Enhancement algorithm for reverse loop technique on planar reverse loop antenna

TELKOMNIKA, Vol.17, No.6, December 2019, pp.2713~2721
ISSN: 1693-6930, accredited First Grade by Kemenristekdikti, Decree No: 21/E/KPT/2018
DOI: 10.12928/TELKOMNIKA.v17i6.12087 ◼ 2713
Received December 18, 2018; Revised January 21, 2019; Accepted March 12, 2019
Enhancement algorithm for reverse loop technique
on planar reverse loop antenna
Mohamad Harris Misran*1
, Sharul Kamal Abdul Rahim2
, Maizatul Alice Meor Said3
,
Mohd Azlishah Othman4
1,2
Wireless Communication Centre (WCC), Faculty of Electrical Engineering,
Universiti Teknologi Malaysia, 81310 UTM Skudai Johor, Malaysia
1,3,4
Fakulti Kejuruteraan Elektrik dan Kejuruteraan Komputer, Universiti Teknikal Malaysia Melaka,
Hang Tuah Jaya, 76100 Durian Tunggal, Melaka, Malaysia
*Corresponding author, e-mail: harris@utem.edu.my1
, sharulkamal@fke.utm.my2
, maizatul@utem.edu.my3
Abstract
Finding a trade-off balance between wireless transfer efficiency (WTE) and distance is a key
issue in wireless energy transfer (WET). This paper presents a method of reducing the radical alteration in
WTE versus distance, by using a reverse loop technique on planar reverse loop antenna (PRLA).
The design focuses on 13.56 MHz Near Field Communication (NFC). The first stage uses mathematical
modelling, based on an analytical approach, to determine the size of the reverse loop using Matlab.
The proposed model predicts the size of the reverse loop to stabilize the WTE at a closer distance.
Next, full-wave electromagnetic simulations are applied, using the computer simulation technology (CST)
MICROWAVE STUDIO®, to determine the WTE effect with distance changes with mismatch condition.
Planar loop antennas (PLAs) are fabricated on glass-reinforced epoxy laminated sheets (FR4).
A validation of the simulation result in a real test scenario, using these PLAs and PRLA, confirms
a stability enhancement in WTE at closer distance using the reverse loop technique, compared to
conventional designs.
Keywords: near field communication (NFC), planar loop antenna (PLA), planar reverse loop antenna
(PRLA), wireless energy transfer (WET), wireless transfer efficiency (WTE)
Copyright © 2019 Universitas Ahmad Dahlan. All rights reserved.
1. Introduction
With the evolution of high-end technology, portable devices have become widely used.
Usually, these devices require power from rechargeable batteries to enable mobility.
The batteries only support these devices for limited durations, after which they require
recharging using wired power delivery mechanisms. Consumers usually need to wait for
the completion of the charging process before the devices can be used wirelessly. In its mooted
counteraction of this problem, wireless energy transfer (WET) has garnered significant research
interest. However, even with the latest technologies, there are obstacles to be overcome before
the full commercialization of WET can be implemented [1].
Inductive coupling of WET has attracted a great deal of attention, due to its simplicity
and safety. It is already used in technologies such as RFID and NFC [2]; NFC-enabled
smartphones are even now employing inductive coupling for data transfer in contactless
transactions at 13.56 MHz [3]. Theoretically, NFC can also be used to transfer energy between
devices using inductive coupling at a resonant frequency as shown in Figure 1.
There have been improvements in the performance of inductive coupling and strong
magnetic coupling WET schemes [4-6]. However, as demonstrated in many studies,
the wireless transfer efficiency (WTE) is reduced greatly with altered distances [6-11]. In order
to increase the insensitivity to the distance of the transmitting and receiving antennas, a handful
of techniques has been developed, such as using a loaded capacitor or applying more than two
coils in a system [6, 11, 12].
Coupling coefficient is directly proportional to mutual inductance; M. M value strongly
depends on the distance between the antennas. In short, closer distance will generate higher M
than farther distance. Both antennas are perfectly matched at operating distance for optimum
resonant effect. However, the WTE will radically drop when the transmitter and receiver become
closer. This phenomenon happens because of frequency splitting condition caused by coupling

