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Article

Dual-Band Multilayer Patch Antenna for Multiband Internet-of-Vehicles Applications

by
Ebenezer Tawiah Ashong
1,
Seungwoo Bang
2 and
Jae-Young Chung
3,*
1
Department of Electrical and Electronic Engineering, Ho Technical University, Ho VH-0044-6820, Ghana
2
Institute of New Media and Communications, Electrical and Computer Engineering, Seoul National University, Seoul 08826, Republic of Korea
3
Department of Electrical and Information Engineering, Seoul National University of Science and Technology, Seoul 01811, Republic of Korea
*
Author to whom correspondence should be addressed.
Electronics 2025, 14(22), 4400; https://doi.org/10.3390/electronics14224400
Submission received: 16 September 2025 / Revised: 6 November 2025 / Accepted: 10 November 2025 / Published: 12 November 2025
(This article belongs to the Special Issue Antennas for IoT Devices, 2nd Edition)

Abstract

The growing demand for internet-of-vehicles (IoV) communication requires compact antennas capable of supporting multiple frequency bands while maintaining stable radiation characteristics. This paper presents the design and validation of a multilayer microstrip patch antenna that achieves dual-band operation through the integration of shorting vias, a coupled ring, and an embedded parasitic patch. Parametric studies confirm that the adopted techniques yield impedance bandwidths of 28% at 1.8 GHz and 6.4% at 2.4 GHz, with a low-profile structure of 0.055 λ 0 . Measured results demonstrate omnidirectional radiation patterns across the intended bands with a maximum gain of 4.46 dBi at 2.57 GHz. Beyond simulated and laboratory verification, field tests were conducted using LTE communication to evaluate the antenna’s quality of service (QoS) under realistic vehicular conditions. To reduce system cost and simplify testing, a low-cost in-house signal meter based on a Raspberry Pi microcontroller was developed and employed to compare the proposed antenna with a commercial monopole. The results confirm that the multilayer patch antenna provides improved bandwidth, gain, and radiation stability, making it a compact and cost-effective candidate for multiband IoV and V2X communication systems.

