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TELKOMNIKA, Vol.16, No.5, October 2018, pp. 2239~2244
ISSN: 1693-6930, accredited First Grade by Kemenristekdikti, Decree No: 21/E/KPT/2018
DOI: 10.12928/TELKOMNIKA.v16i5.7592  2239
Received October 16, 2017; Revised July 23, 2018; Accepted August 16, 2018
Calibration of Geomagnetic and Soil Temperatur
Sensor for Earthquake Early Warning System
Dodi Yudo Setyawan*1
, Dona Yuliawati2
, Warsito3
, Warsono4
,
1
IIB Darmajaya, Computer Faculty, Computer System Department, Lampung, Indonesia
2
IIB Darmajaya, Computer Faculty, Informatian System Department, Lampung, Indonesia
3
Lampung University, Phisic Department Faculty of Mathematics and Natural Sciences,
Lampung, Indonesia
4
Lampung University, Mathematics Department Faculty of Mathematics and Natural Sciences,
Lampung, Indonesia
*Corresponding author, e-mail: dodi@darmajaya.ac.id
Abstract
The study of Design of Earthquake Early Warning System for Real Time Using Geomagnetism
and Total Electron Content with Fuzzy Logic through competitive grants scheme has obtained the
prototype of the earthquake early warning system. However, it still needs improvements on in the
calibration of thesensor system especially for MAG3110 sensor and DHT11 sensor. This calibration was
done by adjusting the sensor system to the existing measuring devices standards in the Physics
Department laboratory of the Sains Faculty Lampung University, to obtain measurement accuracyand to
get a good result about where and when the earthquake would occurand how strong the earthquake would
be. The calibration of MAG3110 sensor and DHT11 sensor obtained the standard correction results, the
standard deviation of MAG3110 from 3 axes, namely x axis was 8.5, y axis was 2.66, and z axis was 1.9,
whereas the standard deviation for DH11 sensor was 0.1161.
Keywords: calibration, earthquake, geomagnetism, total electron content, fuzzy logic
Copyright © 2018 Universitas Ahmad Dahlan. All rights reserved.
1. Introduction
Earthquakes are a natural phenomenon of the earth that potentialy destroys tall
buildings [1-4]. The study of Design of Earthquake Early Warning System for Real Time Using
Geomagnetism and Total Electron Content with Fuzzy Logic through competitive grants scheme
has obtained the prototypeof the earthquake early warning system [5] andit still needs
calibration for geomagneticuse of MAG3110 sensor and for soil temperature use of DHT11
sensor. The study of soil temperature sensor can use LM35 sensor and SHT11 sensor to
measure the temperature and the Relative Humidity (RH) [6-7]. Calibrating is checking and
adjusting the accuracy of the output of the measuring instrument or sensor by comparing it with
the standard/benchmark [8].
After the calibration it will obtain the characterization of the sensor. Another study of
calibration on sensor obtained the characterization of the sensor to know the characteristics of
carbon-polymer composite sensors tested with 9 types of gases, ie; Acetone, Nitrile Acetone,
Benzene, Ethanol, Methanol, Ethyl Acetone, Chloroform, n-Hexan and Toluene. The testing is
grouped into 4 clusters; selectivity, sensitivity, influence of temperature and humidity [9]. There
are several methods that can be used to perform the calibration, as an example is camera
calibration using orthogonal lines [10] and when it is difficult to make clock of the simulator
synchronized in the real time calibration wideband simulator, it can use deviation value on the
calibration as the sampling deviation [11]. In another study, to get the data from Very Low
Frequency (VLF) receiver is a high sensitivity receiver that is builtbased on AD744
Op-Amp [12]. In parameter calibration can provide references for flexible straw modeling and
parameters calibration of other crops, for terms of those three calibrated parameters exhibited
4.20% difference with the measured one [13].
 ISSN: 1693-6930
TELKOMNIKA Vol. 16, No. 5, October 2018: 2239-2244
2240
2. Research Method
The steps taken in this study are as follows:
a. Designing and constructing calibration models on magnetic fluxgate sensors, ground
temperature sensors with Secondary Reference Standard method.
b. Implementing the mathematical form for calibration process.