◼ ISSN: 1693-6930
TELKOMNIKA Vol. 17, No. 6, December 2019: 2713-2721
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coefficient inflation [13]. In order to maintain a constant transfer within the over-coupled region,
some researchers proposed dynamic impedance matching arrangements to either track
the resonance frequency [14-17] or adaptively impedance match to maintain a stated
frequency [18]. These impedance matching arrangements were implemented using either
lumped reactance [14, 19, 20] or tuning algorithms in controllers [21–23]. An alternative
arrangement, however, is to control the range-profile of the mutual inductance within
the over-coupled region.
Besides, optimal load resistance value existed, with which the coupling efficiency can
be maximised [24]. To achieve this, the resonant capacitor at the load side was replaced by
a more complex impedance matching network in [16, 25]. This matching network tuned
the receiver coil and transformed the load resistance value into one that is optimum.
The matching network was also introduced into the source side in [25-27]. In [25], the matching
network design was integrated into WET system and displayed a good performance. Matching
network can be designed to maximise the output power for transfer efficiency.
This paper focuses on 13.56 MHz WET, in order to take advantage of the fact that
almost all mid- and high-end smartphones are already NFC-enabled. The reverse loop
technique is used to stabilize the WTE when the distance between both antennas is shorter
than optimum operating distance, without any further system adjustment. The M produced is
controlled by introducing a reverse loop into a planar loop antenna (PLA) to minimize the radical
changes in WTE with distance variance. This method yields the development of the planar
reverse loop antenna (PRLA).
Figure 1. NFC transmission system [2]
2. Antenna Design
The inductive coupling link consists of two antennas with separate external matching
circuits. Each matching circuit uses parallel and serial capacitors to tune the antennas for
maximum WTE at the operating frequency. The antennas are designed to be square in order to
fit into mobile phones, thereby optimizing the available area. The PLAs are single square loops,
as shown in Figures 2 (a) and (b). Their side-lengths are set at 60 mm and 40 mm for
the transmitter and receiver, respectively, for an operating distance d of 50 mm.
(a) (b)
Figure 2. (a) Transmitter PLA and (b) receiver PLA

TELKOMNIKA ISSN: 1693-6930 ◼
Enhancement algorithm for reverse loop technique on planar... (Mohamad Harris Misran)
2715
A coupled pair of one-turn square loops in a wireless energy transfer link can be
illustrated in a simplified equivalent circuit, as shown in Figure 3 [28]. The inductance of each
PLA can be calculated using (1), also stated in [29]:
𝐿 𝑇𝑋,𝑅𝑋 = 0.635𝜇𝑙 𝑥 [ln (
2.07
𝑙 𝑦
) + 0.18𝑙 𝑦 + 0.13𝑙 𝑦
2
] (1)
where µ is the conductor (copper) permeability, and
𝑙 𝑦 =
𝑙 𝑎 − 𝑙 𝑏
𝑙 𝑎 + 𝑙 𝑏
(2)
Figure 3. Equivalent circuit for antennas [28]
The average side length of the PLA is given by
𝑙 𝑥 = 0.5(𝑙 𝑎 + 𝑙 𝑏) (3)
with la and lb denoting the largest and smallest side lengths, respectively. Taking the skin effect
into consideration, the resistance of the PLA, R at f = 13.56 MHz, can be computed as:
𝑅 =
𝜌𝑙
4𝐴 𝑟 𝛿
(
𝑡
1 − 𝑒−
𝑡
𝛿
) (4)
𝛿 =
√ 𝜌
√𝜋𝑓𝜇 𝑜
(5)
where ρ is the resistivity of copper (1.7 × 10-8 Wm), A is the cross-sectional area of the loop and
l is the total length of the PLA. t is the thickness of the conductor. Ar and l can be determined
by using
𝐴 𝑟 = 𝑤 × 𝑡 (6)
𝑙 = 4𝑙 𝑠 − 𝑔 + 2𝑝 (7)
where w, ls, g and p are the width, side length, gap length and port line length of the conductor
respectively.
The WTE of the established link is calculated as [11]:

