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[a] Bipolar electrochemistry is employed to demonstrate the formation of goldn anoparticle size gradients on planar surfaces. By controlling the electric field in aH AuCl 4 -containing electrolyte, gold was reduced onto 10 nm diameter particles immobilized on pre-modifiedt hiolatedb ipolar electrode (BPE) templates, resulting in larger particles towards the more cathodic direction. As the gold deposition wast he dominating cathodic reaction, the increased size of the nanoparticles also reflected the current distribution on the bipolar electrode. The size gradients werea lso combined with as econd gradient-forming technique to establish nanoparticle surfaces with orthogonal size and density gradients, resulting in aw ide range of combinations of small/large and few/many particles on as ingle bipolar electrode. Such surfaces are valuable in, for example, cellmateriali nteraction and combinatorial studies, where al arge number of conditions are probeds imultaneously.An umber of new and interesting applications of bipolar electrochemistry have recently appeared, involving small objects and surfacem odifications, [1][2][3][4][5][6][7] as well as sensors and detectors. [8][9][10][11][12] In such experiments,t he object or surface (the bipolar electrode, BPE) is placed in an electrolyte and exposed to an electric field established via two feedere lectrodes. Provided the BPE is conducting and the potential difference across it is sufficiently high, anodic and cathodic reactions can be induced with part of the cell current passingt hrough the BPE. With respect to larger objectsl ike mm-or cm-sizeds urfaces, formation of compositional gradients of materials, [13] such as semiconductors, [14] polymers, [15] metals, [16] and self-assembled monolayers and proteins [6,7] have been generated. In addition, bipolar gradients related to energy conversion have been presented, [17,18] and very recently,w eh ave also shown the possibility to swiftlys creen the corrosion properties of stainless steels functioning as BPEs. [19,20] An equally versatile method to modify surface chemical and morphological properties is the irreversible deposition of nanoparticles. Nanoparticle-coateds urfaces have been used to explore biological phenomenas uch as cell adhesion [21] and improvedb iosensing, [22] as well as energy-harvesting solar devices.[23] We have previously investigated how variation of particle deposition conditions tune the self-organization of gold nanoparticles, especially the distance between them, on dithiol-modified gold surfaces [24] in order to create regular [25] and anisotropic (gradient) [26] nanoparticle arrays for cell-screening purposes.H erein we extend this work by demonstrating the use of bipolar electrochemistry to gradually increase the size of surface immobilized gold nanoparticles, and also to form two orthogonal gradients in size and density on as ingle BPE. We also discuss how the gold deposition can be linked to the BPE current density distribution during the experiment.To first demonstrate the bipolar depo...
[a] Bipolar electrochemistry is employed to demonstrate the formation of goldn anoparticle size gradients on planar surfaces. By controlling the electric field in aH AuCl 4 -containing electrolyte, gold was reduced onto 10 nm diameter particles immobilized on pre-modifiedt hiolatedb ipolar electrode (BPE) templates, resulting in larger particles towards the more cathodic direction. As the gold deposition wast he dominating cathodic reaction, the increased size of the nanoparticles also reflected the current distribution on the bipolar electrode. The size gradients werea lso combined with as econd gradient-forming technique to establish nanoparticle surfaces with orthogonal size and density gradients, resulting in aw ide range of combinations of small/large and few/many particles on as ingle bipolar electrode. Such surfaces are valuable in, for example, cellmateriali nteraction and combinatorial studies, where al arge number of conditions are probeds imultaneously.An umber of new and interesting applications of bipolar electrochemistry have recently appeared, involving small objects and surfacem odifications, [1][2][3][4][5][6][7] as well as sensors and detectors. [8][9][10][11][12] In such experiments,t he object or surface (the bipolar electrode, BPE) is placed in an electrolyte and exposed to an electric field established via two feedere lectrodes. Provided the BPE is conducting and the potential difference across it is sufficiently high, anodic and cathodic reactions can be induced with part of the cell current passingt hrough the BPE. With respect to larger objectsl ike mm-or cm-sizeds urfaces, formation of compositional gradients of materials, [13] such as semiconductors, [14] polymers, [15] metals, [16] and self-assembled monolayers and proteins [6,7] have been generated. In addition, bipolar gradients related to energy conversion have been presented, [17,18] and very recently,w eh ave also shown the possibility to swiftlys creen the corrosion properties of stainless steels functioning as BPEs. [19,20] An equally versatile method to modify surface chemical and morphological properties is the irreversible deposition of nanoparticles. Nanoparticle-coateds urfaces have been used to explore biological phenomenas uch as cell adhesion [21] and improvedb iosensing, [22] as well as energy-harvesting solar devices.[23] We have previously investigated how variation of particle deposition conditions tune the self-organization of gold nanoparticles, especially the distance between them, on dithiol-modified gold surfaces [24] in order to create regular [25] and anisotropic (gradient) [26] nanoparticle arrays for cell-screening purposes.H erein we extend this work by demonstrating the use of bipolar electrochemistry to gradually increase the size of surface immobilized gold nanoparticles, and also to form two orthogonal gradients in size and density on as ingle BPE. We also discuss how the gold deposition can be linked to the BPE current density distribution during the experiment.To first demonstrate the bipolar depo...
In this study, the use of electrochemistry in cell biology is extended by showing that electrochemically generated microscale pH gradients can be used to gain new insights into the regulation of cytosolic pH of normal and cancer cells. The developed procedure involves positioning a carbon fiber microelectrode into the extracellular space of adherently growing cells and setting its potential to values suitable for electrooxidation or electroreduction of water. While the electrooxidation of water decreases the pH of the solution surrounding the microelectrode (because it produces hydronium ions), the electroreduction of water increases the pH of the same solution (because it produces hydroxide ions). Fluorescence microscopy is then used to observe the impact of the electrochemically generated microscale pH gradient on the cytosolic pH of cells loaded with a fluorescent pH sensor. The obtained results indicate that electrochemically induced acid stress affects the cytosolic pH of normal cells significantly faster than that of cancer cells while electrochemically induced alkaline stress appears to have very limited impact on the cytosolic pH of both cell types. In comparison to classic experiments concerning the regulation of cytosolic pH using perfusion chambers, the developed, electrochemistry-based, approach has the advantages of a better spatial and temporal resolution and elimination of the flow-induced shear stress.
A new simple and versatile method for the preparation of surface‐wetting gradients is proposed. It is based on the combination of electrode surface structuration introduced by a sacrificial template approach and the formation of a tunable molecular gradient by bipolar electrochemistry. The gradient involves the formation of a self‐assembled monolayer on a gold surface by selecting an appropriate thiol molecule and subsequent reductive desorption by means of bipolar electrochemistry. Under these conditions, completion of the reductive desorption process evolves along the bipolar surface with a maximum strength localized at the cathodic edge and a decreasing driving force towards the middle of the surface. The remaining quantity of surface‐immobilized thiol, therefore, varies as a function of the axial position, resulting in the formation of a molecular gradient. The surface of the bipolar electrode is characterized at each step of the modification by recording heterogeneous electron transfer. Also, the evolution of static contact angles measured with a water droplet deposited on the surface directly reveals the presence of the wetting gradient, which can be modulated by changing the properties of the thiol. This is exemplified with a long, hydrophobic alkane–thiol and a short, hydrophilic mercaptan.
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