Liguang Qinab,
Wenjie Zhao*a,
Hua Houb,
Yuchun Jinb,
Zhixiang Zeng*a,
Xuedong Wua and
Qunji Xuea
aKey Laboratory of Marine New Materials and Related Technology, Zhejiang Key Laboratory of Marine Materials and Protection Technology, Ningbo Institute of Materials Technology & Engineering, Chinese Academy of Sciences, Ningbo 315201, China. E-mail: zhaowj@nimte.ac.cn; zengzhx@nimte.ac.cn
bSchool of Materials Science and Engineering, North University of China, Taiyuan 030000, China
First published on 3rd November 2014
Aluminum alloy surfaces with micro/nano-structures were fabricated via a simple chemical etching (CE) method. After chemical modification with perfluorodecyltriethoxysilane (PFDS), n-octadecyltriethoxysilane (OTS) and aminopropyltriethoxysilane (APS), surfaces with different wettability were obtained. The morphology and chemical elements of the as-prepared surfaces were investigated by atomic force microscopy (AFM), scanning electron microscopy (SEM) and X-ray photoelectron spectroscopy (XPS). In addition, the influence of the surface morphology and chemical modification on the wetting/dewetting properties was investigated. Finally, the anti-corrosion and tribological properties of the as-prepared self-assembled monolayers (SAMs) were characterized using an electrochemical workstation and UMT-3 tribometer. The influence of surface morphology and SAMs on the anti-corrosion and tribological performances is discussed in detail. The results showed that the optimal preparation conditions consisted of a 40% volume fraction of hydrochloric acid with a CE time of 2 min. The corrosion resistance of the surfaces chemically modified with hydrophobic groups was much better than that of those modified with hydrophilic groups. Also, the combination of micro/nano-structures and suitable SAMs on aluminum alloy surfaces could greatly enhance the friction reduction and wear resistance behavior.
Micro/nano-structures on a surface change the contact mode and wetting/dewetting ability of the interface, which have a determinable influence on the tribological and anti-corrosion6,7 behaviour. Meanwhile, molecular thinness, the relatively strongly chemically bonded interface and the simple, convenient and reliable preparation process make SAMs inherently manufacturable, thus attracting interest for constructing effective boundary lubricants and superhydrophobic interfaces.8–10 Thus tailoring surface topography and surface chemical modification may be two crucial strategies to improve the anti-corrosion and tribological performance of self-assembled samples.11,12 Ou et al.13 prepared superhydrophobic textured copper surfaces by CE/oxidation and surface fluorination, and found that the film showed much better corrosion protection as compared with the control samples. Mo et al.14 showed that tribological performance could be induced by designing a suitable surface texture combined with modification with a hydrophobic anion on the surface. Zhao et al.15 prepared Au surfaces with micro/nano-hierarchical structures by replication of micro-patterned silicon surfaces using polydimethylsiloxane (PDMS) and self-assembly of alkanethiol to create hydrophobic micro/nano-hierarchical structures. All of the above studies verified that surface topography is an effective strategy to enhance anti-corrosion and tribological performance. Through a variety of methods for the preparation of textured or superhydrophobic surfaces, such as laser/plasma/chemical etching,16 chemical vapor deposition,17 micro-contact printing,18 and photolithography,19 various patterned surfaces have been prepared for application in anti-corrosion, lubrication16,20,21 and other fields.22,23
Inspired by the above-mentioned correlation between surface structures and chemical modification, and anti-corrosion and tribological behavior, the structures and chemical composition of aluminum alloy surfaces are adjusted via an acid etching and chemical modification method. In this work, a simple and versatile procedure combining micro/nano-hierarchical structures and further modification with low-surface-energy molecules has been proposed to fabricate hydrophobic and hydrophilic films on aluminum alloy AA 2024 substrates. The procedure is very impressive for its universality, simplicity and flexibility; it can be applied to treat a wide range of aluminum alloys. Moreover, the chemical etching agent is HCl, which is cheap and easy to obtain. Electrochemical and tribological measurements as well as surface analysis methods were used in this paper to reveal the corresponding synergetic anti-corrosion, friction reduction and wear resistance mechanisms of micro/nano-structures and chemical modification.
The tribological tests were conducted on a UMT-3 tribometer (CETR, USA), using a reciprocating ball-on-plate mode. Commercially available steel balls with a diameter of 4 mm were used as the stationary upper counterparts, while the lower Al alloys coated with various SAMs were fixed on the flat base, which reciprocated over a distance of 5 mm. The friction coefficient-versus-time curves were recorded automatically. At least three repeated measurements were performed for each frictional pair. Failure of the SAM film was assumed to occur when the coefficient of friction (COF) rises sharply to a high and stable value similar to that of a clean Al alloy 2024 against the same counterpart (about 0.7).
