Electronics: Broadband Microstrip Antenna For 5G Wireless Systems Operating at 28 GHZ
Electronics: Broadband Microstrip Antenna For 5G Wireless Systems Operating at 28 GHZ
Article
Broadband Microstrip Antenna for 5G Wireless Systems
Operating at 28 GHz
Rafal Przesmycki *, Marek Bugaj and Leszek Nowosielski
Abstract: Communication systems have been driven towards the fifth generation (5G) due to the
demands of compact, high speed, and large bandwidth systems. These types of radio communication
systems require new and more efficient antenna designs. This article presents a new design solution
of a broadband microstrip antenna intended for use in 5G systems. The proposed antenna has a
central operating frequency of 28 GHz and can be used in the LMDS (local multipoint distribution
service) frequency band. The dimensions of the antenna and its parameters have been calculated,
simulated, and optimized using the FEKO software. The antenna has a compact structure with
dimensions (6.2 × 8.4 × 1.57) mm. Rogers RT Duroid 5880 material was used as a substrate for the
antenna construction, which has a dielectric coefficient of 2.2 and a thickness of 1.57 mm. The antenna
described in the article is characterized by a low reflection coefficient of −22.51 dB, a high energy
gain value of 3.6 dBi, a wide operating band of 5.57 GHz (19.89%), and high energy efficiency.
Keywords: antenna; microstrip antenna; antenna 5G; 28 GHz band; 5G wireless system; broad-
band antenna
1. Introduction
The growing demand for telecommunications services is stimulating the development
Citation: Przesmycki, R.; Bugaj, M.;
Nowosielski, L. Broadband Microstrip
of new call-handling technologies. Each generation of mobile technologies has brought
Antenna for 5G Wireless Systems Op-
with it an increase in the data transmission speed along with improved connection quality
erating at 28 GHz. Electronics 2021, and new functionalities. The fourth generation (4G) technology, which is currently in
10, 1. https://dx.doi.org/10.3390/ use, has been available worldwide since 2009. The fifth generation (5G) network will
electronics10010001 enable a number of new services, including those related to the Internet of Things (IoT)
and the concept of smart cities. The new technology will make use of low, medium,
Received: 20 November 2020 and high frequency bands, all of which have their advantages and limitations. However,
Accepted: 18 December 2020 wide-scale deployment of a 5G network requires preparation of antenna infrastructure
Published: 22 December 2020 and implementation of new technological solutions. A significant number of antennas
(apart from antennas used for mobile devices) will be to be installed inside buildings,
Publisher’s Note: MDPI stays neu- especially public utility buildings, including stadiums, railway stations, and shopping
tral with regard to jurisdictional claims centers. It should be noted, at this point, that antennas installed in locations close to crowds
in published maps and institutional would be smaller than those used in current macrocell transmitters. This is a fundamental
affiliations. difference and a common misunderstanding in public discussion. In a traditional antenna
system, the power is radiated according to the established spatial characteristics. Therefore,
the area in which users can be located, is predefined. In contrast, the power in a 5G antenna
Copyright: © 2020 by the authors. Li-
is radiated directionally, and focused on individual users or groups of users. Antenna
censee MDPI, Basel, Switzerland. This radiation directions can change almost automatically, to focus on mobile users [1–3].
article is an open access article distributed In this article, we describe the design process and a model of a microstrip antenna
under the terms and conditions of the designed in FEKO software by Altair. The antenna’s main assumption is its frequency of
Creative Commons Attribution (CC BY) operation in the 28 GHz band, i.e., in one of the frequency bands designed for operation of
license (https://creativecommons.org/ the 5G system [4]. Other important assumptions for the antenna model include a small
licenses/by/4.0/). size and the widest possible bandwidth. The antenna design process has been optimized
to minimize dimensions and weight, thereby enabling the use of the designed antenna in
mobile terminals, as well as facilitating integration with electronic devices.
Figure 1.
Figure 1. The
The 28
28 GHz
GHz (27.50–28.35 GHz) local
(27.50–28.35 GHz) local multipoint
multipoint distribution
distribution service
service (LMDS)
(LMDS) spectrum.
spectrum.
