# Influence of Gas Flow Rate on the Structural and Optical Properties of TiO₂ Prepared by Plasma Jet Technique

<figure><img src="image_1.png" /></figure>

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Mohammed Kh. Ibrahim<fnref n="1" /> ID, Bilal K. Al-Rawi<fnref n="2" />* ID

Corresponding Author Email: sc.bilal_alrawi@uoanbar.edu.iq

Copyright: ©2025 The authors. This article is published by IIETA and is licensed under the CC BY 4.0 license
(http://creativecommons.org/licenses/by/4.0/).

https://doi.org/10.18280/rcma.350404

## ABSTRACT

**Received:** 25 June 2025

**Revised:** 28 July 2025

**Accepted:** 20 August 2025

**Available online:** 31 August 2025

**Keywords:**

energy gap, optical properties, plasma jet, structural properties, titanium oxide

This presents TiO₂ thin film, preparation by Plasma Jet at two levels of gas flow for 1.5 L/min and 2 L/min. The properties of the obtained TiO₂ were explored. The TiO₂ in the thin film was further evidenced by EDX analysis with high Ti to O atomic concentration ratio and no element impurity was detected below the limit. The development of the TiO₂ thin film was confirmed by characterization techniques. X-ray diffraction (XRD) patterns revealed the presence of peaks related to TiO₂ of Rutile phase at planes of 110, 101, 111, 210, and 211° respectively. The different levels of flow of the gas and the effect on the properties of the Nanoparticles as characterized by XRD, FESEM and AFM showed that with the increase in flow the particle size increases and the value of root mean square (RMS) and average roughness also increases. Also for flow levels increasing the absorbance was observed in optical properties, and energy gap value was found as 3.16 for flow level 1.5 L/min and 3.08 for 2 L/min.

## 1. INTRODUCTION

Its unique properties, which depend on the size, are currently considered as a powerful tool and the most successful area for theoretical research, nanoparticles. The term nanoparticles refers to particles that have a diameter less than 100 nm. Metal nanoparticles (NPs) have seen a vast range of applications in various industries such as biosensing, biomedical science, cosmetics, food, electronics, and medicine. The nanoscale hybridization of various elements is of considerable interest to scientists and researchers due to the unique physicochemical characteristics of these hybrids, such as electrical, optical, catalytic, and thermal properties [1-3]. The unique and novel properties are the result of combination of material characteristics that paired with the effect of reduction in the size of the particle from macroscale to nanoscale, increases the surface-to-volume ratio and dramatically changes physicochemical properties [4-6]. Considerable research interest has been drawn to the multifunctional characteristics of nano-structured metal oxide materials with optical, magnetic, electric and also catalytic functions. These unique characteristics make the materials highly applicable to many exciting applications [7]. TiO₂ has attracted considerable attention in recent years as a promising n-type semiconductor, particularly for addressing environmental pollutants. Its wide use is attributed to a combination of advantageous characteristics, including its affordability, chemical stability under irradiation, non-toxicity, and strong oxidative potential. These properties make it especially effective in photocatalytic processes aimed at degrading harmful substances in air and water [8]. The

different methods for the synthesis of the nanoparticles include pulsed laser deposition, sol-gel preparation, chemical coprecipitation, thermal decomposition, hydrothermal, etc. [9-11]. Among the "green" methods of nanomaterial synthesis, plasma synthesis methods have recently attracted substantial attention as novel methods of nanomaterial synthesis due to different properties, in comparison with solid, liquid, and gas-phase synthesis approaches. Traditional synthesis techniques like the sol-gel and hydrothermal methods are often hindered by prolonged reaction times and the need for intricate chemical procedures, which may lead to undesired by-products or compromise the final material's purity. In comparison, the plasma jet technique presents a more streamlined and innovative approach. It facilitates the direct synthesis of nanoparticles without depending on additional chemical agents or surfactants. By utilizing high-energy plasma in a carefully controlled setting, this method ensures the rapid generation of nanomaterials with high structural integrity and minimal surface contamination [12, 13]. Plasma jet is oriented non-thermal plasma of atmospheric pressure where the plasma afterglow (plume, projectile or stream) is stretched away from the nozzle end [14, 15]. This is a method for nano-forming by jetting plasma, in this research forming nanoparticles from titanium oxide and organizing the structural and optic properties.

