New Analysis Method for Wireless Power Transfer System with Multiple n Resonators
 Author: Kim JuHui, Park ByungChul, Lee JeongHae
 Organization: Kim JuHui; Park ByungChul; Lee JeongHae
 Publish: Journal of electromagnetic engineering and science Volume 13, Issue3, p173~177, 30 Sep 2013

ABSTRACT
This paper presents a new method for analyzing the maximum efficiency of a wireless power transfer (WPT) system with multiple
n resonators. The method is based on ABCD matrices and allows transformation of the WPT system with multiplen resonators into a single twoport network system. The general maximum efficiency equation of a WPT system with multiplen resonators is derived using the ABCD matrix. Use of this equation allows placement of the relay resonators for maximum efficiency even though they are asymmetrical. The general maximum efficiency equation and the method of the optimum placement are verified by a full wave simulation. The results show that the method is useful for the analysis of a WPT system with relay resonators.

KEYWORD
ABCD Matrix , Optimum Placement , Relay Resonators , TwoPort Network Theory , Wireless Power Transfer.

Ⅰ. Introduction
Many researchers are currently investigating magnetically coupled wireless power transfer (WPT) systems. A conventional WPT system consists of two main resonators for the transmitter and receiver, which operate at the same resonance frequency [13]. This system, however, has a limitation on the distance between transmitter and receiver for achieving high WPT efficiency. This limitation can be overcome by using some resonators as relays between the two main resonators [4]. The WPT system is then composed of multiple
n resonators, which can achieve a higher WPT efficiency than a conventional WPT system can at the same distance. This system is well analyzed in [5] with respect to the general circuit model and the maximum efficiency with a matched load. However, the general maximum efficiency equation of a WPT system with multiplen resonators described in [5] becomes complicated when analyzing the type of system normally utilized for practical applications.This paper proposes a new analysis method for the WPT system with multiple
n resonators. The method simplifies the entire WPT system into a single two port network expressed by an ABCD matrix. The general maximum efficiency equation of the WPT system with multiplen resonators can then be obtained with elements of the ABCD matrix. This equation provides a much more convenient way to obtain the maximum efficiency and the optimum placement of the asymmetrical relays for the best utilization. The general maximum efficiency equation and the method of the optimum placement of the asymmetrical relays are verified by a full wave simulation of ANSYS HFSS (high frequency structural simulator).Ⅱ. New Analysis Method Using the ABCD Matrix
The schematic diagram of a WPT system with multiple
n resonators is shown in Fig. 1(a). The nonadjacent coupling coefficient is ignored since it is very small in a practical WPT system with the relays. Thus, the WPT system with multiplen resonators can be considered asn ―1 parts of twoport networks connected in series, as shown in Fig. 1(b). Twoport networks have three types of connections: transmitterrelay, relayrelay, and relay receiver. The system in Fig. 1(b) can then be represented as the single twoport network shown in Fig. 1(c) by the matrix multiplication of ABCD matrices. The maximum efficiency equation in [1] can be adapted for this single equivalent twoport network system because the WPT system with two resonators is also a single twoport network.R_{L} at the end of the circuits in Fig. 1(b) and (c) is a matched load required to obtain the maximum efficiency of the WPT system. The matched loadR_{L} can be connected to the receiver either directly or indirectly by inductive coupling with the feeding loop. When the load impedanceZ_{L} is connected through the feeding loop,R_{L} can be expressed with the elements of a feeding loop as:where
κ_{s} is a coupling coefficient between a feeding loop and the receiver,L is the inductance of receiver, andL_{f} is the inductance of a feeding loop.In order to obtain ABCD matrices for three types of twoport networks shown in Fig. 1(b), the circuit equations of a WPT system are needed. When the system operates at the resonance frequency (
f =f_{0} ), the circuit equations derived from Fig. 1(b) are the following equations:Then, Z matrices of each twoport network are obtained by (2)―(4), and they can be transformed into ABCD matrices [6] following Table 1, where
C _{i―1} is(
i =2 ,3 , …,n ), andκ _{i―1} is the coupling coefficient betweeni 1th resonator andi th resonator. The single ABCD matrix of the WPT system with multiplen resonators can then be obtained. Finally, the system is equivalent to a WPT system with two resonators.The maximum efficiency (
η _{max}) equation of the WPT system with two resonators can be applied to the WPT system with multiplen resonators:where
is the figure of merit of a WPT system with two resonators, and
Q_{i} =ω_{o}L_{i} /R_{i} (i =1, 2) is the quality factor of each resonator [1]. The figure of meritU can also be written in terms of elements of the Z matrix and ABCD matrix:where
Z_{ij} (i =1, 2 andj =1, 2) is the element of the Z matrix, andA andD are the elements of the ABCD matrix of the WPT system with 2 resonators. The figure of meritU in terms of the elements of ABCD matrix can be applied to a WPT system with multiplen relays using the elements of its single ABCD matrix and it is renamedU' .The Eq. (5),
