WO2014109460A1 - Wireless power transmission system for free-position wireless charging of multiple devices - Google Patents
Wireless power transmission system for free-position wireless charging of multiple devices Download PDFInfo
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- WO2014109460A1 WO2014109460A1 PCT/KR2013/009280 KR2013009280W WO2014109460A1 WO 2014109460 A1 WO2014109460 A1 WO 2014109460A1 KR 2013009280 W KR2013009280 W KR 2013009280W WO 2014109460 A1 WO2014109460 A1 WO 2014109460A1
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- coil
- transmitting
- transmitter
- wireless power
- impedance matching
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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
- 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
- H02J50/40—Circuit arrangements or systems for wireless supply or distribution of electric power using two or more transmitting or receiving devices
Definitions
- the present invention relates to a short range wireless power transfer system, and more particularly, to a short range wireless power transfer system using a structure having a uniform mutual inductance between wireless power transceivers.
- the power of the transmitting coil (Tx coil) receiving the AC source signal (Vs) is transferred to the load (impedance Z L ) connected to the receiving coil (Rx coil) according to the magnetic field coupling according to mutual inductance M 12 .
- the power transmission unit including a transmission coil (Tx coil) is provided in a transmitter device for power transmission
- the power reception unit including a reception coil (Rx coil) is provided in various electronic devices that use electric power such as a smartphone and an iPad.
- the electronic device may be positioned close to the power supply to wirelessly supply power to the load (eg, a battery, an operation circuit, etc.) through the Rx coil of the electronic device.
- the strength of the magnetic field coupling between the transmission and reception coils depends on the transmission and reception coil structure, geometric arrangement and position, the distance between the transmission and reception coils.
- the optimal power transfer condition of the wireless power transmission system is changed, so that an additional impedance matching circuit or an optimal impedance matching circuit is provided on the transmitter or receiver side to satisfy the maximum power transfer condition.
- complexity such as a current voltage sensing circuit is required.
- the transmission and reception coupling coil in addition to the transmission and reception resonant coil, is used to satisfy the maximum power transfer condition that varies according to the change in distance, but this method requires limited physical movement of the additional transmission and reception coupling coil. In case of using, there is a problem that is difficult to apply.
- the above document (3) proposed a structure that has a uniform magnetic field distribution at a certain height of the coil by bending the shape of the square coil, but this structure has a disadvantage in that the shape of the coil must be changed mechanically.
- the receiver does not have a uniform magnetic field, there is a disadvantage in that it does not have a uniform mutual inductance or a uniform figure of merit.
- the above document (4) discloses a method of maintaining mutual inductance that varies with the distance of a transmission / reception coil using two loop coils connected in series in which the current direction operates in reverse. This is only possible when the center axes of the transmit and receive coils are coincident, but free positioning of the receiver on a flat panel transmitter is difficult and wireless charging of a plurality of receiving devices placed on the transmitter is difficult.
- the present invention has been made to solve the above problems, and an object of the present invention is to provide a structure having a uniform figure of merit (FoM), that is, a uniform mutual inductance between wireless power transceivers. It is possible to have a constant efficiency regardless of the charging position of the receiver by using only a simple impedance matching circuit without using a complicated adaptive impedance matching circuit or a control circuit separately.
- the present invention provides a short range wireless power transmission system capable of simultaneously transmitting power without difficulty.
- the coil structure for wireless power transmission the current flowing in the direction of the input current applied from one end, from one end to the other end, the nose A coil portion connected to and partially concentric with the coil portion in which the current flows in the direction of the input current, the coil portion flowing in a direction opposite to the input current, and having a relative center position horizontally with each target coil. It is for wireless power transfer according to mutual inductance.
- the target coil may be one coil having a relatively horizontal center of position change, or a plurality of coils having a relatively different horizontal center position.
- the coil structure may have a uniform mutual inductance in a predetermined range.
- the magnetic field at the center of the coil structure may be increased relatively to have uniformity of mutual inductance with other coils.
- Coils constituting the coil structure may be formed using a printed circuit board process or a semiconductor process, and coils formed by being distributed and disposed in a multilayer may be connected through a via hole.
- Each coil part of the coil structure may have a shape wound in a concentric circle or a concentric polygon.
- the coil part in which current flows in the direction of the input current may include a coil part wound to be concentric in the center direction a plurality of times so that the current flows in the direction of the input current.
- the coil unit in which current in a direction opposite to the input current flows may include a coil unit wound in parallel with two or more strands so that a current in a direction opposite to the input current flows.
- the coil unit wound by connecting two or more strands in parallel may be wound single or multiple times.
- the coil structure between one end and the other end, including a coil portion flowing current in the direction of the input current applied from the one end, the current in the direction of the input current.
- the second coil part wound to form two or more concentric lines connected in parallel may be wound single or multiple times.
- the coil structure may further include a third coil part wound so as to be concentric with two or more strands connected in parallel so that a current in a direction opposite to the input current flows.
- the second coil portion may be disposed at the center or the outermost portion.
- the transmitting coil or the receiving coil in the wireless power transmission system for transmitting and receiving power between the transmitter coil and the receiver coil of the receiver by magnetic coupling, the transmitting coil or the receiving coil, one side A first coil part wound from the end to the other end so as to be concentric in the center direction of the single or multiple times so that the current flows in the direction of the input current applied from the one end; And a coil part connected to the first coil part in which current flows in the direction of the input current, the center of the first coil part being coincident with the center and being concentric, and in which a current in a direction opposite to the input current flows, or the center is coincident with the first coil part.
- each of the receiving coils it is possible to have a uniform mutual inductance in a predetermined range between the transmitting coils.
- the uniform mutual inductance may be used to transmit power without changing impedance matching at the transmitter or the receiver.
- the transmitter may comprise means for impedance matching of the transmitting coil between an alternating source signal Vs and the transmitting coil.
- the transmitter includes a source coil connected to an AC source signal that is a voltage source, a current source, or a power source, and coupled to a magnetic field spaced apart from a direct connection to the transmitting coil, by mutual inductance between the source coil and the transmitting coil. Impedance matching can be made.
- a capacitor may be included between one end of the AC source signal and one end of the source coil.
- the transmitter may include a transformer for impedance matching, the primary side of which is connected to an AC source signal which is a voltage source, a current source, or a power source, and the secondary side of the transmitting coil.
- the transmitter may include a capacitor for impedance matching connected between the AC source signal, which is a voltage source, a current source, or a power source, and the transmitting coil.
- the transmitter may include an inductor for impedance matching connected between the AC source signal, which is a voltage source, a current source, or a power source, and the transmitting coil.
- the receiver may comprise means for impedance matching to the load between the receiving coil and the load.
- the receiver may include a load coil connected to a load and coupled to a magnetic field spaced apart from a direct connection with the receiving coil, and impedance matching may be performed by mutual inductance between the receiving coil and the load coil.
- a capacitor may be included between one end of the load coil and one end of the load.
- the receiver may include a transformer for impedance matching, in which the receiving coil and the primary side are connected and the load and the secondary side are connected.
- a capacitor may be included between one end of the secondary side and one end of the load.
- the receiver may include an inductor for impedance matching connected between a load and the receiving coil.
- the receiver may include a capacitor for impedance matching connected between a load and the receiving coil.
- a capacitor may be further included between one end of the inductor and one end of the load.
- the transmitter includes a sensing circuit for sensing a load variation according to the quantity of the receiving coils, and by controlling the means for impedance matching to adjust the input impedance changed according to the load variation through the sensing circuit impedance matching is performed; Can be done.
- a wireless power transmission method includes transmitting power wirelessly using an AC source signal in a transmission coil; And wirelessly receiving the power in a receiving coil spaced apart from the transmitting coil by magnetic coupling, wherein the transmitting coil or the receiving coil is between one end and the other end.
- the adaptive impedance matching circuit since the adaptive impedance matching circuit does not need to be used in accordance with the change of the position between the transceiver, the complexity of the system is low and the price is low.
- the use of a single coil allows free positioning of the receiver and transmitter within the wireless power transmission range or effective wireless charging range with uniform mutual inductance within 20% without additional circuitry.
- 1 is an equivalent circuit of a general electromagnetic induction type wireless power transmission system using each resonant coil of a transceiver.
- FIG. 2 is a view for explaining the concept of a wireless power transmission system according to an embodiment of the present invention.
- FIG 3 is a graph showing transmission and reception maximum power transmission efficiency according to a performance index (FOM) of a wireless power transmission system according to an embodiment of the present invention.
- FOM performance index
- M 12 mutual inductance
- FIG. 5 is an example of a coil structure in accordance with one embodiment of the present invention to have an electrically uniform mutual inductance.
- FIG. 6 is an example of a coil actually manufactured to have the structure of FIG. 5.
- FIG. 9 illustrates a configuration in which the coil structure proposed in FIG. 5 is applied to a transmitter of a wireless power transmission system according to an embodiment of the present invention.
- FIG. 10 shows a detailed configuration in which the coil structure proposed in FIG. 5 is applied to a transmitter of a wireless power transmission system according to an embodiment of the present invention.
- FIG. 11 shows another specific configuration in which the coil structure proposed in FIG. 5 is applied to a transmitter of a wireless power transmission system according to an embodiment of the present invention.
- FIG. 12 shows another specific configuration in which the coil structure proposed in FIG. 5 is applied to a transmitter of the wireless power transmission system according to an embodiment of the present invention.
- FIG. 13 shows another specific configuration in which the coil structure proposed in FIG. 5 is applied to a transmitter of a wireless power transmission system according to an embodiment of the present invention.
- FIG. 14 illustrates a configuration of a receiver of a wireless power transmission system according to an embodiment of the present invention.
- FIG. 15 shows a detailed configuration of a receiver of a wireless power transmission system according to an embodiment of the present invention.
- FIG. 16 shows another specific configuration of a receiver of a wireless power transmission system according to an embodiment of the present invention.
- FIG. 17 shows another specific configuration of a receiver of a wireless power transmission system according to an embodiment of the present invention.
- FIG. 18 shows another specific configuration of a receiver of a wireless power transmission system according to an embodiment of the present invention.
- FIG. 19 shows another specific configuration of a receiver of a wireless power transmission system according to an embodiment of the present invention.
- FIG. 20 is an example in which the structures of FIGS. 11 and 15 are combined.
- FIG. 21 is a view for explaining a magnetic field change of the proposed coil structure of FIG. 5 and the structure in which N 3 and N 4 are removed or N 4 is removed from the structure of FIG. 5.
- FIG. 2 is a view for explaining the concept of a wireless power transmission system according to an embodiment of the present invention.
- a wireless power transmission system includes a transmission (resonance) coil (Tx coil) of a transmitter receiving an AC source signal Vs (magnetic inductance L 1 , in an equivalent circuit).
- the resistance is R 1
- the capacitance for resonance is C 1
- the receiver (resonance) coil (Rx coil) of the receiver is provided with a matching unit (Tx matching unit, Rx matching unit) for impedance matching to the transceiver so that the maximum power can be transmitted by electromagnetic induction or magnetic field coupling according to mutual inductance M 12 .
- the transmitter's Tx matching unit matches the impedance seen by the Tx coil with the input impedance Z in (impedance seen by the source) to reflect the transmitted source signal.
- the Rx matching unit of the receiver for minimizing (removing) the impedance matching effect on the load (impedance Z L ) is conjugated with the impedance seen from the Rx coil toward the load. matching) condition must be established.
- the maximum power transfer efficiency ⁇ (the ratio of the power delivered to the load to the transmitted power) is based on the well-known electromagnetic theory. It can be derived as shown in [Equation 1].
- FOM refers to the figure of merit (FoM) of the transmission and reception system.
- FOM the figure of merit
- f r is the resonant frequency of the transmission / reception coil (transmission coil and reception coil)
- R 1 is the resistance of the transmission coil
- R 2 is the resistance of the reception coil
- M 12 is the mutual inductance of the transmission / reception coil.
- the efficiency ⁇ and the performance index FoM of the system depend on M 12 .
- the transmitter can supply the wireless power with the maximum power transfer efficiency to the receiver (Receiver) as described above mounted on a variety of electronic devices using the power, such as a smart phone, iPad, wireless power transmitter (Transmitter)
- the transmitter coil (Tx coil) of the transmitter and the receiver coil (Rx) of the receiver (Receiver) In a power transmission to a receiver having a fixed or mobile load (eg, battery, device operation circuit, etc.) in space, the transmitter coil (Tx coil) of the transmitter and the receiver coil (Rx) of the receiver (Receiver)
- the coil structure of the present invention can be applied to any one or more of the coils, and even if the adaptive impedance matching circuit is not used in accordance with the change of the position between the corresponding transceivers, it is within 20% according to the above principle as described below.
- Wireless power can be supplied with power delivery efficiency. Since there is a constant mutual inductance within the wireless power transmission distance having such a uniform mutual inductance, a plurality of devices can simultaneously receive wireless power to charge the battery or operate the device.
- FIG. 3 is a graph showing the maximum transmission and reception power transmission efficiency ⁇ according to the figure of merit (FOM) of the wireless power transmission system according to an embodiment of the present invention.
- the maximum power transfer efficiency ⁇ is a case where the maximum power transfer condition is satisfied in the Tx matching unit and the Rx matching unit.
- the efficiency ⁇ increases as the performance index FoM increases.
- the higher the FOM the greater the change in maximum power transfer efficiency ⁇ according to the change in the figure of merit.
- M 12 mutual inductance
- the transmitting coil and the receiving coil are arranged side by side so that their centers coincide with each other, and the thickness of each coil having a radius of 10 cm is a very thin filamentary coil.
- the units are all cm.
- 4B illustrates a mutual inductance value in which the center of the Rx coil is changed according to the moving distance rho in parallel in the y direction in the drawing.
- Such a transmission / reception scheme may be an example of a structure in which a receiver is generally placed on a transmitter (eg, 5 cm distance when two coils coincide in the drawing) and wirelessly charges.
- the coil structure for having a uniform mutual inductance has four portions (N, r 1 , r 2 , r 3 , r 4 ) having different radii from the same center (N). 1 , N 2 , N 3 , N 4 ).
- the outermost coil part N 1 starts at one end receiving the input current (I 0 ) and at least one time (eg, three times) from the outermost radius r 1 (eg, 6.5 cm in Table 1 below).
- each loop coil of N 1 has the same current direction as the input current.
- the loop coils wound by the coil part N 1 are described as being equally spaced, but the present invention is not limited thereto and may be wound at boiling intervals.
- each of the other coils N 2 , N 3 , and N 4 may also be formed of a coil wound multiple times, and in this case, the coils may be wound at equal intervals or boiling intervals.
- Coil N nose extending connected to one end of the part N 2 is not smaller radius than the radius of the innermost coil of the coil N 1 r 2 single loop coil wound so as to have a (e. G., Under the reference 6cm in Table 1) It is preferable (plurally possible in some cases).
- the loop coil (s) of the coil portion N 2 has a predetermined distance from the innermost coil of the coils of the coil portion N 1 , and this interval is preferably different from the interval p 1 of the coils of the coil portion N 1 (in the case of Equal intervals available).
- Coco connected to some N 2 at the end N 3 is part of a coil wound so as to have a (see 5.5cm in Table 1, e.g., below) the outermost small radius r 3 than the inside radius r 2, the two coils constant Coils connected in parallel (eg 5mm in Table 1 below) in parallel (3 or more strands can be connected in some cases and the spacing between them is uneven), and coils of coil parts N 1 and N 2 They are formed once or multiple times so that the direction of current is reversed.
- the coil part N 4 which is connected to the end of the coil part N 3 again (the end of two connected coils), has a radius r 4 smaller than the radius of the inner coil of the coil part N 3 (eg, see 4.5 cm in Table 1 below). Coil wound to have two coils connected in parallel at regular intervals (e.g., see 15mm in Table 1 below). In some cases, more than three strands can be connected in parallel, and the spacing between them is uneven. It is formed in single or multiple times so that the current direction is the same as the coils of the coil parts N 1 , N 2 . FIG.
- the capacitor Cp may be connected for resonant frequency and impedance matching.
- Input current (I 0) it is applied to the coil N 1 in Figure 5 the coil N aI 0 and (1-a) in parallel to the coil of 3 I 0 flows is distributed, as in the nose ⁇ I 0 in the parallel coil of some N 4 And (1- ⁇ ) I 0 are distributed and flowed.
- a and ⁇ can be positive or negative, and the magnitude of the absolute value is less than 2.
