- Nano Express
- Open Access
Electrokinetic Properties of TiO2 Nanotubular Surfaces
© The Author(s). 2016
- Received: 26 May 2016
- Accepted: 16 August 2016
- Published: 25 August 2016
Surface charge is one of the most significant properties for the characterisation of a biomaterial, being a key parameter in the interaction of the body implant with the surrounding living tissues. The present study concerns the systematic assessment of the surface charge of electrochemically anodized TiO2 nanotubular surfaces, proposed as coating material for Ti body implants. Biologically relevant electrolytes (NaCl, PBS, cell medium) were chosen to simulate the physiological conditions. The measurements were accomplished as titration curves at low electrolytic concentration (10−3 M) and as single points at fixed pH but at various electrolytic concentrations (up to 0.1 M). The results showed that all the surfaces were negatively charged at physiological pH. However, the zeta potential values were dependent on the electrolytic conditions (electrolyte ion concentration, multivalence of the electrolyte ions, etc.) and on the surface characteristics (nanotubes top diameter, average porosity, exposed surface area, wettability, affinity to specific ions, etc.). Accordingly, various explanations were proposed to support the different experimental data among the surfaces. Theoretical model of electric double layer which takes into account the asymmetric finite size of ions in electrolyte and orientational ordering of water dipoles was modified according to our specific system in order to interpret the experimental data. Experimental results were in agreement with the theoretical predictions. Overall, our results contribute to enrich the state-of-art on the characterisation of nanostructured implant surfaces at the bio-interface, especially in case of topographically porous and rough surfaces.
- TiO2 nanostructured surfaces
- Zeta potential
- Surface charge
- TiO2 nanotubes
Titanium and its alloys are generally considered suitable materials for metallic implants [1, 2], even though they lack per se in terms of biocompatibility, due to their intrinsic inertness. One of the strategies to overcome this issue is to improve their surface properties (i.e. surface roughness and topography, chemical composition, wettability, charge) by creating nanostructured surfaces able to ensure a beneficial, pre-conditioning film of ions and proteins, which will support the further cell adhesion and wound healing, have antibacterial properties, etc.
The surface modifications of Ti-based implants nano-topography have been extensively studied by several authors [3, 4]. In particular, the use of self-assembled titanium dioxide (TiO2) nanostructures have found much interest in various fields of functional biomedical applications, especially attributable to the great advantage of gaining a very highly exposed (effective) surface area. In fact, the extremely high effective surface area of vertically oriented TiO2 nanotubes (NTs) results in a superior surface energy, leading to an increase in the initial protein adsorption that can enhance cellular interactions (increased osseointegration, antibacterial activity, mitigation of the inflammatory response, etc.) [3, 5–8]. Recently, research and development in the area of synthesis and applications of different nanostructured TiO2 materials has been greatly increasing. The TiO2 nanostructures are primarily categorised by their different methods of preparation, such as sol-gel, hydrothermal treatment, assisted-template synthesis, and electrochemical anodization (EA) . EA of Ti is the preferred method for growing self-assembled TiO2 nanotubular structures directly on the substrate materials, as it enables a good control over their geometry and specific diameters, long-range order as well as an ease of application [9, 10]. In view of that, herein we obtained nanotubes with specific diameters by optimising experimental parameters during electrochemical anodization. Such structures were shown to be highly valuable for biological applications not only from the point of increased surface area and possibility to be used as reservoirs for medications, but also for the selective attachment of proteins, which further dictate adhesion of cells. It has been previously shown  that binding of proteins is highly influenced by the size of the nanotube diameter, which is due not only to the increased surface area but also to the possibility of proteins to enter into the narrow interior of the nanotubes (only smaller proteins can enter the NTs 15 nm diameter interior). Thus, different nanotube diameters could play an important role in the designing of implantable devices, as it is possible to selectively promote the growth of one cell type over another.
