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Graphite: structure, bonding and physical properties

Bonding, structure, and the properties of matterStructure and bonding of carbon

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What property of graphite makes it useful in electrodes?

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Electrical conductivity due to delocalised electrons.

Key concepts

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Atomic arrangement and layer structure

Graphite has a two-dimensional arrangement of carbon atoms in hexagonal rings that form flat sheets. Each sheet is called a layer and layers stack in parallel to create the bulk material. The layers show regular repeating hexagons with carbon atoms at the vertices, producing a planar lattice with a defined spacing between layers. Layer stacking produces anisotropy in physical properties: strong bonding exists within sheets, while weak attractions between sheets allow different behaviour parallel and perpendicular to the layers. The layer spacing limits interlayer interactions and determines how easily layers slide.

Bonding within layers (sp2 hybridisation)

Each carbon atom in a graphite layer forms three sigma (σ) covalent bonds to neighbouring carbons using sp2 hybrid orbitals. The three sigma bonds lie in the plane of the layer and create strong, rigid connections between atoms. The planar geometry enforces 120° bond angles and a hexagonal ring structure. One unhybridised p orbital remains on each carbon atom and overlaps with p orbitals on adjacent carbons to form pi (π) molecular orbitals. The sigma framework gives graphite high thermal stability and a high melting point because large energy is required to break the in-plane covalent bonds.

Delocalised electrons and electrical conductivity

The unhybridised p orbitals combine across each layer to form a system of delocalised electrons (pi electron cloud) that extends over the whole sheet. These delocalised electrons move freely within the plane of the layers and carry electrical charge. Delocalisation causes electrical conductivity parallel to the layers because electrons can flow along the pi system. Conductivity perpendicular to the layers is low because electrons cannot easily move between separate sheets due to weak interlayer forces.

Interlayer forces and lubricating behaviour

Adjacent graphite layers interact through weak van der Waals forces or London dispersion forces. These forces are much weaker than the covalent bonds within layers and allow layers to slide past each other under applied stress. Layer sliding produces a low-friction surface and explains graphite's use as a dry lubricant and its characteristic softness. The ease of shear depends on the strength of the weak interlayer attractions and the presence of impurities or adsorbed species between layers.

Macroscopic properties derived from structure

Strong covalent bonding within layers causes graphite to have a very high melting point and thermal stability, because breaking many strong bonds requires large energy input. The delocalised electrons produce electrical conductivity and thermal conduction along layers. The combination of strong in-plane bonds and weak interlayer forces produces material properties that are direction-dependent: high strength and conductivity within layers, softness and lubricity perpendicular to applied shear, and chemical inertness that leads to insolubility in common solvents.

Key notes

Important points to keep in mind

Each carbon in graphite forms three strong in-plane covalent bonds (sp2).

One electron per carbon becomes delocalised across the layer and carries charge.

Weak van der Waals forces between layers allow easy shear and lubrication.

Electrical conductivity in graphite occurs parallel to layers, not perpendicular.

High melting point results from strong covalent bonds within layers.

Graphite is insoluble due to the extended covalent network in each layer.

Properties are anisotropic: different behaviour along and across layers.

Intercalation or impurities change interlayer spacing and electrical properties.

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