- each coil part of a concentric circular shape is configured in the proposed coil structure of the present invention is not limited thereto, and each coil part may be configured in various concentric polygonal shapes, such as a rectangle and a hexagon.
- each coil part is made of a metal conductor wire such as a copper wire has been described as shown in FIG. 6.
- the present invention is not limited thereto. It is also possible.
- four coil parts (N 1 , N 2 , N 3 , N 4 ) are appropriately distributed and arranged on both sides of the substrate such as the printed circuit board or the semiconductor substrate. In this case, the connection between the coil parts formed in each layer may be connected through a via hole or the like.
- the present invention is not limited thereto, and the respective coils N 1 , N 2 , N 3 , N 4 ) does not matter in any position.
- the Rx coil 7 is an example of an actual manufactured Rx coil according to an embodiment of the present invention.
- the Rx coil may be manufactured through a printed circuit board process, and the resonant frequency f r is set to 6.78 MHz.
- the Rx coil may also be manufactured by various methods such as a thin copper wire or a semiconductor process.
- the Rx coil as described above is one example, and the coil structure of the present invention as shown in FIGS. 5 and 6 may be applied to the Rx coil. That is, both the transmission coil (Tx coil) and the reception coil (Rx coil) may be in the form of the coil structure of the present invention as shown in FIGS. 5 and 6, and only the transmission coil (Tx coil) as shown in FIGS. 5 and 6. It may be in the form of the coil structure of the present invention, and only the receiving coil may be in the form of the coil structure of the present invention as shown in FIGS. 5 and 6.
- M 12 mutual inductance
- the transmitting coil (Tx coil) and the receiving coil (Rx coil) have a resonance frequency of 6.78 MHz, the end of the coil part N 4 (the ends of two connected coils) and the coil part N 1 start.
- Capacitor Cp may be connected to an additional 6.78 MHz resonant frequency as shown in FIG. 6 at an appropriate position, such as between the end of coil portion N 4 or the portion where coil portion N 1 starts.
- graphs a and b show a transmission coil having a conventional coil structure using only N 1 and N 2 coil parts except N 3 and N 4 coil parts in the structure of FIG. 6 and a receiving coil having a structure as shown in FIG. 7.
- case 1 moves the center of the receiving coil in the y direction at the coordinates as shown in Figure 4
- case 2 moves the center of the receiving coil in the x direction at the coordinates as shown in Figure 4
- graphs c and d are mutual inductances between a transmitting coil having a structure as shown in FIG. 6 and a receiving coil having a structure as shown in FIG. 7.
- case 2 move the center of the receiving coil in the x direction horizontal to the coil plane at the coordinates as shown in FIG. 4).
- FIG. 9 illustrates a configuration in which the coil structure proposed in FIG. 5 is applied to a transmitter of a wireless power transmission system according to an embodiment of the present invention.
- both ends of the coil proposed in the present invention may be connected to both ends of an impedance matching unit (Tx matching unit) of the transmitter to be used as a transmission coil (Tx coil), in which case the transmission coil (Tx coil)
- Tx matching unit impedance matching unit
- the proposed coil can be equivalent to the resistance R p and the inductance L p as a whole, and between one end of the proposed coil, which is a Tx coil, and one end of the transmitter's Tx matching unit, Capacitor C p may be connected.
- the C p is used for matching the resonant frequency and impedance, and in addition, the capacitor C p may be connected in various forms such as between the end of the coil portion N 4 and the portion where the coil portion N 1 starts.
- FIG. 10 shows a detailed configuration in which the coil structure proposed in FIG. 5 is applied to a transmitter of a wireless power transmission system according to an embodiment of the present invention.
- a source coil (a magnetic inductance L s in an equivalent circuit and a resistor R s ) is connected across an AC source signal Vs (voltage source, current source, or power source).
- Capacitor C s can be connected to either end of the source coil and has a capacitor C p , which is a transmit (resonant) coil spaced apart from the source coil by magnetic coupling.
- One proposed coil (magnetic equivalent inductance L p , equivalent resistance R p ) is provided.
- the source coil and the transmit (resonant) coil (Tx coil) are not directly connected, but are separated by a magnetic field, and mutual inductance M 1 between the source coil and the transmit (resonant) coil (Tx coil) By controlling the impedance matching to function as an impedance matching unit (Tx matching unit).
- the capacitor C S between one end of the AC source signal Vs and one end of the source coil may be used for resonance with the transmission (resonance) coil of the source coil. This is not necessary.
- FIG. 11 shows another specific configuration in which the coil structure proposed in FIG. 5 is applied to a transmitter of a wireless power transmission system according to an embodiment of the present invention.
- the transformer primary side (magnetic inductance L s1 in the equivalent circuit, R s1 in the equivalent circuit) is connected across the AC source signal Vs (voltage source, current source, or power source), and the transformer secondary side is connected.
- Vs voltage source, current source, or power source
- the transformer secondary side is connected.
- the magnetic inductance L T1, resistors R T1 of transmission (resonance) coil (Tx coil) across the capacitor C p is in the proposed coil (equivalent circuit having both ends self-inductance L p, the resistance R p ).
- the transformer functioning as an impedance matching unit may be a structure in which primary and secondary coils are wound around an air core structure, or primary and secondary coils in a material containing a magnetic material, such as a ferrite core. This may be a wound structure.
- FIG. 12 shows another specific configuration in which the coil structure proposed in FIG. 5 is applied to a transmitter of the wireless power transmission system according to an embodiment of the present invention.
- a capacitor C m1 functioning as an impedance matching unit is connected across the AC source signal Vs (voltage source, current source, or power source), and the capacitor is connected in parallel. It is also possible to equip the proposed coil with magnetic current (magnetic inductance L p , equivalent resistance R p ) with C p as a transmitting (resonant) coil (Tx coil).
- FIG. 13 shows another specific configuration in which the coil structure proposed in FIG. 5 is applied to a transmitter of a wireless power transmission system according to an embodiment of the present invention.
- an inductor L m1 functioning as an impedance matching unit is connected across an AC source signal Vs (voltage source, current source, or power source), and a capacitor is connected in parallel. It is also possible to equip the proposed coil with magnetic current (magnetic inductance L p , equivalent resistance R p ) with C p as a transmitting (resonant) coil (Tx coil).
- a matching circuit using various combinations of coils, transformers, capacitors, and inductors may be used.
- FIG. 14 illustrates a configuration of a receiver of a wireless power transmission system according to an embodiment of the present invention.
- the coil structure shown in FIG. 7 or the proposed coil structure shown in FIG. 5 may be applied to the Rx coil described below.
- the load (impedance Z L ) may be a circuit for charging the battery or operating the device.
- C 2 is used to adjust the resonant frequency and impedance matching of the Rx coil.
- FIG. 15 shows a detailed configuration of a receiver of a wireless power transmission system according to an embodiment of the present invention.
- a receiving (resonant) coil Rx coil (self-inductance L 2 , resistance R 2 , capacitance C 2 ), which is a receiving self resonant coil
- a load coil magnetic inductance L L in the equivalent circuit, R L in the equivalent circuit coupled with the magnetic coupling thereof, and a capacitor C L may be connected to either end of the load coil.
- a load is connected to both ends of the coil (or both ends via the capacitor C L ) to form a structure that consumes power.
- the capacitor C L between one end of the load coil and one end of the load can be used for matching the resonant frequency or impedance of the load coil of the source coil. This is not necessary and may be removed in some cases.
- the impedance matching may be performed by adjusting the mutual inductance M L between the Rx coil and the load coil to function as an Rx matching unit.
- FIG. 16 shows another specific configuration of a receiver of a wireless power transmission system according to an embodiment of the present invention.
- both ends of a receiving (resonant) coil (Rx coil) (self-inductance L 2 , resistance R 2 , capacitance C 2 ) in a receiving self resonant coil
- Rx coil receiving (resonant) coil
- To the transformer primary side (magnetic inductance L T2 in the equivalent circuit, R T2 in resistance) and the load across the transformer secondary side (magnetic inductance L L2 in the equivalent circuit, R L2 in resistance) (or both ends via capacitor C L2 ) (Impedance Z L ) is connected to form a structure that consumes power.
- Capacitor C L2 between one end of the transformer secondary and one end of the load can be used for impedance matching, which is not necessary and can be removed in some cases.
- the transformer functioning as an impedance matching unit may be a structure in which primary and secondary coils are wound around an air core structure, or primary and secondary materials in a material including a magnetic material, such as a ferrite core. It may be a structure in which the side coil is wound.
- FIG. 17 shows another specific configuration of a receiver of a wireless power transmission system according to an embodiment of the present invention.
- both ends of a receiving (resonant) coil (Rx coil) (self-inductance L 2 , resistance R 2 , and capacitance C 2 ) are self-resonant coils.
- An inductor L m2 which functions as an impedance matching unit is connected, and a load (impedance Z L ) is connected to both ends of the inductor L m2 (or both ends via the capacitor C m ) to consume power. Achieve.
- Capacitor C m between one end of inductor L m2 and one end of load (impedance Z L ) can be used for impedance matching, which is not necessary and can be eliminated in some cases.
- FIG. 18 shows another specific configuration of a receiver of a wireless power transmission system according to an embodiment of the present invention.
- both ends of a receiving (resonant) coil (Rx coil) (self-inductance L 2 , resistance R 2 , and capacitance C 2 ) in a self-resonant coil are received.
- the capacitor C m which functions as an impedance matching unit, is connected, and a load (impedance Z L ) is connected to both ends of the capacitor C m to form a structure that consumes power.
- FIG. 19 shows another specific configuration of a receiver of a wireless power transmission system according to an embodiment of the present invention.
- the receiver is a receiving (resonant) coil (Rx coil) which is a self-resonant coil (self-inductance L 2 in the equivalent circuit, the resistance R 2 , the capacitance C 2 ) both ends
- the inductor L m2 which functions as an impedance matching unit, is connected, and a load (impedance Z L ) is connected to both ends of the inductor L m2 to form a structure that consumes power. This is a case where the capacitor C m is removed from FIG. 17.
- FIG. 20 is an example in which the structures of FIGS. 11 and 15 are combined.
- the transformer primary side (magnetic inductance L s1 in the equivalent circuit and the resistance R s1 ) is connected across the AC source signal Vs (voltage source, current source, or power source), and the transformer secondary side is connected.
- the magnetic inductance L T1, resistors R T1 of transmission (resonance) coil (Tx coil) across the capacitor C p is in the proposed coil (equivalent circuit having both ends self-inductance L p, the resistance R p ).
- the transformer functioning as an impedance matching unit may be a structure in which primary and secondary coils are wound around an air core structure, or primary and secondary coils in a material containing a magnetic material, such as a ferrite core. This may be a wound structure.
- the receiving (resonating) coil (Rx coil) of the receiver (coupled with the mutual inductance M 12 ) and the inductance M 12 (magnetic inductance L 2 in the equivalent circuit, the resistance is R 2 , the capacitance is C 2 ) and a load coil (magnetic inductance L L in the equivalent circuit, R L in the equivalent circuit) coupled to the magnetic coupling, and any of the load coil
- One end of the capacitor C L may be connected, and a load (impedance Z L ) is connected to both ends of the load coil (or both ends via the capacitor C L ) to form a structure that consumes power.
- the capacitor C L between the load coil and the load can be used for matching the resonant frequency or impedance of the load coil of the source coil, which is not necessary and Can be removed accordingly.
- the impedance matching may be performed by adjusting the mutual inductance M L between the Rx coil and the load coil to function as an Rx matching unit.
- Coil structure having a uniform mutual inductance may have a variety of forms, in particular, the coil structure as shown in Figure 5 proposed in the present invention uses a plurality of coils connected in series, each coil (N 1 , N 2 , N 3 , N 4 ,) may be connected at equal intervals or boiling intervals, there are also a structure in which a plurality of coils are connected in parallel, such a parallel structure may be a coil in which the current flows in the direction opposite to the input current direction, the input current direction The coil may be a current flowing in the same direction.
- the present invention is not limited thereto, and the coils N 1 , N 2 , and N 3 are not limited thereto. , N 4 ) does not matter in any position.
- Such a coil structure increases the magnetic field of at least the weak magnetic field (central in the proposed coil structure), thereby increasing the magnetic field as a whole, around the coil structure (within a certain distance from the center), for example (maximum mutual inductance-minimum).
- the mutual inductance can be maintained to satisfy the mutual inductance) / maximum mutual inductance ⁇ 0.2. This is not done by changing the shape of the coil, but is obtained by adjusting the arrangement of the coil. This was confirmed through simulation results, as shown in FIG. 21. That is, FIG. 21 is a simulation result of the magnetic field H z at a height of 1 cm from each coil structure (H 1 , H 2 , H 3 ), and the graph H 3 removes N 3 and N 4 from the structure of FIG. 5.
- the graph H 2 is the result when N 4 is removed from the structure of FIG. 5, and the graph H 1 is the same as that of FIG. 5.
- the magnetic field of the periphery where the magnetic field is weaker than the center may be reduced in the case of H 1 than in H 2 or H 3 , but this is merely an example, and each coil N 1 , N 2 , N 3 , N
- the magnetic field in the periphery may increase or decrease depending on the arrangement of 4 ,) or the number of turns of the coil.
- the impedance matching circuit By utilizing the coil structure having such a uniform mutual inductance, even if the mutual position of the transceiver is changed, it has a constant mutual inductance or performance index, so that an impedance matching circuit suitable for a predetermined mutual inductance may be configured in the transceiver. That is, there is no need to change the appropriate impedance matching according to the transceiver position. 9 to 20, the impedance matching circuit has various configurations.
- multiple loads such as when the relative center position horizontally different (allowing vertical position changes within a certain distance) simultaneously receive power wirelessly with each Rx coil from each receiver of a plurality of devices.
- the input impedance (Z in ) of the transmitter may vary depending on the number and position of the Rx coil, but impedance matching by the application of a transmission coil (Tx coil) having a uniform mutual inductance as in the present invention Can be easily implemented.
- the input impedance Z in sensing transmitter ( The variation of the load according to the quantity is sensed through not shown in the figure, and the input impedance Z in according to the quantity is independent of each position of the multiple loads (receiver or Rx coil). ) Can be simply implemented to achieve impedance matching.
- the transmission coil may be appropriately designed to always have high efficiency even at the maximum number of loads or less, and thus impedance matching for multiple devices may be performed.
- the input impedance (Z in ) sensing circuit simply senses the load variation according to the quantity and adjusts the input impedance accordingly so that the resistance value and the inductance of the Tx matching unit of the transmitter are adjusted.
- Control of the resistance, inductance, or capacitance values of the Tx matching unit can be achieved by switching means (e.g. MOSFET, BJT, SCR, Thyrister) so that a separate resistor, inductor, capacitor, etc. can be added or removed from the circuit. And the like).
- switching means e.g. MOSFET, BJT, SCR, Thyrister
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Abstract
Description
본 발명은 근거리 무선 전력전송 시스템에 관한 것으로서, 특히, 무선 전력 송수신기 사이가 균일한 상호 인덕턴스를 갖는 구조를 이용한 근거리 무선 전력전송 시스템에 관한 것이다.The present invention relates to a short range wireless power transfer system, and more particularly, to a short range wireless power transfer system using a structure having a uniform mutual inductance between wireless power transceivers.
도 1은 송수신기의 각각의 공진코일을 사용한 일반적인 전자기 유도 방식 무선 전력전송 시스템의 등가회로이다. 송신 코일(Tx coil)의 자기 인덕턴스 L1, 저항은 R1, 공진을 위한 정전용량은 C1이고, 수신 코일(Rx coil)의 자기 인덕턴스 L2, 저항은 R2, 공진을 위한 정전용량은 C2일 때, 교류 소스 신호(Vs)를 받는 송신 코일(Tx coil)의 전력이 상호 인덕턴스 M12에 따른 자기장 결합에 따라 수신 코일(Rx coil)에 연결된 부하(임피던스 ZL)로 전력이 전달될 수 있다. 송신 코일(Tx coil)을 포함한 송전부는 전력 송신을 위한 송신기 장치에 구비되며, 수신 코일(Rx coil)을 포함한 수전부는 스마트폰, 아이패드 등 전력을 사용하는 각종 전자기기에 구비되고, 송전부에 가까이 전자기기를 위치시켜 놓고 전자기기의 수신 코일(Rx coil)을 통해서 부하(예, 배터리, 동작 회로 등)에 무선으로 전력이 공급되도록 할 수 있다. 1 is an equivalent circuit of a general electromagnetic induction type wireless power transmission system using each resonant coil of a transceiver. The magnetic inductance L 1 of the transmitting coil (Tx coil), the resistance is R 1 , the capacitance for resonance is C 1 , the magnetic inductance L 2 of the receiving coil (Rx coil), the resistance is R 2 , and the capacitance for resonance is When C 2 , the power of the transmitting coil (Tx coil) receiving the AC source signal (Vs) is transferred to the load (impedance Z L ) connected to the receiving coil (Rx coil) according to the magnetic field coupling according to mutual inductance M 12 . Can be. The power transmission unit including a transmission coil (Tx coil) is provided in a transmitter device for power transmission, and the power reception unit including a reception coil (Rx coil) is provided in various electronic devices that use electric power such as a smartphone and an iPad. The electronic device may be positioned close to the power supply to wirelessly supply power to the load (eg, a battery, an operation circuit, etc.) through the Rx coil of the electronic device.
