Next Article in Journal
Marine Oil Slick Detection Based on Multi-Polarimetric Features Matching Method Using Polarimetric Synthetic Aperture Radar Data
Previous Article in Journal
A Reference Matching-Based Temperature Compensation Method for Ultrasonic Guided Wave Signals
Previous Article in Special Issue
Investigation of a Magnetic Tunnel Junction Based Sensor for the Detection of Defects in Reinforced Concrete at High Lift-Off
 
 
Font Type:
Arial Georgia Verdana
Font Size:
Aa Aa Aa
Line Spacing:
Column Width:
Background:
Article

Novel Electromagnetic Sensors Embedded in Reinforced Concrete Beams for Crack Detection

1
Built Environment and Sustainable Technologies (BEST) Research Institute, Liverpool John Moores University, Liverpool L3 3AF, UK
2
Sensor City Liverpool Limited, 31 Russell Street, Liverpool L3 5LJ, UK
*
Author to whom correspondence should be addressed.
Submission received: 30 September 2019 / Revised: 21 November 2019 / Accepted: 23 November 2019 / Published: 26 November 2019
(This article belongs to the Special Issue Sensors Fusion in Non-Destructive Testing Applications)

Abstract

:
This paper investigates the possibility of applying novel microwave sensors for crack detection in reinforced concrete structures. Initially, a microstrip patch antenna with a split ring resonator (SRR) structure was designed, simulated and fabricated. To evaluate the sensor’s performance, a series of structural tests were carried out and the sensor responses were monitored. Four reinforced concrete (RC) beam specimens, designed according to the European Standards, were tested under three-point bending. The load was applied incrementally to the beams and the static responses were monitored via the use of a load cell, displacement transducers and crack width gauges (Demec studs). In parallel, signal readings from the microwave sensors, which were employed prior to the casting of the concrete and located along the neutral axis at the mid-span of the beam, were recorded at various load increments. The microwave measurements were analysed and compared with those from crack width gauges. A strong linear relationship between the crack propagation and the electromagnetic signal across the full captured spectrum was found, demonstrating the technique’s capability and its potential for further research, offering a reliable, low-cost option for structural health monitoring (SHM).

1. Introduction

The maintenance of structures is essential in various industries, including civil, offshore, marine and transportation engineering. The inspection of structures in order to detect structural damage and to assess the condition of materials is an important part of the maintenance process. Crack formation and propagation due to fatigue or earthquake loading, corrosion in metals and delamination in composites can be addressed via effective maintenance [1]. Effective maintenance not only improves the health and safety standards of a structure, but can also allow for cost savings. Often costs related to continuous monitoring, inspection and maintenance can affect civil infrastructure systems and potentially result in decision-making under uncertain environments. This is particularly common in highways and railway bridges, where an over-stretched transport network is self-evident [2]. Highways England alone has an annual budget of over £1 billion allocated to the maintenance of UK’s strategic highways, which make up approximately 10% of the overall UK road network [3].
Structural health monitoring (SHM) provides continuous feedback regarding the “state” of the constituent materials and structural members. Continuous monitoring over a period of time offers a full history database for a structure, which can be used to provide a prognosis (evaluation of damage, residual life, etc.) [4]. Deterioration owing to usage, environmental conditions and accidents can be monitored and utilised in order to assess whether the condition of a structure is in accordance with design standard limits and requirements.
In recent years, different SHM technologies have been investigated aiming to minimise the costs related to damage assessment and maintenance works, while securing the reliability of the structural performance. Traditional sensor technologies (e.g., strain sensors, displacement transducers, accelerometers, etc.) can be utilized, along with traditional visual inspection and damage detection, for structures subjected to various load conditions, such as earthquakes, wind and fatigue loading. In addition to traditional sensors, new measuring approaches (e.g., GPS, terrestrial laser scanning, vision-based systems, etc.) have been applied for structural health monitoring purposes [5]. Non-destructive evaluation (NDE) can be time-consuming and expensive, and access is not always possible [6]. Both wired and wireless sensor technologies are available, each of them having their own advantages and limitations, while the main concern should always be obtaining high accuracy data. Existing wired sensor techniques can be expensive in terms of additional costs and the space required for cable installation, while wireless sensors require due consideration for the power supply.
Aiming to complement existing sensing technologies for SHM, the present study investigates the potential of using microwave sensors for crack detection in concrete structures. Recently, electromagnetic sensors have received interest as a method to monitor and predict the excess moisture content in concrete structures due to exposure [7,8,9]. The use of microwave technology offers low cost, low profile flexibility in the design and the adaptation of sensors. This study will demonstrate a potential sensor solution for the detection and prediction of crack propagation in reinforced concrete (RC) beams. Note that wired sensors are examined herein, whereas wireless microwave sensor technologies are planned to be studied in a future research programme, in which energy harvesting systems will be considered as a power source for the sensors.

