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1 luids throughout the drying process using AC-electrowetting.
2 ulated upon an electrode array by the use of electrowetting.
3 ores and limiting solvent penetration during electrowetting.
4 lament, as is demonstrated in the context of electrowetting.
5 also means that it is an ideal substrate for electrowetting.
6 ion staging on the rate and reversibility of electrowetting.
7 used as references to engineer task-specific electrowetting agents (ILs) for future electrowetting-ba
8 he alternative use of ionic liquids (ILs) as electrowetting agents in EWOD-based applications or devi
9                The first cycle revealed slow electrowetting and cation-proton exchange.
10 ray ionization for use in mass spectrometry, electrowetting and lab-on-a-chip manipulations.
11                                   We observe electrowetting and merging of sulfur droplets under diff
12 conversion based on reverse electrosorption, electrowetting, and electrokinetic phenomena.
13                    Here, we demonstrate that electrowetting-assisted drying of solutions of common MA
14 cific electrowetting agents (ILs) for future electrowetting-based applications.
15 ere we show that liquid dielectrophoresis or electrowetting can produce wetting on normally non-wetti
16 ighly compatible with the next generation of electrowetting-coupled air samplers and thus shows stron
17  with exceptionally low power consumption by electrowetting/deelectrowetting at the metal surface.
18 and more homogeneous sample spots on special electrowetting-functionalized e-MALDI target plates.
19 ric field experienced by the lipid membrane, electrowetting has been used to determine the point of z
20 bination of nanofilament silicon and dynamic electrowetting is shown to provide routine detection lim
21                                   The use of electrowetting is shown to result in enhanced interactio
22                                           An electrowetting model describing the measured relationshi
23  concentration dependence of wetting with an electrowetting model.
24              We have developed an integrated electrowetting nanoinjector (INENI) to transfect single
25                          Here, we report the electrowetting of graphene-coated metal meshes for use a
26 ndence; and (iii) a systematic comparison of electrowetting of ILs using AC vs DC voltage fields.
27 estigation of AC frequency dependence on the electrowetting of ILs; (ii) obtaining theoretical relati
28               This paper presents a study of electrowetting of ionic liquids (ILs) under AC voltages,
29                        All tested ILs showed electrowetting of various magnitudes on an amorphous flo
30 s are performed in 64 nL droplets handled by electrowetting on dielectric (EWOD) actuation.
31 eveloped for biocollection take advantage of Electrowetting on Dielectric (EWOD) to recover material,
32  electrolytes are the dominant components in electrowetting on dielectric (EWOD)-based microfluidic d
33 hod combines previously demonstrated reverse electrowetting on dielectric (REWOD) phenomenon with the
34             The enhanced stability of ILs in electrowetting on dielectric at higher voltages was stud
35                                      Dynamic electrowetting on nanostructured silicon surfaces is dem
36          Localized heating of droplets on an electrowetting-on-dielectric (EWOD) chip has been implem
37 othymidine ((18)F-FLT) with high yield on an electrowetting-on-dielectric (EWOD) microfluidic radiosy
38                      The technique relies on electrowetting-on-dielectric (EWOD) to move droplets con
39 electric layer and a hydrophobic topcoat for electrowetting-on-dielectric (EWOD)(11-13); this increas
40 ion method for MALDI-MS, which relies on the electrowetting-on-dielectric (EWOD)-based technique for
41 l synthesis in organic solvents, operated by electrowetting-on-dielectric (EWOD).
42       Based on the high surface area reverse electrowetting-on-dielectric (REWOD) energy harvesting t
43              Within the last decade, reverse electrowetting-on-dielectric (REWOD)-based mechanical mo
44 ng example is the tunable liquid lens, where electrowetting or external pressure manipulates the shap
45                      Moreover, we employ the electrowetting phenomena to create a microlens based on
46 nergy conversion method based on the reverse electrowetting phenomenon.
47                                    Therefore electrowetting properties of 19 different ionic liquids,
48   In this regard, a fundamental study on the electrowetting properties of ILs is essential.
49                                          The electrowetting properties of ILs under AC voltages were
50      Finally, the physical properties and AC electrowetting properties of ILs were measured and tabul
51 re, functionality, and charge density on the electrowetting properties were studied.
52     The physical properties of ILs and their electrowetting properties were tabulated.
53 ge of intercalation, that a fully reversible electrowetting response can be attained.
54 t the positively charged graphene sheet, the electrowetting response is amplified by electrolyte conc
55 ificant effect of anion intercalation on the electrowetting response of graphitic surfaces in contact
56  is validated experimentally by studying the electrowetting response of highly oriented pyrolytic gra
57 r) systems that exhibit a fully reproducible electrowetting response with a near-zero voltage thresho
58                                              Electrowetting reversibility under AC voltage conditions
59 boelectric nanogeneration (TENG) and reverse electrowetting (REWOD), are reported in more detail.
60 se limitations, we have developed an optical electrowetting sequencing platform that uses step-wise n
61                                      Without electrowetting, silicon surfaces comprising dense fields
62 rophobic surfaces, 'fakir' droplets, tunable electrowetting, slip in the presence of surface heteroge
63 w approach is also the first of its kind for electrowetting-style displays by allowing non-aligned la
64 tal role in electron transport energetics by electrowetting the cofactors in the chain upon arrival o
65 ism, which is phenomenologically opposite to electrowetting, the liquid-substrate interaction is not
66                    Deviations from classical electrowetting theory were confirmed.
67 nofilaments can be dynamically controlled by electrowetting, thereby allowing aqueous buffer to penet
68 tivated fluidic valves that operate based on electrowetting through textiles.
69                          Techniques based on electrowetting, topographic micropatterns, and thermal/c
70 mbined theoretical and experimental study on electrowetting using carbon surfaces, introducing new co
71 tion towards the surface oxyhydroxide phase, electrowetting was found to cause a change in the interf
72  via manipulating surface wettability (i.e., electrowetting), which can render low-voltage but forfei
73 h electrical actuation is mainly achieved by electrowetting, with droplets attracted towards and spre