The 28 GHz band and other millimeter frequency bands (mmWave), such as 24 GHz
37/39GHz
and 37/39 GHzbands,
bands,will
willplay
playa akey
keyrole
role
inin
5G5G implementations
implementations under
under thethe
newnew Up-
Upper
per Microwave
Microwave Flexible
Flexible Use License
Use License (UMFUS).
(UMFUS). The UMFUS
The UMFUS bandsbands are standardized
are standardized for
for 3GPP
3GPP
in in accordance
accordance with
with 5G New5GRadio
New Radio (NR) guidelines,
(NR) guidelines, in particular
in particular withinwithin Frequency
Frequency Band
2Band 2 (FR2),
(FR2), whichwhich includes
includes millimeter
millimeter frequencies.
frequencies.
The UMFUS bands are currently maintained and used by national mobile phone opera-
tors, innovative mobile phone companies, regional phone operators, and other organizations
wishing to implement mobile networks or provide fixed wireless access (FWA) services [8–10].
The UMFUS bands are subject to rules and regulations, which impose power limits
at fixed and base stations operating in conjunction with mobile systems (EIRP density
Electronics 2021, 10, 1 4 of 19
limit + 75 dBm/100 MHz). The average power of the sum of all antenna components in a
mobile base station must not exceed a maximum EIRP value of +43 dBm. Network deploy-
ments may use any desired duplex scheme, provided that other technical or operational
requirements are met [13].
The 28 GHz band is ideal for a wide range of applications making use of speeds
>1 Gb/s (depending on channel size), which are achievable using the spectrum designated
by UMFUS. High-speed backhaul, “at home” 5G/FWA, and other applications make use
of the ability to implement fixed PTP (point-to-point) and PTMP (point-to-multi-point)
configurations. The 28 GHz band can also be used for mobile applications, which are
currently a key pillar of 5G deployment championed by national carriers and other organi-
zations [11–13].
resonance frequency, fr , and the relative permittivity, εr , of the dielectric layer of the copper
laminate, which are the foundation of the new antenna [24].
The antenna is designed to operate in a 5G system, on frequencies ranging from
27.50 GHz to 28.35 GHz (LMDS band) and the center frequency fr = 28.00 GHz. Choosing
the thickness of the substrate is one of the most important stages in the antenna design
process, as the thickness of the substrate directly affects the efficiency and bandwidth of
the microstrip antenna. One of the assumptions for this antenna is to obtain the widest
bandwidth possible. As the thickness of the substrate increases, the antenna’s bandwidth
increases, while its efficiency decreases. The upper value of the substrate thickness was
determined from the following relationship [14,15]:
Taking into account the result provided above, the RT Duroid 5880 laminate was selected
as a substrate, with a thickness of h = 1.57 mm, permittivity εr = 2.2, and tanδ = 9.0 × 10−4 .
In the next calculation step, the width of the radiating element should be determined from
the following relationship [16,17]:
r
3 × 108
r
c 2 2
W= = = 4.17 mm. (2)
2 fr εr + 1 2 × 28 × 109 2.2 + 1
To determine the length of the radiating element, the effective permittivity εreff , of the
substrate must first be calculated. It is defined by the following relationship [18,19]:
εr + 1 εr − 1 2.2 + 1 2.2 − 1
ε re f f = + q = + q = 1.6 + 0.21 = 1.81. (3)
2 h
2 1 + 12 W 2 2 1 + 12 × 1.57
4.17
Upon calculating εreff , the effective length of the patch Le should be determined from
the following relationship [20,21]:
c 3 × 108
Le = √ = √ = 3.98 mm. (4)
2 f r ε re f f 2 × 28 × 109 1.81
Then, we calculate by how much the patch should be shortened using the following
relationship [22,25]:
0.412· h ε re f f + 0.3 W h + 0.264 0.412 × 1.57 ( 1.81 + 0.3 ) 4.17
1.57 + 0.264
∆L = = = 0.74 mm.
