The Oriented Attachment Crystal Growth Model in Hydrothermal Synthesis of Magnetite (Fe3O4) NanoparticlesIntroduction
Cancer is a major public health problem and the second leading cause of death globally. The latest update from the IARC (International Agency for Reseach on Cancer), the cancer burden rises to 18.1 million new cases and responsible for an estimated 9.6 million deaths in 2018 [1]. However, conventional treatments such as surgery, radiation, chemotherapy, and biologic therapies (immunotherapy) are limited by the accessibility to the tumor, the risk of operating on a vital organ, the spread of cancer cells throughout the body, and the lack of selectivity toward the tumor cells [2].
In recent times, the drug delivery has been developed as a new method for cancer therapy. The principle of this method is delivering the drug into the target site using a nanoparticle as a “vehicle”. The advantages of nano drug delivery compared to conventional medication methods are (1) it has the ability to treat the specific targets in the body, (2) the dose of the drug is reduced, (3) the concentration of the drug at the nontarget sites is reduced, and (4) the side effects caused by drug toxicity in cells/nontarget tissues are reduced [2].
Magnetite nanoparticle (Fe3O4) is one of the materials that isa very promising candidate for being applied to drug delivery system due to its superparamagnetic and high-biocompatibility properties [3]. The controlled size and the morphology of nanoparticles are needed in drug delivery system because it affects the accessibility, the time residence in the bloodstream and the toxicity in the human body [4,5]. The synthesis of magnetite nanoparticles with controllable size and morphology are remain a challenge. The study of the evolution of crystal growth can help to understand the factors that influence the growth of crystals. An understanding of the factors that affectsthe crystal growth kinetics and microstructure development in nanocrystals is fundamental to control the nanoparticle properties [6]. It is important for the tailoring process of the nanoparticles to have uniform size and morphology [7].
Utami et al. [8] had been studied the effect of temperature on the evolution of crystal growth in the hydrothermal system and modeled it using Ostwald Ripening model. It is found that the crystal growth reaction was controlled by dissolution kinetics at the particle-matrix interface. However, it is known that in the nanoscale systems, the surface contributions to the total energy become increasingly important as the particle size decreases. Nanocrystals have a higher surface energy, which facilitates the ‘‘reaction’’ on the surface, such as the directbonding and the crystallization amongthe particles namely oriented attachment (OA) pathway [9]. Here, we investigated the magnetite coarsening in the hydrothermal system using the oriented attachment approach.
Experimental
This study consisted of three main stages: (1) magnetite nanoparticles preparation using the hydrothermal method, (2) characterizationsusing XRD (X-ray diffraction), TEM (transmission electron microscope), PSA (particle size analyzer), and VSM (vibrating sample magnetometer) and (3) modeling the kinetics of magnetite crystal growth.
<bold id="bold-1">Synthesis of Magnetite Nanoparticles </bold>
The magnetite nanoparticles were synthesized using the hydrothermal method. The various concentrations of FeCl3 (0.05 M, 0.10 M, and 0.15 M), 4 mmol of sodium citrate (0.10 M), and 6 mmol of urea (0.15M) were dissolved intothe 40 cm3 of distilled water, then 0.1 g of PEG was added until it was completely dissolved.The solution was finally transferred into a Teflon-lined autoclave. The Teflon-lined autoclave was put into an oven and the temperature was set to 210oC. The reaction times used in this study were 1, 2, 3, 3.5, 5, 7, 9, and 12 hours. The black precipitateformed was separated by a bar magnet, then washed with water and ethanol, and dried at 60°C overnight. The black precipitates were characterized by XRD, TEM, PSA, BET analyzer and VSM.
CharacterizationXRD Characterization
Identification, crystallinity and size of nanoparticles were determined by XRD. Approximately 200 mg of sample was printed directly on aluminum measuring 2 × 2.5 cm2. Samples were characterized using XRD instrument with Cu radiation light (λ = 1.54 Ǻ) with a voltage of 40 kV and a current of 30 Ma at 2θ of 10-99.97o.
TEM Characterization
The particles size, morphology, and aggregate were analyzed by transmission electron microscope (TEM JEOL JEM 1400) operated at 5 kV under vacuum.
The particle size distribution was analyzed by PSA (Beckman Coulter) at 25oC and the viscosity of 0.8878 cp in water for 30 minutes.
VSM Characterization
Characteristics of magnetic nanoparticles were analyzed by Vibrating Sample Magnetometer (VSM) type VSM1.2H Oxford. Magnetization curves measured at room temperature with a magnetic field that varies in the range -1 to 1 Tesla.
