Research Article  Open Access
Sanaz Khademolqorani, Ali Zeinal Hamadani, Hossein Tavanai, "Response Surface Modelling of Electrosprayed Polyacrylonitrile Nanoparticle Size", Journal of Nanoparticles, vol. 2014, Article ID 146218, 7 pages, 2014. https://doi.org/10.1155/2014/146218
Response Surface Modelling of Electrosprayed Polyacrylonitrile Nanoparticle Size
Abstract
Electrospraying (electrohydrodynamic spraying) is a method of liquid atomization by electrical forces. Spraying solutions or suspensions allow production of fine particles, down to nanometer size. These particles are interesting for a wide variety of applications, thanks to their unprecedented chemical and physical behaviour in comparison to their bulk form. Knowledge of the particle size in powders is important in many studies employing nanoparticles. In this paper, the effect of some process parameters on the size of electrosprayed polyacrylonitrile particles is presented in the form of response surface model. The model is achieved by employing a factorial design to evaluate the influence of parameters on the polyacrylonitrile nanoparticle size and response surface methodology. Four electrospraying parameters, namely, applied voltage, electrospraying solution concentration, flow rate, and syringe needle diameter were considered.
1. Introduction
Nanoparticles are defined as particulate dispersions or solid particles with a size in the submicron range of 10–1000 nm [1]. Nanoparticles can be prepared from a variety of materials such as proteins, polysaccharides, and synthetic polymers. Particles in nanosize range are being investigated for a number of applications such as catalysts, cosmetics, pharmaceutics, medical, and compound materials [2–5].
The properties of materials with nanometer dimensions are significantly different from the same materials in bulk form. This is mainly due to the nanometer size of the materials leading to large fraction of surface atoms, high surface energy, spatial confinement, and reduced imperfections, which are much less pronounced in the corresponding bulk materials. Large fraction of surface atoms result in much more pronounced surface dependent properties of materials. Many of the mechanical properties of nanomaterials, including hardness, elastic modulus, and yield strength, are very different when compared with the bulk form [6–8].
With dimensions going down to nanoscale, the size of the nanomaterials is comparable to the light wavelength and the mean free path of the photons. This means that the photon transport within the materials is changed significantly because of photon confinement and quantization of photon transport, which leads to modified thermal properties [6, 9–11]. The most important property of nanoparticles, that is, inherent large surface to volume ratio, can potentially improve catalytic processes and interfacial driven phenomena such as wetting and adhesion. The estimation of the dependence of particle energy on its size is provided by the GibbsThompson relation. According to this relation, lower particle size increases the chemical potential of metal atoms [2, 4, 12]. The techniques for producing the nanoparticles can be classified into “topdown” and “bottomup” methods [3]. The topdown method transforms the material with an initial size of a few micrometers into nanoparticles with a size of only 40–200 nm. The bottomup method generates nanoparticles by heaping up atoms or assembling nanobuilding blocks. Electrospraying is an example of topdown method which is capable of producing nanoparticles. During electrospraying, under the influence of the applied electrical field, liquid flowing out from a capillary nozzle elongates and forms a cone or jet. As the voltage is increased, the jet breaks down into initial droplets. Then, the solvent evaporates from the initial droplets and the initial droplets break up to smaller particles as a result of the buildup of high repulsive forces inside them. This process which is known as Coulomb explosion continues until the final droplets reach the collector where they lose their electrical charge [13–15].
The charge and size of the droplets can be controlled to some extent by the applied voltage, electrospraying solution concentration, nozzlecollector distance, flow rate of the liquid out of the capillary nozzle, and needle diameter.
Considering the importance of the size of particles on the properties and applications of nanoparticles, in this research, the electrosprayed polyacrylonitrile nanoparticle size was modelled. To obtain the above mentioned model, at first, full factorial experimental design was chosen and nanoparticles were produced. The ANOVA analysis was used to study the significance of the treatments. Then, values for coefficients, values, and and for response surface model were obtained by regression analysis. Response surface method is a collection of mathematical and statistical techniques, suitable for modelling and analysis of engineering applications. The response surface method is applied to situations where several input variables potentially influence some performance or characteristics of the process which are often called response. The relationship between the response () and input variables could be expressed in terms of mathematical notation. Ogata et al. [16] has proposed a model for the mean volumesurface diameter of the droplets generated in the conejet mode of electrospraying. Tomita et al. [17] determined the frequency of droplet generation in the microdripping mode for droplet diameter less than 200 μm.
2. Experimental
2.1. Preparation of Polyacrylonitrile (PAN) Solution
To prepare PAN solution, PAN powder ( g/mol, g/mol) polymerized from acrylonitrile (94 wt.%), methyl methacrylate (4 wt.%), and methacrylic acid (2 wt.%) (provided by Iran Polyacryl company) was dissolved in dimethylformamide (DMF, Merck) for 12 h at room temperature. Concentrations ranging between 1 and 3% (w/w, weight by weight basis) were prepared.
