For a segmented dynamic wireless power transfer (DWPT) system, when electric vehicles (EVs) move over two adjacent transmitting coils, the received power fluctuates greatly and has some loss. Arming at this problem, this paper proposes a dual receiver segmented DWPT topology to reduce the received power fluctuation of the receiving coil passing through the rail junction during the moving process of the EV. Through magnetic field analysis in this paper, tuning the current phase difference between two adjacent transmitting coils to 180° can enhance the magnetic field. In this paper, a dual receiver series topology (DRST) is designed to pick up power, which consists of four fully controlled components and four diodes. According to EVs’ real-time position, the segment DWPT system has three working modes and six working states under the control of DRST. Finally, experiments are carried out. Compared to the single-receiving-coil system, DRST is effective in improving the average output power from 2.007 to 5.657 W and significantly reducing the power fluctuation.

With global energy exhaustion and environmental pollution becoming increasingly prominent, EVs have developed rapidly with the advantages of being clean, energy-saving, and pollution-free.1–3 The traditional wired charging mode of EVs has many potential problems, such as high loss of charging line, mechanical wear, contact with sparks, etc. Wireless charging technology for EVs can effectively solve these problems.4–6 Stationary Wireless Power Transfer (SWPT) and Dynamic Wireless Power Transfer (DWPT) are the main wireless charging modes. For SWPT, fixed charging position and poor anti-offset are the main factors against the popularity of EVs.7–10 As a result, DWPT technology for EVs came into being and became the research focus of many scholars and institutions, which could provide power for EVs when they are moving. Meanwhile, it can reduce the battery capacity requirement or even no batteries with a long mileage.11–14 

In the EVs DWPT system, the transmitting coil buried under the road generates a high-frequency alternating magnetic field, and then the induced electromotive force could be obtained in the receiving coil located in EVs.15–17 The existing literature summarized the development of wireless power supply technology.18,19 Existing literature also studied the magnetic coupling coefficient of EV wireless charging systems, which provided a theoretical basis for the design and optimization of the magnetic coupling coils.20,21 Due to the range and battery capacity issues of electric vehicles, there are many existing studies on dynamic wireless charging. However, the existing dynamic wireless charging modes also have some issues. The long-track DWPT system was originally proposed by Kim et al.22 Due to having only one long guide rail as the transmitter, the coupling of long-track is relatively stable. However, most of the magnetic field of the long rail coil cannot be received by the receiver, resulting in severe magnetic leakage. Moreover, the long-track coil has high internal resistance, which causes severe losses.23–25 For the traditional unipolar segmented DWPT system, if the segmented transmitting coils are turned on one by one, the magnetic field generated by adjacent coils will cancel out, and the mutual inductance will drop dramatically when the EV reaches the position near the adjacent transmitting coils, which would affect the transfer power and the transmission efficiency.26–28 The Electric field Coupled-Wireless Power Transfer (EC-WPT) can avoid the problem of field cancellation between adjacent emitters to some extent. However, adjacent plates will introduce two new problems: (1) If adjacent plates are too close, the two transmitting plates will couple and affect system resonance. (2) If adjacent plates are placed too far apart, the resulting power drop will be significant.29,30 For existing segmented DWPT designs, Song et al. designed a multi-primary winding parallel topology for DWPT but did not analyze the receiving characteristics of the corresponding receiving coils.31 Some studies proposed a multi-phase wireless power supply system, which can effectively turn on the appropriate transmitting coil to supply power to the load.32–34 Still, its design was so cumbersome as to make the operation complicated.

To address the above-mentioned problem, this paper proposes a novel dual receiver topology for the segmented DWPT system. The topology designed can solve the power loss and fluctuation caused by magnetic field cancellation. In addition, the main contributions of the paper are as follows:

  1. This paper uses finite element simulation to analyze the magnetic field cancellation problem of adjacent coils in traditional segmented DWPT. Based on this, a design method of changing the direction of magnetic field and current is proposed.

  2. A dual receiver series topology (DRST) is designed to work in three working modes and six working states. The receivers can receive the optimal power in three stages by this topology. In addition, this paper explains the current flow direction under various working conditions.

  3. The experiments are carried out, and the results show that the proposed DRST is effective to improve the average output power from 2.007 to 5.657 W and significantly reduce the power fluctuation compared to the single receiver.