2. Design of the Experiments

An experimental programme was designed and carried out in order to investigate the accuracy of the microwave sensing technology in predicting the crack formation in reinforced concrete beams. The current section provides details regarding the design of the RC beams (Section 2.1) and of the microwave sensors (Section 2.2).

2.1. Design of the Beams

Four RC beams were designed in accordance with Eurocode 2 [10] to be used for the experimental set-up of this study. The total length of the beams was 1400 mm and their cross-section was rectangular with dimensions of 200 mm × 200 mm. The beams were subjected to a vertical design load equal to a maximum of 100 kN based on the capacity of the actuator and associated load cell. Grade C40/50 was used for the concrete and steel grade S500 (Scimitar Steels, Liverpool, UK) for the reinforcement. The cover to the reinforcement for bond and durability was 30 mm. Steel bars with diameters of 20 mm and 8 mm were used for the longitudinal reinforcement and the hanger bars of the beams, respectively. Finally, shear links (Scimitar Steels, Liverpool, UK) with diameter 8 mm with 100 mm spacing’s were used for the shear reinforcement of the beams. The design of the beams is shown in Figure 1. The microwave sensor (Liverpool John Moores University, Liverpool, UK) was placed 100 mm from the bottom of the concrete specimen in order to capture the crack propagation in the tensile zone just below the neutral axis.

2.2. Design of the Microwave Sensors

In this study, a microstrip patch antenna with a split ring resonator (SRR) structure was designed, simulated and fabricated as a potential microwave sensing technique. SRR structures have been utilised to realise microwave resonators, filters and microwave antennas [11], and have been used for various applications, namely chemical sensors [12], gas sensors [13], crack detection sensors [14], angle sensors [14], alignment and position sensors [15], displacement sensors [16] and microwave imaging sensors [17].
Figure 2 presents (a) a traditional circular patch antenna resonating at 10.8 GHz (30 mm in diameter) and (b) a traditional circular patch antenna with an additional SRR structure, which were modelled and simulated using the High Frequency Structural Simulation software tool (HFSS) (ANSYS Inc., Canonsburg, PA, USA) [18]. SRR structures offer an improved performance compared to traditionally designed microstrip patch antennas as they allow for miniaturised antenna dimensions and/or multiband operations, i.e., multiple resonant frequencies [19]. In this study, the SRR structure was used to provide multiple resonant frequencies between 1 to 10 GHz, which provided more details about the concrete. In addition, the use of SRR shifted the resonant frequencies to lower frequency ranges, which in turn increased the penetration capability of the antenna, while preventing disturbances in the concrete structure by keeping the dimensions of the antenna small. Figure 2c demonstrates the comparison between the resonant frequency response of the traditional circular patch antenna (Figure 2a) and the proposed SRR structure (Figure 2b), which resonated at multiple frequencies below 10.8 GHz, namely 3.4 GHz, 4.7 GHz, 5.7 GHz, 8.7 GHz and 10.6 GHz with a return loss below −10 dB. The dimensions (in mm) of the proposed antenna are presented in Figure 2d.
As the sensor was aimed to be embedded into the concrete, a concrete sample was modelled and simulated using HFSS. According to Piladaeng [20], the concrete dielectric constant for a 7-day-old specimen is between ε′ = 4 and ε′ = 5.5, conductivity (S/m) in the range between 0.18 and 0.25 and dielectric loss factor between ε″ = 0.45 and ε″ = 0.65. Therefore, in this study, the concrete specimen was modelled using ε′ = 5.5, conductivity (S/m) of 0.25 and a loss factor of ε″ = 0.5. The model of the concrete sample was simulated with various crack widths (0.0 mm, 0.1 mm, 0.2 mm, 0.3 mm, 0.4 mm, 0.5 mm and 0.6 mm) and with the SRR antenna underneath the sample (see Figure 3). The simulation was carried out seven times, including the case of an uncracked concrete sample. The simulation measurements (S11, reflection coefficient) were realised in the frequency range of 1 to 10 GHz and with 4000 sweep points.
The simulation results are shown in Figure 4a, which mainly demonstrates a change in the amplitude of the reflected signal (S11). The full simulated frequency spectrum (1–10 GHz, 4000 sweep points) was scanned across using a bespoke LabVIEW (v2013) program (National Instruments, Austin, TX, USA) aiming to identify a linear relationship between the sensor response (S11) and the crack width (mm). Figure 4b presents the linear fit across the full simulated spectrum and the crack width (mm). The strongest linear correlation can be observed around 6.2 GHz. Figure 4c shows the linear relationship between S11 and the crack width (mm) changed at 6.2 GHz, with R2 = 0.91. The figure demonstrates that S11 increased as the crack width grew, i.e., less energy/power was absorbed by the concrete sample as there was an opening air gap, which changed the penetration of the electromagnetic (EM) signal, as well as changing the reflection of the signal. Based on these simulation results and previous work [8], the investigation was taken forward, i.e., to the fabrication of the sensors and subsequently to the experimental testing.
The proposed antennas were fabricated on a double-sided 1.6 mm FR4 PCB (Printed Circuit Board) sheet using an LPKF ProtoMat D104 unit (see Figure 5). Then the SMA connectors were inserted through the probe-fed hole of the antennas and soldered on the patch (top layer) and the ground plane (bottom layer) of the antennas.