◼ ISSN: 1693-6930
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𝜂 =
𝐸
(1 + √1 + 𝐸)
2 (8)
𝐸 = 𝑘2
𝑄 𝑇𝑋 𝑄 𝑅𝑋 (9)
where QTX is the quality factor of the transmitting antenna and QRX is the quality factor of
the receiving antenna; both are defined as
𝑄 𝑅𝑋 =
2𝜋𝑓 𝐿 𝑅𝑋
𝑅 𝑅𝑋
(10)
𝑄 𝑇𝑋 =
2𝜋𝑓 𝐿 𝑇𝑋
𝑅 𝑇𝑋
(11)
k is the coupling coefficient between both antennas and can be determined using:
𝑘 =
𝑀
√𝐿 𝑇𝑋 𝐿 𝑅𝑋
(12)
the mutual inductance between both antennas, M, can be obtained using [29]:
𝑀 =
𝜇 𝑜 𝜋𝑋2
𝑌2
2(𝑋2 + 𝑌2 + 𝑑2)
3
2
(1 +
15
32
𝛾2
+
315
1024
𝛾4
) (
4
𝜋
)
1+
𝑟 𝑚𝑖𝑛
𝑟 𝑚𝑎𝑥
(13)
𝛾 =
2𝑋2
𝑌2
𝑋2 + 𝑌2 + 𝑑2
(14)
rmin and rmax are the corresponding smaller and larger side lengths of the square antennas,
respectively. Here, X is the half side length of the transmitter antenna and Y is the half side
length of the receiver antenna. d denotes the distance between the transmitter and receiver of
the PLA system.
In terms of mutual inductance between transmitter and receiver PLA, M is inversely
proportional to the distance, as shown in Figure 4. In theory, high values of M will produce high
WTE; however, this is only true if both PLAs are perfectly matched. In fixed matching circuits for
inductive WET, the highest WTE will be obtained at a matching operating distance, which in this
case is 50 mm. Deviation from this operating distance will greatly reduce the WTE of
the system. Further distance from the operating point will reduce M value, also causing
WTE reduction.
Figure 4. Mutual inductance, M versus distance between PLAs

2717
Meanwhile, a closer distance from the operating point will increase the M between
PLAs and create the over-coupling condition, as characterized by frequency splitting [13].
The over-coupling phenomena will decrease the WTE greatly, even when M is high at that point.
In theory, the WTE can be stabilized by maintaining a constant M, irrespective of the distance.
This can be achieved by introducing a reverse loop in the transmitter antenna, producing
a PRLA, as shown in Figure 5 (a). The receiver antenna will be using initial single square loop
antenna as presented in Figure 5 (b). This reverse loop will generate an opposite M, as shown
in Figure 6. The net result will be a reduction in the alteration of M as the coupled antennas are
brought closer together.
(a) (b)
Figure 5. (a) Transmitter PRLA and (b) receiver PRLA
Figure 6. Mutual inductance, M versus distance between PRLAs
The first stage in obtaining the side length of the reverse loop requires the choice of two
points of distance. The first point is an optimum operating distance, while the second is a closer
distance than the former. Based on (13), maintaining the value of M at these two points will
result in a stable WTE. The size of the reverse loop to maintain a constant M at both points can
be obtained by solving (15). Matlab is used to solve the proposed equation.
M1,2 are calculated using:
𝑀1,2 =
𝜇 𝑜 𝜋𝐴1,2
2
𝐵1,2
2
2(𝐴1,2
2
+ 𝐵1,2
2
+ 𝑑1,2
2
)
3
2
(1 +
15
32
+
315
1024
𝛾1,2
4
) (
4
𝜋
)
1+
𝑟 𝑚𝑖𝑛
𝑟 𝑚𝑎𝑥
(15)

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𝛾1,2 =
2𝐴1,2
2
𝐵1,2
2
𝐴1,2
2
+ 𝐵1,2
2
+ 𝑑1,2
2 (16)
where A1,2, B1,2 and d1,2 are the half-side length of the transmitter, the half-side length of
the receiver and the distance between PRLAs at different points, respectively. If A1, B1, d1, A2
and d2 are known, the optimum size of the reverse loop side length, B2 can be calculated.
The calculated value of B2 is an optimum value of reverse loop side length that produces
highest and most stable WTE at a distance between antennas closer than matching distance.
To tune the system for optimum performance at f = 13.56MHz, both PLAs and PRLAs
were matched to 50Ω impedances using external capacitor networks, as shown in Figure 6.
Full-wave simulations were carried out in CST to ascertain the effect on WTE with distance.
The antennas were then fabricated to validate the simulated results.
3. Results and Analysis
Simulated antennas are matched using Mini Match matching technique in CST.
Two capacitors are used at each antenna to eliminate the reactance component and get
a resonance at 13.56 MHz, as shown in Figure 3. This matching stage is very important to
ensure the maximum possible output power will be delivered. The fabricated transmitter’s PLA
and PRLA are shown in Figure 7, with the matching circuit shown in the inset. The capacitance
values are shown in Table 1, while Figure 8 shows the lab measurement setup.
Figure 7. Fabricated PLA and PRLA
Figure 8. Measurement setup in lab using vector network analyser

