Drexel Nanotechnology InstituteMaterials and Nanotechnology ConsortiumAn NSF Integrated Graduate Education and Research Traineeship in Nanoscale Science & EngineeringResearch Experience for Teachers in the Area of NanotechnologyMaterials Science and EngineeringCollege of Engineering
NMG members working on CDC include: G. Yushin (group leader), J. Chmiola (electrochemical applications), R. K. Dash (H2, CH4, CO2, and Cl2 gas storage), Z. Cambaz (CDC transformations at the nano-scale), E. Hoffman (gas/liquid separation and purification), D. Vriehof (gas storage), S. Yachamaneni (bio-applications).

CDC is produced by extraction of metals from metal carbides. The method permits synthesis of almost all known carbon structures including amorphous and nanocrystalline graphitic carbon, graphite ribbons, carbon nanotubes, carbon onions, nanodiamond, and ordered graphite. In addition, CDC synthesis allows formation of highly porous carbon materials with good mechanical properties. Microstructure, pore size, pore shape, and surface termination of nanoporous CDC can be precisely controlled by changing the process parameters and the composition and structure of the initial carbide precursor. As such, the process allows optimization of nanoporous CDC for various applications.

Tuning the carbon structure and pore size with high accuracy by using different starting carbides and chlorination temperatures allows rational design of carbon materials with enhanced performance for the variety of applications.

Tuning the Pore Size in Ti3SiC2 - CDC with Sub-A Precision (Y. Gogotsi et al. Nature Materials, 2003 (2) 591-594)

High Resolution TEM images of various forms of carbon produced during chlorination of carbides: amorphous carbon (a), turbostratic graphite (b), fullerene-like carbon (c), nanodiamond (d), carbon onion (e), graphite ribbons (f), carbon nanotubes (g), barrel-like particles (h), and ordered graphite (i). (G. Yushin et al., in Handbook of Nanomaterials ed. by Y. Gogotsi, 2005, CRC Press, 237-280)

Selected Applications

I. Supercapacitors (Electrical Double Layer Capacitors - EDLC)

Supercapacitors are electrochemical energy storage devices akin to batteries. Occupying a region between batteries and dielectric capacitors on the Ragone plot, a plot describing the relationship between energy and power, they have been touted as a solution to the mismatch between the fast growth in power required by devices and the inability of batteries to efficiently discharge at high rates. This large capacity for high power discharge is directly related to the absence of charge transfer resistances that are a consequence of battery Faradaic reactions. This subsequently leads to low temperature dependence and theoretically unlimited cyclibility in supercapacitors. Improvements in the energy density of supercapacitors may help the currently made batteries work better and help usher electrical and fuel cell cars to the road.
Fast growing market of supercapacitors is expected to reach $ 1 billion by 2009. Applications of supercapacitors include: mobile electronics, starting conventional engines and acceleration boost for hybrids, power for electric vehicles, and backup power supplies to name a few.

CDC outperformed other carbon materials for EDLC applications offering the highest volumetric and gravimetric capacitance, and thus the highest energy density for the produced devices.

Performance of CDC-based electrodes: specific capacitance in standard organic electrolytes   Performance of CDC-based electrodes in standard organic electrolytes: equivalent series resistance of the assembled EDLC cell of standard (1 cm2) size.
II. Hydrogen Storage

The success of any future hydrogen economy depends, in large part, on our ability to develop inexpensive materials with sufficient hydrogen-storage capacity. Cryo-adsorption is considered a promising method of enhancing gravimetric and volumetric H2 storage for the future transportation needs.

We have demonstrated that nanoporous CDC with tunable pore size and pore volume up to 1 cc/g available for hydrogen storage possess gravimetric hydrogen storage density up to 3.6 wt% at 1 atm pressure and 77K.  Small pores (1 nm or below) are most efficient for hydrogen sorption while mesopores, detract from volumetric capacity and contribute little to gravimetric capacity. Large SSA and total pore volume increase hydrogen uptake for a given pore size.

Performance of CDC as H2 storage media @ 1 atm, 77K.
III. Methane Storage
The use of natural gas (methane) as an automotive fuel offers considerable advantages, including reduced emission, lower maintenance, and most importantly lower fuel cost relative to gasoline. Moreover, the world-wide reserves of natural gas considerably exceed the oil reserves and thus natural gas may offer a solution when oil wells run dry. However, in order to compete with gasoline now (and offer comparable driving distance for vehicles before re-fueling) advanced methane storage units with large volumetric and gravimetric methane storage capacity need to be developed. Storing natural gas in a compressed form has the disadvantage of the high cost of high pressure cylinders needed to provide the adequate methane storage capacity in a reasonably small volume. The use of inexpensive carbon adsorbent materials may allow storing considerable amounts of natural gas at relatively low pressures (<40 bar), making it more attractive for practical use.

Similar to hydrogen–storage applications, CDC can be optimized to adsorb large quantities of methane. We performed preliminary experiments on selected CDC samples and discovered that CDC outperforms commercially available activated carbons offering nearly 30 vol/vol methane storage at room temperature and atmospheric (≈1 bar) pressure.

Comparison of the highest CH4 storage capacities achieved in nanostructured carbons at 1 Bar. The experiments were performed at room temperature.
 
 

 

 

D.N.I | M. C. F. | I.G.E.R.T. | RET-Nnano | Materials Science & Engineering | College of Engineering