그런데, 이와 같은 무선 전력전송 시스템에서, 위와 같은 송수신 코일들(Tx coil, Rx coil) 사이의 자기장 결합의 세기는 송수신 코일 구조, 기하학적 배치 및 위치, 송수신 코일 사이의 거리에 따라서 달라진다. 다양한 환경의 변화에 따라, 송수신 코일 사이의 자기장 결합 세기가 변경될 경우 무선전력전송 시스템의 최적 전력전달 조건이 변경되어, 최대 전력전달 조건을 만족하기 위해 송신기 또는 수신기 측에 추가적인 임피던스 정합회로 또는 최적 전력전달 조건 제어를 위하여 전류 전압 센싱 회로 등 복잡성이 요구된다. 특히, 평판형 송신기를 사용할 경우, 평판 위에 놓여진 수신기의 위치에 따라 최적 임피던스 정합을 시켜주어야 하기 때문에, 송신기와 수신기 사이의 자유로운 위치(Free positioning)에서의 무선 전력 전송을 지원하기가 어려운 문제점이 있다. 또한, 위치마다 송수신 코일 사이의 상호 인덕턴스가 다르거나, 다중기기가 서로 다른 위치에 놓여 전력을 수신하게 되면 송신기측에서는 개별 기기마다 다른 임피던스 정합의 어려움이 있어서 다중기기에 동시에 전력 전송을 지원할 수 없는 문제점이 있다. However, in such a wireless power transmission system, the strength of the magnetic field coupling between the transmission and reception coils (Tx coil, Rx coil) as described above depends on the transmission and reception coil structure, geometric arrangement and position, the distance between the transmission and reception coils. As the magnetic field coupling strength between the transmitting and receiving coils changes according to various environmental changes, the optimal power transfer condition of the wireless power transmission system is changed, so that an additional impedance matching circuit or an optimal impedance matching circuit is provided on the transmitter or receiver side to satisfy the maximum power transfer condition. In order to control the power delivery condition, complexity such as a current voltage sensing circuit is required. In particular, when a flat panel transmitter is used, it is difficult to support wireless power transmission at a free position between the transmitter and the receiver because an optimum impedance must be matched according to the position of the receiver placed on the flat panel. . In addition, if the mutual inductance between the transmitting and receiving coils are different for each position, or if the multiple devices are located at different positions to receive power, the transmitter may have difficulty in matching impedances to the individual devices, and thus it may not support power transmission to the multiple devices at the same time. There is this.
송수신기 간의 최대 전력 전달을 위한 종래의 무선 전력전송 기술과 관련하여, 다양한 문헌들이 존재하지만 그 중 다음과 같은 4가지 문헌들을 소개한다.Regarding the conventional wireless power transfer technology for maximum power transfer between the transceivers, various documents exist, but the following four documents are introduced.
(1) A. Kurs, A. Karalis, R. Moffatt, J. D. Joannopoulos, P. Fisher, and M. Soljacic, "Wireless power transfer via strongly coupled magnetic resonances", Science, vol. 317, pp. 83-86, July 2007.(1) A. Kurs, A. Karalis, R. Moffatt, J. D. Joannopoulos, P. Fisher, and M. Soljacic, "Wireless power transfer via strongly coupled magnetic resonances", Science, vol. 317, pp. 83-86, July 2007.
(2) J. Park, Y. Tak, Y. Kim, Y. Kim, S. Nam, "Investigation of adaptive matching methods for near-field wireless power transfer", IEEE Transactions on Antennas and Propagation, vol. 59, pp. 1769-1773, May 2011.(2) J. Park, Y. Tak, Y. Kim, Y. Kim, S. Nam, "Investigation of adaptive matching methods for near-field wireless power transfer", IEEE Transactions on Antennas and Propagation, vol. 59, pp. 1769-1773, May 2011.
(3) W.S. Lee, H.L. Lee, K.S. Oh, and J.W. Yu, "Uniform magnetic field distribution of a spatially structured resonant coil for wireless power transfer" Applied physics Letters 100, 2012.(3) W.S. Lee, H.L. Lee, K.S. Oh, and J.W. Yu, "Uniform magnetic field distribution of a spatially structured resonant coil for wireless power transfer"
(4) W. S. Lee, W. I. Son, K. S. Oh, and J. W. Yu, "Contactless energy transfer systems using antiparallel resonant loops" IEEE transactions on industrial electronics, Vol. 60, No. 1, January 2013.(4) W. S. Lee, W. I. Son, K. S. Oh, and J. W. Yu, "Contactless energy transfer systems using antiparallel resonant loops" IEEE transactions on industrial electronics, Vol. 60, no. 1, January 2013.
위의 문헌(1)에서는 송수신 공진 코일에 추가적으로 송수신 커플링 코일을 사용하여 거리의 변동에 따라 달라지는 최대 전력전달 조건을 만족하도록 하였지만, 이 방법은 추가된 송수신 결합 코일을 물리적으로 움직여야 하기 때문에 제한된 공간을 이용한 경우에는 적용이 어려운 문제점이 있다.In the above document (1), in addition to the transmission and reception resonant coil, the transmission and reception coupling coil is used to satisfy the maximum power transfer condition that varies according to the change in distance, but this method requires limited physical movement of the additional transmission and reception coupling coil. In case of using, there is a problem that is difficult to apply.
위의 문헌(2)에서는 송수신 공진 코일의 거리에 따라, 최대 전력 전달을 위하여 최적 주파수를 트래킹하는 방법으로서 거리에 따라 커플링이 달라지면서 나타나는 송수신 투과 특성의 분할(Splitting) 현상을 이용하는 구성을 개시하지만, 근거리 무선전력전송을 위한 주파수가 고정된 경우 이러한 주파수 트래킹 방법을 사용하기는 어려운 문제점이 있다.In the above document (2), a method of tracking an optimum frequency for maximum power transmission according to the distance of a transmission / reception resonance coil is disclosed. However, when the frequency for short range wireless power transmission is fixed, it is difficult to use such a frequency tracking method.
위의 문헌(3)에서는 사각 코일의 모양을 휘게하여 코일의 일정 높이에서 균일한 자기장 분포를 갖도록 하는 구조를 제안하였지만, 이 구조는 기계적으로 코일의 모양을 변경해야 하는 단점이 있다. 또한, 수신기가 균일 자기장을 갖지 않으면, 균일 상호 인덕턴스 또는 균일 성능 지수를 갖지 못하는 단점이 있다.The above document (3) proposed a structure that has a uniform magnetic field distribution at a certain height of the coil by bending the shape of the square coil, but this structure has a disadvantage in that the shape of the coil must be changed mechanically. In addition, if the receiver does not have a uniform magnetic field, there is a disadvantage in that it does not have a uniform mutual inductance or a uniform figure of merit.
위의 문헌 (4)는 전류 방향이 반대로 동작하는 직렬 연결된 두 개의 루프 코일을 활용하여 송수신 코일의 거리에 따라 변화되는 상호 인덕턴스를 유지하는 방법을 개시한다. 이는 송수신 코일의 중심축이 일치된 경우에 대해서만 가능하지만, 평판형 송신기 위에서 수신기의 Free positioning이 어렵고, 또한 송신기 위에 놓인 복수의 수신 기기에 대한 무선 충전이 어렵다.The above document (4) discloses a method of maintaining mutual inductance that varies with the distance of a transmission / reception coil using two loop coils connected in series in which the current direction operates in reverse. This is only possible when the center axes of the transmit and receive coils are coincident, but free positioning of the receiver on a flat panel transmitter is difficult and wireless charging of a plurality of receiving devices placed on the transmitter is difficult.
본 발명은 상술한 문제점을 해결하기 위한 것으로서, 본 발명의 목적은, 무선 전력 송수신기 사이가 균일한 성능 지수(Figure of merit: FoM), 즉, 균일한 상호 인덕턴스를 갖는 구조를 적용함으로써, 기존과 같이 복잡한 적응형 임피던스 정합회로나 제어 회로를 별도로 사용하지 않고도 간단한 임피던스 정합 회로만을 사용하여 수신기의 충전 위치에 상관없이 일정한 효율을 가지게 할 수 있으며, 복수 개의 전자기기로의 무선 전력 전송에서도 임피던스 정합의 어려움 없이 동시에 전력 전송이 가능한 근거리 무선 전력전송 시스템을 제공하는 데 있다. SUMMARY OF THE INVENTION The present invention has been made to solve the above problems, and an object of the present invention is to provide a structure having a uniform figure of merit (FoM), that is, a uniform mutual inductance between wireless power transceivers. It is possible to have a constant efficiency regardless of the charging position of the receiver by using only a simple impedance matching circuit without using a complicated adaptive impedance matching circuit or a control circuit separately. The present invention provides a short range wireless power transmission system capable of simultaneously transmitting power without difficulty.
먼저, 본 발명의 특징을 요약하면, 본 발명의 일면에 따른, 무선 전력 전송을 위한 코일 구조물은, 한쪽 끝에서 다른 쪽 끝 사이에, 상기 한쪽 끝에서 인가되는 입력 전류의 방향으로 전류가 흐르는 코일부와 상기 입력 전류의 방향으로 전류가 흐르는 코일부에 연결되고 그와 동심인, 상기 입력 전류와 반대 방향의 전류가 흐르는 코일부를 포함하고, 상대적인 중심 위치가 수평적으로 다른 각 대상 코일과의 상호 인덕턴스에 따른 무선 전력 전달을 위한 것이다.First, to summarize the features of the present invention, according to one aspect of the present invention, the coil structure for wireless power transmission, the current flowing in the direction of the input current applied from one end, from one end to the other end, the nose A coil portion connected to and partially concentric with the coil portion in which the current flows in the direction of the input current, the coil portion flowing in a direction opposite to the input current, and having a relative center position horizontally with each target coil. It is for wireless power transfer according to mutual inductance.
상기 대상 코일은, 상대적으로 중심이 수평적으로 위치 변동 가능한 하나의 코일, 또는 상대적인 중심 위치가 수평적으로 다르게 놓인 복수의 코일일 수 있다.The target coil may be one coil having a relatively horizontal center of position change, or a plurality of coils having a relatively different horizontal center position.
상기 각 대상 코일에 대하여, 상기 코일 구조물이 미리 결정된 범위의 균일한 상호 인덕턴스를 갖도록 할 수 있다.For each target coil, the coil structure may have a uniform mutual inductance in a predetermined range.
상기 코일 구조물의 중심부의 자기장은 상대적으로 증가시켜, 다른 코일과의 상호 인덕턴스의 균일성을 갖도록 할 수 있다.The magnetic field at the center of the coil structure may be increased relatively to have uniformity of mutual inductance with other coils.
상기 코일 구조물을 이루는 코일들이 인쇄회로기판 공정 또는 반도체 공정을 이용하여 형성되며, 다층에 분산 배치되어 형성된 코일들이 비아(via) 홀을 통해 연결될 수 있다.Coils constituting the coil structure may be formed using a printed circuit board process or a semiconductor process, and coils formed by being distributed and disposed in a multilayer may be connected through a via hole.
상기 코일 구조물의 각 코일부가 동심 원형, 또는 동심 다각형으로 감긴 형태일 수 있다.Each coil part of the coil structure may have a shape wound in a concentric circle or a concentric polygon.
상기 입력 전류의 방향으로 전류가 흐르는 코일부는, 상기 입력 전류의 방향으로 전류가 흐르도록 복수회 중심 방향으로 동심을 이루도록 감긴 코일부를 포함할 수 있다.The coil part in which current flows in the direction of the input current may include a coil part wound to be concentric in the center direction a plurality of times so that the current flows in the direction of the input current.
상기 입력 전류와 반대 방향의 전류가 흐르는 코일부는, 상기 입력 전류와 반대 방향의 전류가 흐르도록 2가닥 이상이 병렬 연결되어 감긴 코일부를 포함할 수 있다.The coil unit in which current in a direction opposite to the input current flows may include a coil unit wound in parallel with two or more strands so that a current in a direction opposite to the input current flows.
상기 2가닥 이상이 병렬 연결되어 감긴 코일부는 단일회 또는 복수회 감길 수 있다.The coil unit wound by connecting two or more strands in parallel may be wound single or multiple times.
또한, 본 발명의 다른 일면에 따른 코일 구조물은, 한쪽 끝에서 다른 쪽 끝 사이에, 상기 한쪽 끝에서 인가되는 입력 전류의 방향으로 전류가 흐르는 코일부를 포함하되, 상기 입력 전류의 방향으로 전류가 흐르도록 단일회 또는 복수회 중심 방향으로 동심을 이루도록 감긴 제1코일부와 상기 중심이 일치하며, 상기 입력 전류의 방향으로 전류가 흐르도록 2가닥 이상이 병렬 연결되어 동심을 이루도록 감긴 제2코일부를 포함하며, 상대적인 중심 위치가 수평적으로 다른 각 대상 코일과 상호 인덕턴스에 따른 무선 전력 전달을 위한 것이다.In addition, the coil structure according to another aspect of the present invention, between one end and the other end, including a coil portion flowing current in the direction of the input current applied from the one end, the current in the direction of the input current The first coil part wound to be concentric in the center direction in a single or multiple times to flow with the center, and the second coil part wound to be concentric in two or more strands connected in parallel so that a current flows in the direction of the input current. It includes, and is for the wireless power transfer according to the mutual inductance with each target coil horizontally different relative center position.
상기 2가닥 이상이 병렬 연결되어 동심을 이루도록 감긴 상기 제2코일부는 단일회 또는 복수회 감길 수 있다.The second coil part wound to form two or more concentric lines connected in parallel may be wound single or multiple times.
상기 코일 구조물은, 상기 입력 전류와 반대 방향의 전류가 흐르도록 2가닥 이상이 병렬 연결되어 동심을 이루도록 감긴 제3코일부를 더 포함할 수 있다.The coil structure may further include a third coil part wound so as to be concentric with two or more strands connected in parallel so that a current in a direction opposite to the input current flows.
상기 제2코일부는 중심부 또는 최외각에 배치될 수도 있다.The second coil portion may be disposed at the center or the outermost portion.
또한, 본 발명의 또 다른 일면에 따른, 자기 결합(magnetic coupling)에 의한 송신기의 송신 코일과 수신기의 수신 코일 간의 전력 송수신을 위한 무선 전력전송 시스템에 있어서, 상기 송신 코일 또는 상기 수신 코일은, 한쪽 끝에서 다른 쪽 끝 사이에, 상기 한쪽 끝에서 인가되는 입력 전류의 방향으로 전류가 흐르도록 단일회 또는 복수회 중심 방향으로 동심을 이루도록 감긴 제1코일부; 및 상기 입력 전류의 방향으로 전류가 흐르는 상기 제1코일부에 연결되고 상기 제1코일부와 상기 중심이 일치하고 동심이며, 상기 입력 전류와 반대 방향의 전류가 흐르는 코일부, 또는 상기 중심이 일치하며, 상기 입력 전류의 방향으로 전류가 흐르도록 2가닥 이상이 병렬 연결되어 동심을 이루도록 감긴 코일부를 포함하고, 상기 송신 코일에서 상대적인 중심 위치가 수평적으로 다른 하나 이상의 각 수신 코일로 전력을 송신하기 위한 것을 특징으로 한다.In addition, according to another aspect of the present invention, in the wireless power transmission system for transmitting and receiving power between the transmitter coil and the receiver coil of the receiver by magnetic coupling, the transmitting coil or the receiving coil, one side A first coil part wound from the end to the other end so as to be concentric in the center direction of the single or multiple times so that the current flows in the direction of the input current applied from the one end; And a coil part connected to the first coil part in which current flows in the direction of the input current, the center of the first coil part being coincident with the center and being concentric, and in which a current in a direction opposite to the input current flows, or the center is coincident with the first coil part. And a coil unit wound in parallel to be concentric with two or more strands connected in parallel so that current flows in the direction of the input current, and transmits power to each of the one or more receiving coils whose center positions are horizontally different from each other in the transmitting coil. It is characterized by.
