Technical publication
Back to publications
Reactors & equipment
Cavitation Driven Exfoliation of Graphene and Two Dimensional Materials
okozyuk.com
Published
Read complete publication for whole-document Find and printing. Browser Find and native printing on this reader include only loaded content.
3 Structure, Interlayer Attraction, and Exfoliation Thermodynamics
3.1 Layered Crystal Geometry
Graphite consists of graphene layers bonded strongly within each basal plane and held together much more weakly between planes. The large difference between in plane bonding and interlayer attraction permits sliding and peeling. Similar structural anisotropy occurs in many layered solids, although the interlayer interaction may include van der Waals attraction, electrostatic contributions, ionic character, surface oxidation, adsorbed water, or intercalated species. Consequently, identical reactor settings can produce substantially different outcomes for graphite, boron nitride, transition metal dichalcogenides, black phosphorus, and layered oxides.
The ideal minimum work required to create two new surfaces can be represented by a surface energy balance. For flake area A and effective cleavage energy Gc, the reversible work is:
Wmin is the ideal minimum work, Gc is the effective cleavage energy per unit area, and A is the newly separated area. Actual process energy is substantially greater because only a fraction of the supplied energy is transmitted to an advancing interlayer crack.
The engineering objective is not simply to exceed the ideal cleavage work. Stress must be transmitted to a defect, edge, fold, gallery, or liquid wedge in a direction that advances separation. Energy dissipated as uniform heating, pumping loss outside the active region, or random turbulence remote from particles does not directly create product. Nominal motor power is therefore an inadequate basis for comparison unless calorimetry, hydraulic power, active volume, residence time, and recovered product mass are also reported.
3.2 Wetting and Solvent Matching
Freshly separated surfaces tend to restack unless the liquid and any stabilizer reduce the free energy of dispersion. Solvent screening can use surface tension, solubility parameters, polarity, hydrogen bonding capability, viscosity, boiling point, toxicity, cost, and recoverability. Mixtures can be more effective than a single liquid because they allow surface energy and viscosity to be adjusted independently. A hydrodynamic study using isopropyl alcohol and water found an optimum near 40 volume percent isopropyl alcohol, where surface tension, Hansen distance, viscosity, and dispersion stability provided a favorable combination [15]. To quantify thermodynamic affinity and compatibility between a solid solute or nanoparticle () and the liquid solvent medium (), the Hansen solubility parameter distance () is used Equation (3.2):
Ra is the Hansen solubility parameter distance between solid s and liquid l. δD, δP, and δH are dispersive, polar, and hydrogen bonding components. While a smaller value generally indicates higher thermodynamic compatibility and wetting propensity between the liquid and the solid surface, solubility parameters alone are insufficient for dynamic systems. Effective process optimization requires simultaneously accounting for hydrodynamic constraints, such as cavitation bubble dynamics, liquid compressibility, and medium viscosity.
Surfactants and polymers can adsorb on newly exposed surfaces and provide electrostatic, steric, or combined stabilization. Sodium cholate, sodium deoxycholate, carboxymethyl cellulose, polyvinylpyrrolidone, proteins, and other dispersants have been used. Stabilizer concentration should be optimized rather than maximized. Insufficient stabilizer permits restacking, whereas excessive stabilizer increases viscosity, foaming, purification burden, conductivity loss, and cost. Cavitation can also degrade the stabilizer, so stability must be measured after processing rather than inferred from the initial formulation [10-14,20,21].
Table 3.1. Selection factors for the liquid medium and stabilizer.
| Factor | Why it matters | Preferred evidence | Common failure mode |
|---|---|---|---|
| Surface compatibility | Controls wetting, dispersion free energy, and restacking tendency. | Measured concentration after standardized separation; long term sedimentation; Hansen or surface energy screening. | A liquid that wets graphite initially but cannot stabilize the thinner product. |
| Viscosity | Affects shear stress, pressure loss, cavitation inception, heat generation, and pumping. | Viscosity at process temperature and solids loading. | A formulation that cavitates well when dilute but becomes noncavitating at production concentration. |
| Vapor pressure | Changes bubble formation and collapse intensity. | Vapor pressure and cavitation number at actual temperature. | Excessive vapor cushioning or insufficient cavity formation. |
| Boiling point and recovery | Determines drying duty, solvent loss, and residual solvent. | Mass balance around recovery equipment and residual solvent analysis. | High energy drying or unsafe vapor accumulation. |
| Stabilizer adsorption | Prevents restacking and controls rheology. | Zeta potential, rheology, TGA, surface analysis, redispersion test. | Excess residue lowers electrical or thermal performance. |
| Corrosion and compatibility | Protects pumps, seals, valves, nozzles, and analytical equipment. | Materials compatibility test and extractables analysis. | Metal contamination or seal swelling. |
| Safety and environment | Determines containment, ventilation, fire protection, and waste treatment. | SDS, exposure assessment, flash point, emissions and waste inventory. | A laboratory solvent that is unacceptable at plant scale. |