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Article

Graphene Nanoparticle-Based, Nitrate Ion Sensor Characteristics

by
Mohammad Taghi Ahmadi
1,*,
Morteza Bodaghzadeh
1,
Seyed Saeid Rahimian Koloor
2,3,* and
Michal Petrů
2
1
Nanotechnology Research Center, Nano-Physic Group, Physics Department, Urmia University, Urmia 5756151818, Iran
2
Institute for Nanomaterials, Advanced Technologies and Innovation, Technical University of Liberec, Studentská 2, 461 17 Liberec, Czech Republic
3
School of Mechanical Engineering, Universiti Teknologi Malaysia, Johor Bahru 81310, Malaysia
*
Authors to whom correspondence should be addressed.
Nanomaterials 2021, 11(1), 150; https://doi.org/10.3390/nano11010150
Submission received: 19 October 2020 / Revised: 24 December 2020 / Accepted: 5 January 2021 / Published: 9 January 2021
(This article belongs to the Special Issue Nanosensors)

Abstract

:
Gathering and sensing of nitrate ions in the environment due to the abundant use in industry and agriculture have become an important problem, which needs to be overcome. On the other hand, new materials such as carbon-based materials with unique properties have become an ideal choice in sensing technology. In this research, the high-density polyethylene (HDPE) polymer as a carbon source in the melted form was used and carbon nanoparticles in the form of a strand between two electrodes were analyzed. It was fabricated between copper electrodes by the pulsed arc discharge method. Subsequently, the constructed metal–nanoparticle–metal (MNM) contact was employed to recognize the nitrate ions. Therefore, NaNO3, Pb(NO3)2, Zn(NO3)2, and NH4NO3 samples as a usual pollutant of industrial and agricultural wastewater were examined. All nitrate compounds in ten different densities were tested and sensor I-V characteristic was investigated, which showed that all the aforesaid compounds were recognizable by the graphene nano-strand. Additionally, the proposed structure in the presence of ions was simulated and acceptable agreement between them was reported. Additionally, the proposed structure analytically was investigated, and a comparison study between the proposed model and measured results was carried out and realistic agreement reported.

1. Introduction

Nitrate ions are widespread in the environment due to their high solubility in most liquids. These ions are known as water pollutants, which can be found in industrial and agricultural wastewater and have been considered to be an important threat to environmental waters [1,2]. The main source of nitrate ions produced by the human is non-organic fertilizers, food preservatives, reactive in explosive materials, glass industry, and other chemical processes. In surface water, the normal amount of nitrate ions is in the order of a few tens of ppm, but a high density of these ions has been produced by agriculture and urban wastewater [3]. Nitrate ion accumulation in drinking water can lead to serious and dangerous disease [4,5,6,7]. Up until now, different methods such as fluorescent spectroscopy, Raman spectroscopy, and chromatography have been utilized to find nitrate ions, but they need complicated instruments and are expensive [8,9,10,11,12,13,14,15,16]. However, current-voltage analysis as a sensing element in three or two-terminal devices with high sensitivity, requiring cheap facilities and proper for direct analysis, have been focused on [17]. After the discovery of nanoscale carbon-based materials [18], many studies have been carried out to use them in electronic devices [19,20]. According to their geometry, they can be conductive or semiconductor, which has diversified their application in diodes, transistors, and sensors [21,22,23,24]. A carbon-based sensor, which converts one physical phenomenon to an electrical signal, can be employed in identification systems [25,26,27,28,29]. Among the studies that have concentrated on the utilization of various nanoparticles in nitrate/nitrite detection sensors in the recent five years, K.R. Venugopala Reddy et al. (2020) employed cobalt (II) tetra methyl-quinoline oxy bridged phthalocyanine carbon nanoparticles [30,31,32,33,34,35,36,37,38,39], and Kattar Hanane et al. (2020) suggested tetradodecyl ammonium nitrate (TDAN) application [31]. Additionally, more sensors by Saad S. M. Hassan et al. (2019) Multi-walled carbon nanotubes (MWCNTs) have been investigated [32]; Lei Wu et al. (2018) employed Cu2O/CNT composites [33]; Yi Zhang et al. (2018) proposed a Ag/Cu/MWNTs/GCE platform [34]; Abdel Hameed et al. (2018) supported Cu@Pt/Gr nanoparticles on graphene configuration [35]; the Ghanei-Motlagh Taher (2018) Ag/HNT/MoS2 arrangement was configured [36]; Yue Wan et al. (2017) approved the application of a AgNP/MWCNT/GCE structure [37]; Bagheri et al. (2017) hired a Cu/MWCNT/RGO/GCE assembly [38]; and finally, Menart et al. (2015) worked on AgPs [39]. However, in this research, a graphene nanoparticle-based strand was fabricated by the pulsed arc discharge method between two metal electrodes. Due to the Fermi-level difference between the metal electrodes and graphene nanoparticle-based strand, in the shaped sensor, a Schottky-barrier was formed and examined. By adding a small amount of nitrate ion impurity to the sensor, the number of carriers varied and the I-V characteristic was altered, which led to electrical resistance variability in the strand, therefore, the resistance deviation in the nanoparticles was used in the measurement of physical phenomena. Its advantages over other nitrite reported sensors in the form of low manufacturing cost, fast production speed, and high efficiency can be highlighted.