3. Experimental Programme

In order to evaluate the capability of the microwave sensors to predict the crack formation, four reinforced concrete beams, in line with the design described in Section 2.1, were tested under three-point loading. The experimental programme was carried out at the Henry Cotton Laboratory of Liverpool John Moores University. The preparation of the specimens, including the attached instrumentation, is described in Section 3.1, while Section 3.2 provides information on the test set-up and the process utilised.

3.1. Specimens’ Preparation and Instrumentation

Initially, the formwork for the concrete beams was constructed and the longitudinal steel reinforcement bars and the shear links were fabricated. Upon careful treatment of the surfaces, six strain gauges (Techni Measure - Sensors & Transducers, Doncaster, UK) were attached at the tensile reinforcement bars of the specimens. In particular, the strain gauges were adhered to the bottom and the top of a tensile reinforcement bars and at the mid and quarter span. A microwave sensor was located at the neutral axis (NA) of the cross-section mid-span of each specimen, where negligible longitudinal stresses and strains were expected.
Following this, the concrete mix was prepared in accordance with the BRE (Building Research Establishment) concrete mix design [21], which gave a 28-day compressive strength equal to 57 N/mm2. Crushed limestone aggregates (Beers Timber and Building Suppliers, Liverpool, UK) (20 mm down), sand (Mersey Grit) (Beers Timber and Building Suppliers, Liverpool, UK), OPC Type II (Travis Perkins, Liverpool, UK) and a water-to-cement ratio equal to 0.45 were used. A slump test was also performed to ensure that the mix was in accordance with the design guidelines. The beams were cast and the concrete was vibrated using a poker vibrator according to the design guidelines [21]. Note that the microwave sensor was embedded into concrete and the accuracy of its location was regularly checked during casting.
Concrete cubes with dimensions of 150 × 150 × 150 mm were also prepared in order to check the compressive strength of the concrete at 7 and 28 days.
The specimens’ preparation, including the details of the attached sensors and gauges along with the concrete casting, are shown in Figure 6.
Upon demoulding, the beams were painted on both lateral sides in order to make the crack formation and propagation detectable. Demec studs were applied at the central tension region of the beams in order to monitor the crack opening within the most heavily stressed areas. Four stud sets were bonded on the concrete’s surface at a set horizontal distance of 50 mm on either side of the centreline and at vertical distances equal to 80 mm, 60 mm, 40 mm and 20 mm from the beam’s neutral axis (NA).

