Nanomaterials Engineering for Hydrogen Storage
January 2004 - December 2007 (Completed)
Investigators
Kyeongjae (KJ) Cho, Mechanical Engineering;
Bruce Clemens, Materials Science and Engineering;
Hongjie Dai, Chemistry;
Anders Nilsson, Stanford Synchrotron Radiation Laboratory, Stanford University
Objective
The objective of this project is to develop optimized nanocomposite materials for high-density H2
reversible storage applications. Specifically, carbon nanotube-catalyst
nanoparticle composite materials with well-controlled nanotube size
will be developed, that are optimized to satisfy the target fundamental
characteristics for hydrogen storage. A systematic design and
fabrication process will be followed that will permit not only
controlled growth of carbon nanotubes but also incorporation of
nanoparticles to decorate the nanotubes to catalyze H2 adsorption and
desorption processes.
Background
Nanomaterials have diverse tunable physical properties as a function
of their size and shape due to strong quantum confinement effects and
large surface/volume ratios. A single wall carbon nanotube (SWCNT) has
the same structure as a roll of a single graphene sheet and has
nanometer sized diameters ranging from 4 to over 100 Å. Due to their
large surface areas with relatively small mass, SWCNTs have been
considered as potential materials for high capacity hydrogen storage.
Theoretically, they can store hydrogen up to 7.7 wt%, as every carbon
atom in SWCNTs chemisorbs one hydrogen atom. In addition, the
subsequent physisorption of hydrogen on the surfaces of hydrogenated
SWCNTs can increase the capacity of hydrogen storage even further. In
spite of the strong potential of SWCNTs, current experimental findings
are not very promising mainly due to the lack of control in preparing
SWCNTs as a hydrogen storage medium. It has recently been shown that
the H-CNT interaction energy is a very sensitive function of the
nanotube size, and a sample of a wide range of CNT sizes would have
only a small fraction of the CNT surface suitable for hydrogen storage.
There is currently much skepticism on carbon nanotube hydrogen storage
due to early mistakes in experimental publications and therefore a
rational basis for high capacity hydrogen storage materials is being
developed through the systematic nano-materials research undertaken in
this effort.
Figure 1: Flow diagram of the project
Approach
The framework of nanomaterial design, fabrication and
characterization illustrated in Figure 1 will be used to optimize the
catalyzed nanotube for hydrogen storage. A systematic search process in
material parameter space (particle composition and size) will be
applied. The materials design will be implemented by fabrication and
characterization of the nanocomposite materials for their reversible
hydrogen storage capacity. The four main thrusts of this approach are
discussed below:
- Computation:
Intelligent Computer Aided Materials Design (ICAMD) principles and
simulation tools will be applied to the design of the desired
nanocomposite materials based on the merging of evolutionary computing
techniques such as the genetic algorithm (GA) approach with quantum
ab-initio and tight-binding simulation methods for applications
pathways.The simulation process involves: (a) design and construction
of an appropriate "fitness function," based on final application
specifications, against which the overall design and application
pathway is continually optimized; (b) generation of a population of
structures and their associated physical and chemical characteristics;
(c) GA based evolution of the population until a best fit with the
fitness-function is achieved within a prescribed error bar; and (d)
comparison and experimental feasibility testing of the best fit design
by additional quantum simulation and comparison with experimental data.
- Control of Chemical Reactivity:
One of the most critical requirements for hydrogen storage materials
besides storage capacity is reversibility. The storage material should
be able to both absorb and release hydrogen easily. The reversibility
can be controlled by the hydrogenation energy of a SWCNT, which is
enhanced as the curvature of the SWCNT increases. Different atomic
scale catalysts will be designed which can remove most of the energy
barrier of around 2 eV between H2 gas and the chemisorbed H atoms, and
SWCNTs with radii equal to or smaller than a (12, 0) SWCNT will be
grown.
- Fabrication: Three
conceptually different approaches will be applied to fabricate
nanoclusters with the right size and spatial distributions that can
serve as catalytic centers for growth of SWCNTs. These include (a)
catalytic nanocluster formation using an inert gas buffer plus Coulomb
charging (BLC) technique as depicted in Figure 2. First principles
based simulation approaches will be used to map out the precise growth
conditions for size selection and control for a variety of
nanocluster-substrate combinations and the process may be modified to
generate a hybrid nanocluster-nanotube system with both size and radius
selectivity. (b) Size selection of catalytic nanoclusters induced by
the steering effect of substrate superstructures. In this approach,
these nanochemical features will be used to investigate the effect of
spatially varying surface chemistry on thin film growth and nucleation.
(c) Selection of magic sized nanoclusters due to quantum size effects.
The confined motion of the conduction electrons in the nanometer or
smaller size regime in a metallic system may lead to the existence of
highly preferred length scales (both horizontal and vertical)
- Characterization:
The adsorption of hydrogen in carbon nanotubes will be followed using
two different techniques: X-ray spectroscopy and Temperature Desorption
Spectroscopy (TDS). The former will be used to study electronic
structure rearrangements as a signature of hydrogenation of the carbon
Φ-system, and the latter will measure the strength of adsorption (i.e.
chemisorption, physisorption, and/or van der Waals interaction) and the
amount of hydrogen that is released due to an increase in temperature
via linear heating of the sample. The total amount of hydrogen can be
calibrated against hydrogen monolayer coverage on metal
surfaces.
Issued March 2004