상기 각 수신 코일에 대하여, 상기 송신 코일과의 사이에 미리 결정된 범위의 균일한 상호 인덕턴스를 갖도록 할 수 있다.For each of the receiving coils, it is possible to have a uniform mutual inductance in a predetermined range between the transmitting coils.
균일한 상기 상호 인덕턴스를 이용하여 상기 송신기 또는 상기 수신기에서 임피던스 매칭을 변경하지 않고 전력을 송신할 수도 있다.The uniform mutual inductance may be used to transmit power without changing impedance matching at the transmitter or the receiver.
상기 송신기는, 교류 소스 신호(Vs)와 상기 송신 코일 사이에, 상기 송신 코일에 대한 임피던스 매칭을 위한 수단을 포함할 수 있다.The transmitter may comprise means for impedance matching of the transmitting coil between an alternating source signal Vs and the transmitting coil.
상기 송신기는, 전압원, 전류원, 또는 전력소스인 교류 소스 신호에 연결되고 상기 송신 코일과는 직접 연결되지 않고 이격되어 자기장으로 결합되는 소스 코일을 포함하고 상기 소스 코일과 상기 송신 코일 간의 상호 인덕턴스에 의해 임피던스 매칭이 이루어질 수 있다.The transmitter includes a source coil connected to an AC source signal that is a voltage source, a current source, or a power source, and coupled to a magnetic field spaced apart from a direct connection to the transmitting coil, by mutual inductance between the source coil and the transmitting coil. Impedance matching can be made.
상기 교류 소스 신호의 한쪽 끝 단과 상기 소스 코일의 한쪽 끝 단 사이에 커패시터를 포함할 수 있다.A capacitor may be included between one end of the AC source signal and one end of the source coil.
상기 송신기는, 전압원, 전류원, 또는 전력소스인 교류 소스 신호와 1차측이 연결되고, 상기 송신 코일과 2차측이 연결된, 임피던스 매칭을 위한 트랜스포머를 포함할 수 있다.The transmitter may include a transformer for impedance matching, the primary side of which is connected to an AC source signal which is a voltage source, a current source, or a power source, and the secondary side of the transmitting coil.
상기 송신기는, 전압원, 전류원, 또는 전력소스인 교류 소스 신호와 상기 송신 코일 사이에 연결된 임피던스 매칭을 위한 커패시터를 포함할 수 있다.The transmitter may include a capacitor for impedance matching connected between the AC source signal, which is a voltage source, a current source, or a power source, and the transmitting coil.
상기 송신기는, 전압원, 전류원, 또는 전력소스인 교류 소스 신호와 상기 송신 코일 사이에 연결된 임피던스 매칭을 위한 인덕터를 포함할 수 있다.The transmitter may include an inductor for impedance matching connected between the AC source signal, which is a voltage source, a current source, or a power source, and the transmitting coil.
상기 수신기는, 상기 수신 코일과 부하 사이에, 상기 부하에 대한 임피던스 매칭을 위한 수단을 포함할 수 있다.The receiver may comprise means for impedance matching to the load between the receiving coil and the load.
상기 수신기는, 부하에 연결되고 상기 수신 코일과는 직접 연결되지 않고 이격되어 자기장으로 결합되는 부하 코일을 포함하고 상기 수신 코일과 상기 부하 코일 간의 상호 인덕턴스에 의해 임피던스 매칭이 이루어질 수 있다.The receiver may include a load coil connected to a load and coupled to a magnetic field spaced apart from a direct connection with the receiving coil, and impedance matching may be performed by mutual inductance between the receiving coil and the load coil.
상기 부하 코일의 한쪽 끝 단과 상기 부하의 한쪽 끝 단 사이에 커패시터를 포함할 수 있다.A capacitor may be included between one end of the load coil and one end of the load.
상기 수신기는, 상기 수신 코일과 1차측이 연결되고, 부하와 2차측이 연결된, 임피던스 매칭을 위한 트랜스포머를 포함할 수 있다.The receiver may include a transformer for impedance matching, in which the receiving coil and the primary side are connected and the load and the secondary side are connected.
상기 2차측 한쪽 끝 단과 상기 부하의 한쪽 끝 단 사이에 커패시터를 포함할 수 있다.A capacitor may be included between one end of the secondary side and one end of the load.
상기 수신기는, 부하와 상기 수신 코일 사이에 연결된 임피던스 매칭을 위한 인덕터를 포함할 수 있다.The receiver may include an inductor for impedance matching connected between a load and the receiving coil.
상기 수신기는, 부하와 상기 수신 코일 사이에 연결된 임피던스 매칭을 위한 커패시터를 포함할 수 있다.The receiver may include a capacitor for impedance matching connected between a load and the receiving coil.
상기 인덕터의 한쪽 끝단과 상기 부하의 한쪽 끝단 사이에 커패시터를 더 포함할 수 있다.A capacitor may be further included between one end of the inductor and one end of the load.
상기 송신기는, 상기 수신 코일의 수량에 따른 부하량 변동을 센싱하는 센싱 회로를 포함하고, 상기 센싱 회로를 통하여 상기 부하량 변동에 따라 달라진 입력 임피던스가 조절되도록 상기 임피던스 매칭을 위한 수단을 제어하여 임피던스 매칭이 이루어지도록 할 수 있다.The transmitter includes a sensing circuit for sensing a load variation according to the quantity of the receiving coils, and by controlling the means for impedance matching to adjust the input impedance changed according to the load variation through the sensing circuit impedance matching is performed; Can be done.
그리고, 본 발명의 또 다른 일면에 따른, 무선 전력전송 방법은, 송신 코일에서 교류 소스 신호를 이용하여 무선으로 전력을 송신하는 단계; 및 상기 송신 코일과 자기 결합(magnetic coupling)으로 이격된 수신 코일에서 무선으로 상기 전력을 수신하는 단계를 포함하고, 상기 송신 코일 또는 상기 수신 코일은, 한쪽 끝에서 다른 쪽 끝 사이에, 상기 한쪽 끝에서 인가되는 입력 전류의 방향으로 전류가 흐르도록 단일회 또는 복수회 중심 방향으로 동심을 이루도록 감긴 제1코일부; 및 상기 입력 전류의 방향으로 전류가 흐르는 상기 제1코일부에 연결되고 상기 제1코일부와 상기 중심이 일치하며 동심이고, 상기 입력 전류와 반대 방향의 전류가 흐르는 코일부, 또는 상기 중심이 일치하며, 상기 입력 전류의 방향으로 전류가 흐르도록 2가닥 이상이 병렬 연결되어 동심을 이루도록 감긴 코일부를 포함하고, 상기 무선으로 전력을 송신하는 단계에서, 상기 송신 코일에서 상대적인 중심 위치가 수평적으로 다른 하나 이상의 각 수신 코일로 전력을 송신하기 위한 것을 특징으로 하는 한다.In addition, according to another aspect of the present invention, a wireless power transmission method includes transmitting power wirelessly using an AC source signal in a transmission coil; And wirelessly receiving the power in a receiving coil spaced apart from the transmitting coil by magnetic coupling, wherein the transmitting coil or the receiving coil is between one end and the other end. A first coil part wound to be concentric in the center direction of the single or multiple times so that the current flows in the direction of the input current applied from the; And a coil part connected to the first coil part through which current flows in the direction of the input current, the center of the coil being coincident with the center of the first coil part, and having a current flowing in a direction opposite to the input current, or the center of the coil part. And a coil unit wound in parallel so that two or more strands are connected in parallel so that a current flows in the direction of the input current, and in the step of transmitting power wirelessly, a relative center position of the transmitting coil is horizontally It is characterized in that for transmitting power to each other one or more receiving coils.
본 발명에 따른 근거리 무선 전력전송 시스템에 따르면, 송수신기 간의 위치의 변경에 따라 적응형 임피던스 정합 회로를 사용하지 않아도 되기 때문에 시스템의 복잡도가 낮아지며, 가격 또한 저렴하다.According to the short-range wireless power transmission system according to the present invention, since the adaptive impedance matching circuit does not need to be used in accordance with the change of the position between the transceiver, the complexity of the system is low and the price is low.
또한, 단일 코일을 이용하여 별도의 추가적인 회로 없이 20% 이내의 균일 상호 인덕턴스를 갖는 무선 전력 전송 거리 또는 유효 무선 충전 범위 내에서 수신기와 송신기의 배치가 자유로운 Free positioning 이 가능하다. In addition, the use of a single coil allows free positioning of the receiver and transmitter within the wireless power transmission range or effective wireless charging range with uniform mutual inductance within 20% without additional circuitry.
그리고, 균일 상호 인덕턴스를 갖는 무선 전력 전송 거리 내에서 일정한 상호 인덕턴스를 갖기 때문에 복수개의 기기에서 동시에 무선 전력을 수신하여 각 기기의 동작을 위한 전력 제공이나 충전이 가능하다. In addition, since it has a constant mutual inductance within the wireless power transmission distance having a uniform mutual inductance, it is possible to simultaneously receive wireless power from a plurality of devices to provide or charge power for the operation of each device.
도 1은 송수신기의 각각의 공진코일을 사용한 일반적인 전자기 유도 방식 무선 전력전송 시스템의 등가회로이다.1 is an equivalent circuit of a general electromagnetic induction type wireless power transmission system using each resonant coil of a transceiver.
도 2는 본 발명의 일실시예에 따른 무선 전력전송 시스템의 개념을 설명하기 위한 도면이다.2 is a view for explaining the concept of a wireless power transmission system according to an embodiment of the present invention.
도 3은 본 발명의 일실시예에 따른 무선 전력전송 시스템의 성능 지수(FOM)에 따른 송수신 최대 전력전달 효율을 나타내는 그래프이다.3 is a graph showing transmission and reception maximum power transmission efficiency according to a performance index (FOM) of a wireless power transmission system according to an embodiment of the present invention.
도 4는 본 발명의 일실시예에 따른 무선 전력전송 시스템에서 송수신 코일 사이의 상호 인덕턴스(M12)에 대한 계산 결과의 일례이다.4 is an example of a calculation result for the mutual inductance (M 12 ) between the transmission and reception coils in the wireless power transmission system according to an embodiment of the present invention.
도 5는 전기적으로 균일한 상호 인덕턴스를 갖도록 하는 본 발명의 일실시예에 따른 코일 구조의 예이다. 5 is an example of a coil structure in accordance with one embodiment of the present invention to have an electrically uniform mutual inductance.
도 6은 도 5의 구조를 갖도록 실제 제작된 코일의 예시다.6 is an example of a coil actually manufactured to have the structure of FIG. 5.
도 7은 본 발명의 일실시예에 따른 실제 제작된 수신 코일의 예시다.7 is an example of an actual manufactured receiving coil according to an embodiment of the present invention.
도 8은 본 발명의 일실시예에 따른 무선 전력전송 시스템의 송수신 코일 사이의 상호 인덕턴스 측정 결과이다.8 is a result of measuring mutual inductance between transmission and reception coils of a wireless power transmission system according to an embodiment of the present invention.
도 9는 본 발명의 일실시예에 따른 무선 전력전송 시스템의 송신기(Transmitter)에 도 5와 같이 제안된 코일 구조를 적용한 구성을 나타낸다. FIG. 9 illustrates a configuration in which the coil structure proposed in FIG. 5 is applied to a transmitter of a wireless power transmission system according to an embodiment of the present invention.
도 10은 본 발명의 일실시예에 따른 무선 전력전송 시스템의 송신기(Transmitter)에 도 5와 같이 제안된 코일 구조를 적용한 구체적인 구성을 나타낸다. FIG. 10 shows a detailed configuration in which the coil structure proposed in FIG. 5 is applied to a transmitter of a wireless power transmission system according to an embodiment of the present invention.
도 11은 본 발명의 일실시예에 따른 무선 전력전송 시스템의 송신기(Transmitter)에 도 5와 같이 제안된 코일 구조를 적용한 다른 구체적인 구성을 나타낸다. FIG. 11 shows another specific configuration in which the coil structure proposed in FIG. 5 is applied to a transmitter of a wireless power transmission system according to an embodiment of the present invention.
도 12는 본 발명의 일실시예에 따른 무선 전력전송 시스템의 송신기(Transmitter)에 도 5와 같이 제안된 코일 구조를 적용한 또 다른 구체적인 구성을 나타낸다. FIG. 12 shows another specific configuration in which the coil structure proposed in FIG. 5 is applied to a transmitter of the wireless power transmission system according to an embodiment of the present invention.
도 13은 본 발명의 일실시예에 따른 무선 전력전송 시스템의 송신기(Transmitter)에 도 5와 같이 제안된 코일 구조를 적용한 또 다른 구체적인 구성을 나타낸다. FIG. 13 shows another specific configuration in which the coil structure proposed in FIG. 5 is applied to a transmitter of a wireless power transmission system according to an embodiment of the present invention.
도 14는 본 발명의 일실시예에 따른 무선 전력전송 시스템의 수신기(Receiver)의 구성을 나타낸다. 14 illustrates a configuration of a receiver of a wireless power transmission system according to an embodiment of the present invention.
도 15는 본 발명의 일실시예에 따른 무선 전력전송 시스템의 수신기(Receiver)의 구체적인 구성을 나타낸다. 15 shows a detailed configuration of a receiver of a wireless power transmission system according to an embodiment of the present invention.
도 16은 본 발명의 일실시예에 따른 무선 전력전송 시스템의 수신기(Receiver)의 다른 구체적인 구성을 나타낸다. 16 shows another specific configuration of a receiver of a wireless power transmission system according to an embodiment of the present invention.
도 17은 본 발명의 일실시예에 따른 무선 전력전송 시스템의 수신기(Receiver)의 또 다른 구체적인 구성을 나타낸다. 17 shows another specific configuration of a receiver of a wireless power transmission system according to an embodiment of the present invention.
도 18은 본 발명의 일실시예에 따른 무선 전력전송 시스템의 수신기(Receiver)의 또 다른 구체적인 구성을 나타낸다. 18 shows another specific configuration of a receiver of a wireless power transmission system according to an embodiment of the present invention.
도 19는 본 발명의 일실시예에 따른 무선 전력전송 시스템의 수신기(Receiver)의 또 다른 구체적인 구성을 나타낸다. 19 shows another specific configuration of a receiver of a wireless power transmission system according to an embodiment of the present invention.
도 20은 도 11과 도 15의 구조를 결합한 경우의 예시이다.FIG. 20 is an example in which the structures of FIGS. 11 and 15 are combined.
도 21은 도 5의 제안된 코일 구조와 도 5의 구조에서 N3와 N4를 제거하거나 N4만을 제거한 구조의 자기장 변화를 설명하기 위한 도면이다. FIG. 21 is a view for explaining a magnetic field change of the proposed coil structure of FIG. 5 and the structure in which N 3 and N 4 are removed or N 4 is removed from the structure of FIG. 5.
이하 첨부 도면들 및 첨부 도면들에 기재된 내용들을 참조하여 본 발명의 바람직한 실시예를 상세하게 설명하지만, 본 발명이 실시예들에 의해 제한되거나 한정되는 것은 아니다. Hereinafter, exemplary embodiments of the present invention will be described in detail with reference to the accompanying drawings and the contents described in the accompanying drawings, but the present invention is not limited or limited to the embodiments.
도 2는 본 발명의 일실시예에 따른 무선 전력전송 시스템의 개념을 설명하기 위한 도면이다.2 is a view for explaining the concept of a wireless power transmission system according to an embodiment of the present invention.