ε re f f − 0.258 W h + 0.8
4.17
(1.81 − 0.258) 1.57 + 0.8
(5)
The final patch length value is:
Once the size of the radiating element is determined, the size of the reference plane
also needs to be determined. The size of the reference plane is assumed to be greater
than the radiating element by approximately six thicknesses of the substrate, by both
width and length. The dimensions of the reference plane are determined by the following
relationship [26,27]:
Ls = L + 6h = 2.58 + 6 × 1.57 = 12 mm. (7)
Ws = W + 6h = 4.17 + 6 × 1.57 = 13.59 mm. (8)
In the next step, we determine the inset feed gap from the following relation [21]:
Electronics 2021, 10, 1 6 of 19
The last step of the numerical antenna design process is to determine the size of the
feed line. By calculating the dimensions of a microstrip feed line with a characteristic
impedance ZC = 50 Ω, we start the determination of auxiliary variables a and b as:
q
Zc ε r +1 ε r −1 0.11
a= 60 2 + ε r +1 0.23 + εr = 1.158
2
(10)
60π
b= √
Zc ε r
= 7.97
Since parameter a is less than 1.52, the width and length of the feed line is determined
from the following relationships [21,23]:
n h io
r −1
W f = π2 b − 1 − ln(2b − 1) + ε2ε ln(b − 1) + 0.39 − 0.61 ·h
r εr (11)
= 3.07 mm.
Figure 2.
Figure Antenna model
2. Antenna model view,
view, front
front and
and back
back side.
side.
6. Optimization
6. Optimization Process
Process and
and Discussion
Discussion of of Simulation
Simulation Results
Results
Computer simulations can help to determine the electrical parameters and radial
Computer simulations can help to determine the electrical parameters and radial
characteristics of the antenna; in this case, we used FEKO software developed by the Altair
characteristics of the antenna; in this case, we used FEKO software developed by the Altair
company.
company.
The analysis of electrical parameters of the radiating element design solution and
The analysis of electrical parameters of the radiating element design solution and
other antenna elements indicates that there is room to improve the electrical parameters of
other antenna elements indicates that there is room to improve the electrical parameters
of the antenna by reducing VSWR, increasing the width of the operating band, miniatur-
izing antenna dimensions, and increasing antenna gain. For this purpose, the design was
optimized for the parameters mentioned above, using FEKO software from the Altair
company. The calculated parameters of the rectangular patch were used to create a pre-
6. Optimization Process and Discussion of Simulation Results
Computer simulations can help to determine the electrical parameters and radial
characteristics of the antenna; in this case, we used FEKO software developed by the Altair
company.
The analysis
Electronics of1electrical parameters of the radiating element design solution and
2021, 10, 7 of 19
other antenna elements indicates that there is room to improve the electrical parameters
of the antenna by reducing VSWR, increasing the width of the operating band, miniatur-
izing antenna dimensions, and increasing antenna gain. For this purpose, the design was
the antenna by reducing VSWR, increasing the width of the operating band, miniaturizing
optimized for the parameters mentioned above, using FEKO software from the Altair
antenna dimensions, and increasing antenna gain. For this purpose, the design was opti-
company. The calculated parameters of the rectangular patch were used to create a pre-
mized for the parameters mentioned above, using FEKO software from the Altair company.
liminary simulation of the electrical parameters of the developed antenna model. Then,
The calculated parameters of the rectangular patch were used to create a preliminary
the model underwent a process of optimization, with the main assumption that the an-
simulation of the electrical parameters of the developed antenna model. Then, the model
tenna must operate at the resonance frequency of 28 GHz.
underwent a process of optimization, with the main assumption that the antenna must
The FEKO software supports the ability to define the electrical parameters optimiza-
operate at the resonance frequency of 28 GHz.
tion process for the designed antenna and provides a number of options related to opti-
The FEKO software supports the ability to define the electrical parameters optimization
mization. The algorithm of the optimization
process forprocess used by
the designed the FEKO
antenna and software
provides is shown of options related to optimization.
a number
in Figure 3. The algorithm of the optimization process used by the FEKO software is shown in Figure 3.
In the optimization process of the proposed antenna, the option “specify maximum
number of runs by the solver” was chosen. In the next step, we have to define the pa-
rameters of the antenna model that are to be changed during the optimization process in
order to achieve an optimal solution. The parameters define the variables, which can be
changed during the optimization process. These parameters are local for each optimization
search, and a correct search must contain at least one defined parameter. Any variable
defined in the FEKO software can be used as an optimization parameter, for example,
the physical dimensions of the model, load, and source (amplitude and phase), provided
that no relationship is implied between the optimization parameters in the same search.
During the optimization process, the length and width of the antenna base with the
screen (Ws , We , Ls , and Le ), the length and width of the radiator (Lp and Wp ), the length
and width of the power line (Lf and Wf ) and the length and width of the patch inset (Y0 and
X0 ) were changed. Other structural elements, such as thickness and permittivity of the
substrate, were not changed [28–31].
