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International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056
Volume: 09 Issue: 02 | Feb 2022 www.irjet.net p-ISSN: 2395-0072
© 2022, IRJET | Impact Factor value: 7.529 | ISO 9001:2008 Certified Journal | Page 479
Behavior of Ultrasound Energy in the Presence of Obstacle
Kolimi Rakshitha1, S. Sundar Kumar2, Vimal Mohan3, E. Aruna Kanthi4,P. Srinivasan5
1Dept. of Civil Engineering, JNTU College of Engineering, Anantapur, Andhra Pradesh, India.
2Senior Scientist, CSIR-SERC, Chennai, 600113, Tamil Nadu, India.
3Senior Scientist, CSIR-SERC, Chennai, 600113, Tamil Nadu, India.
4 Professor, Dept. of Civil Engineering, JNTU College of Engineering, Anantapur, Andhra Pradesh, India.
5Chief Scientist and Head, CSIR-SERC, Chennai, 600113, Tamil Nadu, India.
---------------------------------------------------------------------***----------------------------------------------------------------------
Abstract - In this paper, we study the behavior of a
ultrasound energy in presenceofanobstacle.Theultrasound
signal of 50kHz is passed through the concrete cubes of
different size and grade. The concrete cubes are embedded
with the obstacles of different densities. Using Mat lab and
fundamentals ofultrasound energy,energycurvesaredrawn
and area under the curve is calculated. The area under the
energy curve is absorbed when passed through an obstacle.
This shows that the energy is decreased when ultrasound
signal from one medium to another.
Key Words: Concrete, Obstacle, Ultrasound, Ultrasonic,
Ultrasound energy, Mat lab, acoustic attenuation, Ultrasonic
signal.
1.INTRODUCTION
Ultrasonic waves are sound waves that are beyond the
normal hearing range of the human beings. Thefrequencyof
such waves are above 20kHz. This waves have similar
properties to that of sound waves. This waves are used in
various field such as Medicine, Industries and construction.
It is used for Non-Destructive Evaluation in the field of
construction.
Ultrasonic Pulse Velocity is usually used in the structural
health monitoring to determine the quality of concrete. But
this method deals with the overall quality but cannot find
any foreign objects present intheconcrete.Toovercomethis
drawback, we use ultrasoundenergytodistinguishobstacles
in the concrete.
The signal processing software suchasMatlab,labview,etc.,
makes it simple for us to derive energy from the signal. In
this paper, we use Mat lab to calculate energy of the
ultrasonic signal.
1.1 Principle of ultrasonic wave:
There are three principles ofultrasonics . TheyareLawof
reflection, refraction and shadow method. The law of
reflection states that when a waveispassedthroughmaterial
with two different media a part of wave is reflected and the
remaining flow through the second material but not in
direction same as incident wave. The law of refraction states
that that “the angle made by the incident wave with the
normal plane to the interface is the same as the angle made
by the reflected wave with the normal plane to the interface
of material”. The detectionofdecreaseinenergyofUltrasonic
beam due to absorption of energy by flaw. This involves the
transformation of energy due to internal friction of defect or
failure to transfer energy across the air gap of defect. This is
known as the shadow method. In this paper, we use the
shadow method.
1.2 Methods of transmission
To assess the condition of a concretethetransistortimeof
high frequency sound waves are used.ASTMstandardC-597
talks about ultrasonic testing procedures. Two separate
transducers are required to measure sound velocity in non-
homogenous materials as concrete. One is for transmitting
and the other is for receiving. Sound velocityiscalculatedby
measuring the time required to transmit over a known path
length. The uniformity in concrete is established by the
measurement of average sound velocity through the
concrete. There are three approaches for measuring the
sound velocity in concrete. They are direct, indirect and
semi-direct. Direct method is method in which we keepboth
the transducers opposite sides of object,Indirectmethod isa
method in which we place both the transducers on the same
side of the object. In Semi-direct method, we place
transducers on adjacent sides of object. Here, we use the
direct method.