3.2. Experimental Set-Up

Having attached the required instrumentation (i.e., strain gauges attached on the tensile reinforcement bars, microwave sensors embedded in the concrete beam and Demec studs glued on the concrete beam’s surface), the specimens were cured for 7 days and were then located at the test rig for the experimental investigation. The beams spanned 1200 mm with an overhang of 100 mm from both sides of the supports. Simply-supported conditions were achieved with the use of roller supports. A calibrated hydraulic 100 kN load actuator was used for the load application. A constant slow loading rate, excluding any dynamic effects, was implemented, while a load cell was used for the recording of the load increments. Two strain gauge type displacement transducers (DTs) were placed at the mid-span in order to measure the vertical deflections of the specimens during testing. Synchronised data acquisition systems were used for the structural response measurements. The experimental set-up, along with the employed instrumentation, are shown in Figure 7 and Figure 8. The cables shown in Figure 8 present the current available instrumentation for the structural response monitoring via strain gauges, Linear Variable Displacement Transducers (LVDTs) and the load cell. The microwave sensor in this study was connected using a single coaxial cable, which will be eliminated in the future.

4. Results

4.1. Results on the Structural Response

The structural response for all specimens is shown in Figure 9, where the applied load is plotted against the average of the two DTs for the mid-span displacement. As shown, the load versus vertical displacement response of the beams were linear, and very similar for all specimens. The crack width recordings for the specimens are presented in Figure 10, where in all cases, the crack opening increased for higher loads. Additionally, the observed crack width openings were more pronounced for a vertical distance of 80 mm from the neutral axis, where the tensile stresses were higher, compared to those of smaller vertical distances from the neutral axis. The strain gauges measurements were only used to further validate the structural response of the beam and will not be further utilised in this paper.
For each of the specimens, a concrete cube compressive strength test was performed. The average compressive strength was 49.92 N/mm2 and 57.15 N/mm2 for the 7- and 28-day tests, respectively. In Figure 11, a typical cracked specimen at the end of the testing is depicted. The crack evolution and propagation was marked during testing. A symmetrical crack pattern, as anticipated for reinforced concrete beams under pure flexure, was observed in most cases. It is noteworthy that even though the specimens did not reach their failure load, the recorded response up to 100 kN allowed for the comparison between the Demec studs and the new sensor signal values, thus serving the scope of this study, as will be discussed in Section 4.2.

4.2. Results for the Microwave Sensor

The microwave measurements were provided by the S-parameter (i.e., S11, reflection coefficient), namely complex data (real and imaginary data of the signal) and magnitude from the Vector Network Analyser (VNA) (Rohde & Schwarz, Munich, Germany). The data was captured via a bespoke LabVIEW program on a laptop connected to the VNA. The data acquisition took place at each load increment. The recorded measurements were in the 1 to 10 GHz frequency range using the maximum number of sweep points available (4000). The captured results were analysed against the crack width of the samples in order to determine a relationship between the changes in the EM response and the crack width. Figure 12 demonstrates a linear relationship between the crack propagation and the EM signal across the fully captured spectrum (1–10 GHz). The strongest linear relationship was identified between the 2.8 GHz and 3 GHz frequency range.
The EM response from all four specimens demonstrated a strong linear relationship against the crack width with R2 above 0.90 for specimens 1, 2, 3 and 4 (Figure 13). The slopes of the linear regression lines for the four specimens at 20 mm, 40 mm, 60 mm and 80 mm distances from NA (Figure 14) demonstrate a similar response for specimens 1, 2 and 4, namely the slope increased with the increase of the distance from the NA. For specimen 3, the crack width at 20 mm and 60 mm distances from NA were found to be similar (Figure 13c), leading to a slope decrease from 40 mm to 60 mm, as shown in Figure 14. In addition, the sensor response varied between the specimens owing to the inconsistency of the crack patterns on each specimen. Note also that only small changes (crack widths less than 1 mm) were considered for this study. Nevertheless, the sensor was able to determine these small changes in the structure, i.e., it demonstrated a potential to detect anomalies in RC structures, which could be used as an indicator of a structural failure. Further study is required for the proposed technique, namely more samples with various crack widths and patterns in order to obtain necessary parameters/data for the analysis or the potential implementation of machine learning algorithms.