The rest of the paper is organized as follows: Sec. II analyzes the magnetic field characteristics at the near of coils under unipolar and bipolar power supply modes and gives the mutual inductance equivalent circuit diagram of the double receiving-coil. Section III describes the working principle of the proposed DRST and elaborates on its three working modes and six working states. Finally, the experimental results verify the theoretical analysis and show that the proposed system topology is effective and reliable in Sec. IV.

The typical segmented DWPT system for EVs is shown in Fig. 1, which mainly consists of two parts, called transmitter and receiver devices, respectively. The transmitter device comprises multiple-segmented guide rail coils and converts electric energy into magnetic field energy. The receiver device includes a receiving coil, rectifier unit, and battery pack, which could pick up the magnetic field energy and supply for EVs. The transmitting coils are orderly arranged under the road. When EVs pass the two adjacent transmitting coils, the relative position of the receiving and transmitting coils will go through three stages, as shown in Fig. 2.

FIG. 1.

Basic structure of electric vehicle DWPT system.

FIG. 1.

Basic structure of electric vehicle DWPT system.

Close modal
FIG. 2.

Schematic diagram of coupling coil position.

FIG. 2.

Schematic diagram of coupling coil position.

Close modal

In the traditional segmented DWPT system with unipolar power supply mode, the currents of the adjacent sides of two transmitting coils are opposite. Adjacent wires will generate opposite magnetic fields, which will weaken the magnetic field, as shown in Fig. 3. Bipolar power supply mode is an effective measure to reduce the magnetic field mutual cancellation by tuning the currents of the adjacent coils with a 180° phase difference. The currents and the magnetic field are shown in Fig. 4.

FIG. 3.

Current and magnetic field with unipolar power supply mode. (a) Current of adjacent coils. (b) Magnetic field of adjacent coils.

FIG. 3.

Current and magnetic field with unipolar power supply mode. (a) Current of adjacent coils. (b) Magnetic field of adjacent coils.

Close modal
FIG. 4.

Current and magnetic field with bipolar power supply mode. (a) Current of adjacent coils. (b) Magnetic field of adjacent coils.

FIG. 4.

Current and magnetic field with bipolar power supply mode. (a) Current of adjacent coils. (b) Magnetic field of adjacent coils.

Close modal

In Fig. 4(b), the magnetic field near two adjacent sides has been significantly enhanced. However, the current phase difference between the two transmitting coils is also 180°. Furthermore, to improve the performance of the segmented DWPT system, a dual receiver on the same plane is adopted to pick up the power, and its equivalent circuit is shown in Fig. 5.

FIG. 5.

Equivalent circuit diagram of dual receiver DWPT system.

FIG. 5.

Equivalent circuit diagram of dual receiver DWPT system.

Close modal

In Fig. 5, the SS resonant compensation topology transfers power. uin stands for the high-frequency power source. For the convenience of expression, Lp and Ls represent the two coils with the inductances of Lp and Ls, and the subscripts “P” and “S” stand for the transmitting and receiving coils, respectively. Cp1 and Cp2, Rp1, and Rp2, ip1, and ip2 stand for the inductances, capacitances, resistances, and currents of two adjacent transmitting coil circuits, while Cs1 and Cs2, Rs1, and Rs2, is1, and is2 represent the corresponding parameters of two receiving coil circuits. Mi (i = 1,2,3,4) stands for the mutual inductance of Lp and Ls, as in Fig. 5.

To solve the problem of the 180° phase difference between the current of the two receiving coils mentioned in Sec. II, a DRST for the bipolar segmented DWPT system is proposed, and its circuit topology is shown in Fig. 6.

FIG. 6.

DRST of bipolar segmented DWPT system.

FIG. 6.

DRST of bipolar segmented DWPT system.

Close modal

In Fig. 6, Si (i = 1,2,3,4,5,6) and Di (i = 1,2,3,4) represent fully controlled components and diodes, respectively. When the S5 and S6 are turned on simultaneously, the currents in the adjacent sides of two transmitting coils are in-phase, and the enhanced magnetic field can be achieved, as shown in Fig. 4(b).