1.3 Properties of Ultrasonic wave:
Ultrasonic waves while passing through materials
experience resistance by the stress front or pressure in the
passage of waves. This resistancedependsonthepropertyof
the material.
1.3.1. Acoustic Impedance:
Acoustic Impedance is the resistance experienced by
Ultrasound to the passage. It is denoted by Z.
Z= ρ x V [ eq. 1]
Where ρ is density of the material and V is the Velocity ofthe
sound wave.
International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056
Volume: 09 Issue: 02 | Feb 2022 www.irjet.net p-ISSN: 2395-0072
© 2022, IRJET | Impact Factor value: 7.529 | ISO 9001:2008 Certified Journal | Page 480
1.3.2. Acoustic Attenuation:
Attenuation is the property of material which reduces the
energy as the ultrasound wave passes through it. Higher the
attenuation, lower the penetrability of the wave. Large
amounts of this attenuation leads to loss of back wall
reflection.
The main Phenomena due to this attenuation are Scattering,
Diffusion, Viscous damping losses and Relaxation losses.
Scattering and diffusion are caused due to the wave motion
of ultrasound. Viscous damping and relaxation losses are
caused by the stressing of atoms in material.Weuseacoustic
attenuation in this paper.
1.4 Data Collection:
The signal is transmitted through the transducer and
received is collected through the digital oscilloscope.
Generally, the data is collected and represented in three
formats. They are A-scan, B-Scan and C-Scan.
A-Scan represents the strength of the signal orAmplitude
with the time as the function. This represents the waveform
of the signal. The energy depends on the square of the
amplitude. Hence, this setup isusedintheultrasoundenergy
method. B-Scan presents the change in the time of flight of
signal with respect to that of the distance. It displays the
time of flight on the Y-Axis and Scan distance on the X-Axis.
This representation is used in the ultrasonic pulse echo
method. C-Scan displays the features of the test specimen
such as location and size. It is like the plan view of the
specimen. It gives the image of the feature of the defects or
specimen. This is generally used in the ultrasound
tomography method. In this paper, we use B-Scan.
1.5 Energy:
Vibratory waves are introduced into the medium at
frequencies above 20kHz to produce ultrasonic waves. The
energy produced by these waves is known as ultrasound
energy.
As per the Moradi-Marani, Farid, et al. Construction and
Building Materials,2014, the energy can be calculated
through the following equation
[eq. 2]
E is Energy of Ultrasonic wave
A is Amplitude of Ultrasonic wave
t’ is time travelled by the wave
The Mat lab code is written using eq.2 and energy curves
are drawn. Since, the energy is sensitive to minor changes,
we study the behaviour of ultrasound energy to an obstacle
present in the concrete.
2. EXPERIMENT
2.1 Materials
According to IS 12269, OPC grade 53 cement istakeninto
consideration. A locally accessible coarse aggregate mixture
of 60% 10mm and 40% 20mm with a specific gravityof2.83
is employed. The fine aggregate utilisedhasa specificgravity
of 2.6. In M40 concrete, Conplast SP – 430 is utilised as a
superplasticizer. The M20, M30, and M40 concrete are
designed with obstacles in accordance with IS 10262: 2019.
Thermocol and plywood with 50mm thickness and110 mm
in length and breadth are used as obstaclesin220mmcubes,
and thermocol and plywood with 50mm thickness and
160mm in length and breadth are used as obstacles in
320mm cubes. The 16mm rod is 34 mm from the right and
75 mm from the back edge of the concrete cube in 220 mm.
The 20mm rod is 75 mm from the concrete cube's left edge
and 40 mm from the front edge. The 32mm rod is 30mm
from the left edge of the concrete cube and 70mm from the
back edge. The 16mm rod is 80mm fromtherightand95mm
from the back edge of the concrete cube in 320 mm. The
20mm rod is 40mm from the left edge of the concrete cube
and 75mm from the front edge. The 32mm rod is 60mm
from the left edge of the concrete cube and 100mm from the
back edge.