5. Conclusions

Aiming to assess microwave sensing technology as a means of structural health monitoring, four reinforced concrete beams were tested under three-point loading in the Henry Cotton Laboratory of Liverpool John Moores University. In addition to the commonly implemented instrumentation in structural testing (i.e., load cells, displacement transducers, Demec studs, etc.), a novel microwave sensor, specifically designed for this application, was inserted into each beam’s reinforcement cage before the concrete’s casting. In order to allow for a reduced size of the sensor and to shift the resonant frequencies to lower frequency ranges, hence increasing the antenna’s penetration capability, a microstrip patch antenna with an SRR structure was designed and subsequently fabricated.
During the load application, both the structural performance and the signal measurements were incrementally recorded. As anticipated, a linear load–displacement structural response was found to be very similar for all specimens. The microwave data sets, which were captured via a bespoke LabVIEW program, were provided by the S11 reflection coefficient, and were within the 1–10 GHz frequency range. For the largest anticipated tensile crack at the mid-span of the beam, the readings for the crack width gauges and the sensors were processed and compared. A strong linear relationship with R2 values very close to unity were observed. The variance on the sensor response was related to the different crack patterns observed in each specimen. The present study considered crack widths below 1 mm and thus only small changes in the concrete structure. It is noteworthy that the sensor was able to detect these small changes in the concrete’s structure, demonstrating that the proposed technique could be further studied in order to detect cracking in RC structures. Further investigation is required to obtain more data for various crack patterns and widths, thus enhancing the measurements’ repeatability and reliability and allowing for the technique’s validation.
Future studies could also investigate the possibility of insulating/sealing the antennas to avoid direct contact with the concrete, which might change the properties of the antenna owing to the physical and chemical properties of the concrete mixture. The extra layer could protect antennas from possible corrosion/oxidation of the copper part of the antenna. Finally, additional sensors (i.e., moisture and temperature) could be added to provide additional variables for the sensor algorithm, which could further improve crack detection.

Author Contributions

M.G., M.M., G.S.K., W.A. and P.K. organised the conceptualisation of the idea and the methodology employed in this paper. Following that, P.K., M.G. and M.M. worked on the software, data validation and formal analysis for the investigation. K.H., G.S.K., W.A. and M.G. worked on the concrete samples’ preparation. M.M. and M.G. undertook data acquisition. The original writing and draft preparation were carried out by M.G., M.M. and P.K., and W.A. carried out the review and editing. The project was supervised by P.K.

Funding

This research was funded by Liverpool John Moores University under the Pump Priming Award Scheme 2019.

Acknowledgments

The authors of this paper would like to thank Sensor City Liverpool Limited for providing access to their lab facilities to print the electromagnetic sensors.

Conflicts of Interest

The authors declare no conflict of interest.