According to the three stages mentioned in Fig. 2, when EV is driving from transmitting coil 1 to coil 2, the waveforms of main parameters and the status of S1S6 are shown in Fig. 7. In addition, the DWPT system has three working modes, including six working states, as shown in Fig. 8, where the red dotted line with the arrow indicates the actual flow direction of the current.

FIG. 7.

Main working waveforms.

FIG. 7.

Main working waveforms.

Close modal
FIG. 8.

Equivalent circuit of working mode in Mode 1. (a) Positive period. (b) Negative period.

FIG. 8.

Equivalent circuit of working mode in Mode 1. (a) Positive period. (b) Negative period.

Close modal

Mode 1: t0 ≤ t <t1. In the first stage, the receiving coils LS1 and LS2 are above the transmitting coil 1. S1, S4, and S5 are turned on, while S2, S3, and S6 are turned off. uin supplies power to LP1, and the working states during the positive and negative half cycle of uin are shown in Figs. 8(a) and 8(b), respectively.

Mode 2: t1 ≤ t <t2. In the second stage, LS1 is above the transmitting coil 1 and LS2 is above the transmitting coil 2. S2, S3, S5, and S6 are turned on, while S1 and S4 are turned off. uin supplies power to LP1 and LP2, and the working states during the positive and negative half cycles of uin are shown in Figs. 9(a) and 9(b), respectively.

FIG. 9.

Equivalent circuit of working mode in Mode 2. (a) Positive period. (b) Negative period.

FIG. 9.

Equivalent circuit of working mode in Mode 2. (a) Positive period. (b) Negative period.

Close modal

Mode 3: t2 ≤ t <t3. In the third stage, LS1 and LS2 are above the transmitting coil 2. S1, S4, and S6 are turned on, while S2, S3, and S5 are turned off. uin supplies power to LP2, and the working states during the positive and negative half cycle of uin are shown in Figs. 10(a) and 10(b), respectively.

FIG. 10.

Equivalent circuit of working mode in Mode 3. (a) Positive period. (b) Negative period.

FIG. 10.

Equivalent circuit of working mode in Mode 3. (a) Positive period. (b) Negative period.

Close modal

According to the above-mentioned analysis, the status of S1S6 in the different stages can be seen in Table I. Where 1 and 0 stand for on and off of the switch tubes, respectively.

TABLE I.

Status of S1S6 in different modes.

Working modeS1S2S3S4S5S6
Mode 1 
Mode 2 
Mode 3 
Working modeS1S2S3S4S5S6
Mode 1 
Mode 2 
Mode 3 

Figure 11 shows the experimental device for the DWPT system, and the critical system parameters are given in Table II. In Fig. 11, the power amplifier AG1019 is used to provide high-frequency power. As the control unit, DSP is adopted to generate PWM wave to drive S1S6. Figure 12 shows the single receiver and dual receiver used in the experiment. Figure 13 shows the specific dimensions of the coupling mechanism.

FIG. 11.

Prototype of experimental device.

FIG. 11.

Prototype of experimental device.

Close modal
TABLE II.

Main parameters of the system.

ParametersValue
AC output power/W 10 
Frequency/kHz 85 
Self-inductance of transmitting coil/μ44.1 
Self-induction of receiving coil/μ15.3 
Resonant capacitor at transmitter/nF 79.6 
Resonant capacitor at receiver/nF 229 
Turn ratio 
ParametersValue
AC output power/W 10 
Frequency/kHz 85 
Self-inductance of transmitting coil/μ44.1 
Self-induction of receiving coil/μ15.3 
Resonant capacitor at transmitter/nF 79.6 
Resonant capacitor at receiver/nF 229 
Turn ratio 
FIG. 12.

Physical display of receiving coil.

FIG. 12.

Physical display of receiving coil.

Close modal
FIG. 13.

The specific dimensions of coupling mechanism.

FIG. 13.

The specific dimensions of coupling mechanism.

Close modal

For the convenience of description, a point P (0, 2, 8) on the receiving coil is taken as the reference point, as shown in Fig. 13. So that the x-coordinate component of P (Px) can be used to represent the real-time position of EV. For the double-receiving-coil segmented DWPT system, when 0 ≤ Px < 24 and 34 ≤ Px, the two receiving coils are powered by one transmitting coil, corresponding to Stage 1 and Stage 3 in Fig. 2. When 24 ≤ Px < 34, EV is powered by two transmitting coils, corresponding to Stage 2 Fig. 2. For different power supply modes, the output voltage of the system varies greatly only in stage 2. Figures 14 and 15 show the output voltage waveform when Px = 24 and Px = 29 for unipolar and bipolar power supply modes.

