Elsevier

Applied Surface Science

Volume 265, 15 January 2013, Pages 88-93
Applied Surface Science

Advancing and receding angles – Dynamic contact angle measurements on mixed alkyl monolayers

https://doi.org/10.1016/j.apsusc.2012.10.128Get rights and content

Abstract

Mixtures of 1-decene and methyl-10-undecenoate with different mole fractions were used to prepared mixed monolayers on silicon (1 0 0) surfaces. The formed layers were characterized by dynamic contact angle measurements of two different liquids using the dynamic sessile drop method. The advancing and receding contact angles as well the calculated molar wetting free energies decreased with increasing mole fraction of methyl-10-undecenoate. Otherwise the molar dewetting free energies as well as the contact angle hysteresis stay nearly constant. A difference in the wetting and dewetting properties on mixed monolayers is observed, whereby mainly dispersive interactions are responsible for wetting. Furthermore we show that the contact angle hysteresis is independent of surface roughness, surface composition and surface free energy, which indicates that neither surface roughness nor heterogeneities are responsible for this hysteresis. We attribute the hysteresis to interactions between the liquid and the silicon substrate.

Highlights

▸ Dynamic contact angles are studied on mixed alkyl monolayers bound to silicon. ▸ Dispersive forces determine the wetting behavior on mixed monolayers. ▸ No pinning effect of the polar groups in the monolayer can be found. ▸ Long range interactions are responsible for contact angle hysteresis.

Introduction

Contact angle measurements are of increasing interest in investigations of surface properties like self cleaning surfaces and superhydrophobicity [1], [2], [3], [4], [5]. Here two different variants are commonly used as they give a fast experimental overview of the macroscopic characteristics: static contact angle measurements [6] as well as advancing and retracting contact angle measurements (in the following dynamic contact angle) [7], [8], [9], [10], [11], [12], [13], [14], [15], [16], [17], [18], [19], [20], [21], [22], [23], [24]. The preferred method for characterization, the dynamic contact angle measurements, is carried out on bare or monolayer-terminated surfaces. Most investigations were done on monolayers consisting of one type of molecule [7], [8], [9], [10], [11], [12], [13], [14], [15], [16] while measurements on mixed monolayers are quite rare [17], [18], [19], [20], [21], [22], [23], [24]. Extrand [7], [8], [9] performed investigations on the molar free wetting and dewetting energies on monolayer terminated surfaces consisting one type of molecule. Mixed monolayers on gold have been investigated by dynamic contact angle measurements [25] and the results were investigated with respect to the molar free energy [7].

Generally during dynamic contact angle measurements two specific contact angles occur: the advancing and receding contact angle. The advancing contact angle θa can be measured by inflating a liquid drop on a substrate surface, while the receding contact angle θr arises by shrinking a liquid drop on the surface. The difference between the two angles is known as the contact angle hysteresis.

Different interactions between the liquid and the surface cause contact angle hysteresis. Generally the receding contact angle is smaller than the static contact angle. Compared to the static contact angle the advancing contact angle is either larger or in the cases of polar liquids about the same [20]. In the case of mixed monolayers the fraction of dispersive surface groups can play a role for the advancing contact angle of polar liquids, since these groups prevent an unhindered spreading of the polar liquid. On the other hand polar groups support a spreading of the polar liquids. Consequently, polar groups determine the receding contact angle, since the polar liquid sticks on these groups [26]. In contrast for dispersive liquids the polar groups are crucial for the advancing contact angle and the dispersive groups for the receding contact angle. Beside this also roughness and heterogeneity of a surface can influence the contact angle and as it has been shown that also perfectly flat and homogenous surfaces are characterized by contact angle hysteresis [9], further parameters has to be taken into account.

In the present work a series of mixed 1-decene (DEC)/methyl-10-undecenoate (MUD) monolayers on silicon were prepared and characterized by dynamic contact angle measurements. These films are prepared by covalent attachment of alkenes to a bare silicon surface, which is different from often described monolayers on gold or oxide surfaces [9], [19], [27], [28]. The alkyl monolayer formation is well-known and can be realized e.g. by thermal reaction [19], [27], [28], [29]. By using terminal functionalized alkenes (e.g. carboxyl, hydroxyl, amino or ester groups) the properties of the monolayer can be easily modified which enables a wide variation of the surface properties [29], [30], [31]. Additionally the surface properties can be tuned gradually by mixing different alkenes [32]. Such mixed monolayers can act as nanostructures in hierarchical-structured surfaces which are known to influence the properties of liquids and the underlying microstructured substrate [33].

The aim of this study is to investigate the dependence of the dynamic contact angles and the associated molar wetting energies on the distribution of MUD within the DEC layer. Therefore we studied a series of monolayers with a different mixing ratio between DEC and MUD with the dynamic sessile drop method.