References

  1. Staszewski, W. Structural Health Monitoring Using Guided Ultrasonic Waves. In Advances in Smart Technologies in Structural Engineering; Springer: Berlin/Heidelberg, Germany, 2004; pp. 117–162. [Google Scholar]
  2. Rafiq, M.I. Structural health monitoring for maintenance management of deteriorating structures: Current practice and state of the art. In Proceedings of the 2nd International and 6th National Conference on Earthquake & Structures, Kerman, Iran, 14–15 October 2015; pp. 1–19. [Google Scholar]
  3. Highways Agency. Highways Agency Business Plan 2014-15; Highways Agency: London, UK, 2014. [Google Scholar]
  4. Balageas, D.; Fritzen, C.P.; Güemes, A. Structural Health Monitoring; ISTE: Newport Beach, CA, USA, 2006. [Google Scholar]
  5. Park, H.S.; Shin, Y.; Choi, S.W.; Kim, Y. An Integrative Structural Health Monitoring System for the Local/Global Responses of a Large-Scale Irregular Building under Construction. Sensors 2013, 13, 9085–9103. [Google Scholar] [CrossRef]
  6. Chang, P.C.; Flatau, A.; Liu, S.C. Review Paper: Health Monitoring of Civil Infrastructure. Struct. Heal. Monit. 2003, 2, 257–267. [Google Scholar] [CrossRef]
  7. Kot, P.; Ali, A.S.; Shaw, A.; Riley, M.; Alias, A. The application of electromagnetic waves in monitoring water infiltration on concrete flat roof: The case of Malaysia. Constr. Build. Mater. 2016, 122, 435–445. [Google Scholar] [CrossRef]
  8. Teng, K.H.; Kot, P.; Muradov, M.; Shaw, A.; Hashim, K.; Gkantou, M.; Al-Shamma’a, A. Embedded Smart Antenna for Non-Destructive Testing and Evaluation (NDT & E) of Moisture Content and Deterioration in Concrete. Sensors 2019, 19, 547. [Google Scholar]
  9. Kot, P.; Shaw, A.; Riley, M.; Ali, A.S.; Cotgrave, A. The Feasibility of Using Electromagnetic Waves in Determining Membrane Failure through Concrete. Int. J. Civ. Eng. 2017, 15, 355–362. [Google Scholar] [CrossRef]
  10. Eurocode 2: Design of Concrete Structures–Part 1-1: General Rules and Rules for Buildings; EN 1992-1-1; European Committee for Standardisation (CEN): Brussels, Belgium, 2004.
  11. Salim, A.; Sungjoon, L. Complementary split-ring resonator-loaded microfluidic ethanol chemical sensor. Sensors 2016, 16, 1802. [Google Scholar] [CrossRef] [PubMed]
  12. Rawat, V.; Dhobale, S.; Kale, S.N. Ultra-fast selective sensing of ethanol and petrol using microwave-range metamaterial complementary split-ring resonators. J. Appl. Phys. 2014, 116, 164106. [Google Scholar] [CrossRef]
  13. Barochi, G.; Rossignol, J.; Bouvet, M. Development of microwave gas sensors. Sens. Actuators B Chem. 2011, 157, 374–379. [Google Scholar] [CrossRef]
  14. Albishi, A.; Ramahi, O. Detection of surface and subsurface cracks in metallic and non-metallic materials using a complementary split-ring resonator. Sensors 2014, 14, 19354–19370. [Google Scholar] [CrossRef] [PubMed]
  15. Naqui, J.; Durán-Sindreu, M.; Martín, F. Novel sensors based on the symmetry properties of split ring resonators (SRRs). Sensors 2011, 11, 7545–7553. [Google Scholar] [CrossRef] [PubMed]
  16. Horestani, A.K.; Fumeaux, C.; Al-Sarawi, S.F.; Abbott, D. Displacement sensor based on diamond-shaped tapered split ring resonator. IEEE Sens. J. 2014, 13, 1153–1160. [Google Scholar] [CrossRef]
  17. Islam, M.; Islam, M.; Samsuzzaman, M.; Faruque, M.; Misran, N. A negative index metamaterial-inspired UWB antenna with an integration of complementary SRR and CLS unit cells for microwave imaging sensor applications. Sensors 2015, 15, 11601–11627. [Google Scholar] [CrossRef] [PubMed]
  18. Ansys. 3D Electromagnetic Field Simulator for RF and Wireless Design. 2019. Available online: https://www.ansys.com/products/electronics/ansys-hfss (accessed on 1 November 2019).
  19. Kaushal, D.; Shanmuganantham, T. Parametric enhancement of a novel microstrip patch antenna using Circular SRR Loaded Fractal Geometry. Alex. Eng. J. 2018, 57, 2551–2557. [Google Scholar] [CrossRef]
  20. Piladaeng, N.; Angkawisittpan, N.; Homwuttiwong, S. Determination of relationship between dielectric properties, compressive strength, and age of concrete with rice husk ash using planar coaxial probe. Meas. Sci. Rev. 2016, 16, 14–20. [Google Scholar] [CrossRef] [Green Version]