1. Introduction

The Internet of Vehicles (IoV), an evolution of vehicular ad hoc networks (VANETs), has emerged as a key enabler of intelligent transportation systems. By supporting vehicle-to-everything (V2X) communications, IoV extends the Internet-of-Things (IoT) paradigm to vehicles, enabling real-time data exchange among vehicles, roadside infrastructure, and cloud services. Such connectivity underpins safety, traffic efficiency, and energy management applications. While advanced standards such as dedicated short-range communication (DSRC) and cellular V2X (C-V2X) are being developed, existing networks including long-term evolution (LTE) and wireless local area networks (WLANs) remain critical for near-term IoV deployment because of their ubiquity and reliability [1,2,3]. The performance of these systems, however, depends strongly on the antenna subsystems integrated into vehicles [4,5].
Vehicular antennas must be compact, rugged, and multiband while maintaining omnidirectional radiation to ensure link stability regardless of orientation. Conventional whip antennas, though still common, are tall (≈ λ / 4 ), mechanically fragile, and aesthetically intrusive. To overcome these drawbacks, Delaveaud et al. [6] introduced the monopolar wire-patch antenna, and Economou and Langley [7] demonstrated a triangular dual-band patch with monopole-like radiation. These early monopolar designs, however, offered narrow bandwidths (1.5–3%), insufficient for modern vehicular LTE B1/B3 standards.
Subsequent works sought to enhance bandwidth using structural innovations. Al-Zoubi et al. [8] employed coupled rings to generate additional resonances, while Liu et al. [9] showed that multiple shorting vias broaden the impedance response. Chen and Dou [10] extended this concept using non-uniform via arrays and ring slots, achieving bandwidths near 32%. Further improvements include ultra-low-profile monopoles [11], coupled-fed filtering patches [12], substrate-integrated-waveguide (SIW) monopoles [13], and omnidirectional filtering patches with multi-state operation [14]. Characteristic-mode-based approaches have also been applied to optimize UWB and multiband monopolar antennas [15,16].
Recently, IoV-specific antenna designs have gained momentum. Li et al. [17] proposed an ultra-thin multiband logo antenna, Lakshmi et al. [18] introduced a flexible conformal antenna for sub-6 GHz vehicular use, and Yahya et al. [19] reported a compact dual-band V2V antenna. Kannappan et al. [20] developed transparent tri-band antennas, while Keshavarz et al. [21] demonstrated dual-band vehicular MIMO arrays. Yadav et al. [22] also introduced a multiband high-frequency antenna targeting 6G and automotive radar Despite these advances, many reported IoV antennas either lack sufficient bandwidth to simultaneously cover LTE B1/B3 and WLAN, depend on costly substrates, or omit real-world vehicular validation.
To address these challenges, this work proposes a multilayer microstrip patch antenna that combines structural simplicity, cost-effectiveness, and robust wideband performance across key IoV frequency bands. The main contributions are summarized below:
  • A compact multilayer patch antenna is designed for dual-band operation at LTE B1/B3 and WLAN frequencies.
  • The antenna achieves 28% and 6.4% measured impedance bandwidths with a low profile of 0.055 λ 0 , far shorter than conventional monopoles.
  • Integration of shorting vias, a coupled ring, and an embedded parasitic patch enables broadband matching and omnidirectional radiation.
  • Two-stage validation—anechoic-chamber measurements and LTE field trials—confirms stable radiation, 4.46 dBi peak gain, and improved signal strength, SNR, and throughput compared with a commercial monopole.
  • The antenna offers low-cost FR-4 implementation, robust multiband IoV/V2X performance, and scalability for vehicular communication systems.
Our design originates from a circular monopolar patch operating in the TM 02 mode, known for omnidirectional radiation [6,7]. We (i) introduce a distributed shorting-via array to excite a composite TM 01 / TM 02 response [9,10]; (ii) add a coupled ring to tune the effective electrical size and control mode spacing [8]; and (iii) embed a vertically spaced parasitic patch to reshape impedance and create an additional controlled resonance. Co-optimizing the ring dimensions ( a , b ) , via placement ( d , r ) , and parasitic parameters ( h 2 , R mid ) yields dual impedance bandwidths of 28% (1.71–2.28 GHz) and 6.4% (2.41–2.57 GHz) with monopole-like radiation at a 0.055 λ 0 profile on FR-4. The design is experimentally verified through chamber and vehicular field measurements, demonstrating simultaneous wide LTE B1/B3 and WLAN coverage, sub- 0.06 λ 0 height, and practical IoV applicability.

2. Antenna Design and Optimization

2.1. Antenna Geometry

The geometry of the proposed antenna is shown in Figure 1a–c, with key dimensions listed in Table 1. A circular radiating patch is implemented on a two-layer FR-4 stack ( ε r = 4.1 , tan δ = 0.02 ) of radius R g . The upper metallization hosts the main patch and a concentric coupled ring (inner radius a, outer radius b) (Figure 1a), while an embedded parasitic patch of radius R mid is placed between the substrates above the ground plane (Figure 1b). Although the parasitic patch geometrically overlaps the feed and via ring regions, small clearance gaps are provided around these elements to prevent direct electrical contact while preserving electromagnetic coupling. Fifteen shorting vias of radius r, equally spaced on a circle of radius d, connect the radiator to ground. A 50 Ω coaxial probe feeds the antenna at the center. For visibility, Figure 1c exaggerates metal thicknesses.
The monopole-like azimuth pattern arises from in-phase vertical currents on the central probe and shorting vias [6,7]; Figure 2 shows the strongest, in-phase currents at these locations [10]. The distributed via ring also enables miniaturization, yielding a 0.055 λ 0 profile at 1.7 GHz.
FR-4 ( ε r 4.1 , tan δ 0.02 ) was adopted as a practical substrate balancing bandwidth, efficiency, cost, and mechanical robustness. A lower- ε r material (e.g., Rogers RT/Duroid 5880) would improve radiation efficiency and bandwidth but increase patch diameter by ∼30–35%; a higher- ε r substrate would reduce footprint but narrow impedance bandwidth and lower efficiency. Alternative miniaturization (e.g., slots, meanders, reactive surfaces, local high- ε r loading) is possible if further size reduction is required.

