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International Journal of Electrical and Computer Engineering (IJECE)
Vol. 10, No. 3, June 2020, pp. 2245~2249
ISSN: 2088-8708, DOI: 10.11591/ijece.v10i3.pp2245-2249  2245
Journal homepage: http://ijece.iaescore.com/index.php/IJECE
Wireless power transfer using
multiple-transmitters for high stability for position
Kazuma Onishi, Kazuya Yamaguchi, Kenichi Iida
Department of Control Engineering, National Institute of Technology, Nara College, Japan
Article Info ABSTRACT
Article history:
Received May 24, 2019
Revised Nov 5, 2019
Accepted Nov 24, 2019
The aim of this study is to optimize the system in the wireless power supply
using multiple transmitters by algebraically analyzing the effects of both
a circuit parameter and an axis displacement, etc. In addition to these analyses,
the other aim is designing, producing and evaluating wireless charger with
high stability for position. In the proposed method, we analyzed the situation
in which three transmitters are used as power sources. It is turned out that
the optimum arrangement of three transmitters is equilateral triangular from
Biot-Savart law and circuit equation. In the experiment, transmitted power is
measured when the receiver is moved on the vertical plane in regard to central
axis of coils. It is confirmed that 4~4.5mW is transmitted at the face-to-face of
transmitters and 2.4mW is transmitted at the center of transmitters.
Keywords:
Axial displacement
Multiple transmitter
Wireless power transfer
Copyright © 2020 Institute of Advanced Engineering and Science.
All rights reserved.
Corresponding Author:
Kazuya Yamaguchi,
Department of Control Engineering, National Institute of Technology, Nara College,
22 Yata-cho, Yamatokoriyama, Nara, Japan.
Email: k-yamaguchi@ctrl.nara-k.ac.jp
1. INTRODUCTION
1Wireless power transfer (WPT) has been studied in various fields such as industry [1, 2],
manufacturing [3], medicine [4, 5], and information [6, 7]. The basic principle has been proposed in the 19th
century, and since the MIT report in 2007 [8], it has much attracted many researchers. Recently, many papers
about WPT have been published, and various products have been examining and commercializing.
For example, studies such as examination of design of coils [9-12] and comparison of efficiency by change of
applied voltage waveform [13, 14], are investigating. As products, WPT system is applied for power supply
on various fields, for instance mobile devices and IoT [15], vehicles traveling on the road [16-19], and micro
implant devices [20-22]. As mentioned above, researches finding ideal conditions are actively conducted to
improve the performance of WPT [23, 24].
On the other hand, analysis of the situations which degrade performance are not viewed as important,
for example leakage flux and misalignment between transmitters and receivers [25, 26]. As a result, there are
some restrictions with relation to design of circuits. On the other hand, considering flexibility of the receiver
position, the size of the receiving coil depends on the receiving device, and the loss due to leakage magnetic
flux etc. occurs remarkably when transmitting coil is too large. Therefore, it is assumed that it is more
advantageous to operate WPT circuit by using a few coils than to handle a single large coil in some situations.
This paper aims realization of stable power transmission regardless of the position of the receiving
coil with using multiple transmitters. In order to utilize multiple transmitters, the electromagnetic interaction
between transmitters and receiver must be considered. A calculation method is considered and a mathematical
formula based on electromagnetism and circuit theory is expressed so that the user could arbitrarily
set parameters such as the number and position of transmitters to improve the versatility. Finally,
the experimental verification is performed using the actually designed electric circuit, and it is compared with
the theoretical result.
 ISSN: 2088-8708
Int J Elec & Comp Eng, Vol. 10, No. 3, June 2020 : 2245 - 2249
2246
2. CALCULATION OF POWER
2.1. Calculation of mutual inductance occurred between two coils arranged in three-dimensional space
Analysis is performed on the case where two coils are arranged in a three-dimensional space in
Figure 1. The coordinate of the transmitting coil is (0,0,0), and the coordinate of the receiving coil is
(d_x,d_y,h). At this time, d_x and d_y represent an off-axis distance from z-axis, and h represents a facing
distance between the coils.