Working procedures in this research are as follows:
a. Preparing the Sheet of Calibration Result Report (CRL)
b. Recording number of calibration orders, equipment specifications, environmental
temperature conditions and information specified on the worksheet
c. Conducting initial check of sensor connection and sensor position.
d. Turning on standard indicators and sensor indicators to be calibrated.
e. Collecting data is then recorded in CRL as many as ten cycles with inteval ten minutes
f. Repeating steps for five different points until all the data is complete.
g. Turning off all equipment when it's done
3. Results and Analysis
3.1 Magnet Sensor MAG3110 Calibration Data (3 dimensions x, y, z)
The calibration data were conducted using MAG3110 in 5 cm depth. Tables 1-5 shows
the result of the calibration process.
No. Order : 0 Location : Lab. FisDas
Device : MAG3110 Environment condition : Fluxmagnet (µT)
Brand : Extrinsic Depth of measurement : 5 cm
Resolution : 0.10 T
Range : Full Scale Range 1000 T
Table 1. Depth 5 cm Area 2
Std (µT) MAG3110 (µT) Correction (µT)
X y z x y z x y z
1292 -455 365 1293 -451 362 1 1 2
1292 -454 365 1283 -456 365 10 2 0
1293 -454 365 1273 -457 365 20 3 0
1293 -454 365 1284 -456 367 9 2 -2
1293 -454 365 1291 -457 367 2 3 -2
1293 -454 365 1290 -457 368 3 3 -3
1293 -452 365 1290 -457 362 3 3 3
1293 -454 365 1290 -457 364 5 3 1
1293 -454 365 1287 -457 364 6 3 3
1293 -454 365 1286 -457 364 7 3 2
Table 2. Depth 5 cm Area 2
Std (µT) MAG3110 (µT) Correction (µT)
x y z x y z x y z
1292 -455 365 1293 -451 362 1 1 2
1293 -454 365 1283 -456 365 10 2 0
1293 -454 365 1273 -457 365 20 3 0
1293 -454 365 1284 -456 367 9 2 -2
1293 -454 365 1291 -457 367 2 3 -2
1293 -454 365 1290 -457 368 3 3 -3
1293 -452 365 1290 -457 362 3 3 3
1293 -454 365 1290 -457 364 5 3 1
1293 -454 365 1287 -457 364 6 3 1
1293 -454 365 1286 -457 364 7 3 1
Table 3. Depth 5 cm Area 3
Std (µT) MAG3110 (µT) Correction (µT)
x y z x y z x y z
1292 -455 365 1293 -455 362 1 0 2
1293 -454 365 1283 -456 365 10 2 0
1293 -454 365 1273 -457 365 20 3 0
1293 -454 365 1284 -456 367 9 2 -2
1293 -454 365 1291 -457 367 2 3 -2
1293 -454 365 1290 -457 368 3 3 -3
1293 -452 365 1290 -457 362 3 3 3
1293 -454 365 1290 -457 364 5 3 1
1293 -454 365 1287 -457 364 6 3 1
1293 -454 365 1286 -457 364 7 3 1
Table 4. Depth 5 cm Area 4
Std (µT) MAG3110 (µT) Correction (µT)
x y z x y z x y z
1292 -454 365 1293 -454 362 0 0 3
1293 -454 365 1283 -456 365 10 2 0
1293 -454 365 1273 -457 365 20 3 0
1293 -454 365 1284 -456 367 9 2 -2
1293 -454 365 1291 -457 367 2 3 -2
1293 -454 365 1290 -457 368 3 3 -3
1293 -452 365 1290 -457 362 3 3 3
1293 -454 365 1290 -457 364 5 3 1
1293 -454 365 1287 -457 364 6 3 1
1293 -454 365 1286 -457 364 7 3 1
TELKOMNIKA ISSN: 1693-6930 
Calibration of Geomagnetic and Soil Temperatur Sensor for …. (Dodi Yudo Setyawa)
2241
Table 5. Depth 5 cm Area 5
Std (µT) MAG3110 (µT) Correction (µT)
x y z x y z x y z
1293 -454 365 1293 -454 362 0 0 3
1293 -454 365 1283 -456 365 10 2 0
1293 -454 365 1273 -457 365 20 3 0
1293 -454 365 1284 -456 367 9 2 -2
1293 -454 365 1291 -457 367 2 3 -2
1293 -454 365 1290 -457 368 3 3 -3
1293 -454 365 1290 -457 362 3 3 3