2. Experimental Measurements

The entire experimental setup for carbon nanoparticle growth is presented in Appendix A; however, the schematic of the fabricated graphene nanoparticles (GNPs) in the melted high density poly ethylene (HDPE) composite is shown in Figure 1. A pulsed arc discharge method is employed in the presented work. In this mechanism, the voltage between two metal electrodes can be changed from 1–20 KV in low sequences.
Two metal electrodes fixed on a glass substrate for easy nitrate ion injection into the sensor, hollow stainless-steel electrodes were employed. Three arrangements in the placement of electrodes on the substrate can be recognized such as plane to plane (PTP), tip to the plane (TTP), and tip to tip (TTT) configurations, which deepens the electrode shape. To increase the growth rate in the presented work, the TTT was employed. To synthesize stable carbon nanoparticles, melted high-density polyethylene (HDPE, (C2H4)n), due to a large number of carbon atoms in its chain, was used as a carbon source between the two electrodes. At atmospheric pressure, the HDPE was melted and placed between two electrodes. The high electric field graphene nanoparticles were synthesized between two electrodes within 24 s at the voltage of about 4.4 kV. Initially, the fabricated strand was analyzed by the nano-focus (Mahr Metering Systems GmbH, Göttingen, Germany) as shown in Figure 2e, which indicates the topological presence of carbon nanoparticles in the sensor. For a closer look, images of the scanning electron microscope (SEM) (TESCAN, Brno, Czech Republic) were taken as depicted in Figure 2a for 200 nm, Figure 2b for 500 nm, Figure 2c for 1000 nm, and Figure 2d for 2000 nm.
Among the various kinds of carbon nanoparticles, graphite, graphene, and CNTs, particularly the high electrical conductivity of CNTs, have been reported. Additionally, based on the results presented by [40,41,42] and a comparison of the scanning electron microscopy (SEM) images in Figure 2a–d with SEM images taken by [43], coated CNTs by HDPE can be concluded similarly to the composites presented in [43]. Furthermore, bundled multiwall carbon nanotubes (MWCNTs) coated by HDPE chains with a similar manufacturing process have also been explained in our previous works [43]. Moreover, the Fourier transform infrared (FTIR) analysis as shown in Figure 2f indicates the composite form of GNPs in HDPE. The peaks at 2926 cm−1 and 2853 cm−1 and 725 cm−1 signify the CH2 groups in hydrocarbons [43]. The peak at 3443 cm−1 [43] and 3412 cm−1 [44] in the Fourier transform infrared (FTIR) (JASCO, Easton, MD, USA) spectrum of the GNPs can be assigned to the O-H vibration in the carboxyl group and the peaks at 1020–1090 cm−1 can be assigned to CNT-COOH and peaks at 1120 cm−1 signify the C=C, CNT, and the backbone of carbon nanotubes and peaks at 3700–3800 cm−1 can be assigned to CNT, OH groups from the unbound [45]. Based on research in [43,44,45,46,47,48,49] and a comparison with the FTIR analysis taken from the sample, it can be concluded that the carbon nanoparticles grown also contained multiwall carbon nanotubes and GNPs.
After the growth of carbon nanoparticles between two electrodes, to examine their sensing phenomenon, solutions prepared in 10 different concentrations of four nitrate ions—NaNO3, Pb(NO3)2, Zn(NO3)2, and NH4NO3 in distilled water—for injection into the built sensor and the identification of nitrate ions tested. Therefore, the amount of nitrate ions in each solution was measured and prepared according to the minimum allowable amount of different nitrate ions in drinking water in the World Health Organization (WHO) guidelines [50]. First of all, NaNO3, as a common water pollutant from agricultural and industrial activities in 10 solutions was tested. To prepare the desired solution, the required amount of NaNO3 was measured and dissolved in distilled water. The 50 ppm, 100 ppm, 200 ppm, 500 ppm, 1000 ppm, 2000 ppm, 3000 ppm, 4000 ppm, and 5000 ppm solutions were selected.
A current-voltage curve was taken from the fabricated sensor before ion injection and then each solution was injected into the device and subsequently an I-V curve was taken for each one. The I-V characteristic of the experimental data for this sensor without/with different NaNO3 concentrations is plotted in Figure 3, which indicates that the sensor current-voltage characteristic is affected by NaNO3 ion concentrations. The experimental results can be fitted by the Fourier model as:
f(x) = a0 + a1cos(xw) + b1sin(xw) + a2cos(2xw) + b2sin(2xw) + a3cos(3xw) + b3sin(3xw) + a4cos(4xw) + b4sin(4xw) + a5cos(5xw) + b5sin(5xw) + a6cos(6xw) + b6sin(6xw) + a7cos(7xw) + b7sin(7xw) + a8cos(8xw) + b8sin(8xw)
where the fitting parameters (a0–8, b1–8, w) are calculated as shown in Table 1 for NaNO3.
Based on the tabulated Fourier model (Table 1), the values for fitting parameters with corresponding regressions of NaNO3 exposure were re-plotted as shown in Figure 4.
Another common water pollutant, namely NH4NO3, has many applications in agricultural fertilizers and explosives production, is known as a nitrate ion source, and needs to be considered [38]. Therefore, ten NH4NO3 solutions prepared like the previous sample and injected to the sensitive region of sensor and sensor response to the NH4NO3 ions were plotted as shown in Figure 5.
To compare the efficacy of these ion concentrations on the sensor operation, fitting parameters for NH4NO3 were calculated from the Fourier model as shown in Table 2.
When the fitting parameters for each concentration were calculated, the proper linear I-V characteristic was re-plotted as shown in Figure 6.
Like the sodium nitrate by concentration, the current also lifted on the ammonium nitrate (NH4NO3), and this similarity can be described by the ion concentration gradient.
Lead nitrate can be leaked to the environment from industrial activities, especially from battery manufacturing companies, which needs to be investigated carefully. Therefore, lead nitrate Pb(NO3)2 was tested with the same concentration as other nitrate ions, and the experimental response is plotted as shown in Figure 7.
Again, the Fourier model was used for fitting, and lead nitrate-related fitting parameters were carried out as shown in Table 3.
To obtain the comparable scale in current-voltage relation according to the experimental outcomes, lead nitrate fitting parameters were employed and the I-V performance of the fabricated sensor was plotted as depicted in Figure 8.
Finally, ten solutions of zinc nitrate (Zn(NO3)2) were tested by the proposed sensor mechanism for 0 ppm, 50 ppm, 100 ppm, 200 ppm, 500 ppm, 1000 ppm, 2000 ppm, 3000 ppm, 4000 ppm, and 5000 ppm concentrations, the outcomes of which are reported in Figure 9.
In the zinc nitrate case, the best results on regressions were also obtained from the Fourier model, therefore the same fitting model was used and fitting parameters corresponding to the Zn(NO3)2 are tabulated in Table 4.
As a final point, the Zn(NO3)2 corresponding fitted current-voltage characteristic was plotted and a sensor behavior assessment was carried out as shown in Figure 10.
Like the other nitrate ions under different ion concentrations, the variation in the current-voltage characteristic was also analyzed for the zinc nitrate solution. The solution concentration effect of the graphene nanoparticle-based sensor in the attendance of nitrate family was almost the same by other nitrate ions. In the other words, by increasing the solution concentration for all nitrate ions, the current was increased, as shown in Figure 4, Figure 6, Figure 8 and Figure 10, which can be described by the same ion creation in the sensing region. Additionally, a comparison study between different nitrate families indicated that current variation under sodium nitrate exposure was lower than other nitrates and ammonium nitrate demonstrated a larger variation in I-V characteristics. It can be deduced that the graphene nanoparticle strand illustrated more sensitivity to ammonium nitrate compounds.