Figure 1. Two coils arranged in three-dimensional space
From the above, the mutual inductance between the coils is obtained according to the Biot-Savart law as
follows:
𝑀 ≃
𝜇0 𝑆1 𝑆2
2𝜋(𝑟1
2+𝑑 𝑥
2+𝑑 𝑦
2+ℎ2)
3
2
[H] (2)
𝑆1 = 𝜋𝑟1
2
𝑁1, 𝑆2 = 𝜋𝑟2
2
𝑁2
2.2. Power calculation of wireless power transfer circuits using three transmitting circuits
A wireless power transfer circuit for charging a battery is designed as follows in Figure 2. The left
side is a group of transmitting circuits, and the right side is a receiving circuit which contains which battery
device. 𝑢 is the voltage of power supply, 𝑅1, 𝑅2, 𝑅3, 𝑅0, 𝐶1, 𝐶2, 𝐶3, 𝐶0 are parasitic components, 𝐿1, 𝐿2, 𝐿3, 𝐿0
are the self inductances, 𝑀10, 𝑀20, 𝑀30 are mutual inductances between transmitting circuits and receiving
circuit, 𝑀12, 𝑀13, 𝑀23 are mutual inductances between both transmitting circuits and 𝑅 𝐿 is the resistance of
device. From Figure 2, a circuit equation is obtained as (2).
Figure 2. Wireless power transfer circuits using three transmitting circuits
Int J Elec & Comp Eng ISSN: 2088-8708 
Wireless power transfer using multiple-transmitters for high stability for position (Kazuma Onishi)
2247
[
𝑢
𝑢
𝑢
0
] = [
𝑍1 𝑗𝜔𝑀12 𝑗𝜔𝑀13 𝑗𝜔𝑀10
𝑗𝜔𝑀12 𝑍2 𝑗𝜔𝑀23 𝑗𝜔𝑀20
𝑗𝜔𝑀13 𝑗𝜔𝑀23 𝑍3 𝑗𝜔𝑀30
𝑗𝜔𝑀10 𝑗𝜔𝑀20 𝑗𝜔𝑀30 𝑍0
] [
𝑖1
𝑖2
𝑖3
𝑖0
] (2)
𝑍 𝑛 = 𝑅 𝑛 + (𝑗𝜔𝐶 𝑛)−1
+ 𝑗𝜔𝐿 𝑛[Ω], 𝑛 = 0,1,2,3
The power at the load 𝑃L can be obtained by solving the current 𝑖 𝑜 of receiving circuit from the above
simultaneous equations and substituting it into the following equation:
𝑃load = 𝑅L 𝑖0
2
[W] (3)
3. EXPERIMENTAL VERIFICATION
3.1. Condition of experiment for wireless power transfer by using three transmitting circuits
The experimental circuit is shown in Figure 3. The values of the circuit elements and the setting of
the coordinate conditions are shown in Table 1 and Table 2 respectively.
Figure 3. Experimental circuit
Table 1. Values of circuit elements
Values of circuit elements
𝑅1 46.5Ω 𝑅2 46.3Ω 𝑅3 46.7Ω 𝑅0 46.8Ω
𝐶1 367pF 𝐶2 374pF 𝐶3 360pF 𝐶0 372pF
𝐿1 24.8μH 𝐿2 24.8μH 𝐿3 24.9μH 𝐿0 24.9μH
Table 2. The coordinate conditions
Parameters Values [mm]
Facing distance between coils ℎ 15 or 35
Center coordinates of transmitting coils (-25-25,ℎ) , (25,-25,ℎ) , (0,25,ℎ)
Moving range in the 𝑥-axis direction -50~50
Moving range in the 𝑦-axis direction -50~50
Moving width in the 𝑥-axis direction 5
Moving width in the 𝑦-axis direction 10
3.2. Variation of load power versus receiver coil coordinates
The variation of load power is investigated by changing the coordinates of the receiving coil with
respect to the transmitting coil and the facing distance between the transmitting coil and the receiving coil.