1293 -454 365 1290 -457 364 3 3 1
1293 -454 365 1287 -457 364 6 3 1
1293 -454 365 1286 -457 364 7 3 1
From the Tables 1-5 data, the average correction of the x coordinates of the reading of the
device taken from the sensor is:
𝐷̅ 𝑥 =
0 + 10 + 20 + 9 + 2 + 3 + 3 + 3 + 6 + 7
10
𝐷𝑥̅̅̅̅ = 6,3
The standard deviation for the x coordinate of the device can be calculated in the following way
𝜎 = √
∑(𝐷𝑥̅̅̅̅1 − 𝐷𝑥̅̅̅̅)2
𝑛
𝜎 = √
(0 − 6,3)2+(10 − 6,3)2 + ⋯
10
𝜎 = 8,5
Then:
Average correction : 6.3
Standard Deviation of the correction : 8.5
Minimum tool correction : 0
From the Tables 1-5 data, the average correction of the y coordinates of the reading of the
device taken from the sensor is
𝐷̅ 𝑦 =
0 + 2 + 3 + 2 + 3 + 3 + 3 + 3 + 3 + 3
10
𝐷𝑦̅̅̅̅ = 2,5
The standard deviation for the y coordinate of the device can be calculated in the following way
𝜎 = √
∑(𝐷𝑦̅̅̅̅1 − 𝐷𝑦̅̅̅̅)2
𝑛
𝜎 = √
(0 − 2,5)2+(2 − 2,5)2 + ⋯
10
𝜎 = 2,66
Then:
Average correction : 2,5
Standard Deviation of the correction : 2,66
Minimum tool correction : 0
From the Tables 1-5 data, the average correction of the z coordinates of the reading of the
device taken from the sensor is
 ISSN: 1693-6930
TELKOMNIKA Vol. 16, No. 5, October 2018: 2239-2244
2242
𝐷̅ 𝑧 =
3 + 0 + 0 − 2 − 2 − 3 + 3 + 1 + 1 + 1
10
𝐷𝑧̅̅̅̅ = 0,2
The standard deviation for the z coordinate of the device can be calculated in the following way
𝜎 = √
∑(𝐷𝑧̅̅̅̅1 − 𝐷𝑧̅̅̅̅)2
𝑛
𝜎 = √
(3 − 0,2)2+(0 − 0,2)2 + ⋯
10
𝜎 = 1,9
Then:
Average correction : 0,2
Standard Deviation of the correction : 1,9
Minimum tool correction : -3
3.2 Calibration Data of DHT11 Sensor
The calibration data were conducted using DHT11 in 5 cm depth. Tables 6-10 shows
the result of the calibration process.
No. Order : 1 Location : Lab. FisDas
Device : DHT11 Environment condition : Temp (oC)
Brand : DFRobotDHT11 Depth of measurement : 5 cm
Resolution : 1 oC
Range : 0 - 50 oC
Table 6. Depth 5 cm Area 1
Std(o
C) DHT11(o
C) Correction(o
C)
24,98 25 -0,02
24,98 25 -0,02
24,98 25 -0,02
24,98 25 -0,02
24,98 25 -0,02
24,98 25 -0,02
24,98 25 -0,02
24,98 25 -0,02
24,98 25 -0,02
24,98 25 -0,02
Table 7. Depth 5 cm Area 2
Std(o
C) DHT11(o
C) Correction(o
C)
25,11 26 -0,89
25,11 26 -0,89
25,11 26 -0,89
25,11 26 -0,89
25,11 26 -0,89
25,11 26 -0,89
25,11 26 -0,89
25,11 26 -0,89
25,11 26 -0,89
25,11 26 -0,89
Table 8. Depth 5 cm Area 3
Std(o
C) DHT11(o
C) Correction(o
C)
25,25 26 -0,75
25,25 26 -0,75
25,25 26 -0,75
25,25 26 -0,75
25,25 26 -0,75
25,25 26 -0,75
25,25 26 -0,75
25,25 26 -0,75
25,25 26 -0,75
25,25 26 -0,75
Table 9. Depth 5 cm Area 4
Std(o
C) DHT11(o
C) Correction(o
C)
25,65 27 -1,35
25,65 27 -1,35
25,65 27 -1,35
25,65 27 -1,35
25,65 27 -1,35
25,65 27 -1,35
25,65 27 -1,35
25,65 27 -1,35
25,65 27 -1,35
25,65 27 -1,35
TELKOMNIKA ISSN: 1693-6930 
Calibration of Geomagnetic and Soil Temperatur Sensor for …. (Dodi Yudo Setyawa)
2243
Table 10. Depth 5 cm Area 5
Std(o
C) DHT11(o
C) Correction(o
C)
23,97 24 -0,03
23,97 24 -0,03
23,97 24 -0,03
23,97 24 -0,03
23,97 24 -0,03
23,97 24 -0,03
23,97 24 -0,03
23,97 24 -0,03
23,97 24 -0,03
23,97 24 -0,03
From the Tables 6-10 data, the average correction of the instrument reading taken from the
maximum temperature is:
𝐷̅ =