2.2. Resonance Behavior and Bandwidth Enhancement

Design sequence: (1) Size the circular patch for the TM 02 mode near the low band using the cavity model [23]. (2) Place a via ring at radius d to lower input resistance and broaden the low-band match through TM 01 coupling [6,9,10]. (3) Add a coupled ring and tune ( a , b ) to control resonance placement and spacing [8]. (4) Embed a parasitic patch at height h 2 and adjust R mid to introduce a controlled resonance and flatten the impedance. (5) Co-optimize ( d , r , a , b , h 2 , R mid ) for ≈ 50 Ω matching across both bands while preserving the monopole-like radiation of Section 2.
The circular patch is approximated by a cylindrical cavity with TM mn resonances [23]:
f m n = c 2 π R eff ε r x m n ,
where R eff includes fringing and x m n is the n-th root of J m ( x ) = 0 . The dominant TM 02 mode provides the monopole-like radiation; shorting vias also excite TM 01 , broadening the impedance response [6,9].
Parasitic-patch effect: Figure 3 compares input impedances with and without the parasitic patch, showing markedly improved matching across LTE and WLAN when coupled. Without the parasitic patch, the input impedance is high near 2.4 GHz; introducing the patch lowers the impedance around 2.6 GHz and raises it at ∼2.3 GHz, smoothing broadband coverage.
The parametric responses in Figure 4 isolate the effects of the parasitic patch’s height h 2 and radius R mid while holding all other parameters at their optimized values (Table 1). In Figure 4a, increasing h 2 reduces the separation between the parasitic and top patches, strengthening interlayer coupling. This brings the two resonant minima closer together and broadens the overall response, but the effective 10 dB impedance bandwidth narrows because the return loss becomes shallower. Smaller h 2 values (weaker coupling) yield clearer mode separation and deeper minima, resulting in improved dual-band impedance matching.
Design trade-off: Coupling strength via h 2 and resonance alignment via R mid set the bandwidth–matching trade-off: stronger coupling (larger h 2 ) enhances interaction but reduces return-loss depth; weaker coupling (smaller h 2 ) deepens minima but narrows overall bandwidth. The optimized geometry in Table 1 maintains both LTE and WLAN bands below 10 dB with smooth impedance and stable radiation.
The effect of the coupled ring is addressed next (Section 2.3), where ( a , b ) control the TM 02 placement and bandwidth (Figure 5).

2.3. Coupled Ring Optimization

The coupled ring modifies the boundary fields of the circular patch, effectively tuning the TM 02 resonance predicted by the cavity model in Equation (1). Varying the ring radii alters the effective cavity radius R eff : increasing the outer radius b (widening the ring) lowers both resonant frequencies, while increasing the inner radius a (narrowing the ring) shifts them upward. This provides a convenient geometric handle for positioning and separating the operating bands without disturbing the monopole-like radiation established by the feed and via currents.
Beyond frequency tuning, the ring functions as a weakly coupled resonator that interacts with the TM 02 mode, flattening the input-reactance slope and broadening the 10 dB impedance bandwidth. This behavior follows classical coupled-resonator theory [24,25] and has been experimentally verified for ring-coupled circular patches exhibiting broadband, monopole-like radiation [8]. In the present design, the coupled ring therefore serves two primary roles: (i) bandwidth enhancement and (ii) dual-band co-tuning in conjunction with the embedded parasitic patch.
Figure 5a,b illustrate the parametric influence of the inner and outer ring radii. Increasing a shifts both resonances upward and initially improves the low-band return loss, but beyond an intermediate value ( a 34 mm) the matching degrades and the bandwidth narrows. Conversely, increasing b lowers both resonances and strengthens coupling between the ring and main radiator: larger b values broaden the low-band response but yield shallower minima, while smaller b values produce deeper matching but narrower bandwidth.
Overall, the parameters a and b control a clear trade-off between bandwidth and matching depth. Stronger coupling (larger b, smaller a) enhances bandwidth at the cost of reduced return-loss depth, whereas weaker coupling (smaller b, larger a) deepens the minima but narrows the bands. The optimized combination reported in Table 1 achieves balanced coupling, maintaining reflection coefficients below 10 dB across the LTE and WLAN bands with smooth transitions between resonances.