The calculated power is shown in Figures 4 and 5, and the experimental power are shown in Figures 6 and 7,
respectively.
 ISSN: 2088-8708
Int J Elec & Comp Eng, Vol. 10, No. 3, June 2020 : 2245 - 2249
2248
Figure 4. Calculated power where ℎ = 15mm Figure 5. Calculated power where ℎ = 35mm
Figure 6. Experimental power where ℎ = 15mm Figure 7. Experimental power where ℎ = 35mm
3.3. Discussion
The comparison of the maximum power and the stability region is shown in Table 3. Then,
the stability region is a range in which the output power is 80% or more of the maximum power. As the facing
distance of the coils increases, the maximum power decreases significantly while the stability region expands.
Therefore, it is important to consider the trade-off between power and region in the situation. The defect in
the approximation of calculation and experimental circuit are considered as the cause of error.
Table 3. Maximum power and Stability region
Maximum power [mW] Stability region [%]
ℎ = 15mm ℎ = 35mm ℎ = 15mm ℎ = 35mm
Calculated 17.82 1.585 9.62 38.4
Experiment 9.55 4.65 12.6 4.8
4. CONCLUSION
This study tried to realize stable wireless power transfer regardless of the arrangement of receiving
coil by using multiple transmitters in the circuit. Mutual inductance was derived by using geometrical equation
and the power was obtained from the circuit equation considering interactions. Moreover, experiments were
performed to prove the validity of the calculation and investigate errors and their causes. As a result, while it
was possible to transmit power less than that of expectation, some similarities were found in the trends.
In the future, it is necessary to consider the increase in transmission power, the improvement in efficiency, and
the effects caused by the increase in coils.
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2249
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Wireless power transfer using multiple-transmitters for high stability for position

  • 1. International Journal of Electrical and Computer Engineering (IJECE) Vol. 10, No. 3, June 2020, pp. 2245~2249 ISSN: 2088-8708, DOI: 10.11591/ijece.v10i3.pp2245-2249  2245 Journal homepage: http://ijece.iaescore.com/index.php/IJECE Wireless power transfer using multiple-transmitters for high stability for position Kazuma Onishi, Kazuya Yamaguchi, Kenichi Iida Department of Control Engineering, National Institute of Technology, Nara College, Japan Article Info ABSTRACT Article history: Received May 24, 2019 Revised Nov 5, 2019 Accepted Nov 24, 2019 The aim of this study is to optimize the system in the wireless power supply using multiple transmitters by algebraically analyzing the effects of both a circuit parameter and an axis displacement, etc. In addition to these analyses, the other aim is designing, producing and evaluating wireless charger with high stability for position. In the proposed method, we analyzed the situation in which three transmitters are used as power sources. It is turned out that the optimum arrangement of three transmitters is equilateral triangular from Biot-Savart law and circuit equation. In the experiment, transmitted power is measured when the receiver is moved on the vertical plane in regard to central axis of coils. It is confirmed that 4~4.5mW is transmitted at the face-to-face of transmitters and 2.4mW is transmitted at the center of transmitters. Keywords: Axial displacement Multiple transmitter Wireless power transfer Copyright © 2020 Institute of Advanced Engineering and Science. All rights reserved. Corresponding Author: Kazuya Yamaguchi, Department of Control Engineering, National Institute of Technology, Nara College, 22 Yata-cho, Yamatokoriyama, Nara, Japan. Email: k-yamaguchi@ctrl.nara-k.ac.jp 1. INTRODUCTION 1Wireless power transfer (WPT) has been studied in