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Many active drug compounds share the same problem: low solubility and rapid elimination from the body before they can deliver a therapeutic effect. In one study, syringic acid encapsulated in MIL-100(Fe) reached a drug loading of 64.42% in just 12 hours, and when tested in a rat model, its bioavailability increased almost 11-fold compared to plain oral administration. That result was made possible by MIL-100(Fe)'s giant mesoporous cages, measuring 25 and 29 angstroms across,

Most MOFs remain stuck at the laboratory scale, difficult to produce beyond a few grams at a time. Al-Fum is the exception. Known commercially as Basolite A520, it's one of the first MOFs BASF successfully manufactured at ton scale through a fully solvent-free, water-based synthesis, reaching a space-time yield of 3,600 kilograms per cubic meter per day, a breakthrough that even won the Pierre Potier Prize for sustainable chemistry innovation. Al-Fum (Aluminum Fumarate) is an

Most CO₂-capturing MOFs share the same weakness: their performance collapses the moment water vapor is present, and real-world industrial flue gas is almost always humid. MIL-96(Al) does the opposite. Research testing this material at relative humidity levels up to 40% found that at a moderate 10% RH, its affinity for CO₂ actually increases, because water and CO₂ fill different pore cavities within its structure rather than competing for the same space. MIL-96(Al) is an alumi

In Death Valley National Park, one of the hottest and driest places on Earth, a device loaded with MOF-303 harvested 210 grams of water per kilogram of MOF each day, powered by nothing but sunlight, with no electricity or external cooling. In the Mojave Desert, where relative humidity can drop as low as 10%, a different version of the device recorded up to 1.3 liters of water per kilogram of MOF per day. MOF-303 (Al) is the material behind that achievement: an aluminum-based

Nickel has one advantage that copper lacks in a comparable MOF: it switches easily between the Ni²⁺ and Ni³⁺ oxidation states, storing charge through a strong pseudocapacitive mechanism. A pristine Ni-BTC electrode has been reported to reach a specific capacitance of 234 F/g at a current density of 0.43 A/g, and when combined with Ti₃C₂Tₓ MXene into a composite nanosheet, that performance jumps to 867.3 F/g at 1 A/g. Ni-BTC (Nickel 1,3,5-Benzenetricarboxylate) is the MOF behi

Most MOFs keep their metal ions tucked fully inside the framework, fully coordinated and hard for other molecules to reach. Cu-BTC, does the opposite: once the water molecules bound to its copper dimers are removed through activation, what's left are open metal sites that can interact directly with gas molecules or act as catalytic centers. That combination, together with a surface area reported in the literature at up to nearly 1,900–1,944 m²/g, makes Cu-BTC one of the most

Separating propylene from propane by conventional distillation is one of the most energy-intensive processes in the petrochemical industry, since the two molecules' boiling points differ by only a few degrees Celsius. ZIF-8 membranes offer a shortcut: thanks to a pore aperture of only about 4 angstroms that can flex open and closed with the motion of its ligand, polycrystalline ZIF-8 membranes have been reported to achieve a propylene/propane separation factor of around 300,

One gram of ZIF-67 carries an internal surface area of up to 1,017 m²/g, equivalent to more than twice the area of a basketball court, packed into powder grains only about 1.3 micrometers across. That surface area is exactly why Zeolitic Imidazolate Framework-67 (ZIF-67) is so sought after for applications that need maximum contact area in the smallest possible volume, from electrocatalysis to gas storage to energy storage. ZIF-67 belongs to the metal-organic framework (MOF)

Vanadium MXene produced by etching V₂AlC has been shown to reach a gravimetric capacitance of 181.1 F/g and a volumetric capacitance of 317.8 F/cm³ as a supercapacitor electrode, retaining 89.1% of its capacitance after 5,000 charge-discharge cycles. That performance is a big reason vanadium-based MXene is getting more attention as an alternative to the more commonly used titanium MXene. Vanadium Aluminum Carbide (V₂AlC) is the raw material behind that performance, a layered

Ti₃AlC₂ has a property most ceramics simply don't: it can heal its own cracks. Heat it in air to around 1,100°C and the aluminum in its structure reacts with oxygen to form a protective α-Al₂O₃ layer that fills the crack from within. That behavior exists because Ti₃AlC₂ belongs to the MAX phase family, a class of layered materials that combines metallic and ceramic properties in a single structure. It's soft enough to machine at room temperature, yet its Young's modulus still

