PROPOSAL
INSENTIF ARTIKEL PADA PROSIDING INTERNASIONAL TERINDEKS
BATCH I
Dr. M. Syukri Surbakti, S.Si., M.Si.
NIP. 197310302000121001
UNIVERSITAS SYIAH KUALA BANDA ACEH
2020
BIODATA PENGUSUL
Nama : Dr. M. Syukri Surbakti, S.Si, M.Si.
Alamat Korespondensi : Jurusan Fisika FMIPA Universitas Syiah Kuala Darussalam Banda Aceh 23111
Telepon/Faks : Telp. 0651-741265 HP : +62 81362787433 Email : msyukris@unsyiah.ac.id
Riwayat Pendidikan:
Jenjang Tahun
Lulus Perguruan Tinggi Bidang Spesialisasi Sarjana 1997 Universitas Sumatera Utara Medan Fisika
Master 2003 Universitas Gadjah Mada Geofisika Doktor 2013 Universiti Sains Malaysia Geofisika dan
Penginderaan Jauh
Pengalaman Penelitian 3 tahun terakhir
No. Judul Sponsor Tahun Posisi
1
Pengembangan dan Pembuatan Alat Geometry Normalized Electromagnetic System (GNES) Pada Aplikasi Early Warning System Untuk Tanah Longsor dan Likuifaksi
PNBP, Unsyiah
2019 Ketua
2
Identifikasi sifat fisis dan kimia kopi unggulan Indonesia
WCR 2020 Anggota
Pengalaman Publikasi selama 3 tahun terakhir
No. Judul Nama Jurnal dan Volume
1
Multi-frequency effect towards High Conductivity Overburden Responses using Vertical Coplanar (VCP) coil configuration for Landslide Instrumentation
Journal of Physics: Conference Series 1120: 012069. Tahun 2018
2 Analisis Kerentanan Situs Heritage Terhadap Ancaman Letusan Gunung Api Sinabung
Jurnal Geografi, Vol 11, No 1 (2019). Tahun 2019
3
Multi-frequency effect towards High Conductivity Overburden Responses using Horizontal Coplanar (HCP) coil
configuration for Landslide Hazard Instrumentation
IOP Conference Series: Earth and Environmental Science 273:
012022. Tahun 2019
4
Viscosity Measurement of Blended
Patchaoli Oil at Atmospheric Pressure and Room Temperature
Journal of Engineering and
Technological Sciences, 51(5), 683-
692, 2337-5779. Tahun 2019
5
The 2D resistivity modelling on north sumatran fault structure by using magnetotelluric data
IOP Conference Series: Earth and Environmental Science 364 (1), 012036. Tahun 2019
6
NDVI Based Analysis on the Impact of 2004 Tsunami Disaster Recovery Toward
Vegetation Condition in Banda Aceh
Journal of Aceh Physics Society 8 (3), 66-7. Tahun 2019
7
Remote Sensing Satellite Imagery and In-Situ Data for Identifying
Geothermal Potential Sites: Jaboi, Indonesia
Int. Journal of Renewable Energy Development (IJRED), 9 (2), 237- 245, 2252-4940. Tahun 2020
8 Design and testing of portable laser-based viscometer
MS&E 796 (1), 012027. Tahun 2020
9
Physical model of discontinuity response in landslide application using geometry
normalized electromagnetic system (GNES)
AIP Conference Proceedings 2221 (1), 100009. Tahun 2020
10
Application of magnetic method for mapping buried structures around
archaeological site of Masjid Tuha Indrapuri
Jurnal Natural 20 (2), 31-35. Tahun 2020
Banda Aceh, 26 April 2020 Pengusul,
Dr. M. Syukri Surbakti, S.Si, M.Si.
NIP. 197310302000121001
Editorial Board
Reviewer Chair:
Prof. Dr. Timbangen Sembiring, M.Sc.
Members:
1. Prof. Dr. Nasruddin MN, M.Eng.Sc.
2. Prof. Dr. Kerista Sebayang, M.S.
3. Tulus Ikhsan Nasution, M.Sc., Ph.D.
4. Saharman Gea, Ph.D 5. Belete Asefa Aragaw, Ph.D
6. Dr.Syahrul Humaidi, M.Sc.
AIP Conference Proceedings 2221, 010001 (2020); https://doi.org/10.1063/12.0000364 2221, 010001
© 2020 Author(s).