2.2 Procedure:
Portable UltrasonicNon-destructiveDigital IndicatingTester
(PUNDIT) transducers with a frequency of 54 kHz are saved
on opposing edges of the cube as mentioned in 1.2 for direct
transmission. BNC cables are used to link the transmitter
and receiver to the PUNDIT. BNC cables are used to connect
Table 1. Area under energy curves of the ultrasonic
signals passed through Concrete cubes of 220mm
Part of testing Area under Energy curve (J-s)
M20 M30 M40
Sampling
interval
4.00E-
05
2.00E-04 1.00E-06
without
obstacle
2.02E-
05
3.72E-04 2.91E-03
without
plywood
2.64E-
05
9.52E-04 2.68E-03
with
plywood
2.65E-
05
1.18E-03 2.63E-03
without
thermocol
2.59E-
05
3.00E-04 2.79E-03
with
thermocol
2.13E-
05
3.92E-06 2.82E-03
International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056
Volume: 09 Issue: 02 | Feb 2022 www.irjet.net p-ISSN: 2395-0072
© 2022, IRJET | Impact Factor value: 7.529 | ISO 9001:2008 Certified Journal | Page 481
PUNDIT to the digital oscilloscope. The signal from the
digital oscilloscope is sent to the computer through USB.
Within the digital oscilloscope, the output signal iscaptured.
The amplitude and temporal components are calculated
using B-scan, as described in 1.4. MATLAB is used to import
the amplitude, time components, and sample frequency.
Equation 2 is used to determine the signal's energy, and the
mat lab code is used to draw the energy curve.
Repeat the experiment on a concrete cube withnoobstacles,
a concrete cube with and withoutplywood,withand without
thermocol, and rods of 16mm, 20mm, and 32mm in
diameter. Calculate the area beneath the energy curve using
the MATLAB 'trapz' function and compare the area beneath
the curves in tables 1 and 2.
3. RESULTS
Table 1 and 2 shows the area under the energy curve of the
ultrasonic signal passed through the M20, M30 and M40
concrete cube of 220mm dimension with and without
foreign objects in it . Table 3 and 4 shows the area under the
energy curve of the ultrasonic signal passed through the
M20, M30 and M40 concrete cubeof320mmdimensionwith
and without foreign objects in it.
The table 1 and 3 shows that the area under the energy
curve when passed through an obstacle is lesser that of the
concrete without an obstacle. This displays that the
absorption of the energy of ultrasonic wave when passed
through a concrete block with obstacle. Table2and4depicts
the area under the energy curves that pass through the
concrete with rods of 16mm, 20mm and 32 mm are almost
similar in all grades of concrete. So this shows that the
reinforcement does not affect the energy as other two
obstacles.
Table 3. Area under energy curves of the ultrasonic
signals passed through Concrete cubes of 320mm
Part of
testing
Area under Energy curve (J-s)
M20 M30 M40
Sampling
interval
2.00E-
04
2.00E-
04
1.00E-
06
without
obstacle
3.50E-
04
7.32E-
04
2.81E-
03
without
plywood
2.47E-
04
6.66E-
04
2.68E-
03
with
plywood
1.48E-
06
6.78E-
04
2.60E-
03
without
thermocol
3.10E-
04
7.11E-
04
2.72E-
03
with
thermocol
2.53E-
04
6.91E-
04
2.70E-
03
Table 4. Area under energy curves of the ultrasonic
signals passed through Concrete cubes of 320mm -
Rods
Part of
testing
Area under Energy curve (J-s)
M20 M30 M40
Sampling
interval
2.00E-
04
2.00E-
04
1.00E-
06
without
rods
3.50E-
04
7.32E-
04
2.81E-
03
with
16mm
Rod
2.52E-
04
6.79E-
04
2.84E-
03
with
20mm
Rod
2.53E-
04
6.95E-
04
2.68E-
03
with
32mm
Rod
2.19E-
04
7.25E-
04
2.60E-
03
4. CONCLUSION
The area under the energy curve is reduced when passed
through an obstacle other than reinforcement. The
reinforcement does not affect theenergy. Hence,theenergy
of an ultrasonic wave is absorbed when passed through the
concrete block with a foreign object. This method can be
used to detect foreign objects present in the concreteaswell
as reinforced concrete structures.