<bold id="bold-b8bb265047bcfa4eb97adc2a5a2c7a28">Kinetic Modeling of Crystal Growth</bold>
The Oriented Attachment (OA) crystal growth model explained the crystal growth based on the joining of crystal particles. The primary particles met with other primary particles forming secondary particles. The secondary particles met with the primary particles forming the tertiary particles and so on to form larger ones without the dissolution of either particle. The driving force of this process was attributed to the decrease in surface and grain boundary free energies [10]. The general equation of Oriented Attachment crystal growth model was presented in equation 1:
where \( D \) was crystal diameter, \( Do \) was the diameter of crystal formed initially, \( K \) was constant and \( t \) wasthe time reaction. The \( K \) value was obtained from theintercept of the experimental data following equation:
\begin{equation} \ln\left [ \left ( 1-\alpha \right )\left [ \frac{D_{0}}{D} \right ]^{3} \right ]=\ln k + \ln t \tag{2} \end{equation}
Furthermore, the value of \( D \) and \( Do \) were obtained to the model curve. The experimental curve then matched with the model.
Result and DiscussionMagnetic Properties and VSM Results
The formation of magnetite nanoparticle is shown by the formation of black precipitate at 3.5 h synthesis (Figure 1). The precipitate iswell dispersed in water (Figure 1 a). These properties are expected in the development of drug delivery. The presence of PEG that has an-OH group on the surface makes the nanoparticles are hydrophilic and negatively charged. Thus, it makesthe nanoparticles have a longer residence time in the bloodstream (high bioavailability) because it corresponds to the nature of the plasma proteins which is also hydrophilic and negatively charged. In general, phagocytosis will occur in particles of non-polar (hydrophobic) and positively charged as it is considered as a foreign substance to the body. In addition, the presence of PEG on the surface of magnetite nanoparticles also prevents oxidation by the air and becomes a place for drug attachment [11,12].
fig-7dbae4ab1c50ba0e1d9dd237870e0c23
The as-synthesized black precipitate disperse well in water (a) the precipitate interacts with external magnetic field (b) re-dispersible powder in the water after the magnetic field is removed (c)
When it is brought closer to the external magnetic field, the precipitate interacts with magnetic field (Figure 1b). Magnetic properties of the precipitate appear when it is exposed to the external magnetic fieldand then disappear when the magnetic field is eliminated (Figure 1c). This shows that the magnetite hassuperparamagnetic properties.
fig-16a6a40c46b67edfcaf0376a0617540c
Hysteresis curve of the as-synthesized magnetite nanoparticles
The VSM hysteresis curve of the precipitated magnetic is depicted in Figure 2. There is a very narrow hysteresis loop with coercivity’s (Hc) value of near zero (0,02T). This reaffirms that as-synthesized magnetite nanoparticle has superparamagnetic properties. This superparamagnetic properties gives advantages in drug delivery application such as easy to guide to the parts of body by external magnetic field and preventing the effects of agglomeration after the application of external magnetic fields [13].
XRD Analysis
The XRD patterns match with the standar pattern of Fe3O4 with the highest intensities at 2Ө 35.54°; 57.06°; and 62.66° which confirm that the precipitate is pure magnetite (Figure 3). The intensity of the peak rises as the time increase, indicates an increasing in crystallinity of magnetite (Figure 3).
fig-66827095528bb4f9bec9fc34cac94fce
The XRD pattern of as-synthesized magnetite at 210oC for 3.5h (a), 5h (b), and 12 h(c)
The XRD pattern of samples synthesized from various FeCl3 concentrations are shown in Figure 4. All of sample patterns are well-matched with the standard pattern of Fe3O4, indicate a pure Fe3O4 are formed in different concentration. The intensities of XRD peaks show higher intensity in higher concentrations, indicates higher crystallinity product was obtained from the higher concentration of FeCl3. However, the peak boardening decrease with higher concentration shows bigger crystallite size obtained in higher concentration of FeCl3.
fig-d70c0f3b48e5b76a47798a7848d0a8f7
Diffractogram of the as-synthesized samples at temperatures of 210 ° C 12 hours, FeCl3 concentrations of (a) 0.05 M, (b) 0.10 M and (c) 0.15 M
TEM Images Analysis
The morphology of magnetite nanoparticles is shown by the TEM images (Figure 5). TEM image shows that at 3.5 hours, thenano-sized particles formed are uniform in diameter, they are about less than 10 nm (Figure 5a). It can be seen that at the initial formation step, the single crystal is formed. The dark region shows a high cristallinity and the light region shows a low crystallinity. The light region of particle is larger than the dark region indicatinga low cristallinity (high amorphouse phase) of nanoparticles formed at the initial formation as indicated in XRD data.