η_{max} , should also be modified to make a general maximum efficiency equation because Eq. (5) is suitable only for a WPT system with two resonators. The WPT systems with multiplen resonators are classified into two types of systems by the phase difference of the current on the receiving resonator. The phase difference isπ /2 between the odd and even numbers of resonators. Thus, the modification of phase for power isj^{2} , which is multiplied in Eq. (5) when the number of resonators is odd. Finally, the general maximum efficiency equation of a WPT system with multiplen resonators is given by:As an example, the maximum efficiency equations of WPT systems with three and four resonators derived by (6) and (7) are represented as:
where
U _{i―1}^{2} =κ _{i―1}^{2} Q _{i―1}Q_{i} (i =2 ,3 , …,n ) is the square of figure of merit betweeni 1 th resonator andi th resonator.Q_{i} =ω_{0}L_{i} /R_{i} is the quality factor ofi th resonator. The matched loadR_{L} is also expressed with the elements of ABCD matrix.The maximum efficiency of a WPT system with multiple
n resonators and the matched loadR_{L} can then be obtained by the elements of the single equivalent ABCD matrix for the system, (6), (7), and (10). These equations provide a much simpler form than those in [5].The maximum efficiencies calculated by Eq. (7) are compared with those simulated by ANSYS HFSS, as shown in Fig. 2. The systems operate at 6.78 MHz and have three and four identical resonators, as shown in Fig. 2(a) and (b), respectively. The square resonators [7] used for this system have the following dimensions:
a =20 cm,w =2 cm,t =0.2 cm, andC =1,498 pF, and the material of resonators is assigned as copper. The total distance of both systems is changed from 30 to 90 cm. The resonators in the WPT system are equally spaced and haveQ_{i} of 950, and the coupling coefficientκ_{i} is found from even and odd mode analysis at each corresponding distance between two adjacent resonators [1]. In Fig. 2(c), the efficiencies obtained by two different methods agree well, indicating the validation of the derived equations. However, small differences appear as the distance increases due to the nonadjacent coupling. As the distance gets progressively longer, the difference between the adjacent and nonadjacent coupling coefficient become smaller and, thus, the nonadjacent coupling coefficient has a much stronger influence on the efficiency.Ⅲ. Optimum Placement of Asymmetrical Relays
The optimum placement of a WPT system with the asymmetrical relay resonators can also be found with (7). When the WPT system has different sizes of resonators or more than 2 relays, the maximum efficiency will be determined not by the equal spacing but by the optimum placement. The optimum placement should be found by observing the maximum efficiencies at the various placements. These can be easily obtained by calculating (7) with respect to different placements. The optimum placement can then be found from the peak value of the calculation from (7).
This method is verified by constructing the WPT system with four resonators shown in Fig. 3(a). The system operates at 6.78 MHz and has four square resonators, as shown in Fig. 3(a). Each resonator has
Q _{1}=Q _{4} of 878,Q _{2} of 1,004,Q _{3} of 567, and the adjacent coupling coefficients are changed by the different distances. The square resonators [7], assigned as copper, used for this system have the following dimensions:a _{1}=a _{4}=20 cm,a _{2}=30 cm,a _{3}=10 cm;w _{1}=w _{2}=w _{4}=2 cm,w _{3}=1.5 cm;t =0.2 cm; andC _{1}=C _{4}=1,467 pF,C _{2}=804 pF,C _{3}=3,860 pF. The total distance between the transmitter and receiver is 75 cm. The optimum distance ofd _{1} andd _{2} should be determined to obtain the maximum efficiency. The maximum efficiencies calculated using Eq. (7) are compared with those simulated by ANSYS HFSS, as shown in Fig. 3(b), changingd _{1} andd _{2} from 28 to 38 cm and from 10 to 20 cm, respectively. The results from calculation and simulation are obtained at every 1 cm. The coupling coefficients used for calculated maximum efficiencies are calculated from the field calculation ofH_{Z} in [8]. The maximum efficiencies and the optimum placement of the WPT system for the verification can then be found from simulation and calculation. The optimum placement is found atd _{1}=34 cm,d _{2}=16 cm with the efficiency of 81.17% from the simulation and atd _{1}=37 cm,d _{2}=15 cm with the efficiency of 77.3% from the calculation. The results show that the tendency for variation in both methods agrees well, despite the small difference caused by the nonadjacent coupling. Thus, the maximum efficiency and the optimum placement can be found quite simply using the proposed calculation.Ⅳ. Conclusion
A simple method to obtain the maximum efficiency of a WPT system with multiple
n resonators is presented in this paper. This method is based on ABCD matrices and allows the WPT system with multiplen resonators to be transformed into a single twoport network system. The general maximum efficiency equation of a WPT system with multiplen resonators is derived using the ABCD matrix and is verified by a full wave simulation. This equation is also applied to a WPT system with asymmetrical relays for placement of the relays for the maximum efficiency. The method of optimum placement is also verified by a full wave simulation. The results indicate that our method can be extended to analyze WPT systems with asymmetrical relay resonators.

[Fig. 1.] (a) Wireless power transfer (WPT) system with n resonators, (b) the equivalent circuit model of a WPT system with n resonators at the resonance frequency (f=f0), and (c) the equivalent twoport network of a WPT system with n resonators.

[Table 1.] The Z matrix and ABCD matrix of each divided twoport network of a wireless power transfer system

[Fig. 2.] (a) Wireless power transfer (WPT) system with three identical resonators, (b) WPT system with four identical resonators, and (c) maximum efficiency of WPT systems with three and four resonators at 6.78 MHz. HFSS=high frequency structural simulator.

[Fig. 3.] (a) Wireless power transfer (WPT) system with two asymmetric relay resonators and (b) maximum efficiency having different size of relay resonators at 6.78 MHz.