3. Simulation Study

Due to the limitations of the simulator, the simulation study could only be undertaken for the carbon nanotube-based sensors. Therefore, in the simulator, a carbon nanotube (CNT) with chirality (4,4) was positioned on top of a dielectric that was controlled by a metal gate under the dielectric. Ideally, nitrate ion impurities placed around the designed channel region and the device function in the attendance of nitrate ions were examined. First, a bare CNT semi-field effect transistor (CNTFET) was designed (Figure 11a) and its I-V characteristic was carried out in the original form (Figure 11b) and fitted form (Figure 11c) is reported in Figure 11.
In all samples, carbon nanotubes (4,4), which are a conductive nanotube, were used and the C–C bond length in all samples was selected as about 1.42086 A° and the repeated number for the nanotube length was set as C = 6. The lattice parameters were performed by the software itself for each given transistor and then fitted automatically to optimize the lattice. The left and right electrodes were considered to be metal, with a thickness of 2 A°. For each structure, two gates were placed under the simulated carbon nanotube. The metal gate was located at the bottom with a height of 1 A° and a voltage of 1 Volt was applied.
Initially, sodium nitrate was placed at the interaction with the carbon nanotube field-effect transistor (CNTFET) channel and the structure was optimized by the software Optimizer to allow all grafting to apply its effect on the channel region, and then the entire structure was relaxed. At room temperature, a voltage of 0–2 V was applied. Subsequently, the current-voltage feature was analyzed and fitted by MATLAB software as shown in Figure 12.
Similar to sodium nitrate, ammonium nitrate (Figure 13a–c), lead nitrate (Figure 13d–f), and zinc nitrate (Figure 13g–i) were proposed to the CNTFET channel at room temperature as shown in Figure 13.

4. Results and Discussion

To analyze the effect of analyte concentration on the fabricated sensor, in a certain voltage, the sensor responses for different pollutions were extracted from corresponding Figure 4, Figure 6, Figure 8 and Figure 10. Subsequently, its current at a specified voltage (1 V) for each pollutant, namely NaNO3, Pb(NO3)2, Zn(NO3)2, and NH4NO3 ions in concentrations of 50 ppm, 100 ppm, 200 ppm, 500 ppm, 1000 ppm, 2000 ppm, 3000 ppm, 4000 ppm, and 5000 ppm was calculated and plotted as shown in Figure 14. It can be concluded that by increasing the pollution concentration, the corresponding current was increased, which can be explained in the form of injected carrier increment in the sensitive region. It seems that all pollutants from this family follow the same trends on graphene-based metal–semiconductor–metal (MSM) structures.
Finally, to compare the simulation results, all simulated sensors on the FET platform were plotted in one graph as reported in Figure 15.
Since the simulated platform was not similar to the fabricated graphene nanoparticle-based sensor, therefore perfect agreement was not expected. However, for higher applied voltages, the higher current, the same as the fabricated device, was absorbed, which is related to the ammonium nitrate followed by zinc nitrate and lead nitrate; the lowest level current belonged to sodium nitrate. As the last point, the current–voltage model in the FET platform was tested with the sodium nitrate sensor as an example of a nitrate family sensor, and acceptable agreement between the FET regular model (Equation (2)) and the fabricated sensor is reported as shown in Figure 16.
I   =   N c F 1 2   ( η ) . qV
where Nc is the effective density of state of graphene-based materials; q = 1.602 × 10−19 is an electron electric charge; F 1 2 (η) is the Fermi integral of order (−1/2); and V is the carrier velocity [29]. Additionally, the proposed model was compared with the experimental and simulated results as shown in Figure 16, but a discrepancy in the different conditions was detected.
It can be concluded that the proposed model is accurate for an ideal case, but simulation results due to software boundary can be adopted for carbon-based devices. However, the fabricated device can be assumed as several parallel carbon nanoparticles-based devices, therefore, a discrepancy was observed with a minimum value of sodium nitrate, as shown in Figure 16.