2.2. Electrospraying of PAN Solution
The setup used for electrospraying PAN solutions, consists of a dosing pump, syringe, and needle set, aluminium foil collector, and high voltage source as shown in Figure 1. The polymer solution is placed into a syringe (1 mL) with the needle connected to a high voltage source and the syringe connected to dosing pump (syringe pump model STC527, TERUMO). The horizontal syringe needle and the vertical aluminium foil collector were connected to positive and negative electrodes of high voltage source (Emersun, 220 V, AC inputup to 25 kV DC output), respectively. The electrical field is formed between the collector and the tip of the syringe tube.
The levels of electrospraying variables, that is, the applied voltage, solution concentration, volume flow rate, and syringe needle diameter, are shown in Table 1. The needlecollector distance was fixed at 15 cm.

2.3. Measurements
After the formation of the nanoparticles on the aluminium collector, several images from each sample were taken by scanning electron microscopy (SEM, Seron Technology, AIS2100 model, Amirkabir University) and then, for all the samples, the diameter of 150 nanoparticles was measured by measurement software (manual microstructure distance measurement, Nahamin Pardazan Asia co).
3. Modelling
3.1. Design of Experiments
In general, design of experiments (DOE) or experimental design is the design of any informationgathering exercise where variation is present, whether under the full control of the experimenter or not. In the design of experiments, the experimenter is often interested in the effect of some process or intervention (the treatment) on one or moe outcomes of the experiment (the experimental units). It can be said that design of experiments is a discipline that has broad application in science.
A full factorial experiment is an experiment whose design consists of two or more factors, each with discrete possible values or “levels,” and whose experimental units take on all possible combinations of these levels across all such factors. A full factorial design is also called a fully crossed design. Such an experiment allows studying the effect of each factor on the response variable, as well as the effects of interactions between factors on the response variable [18].
Consodering the conditions of our research, the full factorial design was chosen for data collection. Four factors each at three levels (3^{4} design) (Table 1) resulting in 81 treatments combinations were chosen. Also, because of three levels in each parameter, quardratic modelling could be applied. Uncoded variables for experimental and test data with corresponding responses are shown in Table 2.

3.2. Response Surface Methodology (RSM)
In statistics, response surface methodology (RSM) explores the relationships between several explanatory variables and one or more response variables. This method was introduced by G. E. P. Box and K. B. Wilson in 1951. The main idea of RSM is to use a sequence of designed experiments to obtain an optimal response. Box and Wilson suggest using a seconddegree polynomial model to do this. They acknowledge that this model is only an approximation, but use it because such a model is easy to estimate and apply, even when little is known about the process. The planning and analysis of this study were performed within the context of RSM [19, 20].
4. Results and Discussion
In this section, a rundown on the achieved results is presented. As a typical image, Figure 2 shows the SEM image of PAN nanoparticles electrosprayed at 14 kV voltage, 2 w/w% solution concentration, and 0.0263 mL/h flow rate (needle diameter = 0.8 mm). The corresponding diameter (size) distribution of particles shown in Figure 2 is shown in Figure 3.
In general, analysis of variance (ANOVA) is a collection of statistical models and their associated procedures in which the observed variance in a particular variable is partitioned into components attributable to different sources of variation. In its simplest form, ANOVA provides a statistical test of whether or not the means of several groups are all equal and, therefore, generalizes test to more than two groups. Doing multiple twosample tests would result in an increased chance of committing a type I error. For this reason, ANOVA is useful in comparing three or more means. The result of the ANOVA analysis is shown in Table 3. As can be seen, all main effects and the interaction between voltage and flow rate are significant ( value < 0.05). Regression analysis which is widely used for prediction and forecasting makes the relationship between the independent variable and the dependent variable clear. If a relationship exists, its form is explored by regression analysis. In restricted circumstances, regression analysis can be used to infer causal relationships between the independent and dependent variables. After implementing RSM to the data set, the values of coefficients and their values for regression model were obtained as presented in Table 4.


As can be seen from Table 4, the main effect of flow rate is not significant ( value > 0.05). Furthermore, the represents the proportion of the total variability that has been explained by the regression model. The of appropriate model is about 0.96, illustrating that the model was able to explain 96% of the variability of the mean particle size. The final response surface model fitted to the mean nanoparticle size is shown as follows:
It is worth mentioning that the practical performance of regression analysis methods depends on the form of the data generating process as well as its relationship to the employed regression approach. Since the true form of the datagenerating process is in general not known, regression analysis often depends to some extent on making assumptions about this process.
These assumptions were considered for the model and are shown in Figures 4, 5, and 6. The pattern and shape of these figures confirm the validity of the model. Figure 4 shows a random pattern of residuals on both sides of zero without any recognizable patterns in residual plot. Figure 5 shows normal distribution, as the points in this plot should generally form a straight line. Figure 6 shows the plot of all residuals in the order that the data was collected in and can be used to find nonrandom error, especially of timerelated effects. A positive correlation is indicated by the clustering of residuals with the same sign. A negative correlation is indicated by rapid changes in the signs of consecutive residuals.