3. Experimental Validation

With the optimized geometry established, a prototype was fabricated and experimentally characterized to validate the simulated design outcomes. A photograph of the prototype (top view) is shown in Figure 6a, while the setup for reflection coefficient measurement is shown in Figure 6b. The total height is less than 10 mm, which is significantly lower than that of a conventional quarter-wavelength monopole. The measurement setup for radiation pattern evaluation is shown in Figure 7, where the antenna under test was placed in an anechoic chamber with a standard horn antenna as the receiving probe.
The simulated and measured reflection coefficients ( S 11 ), obtained using ANSYS HFSS R2021 and a vector network analyzer, are compared in Figure 8a. Good agreement is observed between simulation and measurement. The measured impedance bandwidths, defined by S 11 10 dB, are 28% (1710–2280 MHz) and 6.4% (2410–2570 MHz), fully covering LTE Bands B3/B1 and the 2.4 GHz WLAN band.
The measured and simulated realized gains from 1.6–2.7 GHz are presented in Figure 8b. Both exhibit strong correlation, with a maximum measured gain of 4.46 dBi at 2.57 GHz. The localized gain reduction near 2.35 GHz coincides with the notch region between the two resonant modes in Figure 8a. This frequency lies outside LTE Band 1 (2110–2170 MHz) and corresponds to the transition between the TM 01 -dominated low-band mode (covering LTE B3/B1) and the TM 02 -coupled high-band mode (covering 2.4 GHz WLAN). In this inter-band region, out-of-phase surface currents on the main and parasitic patches produce partial radiation cancellation, leading to the observed dip in gain. Within LTE B1/B3, however, the realized gain remains above 2 dBi and varies only slightly across the sub-bands, maintaining omnidirectional azimuth radiation as shown in Figure 9. This stable sub-band behavior ensures robust IoV and LTE performance at the upper edge of the low band.
Although radiation efficiency was not directly measured, full-wave simulations using FR-4 ( tan δ = 0.02 ) predict efficiencies of approximately 70–85% across the operating bands. Slightly lower efficiency at the upper band (2.4–2.6 GHz) results from increased dielectric and conductor losses, yet the achieved gain and bandwidth confirm that the antenna maintains acceptable performance for low-cost IoV and IoT applications.
Radiation patterns at 1.8, 2.1, and 2.44 GHz—the center frequencies of the target bands—are shown in Figure 9. Measured and simulated co- and cross-polarized traces are overlaid and normalized to the peak co-polar level; the black solid line denotes the measured cross-polarization. The antenna exhibits omnidirectional azimuth patterns ( θ = 90 ) with vertical polarization, consistent with a monopole-like radiator. The azimuthal cross-polar discrimination (XPD) remains above 15 dB across all frequencies, confirming good polarization purity. Similar behavior is observed in elevation, except near nulls where the co-polar reference level is minimal. Overall, the antenna demonstrates stable radiation patterns and sufficient polarization isolation for vehicular and IoT multipath environments.
A comparison with representative omnidirectional and multiband patch antennas is summarized in Table 2. The proposed design achieves the widest low-band fractional bandwidth while maintaining a lower profile on cost-effective FR-4. Compared with the early monopolar patch in [7], the proposed antenna provides substantially broader impedance bandwidth at the low band while retaining an even lower electrical profile. More recent IoV-oriented solutions—such as flexible conformal, logo-integrated, and compact vehicular patches [17,18,19]—offer application-specific advantages but do not simultaneously achieve wide LTE B1/B3 coverage, omnidirectional radiation, sub- 0.06 λ 0 height, and low-cost FR-4 fabrication as demonstrated here.
Although the present work focuses on a single radiator, its measured characteristics indicate suitability for multi-element integration in IoV terminals. The antenna maintains vertical polarization, omnidirectional azimuth radiation, and stable gain across LTE B1/B3 and WLAN bands—features that typically yield low envelope correlation and strong diversity performance in vehicular MIMO arrays [26,27,28]. Comparable compact elements achieve ECC values below 0.1 with inter-element spacing of approximately 0.4–0.6 λ 0 . Comprehensive array characterization, including mutual coupling and ECC measurement, is reserved for future work.