various fields such as industry [1, 2], manufacturing [3], medicine [4, 5], and information [6, 7]. The basic principle has been proposed in the 19th century, and since the MIT report in 2007 [8], it has much attracted many researchers. Recently, many papers about WPT have been published, and various products have been examining and commercializing. For example, studies such as examination of design of coils [9-12] and comparison of efficiency by change of applied voltage waveform [13, 14], are investigating. As products, WPT system is applied for power supply on various fields, for instance mobile devices and IoT [15], vehicles traveling on the road [16-19], and micro implant devices [20-22]. As mentioned above, researches finding ideal conditions are actively conducted to improve the performance of WPT [23, 24]. On the other hand, analysis of the situations which degrade performance are not viewed as important, for example leakage flux and misalignment between transmitters and receivers [25, 26]. As a result, there are some restrictions with relation to design of circuits. On the other hand, considering flexibility of the receiver position, the size of the receiving coil depends on the receiving device, and the loss due to leakage magnetic flux etc. occurs remarkably when transmitting coil is too large. Therefore, it is assumed that it is more advantageous to operate WPT circuit by using a few coils than to handle a single large coil in some situations. This paper aims realization of stable power transmission regardless of the position of the receiving coil with using multiple transmitters. In order to utilize multiple transmitters, the electromagnetic interaction between transmitters and receiver must be considered. A calculation method is considered and a mathematical formula based on electromagnetism and circuit theory is expressed so that the user could arbitrarily set parameters such as the number and position of transmitters to improve the versatility. Finally, the experimental verification is performed using the actually designed electric circuit, and it is compared with the theoretical result.
  • 2.  ISSN: 2088-8708 Int J Elec & Comp Eng, Vol. 10, No. 3, June 2020 : 2245 - 2249 2246 2. CALCULATION OF POWER 2.1. Calculation of mutual inductance occurred between two coils arranged in three-dimensional space Analysis is performed on the case where two coils are arranged in a three-dimensional space in Figure 1. The coordinate of the transmitting coil is (0,0,0), and the coordinate of the receiving coil is (d_x,d_y,h). At this time, d_x and d_y represent an off-axis distance from z-axis, and h represents a facing distance between the coils. Figure 1. Two coils arranged in three-dimensional space From the above, the mutual inductance between the coils is obtained according to the Biot-Savart law as follows: 𝑀 ≃ 𝜇0 𝑆1 𝑆2 2𝜋(𝑟1 2+𝑑 𝑥 2+𝑑 𝑦 2+ℎ2) 3 2 [H] (2) 𝑆1 = 𝜋𝑟1 2 𝑁1, 𝑆2 = 𝜋𝑟2 2 𝑁2 2.2. Power calculation of wireless power transfer circuits using three transmitting circuits A wireless power transfer circuit for charging a battery is designed as follows in Figure 2. The left side is a group of transmitting circuits, and the right side is a receiving circuit which contains which battery device. 𝑢 is the voltage of power supply, 𝑅1, 𝑅2, 𝑅3, 𝑅0, 𝐶1, 𝐶2, 𝐶3, 𝐶0 are parasitic components, 𝐿1, 𝐿2, 𝐿3, 𝐿0 are the self inductances, 𝑀10, 𝑀20, 𝑀30 are mutual inductances between transmitting circuits and receiving circuit, 𝑀12, 𝑀13, 𝑀23 are mutual inductances between both transmitting circuits and 𝑅 𝐿 is the resistance of device. From Figure 2, a circuit equation is obtained as (2). Figure 2. Wireless power transfer circuits using three transmitting circuits