Preface: The 1st International Conference on Physics and Applied Physics (the 1st ICP&AP) 2019
Cite as: AIP Conference Proceedings 2221, 010001 (2020); https://doi.org/10.1063/12.0000364 Published Online: 31 March 2020
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Preface: The 1st International Conference on Physics and Applied Physics (The 1
stICP&AP) 2019
Industry 4.0 emphasizes the integration among physical, digital and biological systems, which can be applied for human lives and civilizations. The extent to which this transformation will have a positive impact depends on how we can navigate the risks and opportunities that arise in the future. In order to face the challenge of industry 4.0, we need to prepare ourselves by employing these four issues: critical thinking, creativity, communication, collaboration.
Based on the above explanation of industry 4.0, Universitas Sumatera Utara (USU), Indonesia, found that it was necessary to involve as a part of this industry trend, especially in Department of Physics, as a foundation of technology and sciences institute. Thus, Department of Physics USU addressed the above four issues, required for industry 4.0, by conducting an event called International Conference on
Physics and Applied Physics (ICP&AP), which will be held on 12th – 13th September 2019. Thetheme that will be delivered is “Fundamental and Innovative Research for Improving Competitive
Dignified Nation and Industrial Revolution 4.0”.Moreover, the conference itself will provide as a place to yield several benefits for both the researchers and the development of science and technology, namely:
Increasing the role of Applied Physics and Physics in the face of the 4.0 Industrial Revolution.
Discussing the results of research related to Physics and Applied Physics with fellow researchers and policymakers.
Facilitating communication and discussion regarding problems, opportunities and actual progress of Physics and Applied Physics to support the acceleration of development.
The seminar participants are expected to number more than 150 participants from within and outside the country.
Keynote Speakers
Prof Ming Way Lee (National Chung Hsing University, Taiwan)
Inturu Omkaram, M.Sc., M.Phill, Ph.D. (Kyung Hee University, South Korea)
Dr. Nafizhah Oesman (UiTM Perlis Malaysia)
Dr. Syahrul Humaidi (USU, Indonesia)
The 1st International Conference on Physics and Applied Physics (The 1st ICP&AP) 2019
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Conference date: 12–13 September 2019 Location: Medan, Indonesia
ISBN: 978-0-7354-1980-3
Editors: Timbangen Sembiring, Nasruddin MN, Kerista Sebayang, Tulus Ikhsan Nasution, Saharman Gea, Belete Asefa Aragaw and Syahrul Humaidi
Volume number: 2221 Published: Mar 31, 2020
DISPLAY : 20 50 100 all
PRELIMINARY
Full . March 2020THE 1ST INTERNATIONAL CONFERENCE ON PHYSICS AND APPLIED PHYSICS (THE 1ST ICP&AP) 2019: Fundamental and
Innovative Research for Improving Competitive Dignified Nation and Industrial Revolution 4.0
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Preface: The 1st International Conference on Physics and Applied Physics (the 1st ICP&AP) 2019
AIP Conference Proceedings 2221, 010001 (2020); https://doi.org/10.1063/12.0000364
PLENARY AND KEYNOTE PAPER
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Syahrul Humaidi
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AIP Conference Proceedings 2221, 100009 (2020); https://doi.org/10.1063/5.0004388 2221, 100009
© 2020 Author(s).