In the next step, we define the range of parameters to be changed, specifying their
minimum, maximum, and initial values. For each optimization parameter, a minimum value
and a maximum value must be defined, and optionally, an initial value can be given as
well. The initial value will influence the optimization process when using particle swarm
optimization or genetic algorithm. If the starting value is not specified by the user, the value in
the middle of the range of the parameter will be taken as the starting point of the optimization.
In our optimization process, we selected the minimum, maximum, and start values based on
calculated parameters of the rectangular patch and the center frequency.
In the next step, we define an optimization mask. An optimization mask is a set of
user-defined values forming a continuous line. The mask is a criterion to which the optimal
solution must adhere. It is specified that the optimized solution is smaller, equal, or larger
than the mask. When calculating an optimal solution, the target values are compared with
the mask. If the mask criterion is met, the values are added to the value table. We do not
define an optimization mask in our optimization process.
The last step of the optimization process is the selection of the optimization target.
The objectives, which need to be defined, specify the desired state that the optimization
process should try to achieve by changing certain parameters of the antenna model.
For each optimization search, goals should be defined to determine the desired state
that the optimization process should aim to achieve. Many goals can be defined, but a
correct optimization search must include at least one goal. During the optimization process
we define the following goals:
• Impedance goal (input impedance, input admittance, reflection coefficient (S11 ), trans-
mission coefficient, VSWR, return losses, current);
• Near-field goal (E field – electric field, H field – magnetic field, directional component,
coordinate system);
• Far-field goal (E field, antenna gain, directivity, RCS – Radar Cross Section);
• S-parameter goal (coupling coefficient, reflection coefficient, transmission coefficient,
VSWR, return losses);
• SAR (Specific Absorption Rate) goal;
• Power goal (efficiency, active power, power loss);
• Transmission/reflection coefficients goal (reflection, transmission, co-polarization,
and cross-polarization);
• Receiving antenna power goal (efficiency, active power, and power loss).
In our optimization process, we chose an impedance target (reflectance and VSWR)
with a target minimization operator. The impedance target provides optimization related
to the impedance and admittance of any voltage or current source, which is solved within
the FEKO model. The reflectance ratio is calculated in relation to the indicated reference
impedance.
In the case of an impedance target, the reflection factor is calculated directly from the
observed input impedance. Therefore, this value is the active reflection factor, and may
Electronics 2021, 10, 1 9 of 19
differ from the S11 , which was calculated during the calculation of the S parameter in the
multiport model. The voltage standing waveform factor for the observed input impedance
is considered in relation to the indicated reference impedance.
Once the parameters of the optimization process have been defined, we can run
“OPTFEKO” to calculate the optimal solution for the specified parameters. Once the
optimal values for the model are obtained, the FEKO model with the optimal parameters is
created.
The optimization process resulted in a final design of the antenna model, as shown in
Electronics 2020, 9, x FOR PEER REVIEW 10 of 20
Figure 4. Dimensions of this design are shown in Table 2.
Figure4.4.The
Figure Theoptimized
optimizedantenna
antennamodel
modelview,
view,front
frontand
andback
backside
sidewith
withdimensions.
dimensions.
Table 2. Dimensions of the optimized antenna model.
The resulting antenna design was simulated with the use of FEKO software from the
Altair company,
Antennawhich provided results forSymbol
Component the following electrical parameters:
Dimensions (mm) reflection
coefficient, standing wave
Ground plane widthratio, input impedance,
W S = We antenna gain, current
8.40 distribution in
the antenna, and radiation characteristics.