fig-40d29cd761841321563ac220971e7374
TEM image of nanoparticles synthesized at temperature of 210 ° C at 3.5 h (a), 7 h (b), and 12 h (c) with magnification of 80,000X
The 7 hours synthesis results particles which have less regulated morphology and agglomerated with the final diameter of about 100 nm (Figure 5b). At 12 hours, the particles are more crystalline and the agglomeration still occur with the final diameter of more than 100 nm (Figure 5c). The TEM image reveals that at longer reaction time, the initial particle coalesences to decrease the interfacial energy, as the basis of modeling with the Oriented Attachment approach. The agglomeration is not expected for drug delivery application due to anisotropy in pharmacology effect. However, magnetite nanoparticles obtained in this experimentare in accordance with the criteria of drug delivery, which are 10 nm - 200 nm [2].
PSA Results
The Particle Size Analyzer (PSA) results are depicted in Figure 6 and Table 1. Based on Figure 6, it can be seen that the different synthesis conditions produce different distribution of magnetite nanoparticles size. The particle size distributionof sample synthesized at 0.1 M reactant concentration is narrow (Figure 6a and Figure 6c), while for sample synthesized at 0.15 M concentration the particle size distribution is wide indicating higher polidispersity (Figure 6b).
fig-9985b07e21718e5172c54d48fdcb597c
Distribution of particle diameter of the as-synthesized magnetite at 210 ° C (a) 3.5 hours 0.10 M (b) 12 hours 0.10 M and (c) 12 hours 0.15M
table-wrap-84db80cf8bf18d9516e3a806f09a9a83
Table 1. Particle size of the as-synthesized magnetite based on PSA characterization
Table caption
Sum of particle size distribution at synthesis condition :
0.1 M 3.5 h
0.1 M 12 h
0.15 M 12 h
size (nm)
percentage (%)
size (nm)
percentage (%)
size (nm)
percentage (%)
<10
0
<10
0
<10
0
10
13
10 - 20
8.68
10 - 20
0
11
15
20 - 30
5.41
20 - 30
0
12
14
30 - 40
41.69
30 - 40
0
13
13.79
40 - 50
25.12
40 - 50
60.59
14
15.31
50 - 60
7.5
50 - 60
31.39
15 - 20
26
60 -70
11.6
60 -70
8.02
> 20
2.9
> 70
4.4
> 70
0
total
100
total
100
total
100
Table 1 shows, for sample synthesized using 0.1 M reactant for 3.5 hours, the particle size in range of 10-20 nm is about 97%, while forthe sample synthesized for 12 hours s the particle size in range of 30-50 nm is about 66.81%.It also shows that the percentage of the small particle decreases by the time but the percentage of the bigger particles increases. It reveals a coarsening in the hydrothermal system as the longer reaction time with hypothetically Oriented Attachment path way. For the sample synthesized at reactant concentration of 0.15 M and 12 hours synthesis, the particle size in range of 40-70 nm is about 100%. Thus, it can be concluded that the higher concentration of FeCl3 will produce larger particle diameter but narrower particle size distribution. PSA results also prove that the longer the reaction time, the more particle diameter increases will be. This also prove the occurrence of coalescence of small particles into large particles, seen from the reduced percentage of small particles formed after 12 hours compared to the percentage of small particles formed at 3.5 hours.
Modeling of Magnetite Nanoparticle Crystals Growth by Oriented Attachment (OA) Approach
The XRD, TEM and PSA data show the tendency of the nanoparticle growth from combining small particles into larger particles through the agglomeration. To prove the occurrence of Oriented Attachment pathway in the process of magnetite crystal growth in hydrothermal system, modeling is made. Based on experimental data obtained from X-ray diffraction, the crystal diameters are determined by Scherres formula. Then, the k values are obtained from the concentrations of 0.05 M, 0.1 M and 0.15 M. From this k value the diameter of the model is determined by substituting the parameters Do and t (Equation 1). The plot of crystal diameter vs time at various reactant concentrations are shown in Figure 7.
fig-ee8d0ade0c6b1dd1a6d5ce828e835300
Diameter of magnetite crystal particles from experiment and model at reactant concentration of 0.05 M (a); 0.1 M (b); 0.15 M (c)
In Figure 7, it can be seen that the crystal diameter from the experimental results on the increase in reaction time become closer to the model point. The elevation points isshrink from the reaction time of 5, 7, 9 and 12 hours. It can be concluded that increasing reaction time the growth of magnetite crystals following the Oriented Attachment (OA) model.