Physical model of discontinuity response in landslide application using geometry
normalized electromagnetic system (GNES)
Cite as: AIP Conference Proceedings 2221, 100009 (2020); https://doi.org/10.1063/5.0004388 Published Online: 31 March 2020
Muhammad Syukri Surbakti, Bukhari, Nazli Ismail, Nasrullah Idris, Muhammad Isa, Elin Yusibani, Zakaria, Muhammad Nurman, and Mohd Zubir Mat Jafri
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Physical Model of Discontinuity Response in Landslide Application Using Geometry Normalized Electromagnetic
System (GNES)
Muhammad Syukri Surbakti
1,a), Bukhari
1,2,b), Nazli Ismail
1,c), Nasrullah
Idris
1,d),Muhammad Isa
1,e), Elin Yusibani
1,f),Zakaria
1,g), Muhammad Nurman
3,h), and MohdZubir Mat Jafri
4,i)1Department of Physics, Faculty of Mathematics and Natural Sciences, Universitas Syiah Kuala Jln. SyechAbdul Ra’uf No. 3 Darussalam, 23111 Banda Aceh, Aceh, Indonesia
2Doctorate Program of Mathematics and Applied Science (DMAS), Postgraduate Program, Universitas Syiah Kuala, Banda Aceh 23111, Indonesia.
3SMAN 2 Binjai, Jalan Padang No. 8, Binjai 20722, Indonesia.
4 School of Physics, UniversitiSains Malaysia, Minden 11800, Penang, Malaysia
a)Corresponding author: msyukris@unsyiah.ac.id
b)bukhari@unsyiah.ac.id
c)nazli.ismail@unsyiah.ac.id
d)nasrullah.idris@unsyiah.ac.id
e)muhammadisa@gmail.com
f)e_yusibani@unsyiah.ac.id
g)zakaria@unsyiah.ac.id
h)mrsurbakti@gmail.com
i)mjafri@usm.my
Abstract.The discontinuity in a fractured land in landslide application could be represented by the metal defects in the physical modeling that will usually reduce the mass of the metal. The scale factor n is important for interpreting the field data using the physical model data. In this physical modeling (n=100), the anomaly targets are aluminum plates and aluminum plates with the discontinuities. It is assumed the nonconductive environment. In the free-air condition which has zero conductivity is become representative of this environment. In the zero conductivity, the secondary field from the medium is not presence. In this condition, there are no phase differences between transmitted electromagnetic fields and that was received by the receiver. The discontinuity in this term is any treatment or defect that causes disruption or leads to a reduction in response triggered by the eddy currents. The discontinuities used on the thin plates and flaws will interrupt or reduce the eddy current flow on the plate, thereby reducing the induced voltage on the receiving coil and increasing its effective impedance. This is the basis of eddy current measurement. The electromagnetic field response to a metal that has discontinuities will change the eddy current portion. The eddy current that changes, therefore, will change the second field so that the percent response (% Response) of the receiver in the Geometry Normalized Electromagnetic System (GNES) instrument will also change.
The 1st International Conference on Physics and Applied Physics (The 1st ICP&AP) 2019
INTRODUCTION
The geometry normalized electromagnetic system (GNES) instrument has developed in several applications, such as metal defect detection [1], and landslide instrument [2]. GNES transmitters in this landslide application use five frequency pairs (FP), namely 112.5 Hz and 337.5 Hz; 112.5 Hz and 1012.5 Hz; 112.5 Hz and 3037.5 Hz; 337.5 Hz and 1012.5 Hz; 337.5 Hz and 3037.5 Hz as FP1, FP2, FP3, FP4 and FP5, respectively. This instrument can operate on other frequency pairs in the range of 0.01 Hz to more than 1 MHz because it uses an integrated XR2206 oscillator component. With this frequency selection, the GNES system can be set according to the frequency that matches the material and object of research [3, 4]. The frequency is to avoid environmental noise [5, 6] and to choosethe skindepth [7, 8]. The discontinuity technique is also used in metal defect sensors which are generally designed using non-destructive testing with array sensors to monitoring quantitative defects [9]. The metal defects could be detected by wavelet decomposition and spectrum analysis using the pulsed eddy current (PEC) technique [10]. Detection of discontinuities in the form of metal defects can also be detected and visualized using induction thermal imaging [11]. In the measurement of GNES, the variable obtained from this measurement is the voltage with the percent response. The graph obtained from this measurement data is then interpreted and the results compared with theoretical and experimental data and interpret results.
Thin plate discontinuities and defects (Fig. 1) will inhibit or reduce eddy current flow, thereby reducing reception at the receiving coil and increasing its effective impedance [12].