Ground plane length L S = Le 6.20
Patch width Wp 3.66
6.1. Q Factor Patch length Lp 2.14
Copper thickness Cu 0.05
The QSubstrate
factor ofthickness
an antenna is defined in the
h same way as for resonant 1.57 circuits, i.e., the
ratio of energy stored to energy lost during one
Permittivity Er period of vibration. 2.2 The difference is in
the user’s expectations, while for resonant circuits,
Feed line width Wf a high Q factor is usually
1.26 required, the
Feed for
opposite is true lineantennas.
length By determiningLthe
f 3.10to easily estimate
Q factor, it is possible
the bandwidth Inset
offeed gap
an antenna. The larger BWYis0 because of a reduction 0.50in the Q factor of
Width feed gap X0 0.68
the patch resonator, which is due to less energy being stored beneath the patch, and due
to higher radiation. In order to determine the Q factor value in the first step, we analyti-
callyThe resultingthe
determine antenna designofwas
bandwidth the simulated
antenna basedwith the use dimensions
on the of FEKO software
of the from the
proposed
Altair company,
antenna model which provided
(dimensions results
of the for theelement
radiating followingandelectrical parameters:
the thickness of the reflection
substrate),
coefficient, standing wave
using the following ratio, input impedance, antenna gain, current distribution in the
dependencies:
antenna, and radiation characteristics.
𝜀𝑟 − 1 ℎ 𝑊 2.2 − 1 1.57 3.66
𝐵𝑊 = 3.771 ∙ [ 2
] ∙ ∙ ( ) = 3.771 ∙ [ ]∙ ∙( )
6.1. Q Factor (𝜀𝑟 ) 𝜆0 𝐿 2.22 10.7 2.14 (13)
1.2
The Q factor of an antenna = is3.771 [
defined ] ∙ the
in 0,146728 ∙ 1.71028
same way as for=resonant
23% circuits, i.e.,
4.84
the ratio of energy stored to energy lost during one period of vibration. The difference is
in theThe theoretical
user’s bandwidth
expectations, while for forresonant
the antenna, calculated
circuits, a high Q from mathematical
factor relation-
is usually required,
ships,
the is about
opposite 23%.for
is true Theantennas.
BW of theBy microstrip
determining antenna
the Qis inversely proportional
factor, it is possible to to its Q
easily
factor and
estimate theisbandwidth
given by [32]
of the following:The larger BW is because of a reduction in the
an antenna.
Q factor of the patch resonator, which is due(𝑉𝑆𝑊𝑅 to less energy
− 1) being stored beneath the patch,
𝐵𝑊 =
and due to higher radiation. In order to determine the Q factor value in the first step, (14)
𝑄 𝑉𝑆𝑊𝑅
we analytically determine the bandwidth of the antenna based on the dimensions of the
Having determined the theoretical bandwidth BW and taking VSWR = 2 as the limit
value for the bandwidth, after transforming the above Relation (14) the Q factor of the
antenna was determined as:
(𝑉𝑆𝑊𝑅 − 1) (2 − 1) 1
𝑄= = = = 3.07. (15)
𝐵𝑊 𝑉𝑆𝑊𝑅 0.23 2 0.3252
Electronics 2021, 10, 1 10 of 19
proposed antenna model (dimensions of the radiating element and the thickness of the
substrate), using the following dependencies:
BW = 3.771· ε r −12 · λh0 · WL
(ε r )
h i h i (13)
= 3.771 × 2.2 −1 × 1.57 × 3.66 = 3.771 1.2 × 0.146728 × 1.71028 = 23%
2.22 10.7 2.14 4.84
The theoretical bandwidth for the antenna, calculated from mathematical relationships,
is about 23%. The BW of the microstrip antenna is inversely proportional to its Q factor
and is given by [32] the following:
(VSWR − 1)
BW = √ (14)
Q VSWR
Having determined the theoretical bandwidth BW and taking VSWR = 2 as the limit
value for the bandwidth, after transforming the above Relation (14) the Q factor of the
antenna was determined as:
(VSWR − 1) (2 − 1) 1
Q= √ = √ = = 3.07. (15)
BW VSWR 0.23 2 0.3252
The analytically low value of the antenna’s Q factor confirms its ability to operate in a
wide frequency range.
Figure 5. The reflection coefficient as a function of frequency for the proposed antenna working in the fifth generation
Figure 5. The reflection coefficient as a function of frequency for the proposed antenna working in the fifth generation (5G) system.
(5G) system.
Figure 5. The reflection coefficient as a function of frequency for the proposed antenna working in the fifth generation
(5G) system.
6.3. Voltage Standing Wave Ratio
6.3.
InVoltage Standing
the case Wave antenna,
of a patch Ratio the voltage standing wave ratio (VSWR) should not be
greater In the 2case
than of a the
across patch antenna,
entire the voltage
frequency standing
band. Ideally, wave
thisratio
value(VSWR)
shouldshould
equalnot
1 [24,34].