−1,35 − 1,35 − 1,35 − 1,35 − 1,35 − 1,35 − 1,35 − 1,35 − 1,35 − 1,35
10
𝐷̅ = −1,485
The standard deviation of the device can be calculated in following way
𝜎 = √
∑(𝐷̅1 − 𝐷̅)2
𝑛
𝜎 = √
(−1,35 + 1,485)2+(−1,35 + 1,485)2 + ⋯
10
𝜎 = 0,1161
Then:
Average correction : -1,485
Standard Deviation of the correction : 0,1161
Minimum tool correction : -0,02
4. Conclusion
The calibration of MAG3110 sensor and DHT11 sensor obtain the standard correction
results, the standard deviation of MAG3110 from 3 axes, namely x axis is 8.5 then y axis is 2.66
then z axis is 1.9, whereas the standard deviation for DH11 sensor is 0.1161. The calibration
data is expected to improve the earthquake early warning system.
References
[1] Murdiono at al. Intelligent Monitoring System on Prediction of Building Damage Index using Neural-
Network. TELKOMNIKA (Telecommunication Computing Electronics and Control).
2012; 10(1): 155-164.
[2] Seth Stein & Mian Liu, Long aftershock squences within continents and implications for earthquake
hazard assessment, Nature, London. 2009; 462(7269): 87-9.
[3] Liu, ChiChing; Linde, Alan T; Sacks, I Selwyn, Slow earthquakes triggered by typhoons,Nature;
London. 2009; 459(7248): 833-6.
[4] Nakai, Hisao; Itatani, Tomoya; Horiike, Ryo; Kyota, Kaoru; Tsukasaki, Keiko. PLoS ONE, Tsunami
evacuation simulation using geographic information systems for homecare recipients depending on
electric devices. 2018; 13(6): 18
[5] Setyawan DY, Zaidal N. Earthquake Early Warning System Real Time Design Using Total Electron
Content and Geomagnetism with Fuzzy Logic. IJCSI International Journal of Computer Science
Issues. 2014; 11(6,1): 38.
 ISSN: 1693-6930
TELKOMNIKA Vol. 16, No. 5, October 2018: 2239-2244
2244
[6] Jazi Eko Istiyanto, Eko Purwadi. Alat Pemantau Suhu Jarak Jauh Berbasis SMS (AN SMS-Based
Remotee Temperature Monitoring Device).TELKOMNIKA (Telecommunication Computing
Electronics and Control). 2006; 3(2): 95–99.
[7] Seno D Panjaitan at al. Telemonitoring Temperature and Humidity at Bio-energy Process using
Smart Phones. TELKOMNIKA (Telecommunication Computing Electronics and Control). 2016; 14(2):
762-771.
[8] Alan S Morris. Measurement and Instrumentation Principles. Third edition, Madras India, Planta A
Tree. 2001: 64.
[9] Budi Gunawan at al. Characterization of Polymeric Chemiresistors for Gas Sensor. TELKOMNIKA
(Telecommunication Computing Electronics and Control). 2012; 10(2): 275-280.
[10] Yue Zhao, Jianchong Lei. A Camera Self-Calibration Method Based on Plane Lattice and
Orthogonality. TELKOMNIKA (Telecommunication Computing Electronics and Control). 2013; 11(4):
767-774.
[11] Song Bingbing al al. Sampling Deviation Real-Time Calibration Method for Wideband Simulator.
TELKOMNIKA (Telecommunication Computing Electronics and Control). 2015; 13(2): 510–517.
[12] Achmad Munir al al. High Sensitivity Very Low Frequency Receiver for Earthquake Data Acquisition.
TELKOMNIKA (Telecommunication Computing Electronics and Control). 2017; 15(1): 150–155.
[13] Liu F Y, et al. Modeling of flexible wheat straw by discrete element method and its parameters
calibration, International Journal of Agricultural & Biological Engineering. 2018; 11(3): 42-46.