FIG. 14.

Output voltage waveform in unipolar power supply mode. (a) Px = 24. (b) Px = 29.

FIG. 14.

Output voltage waveform in unipolar power supply mode. (a) Px = 24. (b) Px = 29.

Close modal
FIG. 15.

Output voltage waveform in bipolarity power supply mode. (a) Px = 24. (b) Px = 29.

FIG. 15.

Output voltage waveform in bipolarity power supply mode. (a) Px = 24. (b) Px = 29.

Close modal

Furthermore, the comparison experiment on receiving power between the single-receiving-coil system and the double-receiving-coil system is carried out. In addition, to simplify the description, the double-receiving-coil system and the single-receiving-coil system are labeled as DCS and SCS. In the experiment, the output power is recorded when Px moves from 24 to 35 cm in steps of 1 cm, as shown in Fig. 13.

In Fig. 16, it is obvious that the output power of DCS is higher than that of SCS, and the maximum output power of 5.73 W at Px = 29 is 5.43 W higher than that of SCS. When 24 < Px < 34, the average output power of DCS is about 5.657 W, and that of CSC is 2.007 W. Meanwhile, the power fluctuation of DCS with the maximum of 6.31% is far less than that of CSC with the maximum of 85.05%. The experimental results fully prove that the proposed DRST is effective to improve the output power and reduce the power fluctuation when EVs passing the adjacent two transmitting coils.

FIG. 16.

Coil receiving power.

FIG. 16.

Coil receiving power.

Close modal

This paper mainly investigates the optimal design of a segmented DWPT system for EVs. In the traditional unipolar power supply mode, the DWPT system has a large fluctuation of receiving power when EVs move over two adjacent transmitting coils. Consequently, this paper selects the bipolar power supply mode achieved by two fully controlled components (S5 and S6). By turning the current with the same phase in the two adjacent lines of two transmitting coils, the magnetic field at the junction of two adjacent coils is obviously enhanced, and it is conducive to improve the stability of transmission power. Furthermore, a DRST is proposed to pick up the power. By controlling S1, S2, S3, and S4, three working modes with six working states could be achieved to obtain a small fluctuation of receiving power. The experimental results show that DRST is effective to output the power with a higher average value and a minor fluctuation.

This work was supported by the Postgraduate Research & Practice Innovation Program of Jiangsu Province under Grant No. KYCX23−3091.

The authors have no conflicts to disclose.

Yaqiang Zou: Conceptualization (lead); Supervision (lead); Validation (lead). Tian Xu: Formal analysis (lead); Investigation (lead); Methodology (lead); Software (lead); Validation (equal); Writing – original draft (lead); Writing – review & editing (lead). Zhong Li: Funding acquisition (equal); Methodology (equal); Validation (equal); Visualization (equal). Hao Qiang: Conceptualization (equal); Data curation (lead); Project administration (lead); Resources (lead).

The data that support the findings of this study are available from the corresponding author upon reasonable request.

