4.7 Article

General Capacitance Upper Limit and Its Manifestation for Aqueous Graphene Interfaces

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MDPI
DOI: 10.3390/ijms241310861

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graphene; molecules; interface; nanostructures; capacitance; electric permittivity; capacitance limit; water; sensor; impedance spectroscopy

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The correct formula for double-layer capacitance (C-dl) in graphene interfaces with liquid is controversial. We proposed a model that considers the capacitance of a charge accumulation layer (C-ca) and a capacitance-limiting edge region (C-e) with negligible electric susceptibility and conductivity. These capacitances are connected in series, and C-dl can be obtained from 1/C-dl = 1/C-ca + 1/C-e. Experimental results on the graphene/water interface capacitance imply that the distance from charge carriers in graphene to molecular charges at the interface is around 0.05-0.1 nm. The generalized model predicts a capacitance upper limit of approximately 18 μF/cm2.
Double-layer capacitance (C-dl) is essential for chemical and biological sensors and capacitor applications. The correct formula for C-dl is a controversial subject for practically useful graphene interfaces with water, aqueous solutions, and other liquids. We have developed a model of C-dl, considering the capacitance of a charge accumulation layer (C-ca) and capacitance (C-e) of a capacitance-limiting edge region with negligible electric susceptibility and conductivity between this layer and the capacitor electrode. These capacitances are connected in series, and C-dl can be obtained from 1/C-dl = 1/C-ca + 1/C-e. In the case of aqueous graphene interfaces, this model predicts that C-dl is significantly affected by C-e. We have studied the graphene/water interface capacitance by low-frequency impedance spectroscopy. Comparison of the model predictions with the experimental results implies that the distance from charge carriers in graphene to the nearest molecular charges at the interface can be similar to(0.05-0.1)nm and is about a typical length of the carbon-hydrogen bond. Generalization of this model, assuming that such an edge region between a conducting electrode and a charge accumulating region is intrinsic for a broad range of non-faradaic capacitors and cannot be thinner than an atomic size of similar to 0.05 nm, predicts a general capacitance upper limit of similar to 18 & mu;F/cm(2).

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