1. INTRODUCTION
⌅Nondestructive
test techniques (NDT) represent a variety of techniques like flux
leakage method, building radar, radiographic methods, acoustic methods
and sonic methods used to investigate and assess materials and
structures. Nondestructive testing has an important place in determining
the strength properties of natural stone and concrete used in modern
construction and historical buildings (1-101.
Karakuş, M.; Tütmez, B. (2006) Fuzzy and multiple regression modelling
for evaluation of intact rock strength based on point load, Schmidt
hammer and sonic velocity. Rock Mech. Rock Eng. 39 [1], 45-57. https://doi.org/10.1007/s00603-005-0050-y.
2.
Vasconcelos, G.; Lourenço, P.B.; Alves, C.A.; Pamplona, J. (2007)
Prediction of the mechanical properties of granites by ultrasonic pulse
velocity and Schmidt hammer hardness. North American Masonry Conference
June 3-7 Missouri USA.
3. Sharma, P.K.; Singh, T.N. (2008) A
correlation between P-wave velocity, impact strength index, slake
durability index and uniaxial compressive strength. B. Eng. Geol. Environ. 67 [1], 17-22. https://doi.org/10.1007/s10064-007-0109-y.
4.
Kurtuluş, C.; Irmak, T.S.; Sertçelik, I. (2010) Physical and mechanical
properties of Gokceada: Imbros (NE Aegean Sea) island andesites. B. Eng. Geol. Environ. 69 [2], 321-324. https://doi.org/10.1007/s10064-010-0270-6.
5.
Sharma, P.K.; Khandelwal, M.; Singh, T.N. (2011) A correlation between
Schmidt hammer rebound numbers with impact Strength index, slake
durability index and P-wave velocity. Int. J. Earth Sci. 100 [1], 189-195. https://doi.org/10.1007/s00531-009-0506-5.
6.
Fort, R.; de Buergo, M.A.; Perez-Monserrat, E.M. (2013) Non-destructive
testing for the assessment of granite decay in heritage structures
compared to quarry stone. Int. J. Rock. Mech. Min. 61, 296-305. https://doi.org/10.1016/j.ijrmms.2012.12.048.
7. Pamuk, E.; Büyüksaraç, A. (2017) Investigation of strength characteristics of natural Stones in Ürgüp (Nevşehir/Turkey). Bitlis Eren Univ. J. Sci. Technol. 7 [2], 74-79. https://doi.org/10.17678/beuscitech.305653.
8. Işık, E.; Bakış, A.; Akıllı, A.; Hattaoğlu, F. (2015) Usability of ahlat stone as aggregate in reactive powder concrete. Int. J. App. Sci. Eng. Res. 4 [4], 507-514.
9.
Işık, E.; Büyüksaraç, A.; Avşar, E.; Kuluöztürk, M.F.; Günay, M. (2020)
Characteristics and properties of Bitlis ignimbrites and their
environmental implications. Mater. Construcc. 70 [338], e214. https://doi.org/10.3989/mc.2020.06519.
10.
Karahan, Ş.; Büyüksaraç, A.; Işık, E. (2020) The Relationship between
concrete strengths obtained by destructive and non-destructive methods. Iran. J. Sci. Technol. Transact. Civ. Engineer. 44, 91-105. https://doi.org/10.1007/s40996-019-00334-3.
).
Contrary to this, some test techniques cause damage to the structure
and as a result only controlled numbers of test samples can be taken.
Nondestructive test systems are generally used to identify the material
properties or to show the presence of abnormalities in a material. In
other words, the technique used determines the physical properties of
the material or changes occurring in the physical properties. There are a
variety of electromagnetic NDT techniques available to assess metallic
materials and assemblies. These include magnetic flux leakage (MFL)
methods, puls magnetic flux leakage (PMFL) method, eddy current (EC)
method, puls eddy current (PEC) method, magnetic particle test (MPT)
method, etc. These methods examine the interaction between conductive
samples to be investigated and electromagnetic fields (1111.
Okolo, K.W. (2018) Modelling and experimental investigation of magnetic
flux leakage distribution for hairline crack detection and
characterization. Wolfson Centre for Magnetics School of Engineering,
Cardiff University. (PhD Thesis).