## 2. EXPERIMENTAL WORK

Figure 1 is the non-thermal plasma working system

<footnote n="1">¹Ministry of Education, Anbar Education Directorate, Al Rumadi 31001, Iraq</footnote>

<footnote n="2">²Department of Physics, College of Education for Pure Science, University of Anbar, Al Rumadi 31001, Iraq</footnote>
operated at atmospheric pressure with the scale-up of small
figures indicated by the bold-line rectangle inside the figure,
the glowing tip of plasma jet in the beaker where argon gas
come out from its tip and interacts with deionized water and
immersed metal. A Ti metal slide of 7 cm × 1 cm was
immersed in 5 ml deionized water inside a glass beaker and
the plasma nozzle was placed at a distance of 2 cm from the
surface of the liquid in the beaker. The argon gas molecules
reacted with the beaker's liquid and reacted in series with the
metal surface, forming the metal's nanoparticles. Experimental
preparation of nanoparticles (NPs) was carried out at an argon
gas flow of 1.5 to 2 L/min and an applied voltage of 16 kV
with an exposure time of 6 minutes. The plasma needle, which
was perpendicular to the beaker containing deionized water,
was where the metal sheet lay in place. The choice of plasma
jet parameters in this study was not arbitrary but based on a
series of initial optimization experiments designed to identify
conditions that promote both plasma stability and consistent
nanoparticle formation. Among the tested configurations, the
selected flow rates and discharge settings consistently yielded
a steady plasma arc with minimal oscillations, which is
essential for ensuring continuous and uniform energy delivery
to the metallic precursor material. In the case of titanium
dioxide (TiO₂) nanoparticle synthesis, these conditions
facilitated efficient breakdown of the titanium precursor under
high-temperature plasma. A key factor influencing the
characteristics of the resulting nanoparticles is the duration of
plasma exposure. Longer exposure times tend to increase the
thermal energy imparted to the system, which in turn promotes
extended nucleation and subsequent particle growth through
mechanisms such as surface diffusion, aggregation, and

coalescence. The fundamental process of nanoparticle
formation in a plasma jet environment can be understood
through a three-stage mechanism. Initially, high-energy
collisions within the plasma cause the vaporization or
atomization of titanium species. These atoms then undergo
rapid nucleation in the cooling region of the plasma plume.
Following this, the newly formed nuclei collide and merge to
form larger particles, a process enhanced by the high kinetic
energy environment. Finally, as the particles exit the plasma
zone and encounter ambient oxygen, a surface oxidation
reaction occurs, transforming the metallic core into titanium
dioxide (TiO₂) nanoparticles. This synthesis route, therefore,
enables direct control over critical material parameters such as
particle size, crystallinity, and purity by simply adjusting
operating conditions making the plasma jet approach both
versatile and scalable for advanced nanomaterial fabrication.
Thin films have been prepared to characterize as-synthesized
TiO₂ nanoparticles. Glass substrate 3 × 2 cm² has prepared in
ultrasonic waves bath by cleaning in distilled water and
alcohol for 10 min only to remove contamination. This is the
drop-casting method used to deposit nanoparticle solution on
the substrate. To ensure the statistical reliability of the findings,
three independent TiO₂ thin film samples were prepared for
each experimental condition (1.5 and 2 L/min gas flow rates).
All samples underwent identical plasma jet treatment under
controlled parameters. The experiments were repeated, and the
results demonstrated consistent trends in structural and
morphological features across samples, confirming
reproducibility. This strengthens the validity of the observed
correlation between gas flow rates and film characteristics.

<figure><img src="image_2.png" /><figcaption>**Figure 1.** Experimental setup of plasma jet system</figcaption></figure>

**3. RESULT AND DISSECTION**

It is used to find the crystal structure of the materials using X-ray. X-ray diffraction is a process where a crystalline material scatters a beam of X-rays according to its atomic arrangement, thus allowing determination of the crystal structure. Figure 2 the patterns of XRD diffraction of synthesized TiO₂ nanoparticle films on glass substrate. The diffraction pattern shown in Figure 2 proves that TiO₂ of single

Rutile phase was formed were identified by matching with
standard card No 96-900-4142 [16]. It is clear that the size of
the crystal increases from (14.62 nm) to (15.72 nm) with the
increase of gas flow rate, this is due to the fact that with the
increase of gas flow rate, the crystal growth increase and that
is Evident in the peaks that are clearer and more connected, in
addition to the crystal purity increase. Table 1 shows the
values of mean crystallite size, full width at half maximum
FWHM and Miller indices (hkl).
<figure><img src="image_3.png" /><figcaption>Figure 2. XRD patterns of TiO₂ with different gas flow rates</figcaption></figure>

Figure 3 and Table 2 show that in TiO₂ NPs, the increased gas flow rate causes an increase in the grain size, and consequently, large crystalline grains are formed. In some cases, the value of the RMS roughness, which is a measure of surface irregularities, can also increase with the increase in the gas flow rate. Similarly, roughness average (RA) is also one of the surface roughness parameters, which might be increased due to an increase in the size of the nanoparticles as the particles will aggregate [17]. Then changes of the surface features or grain structure refinement occur, due to the increased flow. This results in higher effects and more visible changes in the texture, which makes it more efficient.