After fitting RSM to data, contour plots were prepared as illustrated in Figures 7, 8, and 9. Contour plot is a graphic representation of the relationships between three numeric variables in two dimensions. Two variables represent and axes, and a third one represents , which shows the contour levels. The contour levels are plotted as curves and the area between curves can be color coded to indicate interpolated values. For example, if a size is chosen between 156 and 162 nm, concentration between 2.5 and 3 w/w%, voltage over 12 kV, needle diameter lower than 0.8 mm, and feed rate lower than 0.8 mL/h are recommended.
5. Conclusion
The effect of some process parameters on the diameter of electrosprayed polyacrylonitrile particles is presented in the form of response surface model. The validity of the model is confirmed with the help of residual versus the fitted value, normal probability plot of the residuals and residual versus the order of mean nanoparticle size.
Conflict of Interests
The authors declare that there is no conflict of interests regarding the publication of this paper.
References
 V. J. Mohanraj and Y. Chen, “Nanoparticles—a review,” Tropical Journal of Pharmaceutical Research, vol. 5, pp. 561–573, 2006. View at: Google Scholar
 L. Gasman, Nanotechnology Application and Markets, Artech House, London, UK, 2006.
 T. H. Hou, C. H. Su, and W. L. Liu, “Parameters optimization of a nanoparticle wet milling process using the Taguchi method, response surface method and genetic algorithm,” Powder Technology, vol. 173, no. 3, pp. 153–162, 2007. View at: Publisher Site  Google Scholar
 Y. Ning, “Platinum nanoparticle catalysts,” Platinum Metals Review, vol. 3, no. 46, pp. 115–119, 2002. View at: Google Scholar
 C. T. Campbell, S. C. Parker, and D. E. Starr, “The effect of sizedependent nanoparticle energetics on catalyst sintering,” Science, vol. 298, no. 5594, pp. 811–814, 2002. View at: Publisher Site  Google Scholar
 J. T. Lue, “Physical properties of nanomaterials,” in Encyclopedia of Nanoscience and Nanotechnology, vol. 5, pp. 1–46, 2007. View at: Google Scholar
 B. Hamdoun, D. Ausserré, S. Joly, Y. Gallot, V. Cabuil, and C. Clinard, “New nanocomposite materials,” Journal de Physique II, vol. 6, no. 4, pp. 493–501, 1996. View at: Publisher Site  Google Scholar
 D. Vollath, Nanomaterials; An Introduction to Synthesis, Properties and Application, WileyVCH Verlag GmbH&Co, 2nd edition, 2013.
 R. Nagarajan and T. A. Hatton, Nanoparticles: Synthesis, Stabilization, Passivation and Functionalization, American Chemical Society, Washington, DC, USA, 2008. View at: Publisher Site
 G. Schmid, Nanoparticles; from Theory to Application, WileyVCH Verlag GmbH&Co. KGaA, 2nd edition, 2010. View at: Publisher Site
 http://123seminarsonly.com/SeminarReports/016/55231535PropertiesofNanoMaterials.pdf.
 E. Roduner, “Size matters: why nanomaterials are different,” Chemical Society Reviews, vol. 35, no. 7, pp. 583–592, 2006. View at: Publisher Site  Google Scholar
 A. Jaworek and A. T. Sobczyk, “Electrospraying route to nanotechnology: an overview,” Journal of Electrostatics, vol. 66, no. 34, pp. 197–219, 2008. View at: Publisher Site  Google Scholar
 K. Okuyama and W. Lenggoro, “Preparation of nanoparticles via spray route,” Chemical Engineering Science, vol. 58, no. 3–6, pp. 537–547, 2003. View at: Publisher Site  Google Scholar
 A. Jaworek and A. Krupa, “Jet and drops formation in electrohydrodynamic spraying of liquids: a systematic approach,” Experiments in Fluids, vol. 27, no. 1, pp. 43–52, 1999. View at: Publisher Site  Google Scholar
 S. Ogata, T. Hatae, K. Shoguchi, and H. Shinohara, “The dimensionless correlation of mean particle diameter in electrostatic atomization,” International Chemical Engineering, vol. 18, no. 3, pp. 488–493, 1978. View at: Google Scholar
 Y. Tomita, Y. Ishibashi, and T. Yooyama, “Fundamental studies on an electrostatic inkjet printer,” Bulletin of the JSME, vol. 29, no. 257, pp. 3737–3743, 1986. View at: Publisher Site  Google Scholar
 M. Anderson, Design of Experiments, American Institute of Physics, The Industrial Physicist, 1997.
 D. C. Montgomery and S. M. Kowalski, Design and Analysis of Experiments, John Wiley & Sons, New York, NY, USA, 7th edition, 2011.
 G. E. P. Box, J. S. Hunter, and W. Hunter, Statistics for Experimenters: Design, Innovation, and Discovery, Wiley, 2nd edition, 2005. View at: MathSciNet
Copyright
Copyright © 2014 Sanaz Khademolqorani et al. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.