  • 3. Int J Elec & Comp Eng ISSN: 2088-8708  Wireless power transfer using multiple-transmitters for high stability for position (Kazuma Onishi) 2247 [ 𝑢 𝑢 𝑢 0 ] = [ 𝑍1 𝑗𝜔𝑀12 𝑗𝜔𝑀13 𝑗𝜔𝑀10 𝑗𝜔𝑀12 𝑍2 𝑗𝜔𝑀23 𝑗𝜔𝑀20 𝑗𝜔𝑀13 𝑗𝜔𝑀23 𝑍3 𝑗𝜔𝑀30 𝑗𝜔𝑀10 𝑗𝜔𝑀20 𝑗𝜔𝑀30 𝑍0 ] [ 𝑖1 𝑖2 𝑖3 𝑖0 ] (2) 𝑍 𝑛 = 𝑅 𝑛 + (𝑗𝜔𝐶 𝑛)−1 + 𝑗𝜔𝐿 𝑛[Ω], 𝑛 = 0,1,2,3 The power at the load 𝑃L can be obtained by solving the current 𝑖 𝑜 of receiving circuit from the above simultaneous equations and substituting it into the following equation: 𝑃load = 𝑅L 𝑖0 2 [W] (3) 3. EXPERIMENTAL VERIFICATION 3.1. Condition of experiment for wireless power transfer by using three transmitting circuits The experimental circuit is shown in Figure 3. The values of the circuit elements and the setting of the coordinate conditions are shown in Table 1 and Table 2 respectively. Figure 3. Experimental circuit Table 1. Values of circuit elements Values of circuit elements 𝑅1 46.5Ω 𝑅2 46.3Ω 𝑅3 46.7Ω 𝑅0 46.8Ω 𝐶1 367pF 𝐶2 374pF 𝐶3 360pF 𝐶0 372pF 𝐿1 24.8μH 𝐿2 24.8μH 𝐿3 24.9μH 𝐿0 24.9μH Table 2. The coordinate conditions Parameters Values [mm] Facing distance between coils ℎ 15 or 35 Center coordinates of transmitting coils (-25-25,ℎ) , (25,-25,ℎ) , (0,25,ℎ) Moving range in the 𝑥-axis direction -50~50 Moving range in the 𝑦-axis direction -50~50 Moving width in the 𝑥-axis direction 5 Moving width in the 𝑦-axis direction 10 3.2. Variation of load power versus receiver coil coordinates The variation of load power is investigated by changing the coordinates of the receiving coil with respect to the transmitting coil and the facing distance between the transmitting coil and the receiving coil. The calculated power is shown in Figures 4 and 5, and the experimental power are shown in Figures 6 and 7, respectively.
  • 4.  ISSN: 2088-8708 Int J Elec & Comp Eng, Vol. 10, No. 3, June 2020 : 2245 - 2249 2248 Figure 4. Calculated power where ℎ = 15mm Figure 5. Calculated power where ℎ = 35mm Figure 6. Experimental power where ℎ = 15mm Figure 7. Experimental power where ℎ = 35mm 3.3. Discussion The comparison of the maximum power and the stability region is shown in Table 3. Then, the stability region is a range in which the output power is 80% or more of the maximum power. As the facing distance of the coils increases, the maximum power decreases significantly while the stability region expands. Therefore, it is important to consider the trade-off between power and region in the situation. The defect in the approximation of calculation and experimental circuit are considered as the cause of error. Table 3. Maximum power and Stability region Maximum power [mW] Stability region [%] ℎ = 15mm ℎ = 35mm ℎ = 15mm ℎ = 35mm Calculated 17.82 1.585 9.62 38.4 Experiment 9.55 4.65 12.6 4.8 4. CONCLUSION This study tried to realize stable wireless power transfer regardless of the arrangement of receiving coil by using multiple transmitters in the circuit. Mutual inductance was derived by using geometrical equation and the power was obtained from the circuit equation considering interactions. Moreover, experiments were performed to prove the validity of the calculation and investigate errors and their causes. As a result, while it was possible to transmit power less than that of expectation, some similarities were found in the trends. In the future, it is necessary to consider the increase in transmission power, the improvement in efficiency, and the effects caused by the increase in coils. REFERENCES [1] Giuseppe Faraci, Angelo Raciti, Santi Agatino Rizzo, Giovanni Schembra, "Green wireless power transfer system for a drone fleet managed by reinforcement learning in smart industry," Applied Energy, Available online 29 November 2019, 114204, pp.1-12, 2019. [2] Hans De Clercq, Robert Puers, "Contactless energy transfer at the bedside featuring an online power optimization strategy," Sensors and Actuators A 217 (2014), pp.160-167, 2014.
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