Together with the choice for the most suitable surface modification technique, the evaluation of the physico-chemical properties of a biomaterial surface is compulsory for the proper design of body implants and to predict a priori the influence of the material properties on the events occurring at the bio-interface [12, 13]. In fact, the surface properties are responsible for the interactions with the surrounding tissues and, influencing the “race for the surface” between cells and bacteria , affect the consequent acceptance of the implant. The most studied surface characteristics concern the roughness and topography, chemical composition, and wettability, either at the micro- or nano-scale. Besides, the assessment of the surface charge of solids becomes fundamental when the adsorption of certain ions and proteins from the body fluids to the implant is considered. Therefore, the study of the implant surface electrokinetic behaviour is highly valuable, especially in connection with surface topography and wettability.
In fact, the electrostatic interactions are fundamental for binding with ions, plasma proteins and, subsequently, cells and tissues. For instance, the local surface charge can be related to the surface nano-roughness provided by the presence of TiO2 NTs. In particular, the high surface charge density at the sharp or convex edges of the nanotubes provides prominent binding sites for mono/divalent ions and for proteins with a distinctive quadrupolar charge distribution, able to mediate the further adhesion of osteoblasts . Accordingly, in our previous study, the binding of certain plasma proteins (important in wound healing and inflammatory responses) to TiO2 NTs with different diameters was studied . In that case, the surface charge of the nanotubes was assessed by measuring the zeta potential of NTs sheared out of the Ti-substrate. Even though the used electrophoretic mobility technique allowed the determination of ζ of the NTs in suspension, no significant difference was observed between the NTs with different diameters, either in terms of isoelectric point (IEP) values or ζ magnitude in dependence of the pH. Therefore, in the next step, the zeta potential of self-assembled TiO2 NTs on Ti surfaces was measured by streaming potential technique, when still adhered to the substrate . Streaming potential represents a reliable method to evaluate the surface charge by determining the zeta potential (ζ) at the interface between the material and the fluid around [12, 13, 16]. Differently from electrophoresis and electroacoustic techniques, the streaming potential technique consists in the formation of an electric field as the electrolyte flows tangentially to a stationary charged solid surface, so that the zeta potential is calculated out of the generated streaming potential.
Thus, the purpose of this work was to assess measurements of surface charge of electrochemically anodized titanium-based substrates used for hard tissue replacement. Zeta potential of TiO2 nanotubes and various elongated titanate derivatives has been already assessed via electrophoretic mobility measurements [17–19]. However, this technique does not allow the direct determination of surface charge on solid materials, only on suspensions or dispersions.
To our best knowledge, for the first time an electrokinetic study of zeta potential of TiO2 nanotube-coated titanium was accomplished systematically in biologically relevant electrolytes. The experimental data were supported by theoretical models, which resulted in equations specific to our system but applicable also to other nanoporous structures.
Growth of TiO2 Nanotubes
Anodization conditions used for fabrication of TiO2 nanotubes
Anodization time (h)
Characterisation of the Nanotube Arrays Morphology
The morphology of top view of the TiO2 nanostructures was observed using a field-emission scanning electron microscope (FE-SEM, Hitachi S4800). High contrast micrographs of nanostructured samples were obtained without any sputtering, as the obtained images already displayed reasonably good contrast.
The topographical features of Ti foil and TiO2-nanostructured surfaces were examined by Atomic Force Microscopy (Solver PRO, NT-MDT, Russia) in tapping mode in air. The samples were scanned with a standard Si cantilever at a constant force of 22 N/m and resonance frequency of 325 kHz (10-nm tip radius, 95-μm tip length). For comparison, the average surface roughness (R a) was calculated from 1 × 1μm2 area and the average values made on five different areas are presented.