). NDT methods come
to the agenda for investigation of reinforced concrete structures
without harming the region to be researched. During building
inspections, it is important to identify the steel elements, grout
thickness, diameter and corrosion status of reinforcement within the
columns and walls of a building. NDT are performed without causing any
disruption to the structure and ensure safe use of engineering
structures. There are a variety of NDT available to identify steel
elements within concrete and to assess concrete structures.
MFL
is commonly used to detect elements made of ferromagnetic material
without damaging. It is a nondestructive test method that was firstly
developed to investigate concrete bridges at the end of the 1970s and
has been further developed through the years. Later it was used to
identify surface and subsurface defects in structures like underground
pipelines, floors of petrol storage tanks and railway lines etc. and
additionally to identify defects in symmetric components like steel
rods, pipes and tubes (1212. Rao, B.P.C. (2012) Magnetic flux leakage technique. J. Non Destr. Test. Eval. 11 [3], 7-17.
).
The MFL method was investigated by many researchers and successful results were obtained. Li et al. (1313. Li, L.; Huang, S.; Zheng, P.; Shi, K. (2002) Evaluation of surface cracks using magnetic flux leakage testing. J. Mater. Sci. Technol. 18 [4], 319-321.
)
discussed results for magnetic field distribution characteristics of
finite elements (FEM) of fractured surfaces with a variety of widths
(fracture depth 0.2 mm, width interval 0.02-1.00 mm). In conclusion,
they stated that the fracture width and distance between surface and
sensor will affect the signal. Additionally, they considered effects on
peak-peak values for normal components of distance parameters between
different surfaces and sensor in the magnetic flux leakage test. They
stated the effect may be applied to assess surface breaking cracks with
different widths and depths and that using alternative current (AC)
field magnetization provided an idea to correct the tips of narrow sharp
fractures. Ramirez et al. (1414.
Ramirez, A.R.; Mason, J.S.D.; Pearson, N. (2009) Experimental study to
differentiate between top and bottom defects for MFL tank floor
inspections. NDT&E Intern. 42 [1], 16-21. https://doi.org/10.1016/j.ndteint.2008.08.005.
)
performed specially designed experimental studies to assess the ability
of an MFL-based machine to distinguish defects in the top and bottom of
tanks. Some studies consider this type of top and bottom classification
to be possible, but in this study, the experimental results designed
for this purpose showed that this type of differentiation between
signals from upper and lower defects may not be possible using standard
MFL-based techniques. Sun and Kang (1515. Sun, Y.; Kang, Y. (2010) A new MFL principle and method based on near-zero background magnetic field. NDT&E Intern. 43 [4], 348-353. https://doi.org/10.1016/j.ndteint.2010.01.005.
)
proposed a new MFL principle and technique based on creating a
background magnetic field near to zero for the first time based on
magnetic compression effect (MCE) analysis in available MFL
applications. They determined the feasibility of the proposed principle
with simulations and experiments. They determined that contact probes
applying the proposed MFL principle may prevent severe wear and could be
applied to pipes at high temperatures. Tsukada et al. (1616.
Tsukada, K.; Yoshioka, M.; Kiwa; T.; Hirano, Y. (2011) A magnetic flux
leakage method using a magnetoresistive sensor for non destructive
evaluation of spot welds. NDT&E Intern. 44 [1], 101-105. https://doi.org/10.1016/j.ndteint.2010.09.012.
)
used magnetic flux leakage studies to nondestructively assess spot
welding and compared the sturdiness of spot welding, commonly used to
join metal plates, with destructive and nondestructive methods. They
developed an MFL system using a magnetic resistance (MR) sensor to
examine spot welds without destruction. In the study they determined a
linear correlation between the nondestructive magnetic flux leakage test
and destructive shear tests. Rao (1212. Rao, B.P.C. (2012) Magnetic flux leakage technique. J. Non Destr. Test. Eval. 11 [3], 7-17.
)
explained the operating principle, capability, applications and
limitations of the MFL technique to detect defects in ferromagnetic
objects. The topics related to parameters affecting MFL signals and
theoretical modelling with analyses were discussed. They emphasized the
latest developments in MFL technology for automatic detection and
determining the dimensions of defects. Göktepe and Perin (1717. Göktepe, M.; Perin, D. (2012) Inspection of rebars in concrete blocks. Int. J. Appl. Electromagn. Mech. 38 [2-3], 65-78. https://doi.org/10.3233/JAE-2012-1409.