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Fig. 1 Schematic illustration of the preparation process of micro/nano-textures and SAMs on an Al alloy substrate. |
The driving force for this self-assembly is the in situ formation of polysiloxane, which is connected to the surface hydroxyl groups (–OH) via Si–O–Al bonds.27 The process in which the OTS-SAM with –CH3 outer groups is covalently anchored onto the Al alloy wafer is shown in Fig. 2. The figure also indicates how the PFDS-SAM with –CF3 and APS-SAM with –NH2 outer groups are formed.
To characterize the surface features of various samples, FESEM and three-dimensional (3D) AFM images were obtained as shown in Fig. 3 and 4, respectively. For the bare substrate, abrasive grooves are observed (Fig. 3a); the treated Al alloys with different processing times ((b) 30 s; (c) 60 s; (d) 90 s; (e) 120 s; (f) 180 s) exhibit different rough surface structures. It can be seen from Fig. 3b–d that the surface morphology of the samples is not completely chemically etched. Scratches exist from the pretreatment as well as a few grooves from etching by dilute hydrochloric acid on the surfaces. By contrast, with the increase of etching time, the Al alloy surfaces become rougher. There are irregularly shaped particles on the surfaces. Under higher magnifications (Fig. 3g and h), these petals can be clearly observed, with a height of several tens of nanometers and a length of several micrometers. The disordered arrangement of these petals leads to a rough structure. Roughness values (Ra) can be read from Fig. 4. The Ra values of the various samples etched for different times are 0.432 μm, 0.679 μm, 0.799 μm, 2.55 μm, 3.89 μm, and 3.28 μm (Fig. 4a–f), respectively. The value of Ra increased with the chemical etching time. So, it can be concluded that such a CE process plays an essential role in fabricating micro/nano-structures on Al alloys and in determining the Ra value. When the CE time is more than 2 min, the surface of the Al alloy is completely etched, and the as-prepared surface is much rougher.
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Fig. 3 FESEM images for samples etched for different times: (a) 0 s; (b) 30 s; (c) 60 s; (d) 90 s; (e) 120 s; (f) 180 s; (g) and (h) are higher-magnification images of (c) and (e), respectively. |
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Fig. 4 3D AFM topographic images and roughness parameters for samples etched for different times: (a) 0 s; (b) 30 s; (c) 60 s; (d) 90 s; (e) 120 s; (f) 180 s. |
XPS was performed to investigate the surface chemistry of samples treated with OTS, PFDS and APS. Besides the signals originating from the Al alloy substrates, other signals in the survey spectra (such as F1s, Si2p, C1s, N1s and O1s) can be attributed to the chemically adsorbed silane coupling agents. Specifically, the F1s signal (688 eV) (Fig. 5b) is consistent with the results reported by Saleema.28 In both of the two experiments, F element exists as part of an F–C bond of the silane. Moreover, the high resolution C1s core level spectra (Fig. 5b), resolved into four components,29 namely, –CF3, –CF2, –CH2–CF2, and –CH2–CH2–, can be used as evidence for the adsorption of PFDS. The O1s peak (Fig. 5) can be resolved into three components with binding energies of 530.6 eV, 531.8 eV and 533.1 eV, illustrating the formation of Al–O–Al, Si–O–Al and Si–O–Si,30 respectively. This may prove the assumption that the alloy substrate is not only changed by the formation of direct bonds with oxygen but also the chemically adsorbed materials from OTS, PFDS or APS. Fig. 5c also shows the deconvoluted N1s region. The single strong peak at 400.5 eV is attributed to –NH2 from the APS.