5. Conclusions

Nitrate ions, as the main industrial and agricultural contaminations, are direct indicators on human health, therefore detection and gathering these ions from the environment are critical issues that need to be overcome. Moreover, new materials such as graphene nanoparticles in the application of this process have been encouraged. In this research, high-density graphene nanoparticles fabricated from a polyethylene polymer in strand form as a sensing environment was employed. Therefore, the current–voltage characteristic of metal–nanoparticle–metal (MNM) contact in the presence of nitrate ions such as NaNO3, Pb(NO3)2, Zn(NO3)2, and NH4NO3 was explored. Additionally, graphene nanoparticle-based sensor experimental results were compared with the simulation and theoretical model. It was concluded that sodium nitrate ions under identical applied voltage produce less current between nitrate families, which can vary from 0 up to 10 mA. The current variation under lead nitrate was about 0–14 mA and zinc nitrate indicated a current variation of about 0–16 mA, which is closer to the lead nitrate effect. However, the current deviation in the graphene strand for ammonium nitrate was 2.5 times greater than sodium nitrate, 1.79 times of lead nitrate, and 1.56 times than that of zinc nitrate. Therefore, a graphene nanoparticle strand structure as a sensing platform in the ionized medium is suggested.

Author Contributions

Conceptualization, M.T.A.; methodology, M.T.A., and M.B.; software, M.T.A., and M.B.; validation, M.T.A., and S.S.R.K.; formal analysis, M.T.A., and M.B.; investigation, M.T.A., and M.B.; resources, M.T.A., S.S.R.K., and M.P.; data curation, M.B.; writing—original draft preparation, M.T.A., and M.B.; writing—review and editing, M.T.A., M.B., and S.S.R.K.,; visualization, M.T.A., M.B., S.S.R.K., and M.P.; validation, M.T.A., M.B., S.S.R.K., and M.P.; supervision, M.T.A., and M.P.; project administration, M.T.A., S.S.R.K., and M.P.; funding acquisition, S.S.R.K., and M.P. All authors have read and agreed to the published version of the manuscript.

Funding

This research received no external funding.

Institutional Review Board Statement

Not applicable.

Informed Consent Statement

Not applicable.

Data Availability Statement

Data available in a publicly accessible repository.

Acknowledgments

The research was supported by the Ministry of Education, Youth, and Sports of the Czech Republic and the European Union (European Structural and Investment Funds Operational Program Research, Development, and Education) in the framework of the project “Modular platform for autonomous chassis of specialized electric vehicles for freight and equipment transportation”, Reg. No. CZ.02.1.01/0.0/0.0/16_025/0007293 as well as the financial support from internal grants from the Institute for Nanomaterials, Advanced Technologies, and Innovations (CXI), Technical University of Liberec (TUL).

Conflicts of Interest

The authors declare no conflict of interest.

Abbreviations

High-Density Polyethylene(HDPE)
Nano-Particles(GNPs)
Metal–Nanoparticle–Metal(MNM)
Current-Voltage(I-V)
Plane to Plane(PTP)
Tip to Plane(TTP)
Tip to Tip(TTT)
Scanning Electron Microscope(SEM)
Fourier-Transform Infrared spectroscopy(FTIR)
Carbon Nanotubes(CNTs)
Multiwall Carbon Nanotubes(MWCNTs)
Ammonium Nitrate(AN)
Carbon Nanotube Field Effect Transistor(CNTFET)

Appendix A

Figure A1. Complete experimental setup for GNP growth.
Figure A1. Complete experimental setup for GNP growth.
Nanomaterials 11 00150 g0a1
Figure A2. Experimental fabrication schematic diagram.
Figure A2. Experimental fabrication schematic diagram.
Nanomaterials 11 00150 g0a2

