Oliver
Roling‡
,
Lucas
Stricker‡
,
Jens
Voskuhl‡
,
Sebastian
Lamping
and
Bart Jan
Ravoo
*
Organic Chemistry Institute and Center for Soft Nanoscience, Westfälische Wilhelms-Universität Münster, Corrensstrasse 40, 48149 Münster, Germany. E-mail: b.j.ravoo@uni-muenster.de
First published on 8th December 2015
Surface immobilised polymer brushes containing azobenzene units were prepared using a combination of microcontact chemistry and surface-initiated atom transfer radical polymerisation (SI-ATRP). These brushes were investigated using AFM, XPS and UV/vis spectroscopy. It was shown that two surfaces bearing azobenzene brushes can be glued together in the presence of a β-cyclodextrin polymer and hold as much as 700 ± 150 g cm−2.
ATRP-TAD functionalised substrates were subjected to random copolymerisation using HEA and 7.5 mol% of AZA in order to yield guest modified polymer brush surfaces. The brushes were investigated concerning their height and composition as well as their photophysical properties. In a first experiment a structured surface bearing line patterns of ATRP-TAD was polymerised yielding well defined polymer brushes. These structured polymer brush substrates were used as references for convenient polymer brush height determination by atomic force microscopy (AFM). For all other experiments PAZA–PHEA copolymer brushes were grafted from surfaces which were fully functionalised with ATRP-TAD using flat non-patterned PDMS stamps. AFM showed a height of around 16 nm over a large area on the stripe patterns (Fig. 2a and ESI,† Fig. S2). To get a deeper insight into the consecutive steps of the surface modification, X-ray photoelectron spectroscopy (XPS) of the bare undecenyl SAM, the printed ATRP-initiator as well as grown PAZA–PHEA brushes was performed (Fig. 2b–d). The survey scan gives an overview of the whole scanned area (Fig. 2b). It is obvious that especially a dramatic change in the range between 0 and 230 eV is obtained when the polymer brushes are grown. This is easy to understand since these signals are due to silicon which is then shielded by the 16 nm polymer brushes. Taking a closer look at the nitrogen signal it is visible that after printing of the TAD initiator a characteristic signal at ca. 401 eV occurs which belongs to the electron poor nitrogens in the heterocycle and the amide bond. (Fig. 2c)15 After polymerisation the signal vanishes due to shielding by the brushes and a new signal at lower binding energy (400 eV) occurs. This signal belongs to the less electron poor azobenzenes. Also the carbon signals showed the successful growth of the brushes (Fig. 2d). The alkene terminated SAM shows a single C1s signal at 285 eV, whereas the C1s peak of ATRP-TAD functionalised SAMs shows a small shoulder for higher oxidized carbons as well. After polymerisation, three different species stemming from the aliphatic backbone (285 eV), higher oxidized carbons of the C–O bonds contained in HEA side arms (286 eV) and carboxylic carbons (289 eV) are visible.
With these surfaces in stock the supramolecular adhesion (“supramolecular velcro”) of homogeneously functionalized PAZA–PHEA brush substrates was investigated. After incubation of one surface with the commercially available β-CD polymer (100 mg mL−1 in H2O) for 10 min followed by washing with copious amounts of water a second surface was placed on top and the contacted substrates were dried for 1 h (area of contact ca. 1.4 cm × 1.3 cm). Since azobenzenes are known to bind to β-CD we expected a strong interaction between the surfaces since a multivalent binding between azobenzene brushes and the β-CD polymer should occur. From Fig. 3a it is seen that the surfaces stick to each other. They were placed on a holder (Fig. 3b) and we attached weights in a step by step fashion in order to check for the maximum load ability of the supramolecular adhesive. As can be seen in Fig. 3c–e we reattached weights after every rupture of the surfaces to see if weakening of the sticking ability of the surfaces occurs. The disrupted surfaces were washed and sonicated with ethanol to remove the CD polymer, dried, reincubated with the β-CD polymer and finally placed on top of each other again. Upon the third reattachment, the strength of our system decreased to 50% as exemplified by Fig. 3e. The exact reasons for the weakening of adhesion strength remain elusive. However, weakening of adhesion may be due to surface contaminations or structural changes and deformations of polymer brushes. The average gluing capacity of the surfaces was determined to be 700 ± 150 g cm−2. Control experiments without polymer brushes or without the β-CD polymer gave no significant interaction between the surfaces. The strength of the glue is related to the contact area and is increased to a value of 1.9 kg at a contact area of 2.24 cm2 (see the ESI,† Fig. S3).
Fig. 3 (a and b) Close up photographs and setup of the glued glass surfaces, (c) weight attached, (d) weight attached after first rupture and (e) weight attached after second rupture. |
Since it may be assumed that azobenzenes are involved in the binding process we expected a light-responsive behaviour of the brushes leading to the disruption of the surface adhesion under UV irradiation. Surprisingly, no significant effect of UV irradiation on the adhesion was observed. The lack of effect may have various reasons. On the one hand it is known that the photoirradiation of azobenzenes leads to a photostationary state, implying that even after extensive irradiation with UV light a significant amount of trans-azobenzene (ca. 20%) remains so that multivalent binding persists.24–26 Furthermore the local concentration of the azobenzenes is high and the degree of translational and rotational freedom in the brushes is severely hindered, which could lead to an even less effective photo-isomerisation.
To get a deeper insight into the photophysical properties of the PAZA–PHEA copolymer brushes UV/vis measurements were conducted. To this end the AZA-monomer was measured in the trans-state and in the cis-state which is obtained after irradiation with UV light (365 nm) (see the ESI,† Fig. S1). A pronounced shift in absorption as well as the occurrence of a characteristic peak at 440 nm is observed. After irradiation with visible light (465 nm) the trans-form is re-obtained. The same spectral changes were also observed for the free polymer which is grown in solution during SI-ATRP at the surfaces (Fig. 4a). Thus, the polymer shows a similar behaviour to the free monomer indicating that the copolymerisation of HEA and AZA does not affect the photoisomerisation. In a further experiment two surfaces coated with PAZA–PHEA brushes were incubated with the CD polymer and placed on top of each other, following the aforementioned procedure. UV/vis measurements reveal a characteristic absorption at 360 nm (π→π*) (Fig. 4b). However, when irradiated with UV light at 365 nm a decrease in absorption was observed surprisingly without a shift to lower wavelength. Furthermore no increase of the absorption at 440 nm (n→π*) was detectable. These findings lead to the assumption that a complete trans–cis isomerisation is not possible in the polymer brush and only a small amount of azobenzenes can undergo an isomerisation, explaining the stability of the glued surfaces under UV-light irradiation.
We present a supramolecular adhesive based on non-covalent host–guest interactions between azobenzenes in polymer brushes and a β-CD polymer. The brushes were investigated using AFM giving a height of ca. 16 nm and XPS verifying the presence of azobenzene in the brushes. Adhesion tests showed an average gluing capacity of around 700 g cm−2. Negative control experiments give no significant adhesion. As a consequence of high local concentration, multivalency, the unfavourable photostationary state and hindered rotational freedom, no light response of the supramolecular adhesion was observed. Nevertheless, this new type of polymer brush adhesive may find application in materials science as well as in surface related biomedical applications.
This work was funded by the Volkswagen Foundation.
Footnotes |
† Electronic supplementary information (ESI) available: Materials and methods, synthetic procedures, and additional spectra. See DOI: 10.1039/c5cc08968a |
‡ These authors contributed equally. |
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