REFERENCES
[1] “Handbook on Non-destructive Testing of Concrete”,
2004 by V.M. Malhotra.
[2] "Ultrasonic characterization of damage in concrete."by
Manu Santhanam. Structural Longevity 3.1-2 (2010):
111-125.
Table 2. Area under energy curves of the ultrasonic
signals passed through Concrete cubes of 220mm -
Rods
Part of
testing
Area under Energy curve (J-s)
M20 M30 M40
Sampling
interval
1.00E-
06
1.00E-
06
1.00E-
06
without
rods
2.93E-
03
2.82E-
03
2.91E-03
with
16mm Rod
2.92E-
03
2.94E-
03
2.81E-03
with
20mm Rod
2.73E-
03
2.95E-
03
2.88E-03
with
32mm Rod
2.81E-
03
2.98E-
03
2.74E-03
International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056
Volume: 09 Issue: 02 | Feb 2022 www.irjet.net p-ISSN: 2395-0072
© 2022, IRJET | Impact Factor value: 7.529 | ISO 9001:2008 Certified Journal | Page 482
[3] Moradi-Marani, Farid, Patrice Rivard, Charles-Philippe
Lamarche, and Serge Apedovi Kodjo. "Evaluating the
damage in reinforced concrete slabs under bending test
with the energy of ultrasonic waves." Construction and
Building Materials 73 (2014): 663-673.
[4] Bureau of Indian Standards: IS13311-1(1992):Method
of Non-destructive testing of concrete,Part1:Ultrasonic
pulse velocity [CED 2: Cement and Concrete].
[5] Bureau of Indian Standard: IS 12269 (1987) 53 grade
ordinary Portland cement [CED 2: Cement and
Concrete].
[6] Bureau of Indian Standard: IS 10262 (2019) Concrete
mix proportioning guidelines (second revision)
[7] https://youtu.be/xGP9dRcUHDU : Planys technologies

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Behavior of Ultrasound Energy in the Presence of Obstacle

  • 1. International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 09 Issue: 02 | Feb 2022 www.irjet.net p-ISSN: 2395-0072 © 2022, IRJET | Impact Factor value: 7.529 | ISO 9001:2008 Certified Journal | Page 479 Behavior of Ultrasound Energy in the Presence of Obstacle Kolimi Rakshitha1, S. Sundar Kumar2, Vimal Mohan3, E. Aruna Kanthi4,P. Srinivasan5 1Dept. of Civil Engineering, JNTU College of Engineering, Anantapur, Andhra Pradesh, India. 2Senior Scientist, CSIR-SERC, Chennai, 600113, Tamil Nadu, India. 3Senior Scientist, CSIR-SERC, Chennai, 600113, Tamil Nadu, India. 4 Professor, Dept. of Civil Engineering, JNTU College of Engineering, Anantapur, Andhra Pradesh, India. 5Chief Scientist and Head, CSIR-SERC, Chennai, 600113, Tamil Nadu, India. ---------------------------------------------------------------------***---------------------------------------------------------------------- Abstract - In this paper, we study the behavior of a ultrasound energy in presenceofanobstacle.Theultrasound signal of 50kHz is passed through the concrete cubes of different size and grade. The concrete cubes are embedded with the obstacles of different densities. Using Mat lab and fundamentals ofultrasound energy,energycurvesaredrawn and area under the curve is calculated. The area under the energy curve is absorbed when passed through an obstacle. This shows that the energy is decreased when ultrasound signal from one medium to another. Key Words: Concrete, Obstacle, Ultrasound, Ultrasonic, Ultrasound energy, Mat lab, acoustic attenuation, Ultrasonic signal. 1.INTRODUCTION Ultrasonic waves are sound waves that are beyond the normal hearing range of the human beings. Thefrequencyof such waves are above 20kHz. This waves have similar properties to that of sound waves. This waves are used in various field such as Medicine, Industries and construction. It is used for Non-Destructive Evaluation in the field of construction. Ultrasonic Pulse Velocity is usually used in the structural health monitoring to determine the quality of concrete. But this method deals with the overall quality but cannot find any foreign objects present intheconcrete.Toovercomethis drawback, we use ultrasoundenergytodistinguishobstacles in the concrete. The signal processing software suchasMatlab,labview,etc., makes it simple for us to derive energy from the signal. In this paper, we use Mat lab to calculate energy of the ultrasonic signal. 