Concepedia

TLDR

The phenomenon of contact electrification has been known for millennia, yet the identity of its charge carriers and the mechanisms of their transfer remain debated. The study investigates CE and triboelectric charging in a metal–dielectric pair under varying thermal conditions, focusing on how temperature differences between contacting materials influence charge transfer. Using atomic force microscopy and Kelvin probe force microscopy, the authors model electron transfer between solids at different temperatures with a thermionic‑emission band‑structure framework. The results demonstrate that nanoscale CE follows a modified thermionic‑emission model, with hotter solids acquiring positive charges and cooler solids negative charges, and that even identical materials can undergo CE due to local temperature differences arising from nanoscale rubbing.

Abstract

The phenomenon of contact electrification (CE) has been known for thousands of years, but the nature of the charge carriers and their transfer mechanisms are still under debate. Here, the CE and triboelectric charging process are studied for a metal-dielectric case at different thermal conditions by using atomic force microscopy and Kelvin probe force microscopy. The charge transfer process at the nanoscale is found to follow the modified thermionic-emission model. In particular, the focus here is on the effect of a temperature difference between two contacting materials on the CE. It is revealed that hotter solids tend to receive positive triboelectric charges, while cooler solids tend to be negatively charged, which suggests that the temperature-difference-induced charge transfer can be attributed to the thermionic-emission effect, in which the electrons are thermally excited and transfer from a hotter surface to a cooler one. Further, a thermionic-emission band-structure model is proposed to describe the electron transfer between two solids at different temperatures. The findings also suggest that CE can occur between two identical materials owing to the existence of a local temperature difference arising from the nanoscale rubbing of surfaces with different curvatures/roughness.

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