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Figure 1. Schematic of fabricated graphene nanoparticle/high density poly ethylene (GNP/HDPE) composite between two metallic electrodes.
Figure 1. Schematic of fabricated graphene nanoparticle/high density poly ethylene (GNP/HDPE) composite between two metallic electrodes.
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Figure 2. Scanning electron microscopy (SEM) photograph of Multi-walled carbon nanotubes/ high-density polyethylene (MWCNT/HDPE) nanocomposite sample. Imaging mode (a) ×100,000 at 15 KV, (b) ×60,000 at 15 KV, (c) ×40,000 at 15 KV, (d) ×17,400 at 15 KV and nano focus analysis of the sample (e) and Fourier transform infrared (FTIR) analysis of sample (f).
Figure 2. Scanning electron microscopy (SEM) photograph of Multi-walled carbon nanotubes/ high-density polyethylene (MWCNT/HDPE) nanocomposite sample. Imaging mode (a) ×100,000 at 15 KV, (b) ×60,000 at 15 KV, (c) ×40,000 at 15 KV, (d) ×17,400 at 15 KV and nano focus analysis of the sample (e) and Fourier transform infrared (FTIR) analysis of sample (f).
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Figure 3. Current-voltage (I-V) characteristic of experimental data for the proposed sensor without/with nine different NaNO3 concentrations.
Figure 3. Current-voltage (I-V) characteristic of experimental data for the proposed sensor without/with nine different NaNO3 concentrations.
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Figure 4. Fitted I-V characteristic of the experimental data with the Fourier model for the proposed sensor without NaNO3 exposure (a) and after injecting NaNO3 ions for nine different densities of (b) 50 ppm, (c) 100 ppm, (d) 200 ppm, (e) 500 ppm, (f) 1000 ppm, (g) 2000 ppm, (h) 3000 ppm, (i) 4000 ppm, and (j) 5000 ppm.
Figure 4. Fitted I-V characteristic of the experimental data with the Fourier model for the proposed sensor without NaNO3 exposure (a) and after injecting NaNO3 ions for nine different densities of (b) 50 ppm, (c) 100 ppm, (d) 200 ppm, (e) 500 ppm, (f) 1000 ppm, (g) 2000 ppm, (h) 3000 ppm, (i) 4000 ppm, and (j) 5000 ppm.
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Figure 5. I-V characteristic of experimental data for the proposed sensor without/with ten different NH4NO3 concentrations.
Figure 5. I-V characteristic of experimental data for the proposed sensor without/with ten different NH4NO3 concentrations.
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Figure 6. Fitted I-V diagram of experimental data with Fourier model for the proposed sensor without NH4NO3 exposure (a) and after injecting NH4NO3 ions for nine different densities (b) 50 ppm, (c) 100 ppm, (d) 200 ppm, (e) 500 ppm, (f) 1000 ppm, (g) 2000 ppm, (h) 3000 ppm, (i) 4000 ppm, (j) 5000 ppm.
Figure 6. Fitted I-V diagram of experimental data with Fourier model for the proposed sensor without NH4NO3 exposure (a) and after injecting NH4NO3 ions for nine different densities (b) 50 ppm, (c) 100 ppm, (d) 200 ppm, (e) 500 ppm, (f) 1000 ppm, (g) 2000 ppm, (h) 3000 ppm, (i) 4000 ppm, (j) 5000 ppm.
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Figure 7. I-V diagram of experimental data for the proposed sensor without/with ten different Pb(NO3)2 concentrations.
Figure 7. I-V diagram of experimental data for the proposed sensor without/with ten different Pb(NO3)2 concentrations.
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Figure 8. Fitted I-V diagram of the experimental data with the Fourier model for the proposed sensor without Pb(NO3)2 exposure (a) and after injecting Pb(NO3)2 ions for nine different densities of (b) 50 ppm, (c) 100 ppm, (d) 200 ppm, (e) 500 ppm, (f) 1000 ppm, (g) 2000 ppm, (h) 3000 ppm, (i) 4000 ppm, and (j) 5000 ppm.
Figure 8. Fitted I-V diagram of the experimental data with the Fourier model for the proposed sensor without Pb(NO3)2 exposure (a) and after injecting Pb(NO3)2 ions for nine different densities of (b) 50 ppm, (c) 100 ppm, (d) 200 ppm, (e) 500 ppm, (f) 1000 ppm, (g) 2000 ppm, (h) 3000 ppm, (i) 4000 ppm, and (j) 5000 ppm.
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Figure 9. I-V diagram of experimental data for the proposed sensor without/with ten different Zn(NO3)2 concentrations.