4. Field Validation of LTE Performance for IoV

Following the simulated and chamber measurements that confirmed the antenna’s wide impedance bandwidth, omnidirectional radiation, and stable gain, a field validation was conducted to assess its behavior under realistic vehicular conditions, as emphasized in recent IoV studies [20,21]. An in-house LTE signal meter, implemented on a Raspberry Pi microcontroller, was used for the drive test. The system integrates a Quectel EC25 LTE module via USB and measures key performance indicators (KPIs)—received signal strength indicator (RSSI), reference signal received power (RSRP), reference signal received quality (RSRQ), signal-to-noise ratio (SNR), and data throughput—according to 3GPP definitions [29].
A photograph and block diagram of the signal meter are shown in Figure 10. During the field test, the proposed antenna and a commercial monopole were mounted on the roof of an autonomous vehicle (Figure 11) and connected to the signal meter via coaxial cables for simultaneous performance evaluation. The commercial monopole, operating over 704–960 MHz and 1710–2690 MHz with a 110 mm height, served as a practical reference representative of widely used vehicular and IoT antennas. Its overlapping LTE B1/B3 and 2.4 GHz WLAN coverage provided a relevant baseline for assessing real-world communication quality under identical conditions.
The field-test results, summarized in Figure 12, compare the proposed antenna and the commercial monopole under identical drive-test conditions. Power-related KPIs (RSSI, RSRP, RSRQ, and SNR) were averaged across the route, while data throughput was continuously recorded. The proposed antenna achieved approximately 7 dB and 6 dB higher RSSI and SNR, respectively, with more stable throughput despite being nearly one-tenth the height of the monopole. These results confirm that the low-profile design provides robust link quality and high QoS for vehicular IoV communications.
Table 3 compares the two antennas. Although the commercial monopole exhibits slightly higher peak gain, it occupies over ten times the physical height. The proposed antenna, fabricated on FR-4, achieves competitive gain while maintaining compact dimensions and complete LTE/WLAN coverage, underscoring its practicality for IoV integration.
While this study primarily focused on electromagnetic performance, environmental factors such as temperature variation, humidity, and mechanical vibration may affect impedance stability and efficiency in long-term IoV operation. Future work will include environmental qualification tests and integration of protective features such as a low- ε r radome, hydrophobic coating, and corrosion-resistant materials to ensure durability and performance consistency.

5. Conclusions

This paper presented a multilayer microstrip antenna that combines a circular patch with shorting vias, a coupled ring, and an embedded parasitic patch for Internet-of-Vehicles (IoV) terminals to realize dual-band operation at 1.8 GHz (LTE B3) and 2.4 GHz (WLAN). The prototype, implemented on low-cost FR-4, achieves measured impedance bandwidths of 28% and 6.4% with a compact profile of 0.055 λ 0 .
Performance was validated in two stages. Anechoic-chamber measurements confirmed wideband matching, omnidirectional patterns, and a peak realized gain of 4.46 dBi. Field trials using an in-house Raspberry Pi-based LTE meter further demonstrated improved RSSI, SNR, and throughput versus a commercial vehicular monopole, despite the proposed antenna’s much lower profile.
These results indicate a practical, scalable radiator that combines compact size, robust omnidirectional radiation, and economical fabrication for multiband IoV/V2X connectivity.

Author Contributions

Conceptualization, J.-Y.C.; software, S.B. and E.T.A.; validation, S.B. and E.T.A.; formal analysis, S.B. and E.T.A.; investigation, S.B. and E.T.A.; resources, J.-Y.C.; writing—original draft preparation, S.B. and E.T.A.; writing—review and editing, E.T.A.; visualization, S.B. and E.T.A.; supervision, J.-Y.C.; project administration, J.-Y.C.; funding acquisition, J.-Y.C. All authors have read and agreed to the published version of the manuscript.

Funding

This research was supported by Seoul National University of Science and Technology.