도 2와 같이, 본 발명의 일실시예에 따른 무선 전력전송 시스템은, 교류 소스 신호(Vs)를 받는 송신기(Transmitter)의 송신 (공진) 코일(Tx coil)(등가회로에서 자기 인덕턴스 L1, 저항은 R1, 공진을 위한 정전용량은 C1)이, 수신기(Receiver)의 수신 (공진) 코일(Rx coil)(등가회로에서 자기 인덕턴스 L2, 저항은 R2, 공진을 위한 정전용량은 C2)로 상호 인덕턴스 M12 따른 전자기 유도 또는 자기장 결합으로 최대의 전력을 전송할 수 있도록, 송수신기에 임피던스 매칭을 위한 매칭 유닛(Tx matching unit, Rx matching unit)을 구비한다. As shown in FIG. 2, a wireless power transmission system according to an embodiment of the present invention includes a transmission (resonance) coil (Tx coil) of a transmitter receiving an AC source signal Vs (magnetic inductance L 1 , in an equivalent circuit). The resistance is R 1 , the capacitance for resonance is C 1 , the receiver (resonance) coil (Rx coil) of the receiver (magnetic inductance L 2 in the equivalent circuit, the resistance R 2 , the capacitance for resonance is C 2 ) is provided with a matching unit (Tx matching unit, Rx matching unit) for impedance matching to the transceiver so that the maximum power can be transmitted by electromagnetic induction or magnetic field coupling according to mutual inductance M 12 .
최대 전력 전달을 위하여, 송신기의 임피던스 매칭 유닛(Tx matching unit)은 송신 코일(Tx coil)로 바라보는 임피던스를 입력 임피던스(Zin)(소스에서 바라보는 임피던스)와 매칭시켜서 송신되는 소스 신호의 반사를 최소화(제거)하여야 하고, 부하(임피던스 ZL)에 대한 임피던스 매칭 효과를 얻기 위한 수신기의 임피던스 매칭 유닛(Rx matching unit)은 수신 코일(Rx coil)에서 부하 쪽으로 바라보는 임피던스의 공액 매칭(conjugate matching) 조건이 성립되어야 한다.For maximum power transfer, the transmitter's Tx matching unit matches the impedance seen by the Tx coil with the input impedance Z in (impedance seen by the source) to reflect the transmitted source signal. The Rx matching unit of the receiver for minimizing (removing) the impedance matching effect on the load (impedance Z L ) is conjugated with the impedance seen from the Rx coil toward the load. matching) condition must be established.
이때 매칭 유닛(Tx matching unit, Rx matching unit)에 의한 전도 저항 손실이 없을 경우, 최대 전력전달 효율 η(전송한 전력에 대한 부하에 전달된 전력의 비율)는 잘 알려져 있는 전자기학적 이론을 근거로 [수학식1]과 같이 유도 될 수 있다.At this time, if there is no conduction resistance loss by the matching unit (Tx matching unit), the maximum power transfer efficiency η (the ratio of the power delivered to the load to the transmitted power) is based on the well-known electromagnetic theory. It can be derived as shown in [Equation 1].
[수학식1][Equation 1]
여기서 FOM은 송수신 시스템의 성능 지수(Figure of merit: FoM)를 말한다. 본 발명에서 제안된 하기하는 바와 같은 코일을 사용할 경우 [수학식1]의 R1을 Rp로 변경하면 FOM과 최대 전력전달 효율 η를 구할 수 있다. 여기서, fr은 송수신 코일(송신코일과 수신코일)의 공진 주파수이며, R1은 송신 코일의 저항, R2는 수신 코일의 저항, M12은 송수신 코일의 상호 인덕턴스이다. [수학식1]에서 송수신 코일의 저항은 송수신 코일의 위치 변경 등에 거의 변동이 없기 때문에 시스템의 효율 η과 성능 지수 FoM는 M12에 따라 달라진다. Here, FOM refers to the figure of merit (FoM) of the transmission and reception system. In the case of using the coil as described below in the present invention, by changing R 1 to R p in
본 발명에서, 송신기(Transmitter)는 스마트폰, 아이패드 등 전력을 사용하는 각종 전자기기에 장착된 위와 같은 수신기(Receiver)로 최대 전력 전달 효율로 무선 전력을 공급할 수 있으며, 무선 전력 송신기(Transmitter)에서 공간상 고정형 또는 이동형 부하(예, 배터리, 기기 동작 회로 등)를 갖는 수신기(Receiver)로의 전력 전송에 있어서, 송신기(Transmitter)의 송신 코일(Tx coil)과 수신기(Receiver)의 수신 코일(Rx coil) 중 어느 하나 이상에 본 발명의 제안된 코일 구조물이 적용될 수 있는, 해당 송수신기 간의 위치의 변경에 따라 적응형 임피던스 정합 회로를 사용하지 않아도, 하기하는 바와 같이 위와 같은 원리에 따라 20% 이내의 성능 지수 FOM또는 균일 상호 인덕턴스 M12를 갖는 무선 전력 전송 거리 내에서 간단하고 저렴하게 자유로운 Free positioning 에 적응하여 최대 전력 전달 효율로 무선 전력을 공급할 수 있다. 이와 같은 균일 상호 인덕턴스를 갖는 무선 전력 전송 거리 내에서 일정한 상호 인덕턴스를 갖기 때문에 복수개의 기기에서 동시에 무선 전력을 수신하여 배터리를 충전하거나 기기를 작동시킬 수 있다. In the present invention, the transmitter (Transmitter) can supply the wireless power with the maximum power transfer efficiency to the receiver (Receiver) as described above mounted on a variety of electronic devices using the power, such as a smart phone, iPad, wireless power transmitter (Transmitter) In a power transmission to a receiver having a fixed or mobile load (eg, battery, device operation circuit, etc.) in space, the transmitter coil (Tx coil) of the transmitter and the receiver coil (Rx) of the receiver (Receiver) The coil structure of the present invention can be applied to any one or more of the coils, and even if the adaptive impedance matching circuit is not used in accordance with the change of the position between the corresponding transceivers, it is within 20% according to the above principle as described below. Simple and inexpensive adaptation to free positioning within wireless power transmission distances with figure of merit FOM or uniform mutual inductance M 12 Wireless power can be supplied with power delivery efficiency. Since there is a constant mutual inductance within the wireless power transmission distance having such a uniform mutual inductance, a plurality of devices can simultaneously receive wireless power to charge the battery or operate the device.
도 3은 본 발명의 일실시예에 따른 무선 전력전송 시스템의 성능 지수(FOM)에 따른 송수신 최대 전력전달 효율(η)을 나타내는 그래프이다. 여기서 최대 전력전달효율(η)은 송수신 매칭 유닛(Tx matching unit, Rx matching unit)에서 위와 같은 최대 전력전달 조건을 만족한 경우로서, 도 3과 같이 성능 지수(FoM)가 증가할수록 효율(η)이 증가하며, 성능지수(FOM)가 낮을수록 성능 지수의 변화에 따라 최대 전력전송 효율(η)의 변화가 더 큼을 알 수 있다.3 is a graph showing the maximum transmission and reception power transmission efficiency η according to the figure of merit (FOM) of the wireless power transmission system according to an embodiment of the present invention. Here, the maximum power transfer efficiency η is a case where the maximum power transfer condition is satisfied in the Tx matching unit and the Rx matching unit. As shown in FIG. 3, the efficiency η increases as the performance index FoM increases. The higher the FOM, the greater the change in maximum power transfer efficiency η according to the change in the figure of merit.
도 4는 본 발명의 일실시예에 따른 무선 전력전송 시스템에서 송수신 코일 사이의 상호 인덕턴스(M12)에 대한 계산 결과의 일례이다.4 is an example of a calculation result for the mutual inductance (M 12 ) between the transmission and reception coils in the wireless power transmission system according to an embodiment of the present invention.
도 4의 (a)와 같이 송신 코일(Tx coil)과 수신 코일(Rx coil)은 중심이 일치되도록 나란하게 배치되어 있고, 반경이 10cm인 각 코일의 두께는 매우 가는 필라멘트리(filamentary) 코일로 가정하며, 단일 턴수로 가정한다. 단위는 모두 cm이다. 도 4의 (b)는 수신 코일(Rx coil)의 중심이 도면에서 y 방향으로 평행하게 이동 거리(rho)에 따라 변화되는 상호인덕턴스 값을 나타낸다. 이러한 송수신 구성은 일반적으로 송신기 위에 수신기를 올려 놓고(예, 도면에서 두 코일의 중심이 일치할 때 5cm 거리) 무선 충전하는 구조의 예가 될 수 있다. 그림에서처럼 두 코일의 중심이 일치할 때(y=0) 가장 큰 상호인덕턴스 값을 나타내며, rho가 증가할수록 점점 줄어들며 중심간 차이가 약 17cm근처에서는 상호인덕턴스 값이 0을 나타낸다. 즉, 두 코일의 상대적인 수평적 위치 변화(한 코일을 코일면에 수평으로 이동)에 따라 두 코일의 중심 간 거리가 달라지고 자기장이 커플링되는 면적이 바뀌어 상호 인덕턴스가 변화된다. 이러한 이유로 수신기가 송신기의 실제 충전 영역에서 움직일 때, 송수신 코일 사이의 상호 인덕턴스가 변화되며 이로 인해 최적 전력 전달 조건이 변경되어, 위치에 따라 최대 전력전달 효율(η)을 얻기 위해서는 송수신 매칭 유닛(Tx matching unit, Rx matching unit)에서 최대 전력전달 조건을 만족하도록 설계하여야 한다.As shown in (a) of FIG. 4, the transmitting coil and the receiving coil are arranged side by side so that their centers coincide with each other, and the thickness of each coil having a radius of 10 cm is a very thin filamentary coil. Assume, assume a single turn. The units are all cm. 4B illustrates a mutual inductance value in which the center of the Rx coil is changed according to the moving distance rho in parallel in the y direction in the drawing. Such a transmission / reception scheme may be an example of a structure in which a receiver is generally placed on a transmitter (eg, 5 cm distance when two coils coincide in the drawing) and wirelessly charges. As shown in the figure, the maximum mutual inductance value is shown when the centers of two coils coincide (y = 0), and the value decreases with increasing rho, and the mutual inductance value is 0 when the difference between centers is about 17cm. That is, the distance between the centers of the two coils is changed according to the change in the relative horizontal position of the two coils (moving one coil horizontally on the coil surface), and the area in which the magnetic field is coupled is changed, thereby changing the mutual inductance. For this reason, when the receiver moves in the actual charging area of the transmitter, the mutual inductance between the transmitting and receiving coils changes, thereby changing the optimum power transfer condition, so that the transmission and reception matching unit (Tx) can be used to obtain the maximum power transfer efficiency (η) according to the position. matching unit, Rx matching unit).
도 5는 전기적으로 균일한 상호 인덕턴스를 갖도록 하는 본 발명의 일실시예에 따른 코일 구조의 예이다. 도 5를 참조하면, 본 발명의 일실시예에 따라 균일한 상호 인덕턴스를 갖도록 하기 위한 코일 구조는 동일 중심으로부터 반경이 서로 다른(r1, r2, r3, r4) 4개의 부분(N1, N2, N3, N4)으로 이루어진다. 5 is an example of a coil structure in accordance with one embodiment of the present invention to have an electrically uniform mutual inductance. Referring to FIG. 5, the coil structure for having a uniform mutual inductance according to an embodiment of the present invention has four portions (N, r 1 , r 2 , r 3 , r 4 ) having different radii from the same center (N). 1 , N 2 , N 3 , N 4 ).
가장 외곽의 코일부 N1은 입력 전류(I0)를 받는 한쪽 끝단에서 시작되어 최외곽 반경 r1(예, 아래 [표1]의 6.5cm 참조)으로부터 1회 이상(예, 3회) 등간격(p1)(예, 아래 [표1]의 1.5mm 참조)으로 감긴 루프 코일(들)로 이루어지는 부분으로서, N1의 각 루프 코일은 입력 전류와 동일한 전류 방향을 갖는다. 여기서 코일부 N1으로 감긴 루프 코일들은 등간격인 것으로 예를 들어 설명하지만 이에 한정되는 것은 아니고 비등간격으로 감길 수도 있다. 이하 다른 코일들 N2, N3, N4 각각도 복수회 감긴 코일로 이루어질 수 있으며 이때 등간격 또는 비등간격으로 감기는 형태일 수 있다.The outermost coil part N 1 starts at one end receiving the input current (I 0 ) and at least one time (eg, three times) from the outermost radius r 1 (eg, 6.5 cm in Table 1 below). As part of loop coil (s) wound at intervals p 1 (eg, 1.5 mm in Table 1 below), each loop coil of N 1 has the same current direction as the input current. Here, the loop coils wound by the coil part N 1 are described as being equally spaced, but the present invention is not limited thereto and may be wound at boiling intervals. Hereinafter, each of the other coils N 2 , N 3 , and N 4 may also be formed of a coil wound multiple times, and in this case, the coils may be wound at equal intervals or boiling intervals.
코일부 N1의 끝에 연결되어 연장되는 코일부 N2은 코일부 N1의 가장 안쪽 코일의 반경보다 작은 반경 r2(예, 아래 [표1]의 6cm 참조)를 갖도록 감긴 단일 루프 코일인 것이 바람직하다(경우에 따라 복수 가능). 코일부 N2의 루프 코일(들)은 코일부 N1의 코일들 중 가장 안쪽 코일로부터 일정 간격을 가지며 이 간격은 코일부 N1의 코일들의 간격(p1)과 다른 것이 바람직하다(경우에 따라 동일 간격 가능).Coil N nose extending connected to one end of the part N 2 is not smaller radius than the radius of the innermost coil of the coil N 1 r 2 single loop coil wound so as to have a (e. G., Under the reference 6cm in Table 1) It is preferable (plurally possible in some cases). The loop coil (s) of the coil portion N 2 has a predetermined distance from the innermost coil of the coils of the coil portion N 1 , and this interval is preferably different from the interval p 1 of the coils of the coil portion N 1 (in the case of Equal intervals available).
코일부 N2의 끝에 연결되는 코일부 N3은 반경 r2 안쪽에 그 보다 작은 최외곽 반경 r3(예, 아래 [표1]의 5.5cm 참조)를 갖도록 감긴 코일로서, 두 개의 코일이 일정 간격(예, 아래 [표1]의 5mm 참조)으로 병렬 연결된 코일(경우에 따라 3가닥 이상의 병렬 연결 형태 가능하며 그 코일들 사이의 간격은 비균등)이며, 코일부 N1, N2의 코일들과는 전류 방향이 반대가 되도록 단일회 또는 복수회 형성된다. Coco connected to some N 2 at the end N 3 is part of a coil wound so as to have a (see 5.5cm in Table 1, e.g., below) the outermost small radius r 3 than the inside radius r 2, the two coils constant Coils connected in parallel (eg 5mm in Table 1 below) in parallel (3 or more strands can be connected in some cases and the spacing between them is uneven), and coils of coil parts N 1 and N 2 They are formed once or multiple times so that the direction of current is reversed.
다시 코일부 N3의 끝(두 개의 연결된 코일의 끝)에 연결되는 코일부 N4은 코일부 N3의 안쪽 코일의 반경보다 작은 반경 r4(예, 아래 [표1]의 4.5cm 참조)를 갖도록 감긴 코일로서, 두 개의 코일이 일정 간격(예, 아래 [표1]의 15mm 참조)으로 병렬 연결된 코일(경우에 따라 3가닥 이상의 병렬 연결 형태 가능하며 그 코일들 사이의 간격은 비균등)이며, 코일부 N1, N2의 코일들과 전류 방향이 동일하도록 단일회 또는 복수회 형성된다. 코일부 N4의 끝단(두 개의 연결된 코일의 끝)과 코일부 N1이 시작되는 부분 사이, 또는 코일부 N4의 끝단이나 코일부 N1이 시작되는 부분 중 어느 한쪽 등 적절한 위치에 도 6과 같이 공진 주파수 및 임피던스 정합을 위해 커패시터(Cp)가 연결될 수 있다. The coil part N 4, which is connected to the end of the coil part N 3 again (the end of two connected coils), has a radius r 4 smaller than the radius of the inner coil of the coil part N 3 (eg, see 4.5 cm in Table 1 below). Coil wound to have two coils connected in parallel at regular intervals (e.g., see 15mm in Table 1 below). In some cases, more than three strands can be connected in parallel, and the spacing between them is uneven. It is formed in single or multiple times so that the current direction is the same as the coils of the coil parts N 1 , N 2 . FIG. 6 at an appropriate position, such as between the end of the coil portion N 4 (the ends of two connected coils) and the portion where the coil portion N 1 starts, or the end of the coil portion N 4 or the portion where the coil portion N 1 starts. As described above, the capacitor Cp may be connected for resonant frequency and impedance matching.