1.1 Principle of ultrasonic wave: There are three principles ofultrasonics . TheyareLawof reflection, refraction and shadow method. The law of reflection states that when a waveispassedthroughmaterial with two different media a part of wave is reflected and the remaining flow through the second material but not in direction same as incident wave. The law of refraction states that that “the angle made by the incident wave with the normal plane to the interface is the same as the angle made by the reflected wave with the normal plane to the interface of material”. The detectionofdecreaseinenergyofUltrasonic beam due to absorption of energy by flaw. This involves the transformation of energy due to internal friction of defect or failure to transfer energy across the air gap of defect. This is known as the shadow method. In this paper, we use the shadow method. 1.2 Methods of transmission To assess the condition of a concretethetransistortimeof high frequency sound waves are used.ASTMstandardC-597 talks about ultrasonic testing procedures. Two separate transducers are required to measure sound velocity in non- homogenous materials as concrete. One is for transmitting and the other is for receiving. Sound velocityiscalculatedby measuring the time required to transmit over a known path length. The uniformity in concrete is established by the measurement of average sound velocity through the concrete. There are three approaches for measuring the sound velocity in concrete. They are direct, indirect and semi-direct. Direct method is method in which we keepboth the transducers opposite sides of object,Indirectmethod isa method in which we place both the transducers on the same side of the object. In Semi-direct method, we place transducers on adjacent sides of object. Here, we use the direct method. 1.3 Properties of Ultrasonic wave: Ultrasonic waves while passing through materials experience resistance by the stress front or pressure in the passage of waves. This resistancedependsonthepropertyof the material. 1.3.1. Acoustic Impedance: Acoustic Impedance is the resistance experienced by Ultrasound to the passage. It is denoted by Z. Z= ρ x V [ eq. 1] Where ρ is density of the material and V is the Velocity ofthe sound wave.
  • 2. International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 09 Issue: 02 | Feb 2022 www.irjet.net p-ISSN: 2395-0072 © 2022, IRJET | Impact Factor value: 7.529 | ISO 9001:2008 Certified Journal | Page 480 1.3.2. Acoustic Attenuation: Attenuation is the property of material which reduces the energy as the ultrasound wave passes through it. Higher the attenuation, lower the penetrability of the wave. Large amounts of this attenuation leads to loss of back wall reflection. The main Phenomena due to this attenuation are Scattering, Diffusion, Viscous damping losses and Relaxation losses. Scattering and diffusion are caused due to the wave motion of ultrasound. Viscous damping and relaxation losses are caused by the stressing of atoms in material.Weuseacoustic attenuation in this paper. 