Characterisation of the Nanotube Arrays Surface Charge by Electrokinetic Measurements
where dI str/d∆p represents the streaming current dependence to the pressure difference ∆p between the ends of the capillary in the measuring cell, η is the viscosity, ε is relative permittivity, ε 0 is the permittivity of the free space, and L and A are the length and the rectangular cross section of the capillary, respectively. According to the calibration, the precision of the instrument during the measurements was ±0.2 pH unit. Titration curves (dependence of ζ to the pH) were recorded in 0.001 mol/L biologically relevant media, in particular: sodium chloride saline solution (NaCl, Sigma-Aldrich), sodium chloride saline solution buffered with Tris(hydroxymethyl)aminomethane (TRIS, Alfa Aesar), phosphate buffer saline solution (PBS, tablets, Sigma-Aldrich), and Dulbecco’s modified Eagle medium (DMEM, GlutaMAX Supplement, Life Technologies). The influence of the electrolytic concentration on the ζ measurements was verified by systematically varying the molarity of the TRIS-buffered NaCl saline solution from 0.001 mol/L up to 0.1 mol/L.
Topographical investigations of the self-assembled TiO2 NT coatings were performed in terms of morphology and roughness prior any streaming potential measurement.
Effects of the Synthesis Parameters on the Nanotubes Morphology
Effect of the Biological Media on the Measured ζ Values
In the first set of experiments, the electrolytic concentration was kept constant at 1.5 mM, while the nature of the present ions in solution varied.
Effect of the Electrolytic Concentration on the ζ Values
The second set of experiments considered the influence of the electrolytic concentration on the Debye length and the width of the electrical double layer. NaCl was chosen as representative 1:1 electrolytic solution and the electrolytic concentration was systematically increased from 0.001 M up to 0.1 M (the limit of the electrokinetic analyser).
It is well known that the interaction and acceptance of a biomaterial at the biological level strongly depend on the surface properties of the implant itself. If on one hand the mechanical performances account on the bulk properties of the material, the surface properties such as charge, topography, roughness, and wettability are responsible for the first biological events after implantation. The growth of TiO2 nanotubes on Ti-based implants by electrochemical anodization has been reported to be a promising method to tailor the abovementioned surface properties at the nano- and micro-level, providing nano-roughness, high effective surface area and porosity, chemical stability, and high hydrophilicity [9, 10, 25]. However, due to technical limitations, not so much is known about the surface charge of TiO2 NTs-coated titanium implant surfaces. In our previous studies [12, 16], streaming potential technique was successfully applied to assess zeta potential values of titanium dioxide structures on Ti surfaces. In the case of NTs , the titration curves in very diluted, monovalent electrolytic solution (KCl) showed that all the surfaces were negatively charged at physiological pH, but they varied sequentially in ζ magnitude by changing the top diameter of the tubes . Proceeding from these experiences, the current research concerned the systematic study of the surface charge properties in biologically relevant media of TiO2 NT arrays grown on titanium substrates, in dependence of their NTs diameter, the electrolytic concentration, and the type of media.
Tailoring the synthesis parameters during the electrochemical anodization resulted into nanotubes with controlled diameters (with variable porosities). SEM (Fig. 1) and AFM (Fig. 2) analyses confirmed about the uniformity of nanotubular surface and hollowness of TiO2 nanostructures. The experimental results show that by appropriate electrochemical anodization conditions, it is possible to form uniform layer of nanotubes with 15, 50, and 100 nm in diameter. Differences in the average surface roughness of nanotubes and Ti foil were also experimentally evaluated, and it was shown that the most prominent increase in surface roughness was observed for the 100-nm nanotubes. These surface features, together with the information about the zeta potential values measured for biologically relevant electrolytes, provide important information on the interfacial phenomena which could be transferred into relevant biological environment (body implants).
It has to be mentioned here that the variability of the samples in terms of nanotubes diameter distribution (see Fig. 1) gave a certain variability also in the obtained zeta potential values, despite the high instrumental accuracy. In particular, the standard deviation calculated from the SEM micrographs match perfectly with the one observed for the experimental ζ-values. Accordingly, the accuracy of the zeta potential measurement is higher than the homogeneity of the nanotubular structures.