2719
Table 1. Capacitor values for matching circuit
PLA PRLA
Capacitor
Value (pF)
Capacitor
Value (pF)
CST Actual CST Actual
C1 74.5 75 C1 52.58 52
C2 650.3 651 C2 541 545
C3 1085.8 1090 C3 1117 1120
C4 104.9 105 C4 69 68
The M of the system using PRLA is shown in Figure 9. Even though the PRLA has
a lower M compared to the PLA, the M for the PRLA loop is much more stable over distance.
This ensures the reduction of the over-coupling effect at closer distances; accordingly,
frequency-splitting phenomena can be minimized. The WTE alteration, with shorter coupling
distances than the matching distance, is thus reduced.
In Figure 9, the total M produced by the PLRA is shown. Total M is decreased because
the reverse loop in PRLA introduced negative M. The maximum M obtained indicates that
the optimum WTE can be achieved at perfectly matched conditions. Here, the maximum WTE
can be reached at a matching distance equal to 25 mm. Figure 10 shows the WTE alteration of
both PLAs and PRLAs antennas for various distances. Even though the WTE for PRLA is lower
than PLA at matching distance, WTE for PRLA has better stability than PLA. Frequency splitting
phenomena has been reduced greatly by introducing reverse loop into PRLA. As a result, WTE
for PRLA at closer distance from matching distance is higher than PLA.
Figure 9. Total mutual inductance, M versus distance between PRLAs
Figure 10. Transfer efficiency with distance alteration

◼ ISSN: 1693-6930
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Figure 11 compares the WTE performance of the PRLA and conventional PLA as
the operating distance is varied. Differences in capacitor values within a 5% tolerance contribute
to differences between the simulation and measurement results. Non-existent values for
required capacitors in the market also led to this dissimilarity.
However, there is acceptable agreement between the measured and simulated profiles
of WTE. Overall, the PLRA is shown to stabilise the WTE at closer distances. An improvement
of 150% for S21 at a distance of 10mm is recorded. In addition, the PLRA is able to maintain
S21 over 0.5 at a greater distance than the conventional PLA. PLA has S21 larger than 0.5 from
25 mm to 75 mm while PRLA manage to maintain S21 above 0.5 from 0 up to 60 mm, which
produce range improvement of 20%.
Figure 11. Transfer efficiency with varied distances
4. Conclusion
WTE can be stabilised over shorter coupling distances by using the reverse loop
technique at a closer distance. By controlling the increase in mutual inductance between a pair
of coupled antennas at shorter distances, the alteration of WTE is reduced. This leads to
an improvement in the stability of WET.
Acknowledgements
The authors would like to thank Universiti Teknikal Malaysia Melaka (UTeM) for
supporting this research work under the grant PJP/2017/FKEKK/HI13/S01541. This research
also was supported by Universiti Teknologi Malaysia.
References
[1] Shoki H. Issues and initiatives for practical deployment of wireless power transfer technologies in
Japan. Proceedings of the IEEE. 2013; 101(6): 1312–1320.
[2] http: //www.mouser.com/pdfdocs/... ...STMicroelectronicsIntroductiontoNFC.pdf. Accessed 21st
June
2016 at 4:00 pm.
[3] Strommer E, Jurvansuu M, Tuikka T, Ylisaukko-Oja A, Rapakko H, Vesterinen J. NFC-Enabled
Wireless Charging. 2012 4th
International Workshop on Near Field Communication (NFC).
2012: 36–41.
[4] Jolani F, Yu Y, Chen Z. A Novel Planar Wireless Power Transfer System with Strong Coupled
Magnetic Resonances. 2014 IEEE International Wireless Symposium (IWS). 2014: 1-4.
[5] Mori K, Lim H, Iguchi S, Ishida K, Takamiya M, Sakurai T. Positioning-free resonant wireless power
transmission sheet with staggered repeater coil array (SRCA). IEEE Antennas and Wireless
Propagation Letter. 2013; 11: 1710-1713.