1.4 Data Collection: The signal is transmitted through the transducer and received is collected through the digital oscilloscope. Generally, the data is collected and represented in three formats. They are A-scan, B-Scan and C-Scan. A-Scan represents the strength of the signal orAmplitude with the time as the function. This represents the waveform of the signal. The energy depends on the square of the amplitude. Hence, this setup isusedintheultrasoundenergy method. B-Scan presents the change in the time of flight of signal with respect to that of the distance. It displays the time of flight on the Y-Axis and Scan distance on the X-Axis. This representation is used in the ultrasonic pulse echo method. C-Scan displays the features of the test specimen such as location and size. It is like the plan view of the specimen. It gives the image of the feature of the defects or specimen. This is generally used in the ultrasound tomography method. In this paper, we use B-Scan. 1.5 Energy: Vibratory waves are introduced into the medium at frequencies above 20kHz to produce ultrasonic waves. The energy produced by these waves is known as ultrasound energy. As per the Moradi-Marani, Farid, et al. Construction and Building Materials,2014, the energy can be calculated through the following equation [eq. 2] E is Energy of Ultrasonic wave A is Amplitude of Ultrasonic wave t’ is time travelled by the wave The Mat lab code is written using eq.2 and energy curves are drawn. Since, the energy is sensitive to minor changes, we study the behaviour of ultrasound energy to an obstacle present in the concrete. 2. EXPERIMENT 2.1 Materials According to IS 12269, OPC grade 53 cement istakeninto consideration. A locally accessible coarse aggregate mixture of 60% 10mm and 40% 20mm with a specific gravityof2.83 is employed. The fine aggregate utilisedhasa specificgravity of 2.6. In M40 concrete, Conplast SP – 430 is utilised as a superplasticizer. The M20, M30, and M40 concrete are designed with obstacles in accordance with IS 10262: 2019. Thermocol and plywood with 50mm thickness and110 mm in length and breadth are used as obstaclesin220mmcubes, and thermocol and plywood with 50mm thickness and 160mm in length and breadth are used as obstacles in 320mm cubes. The 16mm rod is 34 mm from the right and 75 mm from the back edge of the concrete cube in 220 mm. The 20mm rod is 75 mm from the concrete cube's left edge and 40 mm from the front edge. The 32mm rod is 30mm from the left edge of the concrete cube and 70mm from the back edge. The 16mm rod is 80mm fromtherightand95mm from the back edge of the concrete cube in 320 mm. The 20mm rod is 40mm from the left edge of the concrete cube and 75mm from the front edge. The 32mm rod is 60mm from the left edge of the concrete cube and 100mm from the back edge. 2.2 Procedure: Portable UltrasonicNon-destructiveDigital IndicatingTester (PUNDIT) transducers with a frequency of 54 kHz are saved on opposing edges of the cube as mentioned in 1.2 for direct transmission. BNC cables are used to link the transmitter and receiver to the PUNDIT. BNC cables are used to connect Table 1. Area under energy curves of the ultrasonic signals passed through Concrete cubes of 220mm Part of testing Area under Energy curve (J-s) M20 M30 M40 Sampling interval 4.00E- 05 2.00E-04 1.00E-06 without obstacle 2.02E- 05 3.72E-04 2.91E-03 without plywood 2.64E- 05 9.52E-04 2.68E-03 with plywood 2.65E- 05 1.18E-03 2.63E-03 without thermocol 2.59E- 05 3.00E-04 2.79E-03 with thermocol 2.13E- 05 3.92E-06 2.82E-03
  • 3. International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 09 Issue: 02 | Feb 2022 www.irjet.net p-ISSN: 2395-0072 © 2022, IRJET | Impact Factor value: 7.529 | ISO 9001:2008 Certified Journal | Page 481 PUNDIT to the digital oscilloscope. The signal from the digital oscilloscope is sent to the computer through USB. Within the digital oscilloscope, the output signal iscaptured. The amplitude and temporal components are calculated using B-scan, as described in 1.4. MATLAB is used to import the amplitude, time components, and sample frequency. Equation 2 is used to determine the signal's energy, and the mat lab code is used to draw the energy curve. Repeat the experiment on a concrete cube withnoobstacles, a concrete cube with and withoutplywood,withand without thermocol, and rods of 16mm, 20mm, and 32mm in diameter. Calculate the area beneath the energy curve using the MATLAB 'trapz' function and compare the area beneath the curves in tables 1 and 2. 