2017
DOI: 10.1103/physrevmaterials.1.035605
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Dependence of triboelectric charging behavior on material microstructure

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Cited by 39 publications
(37 citation statements)
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“…Figure 6 shows the distribution of the X and Y components of the induced electric field, where the Z component distribution is similar to the X one. The presence of the electric field will induce charge transfer in the conductive electrodes as a direct result to contact electrification [9,25]. Also, The field distributions are shown to be consistent with the potential distribution in the sense that the field will exert a force on the charges to move from higher to lower potential zones.…”
Section: Electric Characteristicsmentioning
confidence: 69%
“…Figure 6 shows the distribution of the X and Y components of the induced electric field, where the Z component distribution is similar to the X one. The presence of the electric field will induce charge transfer in the conductive electrodes as a direct result to contact electrification [9,25]. Also, The field distributions are shown to be consistent with the potential distribution in the sense that the field will exert a force on the charges to move from higher to lower potential zones.…”
Section: Electric Characteristicsmentioning
confidence: 69%
“…[7][8][9] The focus in this paper is on inorganic dielectric solids; however, the effect may also play a role in the electrification of organic polymers. In polymers, the effect may be more likely to occur in parallel with other mechanisms, e.g., charge transfer between charge patches on the surfaces, [10][11][12] from surface functional groups with acid/base character, 48 from charge transfer induced by strain, 49 or by material transfer. Finally, the results provide support for charge transfer by electrons rather than ions during many instances of triboelectric charging.…”
Section: Discussionmentioning
confidence: 99%
“…(This helps explain why even the same polymers can be charged by tribo-contacts; it is because even identical polymers will have different material compositions at each depth, which account for the same material charge transfer [29].) Moreover, material transfer is possible if dynamical changes in the surfaces and tribological environments exist, because materials will tend toward a lower potential energy state and these dynamical changes can lead to the potential energy minimum shifts [53,54]. For example, one dynamical change (in quasistatic form) can be strain and its corresponding potential energy form (near the potential energy local maximum, i.e., the local energy barrier at interface) is…”
Section: (Nano-) Materialsmentioning
confidence: 99%
“…Different explanations and theories are provided to understand the electrification, among which pattern and geometry are believed to play a vital role. Wang et al [53] proved that the differences in the microstructure of chemically identical materials trigger distinct tribo-charging behavior. In this sense, as a strained surface will exhibit different microstructures due to voids and seams (which can be scaled from nano-to micrometers) and the different microstructures will trigger different surface potential energy minimum according to catastrophe theories [53,54], as shown in Fig.…”
Section: Microstructure/pattern/geometrymentioning
confidence: 99%
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