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Calibration of Geomagnetic and Soil Temperatur Sensor for Earthquake Early Warning System

  • 1. TELKOMNIKA, Vol.16, No.5, October 2018, pp. 2239~2244 ISSN: 1693-6930, accredited First Grade by Kemenristekdikti, Decree No: 21/E/KPT/2018 DOI: 10.12928/TELKOMNIKA.v16i5.7592  2239 Received October 16, 2017; Revised July 23, 2018; Accepted August 16, 2018 Calibration of Geomagnetic and Soil Temperatur Sensor for Earthquake Early Warning System Dodi Yudo Setyawan*1 , Dona Yuliawati2 , Warsito3 , Warsono4 , 1 IIB Darmajaya, Computer Faculty, Computer System Department, Lampung, Indonesia 2 IIB Darmajaya, Computer Faculty, Informatian System Department, Lampung, Indonesia 3 Lampung University, Phisic Department Faculty of Mathematics and Natural Sciences, Lampung, Indonesia 4 Lampung University, Mathematics Department Faculty of Mathematics and Natural Sciences, Lampung, Indonesia *Corresponding author, e-mail: dodi@darmajaya.ac.id Abstract The study of Design of Earthquake Early Warning System for Real Time Using Geomagnetism and Total Electron Content with Fuzzy Logic through competitive grants scheme has obtained the prototype of the earthquake early warning system. However, it still needs improvements on in the calibration of thesensor system especially for MAG3110 sensor and DHT11 sensor. This calibration was done by adjusting the sensor system to the existing measuring devices standards in the Physics Department laboratory of the Sains Faculty Lampung University, to obtain measurement accuracyand to get a good result about where and when the earthquake would occurand how strong the earthquake would be. The calibration of MAG3110 sensor and DHT11 sensor obtained the standard correction results, the standard deviation of MAG3110 from 3 axes, namely x axis was 8.5, y axis was 2.66, and z axis was 1.9, whereas the standard deviation for DH11 sensor was 0.1161. Keywords: calibration, earthquake, geomagnetism, total electron content, fuzzy logic Copyright © 2018 Universitas Ahmad Dahlan. All rights reserved. 1. Introduction Earthquakes are a natural phenomenon of the earth that potentialy destroys tall buildings [1-4]. The study of Design of Earthquake Early Warning System for Real Time Using Geomagnetism and Total Electron Content with Fuzzy Logic through competitive grants scheme has obtained the prototypeof the earthquake early warning system [5] andit still needs calibration for geomagneticuse of MAG3110 sensor and for soil temperature use of DHT11 sensor. The study of soil temperature sensor can use LM35 sensor and SHT11 sensor to measure the temperature and the Relative Humidity (RH) [6-7]. Calibrating is checking and adjusting the accuracy of the output of the measuring instrument or sensor by comparing it with the standard/benchmark [8]. After the calibration it will obtain the characterization of the sensor. Another study of calibration on sensor obtained the characterization of the sensor to know the characteristics of carbon-polymer composite sensors tested with 9 types of gases, ie; Acetone, Nitrile Acetone, Benzene, Ethanol, Methanol, Ethyl Acetone, Chloroform, n-Hexan and Toluene. The testing is grouped into 4 clusters; selectivity, sensitivity, influence of temperature and humidity [9]. There are several methods that can be used to perform the calibration, as an example is camera calibration using orthogonal lines [10] and when it is difficult to make clock of the simulator synchronized in the real time calibration wideband simulator, it can use deviation value on the calibration as the sampling deviation [11]. In another study, to get the data from Very Low Frequency (VLF) receiver is a high sensitivity receiver that is builtbased on AD744 Op-Amp [12]. In parameter calibration can provide references for flexible straw modeling and parameters calibration of other crops, for terms of those three calibrated parameters exhibited 4.20% difference with the measured one [13].
