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Patterned and switchable surfaces for biomaterial applications

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Andrew Hook – <strong>Patterned</strong> <strong>and</strong> <strong>switchable</strong> <strong>surfaces</strong> <strong>for</strong> <strong>biomaterial</strong> <strong>applications</strong>due to post-deposition alterations. Thermodynamic studies were conducted with twodifferent batches of Si-ALAPP samples.Quartz crystal microbalance (QCM) measurements were taken using anElectrochemical Nanobalance EQCN-701 (Elchema). 9 V Quartz crystals(International Crystal Manufacturing Company) with gold electrodes were used <strong>for</strong>all measurements. The frequency of the crystal was measured <strong>and</strong> processed usingVoltscan <strong>and</strong> Master Windows software. Frequency changes were converted to masschanges using the Sauerbrey equation, shown as equation 3.2, where f is the changein frequency, m is the change in mass, a is a constant related to the crystal used <strong>and</strong>A is the area.m f a(3.2)AAll measurements were conducted in a Faraday cage under N 2 at roomtemperature. For DNA adsorption studies, one side of the quartz crystal was coatedwith an ALAPP film according to the procedure described previously. The coatedside was incubated in a 0.01 M phosphate buffer, pH 7.4, 0.5 M NaCl whilst theuncoated side was exposed to N 2 throughout. After 24 hr incubation, to allow <strong>for</strong>swelling of the polymer film <strong>and</strong> any post-deposition rearrangements <strong>and</strong> afterensuring the crystal had stabilised, a 300 g/ml plasmid solution was added to makea final DNA concentration of 200 ng/ml <strong>and</strong> the change in mass was measured.3.2.5. Data analysisThe adsorption of plasmid DNA to ALAPP <strong>and</strong> PEG films was modelled usingthe Langmuir model. The change in surface concentration of a species was related tothe bulk concentration by equation 3.3, where s corresponds to the surface3-105

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