  21. Teychenné, D.C.; Franklin, R.E.; Erntroy, H.C.; Hobbs, D.W.; Marsh, B.K. Design of Normal Concrete Mixes; H.M.S.O. [for the] Building Research Establishment [and the] Transport and Road Research Laboratory: London, UK, 1975. [Google Scholar]
Figure 1. Design details of the beams used for the experimental set-up in this study: (a) Longitudinal and shear reinforcement; (b) Cross-section of the beam.
Figure 1. Design details of the beams used for the experimental set-up in this study: (a) Longitudinal and shear reinforcement; (b) Cross-section of the beam.
Sensors 19 05175 g001aSensors 19 05175 g001b
Figure 2. Simulated (a) original antenna, (b) antenna with split ring resonators (SRRs), (c) the S11 simulation results and (d) the design of the proposed antenna with dimensions (mm).
Figure 2. Simulated (a) original antenna, (b) antenna with split ring resonators (SRRs), (c) the S11 simulation results and (d) the design of the proposed antenna with dimensions (mm).
Sensors 19 05175 g002
Figure 3. HFSS simulation of the proposed antenna and the concrete sample: (a) 3D view and (b) top view.
Figure 3. HFSS simulation of the proposed antenna and the concrete sample: (a) 3D view and (b) top view.
Sensors 19 05175 g003
Figure 4. Simulated (a) raw data, (b) R2 values across the full spectrum (1–10 GHz) and (c) linear fit between the S11 change and crack width at 6.2 GHz, with R2 = 0.91.
Figure 4. Simulated (a) raw data, (b) R2 values across the full spectrum (1–10 GHz) and (c) linear fit between the S11 change and crack width at 6.2 GHz, with R2 = 0.91.
Sensors 19 05175 g004aSensors 19 05175 g004b
Figure 5. Fabrication of the antennas on a LPKF ProtoMat D104.
Figure 5. Fabrication of the antennas on a LPKF ProtoMat D104.
Sensors 19 05175 g005
Figure 6. Specimens’ preparation.
Figure 6. Specimens’ preparation.
Sensors 19 05175 g006
Figure 7. Experimental set-up.
Figure 7. Experimental set-up.
Sensors 19 05175 g007
Figure 8. Photos from the experimental set-up and instrumentation. LVDTs: ???
Figure 8. Photos from the experimental set-up and instrumentation. LVDTs: ???
Sensors 19 05175 g008
Figure 9. Load versus average mid-span displacement graph of all test specimens.
Figure 9. Load versus average mid-span displacement graph of all test specimens.
Sensors 19 05175 g009
Figure 10. Load versus crack width opening.
Figure 10. Load versus crack width opening.
Sensors 19 05175 g010
Figure 11. Typical cracked specimen at the maximum applied load.
Figure 11. Typical cracked specimen at the maximum applied load.
Sensors 19 05175 g011
Figure 12. Linear fit between the crack width and electromagnetic (EM) response for all four specimens across the 1–10 GHz frequency spectrum.
Figure 12. Linear fit between the crack width and electromagnetic (EM) response for all four specimens across the 1–10 GHz frequency spectrum.
Sensors 19 05175 g012
Figure 13. Linear correlation between the crack width and sensor response at 2.9 GHz.
Figure 13. Linear correlation between the crack width and sensor response at 2.9 GHz.
Sensors 19 05175 g013
Figure 14. Slopes of linear regression lines for four specimens at 20 mm, 40 mm, 60 mm and 80 mm distances from the NA.
Figure 14. Slopes of linear regression lines for four specimens at 20 mm, 40 mm, 60 mm and 80 mm distances from the NA.
Sensors 19 05175 g014

Share and Cite

MDPI and ACS Style

Gkantou, M.; Muradov, M.; Kamaris, G.S.; Hashim, K.; Atherton, W.; Kot, P. Novel Electromagnetic Sensors Embedded in Reinforced Concrete Beams for Crack Detection. Sensors 2019, 19, 5175. https://0-doi-org.brum.beds.ac.uk/10.3390/s19235175

AMA Style

Gkantou M, Muradov M, Kamaris GS, Hashim K, Atherton W, Kot P. Novel Electromagnetic Sensors Embedded in Reinforced Concrete Beams for Crack Detection. Sensors. 2019; 19(23):5175. https://0-doi-org.brum.beds.ac.uk/10.3390/s19235175

Chicago/Turabian Style

Gkantou, Michaela, Magomed Muradov, George S. Kamaris, Khalid Hashim, William Atherton, and Patryk Kot. 2019. "Novel Electromagnetic Sensors Embedded in Reinforced Concrete Beams for Crack Detection" Sensors 19, no. 23: 5175. https://0-doi-org.brum.beds.ac.uk/10.3390/s19235175

Note that from the first issue of 2016, this journal uses article numbers instead of page numbers. See further details here.

Article Metrics

Back to TopTop