  • 2.  ISSN: 1693-6930 TELKOMNIKA Vol. 16, No. 5, October 2018: 2239-2244 2240 2. Research Method The steps taken in this study are as follows: a. Designing and constructing calibration models on magnetic fluxgate sensors, ground temperature sensors with Secondary Reference Standard method. b. Implementing the mathematical form for calibration process. Working procedures in this research are as follows: a. Preparing the Sheet of Calibration Result Report (CRL) b. Recording number of calibration orders, equipment specifications, environmental temperature conditions and information specified on the worksheet c. Conducting initial check of sensor connection and sensor position. d. Turning on standard indicators and sensor indicators to be calibrated. e. Collecting data is then recorded in CRL as many as ten cycles with inteval ten minutes f. Repeating steps for five different points until all the data is complete. g. Turning off all equipment when it's done 3. Results and Analysis 3.1 Magnet Sensor MAG3110 Calibration Data (3 dimensions x, y, z) The calibration data were conducted using MAG3110 in 5 cm depth. Tables 1-5 shows the result of the calibration process. No. Order : 0 Location : Lab. FisDas Device : MAG3110 Environment condition : Fluxmagnet (µT) Brand : Extrinsic Depth of measurement : 5 cm Resolution : 0.10 T Range : Full Scale Range 1000 T Table 1. Depth 5 cm Area 2 Std (µT) MAG3110 (µT) Correction (µT) X y z x y z x y z 1292 -455 365 1293 -451 362 1 1 2 1292 -454 365 1283 -456 365 10 2 0 1293 -454 365 1273 -457 365 20 3 0 1293 -454 365 1284 -456 367 9 2 -2 1293 -454 365 1291 -457 367 2 3 -2 1293 -454 365 1290 -457 368 3 3 -3 1293 -452 365 1290 -457 362 3 3 3 1293 -454 365 1290 -457 364 5 3 1 1293 -454 365 1287 -457 364 6 3 3 1293 -454 365 1286 -457 364 7 3 2 Table 2. Depth 5 cm Area 2 Std (µT) MAG3110 (µT) Correction (µT) x y z x y z x y z 1292 -455 365 1293 -451 362 1 1 2 1293 -454 365 1283 -456 365 10 2 0 1293 -454 365 1273 -457 365 20 3 0 1293 -454 365 1284 -456 367 9 2 -2 1293 -454 365 1291 -457 367 2 3 -2 1293 -454 365 1290 -457 368 3 3 -3 1293 -452 365 1290 -457 362 3 3 3 1293 -454 365 1290 -457 364 5 3 1 1293 -454 365 1287 -457 364 6 3 1 1293 -454 365 1286 -457 364 7 3 1 Table 3. Depth 5 cm Area 3 Std (µT) MAG3110 (µT) Correction (µT) x y z x y z x y z 1292 -455 365 1293 -455 362 1 0 2 1293 -454 365 1283 -456 365 10 2 0 1293 -454 365 1273 -457 365 20 3 0 1293 -454 365 1284 -456 367 9 2 -2 1293 -454 365 1291 -457 367 2 3 -2 1293 -454 365 1290 -457 368 3 3 -3 1293 -452 365 1290 -457 362 3 3 3 1293 -454 365 1290 -457 364 5 3 1 1293 -454 365 1287 -457 364 6 3 1 1293 -454 365 1286 -457 364 7 3 1 Table 4. Depth 5 cm Area 4 Std (µT) MAG3110 (µT) Correction (µT) x y z x y z x y z 1292 -454 365 1293 -454 362 0 0 3 1293 -454 365 1283 -456 365 10 2 0 1293 -454 365 1273 -457 365 20 3 0 1293 -454 365 1284 -456 367 9 2 -2 1293 -454 365 1291 -457 367 2 3 -2 1293 -454 365 1290 -457 368 3 3 -3 1293 -452 365 1290 -457 362 3 3 3 1293 -454 365 1290 -457 364 5 3 1 1293 -454 365 1287 -457 364 6 3 1 1293 -454 365 1286 -457 364 7 3 1