Thermal management in electronics runs into a stubborn contradiction: a filler that conducts heat well enough to pull it away from a hot component usually conducts electricity too which is the last thing you want touching a circuit board or a battery cell. Metals and most carbon fillers force that trade-off. Hexagonal Boron Nitride (h-BN) is one of the few materials that doesn't: it moves heat efficiently while remaining electrically insulating, which is exactly why it's earn

Most 2D conductive materials force a trade-off: graphene derivatives are easy to source but their surface chemistry is hard to tune precisely, while MXenes offer a tunable surface and metallic conductivity but are notoriously sensitive to how they're made. A poorly delaminated batch still carries residual TiC or unreacted MAX phase, which quietly caps the conductivity and electrochemical performance a battery, sensor, or EMI-shielding application actually needs. Titanium Carb

Graphene and its derivatives are among the most important carbon nanomaterials in modern nanotechnology and material science. Thanks to their unique atomic structure, graphene-based materials can be engineered into multiple functional forms for energy systems, conductive materials, coatings, and advanced composites. Graphene-based nanomaterials are widely used in energy storage systems, conductive materials, polymer composites, coatings, and other advanced nanotechnology appl

A thin GO dispersion is great for thin coatings or membranes, but the moment an application needs a thick layer that holds its shape screen printing, doctor-blade coating, extrusion, direct ink writing a runny solution becomes the problem: it drips, spreads past the pattern, or lays down too thin a film per pass. GO Paste is built for exactly that case: Graphene Oxide at high solids content with a shear-thinning, viscous-but-flowable rheology, formulated to be printed, extrud

Powder-form Graphene Oxide comes with a step that's easy to underestimate, before it can actually be used, it has to be dispersed sonicated, stirred, sometimes re-filtered so the GO sheets are properly separated instead of clumping the moment they hit a solvent. Skip that step or do it inconsistently, and results can vary from batch to batch even when the rest of the formulation is identical. GO Dispersion removes that step from your workflow entirely: Graphene Oxide that's a

Graphene's headline stat isn't its conductivity it's strength. A defect free single layer has a tensile strength around 130 GPa and a Young's modulus near 1 TPa, making it one of the strongest materials ever measured. Graphene Nanoplatelets (GNP) package that strength into a practical, stackable multi-layer form: small platelets of few to many layer graphene, produced by exfoliating graphite rather than oxidizing and reducing it. That production route makes GNP the material o

Not every application needs graphene's oxygen chemistry. Sometimes what a formulation actually needs is raw electrical performance: a conductive filler that drops sheet resistance, builds a percolation network at low loading, and doesn't need to be reduced, dispersed in water, or functionalized first. That's the gap Graphene Conductive Grade fills a few-layer graphene material processed specifically to maximize conductivity, rather than dispersibility or reactive chemistry, f

Plain rGO has a well-known problem, the same reduction process that restores its conductivity also strips away most of the oxygen groups that kept it dispersible, so it tends to aggregate and clump once it's back in water or a polymer matrix. Carboxylated Reduced Graphene Oxide (rGO-COOH) is the fix. By retaining or deliberately re-introducing carboxyl (−COOH) groups on the sheet surface, rGO-COOH keeps most of rGO's electrical conductivity while staying dispersible and chemi

Reduced Graphene Oxide, or rGO, has become one of the most sought-after nanomaterials in electronics, energy storage, and sensor research and for good reason. Unlike its precursor, Graphene Oxide (GO), rGO is prized specifically for what it gets back after processing: electrical conductivity. That single property is what unlocks its use in batteries, supercapacitors, flexible circuits, and shielding materials, where GO's insulating, oxygen-rich structure simply won't do the j

For over a decade, graphene and its derivatives have been dubbed the "wonder materials" of the 21st century. With exceptional electrical conductivity, mechanical strength, and thermal properties, the potential seemed boundless. Yet global industries have consistently faced a massive bottleneck: scalability and cost. High-quality graphene materials were notoriously difficult to produce in bulk, keeping them locked behind prohibitive import fees. Today, that narrative is changi