<table><caption>Table 1. Summary of the properties of X-rays of TiO₂ nanostructure</caption><thead><tr><th>Gas Flow (L/Min)</th><th>2θ (Deg.)</th><th>FWHM (Deg.)</th><th>d<sub>hkl</sub> Exp.(Å)</th><th>C.S (nm)</th><th>Hkl</th><th>Phase</th></tr></thead><tbody><tr><td rowspan="7">1.5</td><td>27.49</td><td>0.5977</td><td>3.2420</td><td>13.7</td><td>(110)</td><td>Rutile TiO<sub>2</sub></td></tr><tr><td>36.25</td><td>0.6274</td><td>2.4761</td><td>13.3</td><td>(101)</td><td>Rutile TiO<sub>2</sub></td></tr><tr><td>41.29</td><td>0.4939</td><td>2.1848</td><td>17.2</td><td>(111)</td><td>Rutile TiO<sub>2</sub></td></tr><tr><td>44.04</td><td>0.5862</td><td>2.0545</td><td>14.6</td><td>(210)</td><td>Rutile TiO<sub>2</sub></td></tr><tr><td>54.39</td><td>0.6241</td><td>1.6855</td><td>14.3</td><td>(211)</td><td>Rutile TiO<sub>2</sub></td></tr><tr><td>27.43</td><td>0.5286</td><td>3.2489</td><td>15.5</td><td>(110)</td><td>Rutile TiO<sub>2</sub></td></tr><tr><td>36.19</td><td>0.6435</td><td>2.4801</td><td>13.0</td><td>(101)</td><td>Rutile TiO<sub>2</sub></td></tr><tr><td rowspan="3">2</td><td>41.18</td><td>0.4411</td><td>2.1904</td><td>19.2</td><td>(111)</td><td>Rutile TiO<sub>2</sub></td></tr><tr><td>44.09</td><td>0.5322</td><td>2.0523</td><td>16.1</td><td>(210)</td><td>Rutile TiO<sub>2</sub></td></tr><tr><td>54.34</td><td>0.6017</td><td>1.6869</td><td>14.8</td><td>(211)</td><td>Rutile TiO<sub>2</sub></td></tr></tbody></table>

<figure><img src="image_4.png" /><figcaption>Figure 3. AFM of TiO₂ at (a) in flow 1.5 and (b) in flow 2</figcaption></figure>
<table><caption>**Table 2.** Summary of AFM characteristics</caption><thead><tr><th>Gas Flow (L/Min)</th><th>Grain Size (nm)</th><th>RMS Roughness (nm)</th><th>Roughness Ave. (nm)</th></tr></thead><tbody><tr><td>1.5</td><td>20.52</td><td>5.71</td><td>3.38</td></tr><tr><td>2</td><td>22.22</td><td>14.82</td><td>8.35</td></tr></tbody></table>

<figure><img src="image_5.png" /><figcaption>**Figure 4.** FESEM image of TiO₂ at (a) in flow 1.5 and (b) in flow 2</figcaption></figure>

The microscopic topography of TiO₂ NPs provided in Figure 4. Field Emission Scanning Electron Microscopy (FESEM) was used to confirm the surface morphology of plasma jet prepared TiO₂ nanoparticles (NPs). The FESEM used for the magnification of the TiO₂ NPs, as shown in the image below. Through the image and zoom view, it is indicated to us that the spherical nanostructures with significant particle agglomeration confirm the homogeneity of nanoparticles in size and the Nano size of the TiO₂ NPs sample during the preparation [18]. Subsequently, when the gas flow increases, the granular size of these TiO₂ nanostructures also increases, which corresponds to the increasing average grain sizes of TiO₂ nanoparticles, where the average size of the formed nanoparticles was 74.52 nm at gas flow 1.5 and 86.87 nm at gas flow 2. The XRD and FESEM analyses provide compelling evidence that increasing the gas flow rate during the plasma-assisted synthesis of TiO₂ leads to the formation of nanoparticles with larger average diameters. This phenomenon aligns well with classical nucleation and particle growth theories. In particular, the increase in flow rate shortens the residence time of the reactive species within the high-energy plasma region. As a result, there is insufficient time for widespread nucleation to occur, leading to the

formation of fewer initial nuclei. Under these conditions, the atomic and molecular species generated in the plasma tend to aggregate on a limited number of existing nuclei rather than initiating new ones. This preferential deposition leads to enhanced particle growth rather than broad nucleation, resulting in an overall increase in particle size. Moreover, it is plausible that a higher gas flow rate slightly reduces the average thermal energy within the plasma zone due to faster convective cooling. This subtle decrease in temperature may suppress the nucleation rate further while simultaneously favoring surface diffusion and accretion processes on existing particles. In such an environment, particle coalescence and grain boundary migration dominate the growth dynamics, resulting in larger and more defined nanostructures. From a material design standpoint, this insight highlights the importance of precisely tuning gas flow parameters to control particle morphology. By manipulating flow rates, researchers can engineer TiO₂ nanoparticles with specific size distributions and surface characteristics tailored for applications in photocatalysis, gas sensing, or photovoltaic systems [19, 20].