  • 3. TELKOMNIKA ISSN: 1693-6930  Calibration of Geomagnetic and Soil Temperatur Sensor for …. (Dodi Yudo Setyawa) 2241 Table 5. Depth 5 cm Area 5 Std (µT) MAG3110 (µT) Correction (µT) x y z x y z x y z 1293 -454 365 1293 -454 362 0 0 3 1293 -454 365 1283 -456 365 10 2 0 1293 -454 365 1273 -457 365 20 3 0 1293 -454 365 1284 -456 367 9 2 -2 1293 -454 365 1291 -457 367 2 3 -2 1293 -454 365 1290 -457 368 3 3 -3 1293 -454 365 1290 -457 362 3 3 3 1293 -454 365 1290 -457 364 3 3 1 1293 -454 365 1287 -457 364 6 3 1 1293 -454 365 1286 -457 364 7 3 1 From the Tables 1-5 data, the average correction of the x coordinates of the reading of the device taken from the sensor is: 𝐷̅ 𝑥 = 0 + 10 + 20 + 9 + 2 + 3 + 3 + 3 + 6 + 7 10 𝐷𝑥̅̅̅̅ = 6,3 The standard deviation for the x coordinate of the device can be calculated in the following way 𝜎 = √ ∑(𝐷𝑥̅̅̅̅1 − 𝐷𝑥̅̅̅̅)2 𝑛 𝜎 = √ (0 − 6,3)2+(10 − 6,3)2 + ⋯ 10 𝜎 = 8,5 Then: Average correction : 6.3 Standard Deviation of the correction : 8.5 Minimum tool correction : 0 From the Tables 1-5 data, the average correction of the y coordinates of the reading of the device taken from the sensor is 𝐷̅ 𝑦 = 0 + 2 + 3 + 2 + 3 + 3 + 3 + 3 + 3 + 3 10 𝐷𝑦̅̅̅̅ = 2,5 The standard deviation for the y coordinate of the device can be calculated in the following way 𝜎 = √ ∑(𝐷𝑦̅̅̅̅1 − 𝐷𝑦̅̅̅̅)2 𝑛 𝜎 = √ (0 − 2,5)2+(2 − 2,5)2 + ⋯ 10 𝜎 = 2,66 Then: Average correction : 2,5 Standard Deviation of the correction : 2,66 Minimum tool correction : 0 From the Tables 1-5 data, the average correction of the z coordinates of the reading of the device taken from the sensor is
  • 4.  ISSN: 1693-6930 TELKOMNIKA Vol. 16, No. 5, October 2018: 2239-2244 2242 𝐷̅ 𝑧 = 3 + 0 + 0 − 2 − 2 − 3 + 3 + 1 + 1 + 1 10 𝐷𝑧̅̅̅̅ = 0,2 The standard deviation for the z coordinate of the device can be calculated in the following way 𝜎 = √ ∑(𝐷𝑧̅̅̅̅1 − 𝐷𝑧̅̅̅̅)2 𝑛 𝜎 = √ (3 − 0,2)2+(0 − 0,2)2 + ⋯ 10 𝜎 = 1,9 Then: Average correction : 0,2 Standard Deviation of the correction : 1,9 Minimum tool correction : -3 3.2 Calibration Data of DHT11 Sensor The calibration data were conducted using DHT11 in 5 cm depth. Tables 6-10 shows the result of the calibration process. No. Order : 1 Location : Lab. FisDas Device : DHT11 Environment condition : Temp (oC) Brand : DFRobotDHT11 Depth of measurement : 5 cm Resolution : 1 oC Range : 0 - 50 oC Table 6. Depth 5 cm Area 1 Std(o C) DHT11(o C) Correction(o C) 24,98 25 -0,02 24,98 25 -0,02 24,98 25 -0,02 24,98 25 -0,02 24,98 25 -0,02 24,98 25 -0,02 24,98 25 -0,02 24,98 25 -0,02 24,98 25 -0,02 24,98 25 -0,02 Table 7. Depth 5 cm Area 2 Std(o C) DHT11(o C) Correction(o C) 25,11 26 -0,89 25,11 26 -0,89 25,11 26 -0,89 25,11 26 -0,89 25,11 26 -0,89 25,11 26 -0,89 25,11 26 -0,89 25,11 26 -0,89 25,11 26 -0,89 25,11 26 -0,89 Table 8. Depth 5 cm Area 3 Std(o C) DHT11(o C) Correction(o C) 25,25 26 -0,75 25,25 26 -0,75 25,25 26 -0,75 25,25 26 -0,75 25,25 26 -0,75 25,25 26 -0,75 25,25 26 -0,75 25,25 26 -0,75 25,25 26 -0,75 25,25 26 -0,75 Table 9. Depth 5 cm Area 4 Std(o C) DHT11(o C) Correction(o C) 25,65 27 -1,35 25,65 27 -1,35 25,65 27 -1,35 25,65 27 -1,35 25,65 27 -1,35 25,65 27 -1,35 25,65 27 -1,35 25,65 27 -1,35 25,65 27 -1,35 25,65 27 -1,35
