| Version | Summary | Created by | Modification | Content Size | Created at | Operation |
|---|---|---|---|---|---|---|
| 1 | Jack Zhong | -- | 203 | 2026-09-21 11:29:57 | | | |
| 2 | Catherine Yang | -11 word(s) | 192 | 2026-09-22 02:48:11 | | |
Hard carbon is a non-graphitizable carbon material built from randomly oriented graphene-like nanodomains, curved or fullerene-like fragments, and internal closed pores, and it cannot be converted into graphite even after treatment above about 2500 °C [1]. It is obtained mainly by pyrolysis of biomass, sugars, resins, and polymers at 1000–1600 °C, and its structure is usually described by the interlayer spacing (0.36–0.40 nm, against 0.335 nm for graphite) together with the volume fraction of closed micropores [2]. For sodium-ion batteries the material serves as the negative electrode, where reversible capacities of roughly 250–350 mAh/g are commonly reported [3]. Two storage processes are distinguished in the galvanostatic curve: adsorption of sodium at defect sites and pore surfaces, which gives the sloping region, and insertion or pore filling, which is associated with the low-potential plateau near 0.1 V [4]. Because plateau capacity depends on closed-pore volume, the balance between the sloping and plateau regions is governed by precursor selection, pyrolysis temperature, and heteroatom doping rather than by any single synthesis parameter [5]. Initial Coulombic efficiency, typically 70–90%, and the contribution of sodium metal plating to the measured capacity remain debated [3][4].