Figure 9. I-V diagram of experimental data for the proposed sensor without/with ten different Zn(NO3)2 concentrations.
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Figure 10. Fitted I-V diagram of experimental data with the Fourier model for the proposed sensor without Zn(NO3)2 exposure (a) and after injecting Zn(NO3)2 ions for nine different densities of (b) 50 ppm, (c) 100 ppm, (d) 200 ppm, (e) 500 ppm, (f) 1000 ppm, (g) 2000 ppm, (h) 3000 ppm, (i) 4000 ppm, (j) 5000 ppm.
Figure 10. Fitted I-V diagram of experimental data with the Fourier model for the proposed sensor without Zn(NO3)2 exposure (a) and after injecting Zn(NO3)2 ions for nine different densities of (b) 50 ppm, (c) 100 ppm, (d) 200 ppm, (e) 500 ppm, (f) 1000 ppm, (g) 2000 ppm, (h) 3000 ppm, (i) 4000 ppm, (j) 5000 ppm.
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Figure 11. (a) Designed carbon nanotube field-effect transistor (CNTFET) for CNT (4,4), (b) simulated I-V characteristic without ion exposure, (c) Fourier fitted I-V characteristic without ion exposure.
Figure 11. (a) Designed carbon nanotube field-effect transistor (CNTFET) for CNT (4,4), (b) simulated I-V characteristic without ion exposure, (c) Fourier fitted I-V characteristic without ion exposure.
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Figure 12. (a) Designed CNTFET for CNT (4,4) with attached sodium nitrate, (b) simulated I-V characteristic with NaNO3 exposure, (c) Fourier fitted I-V characteristic with NaNO3.
Figure 12. (a) Designed CNTFET for CNT (4,4) with attached sodium nitrate, (b) simulated I-V characteristic with NaNO3 exposure, (c) Fourier fitted I-V characteristic with NaNO3.
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Figure 13. Designed CNTFET device for CNT (4,4), with NH4NO3 (a), Pb(NO3)2 (b) Zn(NO3)2 (c) exposure. simulated I-V curve with NH4NO3 (d), Pb(NO3)2, (e) Zn(NO3)2, (f) exposure. Fourier fitted I-V characteristic with NH4NO3 (g), Pb(NO3)2 (h), Zn(NO3)2(O) (i) exposure.
Figure 13. Designed CNTFET device for CNT (4,4), with NH4NO3 (a), Pb(NO3)2 (b) Zn(NO3)2 (c) exposure. simulated I-V curve with NH4NO3 (d), Pb(NO3)2, (e) Zn(NO3)2, (f) exposure. Fourier fitted I-V characteristic with NH4NO3 (g), Pb(NO3)2 (h), Zn(NO3)2(O) (i) exposure.
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Figure 14. The relation of current-concentrations of the sensor at a specific voltage of 1 V for each of the NaNO3, Pb(NO3)2, Zn(NO3)2, and NH4NO3 ions in concentrations of 50 ppm, 100 ppm, 200 ppm, 500 ppm, 1000 ppm, 2000 ppm, 3000 ppm, 4000 ppm, and 5000 ppm.
Figure 14. The relation of current-concentrations of the sensor at a specific voltage of 1 V for each of the NaNO3, Pb(NO3)2, Zn(NO3)2, and NH4NO3 ions in concentrations of 50 ppm, 100 ppm, 200 ppm, 500 ppm, 1000 ppm, 2000 ppm, 3000 ppm, 4000 ppm, and 5000 ppm.
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Figure 15. All I-V simulations for the CNTFET based sensor without/with nitrate ions.
Figure 15. All I-V simulations for the CNTFET based sensor without/with nitrate ions.
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Figure 16. I-V characteristic curves for the experimental, simulation, and modeling data.
Figure 16. I-V characteristic curves for the experimental, simulation, and modeling data.
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Table 1. Values for parameters of the Fourier model and the corresponding regressions for NaNO3 exposure.
Table 1. Values for parameters of the Fourier model and the corresponding regressions for NaNO3 exposure.
General Model Fourier: f(x) = a0 + a1cos(xw) + b1sin(xw) + a2cos(2xw) + b2sin(2xw) + a3cos(3xw) + b3sin(3xw) + a4cos(4xw) + b4sin(4xw) + a5cos(5xw) + b5sin(5xw) + a6cos(6xw) + b6sin(6xw) + a7cos(7xw) + b7sin(7xw) + a8cos(8xw) + b8sin(8xw)
Without NaNO350 ppm
NaNO3
100 ppm
NaNO3
200 ppm
NaNO3
500 ppm
NaNO3
1000 ppm
NaNO3
2000 ppm
NaNO3
3000 ppm
NaNO3
4000 ppm
NaNO3
5000 ppm
NaNO3
a02577−4.365 × 1091.6452.0492.8253.492−6.718 × 1010−7.474 × 10424.025.223
a1−32516.984 × 109−0.7392−1.475−1.272−1.5341.079 × 10116.264 × 104−4.804−2.429
b1−29163.161 × 109−0.9671−1.044−1.855−2.2015.253 × 10101.172 × 105−36.7−3.127