Data Availability Statement

The original contributions presented in this study are included in the article. Further inquiries can be directed to the corresponding author.

Acknowledgments

The authors used ChatGPT (OpenAI and GPT-5) to assist with language refinement. All content was carefully reviewed, edited, and verified by the authors, who take full responsibility for the final manuscript.

Conflicts of Interest

The authors declare no conflicts of interest.

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Figure 1. Geometry of the proposed antenna: (a) top view of the upper layer showing the circular radiating patch ( R patch ) and coupled ring (inner a, outer b) with shorting vias (radius r) on the FR-4 substrate of radius R g ; (b) top view of the embedded parasitic patch layer ( R mid ) between substrates, indicating the via circle of radius d and via diameter 2 r ; (c) side view (thickness exaggerated) showing the stacked FR-4 layers ( h 1 , h 2 ), parasitic patch, shorting vias, and coaxial feed. Clearance gaps around the feed and vias prevent direct contact with the parasitic patch.
Figure 1. Geometry of the proposed antenna: (a) top view of the upper layer showing the circular radiating patch ( R patch ) and coupled ring (inner a, outer b) with shorting vias (radius r) on the FR-4 substrate of radius R g ; (b) top view of the embedded parasitic patch layer ( R mid ) between substrates, indicating the via circle of radius d and via diameter 2 r ; (c) side view (thickness exaggerated) showing the stacked FR-4 layers ( h 1 , h 2 ), parasitic patch, shorting vias, and coaxial feed. Clearance gaps around the feed and vias prevent direct contact with the parasitic patch.
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Figure 2. Simulated surface current at ∼1.8 GHz: (a) magnitude; (b) phase.
Figure 2. Simulated surface current at ∼1.8 GHz: (a) magnitude; (b) phase.
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Figure 3. Input impedance with and without the embedded parasitic patch.
Figure 3. Input impedance with and without the embedded parasitic patch.
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Figure 4. Simulated reflection-coefficient responses showing the influence of the embedded parasitic patch. (a) Increasing h 2 strengthens interlayer coupling, bringing the resonant minima closer and broadening the response but with shallower return-loss depth. (b) Increasing R mid enlarges electrical size and shifts both resonances downward (decreasing R mid shifts them upward). All other parameters are fixed at their optimized values in Table 1.
Figure 4. Simulated reflection-coefficient responses showing the influence of the embedded parasitic patch. (a) Increasing h 2 strengthens interlayer coupling, bringing the resonant minima closer and broadening the response but with shallower return-loss depth. (b) Increasing R mid enlarges electrical size and shifts both resonances downward (decreasing R mid shifts them upward). All other parameters are fixed at their optimized values in Table 1.
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Figure 5. Simulated reflection-coefficient responses showing the influence of the coupled ring on the TM 02 resonance and impedance bandwidth. (a) Increasing the inner radius a (narrowing the ring) shifts both resonances upward; low-band matching improves initially but degrades beyond an intermediate value ( a 34 mm), narrowing the bandwidth. (b) Increasing the outer radius b (widening the ring) shifts both resonances downward and strengthens coupling, broadening the low-band response but yielding shallower minima. Overall, a and b govern a trade-off between bandwidth and return-loss depth. All other parameters are fixed at their optimized values in Table 1.
Figure 5. Simulated reflection-coefficient responses showing the influence of the coupled ring on the TM 02 resonance and impedance bandwidth. (a) Increasing the inner radius a (narrowing the ring) shifts both resonances upward; low-band matching improves initially but degrades beyond an intermediate value ( a 34 mm), narrowing the bandwidth. (b) Increasing the outer radius b (widening the ring) shifts both resonances downward and strengthens coupling, broadening the low-band response but yielding shallower minima. Overall, a and b govern a trade-off between bandwidth and return-loss depth. All other parameters are fixed at their optimized values in Table 1.