Thebevoltage
greater standing
than 2 across
wavetheratio
entire
as frequency
a functionband. Ideally, this
of frequency value should
is shown equal6.1As can
in Figure
be [24,34].
seen inThe voltage
Figure 6, standing
the VSWR wave ratio obtained
value as a function
at aofresonance
frequency isfrequency
shown in Figure 6. GHz
of 28.00
As can be seen in Figure 6, the VSWR value obtained at a resonance frequency
equals 1.162, and the VSWR value of 2 was determined at 26.01 and 31.58 GHz respectively. of 28.00
GHz equals 1.162, and the VSWR value of 2 was determined at 26.01 and 31.58 GHz re-
The above values show that the proposed antenna operates in the whole assumed frequency
spectively. The above values show that the proposed antenna operates in the whole as-
band (LMDS), i.e., from 27.50 to 28.35 GHz.
sumed frequency band (LMDS), i.e., from 27.50 to 28.35 GHz.
Figure 7. The chart of the complex input impedance as a function of frequency for the proposed antenna working in the
Figure 7. The chart of the complex input impedance as a function of frequency for the proposed antenna working in the 5G
5G system (real part, blue line and imaginary part, green line).
system (real part, blue line and imaginary part, green line).
6.5. Antenna Gain
Usually, antenna gain is given in relation to an isotropic antenna and is expressed in
dBi. In some cases, antenna gain is also given in relation to the dipole antenna and ex-
pressed in dBd. The energy gain of an antenna is dependent on its directivity and the
energy loss of the antenna, which results from the material it is made of [35,37]. The pro-
Electronics 2021, 10, 1 12 of 19
Figure 8. The chart of antenna gain as a function of frequency for the proposed antenna working in the 5G system.
Figure 8. The chart of antenna gain as a function of frequency for the proposed antenna working in the 5G system.
Figure 8. The chart of Current
6.6. antenna gain as a function
Distribution of frequency
in the Antenna for the proposed antenna working in the 5G system.
6.6. Current Distribution in the Antenna
In In a microstrip antenna, the value of the current should be minimal at the end of the
a6.6.
microstrip antenna,inthe
Current Distribution value of the current should be minimal at the end of
the Antenna
radiating element (the edge of the patch). The voltage at the edge of the patch is phase
the radiatingInelement (the
a microstrip edge the
antenna, of the
valuepatch). The voltage
of the current should beatminimal
the edgeat theofend
theofpatch
the is
shifted in relation to the current. Therefore, peak voltage is present at the end of the patch,
phase radiating
shifted in element
relation (the
to edge
the of the patch).
current. The voltage
Therefore, at the
peak edge ofisthe
voltage patch isat
present phase
the end
with current values close to zero [33,37]. A similar situation occurs in the middle of the
of the shiftedwith
patch, in relation to the
current current.
values Therefore, peak voltageAis present atsituation
the end of occurs
the patch,
wave, further down the line, i.e., atclose to zero
the beginning [33,37].
of the patch. similar
The phase-shifted voltage in the
with current values close to zero [33,37]. A similar situation occurs in the middle of the
middle
in relation to the current phase produces fields on the edges of a microstrip antenna. The
of the wave, further down the line, i.e., at the beginning of the patch. The phase-
wave, further down the line, i.e., at the beginning of the patch. The phase-shifted voltage
shifted voltage
current in relation
distribution of thetodeveloped
the current phaseatproduces
antenna frequenciesfields on the
of 27.51 GHz edges of aGHz
(a), 28.0
in relation to the current phase produces fields on the edges of a microstrip antenna. The
microstrip
(b), and
antenna. 28.35
The GHz (c)
current is presentedofinthe
distribution Figure 9.
developed antenna at frequencies of 27.51 GHz (a),
current distribution of the developed antenna at frequencies of 27.51 GHz (a), 28.0 GHz
28.0 GHz(b), (b), and
and 28.35
28.35 GHzGHz(c) is (c) is presented
presented in Figure in9.Figure 9.
(a)
(a)
Figure 9. Cont.
Electronics 2021, 10, 1 13 of 19
(b)
(c)
Figure 9. Surface current distribution for the proposed 5G antenna at different frequencies. (a) 27.51 GHz; (b) 28.0 GHz; (c) 28.35 GHz.