a2283.3−3.409 × 109−0.575−0.7861−1.003−1.122−5.268 × 10105.174 × 104−29.84−1.644
b22608−3.881 × 109−0.18570.267−0.265−0.4149−6.713 × 1010−7.71 × 1041.621−0.4729
a3624.77.667 × 108−0.3277−0.1439−0.4805−0.69011.012 × 1010−4.992 × 1040.7631−0.8112
b3−869.52.515 × 1090.10740.45910.21450.17244.668 × 1010−535220.60.2365
a4−261.91.259 × 108−0.12080.18−0.1587−0.27354.854 × 109734611.74−0.4314
b457.75−9.719 × 1080.19710.22720.22320.3322−2.006 × 10101.899 × 104−0.33510.3087
a527.35−1.329 × 1080.021840.1596−0.01027−0.0307−4.223 × 1093940−0.1503−0.1108
b515.432.152× 1080.1266−0.0075450.17520.25525.149 × 109−4321−5.3730.3882
a603.356 × 1070.052050.046540.073740.077061.372 × 109−1017−1.7950.09396
b60−2.263 × 1070.0422−0.071360.062530.1278−6.39 × 108−314.90.12810.1743
a70−2.985 × 1060.03−0.012110.027940.05692−2.166 × 1088.980.062850.07132
b705.101 × 1050.01038−0.03823−0.015280.02353−2.25 × 10692.40.31410.05917
a8000.01524−0.0177700.031331.321 × 107000.05525
b800−0.01990.00051030−0.0087496.461 × 10600−0.001115
w0.77380.43152.5242.2892.4852.4280.51591.0271.762.592
R20.999810.999610.99980.99990.99980.999810.9998
SSE0.00057790.00017080.01850.0023410.047670.025910.086880.099760.030640.153
RMSE0.0062070.0039410.023680.0070570.026280.018230.033160.033290.018350.03764
Table 2. Values for fitting parameters from the Fourier model and its corresponding regressions for NH4NO3 exposure.
Table 2. Values for fitting parameters from the Fourier model and its corresponding regressions for NH4NO3 exposure.
General Model Fourier: f(x) = a0 + a1cos(xw) + b1sin(xw) + a2cos(2xw) + b2sin(2xw) + a3cos(3xw) + b3sin(3xw) + a4cos(4xw) + b4sin(4xw) + a5cos(5xw) + b5sin(5xw) + a6cos(6xw) + b6sin(6xw) + a7cos(7xw) + b7sin(7xw) + a8cos(8xw) + b8sin(8xw)
Without NH4NO350 ppm
NH4NO3
100 ppm
NH4NO3
200 ppm
NH4NO3
500 ppm
NH4NO3
1000 ppm
NH4NO3
2000 ppm
NH4NO3
3000 ppm
NH4NO3
4000 ppm
NH4NO3
5000 ppm
NH4NO3
a025771.907−5.103 × 1096.2666.7156.618−4.655 × 1067.38111.7311.23
a1−3251−0.55338.1 × 109−2.979−4.666−6.0124.44× 106−10.42−7.343−8.179
b1−2916−2.0463.832 × 109−3.901−3.432−2.7147.164 × 106−1.082−5.883−6.337
a2283.3−0.7164−3.829 × 109−2.174−2.345−2.2832.773 × 106−2.319−3.641−4.802
b22608−0.3164−4.668 × 109−0.53210.77762.101−5.586 × 1065.580.25121.815
a3624.7−0.40167.452 × 108−1.108−0.37240.5924−3.716 × 1062.811−1.127−0.6932
b3−869.50.071832.98 × 1090.51511.1961.7323.543 × 1053.2261.2582.86
a4−261.9−0.16942.241 × 108−0.33380.40251.1121.076 × 1062.83−0.1191.024
b457.750.06762−1.123 × 1090.65150.46510.10041.409 × 106−0.43640.86361.368
a527.35−0.1128−1.762 × 1080.11170.24530.30582.282 × 1050.69370.34340.9994
b515.430.16182.372 × 1080.3757−0.02259−0.5612−6.053 × 105−1.6740.34030.1117
a600.047414.171 × 1070.13990.02285−0.211−1.678 × 105−0.49290.17890.3885
b600.07607−2.222 × 1070.1197−0.08791−0.25583.396 × 104−0.8130.03491−0.3732
a700−3.531 × 1060.091890−0.12692.033 × 104−0.407300.05043
b7001.672 × 105−0.0191100.049762.13 × 104−0.017030−0.2131
a8000000.005272598.9−0.079720−0.02578
b8000000.03742−24110.11070−0.08339
w0.77382.5860.42142.4032.1292.1251.0322.1022.0442.291
R20.99980.997110.99980.999910.999810.99991
SSE0.00057790.28870.00018250.095080.053210.0008660.2740.076410.2950.1916
RMSE0.0062070.099780.0047760.079620.052920.0071370.074770.052240.09180.05089
Table 3. Values of the fitting parameters of the Fourier model and its corresponding regressions for Pb(NO3)2 exposure.
Table 3. Values of the fitting parameters of the Fourier model and its corresponding regressions for Pb(NO3)2 exposure.
General Model Fourier: f(x) = a0 + a1cos(xw) + b1sin(xw) + a2cos(2xw) + b2sin(2xw) + a3cos(3xw) + b3sin(3xw) + a4cos(4xw) + b4sin(4xw) + a5cos(5xw) + b5sin(5xw) + a6cos(6xw) + b6sin(6xw) + a7cos(7xw) + b7sin(7xw) + a8cos(8xw) + b8sin(8xw)
Without Pb(NO3)250 ppm
Pb(NO3)2
100 ppm
Pb(NO3)2
200 ppm
Pb(NO3)2
500 ppm
Pb(NO3)2
1000 ppm
Pb(NO3)2
2000 ppm
Pb(NO3)2
3000 ppm
Pb(NO3)2
4000 ppm
Pb(NO3)2
5000 ppm
Pb(NO3)2
a02577−9.734 × 108−192.81.5715.8623.135.4374.3677.2759.145
a1−32511.461 × 10973.86−0.94430.7388−1.163−1.114−2.161−2.69−6.585
b1−29169.46 × 108338.7−1.085−6.503−1.938−4.589−2.807−5.421−6.735
a2283.3−5.082 × 108222.6−0.5231−4.109−0.8636−2.563−1.751−3.8−6.326