Fig. 6 shows the results of wettability measurements for the as-fabricated samples. As shown in Fig. 3a, the bare Al alloy used here had a smooth surface without micro- or nanostructures. When the substrates were immersed into the HCl solution, a fast chemical etching process occurred, and the surfaces became rougher with the build-up of numerous intercrossed nano-platelets31 (Fig. 3b–f). When the etching time was 2 min, some micropits existed on the Al alloy substrate, and it was noted that the nano-platelets still covered the surface and each micro-convexity had numerous nanosteps on its surface, indicating the appearance of dual-scale roughness on the Al alloy substrate (Fig. 3h). The value of the surface roughness was 3.89 μm and the WCA reached a maximum of 149° and 145° (Fig. 6) when the surface was modified by PFDS and OTS, respectively. The reasons for this were that the surface was modified with low-surface-energy materials and the Al alloy surface was composed of air trapped notches and micro/nano-convexities.32 This explanation can be expressed theoretically by the Wenzel equation, which explains how surface roughness increases or decreases wettability for a liquid droplet on a rough solid surface:33,34
cos![]() ![]() ![]() | (1) |
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Fig. 6 Relationship between the etching time and the WCA with different low-surface-energy molecules. |
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Fig. 7 Polarization curves of (a) PFDS- and (b) OTS-modified samples, (c) the bare Al substrate, (d) the APS-modified sample and (e) the CE substrate. |
Samples | Ecorr (mV) | Icorr (μA cm−2) |
---|---|---|
OTS-modified sample | −546.8 | 1.321 |
PFDS-modified sample | −564.4 | 1.148 |
APS-modified sample | −1073 | 6.602 |
Bare aluminum alloy | −1057 | 4.303 |
CE substrate | −1112 | 15.35 |
The highest Icorr and most negative Ecorr values of the plots in Fig. 7 suggest that the chemically etched aluminum alloy substrates are the most prone to corrosion. This may be attributed to the fact that after chemical etching, the native oxide is removed, such that a fresh and active surface is obtained and the chemical reactions causing corrosion occur easily. For CE samples modified by OTS and PFDS, a positive shift in Ecorr and a reduction in Icorr are observed, mainly because the generated hydrophobic film can serve as a layer to obstruct the diffusion of water and other corrosive species dissolved in water. Because of the polar terminal groups in APS, the APS-modified sample shows hydrophilic properties, as water and other corrosive species can attach to the surface. A negative shift of Ecorr and an increase of Icorr are observed.
Fig. 8 presents the impedance (a) and phase angle (b) graphs for different samples. Generally, the impedance values at low frequency was consider as an indicator of anti-corrosion performance. The impedance values at 0.1 Hz of the PFDS-, OTS- and APS-modified samples, the bare Al and the CE substrate are 18.77 kΩ cm2, 17.34 kΩ cm2, 14.16 kΩ cm2, 6.74 kΩ cm2 and 1.01 kΩ cm2, respectively. All SAMs-modified surfaces have larger impedance values and a quicker increase in the phase angle than the bare and CE surfaces. Also, it can be seen from Fig. 8 that the impedance spectra of the bare Al, APS-SAM and CE surface have a capacitive loop in the low frequency zone. For the specimens treated with PFDS and OTS, the loop shifts to a higher frequency zone. This is because the structure of the aluminum alloy surface has been changed by CE and self-assembly.
Two methods were used to analyze the EIS data. The former involved reading values directly from the impedance spectra, and the latter involved equivalent circuit modeling. As shown in Fig. 9, the equivalent circuit model (a) is used for the bare aluminum alloy and CE samples, and (b) is for the PFDS-, OTS- and APS-modified samples. In these circuit models, Rct||Qdl is assigned to the impedance of the interface reaction between the film and the substrate. The impedance of a constant phase element (CPE) depends on the frequency via the relation ZCPE = 1/C(jω)n where C is the capacitance, J is the square root of −1 and ω is the angular frequency. As n approaches 1, the impedance of a CPE reduces to that of a true capacitor.35 Rfilm||Cfilm is assigned to the impedance of the interface and Rs represents the resistance of the 3.5 wt% NaCl solution. The values of these parameters are shown in Table 2. The Rct values derived from Table 2 are of almost the same order of magnitude as the |Z| values from electrochemical impedance spectroscopy at 0.1 Hz. This indicates that the equivalent circuit models are well suited for electrochemical impedance spectroscopy.
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Fig. 9 Equivalent circuit models for (a) bare Al and CE samples and (b) OTS-SAM, PFDS-SAM and APS-SAM samples immersed in 3.5 wt% NaCl solution. |
Electrode | OTS-modified sample | PFDS-modified sample | APS-modified sample | Bare Al | CE sample |
---|---|---|---|---|---|
Rct/Ω cm2 | 1.734 × 104 | 1.877 × 104 | 1.416 × 104 | 6.74 × 103 | 1.007 × 103 |
Qdl/Ω−1 sn cm2 | 5.092 × 10−6 | 1.267 × 10−6 | 6.761 × 10−5 | — | — |
ndl | 1 | 1 | 0.6093 | — | — |
Rs/Ω cm2 | 22.21 | 28.53 | 33.31 | 40.78 | 18.66 |
Rfilm/Ω cm2 | 809.8 | 2452 | 399.9 | — | — |
Cfilm/F cm−2 | 3.263 × 10−7 | 1.105 × 10−7 | 4.834 × 10−7 | 8.703 × 10−6 | 3.274 × 10−4 |
Equivalent circuit | R(C(R(CR))) | R(C(R(CR))) | R(Q(R(CR))) | R(CR) | R(CR) |
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Fig. 10 Variation of COF with sliding time for various films: (a) bare Al; (b) APS-SAM; (c) PFDS-SAM; (d) OTS-SAM. |
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Fig. 11 Tribological properties of different samples under an applied load of 4 N and with a sliding frequency of 1 Hz: (a) COF; (b) wear rate for samples with different CE times. |
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