The experimental quantification of surface charge for different TiO2 NT surfaces (NTs-coated Ti-foil) was assessed in various electrolytic solutions, relevant for the biological assessment. The electrolytic concentration was kept very low (1.5 mM) to render the measurements independent to the salt concentration (ionic strength). This allowed to observe the effect of monovalent, divalent, or multivalent ions in the electrolytic solution on the compression of the electrical double layer.
Firstly, NaCl saline solution, widely used for its isotonicity with blood and tissues, was chosen as 1:1 physiological electrolyte (Fig. 3). All the self-assembled TiO2 NT arrays owned very similar IEPs (pH ~5), despites the different top NT diameters (15, 50, and 100 nm). However, all the samples were negatively charged at physiological pH, as already observed in the case of KCl 1:1 electrolyte , but they differed in magnitude. Nevertheless, the lowest recorded ζ value among the samples at pH = 7.4 was around −50 mV, which would correspond to nicely dispersed particles in case of suspensions. Therefore, it can be presumed that the analysed surfaces might display a little higher surface charge density, as estimated in the analysis presented in Fig. 6.
Nevertheless, some interesting differences can be noticed if the results in NaCl and in KCl  at physiological pH are compared. Even though both these salts give rise to 1:1 electrolytes, Na+ and K+ cations differ in specificity to the surface and in their hydrated ionic radius. The ionic specificity gives rise to a specific adsorption on the surface . At pH greater than the IEP, the ionic affinity for negatively charged, hydrophilic surfaces (TiO2 nanotubular surfaces in this work) is expected to follow the indirect Hofmeister series . Accordingly, Na+ would better stabilise the electrical double layer than K+, giving higher ζ in magnitude (this study) and i.e. reducing the agglomeration in case of colloidal particles . The Hofmeister series obey also the hydration rate of ions.
The experimentally determined difference in zeta potential of Ti foil between NaCl and KCl electrolyte is around 5–10 mV, which indicates that we have probably selected too small magnitude of surface charge density σ in the theoretical description of the experimental results for Ti foil presented in Fig. 6. Hence, σ value of Ti foil might be actually more negative than the estimated value −0.05 As/m2.
As shown by the theoretical calculations (Fig. 12), larger cations produce more negative surface potential at OHP than a smaller cation. Since hydrated Na+ are larger than K+, the theoretically predicted values of ζ potential for Ti foil and/or TiO2 NT surfaces are expected to be more negative in NaCl than in KCl, for about 10 mV (see Fig. 12 and ). This behaviour complied with our experimental results for the NTs 50 nm (Fig. 3, orange circles) and NTs 100 nm (Fig. 3, blue rhomboids), while NTs 15 nm acted as an exception (Fig. 3, green triangles), since the experimental data reveal lower absolute ζ-values (less negative charge) in NaCl than in KCl. This could be ascribed to several contingent factors, besides the variability among the samples, which inevitably occurs during the synthesis. For instance, NTs 15 nm presents very specific surface characteristics in comparison to the other two types of NT samples. In fact, NTs 15 nm owns a higher average surface roughness (Fig. 2), a higher surface porosity (Fig. 1), a higher total length of sharp edges of NT walls per unit top surface area (see also [9, 10, 25]), and the highest (accessible) surface area. All these features of NTs 15 nm may generate an “internal” streaming current within the hollow interiors of NTs 15 nm and also vortexes at the NTs surface, in addition to the “external” streaming current in the measuring capillary. Due to particular behaviour, the ζ computed by the Smoluchowski method (Eq. 1) results as “apparent” and rated too low/different. In addition, due to vortexes (turbulent flow), the basic assumption on which the Smoluchowski method was originally derived, i.e. the assumption of laminar flows, is violated. Accordingly, gap height dependence measurements  would be needed to assess more realistic ζ potential values (proposed as our next step).