FIGURE 1. Cracks must interrupt the surface Eddy Current flow in Eddy current examination
MATERIALS AND METHOD Materials Including the Components
Materials of this research including the components are:
a. Aluminum plate Type E1, Type E2, Type E3, Type E4, normal plate, and wire netting.
b. GNES equipment system.
Supporting Equipment
Software, hardware, and laboratory equipment that equipped became supporting equipment are:
a. Embarcadero RAD Studio XE2 software, PCB Designer 1.5.4 and Electronic Workbench Version 5.12.
b. Spectrum analyzer, frequency counter, function generator, oscilloscope,electronictool set, drilling and cutting set.
Discontinuity as a fault model on the ground is represented by thin plates and wire netting. Discontinuity has a very significant contribution to the anomaly response and overburden response. The materials used in this study are aluminum thin plates which are grouped as Type E1, Type E2, Type E3, and Type E4 with dimensions of 20 cm x 20 cm (Fig. 2).
FIGURE 2. Anomaly and overburden for: a. Normal plate and Type E1, b. Type E2 and Type E3, c.Type E4 and wire netting.
RESULTS AND DISCUSSION
The Response Ratios (Secondary to Primary Fields) with the Frequency Pairs in Anomaly Position Point (AP)
The normal thin plate has an anomaly position (AP) with the secondary to primary field ratios (ܸௌΤܸோ) are 0.9, 0.80, 0.74, 0.84, 0.81, 0.82 for FP 1, FP 2, FP 3, FP 4, and FP 5, respectively. The discontinuity will increase the ratios of secondary to primary field for Type E1 anomaly compared to the normal thin plate i.e. 7.5%, 13.7%, 9.39%, 8.70%, and 3.91% for FP 1, FP 2, FP 3, FP 4, and FP 5, respectively in Table 1. The anomaly response will decrease in line with the rise of the ratios. The anomaly contrasts reduction series from the highest to the lowest are in the frequency pairs of FP 2, FP 3, FP 4, FP 1 and FP 5.
TABLE 1. The Response Ratios (Secondary to Primary Fields) with Various Frequencies in Anomaly Position Point (AP).
Frequency Pairs (FP)
Normal
Thin Plate Type E1 Type E2 Type E3 Type E4 Wire Netting
FP 1 0.90 0.97 0.97 1 0.98 0.988
FP 2 0.80 0.91 0.95 0.96 0.99 0.992
FP 3 0.74 0.81 0.85 0.89 0.94 0.958
FP 4 0.84 0.92 0.95 0.95 0.98 0.983
FP 5 0.81 0.84 0.91 0.92 0.95 0.982
Average 0.818167 0.89 0.93 0.95 0.97 0.981
The three of parallel discontinuities (Type E2) will increase the ratios of secondary to primary field for anomaly compared to the normal thin plate i.e. 8.06%, 18.71%, 14.93, 12.66%, and 11.73% for FP 1, FP 2, FP 3, FP 4, and
2cm
2cm 20cm
20cm
FP 5 respectively. The anomaly contrasts reduction series from the highest to the lowest are in the frequency pairs of FP 2, FP 3, FP 4, FP 5 and FP 1.
The four of parallel discontinuity will increase the ratios of secondary to primary field to anomaly Type E3 compared to the normal thin plate i.e. 11.11%, 20.27%, 20.93%, 13.15%, and 13.48% for FP 1, FP 2, FP 3, FP 4, and FP 5 respectively. The anomaly contrasts reduction series from the highest to the lowest are in the frequency pairs of FP 3, FP 2, FP 5, FP 4 and FP 1.
The nine of parallel discontinuity will increase the ratios of secondary to primary field to anomaly Type E4 compared to the normal thin plate i.e. 8.52%, 23.18%, 27.49%, 16.02%, and 17.59% for FP 1, FP 2, FP 3, FP 4, and FP 5 respectively. The anomaly contrasts reduction series from the highest to the lowest are in the frequency pairs of FP 3, FP 2, FP 5, FP 4 and FP 1.