(a)
(b)
(c)
Figure 10. The three-dimensional (3D) view of radiation pattern for the proposed 5G antenna model at different frequencies.
(a) 27.51 GHz; (b) 28.0 GHz; (c) 28.35 GHz.
Electronics 2020, 9, x FOR PEER REVIEW 16 of 20
Electronics 2020, 9, x FOR PEER REVIEW 16 of 20
Figure
Electronics 10.10,The
2021, 1 three-dimensional (3D) view of radiation pattern for the proposed 5G antenna model at different frequen-
15 of 19
Figure 10.27.51
cies. (a) The three-dimensional
GHz; (b) 28.0 GHz;(3D) viewGHz.
(c) 28.35 of radiation pattern for the proposed 5G antenna model at different frequen-
cies. (a) 27.51 GHz; (b) 28.0 GHz; (c) 28.35 GHz.
Figure 11.
Figure The normalized
11. The normalizedradiation
radiationpatterns
patternsfor
forthe
theproposed
proposedantenna
antennamodel
modeloperating
operatingininthe
the5G
5G
system
Figure for
11. 27.51
The GHz
normalized(blue line),
radiation28.0 GHz
patterns(green
for line),
the and
proposed 28.35 GHz
antenna (red
modelline) in polar
operating coordinates
in
system for 27.51 GHz (blue line), 28.0 GHz (green line), and 28.35 GHz (red line) in polar coordi- the 5G
for vertical
system
nates for polarization.
for vertical
27.51 GHz (blue line), 28.0 GHz (green line), and 28.35 GHz (red line) in polar coordi-
polarization.
nates for vertical polarization.
Figure 12.
Figure The normalized
12. The normalizedradiation
radiationpatterns
patternsfor
forthe
theproposed
proposedantenna
antennamodel
modeloperating
operatingininthe
the5G
5G
system
Figure for
12. 27.51
The GHz (blue
normalized line),
radiation28.0 GHz
patterns(green
for line),
the and
proposed 28.35 GHz
antenna (red
modelline) in polar
operating coordinates
in
system for 27.51 GHz (blue line), 28.0 GHz (green line), and 28.35 GHz (red line) in polar coordi-the 5G
system for horizontal
27.51polarization.
for horizontal
nates for GHz polarization.
(blue line), 28.0 GHz (green line), and 28.35 GHz (red line) in polar coordi-
nates for horizontal polarization.
7. Comparison of the Proposed Antenna with Other Antennas
The obtained parameter values for the proposed microstrip antenna can be compared
in terms of impedance matching and appropriate bandwidth, with other published results
for the purposes of comparative evaluation. For example, the frequency response of the
Electronics 2021, 10, 1 measured S11 parameter of the proposed antenna may not be the lowest as compared16with of 19
the S11 values obtained for the antennas presented in [18,20,32], but it is relatively low.
Figure 13 shows a comparison of the reflection factor as a function of frequency for
the proposed antenna, and the antennas developed in other works. The corresponding
7. Comparison
frequency of theusing
responses Proposed Antenna
the VSWR with Other
parameter Antennaswith each other, as shown
are compared
The obtained
in Figure 14. parameter values for the proposed microstrip antenna can be compared
in terms
The of impedance
minimum matching
reflection lossand appropriate
value obtainedbandwidth,
in this study with other−22.51
is about published results
dB (VSWR
for the purposes of comparative evaluation. For example, the frequency response
≈ 1.16), while in [20] it is about −26.00 dB (VSWR ≈ 1.10), in [18] it is about −21.00 dB (VSWR of the
measured S
≈ 1.20), and in parameter of the proposed antenna may not be the lowest as compared
11 [32] it is about −18.00 dB (VSWR ≈ 1.28). Moreover, for the antenna proposed with
the S
in this values obtained for the antennas presented in [18,20,32], but it is relatively
11work, the operating band of the antenna (BW) is the largest, amounting to S11 ≤ −10 low.
Figure≤132)shows
dB (VSWR 5.57 GHz,a comparison of the reflection
and is centered exactly at factor
28 GHz,as awhile
function of frequency
in [20] the operatingfor
the proposed
band is 2. 63 GHzantenna,
and isandalsothe antennas
centered developed
exactly in other
at 28 GHz, in [18]works. The corresponding
the operating band is 2.85
frequency responses using the VSWR parameter are compared with
GHz and is also centered at about 28.1 GHz (shift of about 100 MHz), and in [32] each other, as the
shown
op-
in Figure 14.
erating band is 1.07 GHz and is also centered exactly at 28 GHz.