Also, the wettability and reactivity of the hydroxyl groups on the surface “as-prepared” and “aged” have to be taken into account while interpreting the presented experimental results. Namely, already after a few hours from the preparation, the contact angles of the self-assembled nanotubes structures rise from super-hydrophilic (as-prepared) to hydrophobic by collecting organic contaminants (hydrocarbons) from the environment, if not protected in a controlled atmosphere or treated i.e. with gaseous plasma . NTs 15 nm sample shows the least hydrophilic surface among the three types of NT diameters, indicating a minor amount of free hydroxyl groups and less surface acidity, contributing to inferior ζ-values in magnitude.
All the differences among samples detected in 1:1 electrolytes were then mostly suppressed when multivalent ions electrolytes were used for the studies. Phosphate saline buffer solution was chosen as 1:3 electrolyte, containing monovalent cations such as Na+ and K+, and trivalent phosphate anions PO4 3− (Fig. 4). In comparison to the NaCl case, a noteworthy shift of the IEP towards acidic pH was observed for all the surfaces in PBS, with a more prominent effect for the tubular nanostructures. This indicates the occurrence of a preferential adsorption of phosphate anions on the top edges of the TiO2 NTs rather than on Ti foil, as previously indicated in  for TiO2 nanocrystalline films, even though no significant discrepancy was observed among the different NT diameters. In terms of magnitude of ζ potential, all the curves shifted and converged in a range between −40 and −50 mV at physiological pH. This behaviour may be ascribed to the effect of the multivalent phosphate ions (see also [9, 10, 25]). In fact, at constant electrolytic concentration (very low in our case 0.001 mM), the higher is the electrolyte valence, the larger is the ionic strength. In turn, since the Debye length is inversely proportional to the square root of the ion ionic strength, it is straightforward that the electric double layer shrank in presence of multivalent electrolytes (due to their strong screening effect) and, consequently, the surface charge appeared reduced.
In our experiments, when the electrolytic solution was exchanged with DMEM cell medium (to better mimic the real composition of body fluids), the TiO2 nanostructured surfaces experienced a completely different environment than in the previously described cases. DMEM solution contains very diverse ions, ranging from the monovalent ones (Na+, K+, Cl−), the divalent ones (Ca2+, Mg2+), to the multivalent ones (PO44 3-, SO4 2−), as well as zwitterionic substances such as the amino acids. Such a variety of cations and anions gave rise to a competition not only among these counterions in solution to “neutralise” the surface charge of the scaffolds, but also among each other within the double layer, due to the reciprocal direct attraction/repulsion forces. Therefore, the results on the IEP and on the ζ magnitude (blue titration curve with rhomboids in Fig. 5) depend on the reached equilibrium between the electrostatic forces among all the species involved. Contrarily to the PBS case, where the multivalent ions were represented only by phosphates, in DMEM the mutual effect of multivalent cations and anions resulted in: (a) specific adsorption of phosphates and sulphates which rendered the surface more acidic (pHIEP DMEM ~4) than in the case of NaCl (pHIEP NaCl ~5) but less acidic than in PBS (pHIEP PBS ~2.4); (b) no drastic effect on the double layer compression, with ζ values comparable with the ones in PBS.
As mentioned before, the first part of the results concerned the effect of ion valence on the extension of the electrical double layer. Thus, in some of the above-described experiments the electrolytic concentration was purposely kept very low, in order to exclude its effect on the ionic strength. However, in normal conditions, the biological fluids have a concentration of 0.15 M. Therefore, the influence of the solution concentration was also examined, by systematically varying the experimental electrolytic concentration till 0.1 M (Fig. 11). In order to avoid any impact of the valence, this time the 1:1 NaCl electrolyte was chosen.