b22608−1.132 × 109−104.2−0.06866−3.632−0.4929−1.831−0.1014−1.1651.942
a3624.7−1.054 × 108−83.05−0.2765−3.572−0.5539−2.153−0.7292−2.509−0.4802
b3−869.56.893 × 108−106.60.25091.209−0.14980.65290.56881.6855.391
a4−261.92.008 × 108−34.67−0.01229−0.286−0.354−0.4248−0.1055−0.058053.412
b457.75−2.268 × 10842.770.19862.280.17751.3350.57352.1251.687
a527.35−9.469 × 10713.630.10120.9668−0.17130.47450.18271.0861.597
b515.432.661 × 1076.5470.10310.64240.12670.58440.23690.7821−1.619
a602.152 × 1070.42140.068740.4006−0.04140.31860.13040.6822−0.4063
b606.588 × 106−2.1370.007466−0.22950.1633−0.039740.02699−0.2572−0.9014
a70−2.098 × 10600.02841−0.00066770.016720.028920.051480.08045−0.3317
b70−2.471 × 1060−0.03931−0.12620.0548−0.07618−0.02689−0.31620.0615
a802.989 × 1040−0.0123200.00364800−0.042080
b802.194 × 1050−0.0139200.065500−0.082740
w0.77380.51841.2452.4952.0032.5162.1322.3562.1751.911
R20.999810.99990.99960.99960.99990.99990.99990.99990.9999
SSE0.00057791.203 × 1050.0014870.014780.033130.012410.04060.047640.069050.158
RMSE0.0062070.0010010.0093540.033710.037150.023230.027170.030870.032850.04364
Table 4. Values for fitting parameters of the Fourier model and the corresponding regressions for Zn(NO3)2 exposure.
Table 4. Values for fitting parameters of the Fourier model and the corresponding regressions for Zn(NO3)2 exposure.
General Model Fourier: f(x) = a0 + a1cos(xw) + b1sin(xw) + a2cos(2xw) + b2sin(2xw) + a3cos(3xw) + b3sin(3xw) + a4cos(4xw) + b4sin(4xw) + a5cos(5xw) + b5sin(5xw) + a6cos(6xw) + b6sin(6xw) + a7cos(7xw) + b7sin(7xw) + a8cos(8xw) + b8sin(8xw)
Without Zn(NO3)250 ppm
Zn(NO3)2
100 ppm
Zn(NO3)2
200 ppm
Zn(NO3)2
500 ppm
Zn(NO3)2
1000 ppm
Zn(NO3)2
2000 ppm
Zn(NO3)2
3000 ppm
Zn(NO3)2
4000 ppm
Zn(NO3)2
5000 ppm
Zn(NO3)2
a02577129.52.1065.493 × 10102.852−1.08 × 1083.183−1.369 × 1082.712 × 109−2.359 × 1011
a1−325140.08−1.696−8.591 ×1010−1.5779.435 × 107−2.8011.66 × 108−3.726 × 1093.699 × 1011
b1−2916−234.8−0.9627−4.728 × 1010−1.5811.999 × 108−1.2462.148 × 108−3.254 × 1092.015 × 1011
a2283.3−181.1−0.70063.718 × 1010−1.1031.012 × 108−0.8512.335 × 1075.598 × 108−1.62 × 1011
b22608−66.260.45665.871 × 10100.07772−1.798 × 1080.917−2.338 × 1083.68 × 109−2.509 × 1011
a3624.7−67.730.03618−2.378 × 109−0.3309−1.469 × 1080.2801−1.025 × 1081.135 × 1091.243 × 1010
b3−869.5116.40.4209−3.862 × 10100.39193.64 × 1070.48451.153 × 108−1.956 × 1091.66 × 1011
a4−261.961.060.1922−7.092 × 1090.025237.287 × 1070.20126.899 × 107−9.907 × 1082.94 × 1010
b457.7551.310.090111.5 × 10100.27493.957 × 107−0.06968−2.066 × 1074.143 × 108−6.517 × 1010
a527.3529.60.075814.294 × 1090.08147−1.199 × 107−0.01192−2.204 × 1073.722 × 108−1.823 × 1010
b515.43−25.25−0.06483−3.107 × 1090.06808−3.061 × 107−0.05002−4.96 × 1068.636 × 1071.382 × 1010
a60−7.76−0.01349−1.18 × 1090.05804−2.676 × 10603.251 × 106−6.438 × 1075.083 × 109
b60−12.73−0.034191.466 × 108−0.0019368.545 × 10602.794 × 106−7.057 × 107−7.723 × 108
a70−3.7201.554 × 10801.239 × 1060−1.41 × 1052.277 × 100−6.823 × 108
b701.58106.189 × 1070−8.571 × 1050−3.456 × 1051.477 × 100−2.467 × 108
a800.14580−7.082 × 1060−1.185 × 105004.499 × 1053.216 × 107
b800.58530−8.59 × 1060−564000−1.006 × 1063.62 × 107
w0.77381.7962.1620.52362.130.62211.7580.43570.51080.521
R20.999810.99991111110.9998
SSE0.00057790.0018930.0010790.00030170.00071120.00026980.00028163.573 × 10−57.98 × 10−50.2171
RMSE0.0062070.019460.010390.0065650.01540.0051950.0068510.0029890.0036470.1042
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Ahmadi, M.T.; Bodaghzadeh, M.; Rahimian Koloor, S.S.; Petrů, M. Graphene Nanoparticle-Based, Nitrate Ion Sensor Characteristics. Nanomaterials 2021, 11, 150. https://doi.org/10.3390/nano11010150

AMA Style

Ahmadi MT, Bodaghzadeh M, Rahimian Koloor SS, Petrů M. Graphene Nanoparticle-Based, Nitrate Ion Sensor Characteristics. Nanomaterials. 2021; 11(1):150. https://doi.org/10.3390/nano11010150

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Ahmadi, Mohammad Taghi, Morteza Bodaghzadeh, Seyed Saeid Rahimian Koloor, and Michal Petrů. 2021. "Graphene Nanoparticle-Based, Nitrate Ion Sensor Characteristics" Nanomaterials 11, no. 1: 150. https://doi.org/10.3390/nano11010150

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