)
aimed to image steel elements within reinforced concrete structures
using the MFL technique. The method used was completed nondestructively.
Within the scope of the study, the parallel and perpendicular
measurements were compared and they identified that the practical
perpendicular measurement provided much better results. Loa and Nakagawa
(1818.
Loa, C.C.H.; Nakagawa, N. (2013) Evaluation of eddy current and
magnetic techniques for inspecting rebars in bridge barrierrails. AIP Conf. Proc. 1511, 1371. https://doi.org/10.1063/1.4789202.
)
investigated the EC and MFL methods to identify corrosion damage in
rebar connecting concrete barrier rails with road decks in bridge
structures. These two methods were applied to rebar with and without
artificial defects causing 25% and 50% material loss and results were
compared. In conclusion, both techniques were determined to easily
identify defects from 2.5” (63.5 mm) distance. Shi et al. (1919. Shi, Y.; Zhang, C.; Li, R.; Cai, M.; Jia, G. (2015) Theory and application of magnetic flux leakage pipeline detection. Sensors. 15 [2], 31036-31055. https://doi.org/10.3390/s151229845.
)
performed studies about the theory and application of the MLF method to
determine pipe lines. They discussed quantitative analysis of the MFL
method as the key point in detecting magnetic flux leakage signals.
Additionally, they analyzed the advantages and disadvantages of
different detection methods. Wu et al. (2020.
Wu, D.; Liu, Z.; Wang, X.; Su, L. (2017) Composite magnetic flux leakage
detection method for pipelines using alternating magnetic field
excitation. NDT&E Intern. 91, 148-155. https://doi.org/10.1016/j.ndteint.2017.07.002.
)
proposed a new composite MFL method using alternative magnetic field
induction to detect cracks in pipelines. The results of the study showed
that two vertical detection signals could be differentiated with a
simple low-pass filter and thus they stated that only one scan to
overcome the blind spot problem in traditional MFL detectors could
obtain flaw characteristics in axial and environmental directions. Okolo
(1111.
Okolo, K.W. (2018) Modelling and experimental investigation of magnetic
flux leakage distribution for hairline crack detection and
characterization. Wolfson Centre for Magnetics School of Engineering,
Cardiff University. (PhD Thesis).
) completed magnetic
flux leakage distribution modeling for detection and characterization of
hairline cracks and performed experimental studies. The results of this
study determined the detection and characterization of MFL distribution
caused by hairline cracks with rectangular surface and distant surface.
Wilcke et al. (2121.
Wilcke, M.; Walther, A.; Szielasko, K.; Youssef, S. (2018) The MFL
technique - Basic application for PT cable break detection in concrete
structures. MATEC Web of Conferences 199, 06013 ICCRRR 2018.
)
studied simple applications of the magnetic flux leakage technique to
concrete structures. Due to pre-stressed structural reinforcement being
sensitive to corrosion cracking, they stated the need for detailed
research of fractures within steel elements after stressing. For this
reason, the nondestructive magnetic flux leakage measurement technique
may be applied even within cladding tubes. Antipov and Markov (2222. Antipov, A.G.; Markov, A.A. (2018) A new MFL principle and method based on near-zero background magnetic field. NDT&E Intern. 98, 177-185. https://doi.org/10.1016/j.ndteint.2018.04.011.
)
researched the traditional MFL method for speed limitations in railroad
inspection and overcoming these limitations. They applied two different
methods to research the dependence of flux leakage data on measurement
speed. The first method performed 3D computer simulation of interactions
between a fixed rail and mobile magnetizing system and the second
method used measurement clusters created by an experimental system
comprising mobile sensors and artificial defects created along the rail.
In conclusion, the defects at the center of the rail head could be
identified at speeds above 80 km/h and they stated the distance between
the poles of the magnetizing system should be more than 3 m or some
alternative like MFL remote field analysis should be used. Sadr and
Okhovat (2323. Sadr, A.; Okhovat, R.S. (2016) Extracting the region of interest from MFL signals. Turk. J. Elec. Eng. Comp. Sci. 24, 427-434. https://doi.org/10.3906/elk-1305-70.
)
studied MFL signals for detection of defects in ferromagnetic
materials. They used histograms to eliminate effect of defects.
Myakushev et. al. (2424.