Figure
Figure 13.
13. The
The reflection
reflection coefficient
coefficient as
as aa function
function of
of frequency for the
frequency for the proposed
proposed antenna
antenna and
and antennas
antennas from
from other
other works.
works.
Electronics 2020, 9, x FOR PEER REVIEW 18 of 20
Figure
Figure 14.
14. The
The voltage standing wave
voltage standing waveratio
ratio(VSWR)
(VSWR)asasaafunction
functionofoffrequency
frequencyfor
for the
the proposed
proposed antenna,
antenna, and
and antennas
antennas from
from other works.
other works.
Table 3. Comparisons among the bandwidth achieved in the present work to those achieved in
Electronics 2021, 10, 1 17 of 19
The minimum reflection loss value obtained in this study is about −22.51 dB (VSWR ≈
1.16), while in [20] it is about −26.00 dB (VSWR ≈ 1.10), in [18] it is about −21.00 dB
(VSWR ≈ 1.20), and in [32] it is about −18.00 dB (VSWR ≈ 1.28). Moreover, for the antenna
proposed in this work, the operating band of the antenna (BW) is the largest, amounting to
S11 ≤ −10 dB (VSWR ≤ 2) 5.57 GHz, and is centered exactly at 28 GHz, while in [20] the
operating band is 2. 63 GHz and is also centered exactly at 28 GHz, in [18] the operating
band is 2.85 GHz and is also centered at about 28.1 GHz (shift of about 100 MHz), and in [32]
the operating band is 1.07 GHz and is also centered exactly at 28 GHz.
A comparative summary of the proposed antenna with the antennas described
in [18,20,32] is presented in Table 3. It shows that the proposed microstrip antenna in
this work has the best impedance matching bandwidth performance in all cases, especially
for stringent matching conditions (VSWR ≤2, VSWR ≤1.5, and VSWR ≤1.25).
Table 3. Comparisons among the bandwidth achieved in the present work to those achieved in other published works.
Performance Measure Present Work (Proposed Antenna) Work of [18] Work of [20] Work of [32]
Center frequency 28.00 GHz 28.10 GHz 28.00 GHz 28.00 GHz
VSWR ≤ 1.25 1.15 GHz 0.45 GHz 0.79 GHz NA
BW VSWR ≤ 1.5 2.68 GHz 1.74 GHz 1.57 GHz 0.55 GHz
VSWR ≤ 2 5.57 GHz 2.85 GHz 2.63 GHz 1.07 GHz
Relative BW 19.89% 10.14% 9.39% 3.83%
Gain 5.06 dBi 6.59 dBi 6.37 dBi 6.72 dBi
8. Conclusions
A rectangular microstrip antenna has been proposed for 5G applications in response
to the growing demand for mobile data and mobile devices. This antenna has a resonance
frequency of 28.00 GHz, for which the reflectance is equal to −22.50 dB. The proposed
antenna has a radiation efficiency of 80.18% and the antenna gain for the resonance fre-
quency is 5.06 dB. The results also show that its bandwidth is 5.57 GHz (relative operational
band 19.89%), which is a very good result, much greater than results achieved in other
published works, such as [15,16], where the operating bandwidth of the proposed antennas
is around 1 or 2 GHz [18–20]. The proposed antenna would be a good option for 5G mobile
communication, as it offers the high throughput required. The antenna is very compact
and lightweight, which makes it suitable for devices where space is a major limitation.
Author Contributions: Conceptualization, R.P.; Methodology, R.P. and M.B.; Resources, M.B. and L.N.;
Visualization, R.P. and M.B.; Writing—original draft, R.P., M.B. and L.N.; Writing—review & editing,
L.N. For other cases, all authors have participated. All authors have read and agreed to the published
version of the manuscript.
Funding: This research received no external funding.
Institutional Review Board Statement: Not applicable.
Informed Consent Statement: Not applicable.
Data Availability Statement: Data sharing not applicable. No new data were created or analyzed in
this study. Data sharing is not applicable to this article.
Conflicts of Interest: The authors declare no conflict of interest.
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