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Figure 6. Fabricated prototype and measurement setup: (a) top view of the prototype; (b) S 11 measurement using a vector network analyzer.
Figure 6. Fabricated prototype and measurement setup: (a) top view of the prototype; (b) S 11 measurement using a vector network analyzer.
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Figure 7. Far-field radiation measurement in the anechoic chamber.
Figure 7. Far-field radiation measurement in the anechoic chamber.
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Figure 8. Simulated and measured results of the proposed antenna: (a) reflection coefficient; (b) realized peak gain across 1.6–2.7 GHz.
Figure 8. Simulated and measured results of the proposed antenna: (a) reflection coefficient; (b) realized peak gain across 1.6–2.7 GHz.
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Figure 9. Simulated and measured azimuth (Az) and elevation (El) radiation patterns at 1.8, 2.1, and 2.44 GHz. Co- and cross-polar traces are overlaid and normalized to the peak co-polar level.
Figure 9. Simulated and measured azimuth (Az) and elevation (El) radiation patterns at 1.8, 2.1, and 2.44 GHz. Co- and cross-polar traces are overlaid and normalized to the peak co-polar level.
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Figure 10. Prototype of the developed LTE signal meter used for field validation.
Figure 10. Prototype of the developed LTE signal meter used for field validation.
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Figure 11. Field-test configuration for LTE-IoV validation.
Figure 11. Field-test configuration for LTE-IoV validation.
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Figure 12. Measured field-test results showing RSSI, RSRP, RSRQ, and SNR for the proposed and reference antennas.
Figure 12. Measured field-test results showing RSSI, RSRP, RSRQ, and SNR for the proposed and reference antennas.
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Table 1. Key design parameters of the antenna.
Table 1. Key design parameters of the antenna.
ParameterValue [mm]ParameterValue [mm]
R g 90r0.25
R patch 31d29
R mid 35a32
h 1 9.6b44
h 2 3.2
Table 2. Comparison with representative omnidirectional/multiband patch antennas relevant to IoV applications.
Table 2. Comparison with representative omnidirectional/multiband patch antennas relevant to IoV applications.
Ref.Structure/MethodBands/ServiceProfile ( λ 0 @ f L )BW (%)Peak Gain (dBi)
[7]Triangular monopole-likeNarrowband0.1233.0
[18]Flexible multiband conformal patch (5G)Sub-6 GHz vehiculara209.0
[17]Ultra-thin logo IoVLoRa/GPS/WLAN/5G0.07144.5
[19]Compact dual-band V2VDSRC 5.9 GHz0.08165.2
ProposedRing + vias + embedded parasitic patchLTE B1/B3, WLAN0.05528/6.44.46
BW = impedance bandwidth; IoV = Internet of Vehicles; V2V = Vehicle-to-Vehicle; DSRC = Dedicated Short-Range Communication; λ 0 = free-space wavelength. f L = lowest operating frequency of the antenna. a For conformal antennas such as [18], the effective electrical profile varies with bending and is not directly comparable with rigid monopolar patches.
Table 3. Comparison of antennas evaluated in the field test.
Table 3. Comparison of antennas evaluated in the field test.
AntennaFrequency Range (MHz)Peak Gain (dBi)Physical Height
Monopole704–960, 1710–26905.0110 mm
Proposed1720–2280, 2410–25704.469.6 mm
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Ashong, E.T.; Bang, S.; Chung, J.-Y. Dual-Band Multilayer Patch Antenna for Multiband Internet-of-Vehicles Applications. Electronics 2025, 14, 4400. https://doi.org/10.3390/electronics14224400

AMA Style

Ashong ET, Bang S, Chung J-Y. Dual-Band Multilayer Patch Antenna for Multiband Internet-of-Vehicles Applications. Electronics. 2025; 14(22):4400. https://doi.org/10.3390/electronics14224400

Chicago/Turabian Style

Ashong, Ebenezer Tawiah, Seungwoo Bang, and Jae-Young Chung. 2025. "Dual-Band Multilayer Patch Antenna for Multiband Internet-of-Vehicles Applications" Electronics 14, no. 22: 4400. https://doi.org/10.3390/electronics14224400

APA Style

Ashong, E. T., Bang, S., & Chung, J.-Y. (2025). Dual-Band Multilayer Patch Antenna for Multiband Internet-of-Vehicles Applications. Electronics, 14(22), 4400. https://doi.org/10.3390/electronics14224400

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