3. RESULTS Table 1 and 2 shows the area under the energy curve of the ultrasonic signal passed through the M20, M30 and M40 concrete cube of 220mm dimension with and without foreign objects in it . Table 3 and 4 shows the area under the energy curve of the ultrasonic signal passed through the M20, M30 and M40 concrete cubeof320mmdimensionwith and without foreign objects in it. The table 1 and 3 shows that the area under the energy curve when passed through an obstacle is lesser that of the concrete without an obstacle. This displays that the absorption of the energy of ultrasonic wave when passed through a concrete block with obstacle. Table2and4depicts the area under the energy curves that pass through the concrete with rods of 16mm, 20mm and 32 mm are almost similar in all grades of concrete. So this shows that the reinforcement does not affect the energy as other two obstacles. Table 3. Area under energy curves of the ultrasonic signals passed through Concrete cubes of 320mm Part of testing Area under Energy curve (J-s) M20 M30 M40 Sampling interval 2.00E- 04 2.00E- 04 1.00E- 06 without obstacle 3.50E- 04 7.32E- 04 2.81E- 03 without plywood 2.47E- 04 6.66E- 04 2.68E- 03 with plywood 1.48E- 06 6.78E- 04 2.60E- 03 without thermocol 3.10E- 04 7.11E- 04 2.72E- 03 with thermocol 2.53E- 04 6.91E- 04 2.70E- 03 Table 4. Area under energy curves of the ultrasonic signals passed through Concrete cubes of 320mm - Rods Part of testing Area under Energy curve (J-s) M20 M30 M40 Sampling interval 2.00E- 04 2.00E- 04 1.00E- 06 without rods 3.50E- 04 7.32E- 04 2.81E- 03 with 16mm Rod 2.52E- 04 6.79E- 04 2.84E- 03 with 20mm Rod 2.53E- 04 6.95E- 04 2.68E- 03 with 32mm Rod 2.19E- 04 7.25E- 04 2.60E- 03 4. CONCLUSION The area under the energy curve is reduced when passed through an obstacle other than reinforcement. The reinforcement does not affect theenergy. Hence,theenergy of an ultrasonic wave is absorbed when passed through the concrete block with a foreign object. This method can be used to detect foreign objects present in the concreteaswell as reinforced concrete structures. REFERENCES [1] “Handbook on Non-destructive Testing of Concrete”, 2004 by V.M. Malhotra. [2] "Ultrasonic characterization of damage in concrete."by Manu Santhanam. Structural Longevity 3.1-2 (2010): 111-125. Table 2. Area under energy curves of the ultrasonic signals passed through Concrete cubes of 220mm - Rods Part of testing Area under Energy curve (J-s) M20 M30 M40 Sampling interval 1.00E- 06 1.00E- 06 1.00E- 06 without rods 2.93E- 03 2.82E- 03 2.91E-03 with 16mm Rod 2.92E- 03 2.94E- 03 2.81E-03 with 20mm Rod 2.73E- 03 2.95E- 03 2.88E-03 with 32mm Rod 2.81E- 03 2.98E- 03 2.74E-03
  • 4. International Research Journal of Engineering and Technology (IRJET) e-ISSN: 2395-0056 Volume: 09 Issue: 02 | Feb 2022 www.irjet.net p-ISSN: 2395-0072 © 2022, IRJET | Impact Factor value: 7.529 | ISO 9001:2008 Certified Journal | Page 482 [3] Moradi-Marani, Farid, Patrice Rivard, Charles-Philippe Lamarche, and Serge Apedovi Kodjo. "Evaluating the damage in reinforced concrete slabs under bending test with the energy of ultrasonic waves." Construction and Building Materials 73 (2014): 663-673. [4] Bureau of Indian Standards: IS13311-1(1992):Method of Non-destructive testing of concrete,Part1:Ultrasonic pulse velocity [CED 2: Cement and Concrete]. [5] Bureau of Indian Standard: IS 12269 (1987) 53 grade ordinary Portland cement [CED 2: Cement and Concrete]. [6] Bureau of Indian Standard: IS 10262 (2019) Concrete mix proportioning guidelines (second revision) [7] https://youtu.be/xGP9dRcUHDU : Planys technologies