Myakushev, K.; Slesarev, D.; Sukhorukov, D. (2018) Magnetic flux
leakage (MFL) method for nondestructive testing of prestressed steel
reinforcement strands. 12th European Conference on Non-Destructive
Testing (ECNDT 2018), Gothenburg 2018, June 11-15 (ECNDT 2018).
)
investigated Magnetic flux leakage (MFL) method for nondestructive
testing of pre-stressed steel reinforcement strands and discussed
magnetic, measuring systems and design principles.
When previous studies related to the MFL method are investigated, it appears the MFL method is generally used to determine defects in pipelines and rail systems. Additionally, use to detect corrosion occurring in reinforcement comprising structural elements is encountered. Considering the previous studies, in this study, device for the nondestructive test technique of MFL method was produced and used for detection of reinforcement comprising structural elements in buildings. Thus, important results are reached about detection reinforcement with the MFL method.
2. DESIGN AND PROTOTYPE PREPARATION
⌅In order to perform MFL measurements, a transmitter coil, receiver coil, and transmitter and receiving coil electronic systems are required. For this reason, within the scope of the study all relevant pieces were designed and produced. For the core of the transmitter coil used a ‘soft iron core’ bent into a U shape (Figure 1). Above the core, bent into appropriate shape, 0.55 mm thick enamel-covered copper wire was used to create the transmitter coil.
After preparing the transmitter coil, frequency response graphs were prepared with the aim of determining suitable operating frequencies. When preparing the frequency response graphs, a calibrated function generator output was applied to the transmitter coil with sinus waves at different frequencies. The current induced in the receiver coil due to the current applied to the transmitter coil was recorded with the aid of an oscilloscope. In this way, the response of the designed system at different frequencies was obtained and a frequency-amplitude graph was plotted (Figure 2).
As seen on the graph in Figure 2, the system was observed to reach highest point at amplitudes in the ~ 220 - 400 Hz band, so for this reason the operating frequency was chosen as 300 Hz. After this stage, all prepared electronic device were designed in accordance with 300 Hz center frequency. The designed transmitter circuit was produced using a microprocessor-controlled signal generator so the transmitter frequency would remain stable. The signal amplitude was set to 48 VAC.
The receiver coil was created with a core containing a high permeability ‘soft iron core’, like the transmitter coil, isolated with enamel-covered copper wire. The receiver section may be affected by the electromagnetic field measured in the receiver coil and in the operating environment. For this reason, a capacitor connecting the receiver coil was matched to the transmitting frequency and attempts were made to suppress the effects of signals due to other parts of the electromagnetic spectrum on the coil. The photograph of the receiver and transmitter coils is shown in Figure 3.
Receiver and transmitter coil connections used co-axial cables with the aim of minimizing electromagnetic noise and preserving the signal quality and were ready to connect to electronic cards. The tips of the cables from the coils had appropriate connectors fitted. Electrical parameters of the receiving and transmitter coils are given in Table 1.
Resistance | Impedance | Diameter (mm) | Number of windings | |
---|---|---|---|---|
Receiver | 619.9 Ω | 30.5 µH | 25 | 1200 |
Transmitter | 2.1 Ω | 200 µH | 8 | 350 |
The electronic system to induce an electromagnetic field in the transmitter coil and to record the current induced in the receiver coil was prepared and tested in the laboratory environment. With this aim, an oscillator producing a signal at the desired frequency, an amplifier to increase this signal and sent it to the transmitter coil and electronic system to increase and filter the current induced in the receiver coil were prepared. The block schema is shown in Figure 4.
The signal amplitude sent to the transmitter coil through the electronic system is adjustable. After the signal induced in the receiver coil is amplified and filtered, it may be read as peak to peak amplitude in millivolts. The electronic system was mounted within a plastic box (Figure 5a,b); in this way the electronic circuits comprised as system that could work together. In our system, we used ATMEGA 328 low power, CMOS 8-bit microcontroller from Microchip Company and OP-07 Ultralow Offset Voltage Operational Amplifier from Analog Devices for transmitter waveform generation, then fed this signal to transmitter antenna using TDA 8932 D-Class audio amplifier IC from NXP company. Receiver part of electronics consist of receiver coil, AD524 Precision Instrumentation Amplifier from Analog Devices and UAF42 Universal Active Filter From Burr-Brown company followed by OP-07 Ultralow Offset Voltage Operational Amplifier from Analog Devices. Fluke 289 multimeter used to measure filtered signal amplitude. All system designed to work at 12 Volt direct current power supply.