1.
W.
Dai
,
Z.
Geng
,
B.
Ouyang
, and
Y.
Shen
, “
Design optimization of electromagnetic shielding and charging efficiency for electric vehicle wireless charging system
,”
AIP Adv.
13
,
115128
(
2023
).
2.
L.
Chen
,
F.
Wu
,
T.
Ben
, and
C.
Zhang
, “
Analysis and design of constant current and constant voltage outputs of integrated coil wireless EV charging system
,”
AIP Adv.
13
,
025306
(
2023
).
3.
N.
Ha-Van
,
N.
Dang-Duy
,
H.
Kim
, and
C.
Seo
, “
High-efficiency wireless power transfer by optimal load and metamaterial slab
,”
IEICE Electron. Express
14
,
20170320
(
2017
).
4.
C.
Xia
,
W.
Wang
,
G.
Chen
,
X.
Wu
,
S.
Zhou
, and
Y.
Sun
, “
Robust control for the relay ICPT system under external disturbance and parametric uncertainty
,”
IEEE Trans. Control Syst. Technol.
25
,
2168
2175
(
2017
).
5.
S.
Hekal
,
A. B.
Abdel-Rahman
,
A.
Allam
,
H.
Jia
et al, “
Asymmetric wireless power transfer systems using coupled DGS resonators
,”
IEICE Electron. Express
13
,
20160591
(
2016
).
6.
Y.
Liu
,
J.
Xiao
,
X.
Zhao
,
J.
Wu
,
Y.
Du
,
Y.
Zhao
,
H.
Wang
, and
Z.
Wang
, “
Development and application review on wireless power transmission technology
,”
Adv. Technol. Electr. Eng. Energy
42
,
48
67
(
2023
).
7.
A. F. A.
Aziz
et al, “
Review of inductively coupled power transfer for electric vehicle charging
,”
IET Power Electron.
12
,
3611
3623
(
2019
).
8.
Y.
Jiao
,
R.
Li
, and
G.
Song
, “
Research and optimization of transmission characteristics of magnetically coupled resonant wireless transmission system
,”
Power Syst. Prot. Control
48
,
112
120
(
2020
).
9.
L.
Wu
and
B.
Zhang
, “
Overview of static wireless charging technology for electric vehicles Part 1
,”
Trans. China Electrotech. Soc.
35
,
1153
1165
(
2020
).
10.
L.
Wu
and
B.
Zhang
, “
Overview of static wireless charging technology for electric vehicles: Part Ⅱ
,”
Trans. China Electrotech. Soc.
35
,
1662
1678
(
2020
).
11.
Z.
Zhang
and
B.
Zhang
, “
Development and key technologies of dynamic wireless power transfer system for mobile load
,”
Jiangsu Electr. Eng.
39
,
21
30
(
2020
).
12.
T.
Ohira
, “
Maximum available efficiency formulation based on a black-box model of linear two-port power transfer systems
,”
IEICE Electron. Express
11
,
20140448
(
2014
).
13.
C.
Xia
,
G.
Chen
,
S.
Ren
,
K.
Lei
,
Y.
Zhang
, and
Y.
Sun
, “
Wireless power transfer system using composite resonant network for constant-current power supply of load
,”
Automation Electric Power Syst.
41
,
46
52
(
2017
).
14.
D.
Patil
,
M. K.
Mcdonough
,
J. M.
Miller
,
B.
Fahimi
, and
P. T.
Balsara
, “
Wireless power transfer for vehicular applications: Overview and challenges
,”
IEEE Trans. Transp. Electrification
4
,
3
37
(
2018
).
15.
F.
Lin
,
G. A.
Covic
, and
J. T.
Boys
, “
A comparison of multi-coil pads in IPT systems for EV charging
,” in
IEEE Energy Conversion Congress and Exposition
(
IEEE
,
2018
), pp.
105
112
.
16.
Y.
Li
,
J.
Zhao
,
Q.
Yang
,
L.
Liu
,
J.
Ma
, and
X.
Zhang
, “
A novel coil with high misalignment tolerance for wireless power transfer
,”
IEEE Trans. Magn.
55
,
1
4
(
2019
).
17.
J.
Sathik Mohamed Ali
,
D.
Almakhles
et al, “
A comprehensive review of the on-road wireless charging system for E-mobility applications
,”
Front. Energy Res.
10
,
926270
(
2022
).
18.
C. C.
Mi
,
G.
Buja
,
S. Y.
Choi
, and
C. T.
Rim
, “
Modern advances in wireless power transfer systems for roadway powered electric vehicles
,”
IEEE Trans. Ind. Electron.
63
,
6533