In the wire netting anomaly setting we have the response pattern are also the same as the normal plate but smaller of ratio of secondary to primary fields.The 18x16 mesh of Aluminum wire netting will increase the ratios of secondary to primary field compared to the normal thin plate i.e. 9.814%, 23.701%, 30.090%, 16.716%, and 21.194% for FP 1, FP 2, FP 3, FP 4, and FP 5 respectively. The anomaly contrasts reduction series from the highest to the lowest are in the frequency pairs of FP 3, FP 2, FP 5, FP 4 and FP 1.
As the result that the anomaly contrast are maximum for the normal thin plate followed the Type E1, Type E2, Type E3, Type E4, and Wire Netting as the minimum in TABLE 1. The extreme anomaly reduction are taken place in the FP 2 for Type E1 and Type E2 anomaly, then in the FP 3 for anomaly Type 3, Type 4, and Wire Netting.
The position of the cross section point through P and Q point is caused by the end effect of the overburden. We have P point when the transmitter coil placed precisely above the end of the overburden and Q point if the receiver coil above the other end of the overburden. The values of ܸௌΤܸோ when the transmitter or receiver touching the end of the overburden is 1.
Wire Netting Overburden
The response of wire netting is almost the same as the normal of aluminum plate but the very small response signal will receive by the receiver coils compare to the aluminum plate. The series of the anomaly contrast for all of the frequency pairs (FP) from the highest to the lowest are FP 3, FP 5, FP 2, FP 4 and FP 1. The cross-sections points of the overburden for five of frequency pairs are 68 cm. The ratios of secondary and primary fields start from the higher contrasts to lower contrast are 0.9925 (FP 2), 0.99 (FP 1), 0.9825 (FP 4), 0.98 (FP 5), and 0.9675 (FP 3) in Table 2.
TABLE 2. Interpretation of Wire Netting Response.
Frequency Pairs (FP)
Diagonal Cross Sections
Point (cm)
The Ratio of Secondary to Primary
Fields (ࢂࡿΤࢂࡾ)
FP 1 68 0.99
FP 2 68 0.9925
FP 3 68 0.9675
FP 4 68 0.9825
FP 5 68 0.98
Average 68 0.9825
CONCLUSIONS
A small mass change would be a significant change inthe secondary and primary ratio from the eddy current.
The secondary voltage will be varying caused by the discontinuities but the primary field from the transmitter is constant. The primary and secondary field received by the receiver can be distinguishing because the two signals are different in phase. The best frequency pair used for the detection of the discontinuities according to the contrast of the response obtained is in frequency pair of 3 (FP3). It can be seen that the higherthe frequency difference of source and reference frequency, the higher the contrast level.
ACKNOWLEDGEMENTS
This work was funded by Syiah Kuala University, the Ministry of Research, Technology and Higher Education, in accordance with the assignment agreement for the implementation of research of University of Syiah Kuala Excellent Research in fiscal year 2019 Number: 268/UN11.2/PP/PNBP/SP3/2019 on 13 February 2019.
REFERENCES
1. Z. Zakaria, M. S. Surbakti, S. Syahreza, and M. Z. M. Jafri, “Development of geometry normalized electromagnetic system (GNES) instrument for metal defect detection,” in High-Performance Computing in Geoscience and Remote Sensing VII-2017, IOP Conference Proceedings, edited by B. Huanget al. (Institute of Physics, Bristol, England, 2017), p. 104300J.
2. M. S. Surbakti, B. Bukhari, N. Ismail, N. Idris, E. Yusibani, M. Isa, and S. Syahreza, “Multi-frequency effect towards high conductivity overburden responses using vertical coplanar (VCP) coil configuration for landslide instrumentation,” in Journal of Physics: Conference Series-2018, IOP Conference Proceedings, edited by E.
Coreraet al. (Institute of Physics, Bristol, England, 2018), p. 012069.
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5. G. M. Hoversten, “A comparison of time and frequency domain EM sounding techniques,” Ph.D thesis, California University, 1981.
6. B. K. Sternberg and R. W. NopperJr, U.S. Patent No. 4,613,821 (23 September 1986).
7. J. R. Wait, Geophysics,Geophysics 27(3), 382-385 (1962).
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10. X. Qiu, P. Zhang, and J. Wei, Sensors and Actuators A: Physical203, 272-281 (2013).
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12. J. Hansen, Insight 46(5), 279-281 (2004).
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