After test measurements in the laboratory, the transmitter and receiver coils were placed in a plastic box with no metal connection elements used so as not to affect the system. Connecting cables were isolated with protective tape (Figure 5a). The prepared device created an electromagnetic field with 300 Hz frequency through the transmitter electronics and transmitter coil. The receiver coil was placed on a symmetric axis to the transmitter coil (Figure 3). The electromagnetic field induced by the transmitter intensified in the high-permeability receiver core and created a potential difference in receiver coil with amplitude directly proportional to the induced field in the enamel-coated copper wire around the core. The characteristics of the coils and distances between them were set to provide minimum amplitude in situations where there was no metal close to the sensor. When high-permeability metal is placed close to the sensor, the magnetic flux intensifying in the receiver coil core increases; hence, the potential differences due to the induction increases in direct proportion. These potential differences in the receiver coil were read at measurements in millivolts with the aid of a multimeter after passing through analog conditioners as shown in the flow diagram in Figure 4. The obtained values may be presented as two-dimensional graphs linked to distance or spatially on a grid.
3. TEST MEASUREMENTS
⌅Four different experimental systems were created to test the produced MFL device.
3.1. Test system 1
⌅The first test system included 7 ferromagnetic materials within a 90 × 60 cm area as shown in Figure 6. The depth of ferromagnetic materials are at 2 cm from the top of the test systems 1.
In the first test system the profile intervals were 10 cm and the point intervals were 1 cm with measurements performed with the produced magnetic flux leakage device (Figure 7).
The map obtained as a result of the MFL measurements on the first test system is shown in Figure 8. The locations and geometries of 7 ferromagnetic materials were detected by the produced magnetic flux leakage device.
3.2. Test system 2
⌅The second test system used 3 ferromagnetic materials within an 80 × 50 cm area as shown in Figure 9. The depth of ferromagnetic materials are at 2 cm from the top of the test systems 2.
The profile interval in the second test system was 10 cm and measurements were performed with the MFL device at 1 cm point intervals.
The map obtained as a result of MFL measurements completed for the second test system is shown in Figure 10. Locations and geometries of 3 ferromagnetic materials were identified by the magnetic flux leakage device.
3.3. Test system 3
⌅The third test system placed 7 rebar elements at 20 cm intervals within an 80 × 150 cm area as shown in Figure 11. The depth of reinforcements are at 10 cm from the top of the test system 3.
The profile intervals for the third system were 10 cm and measurements were made with the magnetic flux leakage device at point intervals of 5 cm (Figure 12).
The map obtained with the MFL measurements completed in the third test system is shown in Figure 13. Locations and geometries of 7 rebars were identified by the magnetic flux leakage device.
3.4. Test system 4
⌅The fourth test system placed 4 rebar elements at 20 cm intervals in the X direction and 7 rebars at 20 cm intervals in Y direction within an 80 × 150 cm area as shown in Figure 14. The depth of reinforcements are at 10 cm from the top of the test system 4.
Measurements were performed with a magnetic flux leakage device at profile intervals of 10 cm and point intervals of 5 cm for the fourth test system.
The map obtained from MFL measurements completed in the fourth test setup is shown in Figure 15. 4 rebar at 20 cm intervals in the X direction and 7 rebar located at 20 cm intervals in the Y direction were identified by the magnetic flux leakage device.
4. CONCLUSIONS
⌅There are several studies performed with the MFL method. The majority of these studies use the MFL method to determine defects in pipelines and rail systems. Another area of use is about detection of corrosion occurring in the structural elements. In this study, device for the nondestructive test technique of MFL method was produced and used for detection of reinforcement comprising structural elements in buildings. Thus, our results are showed that the MFL method can be used to detection reinforcement in addition to previous studies. The produced magnetic flux leakage device comprised a total of three sections. The first section included an oscillator with 300 Hz frequency signal output and amplifier circuits to increase amplitude. This section included a Tx (transmitter) comprising a U-core coil creating the primary magnetic field. The second section included a Rx (receiver) detecting the secondary magnetic field induced within ferromagnetic material and the third section was a voltmeter measuring the signal coming from the receiver. The magnetic flux leakage device was tested in 4 different systems. Thus, within the scope of this study, the magnetic flux leakage device provided successful data for determining rebar in reinforced concrete structures.