In the experiments, the decrease of ζ with the increase of the electrolyte concentration, observed for flat Ti foil, is preserved also for 15, 50, and 100-nm NT-coated surfaces (Fig. 10), where the effective/average surface charge density σ obviously depends on the NT diameter and surface roughness. Based on the experimental results presented in Fig. 10, it can be concluded that among the chosen NTs-coated surfaces (Figs. 1 and 2), the TiO2 surfaces formed by NTs with 100-nm diameter display the lowest exposed top surface area (due to the most voids) and the lowest effective/average surface charge density σ among the three NT diameters. In contrast, the substrates covered by NTs with 15 nm diameter present the highest exposed surface area and the highest effective/average surface charge density, partially ascribable to the longest total length of sharp convex top edges of NT walls . The major influence of NT voids on the magnitude of ζ is expected for the NTs 100 nm diameter, while a weaker effect is expected for the NTs 50 nm diameter, and even less for the NTs 15 nm diameter. The assumed trend is actually obeyed in experiments only in the case of NTs 50 nm and NTs 100 nm, while NTs 15 nm showed a distinctive behaviour, owning experimentally determined value of ζ magnitude very similar to the one of NTs 100 nm at all the considered NaCl concentrations (Fig. 10). As in the case of the titration curves in NaCl (Fig. 3), diverse phenomena like for example surface roughness, not included into the experimental determination of ζ(I str), can anyway influence the obtained data for NTs 15 nm and, therefore, partially explain the reason of deviation from the expected results for NTs 15 nm.
This study presents results on surface charge measurements of electrochemically anodized TiO2 nanotubes, proposed as materials for body implants, in biologically relevant electrolytes (NaCl, PBS, cell medium). The use of an electrokinetic analyser allowed for the systematic accomplishment of zeta potential titration curves at low electrolytic concentration (10−3 M), single points at fixed—physiological—pH and at various electrolytic concentrations (up to 0.1 M). Accordingly, the results were presented considering the effect of the ionic strength, as well as the multivalence of the electrolytes in solution. Zeta potential was shown to be mostly influenced by the ionic strength, while the IEPs were mostly affected by the valence and charge of the electrolytic ions, as a proof of their adsorption/interaction with the surfaces. Also, the effects of surface porosity and the surface area, exposed to the solution, were taken into account. Hence, several hypotheses were formulated to explain the behaviour of the three different morphological dimensions of NTs (with 15, 50 and 100 nm in diameter), i.e. considering their topographical characteristics, as well as their wettability and the ion affinity towards the surfaces. The experimental data were supported by the theoretical model, adjusted to our specific system/cases, but applicable also to other nanoporous structures.
Overall, the outcomes definitely broad the scenario of the characterisation of the implant surfaces at the bio-interface. However, in the current study the effect of surface porosity and roughness to the conductance and “apparent” streaming current effects have not been quantitatively assessed; therefore, gap height dependence measurements have been planned as the next step of our investigations.
The authors would like to acknowladge the Slovenian Research Agency (ARRS, grant L7-7566) and the grant (P2-0232) for generous financial support to carry out this research.
ML, MK and IJ designed the experiment, fabricated TiO2 nanotubes, preformed zeta potential measurements, AFM analysis. EK and AI made the numeric simulations. All the authors collaborated in writing the manuscript text and all the authors reviewed the manuscript.
The authors declare that they have no competing intrests.