2721
[6] Lee WS, Oh KS, Yu JW. Distance-insensitive wireless power transfer and near-field communication
using a current-controlled loop with a loaded capacitance. IEEE Transactions on Antennas and
Propagation. 2014; 62(2): 936-940.
[7] Mai R, Zhang Y, Dai R et al. A three-coil inductively power transfer system with constant voltage
output. Energies Journal. 2018; 11(3): 637-649.
[8] Ricketts DS, Chabalko MJ, Hillenius A. Optimization of Wireless Power Transfer for Mobile Receivers
Using Automatic Digital Capacitance Tuning. 2013 European Microwave Conference (EuMC). 2013;
1: 515-518.
[9] Kim Y, Lim S. High efficient misaligned wireless power transfer using magnetic resonant coupling and
additional capacitor. Asia-Pacific Microwave Conference Proceedings, APMC. 2012: 1049-1051.
[10] Ahn D, Hong S. Wireless Power Transfer Resonance Coupling Amplification by Load-Modulation
Switching Controller. IEEE Transactions on Industrial Electronics. 2014; 62(2): 898-909.
[11] Lee WS, Son WI, Oh KS, Yu JW. Contactless energy transfer systems using antiparallel resonant
loops. IEEE Transactions on Industrial Electronics. 2011; 60(1): 350-359.
[12] Zhong WX, Zhang C, Liu X, Hui SR. A Methodology for Making a 3-Coil Wireless Power Transfer
System More Energy Efficient Than a 2-Coil Counterpart for Extended Transmission Distance. IEEE
Transactions on Power Electronics. 2014; 30(2): 933-942.
[13] Imura T, Hori Y. Maximizing Air Gap and Efficiency of Magnetic Resonant Coupling for Wireless
Power Transfer Using Equivalent Circuit and Neumann Formula. IEEE Transactions on Industrial
Electronics. 2011; 58(10): 4746-4752.
[14] Beh TC, Kato M, Imura T, Oh S, Hori Y. Automated impedance matching system for robust wireless
power transfer via magnetic resonance coupling. IEEE Transactions on Industrial Electronics. 2012;
60(9): 3689–3698.
[15] Park J, Tak Y, Kim Y, Kim Y, Nam S. Investigation of adaptive matching methods for near-field
wireless power transfer. IEEE Transactions on Antennas and Propagation. 2011; 59(5): 1769–1773.
[16] Sample AP, Waters BH, Wisdom ST, Smith JR. Enabling seamless wireless power delivery in
dynamic environments. Proc. IEEE. 2013; 101(6): 1343–1358.
[17] Sample AP, Meyer DT, Smith JR. Analysis, experimental results, and range adaptation of
magnetically coupled resonators for wireless power transfer. IEEE Transactions on Industrial
Electronics. 2010; 58(2): 544–554.
[18] Jang BJ, Lee S, Yoon H. Hf-Band Wireless Power Transfer System: Concept, Issues, and Design.
Prog. Electromagn. Ress. 2012; 124: 211–231.
[19] Trigui A, Hached S, Mounaim F, Ammari AC, Sawan M. Inductive Power Transfer System with
Self-Calibrated Primary Resonant Frequency. IEEE Trans. Power Electron. 2015; 30(11):
6078–6087.
[20] Zhao C, Wang Z, Du J, Wu J, Zong S, He X. Active resonance wireless power transfer system using
phase shift control strategy. Appl. Power Electron. Conf. Expo. (APEC). 2014 Twenty-Ninth Annu,
IEEE. 2014: 1336–1341.
[21] Hu W, Zhou H, Deng Q, Gao X. Optimization algorithm and practical implementation for 2-coil
wireless power transfer systems. 2014 Am. Control Conf. 2014: 4330–4335.
[22] Roland M, Witschnig H, Merlin E, Saminger C. Automatic impedance matching for 13.56 MHz NFC
antennas. Proc. 6th
Int. Symp. Commun. Syst. Networks Digit. Signal Process-CSNDSP 08. 2008:
288–291.
[23] Witschnig H, Roland M, Gossar M, Enzinger H. Parameter characterisation and automatic impedance
matching of 13.56 MHz NFC antennas. Elektrotechnik und Informationstechnik. 2009; 126(11):
415–422.
[24] Yilmaz M, Krein PT. Review of battery charger topologies, charging power levels, and infrastructure
for plug-in electric and hybrid vehicles. IEEE Trans. Power Electron. 2013; 28(5): 2151–2169.
[25] Covic GA, Boys JT. Inductive Power Transfer. Proc. IEEE. 2013; 101(6): 1276–1289.
[26] Kurs A, Karalis A, Moffatt R, Joannopoulos JD, Fisher P, Soljačić M. Wireless power transfer via
strongly coupled magnetic resonances. J. Science. 2007; 317(5834): 83–86.
[27] Mayordomo I, Dräger T, Spies P, Bernhard J, Pflaum A. An overview of technical challenges and
advances of inductive wireless power transmission. Proc. IEEE. 2013; 101(6): 1302–1311.
[28] Wei X, Wang Z, Dai H. A Critical Review of Wireless Power Transfer via Strongly Coupled Magnetic
Resonances. Energies Journal. 2014: 4316-4341.
[29] Raju S, Wu R, Chan M, Yue CP. Modeling of Mutual Coupling Between Planar Inductors in Wireless
Power Applications. IEEE Transactions on Power Electronics. 2013; 29(1): 481–490.

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