도 5에서 코일부 N1에 인가되는 입력 전류(I0)는 코일부 N3 의 병렬 코일에서 aI0와 (1-a)I0 분배되어 흐르며, 마찬가지로 코일부 N4 의 병렬 코일에서 βI0와 (1-β)I0 분배되어 흐르게 된다. a와 β는 양수 또는 음수도 가능하며, 절대값의 크기는 2보다 작다. Input current (I 0) it is applied to the coil N 1 in Figure 5 the coil N aI 0 and (1-a) in parallel to the coil of 3 I 0 flows is distributed, as in the nose βI 0 in the parallel coil of some N 4 And (1-β) I 0 are distributed and flowed. a and β can be positive or negative, and the magnitude of the absolute value is less than 2.
이와 같이 제안된 본 발명의 코일 구조에서 동심 원형 형태의 각 코일부를 구성한 예를 설명하였으나, 이에 한정되는 것은 아니며 사각형, 육각형 등 필요에 따라 다양한 동심 다각형 형태로 각 코일부를 구성할 수도 있다. 또한, 각 코일부를 도 6과 같이 구리선 등 금속 도체 와이어로 구성한 예를 설명하였으나, 이에 한정되는 것은 아니며 인쇄회로기판 공정이나 반도체 공정 등 필요에 따라 다양한 공정 기술로 각 코일부의 패턴을 형성하는 것도 가능하다. 이와 같은 인쇄회로기판 공정이나 반도체 공정 등을 이용하는 경우에 해당 인쇄회로기판 또는 반도체 기판 등 해당 기판의 양면 등 다층에 4개의 코일부(N1, N2, N3, N4)를 적절히 분산 배치되도록 형성할 수 있으며, 이때 각 층에 형성된 코일부 간의 연결은 비아(via) 홀 등을 통하여 연결되도록 할 수 있다.As described above, an example in which each coil part of a concentric circular shape is configured in the proposed coil structure of the present invention is not limited thereto, and each coil part may be configured in various concentric polygonal shapes, such as a rectangle and a hexagon. In addition, an example in which each coil part is made of a metal conductor wire such as a copper wire has been described as shown in FIG. 6. However, the present invention is not limited thereto. It is also possible. When using such a printed circuit board process or a semiconductor process, four coil parts (N 1 , N 2 , N 3 , N 4 ) are appropriately distributed and arranged on both sides of the substrate such as the printed circuit board or the semiconductor substrate. In this case, the connection between the coil parts formed in each layer may be connected through a via hole or the like.
또한, 이와 같은 각 코일(N1, N2, N3, N4)의 배치에 있어서 도 5, 도 6과 같이 예시적으로 도시하였지만, 이에 한정되지 않으며, 각 코일(N1, N2, N3, N4)의 배치는 어느 위치 이든 상관이 없다. 또한, 각 코일(N1, N2, N3, N4) 중 생략되는 부분이 있을 수 있으며, 이때 한쪽 끝에서 다른 쪽 끝 사이에 각 코일 부분이 적절히 연결될 수 있고, 코일(N4)은 도 5, 도 6과 같이 중심부(가장 안쪽 영역)가 아니라 최외곽부에 배치하는 것도 가능하다.In addition, in the arrangement of the respective coils (N 1 , N 2 , N 3 , N 4 ) as exemplarily illustrated in FIGS. 5 and 6, the present invention is not limited thereto, and the respective coils N 1 , N 2 , N 3 , N 4 ) does not matter in any position. In addition, there may be a part omitted from each of the coils (N 1 , N 2 , N 3 , N 4 ), where each coil portion may be properly connected between one end to the other end, the coil (N 4 ) is It is also possible to arrange | position to outermost part rather than a center part (innermost area) like FIG. 5, FIG.
표 1
도 7은 본 발명의 일실시예에 따른 실제 제작된 수신 코일(Rx coil)의 예시다. 수신 코일(Rx coil)은 인쇄회로기판 공정을 통하여 제작될 수 있으며, 공진 주파수(fr)는 6.78 MHz가 되도록 하였다. 이외에도 수신 코일(Rx coil) 역시 가는 구리선이나, 반도체 공정 등 위와 같은 다양한 방법으로 제작될 수 있다. 이와 같은 수신 코일(Rx coil)은 하나의 예시적인 것이며, 도 5, 도 6과 같은 본 발명의 코일 구조물 형태를 수신 코일(Rx coil)에 적용할 수도 있다. 즉, 송신 코일(Tx coil)과 수신 코일(Rx coil)을 모두 도 5, 도 6과 같은 본 발명의 코일 구조물 형태로 할 수도 있고, 송신 코일(Tx coil)만 도 5, 도 6과 같은 본 발명의 코일 구조물 형태로 할 수도 있으며, 수신 코일(Rx coil)만을 도 5, 도 6과 같은 본 발명의 코일 구조물 형태로 할 수도 있다.7 is an example of an actual manufactured Rx coil according to an embodiment of the present invention. The Rx coil may be manufactured through a printed circuit board process, and the resonant frequency f r is set to 6.78 MHz. In addition, the Rx coil may also be manufactured by various methods such as a thin copper wire or a semiconductor process. The Rx coil as described above is one example, and the coil structure of the present invention as shown in FIGS. 5 and 6 may be applied to the Rx coil. That is, both the transmission coil (Tx coil) and the reception coil (Rx coil) may be in the form of the coil structure of the present invention as shown in FIGS. 5 and 6, and only the transmission coil (Tx coil) as shown in FIGS. 5 and 6. It may be in the form of the coil structure of the present invention, and only the receiving coil may be in the form of the coil structure of the present invention as shown in FIGS. 5 and 6.
도 8은 본 발명의 일실시예에 따른 무선 전력전송 시스템의 송수신 코일 사이의 상호 인덕턴스(M12) 측정 결과이다.8 is a result of measuring mutual inductance (M 12 ) between the transmission and reception coils of the wireless power transmission system according to an embodiment of the present invention.
송신 코일(Tx coil)과 수신 코일(Rx coil)은 모두 6.78MHz의 공진 주파수를 갖도록 도 6과 같이, 코일부 N4의 끝단(두 개의 연결된 코일의 끝)과 코일부 N1이 시작되는 부분 사이, 또는 코일부 N4의 끝단이나 코일부 N1이 시작되는 부분 중 어느 한쪽 등 적절한 위치에 도 6과 같이 추가적으로 6.78 MHz공진 주파수를 위해 커패시터(Cp)가 연결될 수 있다. As shown in FIG. 6, the transmitting coil (Tx coil) and the receiving coil (Rx coil) have a resonance frequency of 6.78 MHz, the end of the coil part N 4 (the ends of two connected coils) and the coil part N 1 start. Capacitor Cp may be connected to an additional 6.78 MHz resonant frequency as shown in FIG. 6 at an appropriate position, such as between the end of coil portion N 4 or the portion where coil portion N 1 starts.
도 8에서 그래프 a와 b는 도 6의 구조에서 N3과 N4 코일부를 제외한 N1과 N2 코일부만을 사용한 기존 형태의 코일 구조를 갖는 송신 코일과 도 7과 같은 구조의 수신 코일 사이의 상호 인덕턴스로서 case 1(도 4와 같은 좌표에서 수신 코일의 중심을 y 방향으로 이동시킴)과 case 2(도 4와 같은 좌표에서 수신 코일의 중심을 x 방향으로 이동시킴) 경우에 대한 것이다. 도 8에서 그래프 c와 d 는 도 6과 같은 구조의 송신 코일과 도 7과 같은 구조의 수신 코일 사이의 상호 인덕턴스로서 case 1(도 4와 같은 좌표에서 수신 코일의 중심을 코일면에 수평인 y 방향으로 이동시킴)과 case 2(도 4와 같은 좌표에서 수신 코일의 중심을 코일면에 수평인 x 방향으로 이동시킴) 경우에 대한 것이다. In FIG. 8, graphs a and b show a transmission coil having a conventional coil structure using only N 1 and N 2 coil parts except N 3 and N 4 coil parts in the structure of FIG. 6 and a receiving coil having a structure as shown in FIG. 7. As the mutual inductance of, the case 1 (moves the center of the receiving coil in the y direction at the coordinates as shown in Figure 4) and case 2 (moves the center of the receiving coil in the x direction at the coordinates as shown in Figure 4). In FIG. 8, graphs c and d are mutual inductances between a transmitting coil having a structure as shown in FIG. 6 and a receiving coil having a structure as shown in FIG. 7. Direction) and case 2 (move the center of the receiving coil in the x direction horizontal to the coil plane at the coordinates as shown in FIG. 4).
도 8과 같이 그래프a 의 유색으로 처리된 부분인 충전 영역(charging zone)에서 두 코일 사이의 중심과 중심 사이의 거리 ρ(rho)가 변화되면 상호 인덕턴스 변화는 매우 크지만(예를 들어, (최대 상호인덕턴스-최소 상호인덕턴스)/최대상호인덕턴스>0.2), 두 코일 사이의 중심과 중심 간의 차이가 4cm 이내의 충전 영역(charging zone)에서 그래프c에서는 상호 인덕턴스의 변화가 매우 작다(예를 들어, (최대 상호인덕턴스-최소 상호인덕턴스)/최대상호인덕턴스<0.2). 모든 경우에 대해서 충전 영역(charging zone)을 벗어나면 상호 인덕턴스 값이 급격히 떨어지는 것을 알 수 있다.As shown in FIG. 8, when the distance ρ (rho) between the centers and the centers of the two coils is changed in the charging zone, which is the colored portion of the graph a, the mutual inductance change is very large (for example, ( The maximum mutual inductance-minimum mutual inductance) / maximum mutual inductance> 0.2), and in the charging zone where the difference between the center and the center between the two coils is within 4 cm, the change in the mutual inductance is very small in graph c (e.g. , (Maximum mutual inductance min minimum mutual inductance) / maximum mutual inductance <0.2). In all cases, it can be seen that the mutual inductance value drops sharply out of the charging zone.
도 9는 본 발명의 일실시예에 따른 무선 전력전송 시스템의 송신기(Transmitter)에 도 5와 같이 제안된 코일 구조를 적용한 구성을 나타낸다. FIG. 9 illustrates a configuration in which the coil structure proposed in FIG. 5 is applied to a transmitter of a wireless power transmission system according to an embodiment of the present invention.
도 5와 같이 본 발명의 일실시예에 따라 균일한 상호 인덕턴스를 갖도록 하기 위한, 반경이 서로 다른(r1, r2, r3, r4) 4개의 부분(N1, N2, N3, N4)으로 이루어진 본 발명에서 제안된 코일의 양끝단은, 송신기의 임피던스 매칭 유닛(Tx matching unit)의 양끝단에 연결되어 송신 코일(Tx coil)로 사용될 수 있으며, 이때 송신 코일(Tx coil)인 제안된 코일은 전체적으로 저항 Rp 와 인덕턴스 Lp 로 등가화될 수 있으며, 송신 코일(Tx coil)인 제안된 코일의 한쪽 끝단과 송신기의 임피던스 매칭 유닛(Tx matching unit)의 한쪽 끝단 사이에 커패시터 Cp가 연결될 수 있다. Cp는 공진 주파수 및 임피던스 정합을 위해 사용되며, 이외에도 코일부 N4의 끝단과 코일부 N1이 시작되는 부분 사이 등 다양한 형태로 커패시터 Cp가 연결될 수 있다. As shown in FIG. 5, four parts having different radii (r 1 , r 2 , r 3 , r 4 ) to have a uniform mutual inductance according to an embodiment of the present invention (N 1 , N 2 , N 3) , N 4 ), both ends of the coil proposed in the present invention may be connected to both ends of an impedance matching unit (Tx matching unit) of the transmitter to be used as a transmission coil (Tx coil), in which case the transmission coil (Tx coil) The proposed coil can be equivalent to the resistance R p and the inductance L p as a whole, and between one end of the proposed coil, which is a Tx coil, and one end of the transmitter's Tx matching unit, Capacitor C p may be connected. The C p is used for matching the resonant frequency and impedance, and in addition, the capacitor C p may be connected in various forms such as between the end of the coil portion N 4 and the portion where the coil portion N 1 starts.
도 10은 본 발명의 일실시예에 따른 무선 전력전송 시스템의 송신기(Transmitter)에 도 5와 같이 제안된 코일 구조를 적용한 구체적인 구성을 나타낸다. FIG. 10 shows a detailed configuration in which the coil structure proposed in FIG. 5 is applied to a transmitter of a wireless power transmission system according to an embodiment of the present invention.
도 10과 같이, 송신기(Transmitter)에서는 교류 소스 신호(Vs)(전압원, 전류원, 또는 전력소스) 양단에 소스 코일(source coil)(등가회로에서 자기 인덕턴스 Ls, 저항은 Rs)이 연결되고 소스 코일(source coil)의 어느 한쪽 끝에 커패시터 Cs이 연결될 수 있으며, 소스 코일(source coil)과 자기 결합(magnetic coupling)으로 이격된 송신 (공진) 코일(Tx coil)인, 커패시터 Cp 를 구비한 제안된 코일(등가회로에서 자기 인덕턴스 Lp, 저항은 Rp)를 구비한다. As shown in FIG. 10, in a transmitter, a source coil (a magnetic inductance L s in an equivalent circuit and a resistor R s ) is connected across an AC source signal Vs (voltage source, current source, or power source). Capacitor C s can be connected to either end of the source coil and has a capacitor C p , which is a transmit (resonant) coil spaced apart from the source coil by magnetic coupling. One proposed coil (magnetic equivalent inductance L p , equivalent resistance R p ) is provided.
소스 코일(source coil)과 송신 (공진) 코일(Tx coil)은 직접 연결되지 않고 이격되어 자기장으로 결합되며, 소스 코일(source coil)과 송신 (공진) 코일(Tx coil) 사이의 상호 인덕턴스 M1을 조절하여 임피던스 정합을 시킴으로써 임피던스 매칭 유닛(Tx matching unit)으로 기능하도록 한다. 또한, 교류 소스 신호(Vs) 한쪽 끝 단과 소스 코일(source coil) 한쪽 끝 단 사이의 커패시터 CS는 소스 코일(source coil)의 송신 (공진) 코일(Tx coil)과의 공진을 위해 사용될 수 있으며, 이는 반드시 필요한 것은 아니다. The source coil and the transmit (resonant) coil (Tx coil) are not directly connected, but are separated by a magnetic field, and mutual inductance M 1 between the source coil and the transmit (resonant) coil (Tx coil) By controlling the impedance matching to function as an impedance matching unit (Tx matching unit). In addition, the capacitor C S between one end of the AC source signal Vs and one end of the source coil may be used for resonance with the transmission (resonance) coil of the source coil. This is not necessary.
도 11은 본 발명의 일실시예에 따른 무선 전력전송 시스템의 송신기(Transmitter)에 도 5와 같이 제안된 코일 구조를 적용한 다른 구체적인 구성을 나타낸다. FIG. 11 shows another specific configuration in which the coil structure proposed in FIG. 5 is applied to a transmitter of a wireless power transmission system according to an embodiment of the present invention.
도 11과 같이, 송신기(Transmitter)에서는 교류 소스 신호(Vs)(전압원, 전류원, 또는 전력소스) 양단에 트랜스포머 1차측(등가회로에서 자기 인덕턴스 Ls1, 저항은 Rs1)을 연결하고 트랜스포머 2차측(등가회로에서 자기 인덕턴스 LT1, 저항은 RT1) 양단에 송신 (공진) 코일(Tx coil)인, 커패시터 Cp 가 양단에 구비된 제안된 코일(등가회로에서 자기 인덕턴스 Lp, 저항은 Rp)를 구비한다. 여기서 임피던스 매칭 유닛(Tx matching unit)으로 기능하는 트랜스포머는 공심(air core) 구조에 1차측 및 2차측 코일이 감긴 구조일 수도 있고, 페라이트 코어와 같이 자성 재질을 포함한 재료에 1차측 및 2차측 코일이 감긴 구조일 수도 있다.As shown in FIG. 11, in the transmitter, the transformer primary side (magnetic inductance L s1 in the equivalent circuit, R s1 in the equivalent circuit) is connected across the AC source signal Vs (voltage source, current source, or power source), and the transformer secondary side is connected. (in the equivalent circuit the magnetic inductance L T1, resistors R T1) of transmission (resonance) coil (Tx coil) across the capacitor C p is in the proposed coil (equivalent circuit having both ends self-inductance L p, the resistance R p ). Here, the transformer functioning as an impedance matching unit may be a structure in which primary and secondary coils are wound around an air core structure, or primary and secondary coils in a material containing a magnetic material, such as a ferrite core. This may be a wound structure.