In different concentration treatments, the growth response of magnetite crystals is also different. At 0.15 M reactant for 5-hour synthesis, the percent of error reaches 29%. Whereas for 0.10 M and 0.05 M reactants, the error is of 19.15% and 9.6%, respectively. It can be seen that the experiment is closer to the model at a concentration of 0.05 M.
Conclusion
A pure superparamagneticmagnetite nanoparticle has been successfully synthesized viathe hydrothermal method at 210oC.The crystal diameter was about 9.4-30 nm and particle diameter was lower than 200 nm. From the overall characterization, it was concluded that the time and the concentration of reactants (FeCl3) affected the growth of magnetite crystals. An increase in reaction time increased the diameter of the crystal and crystallinity. The diameter particle rose with the time due to occurrence of agglomeration. Judging from the trend, magnetite crystal growth in this study followed the Oriented Attachment model, where the lowest concentration of reactant gave the smallest percentage error of 9.6% while the highest concentration contributed to the highest error of 29%. From this study it was suggested: to produce controllable properties of magnetite nanoparticles for drug delivery purpose, low concentrations (0.05 M FeCl3) was highly recommended.
Acknowledgement
Financial support for this study was provided bythe Ministry of Research, Technology and Higher Education of Republic of Indonesia(Kemenristekdikti).
1203Francehttps://www.iarc.fr/wp-content/uploads/2018/09/pr263_E.pdf2019International Agency for Research on CancerPress release N° 263 : Latest global cancer data: Cancer burden rises to 18.1 million new cases and 9.6 million cancer deaths in 201830622-322200710.1016/s1748-0132(07)70084-1ArrueboManuelFernández-PachecoRodrigoIbarraM. RicardoSantamaríaJesúsNano TodayMagnetic nanoparticles for drug delivery248022201110.4314/ijest.v2i8.63846MohapatraMAnandSInternational Journal of Engineering, Science and TechnologySynthesis and applications of nano-structured iron oxides/hydroxides – a review308198-205153201110.1016/j.jconrel.2011.06.001BaeYou HanParkKinamJournal of Controlled ReleaseTargeted drug delivery to tumors: Myths, reality and possibility095055554-557013201210.3390/ijms13055554YuMiaoHuangShaohuiYuKevin JunClyneAlisa MorssInternational Journal of Molecular SciencesDextran and Polymer Polyethylene Glycol (PEG) Coating Reduce Both 5 and 30 nm Iron Oxide Nanoparticle Cytotoxicity in 2D and 3D Cell Culture37333783200310.1021/nl025836+HuangFengZhangHengzhongBanfieldJillian F.Nano LettersTwo-Stage Crystal-Growth Kinetics Observed during Hydrothermal Coarsening of Nanocrystalline ZnS3102012HwangNong-MoonJungJae-SooLeeDong-KwonMorales-RodriguezRicardoThermodynamics - Fundamentals and Its Application in ScienceThermodynamics and Kinetics in the Synthesis of Monodisperse Nanoparticles04012010345201810.1088/1757-899x/345/1/012010UtamiS PFadliASariE OAddabsiA SIOP Conference Series: Materials Science and EngineeringCrystal-growth kinetics of magnetite (Fe3O4) nanoparticles with Ostwald Ripening Model approach118-342201010.1039/b9nr00047jZhangJingHuangFengLinZhangNanoscaleProgress of nanocrystalline growth kinetics based on oriented attachment81568-157816201410.1039/c3ce41929kZhangHengzhongBanfieldJillian F.CrystEngCommInteratomic Coulombic interactions as the driving force for oriented attachment122014ŁuszczykKatarzynaKaletaJerzyMechRafałInterdisciplinary Journal of Engineering SciencesMagnetic core-shell structures as potential carriers in drug delivery system0120533-372201610.18576/jpac/020201MarkhuliaJ.MikelashviliV.KekutiaSh.SaneblidzeL.JabuaZ.DaraseliaD.JafaridzeD.Journal of Pharmaceutical and Applied ChemistrySome Physical Parameters of PEG-modified Magnetite Nanofluids3180715977-1600914201310.3390/ijms140815977KolhatkarAratiJamisonAndrewLitvinovDmitriWillsonRichardLeeT.International Journal of Molecular SciencesTuning the Magnetic Properties of Nanoparticles