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- Ratner BD (2001) A perspective on titanium biocompatibility. Titanium in medicine: material science, surface science, engineering, biological responses and medical applications. Springer Berlin Heidelberg, Berlin, Heidelberg, pp 1–12Google Scholar
- Geetha M, Singh AK, Asokamani R, Gogia AK (2009) Ti based biomaterials, the ultimate choice for orthopaedic implants—a review. Prog Mater Sci 54(3):397–425View ArticleGoogle Scholar
- Mendonca G, Mendonca DB, Aragao FJ, Cooper LF (2008) Advancing dental implant surface technology—from micron- to nanotopography. Biomaterials 29(28):3822–35View ArticleGoogle Scholar
- Bauer S, Schmuki P, von der Mark K, Park J (2013) Engineering biocompatible implant surfaces: Part I: materials and surfaces. Prog Mater Sci 58(3):261–326View ArticleGoogle Scholar
- Shekaran A, Garcia AJ (2011) Nanoscale engineering of extracellular matrix-mimetic bioadhesive surfaces and implants for tissue engineering. Biochim Biophys Acta 1810(3):350–60View ArticleGoogle Scholar
- Mazare A, Totea G, Burnei C, Schmuki P, Demetrescu I, Ionita D (2016) Corrosion, antibacterial activity and haemocompatibility of TiO2 nanotubes as a function of their annealing temperature. Corros Sci 103:215–22View ArticleGoogle Scholar
- Neacsu P, Mazare A, Cimpean A, Park J, Costache M, Schmuki P et al (2014) Reduced inflammatory activity of RAW 264.7 macrophages on titania nanotube modified Ti surface. Int J Biochem Cell Biol 55:187–95View ArticleGoogle Scholar
- Moerke C, Mueller P, Nebe B (2016) Attempted caveolae-mediated phagocytosis of surface-fixed micro-pillars by human osteoblasts. Biomaterials 76:102–14View ArticleGoogle Scholar
- Kulkarni M, Mazare A, Gongadze E, Perutkova S, Kralj-Iglic V, Milosev I et al (2015) Titanium nanostructures for biomedical applications. Nanotechnology 26(6):062002View ArticleGoogle Scholar
- Lee K, Mazare A, Schmuki P (2014) One-dimensional titanium dioxide nanomaterials: nanotubes. Chem Rev 114(19):9385–454View ArticleGoogle Scholar
- Kulkarni M, Flasker A, Lokar M, Mrak-Poljsak K, Mazare A, Artenjak A et al (2015) Binding of plasma proteins to titanium dioxide nanotubes with different diameters. Int J Nanomedicine 10:1359–73Google Scholar
- Lorenzetti M, Bernardini G, Luxbacher T, Santucci A, Kobe S, Novak S (2015) Surface properties of nanocrystalline TiO 2 coatings in relation to the in vitro plasma protein adsorption. Biomed Mater 10(4):045012View ArticleGoogle Scholar
- Lorenzetti M, Luxbacher T, Kobe S, Novak S (2015) Electrokinetic behaviour of porous TiO2-coated implants. J Mater Sci Mater Med 26(6):1–4View ArticleGoogle Scholar
- Gristina AG (1987) Biomaterial-centered infection: microbial adhesion versus tissue integration. Science 237(4822):1588–95View ArticleGoogle Scholar
- Gongadze E, Kabaso D, Bauer S, Slivnik T, Schmuki P, van Rienen U et al (2011) Adhesion of osteoblasts to a nanorough titanium implant surface. Int J Nanomedicine 6:1801–16Google Scholar
- Kulkarni M, Patil-Sen Y, Junkar I, Kulkarni CV, Lorenzetti M, Iglič A (2015) Wettability studies of topologically distinct titanium surfaces. Colloids Surf B: Biointerfaces 129:47–53View ArticleGoogle Scholar
- Horváth E, Grebikova L, Maroni P, Szabó T, Magrez A, Forró L et al (2014) Dispersion characteristics and aggregation in titanate nanowire colloids. ChemPlusChem 79(4):592–600View ArticleGoogle Scholar
- Liu W, Sun W, Borthwick AGL, Ni J (2013) Comparison on aggregation and sedimentation of titanium dioxide, titanate nanotubes and titanate nanotubes-TiO2: influence of pH, ionic strength and natural organic matter. Colloids Surf A Physicochem Eng Asp 434:319–28View ArticleGoogle Scholar