도 12는 본 발명의 일실시예에 따른 무선 전력전송 시스템의 송신기(Transmitter)에 도 5와 같이 제안된 코일 구조를 적용한 또 다른 구체적인 구성을 나타낸다. FIG. 12 shows another specific configuration in which the coil structure proposed in FIG. 5 is applied to a transmitter of the wireless power transmission system according to an embodiment of the present invention.
도 12와 같이, 송신기(Transmitter)에서는 교류 소스 신호(Vs)(전압원, 전류원, 또는 전력소스) 양단에, 임피던스 매칭 유닛(Tx matching unit)으로 기능하는 커패시터 Cm1가 연결되고, 이와 병렬로 커패시터 Cp 를 갖는 제안된 코일(등가회로에서 자기 인덕턴스 Lp, 저항은 Rp)을 송신 (공진) 코일(Tx coil)로 구비할 수도 있다.As shown in FIG. 12, in the transmitter, a capacitor C m1 functioning as an impedance matching unit is connected across the AC source signal Vs (voltage source, current source, or power source), and the capacitor is connected in parallel. It is also possible to equip the proposed coil with magnetic current (magnetic inductance L p , equivalent resistance R p ) with C p as a transmitting (resonant) coil (Tx coil).
도 13은 본 발명의 일실시예에 따른 무선 전력전송 시스템의 송신기(Transmitter)에 도 5와 같이 제안된 코일 구조를 적용한 또 다른 구체적인 구성을 나타낸다. FIG. 13 shows another specific configuration in which the coil structure proposed in FIG. 5 is applied to a transmitter of a wireless power transmission system according to an embodiment of the present invention.
도 13과 같이, 송신기(Transmitter)에서는 교류 소스 신호(Vs)(전압원, 전류원, 또는 전력소스) 양단에, 임피던스 매칭 유닛(Tx matching unit)으로 기능하는 인덕터 Lm1가 연결되고, 이와 병렬로 커패시터 Cp 를 갖는 제안된 코일(등가회로에서 자기 인덕턴스 Lp, 저항은 Rp)을 송신 (공진) 코일(Tx coil)로 구비할 수도 있다.As shown in FIG. 13, in the transmitter, an inductor L m1 functioning as an impedance matching unit is connected across an AC source signal Vs (voltage source, current source, or power source), and a capacitor is connected in parallel. It is also possible to equip the proposed coil with magnetic current (magnetic inductance L p , equivalent resistance R p ) with C p as a transmitting (resonant) coil (Tx coil).
이와 같은 임피던스 매칭을 위한 도 10 내지 도 13의 방법 이외에도 코일, 트랜스포머, 커패시터, 인덕터 등의 다양한 결합을 이용하는 정합 회로가 사용될 수 있다. In addition to the method of FIGS. 10 to 13 for such impedance matching, a matching circuit using various combinations of coils, transformers, capacitors, and inductors may be used.
도 14는 본 발명의 일실시예에 따른 무선 전력전송 시스템의 수신기(Receiver)의 구성을 나타낸다. 위에서도 기술한 바와 같이 이하에서 언급하는 수신 (공진) 코일(Rx coil)에 대하여, 도 7과 같은 코일 구조 또는 도 5와 같이 제안된 코일 구조를 적용할 수 있다. 14 illustrates a configuration of a receiver of a wireless power transmission system according to an embodiment of the present invention. As described above, the coil structure shown in FIG. 7 or the proposed coil structure shown in FIG. 5 may be applied to the Rx coil described below.
도 14와 같이, 수신기(Receiver)에서는 송신 (공진) 코일(Tx coil)과 상호 인덕턴스 M12 로 커플링되는 수신기(Receiver)의 수신 (공진) 코일(Rx coil)(등가회로에서 자기 인덕턴스 L2, 저항은 R2, 정전용량은 C2)과 이의 양끝단에 연결되는 임피던스 매칭을 위한 매칭 유닛(Rx matching unit)을 구비하며, 매칭 유닛(Rx matching unit) 양단에 부하(임피던스 ZL)가 연결되어 전력을 소모하는 구조를 이룬다. 부하(임피던스 ZL)는 배터리 충전이나 기기의 동작을 위한 회로일 수 있다. C2는 수신 코일(Rx coil)의 공진 주파수 조절과 임피던스 정합을 위해 사용된다. As shown in Fig. 14, in a receiver, a receiver (resonance) coil (Rx coil) of a receiver coupled to a transmit (resonant) coil (Tx coil) and mutual inductance M 12 (magnetic inductance L 2 in an equivalent circuit). , Resistance R 2 , capacitance C 2 ) and an Rx matching unit for impedance matching connected at both ends thereof, and a load (impedance Z L ) is provided at both ends of the Rx matching unit. Connected to form a structure that consumes power. The load (impedance Z L ) may be a circuit for charging the battery or operating the device. C 2 is used to adjust the resonant frequency and impedance matching of the Rx coil.
도 15는 본 발명의 일실시예에 따른 무선 전력전송 시스템의 수신기(Receiver)의 구체적인 구성을 나타낸다. 15 shows a detailed configuration of a receiver of a wireless power transmission system according to an embodiment of the present invention.
도 15와 같이, 수신기(Receiver)에서는 수신 자기 공진 코일(self resonant coil)인 수신 (공진) 코일(Rx coil)(등가회로에서 자기 인덕턴스 L2, 저항은 R2, 정전용량은 C2), 이와 자기 커플링으로 결합된 부하 코일(Load coil)(등가회로에서 자기 인덕턴스 LL, 저항은 RL)을 구비하며, 부하 코일(Load coil)의 어느 한쪽 끝에 커패시터 CL이 연결될 수 있으며, 부하 코일(Load coil) 양단(또는 커패시터 CL을 거친 양단)에 부하(임피던스 ZL)가 연결되어 전력을 소모하는 구조를 이룬다. 부하 코일(Load coil)의 한쪽 끝 단과 부하(임피던스 ZL)의 한쪽 끝 단 사이의 커패시터 CL는 소스 코일(source coil)의 부하 코일(Load coil)의 공진 주파수 또는 임피던스 정합을 위해 사용될 수 있으며, 이는 반드시 필요한 것은 아니고 경우에 따라 제거될 수 있다. 여기서, 수신 (공진) 코일(Rx coil)과 부하 코일(Load coil) 사이의 상호 인덕턴스 ML을 조절하여 임피던스 정합을 시킴으로써 임피던스 매칭 유닛(Rx matching unit)으로 기능하도록 할 수 있다. As shown in Fig. 15, in a receiver, a receiving (resonant) coil Rx coil (self-inductance L 2 , resistance R 2 , capacitance C 2 ), which is a receiving self resonant coil, A load coil (magnetic inductance L L in the equivalent circuit, R L in the equivalent circuit) coupled with the magnetic coupling thereof, and a capacitor C L may be connected to either end of the load coil. A load (impedance Z L ) is connected to both ends of the coil (or both ends via the capacitor C L ) to form a structure that consumes power. The capacitor C L between one end of the load coil and one end of the load (impedance Z L ) can be used for matching the resonant frequency or impedance of the load coil of the source coil. This is not necessary and may be removed in some cases. In this case, the impedance matching may be performed by adjusting the mutual inductance M L between the Rx coil and the load coil to function as an Rx matching unit.
도 16은 본 발명의 일실시예에 따른 무선 전력전송 시스템의 수신기(Receiver)의 다른 구체적인 구성을 나타낸다. 16 shows another specific configuration of a receiver of a wireless power transmission system according to an embodiment of the present invention.
도 16과 같이, 수신기(Receiver)에서는 수신 자기 공진 코일(self resonant coil)인 수신 (공진) 코일(Rx coil)(등가회로에서 자기 인덕턴스 L2, 저항은 R2, 정전용량은 C2) 양단에 트랜스포머 1차측(등가회로에서 자기 인덕턴스 LT2, 저항은 RT2)을 연결하고 트랜스포머 2차측(등가회로에서 자기 인덕턴스 LL2, 저항은 RL2) 양단(또는 커패시터 CL2을 거친 양단)에 부하(임피던스 ZL)가 연결되어 전력을 소모하는 구조를 이룬다. 트랜스포머 2차측 한쪽 끝단과 부하(임피던스 ZL)의 한쪽 끝단 사이의 커패시터 CL2는 임피던스 정합을 위해 사용될 수 있으며, 이는 반드시 필요한 것은 아니고 경우에 따라 제거될 수 있다. 여기서, 여기서 임피던스 매칭 유닛(Rx matching unit)으로 기능하는 트랜스포머는 공심(air core) 구조에 1차측 및 2차측 코일이 감긴 구조일 수도 있고, 페라이트 코어와 같이 자성 재질을 포함한 재료에 1차측 및 2차측 코일이 감긴 구조일 수도 있다.As shown in Fig. 16, in a receiver, both ends of a receiving (resonant) coil (Rx coil) (self-inductance L 2 , resistance R 2 , capacitance C 2 ) in a receiving self resonant coil To the transformer primary side (magnetic inductance L T2 in the equivalent circuit, R T2 in resistance) and the load across the transformer secondary side (magnetic inductance L L2 in the equivalent circuit, R L2 in resistance) (or both ends via capacitor C L2 ) (Impedance Z L ) is connected to form a structure that consumes power. Capacitor C L2 between one end of the transformer secondary and one end of the load (impedance Z L ) can be used for impedance matching, which is not necessary and can be removed in some cases. Here, the transformer functioning as an impedance matching unit may be a structure in which primary and secondary coils are wound around an air core structure, or primary and secondary materials in a material including a magnetic material, such as a ferrite core. It may be a structure in which the side coil is wound.
도 17은 본 발명의 일실시예에 따른 무선 전력전송 시스템의 수신기(Receiver)의 또 다른 구체적인 구성을 나타낸다. 17 shows another specific configuration of a receiver of a wireless power transmission system according to an embodiment of the present invention.
도 17과 같이, 수신기(Receiver)에서는 수신 자기 공진 코일(self resonant coil)인 수신 (공진) 코일(Rx coil)(등가회로에서 자기 인덕턴스 L2, 저항은 R2, 정전용량은 C2) 양단에, 임피던스 매칭 유닛(Rx matching unit)으로 기능하는 인덕터 Lm2가 연결되고, 인덕터 Lm2의 양단(또는 커패시터 Cm을 거친 양단)에 부하(임피던스 ZL)가 연결되어 전력을 소모하는 구조를 이룬다. 인덕터 Lm2의 한쪽 끝단과 부하(임피던스 ZL) 의 한쪽 끝단 사이의 커패시터 Cm는 임피던스 정합을 위해 사용될 수 있으며, 이는 반드시 필요한 것은 아니고 경우에 따라 제거될 수 있다.As shown in Fig. 17, in a receiver, both ends of a receiving (resonant) coil (Rx coil) (self-inductance L 2 , resistance R 2 , and capacitance C 2 ) are self-resonant coils. An inductor L m2 which functions as an impedance matching unit is connected, and a load (impedance Z L ) is connected to both ends of the inductor L m2 (or both ends via the capacitor C m ) to consume power. Achieve. Capacitor C m between one end of inductor L m2 and one end of load (impedance Z L ) can be used for impedance matching, which is not necessary and can be eliminated in some cases.
도 18은 본 발명의 일실시예에 따른 무선 전력전송 시스템의 수신기(Receiver)의 또 다른 구체적인 구성을 나타낸다. 18 shows another specific configuration of a receiver of a wireless power transmission system according to an embodiment of the present invention.
도 18과 같이, 수신기(Receiver)에서는 수신 자기 공진 코일(self resonant coil)인 수신 (공진) 코일(Rx coil)(등가회로에서 자기 인덕턴스 L2, 저항은 R2, 정전용량은 C2) 양단에, 임피던스 매칭 유닛(Rx matching unit)으로 기능하는 커패시터 Cm가 연결되고, 커패시터 Cm의 양단에 부하(임피던스 ZL)가 연결되어 전력을 소모하는 구조를 이룬다. As shown in Fig. 18, in a receiver, both ends of a receiving (resonant) coil (Rx coil) (self-inductance L 2 , resistance R 2 , and capacitance C 2 ) in a self-resonant coil are received. The capacitor C m , which functions as an impedance matching unit, is connected, and a load (impedance Z L ) is connected to both ends of the capacitor C m to form a structure that consumes power.
도 19는 본 발명의 일실시예에 따른 무선 전력전송 시스템의 수신기(Receiver)의 또 다른 구체적인 구성을 나타낸다. 19 shows another specific configuration of a receiver of a wireless power transmission system according to an embodiment of the present invention.
도 19와 같이, 수신기(Receiver)에서는 수신 자기 공진 코일(self resonant coil)인 수신 (공진) 코일(Rx coil)(등가회로에서 자기 인덕턴스 L2, 저항은 R2, 정전용량은 C2) 양단에, 임피던스 매칭 유닛(Rx matching unit)으로 기능하는 인덕터 Lm2가 연결되고, 인덕터 Lm2의 양단에 부하(임피던스 ZL)가 연결되어 전력을 소모하는 구조를 이룬다. 이는 도 17에서 커패시터 Cm을 제거한 경우이다. 19, the receiver (Receiver) is a receiving (resonant) coil (Rx coil) which is a self-resonant coil (self-inductance L 2 in the equivalent circuit, the resistance R 2 , the capacitance C 2 ) both ends The inductor L m2 , which functions as an impedance matching unit, is connected, and a load (impedance Z L ) is connected to both ends of the inductor L m2 to form a structure that consumes power. This is a case where the capacitor C m is removed from FIG. 17.
도 20은 도 11과 도 15의 구조를 결합한 경우의 예시이다.FIG. 20 is an example in which the structures of FIGS. 11 and 15 are combined.
도 20과 같이, 송신기(Transmitter)에서는 교류 소스 신호(Vs)(전압원, 전류원, 또는 전력소스) 양단에 트랜스포머 1차측(등가회로에서 자기 인덕턴스 Ls1, 저항은 Rs1)을 연결하고 트랜스포머 2차측(등가회로에서 자기 인덕턴스 LT1, 저항은 RT1) 양단에 송신 (공진) 코일(Tx coil)인, 커패시터 Cp 가 양단에 구비된 제안된 코일(등가회로에서 자기 인덕턴스 Lp, 저항은 Rp)를 구비한다. 여기서 임피던스 매칭 유닛(Tx matching unit)으로 기능하는 트랜스포머는 공심(air core) 구조에 1차측 및 2차측 코일이 감긴 구조일 수도 있고, 페라이트 코어와 같이 자성 재질을 포함한 재료에 1차측 및 2차측 코일이 감긴 구조일 수도 있다.As shown in FIG. 20, in the transmitter, the transformer primary side (magnetic inductance L s1 in the equivalent circuit and the resistance R s1 ) is connected across the AC source signal Vs (voltage source, current source, or power source), and the transformer secondary side is connected. (in the equivalent circuit the magnetic inductance L T1, resistors R T1) of transmission (resonance) coil (Tx coil) across the capacitor C p is in the proposed coil (equivalent circuit having both ends self-inductance L p, the resistance R p ). Here, the transformer functioning as an impedance matching unit may be a structure in which primary and secondary coils are wound around an air core structure, or primary and secondary coils in a material containing a magnetic material, such as a ferrite core. This may be a wound structure.