Section snippets

Experimental

All chemicals were of reagent grade or the highest available commercial grade quality (spectroscopic grade) and purchased from Merck KGaA (Darmstadt, Germany). Ultrapure water (>18.2  cm; 4 ppb TOC) was obtained from a Millipore Milli-Q Advantage water system (Millipore, Billerica, MA).

The silicon (1 0 0) substrates (>3000 Ω cm, n-type) were cleaned in acetone (at 40 °C), ethanol (40 °C), ‘piranha’ (volume ratio H2SO4:H2O2 3:2, 80 °C, CAUTION: Piranha solution is highly corrosive and should be handled

Results

After the preparation of pure and mixed alkyl monolayers with varying composition of MUD and DEC as described earlier [35], [36], the samples were investigated with dynamic contact angle measurements. Typical results are shown in Fig. 2, where the advancing and receding contact angles of water (Fig. 2 upper part) and diiodomethane (Fig. 2 lower part) are displayed as a function of MUD concentration. Each data point represents the averaged measurement results of five different areas on each of

Discussion

The monolayer consists of the same MUD ratio as reaction solution. This has been demonstrated by different groups with independent techniques [27], [29], [37]. Reason for this is the radical reaction of the monolayer formation process. The distribution of the MUD is statistically within the monolayer, as it has been found in capacitance measurements [37]. Also theoretical calculations supports this random arrangement of MUD, as only a small stabilizing effect of the formation of islands ester

Conclusions

We showed that for mixed monolayers differences in the wetting and dewetting properties can be found. The general behavior of the advancing angle and the receding angle follow the static contact angles. The molar free energies of mixed monolayers were calculated, whereby the free wetting energies show a similar behavior while for the free dewetting energy a nearly constant value was found. This indicates that mainly dispersive interactions are responsible for the wetting which is supported by

Acknowledgements

We thank C. von Borczyskowski for intense discussion and remarks. One author (H.G.) acknowledges financial support by the Deutsche Forschungsgemeinschaft (GR 2659/4-1).

References (49)

  • D. Janssen et al.

    Thin Solid Films

    (2006)
  • C.W. Extrand

    Journal of Colloid and Interface Science

    (1998)
  • J. Piehler et al.

    Biosensors & Bioelectronics

    (1996)
  • S.M. Flores et al.

    Surface Science

    (2006)
  • M. Ara et al.

    Thin Solid Films

    (2006)
  • F. Wei et al.

    Thin Solid Films

    (2002)
  • R.E. Johnson et al.

    Journal of Colloid Science

    (1965)
  • L.S. Penn et al.

    Colloid and Interface Science

    (1980)
  • D.Y. Kwok et al.

    Colloid and Interface Science

    (1995)
  • X. Li et al.

    Langmuir

    (2010)
  • H.L. Li et al.

    Langmuir

    (2010)
  • S.M.M. Ramos et al.

    Langmuir

    (2010)
  • Y.-T. Peng et al.

    Langmuir

    (2010)
  • M. Nosonovsky et al.

    Multiscale Disspiative Mechanisms and Hierarchical Surfaces: Friction, Superhydrophobicity and Biomimetics

    (2008)
  • C.W. Extrand

    Langmuir

    (2003)
  • C.W. Extrand

    Langmuir

    (2004)
  • M.R. Linford et al.

    Journal of the American Chemical Society

    (1993)
  • A.N. Parikh et al.

    Journal of Physical Chemistry

    (1994)
  • T.J. Sende et al.

    Colloids and Surfaces A

    (1994)
  • A.B. Sieval et al.

    Langmuir

    (1998)
  • A.B. Sieval et al.

    Langmuir

    (1999)
  • H. Yasuda et al.

    Journal of Polymer Science

    (1981)
  • A. Heise et al.

    Langmuir

    (1997)
  • M.R. Linford et al.

    Journal of the American Chemical Society

    (1995)
  • Cited by (9)

    • Research on classification of the oral liquid formulations of traditional Chinese medicine and critical quality parameters affecting organoleptic properties based on apparent and oral texture for placebo simulation

      2023, Journal of Drug Delivery Science and Technology
      Citation Excerpt :

      Polar groups, and from the other hand, encourage the diffusion of polar liquids. Because the polar liquid adheres to polar groups, they control the receding contact angle [24]. Furthermore, fluid parameters have to be taken into account during the oral process.

    • Effect of coupling agent on surface free energy of organic modified attapulgite (OAT) powders and tensile strength of OAT/ethylene-propylene-diene monomer rubber nanocomposites

      2015, Powder Technology
      Citation Excerpt :

      It can be defined as the ability of unsaturated surface atoms with a tendency of being compensated from environment. The dispersive interaction is mainly originated from van der Waals force, and polar interaction is mainly originated from the polarity of molecules [23,24]. Experimental measurements of surface energy (Table 1) of OAT modified by various contents of titanate and silane revealed that coupling agent had a drastic effect on the surface energy of fillers.

    View all citing articles on Scopus
    1

    Present address: Department of Physics, University of Konstanz, D-78464 Konstanz, Germany.

    View full text