6545
(
2016
).
19.
K.
Zhuo
,
B.
Luo
,
Y.
Zhang
,
Y.
Zuo
, and
S.
Liu
, “
A coaxial dual-receiver wireless power transfer system with bipolar coils to eliminate cross-coupling and achieve a controllable power distribution
,”
IEICE Electron. Express
17
,
20190693
(
2020
).
20.
Y.
Yang
,
J.
Cui
, and
X.
Cui
, “
Coupling coefficient of magnetic structure coil for wireless charging system of electric vehicles
,”
Smart Power
48
,
56
62
(
2020
).
21.
J.
Zhao
,
Z.
Sun
,
M.
Pecht
, and
S.
Zhou
, “
Analysis and experiments on transmission characteristics of LCCL mobile wireless power transfer system
,”
IEICE Electron. Express
15
,
20180964
(
2018
).
22.
J.
Kim
,
J.
Kim
,
S.
Kong
,
H.
Kim
,
I. S.
Suh
,
N. P.
Suh
,
D. H.
Cho
,
J.
Kim
, and
S.
Ahn
, “
Coil design and shielding methods for a magnetic resonant wireless power transfer system
,”
Proc. IEEE
101
,
1332
1342
(
2013
).
23.
C.
Jiang
,
Y.
Sun
,
Z.
Wang
,
Y.
Su
, and
L.
Zhang
, “
Switching mode analysis of wireless supplying rail for electric vehicles
,”
Automation Electric Power Syst.
41
,
188
193
(
2017
).
24.
Y.
Cheng
,
H.
Hu
,
F.
Ye
,
D.
Shen
, and
S.
Yang
, “
Modeling and simulation of magnetically coupled resonant wireless power transmission system
,”
Electric Eng.
16
,
135
136
(
2018
).
25.
D.
Wu
,
T.
He
,
X.
Wang
, and
Q.
Sun
, “
Analytical modeling and analysis of mutual inductance coupling of rectangular spiral coils in inductive power transfer
,”
Electric Eng.
33
,
680
688
(
2018
).
26.
K.
Lee
,
Z.
Pantic
, and
S. M.
Lukic
, “
Reflexive field containment in dynamic inductive power transfer systems
,”
IEEE Trans. Power Electron.
29
,
4592
4602
(
2014
).
27.
M.
Miller
,
P. T.
Jones
,
J. M.
Li
,
O. C.
Onar
, and
L.
Zhang
, “
ORNL experience and challenges facing dynamic wireless power charging of EV’s
,”
IEEE Circuits Syst. Mag.
15
,
40
53
(
2015
).
28.
S.
Liu
,
Y.
Li
,
Y.
Wu
,
L.
Zhou
,
X.
Zhao
,
R.
Mai
, and
Z.
He
, “
An output power fluctuation suppression method of DWPT systems based on dual-receiver coils and voltage doubler rectifier
,”
IEEE Trans. Ind. Electron.
70
,
10167
10179
(
2023
).
29.
X. D.
Qing
,
Z. H.
Wang
,
Y. G.
Su
,
Y. M.
Zhao
, and
X. Y.
Wu
, “
Parameter design method with constant output voltage characteristic for bilateral LC-compensated CPT system
,”
IEEE J. Emerging Selected Topics Power Electron.
8
,
2707
2715
(
2020
).
30.
D. Y.
Tang
,
W.
Zhou
,
L.
Huang
,
R. K.
Mai
, and
Z. Y.
He
, “
Dynamic electric-filed coupled wireless power transfer system with constant voltage output characteristics
,”
Trans. China Electrotech. Soc.
38
,
5385
5397
(
2023
).[
31.
K.
Song
,
C.
Zhu
,
Y.
Li
,
X.
Guo
,
J.
Jiang
, and
J.
Zhang
, “
Wireless power transfer technology for electric vehicle dynamic charging using multi-parallel primary coils
,”
IEEE Trans. Ind. Electron.
17
,
4445
4453
(
2015
).
32.
Y.
Zhu
and
P.
Duan
, “
Design of three-phase wireless power supply platform based on primary coil switching
,”
Electr. Drive.
48
,
93
96
(
2018
).
33.
Z.
Wang
,
S.
Cui
,
S.
Han
,
K.
Song
,
C.
Zhu
,
M. I.
Matveevich
, and
O. S.
Yurievich
, “
A novel magnetic coupling mechanism for dynamic wireless charging system for electric vehicles
,”
IEEE Trans. Veh. Technol.
67
,
124
133
(
2018
).
34.
S.
Cui
,
Z.
Wang
,
S.
Han
,
C.
Zhu
, and
C. C.
Chan
, “
Analysis and design of multiphase receiver with reduction of output fluctuation for EV dynamic wireless charging system
,”
IEEE Trans. Power Electron.
34
,
4112
4124
(
2019
).