  • 5. TELKOMNIKA ISSN: 1693-6930  Calibration of Geomagnetic and Soil Temperatur Sensor for …. (Dodi Yudo Setyawa) 2243 Table 10. Depth 5 cm Area 5 Std(o C) DHT11(o C) Correction(o C) 23,97 24 -0,03 23,97 24 -0,03 23,97 24 -0,03 23,97 24 -0,03 23,97 24 -0,03 23,97 24 -0,03 23,97 24 -0,03 23,97 24 -0,03 23,97 24 -0,03 23,97 24 -0,03 From the Tables 6-10 data, the average correction of the instrument reading taken from the maximum temperature is: 𝐷̅ = −1,35 − 1,35 − 1,35 − 1,35 − 1,35 − 1,35 − 1,35 − 1,35 − 1,35 − 1,35 10 𝐷̅ = −1,485 The standard deviation of the device can be calculated in following way 𝜎 = √ ∑(𝐷̅1 − 𝐷̅)2 𝑛 𝜎 = √ (−1,35 + 1,485)2+(−1,35 + 1,485)2 + ⋯ 10 𝜎 = 0,1161 Then: Average correction : -1,485 Standard Deviation of the correction : 0,1161 Minimum tool correction : -0,02 4. Conclusion The calibration of MAG3110 sensor and DHT11 sensor obtain the standard correction results, the standard deviation of MAG3110 from 3 axes, namely x axis is 8.5 then y axis is 2.66 then z axis is 1.9, whereas the standard deviation for DH11 sensor is 0.1161. The calibration data is expected to improve the earthquake early warning system. References [1] Murdiono at al. Intelligent Monitoring System on Prediction of Building Damage Index using Neural- Network. TELKOMNIKA (Telecommunication Computing Electronics and Control). 2012; 10(1): 155-164. [2] Seth Stein & Mian Liu, Long aftershock squences within continents and implications for earthquake hazard assessment, Nature, London. 2009; 462(7269): 87-9. [3] Liu, ChiChing; Linde, Alan T; Sacks, I Selwyn, Slow earthquakes triggered by typhoons,Nature; London. 2009; 459(7248): 833-6. [4] Nakai, Hisao; Itatani, Tomoya; Horiike, Ryo; Kyota, Kaoru; Tsukasaki, Keiko. PLoS ONE, Tsunami evacuation simulation using geographic information systems for homecare recipients depending on electric devices. 2018; 13(6): 18 [5] Setyawan DY, Zaidal N. Earthquake Early Warning System Real Time Design Using Total Electron Content and Geomagnetism with Fuzzy Logic. IJCSI International Journal of Computer Science Issues. 2014; 11(6,1): 38.
  • 6.  ISSN: 1693-6930 TELKOMNIKA Vol. 16, No. 5, October 2018: 2239-2244 2244 [6] Jazi Eko Istiyanto, Eko Purwadi. Alat Pemantau Suhu Jarak Jauh Berbasis SMS (AN SMS-Based Remotee Temperature Monitoring Device).TELKOMNIKA (Telecommunication Computing Electronics and Control). 2006; 3(2): 95–99. [7] Seno D Panjaitan at al. Telemonitoring Temperature and Humidity at Bio-energy Process using Smart Phones. TELKOMNIKA (Telecommunication Computing Electronics and Control). 2016; 14(2): 762-771. [8] Alan S Morris. Measurement and Instrumentation Principles. Third edition, Madras India, Planta A Tree. 2001: 64. [9] Budi Gunawan at al. Characterization of Polymeric Chemiresistors for Gas Sensor. TELKOMNIKA (Telecommunication Computing Electronics and Control). 2012; 10(2): 275-280. [10] Yue Zhao, Jianchong Lei. A Camera Self-Calibration Method Based on Plane Lattice and Orthogonality. TELKOMNIKA (Telecommunication Computing Electronics and Control). 2013; 11(4): 767-774. [11] Song Bingbing al al. Sampling Deviation Real-Time Calibration Method for Wideband Simulator. TELKOMNIKA (Telecommunication Computing Electronics and Control). 2015; 13(2): 510–517. [12] Achmad Munir al al. High Sensitivity Very Low Frequency Receiver for Earthquake Data Acquisition. TELKOMNIKA (Telecommunication Computing Electronics and Control). 2017; 15(1): 150–155. [13] Liu F Y, et al. Modeling of flexible wheat straw by discrete element method and its parameters calibration, International Journal of Agricultural & Biological Engineering. 2018; 11(3): 42-46.