<figure><img src="image_6.png" /><figcaption>**Figure 5.** EDX of TiO₂ at (a) in flow 1.5 and (b) in flow 2</figcaption></figure>

Energy Dispersive X-ray Spectroscopy (EDX) was used to determine the elemental composition of synthesized TiO₂ nanoparticles. Microscale EDX pattern of TiO₂ NPs [21] (Figure 5), with the details of EDX quantitative analysis depicted in an insert table as elemental weight%. At gas flow 1.5, only signals of Ti and O with mass ratios 43.88% and 56.12%, respectively, are found for TiO₂ NPs, and 48.10% and 51.90% are found at gas flow 2. The EDX did not detect any impurities of elements within its detection limit. This means that the highly pure and well crystallized fabricated TiO₂ NPs are in good agreement with the XRD data. In addition, the ratios obtained were quite close to the theoretical ones. Although the EDX spectra confirmed the presence of only Ti
and O elements, it is important to note that EDX has a limited detection threshold, especially for low atomic number elements and trace level contaminants. Therefore, the possibility of undetected impurities, such as carbon based residues or alkali metals, cannot be completely excluded. While their concentrations, if present, are likely negligible, they may still influence surface reactivity or electrical behavior. Future studies involving more sensitive techniques such as XPS.

Figure 6 shows the UV–vis absorption spectrum of the TiO₂ nanoparticle. A functional peak in the ultraviolet electromagnetic range. The presence of TiO₂ for absorbing UV (ultraviolet) light could be seen from their optical absorption less than 400 nm. A sharp absorption edge also indicates the crystalline quality of the TiO₂ NPs and confirms the narrow size distribution of the nanoparticles [22]. At the same time, TiO₂ shows increasing absorption of visible light with an increase in the flow of gas. This would support the XRD and FESEM analysis. The band gap can be determined from the following Eq. (1) as shown in Figure 7.

$$ (\alpha h\nu) = A (h\nu - E_g)^n \quad (1) $$

where, α is the material absorption coefficient, h is Planck's constant, v is the frequency, E_g is the band gap energy, and n is the proportionality constant and the type of sample transitions (direct or indirect) [23].

<figure><img src="image_7.png" /><figcaption>Figure 6. UV–visible absorption spectra of TiO₂</figcaption></figure>

<figure><img src="image_8.png" /><figcaption>Figure 7. The measurement of the energy gap</figcaption></figure>

Depending on the gas flow rate applied during the synthesis, the optical energy band gap TiO₂ Nano varies. The band gap

was 3.16 at 1.5 (L/min). It dropped to 3.08 eV at 2 (L/min), further confirming the results of these prior studies [24, 25]. Increasing the granular size of the precipitant material causes an increase in height of the photonic absorption because it increases electron's energy levels by creating donor levels of energy gap and near conduction band, thus absorb large number of photons with less energy. Such variations in atomic arrangement could influence the energy band structure of the deposited material, resulting in a narrower energy gap.

## 4. CONCLUSIONS

The Plasma Jet technique provides an environmentally friendly, economical and readily scalable process for the production of TiO₂ thin film. By EDX analysis, this method is also in agreement with the purity of the metal oxide generated. The observed peaks for TiO₂ were of a Rutile phase as shown in XRD. Peak width at half-maximum and mean crystallite size FWHM were determined. As gas flow further increased, the crystal grain size increased and FESEM images revealed spherical nanostructures. It was discovered that the optical emitting energy gap of the Nano material changes with the gas flow used in the preparation. This research provides more than just a theoretical framework for understanding how gas flow variations influence the structure and optical behavior of TiO₂ nanoparticles during plasma jet synthesis. It opens the door to practical advancements across several high-impact applications. By precisely controlling the size and crystallinity of the nanoparticles, it becomes possible to enhance photocatalytic activity due to improved surface reactivity and tailored bandgap properties. These improvements can significantly increase the efficiency of pollutant degradation and solar energy conversion processes. Additionally, nanoparticles synthesized under optimized conditions exhibit higher stability and responsiveness in gas sensors, contributing to better detection of hazardous gases at lower concentrations. In this regard, the outcomes of the study bridge a critical gap between fundamental materials research and practical, scalable technologies.

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