또한, 수신기(Receiver)에서는 송신 (공진) 코일(Tx coil)과 상호 인덕턴스 M12 로 커플링되는 수신기(Receiver)의 수신 (공진) 코일(Rx coil)(등가회로에서 자기 인덕턴스 L2, 저항은 R2, 정전용량은 C2)과, 이와 자기 커플링으로 결합된 부하 코일(Load coil)(등가회로에서 자기 인덕턴스 LL, 저항은 RL)을 구비하며, 부하 코일(Load coil)의 어느 한쪽 끝에 커패시터 CL이 연결될 수 있으며, 부하 코일(Load coil) 양단(또는 커패시터 CL을 거친 양단)에 부하(임피던스 ZL)가 연결되어 전력을 소모하는 구조를 이룬다. 부하 코일(Load coil)과 부하(임피던스 ZL) 사이의 커패시터 CL는 소스 코일(source coil)의 부하 코일(Load coil)의 공진 주파수 또는 임피던스 정합을 위해 사용될 수 있으며, 이는 반드시 필요한 것은 아니고 경우에 따라 제거될 수 있다. 여기서, 수신 (공진) 코일(Rx coil)과 부하 코일(Load coil) 사이의 상호 인덕턴스 ML을 조절하여 임피던스 정합을 시킴으로써 임피던스 매칭 유닛(Rx matching unit)으로 기능하도록 할 수 있다. Also, in the receiver, the receiving (resonating) coil (Rx coil) of the receiver (coupled with the mutual inductance M 12 ) and the inductance M 12 (magnetic inductance L 2 in the equivalent circuit, the resistance is R 2 , the capacitance is C 2 ) and a load coil (magnetic inductance L L in the equivalent circuit, R L in the equivalent circuit) coupled to the magnetic coupling, and any of the load coil One end of the capacitor C L may be connected, and a load (impedance Z L ) is connected to both ends of the load coil (or both ends via the capacitor C L ) to form a structure that consumes power. The capacitor C L between the load coil and the load (impedance Z L ) can be used for matching the resonant frequency or impedance of the load coil of the source coil, which is not necessary and Can be removed accordingly. In this case, the impedance matching may be performed by adjusting the mutual inductance M L between the Rx coil and the load coil to function as an Rx matching unit.
상술한 바와 같이 본 발명에 따른 근거리 무선 전력전송 시스템에서는, 도 8과 같이 단일 코일을 이용하여 별도의 추가적인 회로 없이 20% 이내의 균일 상호 인덕턴스를 갖는 무선 전력 전송 거리 내에서 수신기와 송신기의 배치가, 상대적으로 중심이 수평적으로 위치 변동할 수 있도록(일정 거리 내에서 수직적 위치 변화도 허용함) 자유로운 Free positioning 이 가능하며, 상대적인 중심 위치가 수평적으로 다르게 놓인(일정 거리 내에서 수직적 위치 변화도 허용함) 복수개의 기기에서 각 수신 코일로 동시에 무선으로 전력을 수신하여 각 기기의 동작을 위한 전력 제공이나 충전이 가능하도록 하였다. 이와 같이 송수신기 간의 위치의 변경에 따라 적응형 임피던스 정합 회로를 사용하지 않아도 되기 때문에 시스템의 복잡도가 낮아지며, 가격 또한 저렴하게 시스템을 구성할 수 있다.As described above, in the short range wireless power transmission system according to the present invention, the arrangement of the receiver and the transmitter within the wireless power transmission distance having a uniform mutual inductance within 20% without a separate additional circuit using a single coil as shown in FIG. Free positioning is possible so that the center can be horizontally shifted relative to the center (allowing vertical position change within a certain distance), and the position of the vertical position where the relative center position is horizontally different (within a certain distance) Allow) It is possible to provide power or charge for the operation of each device by receiving power wirelessly from each of the multiple devices at the same time with each receiving coil. As the position between the transceivers is changed as described above, the system does not have to use an adaptive impedance matching circuit, thereby reducing the complexity of the system and configuring the system at a low cost.
균일 상호 인덕턴스를 갖는 코일 구조는 다양한 형태가 존재할 수 있으며, 특히 본 발명에서 제안한 도 5와 같은 코일 구조는 직렬로 연결된 여러 개의 코일을 사용하며, 각 코일(N1, N2, N3, N4,)은 등간격 또는 비등간격으로 연결될 수 있으며, 복수개의 코일이 병렬로 연결된 구조도 있으며, 이와 같은 병렬로 연결된 구조는 입력 전류 방향과 반대 방향으로 전류가 흐르는 코일일 수도 있고, 입력 전류 방향과 같은 방향으로 전류가 흐르는 코일일 수도 있다. 이와 같은 각 코일(N1, N2, N3, N4)의 배치에 있어서 도 5, 도 6과 같이 예시적으로 도시하였지만, 이에 한정되지 않으며, 각 코일(N1, N2, N3, N4)의 배치는 어느 위치 이든 상관이 없다. Coil structure having a uniform mutual inductance may have a variety of forms, in particular, the coil structure as shown in Figure 5 proposed in the present invention uses a plurality of coils connected in series, each coil (N 1 , N 2 , N 3 , N 4 ,) may be connected at equal intervals or boiling intervals, there are also a structure in which a plurality of coils are connected in parallel, such a parallel structure may be a coil in which the current flows in the direction opposite to the input current direction, the input current direction The coil may be a current flowing in the same direction. In the arrangement of the respective coils N 1 , N 2 , N 3 , and N 4 as illustrated in FIGS. 5 and 6, the present invention is not limited thereto, and the coils N 1 , N 2 , and N 3 are not limited thereto. , N 4 ) does not matter in any position.
이와 같은 코일 구조를 통하여 적어도 자기장이 약한 부분(제안된 코일 구조에서는 중심부)의 자기장은 증가시켜, 전체적으로 코일 구조체 주변(중심으로부터 일정 거리 이내)에서 일정 범위, 예를 들어, (최대 상호인덕턴스-최소 상호인덕턴스)/최대상호인덕턴스<0.2를 만족하도록 상호 인덕턴스를 유지할 수 있게 된다. 이는 코일의 모양의 변경으로 이루어지는 것이 아니라, 코일의 배치를 조정하여 얻어지는 것이다. 이는 도 21과 같이, 시뮬레이션 결과를 통하여 확인되었다. 즉, 도 21은 각 코일 구조(H1, H2, H3)로부터 1cm 높이에서 자기장(Hz)에 대한 시뮬레이션 결과로서, 그래프 H3는 도 5의 구조에서 N3, N4를 제거하였을 때의 결과이며, 그래프 H2는 도 5의 구조에서 N4를 제거하였을 때의 결과이며, 그래프 H1은 도 5의 구조 그대로이다. 도 21에서 알 수 있는 바와 같이, H2와 H3는 중심(radial displacement = rho = 0)의 자기장과 y 방향으로 평행하게 이동 거리 5cm 근처에서의 자기장 차이가 매우 크지만, H1의 경우는 중심에서의 자기장이 매우 크게 나오며 y 방향으로 평행하게 이동한 위치에 따라 자기장이 감소하였다가 증가하는 형태로 나타남을 알 수 있다. 도 21과 같이 자기장이 중심부보다 약한 부분인 주변부의 자기장이 H2나 H3 에서 보다 H1의 경우는 감소될 수 있으나, 이는 예시적인 것이고, 각 코일(N1, N2, N3, N4,)의 배치 상태나 코일의 감은 수 등에 따라 주변부의 자기장은 증가 또는 감소될 수 있다. Such a coil structure increases the magnetic field of at least the weak magnetic field (central in the proposed coil structure), thereby increasing the magnetic field as a whole, around the coil structure (within a certain distance from the center), for example (maximum mutual inductance-minimum). The mutual inductance can be maintained to satisfy the mutual inductance) / maximum mutual inductance <0.2. This is not done by changing the shape of the coil, but is obtained by adjusting the arrangement of the coil. This was confirmed through simulation results, as shown in FIG. 21. That is, FIG. 21 is a simulation result of the magnetic field H z at a height of 1 cm from each coil structure (H 1 , H 2 , H 3 ), and the graph H 3 removes N 3 and N 4 from the structure of FIG. 5. The result of the time, the graph H 2 is the result when N 4 is removed from the structure of FIG. 5, and the graph H 1 is the same as that of FIG. 5. As can be seen in FIG. 21, H 2 and H 3 have a large magnetic field difference near the 5 cm moving distance parallel to the magnetic field of the center (radial displacement = rho = 0) in the y direction, but in the case of H 1 It can be seen that the magnetic field is very large in the center and the magnetic field decreases and increases with the position moved in parallel in the y direction. As shown in FIG. 21, the magnetic field of the periphery where the magnetic field is weaker than the center may be reduced in the case of H 1 than in H 2 or H 3 , but this is merely an example, and each coil N 1 , N 2 , N 3 , N The magnetic field in the periphery may increase or decrease depending on the arrangement of 4 ,) or the number of turns of the coil.
이와 같은 균일 상호 인덕턴스를 갖는 코일 구조를 활용하여, 송수신기의 상호 위치가 변경되더라고 일정한 상호 인덕턱스 또는 성능 지수를 갖기 때문에, 미리 정해진 상호 인덕턴스에 적합한 임피던스 정합 회로를 송수신기에 구성하면 된다. 즉, 송수신기 위치에 따라 적합한 임피던스 매칭을 변경할 필요가 없다. 도 9 내지 도 20과 같이 임피던스 정합 회로는 다양한 구성이 존재한다. By utilizing the coil structure having such a uniform mutual inductance, even if the mutual position of the transceiver is changed, it has a constant mutual inductance or performance index, so that an impedance matching circuit suitable for a predetermined mutual inductance may be configured in the transceiver. That is, there is no need to change the appropriate impedance matching according to the transceiver position. 9 to 20, the impedance matching circuit has various configurations.
또한, 상대적인 중심 위치가 수평적으로 다르게 놓인(일정 거리 내에서 수직적 위치 변화도 허용함) 복수 기기 각각의 수신기에서 각 수신 코일(Rx coil)로 동시에 무선으로 전력을 수신하는 경우와 같이, 다중 부하가 있을 때에는 송신기 측의 입력 임피던스(Zin)가 그 수신 코일(Rx coil)의 수량 및 위치에 따라 달라질 수 있지만, 본 발명과 같이 균일 상호 인덕턴스를 갖는 송신 코일(Tx coil)의 적용으로 임피던스 매칭을 용이하게 구현할 수 있다. In addition, multiple loads, such as when the relative center position horizontally different (allowing vertical position changes within a certain distance) simultaneously receive power wirelessly with each Rx coil from each receiver of a plurality of devices. When the input impedance (Z in ) of the transmitter may vary depending on the number and position of the Rx coil, but impedance matching by the application of a transmission coil (Tx coil) having a uniform mutual inductance as in the present invention Can be easily implemented.
예를 들어, 이와 같은 다중 부하에 대해서는 입력 임피던스(Zin)가 수신기(Receiver) 또는 수신 코일(Rx coil)의 수량에 따라 변경되기 때문에, 송신기(Transmitter)에서 입력 임피던스(Zin) 센싱 회로(도면에서 표시하지 않음)를 통하여 그 수량의 따른 부하의 변동을 센싱하고, 다중 부하(수신기(Receiver) 또는 수신 코일(Rx coil))의 각 위치에는 상관없이 단지 그 수량에 따라 입력 임피던스(Zin)를 조절하여 임피던스 매칭이 이루어지도록 간단하게 구현이 가능하다. For example, for such multiple loads, since the input impedance Z in is changed according to the number of receivers or Rx coils, the input impedance Z in sensing transmitter ( The variation of the load according to the quantity is sensed through not shown in the figure, and the input impedance Z in according to the quantity is independent of each position of the multiple loads (receiver or Rx coil). ) Can be simply implemented to achieve impedance matching.
또한, 도10과 같이 별도의 송신 코일을 삽입하여, 최대 부하 개수 및 그 이하에서도 항상 높은 효율을 갖도록 송신 코일을 적절하게 설계하여 다중 기기에 대한 임피던스 정합을 시켜줄 수 있다.In addition, as shown in FIG. 10, by inserting a separate transmission coil, the transmission coil may be appropriately designed to always have high efficiency even at the maximum number of loads or less, and thus impedance matching for multiple devices may be performed.
종래와 같이 균일 상호 인덕턴스를 갖지 않는 기존의 비균일 상호 인덕턴스 구조에서는 개별 수신기에 의한 상호 인덕턴스가 제각각 다르고 상호 인덕턴스의 변화가 크기 때문에 하나의 송신기로 복수의 부하를 지원할 수가 없는 문제가 있으나, 본 발명과 같이 입력 임피던스(Zin) 센싱 회로(도면에서 표시하지 않음)를 통하여 수량에 따른 부하량 변동을 간단히 센싱하고 그에 맞게 입력 임피던스가 조절되도록 송신기의 임피던스 매칭 유닛(Tx matching unit)의 저항값, 인덕턴스값, 또는 커패시턴스값을 제어하여 임피던스 매칭이 이루어지도록 함으로써 최대 전력전달 효율(η)로 무선 전력의 송수신이 가능하게 할 수 있다. 임피던스 매칭 유닛(Tx matching unit)의 저항값, 인덕턴스값, 또는 커패시턴스값 등의 제어는 별도의 저항, 인덕터, 커패시터 등이 회로 상에 추가되거나 제거되도록 스위칭 수단(예, MOSFET, BJT, SCR, Thyrister 등)을 제어함으로써 이루어질 수 있다. In the conventional non-uniform mutual inductance structure that does not have a uniform mutual inductance as in the prior art, there is a problem in that a plurality of loads cannot be supported by one transmitter because mutual inductances by individual receivers are different and mutual inductances are large. As shown in the figure, the input impedance (Z in ) sensing circuit (not shown) simply senses the load variation according to the quantity and adjusts the input impedance accordingly so that the resistance value and the inductance of the Tx matching unit of the transmitter are adjusted. By controlling the value or the capacitance value so that impedance matching can be performed, it is possible to transmit and receive wireless power at the maximum power transfer efficiency η. Control of the resistance, inductance, or capacitance values of the Tx matching unit can be achieved by switching means (e.g. MOSFET, BJT, SCR, Thyrister) so that a separate resistor, inductor, capacitor, etc. can be added or removed from the circuit. And the like).
이상과 같이 본 발명은 비록 한정된 실시예와 도면에 의해 설명되었으나, 본 발명은 상기의 실시예에 한정되는 것은 아니며, 본 발명이 속하는 분야에서 통상의 지식을 가진 자라면 이러한 기재로부터 다양한 수정 및 변형이 가능하다. 그러므로, 본 발명의 범위는 설명된 실시예에 국한되어 정해져서는 아니 되며, 후술하는 특허청구범위뿐 아니라 이 특허청구범위와 균등한 것들에 의해 정해져야 한다.As described above, the present invention has been described by way of limited embodiments and drawings, but the present invention is not limited to the above embodiments, and those skilled in the art to which the present invention pertains various modifications and variations from such descriptions. This is possible. Therefore, the scope of the present invention should not be limited to the described embodiments, but should be determined not only by the claims below but also by the equivalents of the claims.
Claims (37)
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| US14/406,993 US9711278B2 (en) | 2013-01-09 | 2013-10-17 | Wireless power transmission system for free-position wireless charging of multiple devices |
| US15/624,510 US10141105B2 (en) | 2013-01-09 | 2017-06-15 | Wireless power transmission system for free-position wireless charging of multiple devices |
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| KR20130002460 | 2013-01-09 | ||
| KR1020130077561A KR101497140B1 (en) | 2013-01-09 | 2013-07-03 | Wireless Power Transfer System for Free Positioning Charging of Multiple Devices |
| KR10-2013-0077561 | 2013-07-03 |
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| US14/406,993 A-371-Of-International US9711278B2 (en) | 2013-01-09 | 2013-10-17 | Wireless power transmission system for free-position wireless charging of multiple devices |
| US15/624,510 Continuation US10141105B2 (en) | 2013-01-09 | 2017-06-15 | Wireless power transmission system for free-position wireless charging of multiple devices |
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| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| WO2016108949A1 (en) * | 2014-12-31 | 2016-07-07 | Massachusetts Institute Of Technology | Adaptive control of wireless power transfer |
| US9800076B2 (en) | 2014-02-14 | 2017-10-24 | Massachusetts Institute Of Technology | Wireless power transfer |
| WO2018004130A1 (en) * | 2016-06-30 | 2018-01-04 | 엘지이노텍(주) | Shape of wireless power transmission coil and coil configuration method |
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| Publication number | Priority date | Publication date | Assignee | Title |
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| US9800076B2 (en) | 2014-02-14 | 2017-10-24 | Massachusetts Institute Of Technology | Wireless power transfer |
| US9882419B2 (en) | 2014-02-14 | 2018-01-30 | Massachusetts Institute Of Technology | Adaptive control of wireless power transfer |
| US10491048B2 (en) | 2014-02-14 | 2019-11-26 | Massachusetts Institute Of Technology | Wireless power transfer |
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| US11201502B1 (en) | 2020-06-16 | 2021-12-14 | Nxp Usa, Inc. | Hybrid wireless power transfer system for an electronic device |
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