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. Author manuscript; available in PMC: 2019 Jun 11.
Published in final edited form as: Langmuir. 2018 Jul 18;34(49):14993–14999. doi: 10.1021/acs.langmuir.8b01004

Figure 2.

Figure 2.

(Left) The folding free energy of a stem-loop site-specifically attached to a C6OH SAM-on-gold surface is more sensitive to ionic strength than that of the same stem-loop in solution. This is because attachment to this negatively charged (at the potential applied in our experiments) surface destabilizes the folded state through electrostatic repulsion.5 (Right) This scheme serves to illustrate the dimensions of the stem loop relative to the potential field that forms above the surface when a potential is applied. Specifically, shown are the electric fields produced if the surface is at a potential of 50 (red) or 150 mV (blue) (versus the potential of zero charge; pzc) at ionic strengths of 25 (dashed lines) or 250 mM (solid lines). At low surface charge and/or high ionic strength the electric field experienced by the stem-loop is minimal. The left-hand panel was adapted from ref 5.