- Pavlovic M, Adok-Sipiczki M, Horváth E, Szabó T, Forró L, Szilagyi I (2015) Dendrimer-stabilized titanate nanowire dispersions as potential nanocarriers. J Phys Chem C 119(44):24919–26View ArticleGoogle Scholar
- Roy P, Berger S, Schmuki P (2011) TiO2 nanotubes: synthesis and applications. Angew Chem Int Ed Engl 50(13):2904–39View ArticleGoogle Scholar
- Kowalski D, Kim D, Schmuki P (2013) TiO2 nanotubes, nanochannels and mesosponge: self-organized formation and applications. Nano Today 8(3):235–64View ArticleGoogle Scholar
- Delgado AV, González-Caballero F, Hunter RJ, Koopal LK, Lyklema J (2007) Measurement and interpretation of electrokinetic phenomena. J Colloid Interface Sci 309(2):194–224View ArticleGoogle Scholar
- Niecikowska A, Krasowska M, Ralston J, Malysa K (2012) Role of surface charge and hydrophobicity in the three-phase contact formation and wetting film stability under dynamic conditions. J Phys Chem C 116(4):3071–8View ArticleGoogle Scholar
- Horváth E, Szilágyi I, Forró L, Magrez A (2014) Probing titanate nanowire surface acidity through methylene blue adsorption in colloidal suspension and on thin films. J Colloid Interface Sci 416:190–7View ArticleGoogle Scholar
- Kulkarni M, Mazare A, Schmuki P, Iglič A (2014) Biomaterial surface modification of titanium and titanium alloys for medical applications. Nanomedicine. Manchester: One Central Press. p. 111–36Google Scholar
- Dumont F, Warlus J, Watillon A (1990) Influence of the point of zero charge of titanium dioxide hydrosols on the ionic adsorption sequences. J Colloid Interface Sci 138(2):543–54View ArticleGoogle Scholar
- Oncsik T, Trefalt G, Borkovec M, Szilagyi I (2015) Specific ion effects on particle aggregation induced by monovalent salts within the Hofmeister series. Langmuir 31(13):3799–807View ArticleGoogle Scholar
- Yukselen-Aksoy Y, Kaya A (2011) A study of factors affecting on the zeta potential of kaolinite and quartz powder. Environ Earth Sci 62(4):697–705View ArticleGoogle Scholar
- Coday BD, Luxbacher T, Childress AE, Almaraz N, Xu P, Cath TY (2015) Indirect determination of zeta potential at high ionic strength: specific application to semipermeable polymeric membranes. J Membr Sci 478:58–64View ArticleGoogle Scholar
- Vinogradov J, Jaafar MZ, Jackson MD (2010) Measurement of streaming potential coupling coefficient in sandstones saturated with natural and artificial brines at high salinity. J Geophys Res 115(B12):1–18Google Scholar
- Kulkarni M, Junkar I, Puliyalil H, Iglic A (2016) Wettability switch of anodic titanium dioxide nanotubes with various diameters. Biophys J 110(3, Supplement 1):339aView ArticleGoogle Scholar
- Gongadze E, Iglič A (2015) Asymmetric size of ions and orientational ordering of water dipoles in electric double layer model—an analytical mean-field approach. Electrochim Acta 178:541–5View ArticleGoogle Scholar
- Wicke E, Eigen M (1952) über den Einfluss des Raumbedarfs von Ionen wässriger Lösung auf ihre Verteilung im elektrischen Feld und ihre Aktivitätskoeffizienten. Z Elektrochem 38:551–61Google Scholar
- Eigen M, Wicke E (1954) The thermodynamics of electrolytes at higher concentration. J Phys Chem 58(9):702–14View ArticleGoogle Scholar
- Gongadze E, Iglič A (2012) Decrease of permittivity of an electrolyte solution near a charged surface due to saturation and excluded volume effects. Bioelectrochemistry 87:199–203View ArticleGoogle Scholar
- Woods DR, Diamadopolous E (1988) Importance of surfactants and surface phenomena on separating dilute oil-water emulsions and dispersions. Surfactants Chem/Process Eng 19:369–553Google Scholar