiral type coil unit.
- A wireless power transmitter comprising:a transmission coil for transmitting power supplied from a power source using an electromagnetic induction; anda transmission resonant coil coupled with the transmission coil to transmit the power using resonance,wherein at least one of the transmission coil and the transmission resonant coil comprises:a coil unit formed by winding a plurality of wires which are insulated from each other and shorted at a predetermined interval; anda capacitor connected to the coil unit.
- The wireless power transmitter of claim 6, wherein the wires are shorted at a predetermined interval in a range of 0.01m to 100m.
- The wireless power transmitter of claim 6, wherein the wires include litz wires.
- The wireless power transmitter of claim 6, wherein the coil unit is at least one of a solenoid type coil unit and a spiral type coil unit.
- A wireless power receiver for wirelessly receiving power from a wireless power transmitter to transmit the power to a load, the wireless power receiver comprising:a receiving resonant coil for receiving the power from a transmission resonant coil of the wireless power transmitter by using resonance; anda receiving coil for receiving the power from the receiving resonant coil using an electromagnetic induction to transmit the power to the load,wherein at least one of the receiving resonant coil and the receiving coil comprises:a coil unit formed by winding a plurality of wires which are insulated from each other and shorted at a predetermined interval; anda capacitor connected to the coil unit.
- The wireless power receiver of claim 10, wherein the wires are shorted at a predetermined interval in a range of 0.01m to 100m.
- The wireless power receiver of claim 10, wherein the wires include litz wires.
- The wireless power receiver of claim 7, wherein the coil unit is at least one of a solenoid type coil unit and a spiral type coil unit.
Priority Applications (2)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| US14/124,997 US9601269B2 (en) | 2011-06-08 | 2012-04-24 | Resonant coil, wireless power transmitter using the same, wireless power receiver using the same |
| US15/424,179 US10491043B2 (en) | 2011-06-08 | 2017-02-03 | Resonant coil, wireless power transmitter using the same, wireless power receiver using the same |
Applications Claiming Priority (2)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| KR10-2011-0055290 | 2011-06-08 | ||
| KR1020110055290A KR101163956B1 (en) | 2011-06-08 | 2011-06-08 | Resonant coil, apparatus for transmitting and receiveing a wireless power using the same |
Related Child Applications (2)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| US14/124,997 A-371-Of-International US9601269B2 (en) | 2011-06-08 | 2012-04-24 | Resonant coil, wireless power transmitter using the same, wireless power receiver using the same |
| US15/424,179 Continuation US10491043B2 (en) | 2011-06-08 | 2017-02-03 | Resonant coil, wireless power transmitter using the same, wireless power receiver using the same |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| WO2012169728A2 true WO2012169728A2 (en) | 2012-12-13 |
| WO2012169728A3 WO2012169728A3 (en) | 2013-03-28 |
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| Application Number | Title | Priority Date | Filing Date |
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| PCT/KR2012/003152 Ceased WO2012169728A2 (en) | 2011-06-08 | 2012-04-24 | Resonant coil, wireless power transmitter using the same, wireless power receiver using the same |
Country Status (3)
| Country | Link |
|---|---|
| US (2) | US9601269B2 (en) |
| KR (1) | KR101163956B1 (en) |
| WO (1) | WO2012169728A2 (en) |
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| KR101163956B1 (en) * | 2011-06-08 | 2012-07-06 | 엘지이노텍 주식회사 | Resonant coil, apparatus for transmitting and receiveing a wireless power using the same |
| JP6941256B2 (en) * | 2017-03-30 | 2021-09-29 | 株式会社アイシン | Drive device |
| KR102789847B1 (en) * | 2022-10-27 | 2025-04-03 | 세메스 주식회사 | Wireless powerd device for substrates processing device and fabrication method of wireless powerd device for substrates processing device |
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| WO2012018268A1 (en) * | 2010-08-05 | 2012-02-09 | Auckland Uniservices Limited | Inductive power transfer apparatus |
| KR20120033756A (en) | 2010-09-30 | 2012-04-09 | 엘지이노텍 주식회사 | Wireless power transfer system by using electromagnetic resonance mode |
| KR101163956B1 (en) * | 2011-06-08 | 2012-07-06 | 엘지이노텍 주식회사 | Resonant coil, apparatus for transmitting and receiveing a wireless power using the same |
-
2011
- 2011-06-08 KR KR1020110055290A patent/KR101163956B1/en not_active Expired - Fee Related
-
2012
- 2012-04-24 US US14/124,997 patent/US9601269B2/en active Active
- 2012-04-24 WO PCT/KR2012/003152 patent/WO2012169728A2/en not_active Ceased
-
2017
- 2017-02-03 US US15/424,179 patent/US10491043B2/en active Active
Also Published As
| Publication number | Publication date |
|---|---|
| US10491043B2 (en) | 2019-11-26 |
| US20170149292A1 (en) | 2017-05-25 |
| US9601269B2 (en) | 2017-03-21 |
| WO2012169728A3 (en) | 2013-03-28 |
| KR101163956B1 (en) | 2012-07-06 |
| US20140111020A1 (en) | 2014-04-24 |
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