11 research outputs found
Molecular Dynamics Simulation of the Precipitation of Calcium Silicate Hydrate Nanostructures under Two-Dimensional Confinement by TiO<sub>2</sub>: Implications for Advanced Concretes
Given the environmental
footprint of concrete, the demand for new
concrete with higher macroscopic performances is continuously increasing
to build structures with less concrete while extending the service
life. With the advances in nanotechnology, comprehensive investigations
have shown that nanomodification of concrete can significantly improve
the macroscopic performances. However, many questions regarding the
interaction between nanomaterials and cement hydrates at the nanoscale
are still unclear, which greatly limits the further development of
nanoengineered concrete in construction. Herein, we use reactive molecular
dynamics simulation to investigate the precipitation of calcium silicate
hydrate gel (C–S–H gel, the principal binding phase
of conventional concrete) in the TiO2 nanochannel with
different spacings. Results show that the polymerization kinetics
as well as the final degree of polymerization of C–S–H
can be enhanced under the TiO2 nanoconfinement. Up to 15% Q4 units form in the more polymerized C–S–H
under TiO2 nanoconfinement. Because of the difference in
adsorption capacity for Ca and Si ions, the chemical composition of
C–S–H precipitated on the surface of TiO2 with oxygen dangling bonds will result in the nanosegregation of
Ca-rich and Si-rich regions, while the highly connected Qn units (Q3 and Q4 units) are formed in the Si-rich
regions. We also show that the hydroxylation of TiO2 surface
drives the polymerization process of C–S–H. On the basis
of the water mobility in the C–S–H gels, we demonstrate
the C–S–H growth in a limited spacing and precipitated
on the TiO2 surface, resulting in a more compact nanostructure
Topological Control on Silicates’ Dissolution Kinetics
Like many others,
silicate solids dissolve when placed in contact
with water. In a given aqueous environment, the dissolution rate depends
on the composition and the structure of the solid and can span several
orders of magnitude. Although the kinetics of dissolution depends
on the complexities of both the dissolving solid and the solvent,
a clear understanding of which structural descriptors of the solid
control its dissolution rate is lacking. By pioneering dissolution
experiments and atomistic simulations, we correlate the dissolution
ratesranging over 4 orders of magnitudeof a selection
of silicate glasses and crystals to the number of chemical topological
constraints acting between the atoms of the dissolving solid. The
number of such constraints serves as an indicator of the effective
activation energy, which arises from steric effects, and prevents
the network from reorganizing locally to accommodate intermediate
units forming over the course of the dissolution
Misfit Stresses Caused by Atomic Size Mismatch: The Origin of Doping-Induced Destabilization of Dicalcium Silicate
Density functional theory (DFT) simulations
are carried out to
systemically investigate doping in dicalcium silicate (Ca<sub>2</sub>SiO<sub>4</sub>: C<sub>2</sub>S), a major phase in calcium silicate
cements. By evaluating the energetics of defect formation mechanisms
for species involving Na<sup>+</sup>, K<sup>+</sup>, Mg<sup>2+</sup>, Sr<sup>2+</sup>, Al<sup>3+</sup>, Fe<sup>3+</sup>, B<sup>3+</sup>, and Ge<sup>4+</sup>, we find a strong site preference for all cationic
substitutions. As a result, distinct defects form at low dopant concentrations
(i.e., ≤ 0.52 atom %), in which, expectedly, larger dopants
prefer (larger) Ca<sup>2+</sup> sites, while smaller dopants favor
(smaller) Si<sup>4+</sup> sites, with charge balance being ensured
by the formation of vacancies. Such site preferences arise due to
local atomic distortions, which are induced when doping occurs at
unfavorable substitution sites. Interestingly, we note that the formation
enthalpy of each substitutional defect is proportional to the size
mismatch between the dopant and the native cations. This indicates
that the destabilization of the C<sub>2</sub>S structure has its origins
in an “atomic size misfit” which develops while accommodating
defects in the C<sub>2</sub>S lattice. The outcomes resulting from
this work provide insights that are needed to select dopants to optimize
cement performance by compositional design
Deciphering How Anion Clusters Govern Lithium Conduction in Glassy Thiophosphate Electrolytes through Machine Learning
Glasses such as lithium thiophosphates
(Li2S-P2S5) show promise as solid
electrolytes for batteries,
but a poor understanding of how the disordered structure affects lithium
transport properties limits the development of glassy electrolytes.
To address this, we here simulate glassy Li2S-P2S5 electrolytes with varying fractions of polyatomic anion
clusters, i.e., P2S64–, P2S74–, and PS43–, using classical molecular
dynamics. Based on the determined variation in ionic conductivity,
we use a classification-based machine-learning metric termed “softness”a
structural fingerprint that is correlated to the atomic rearrangement
probabilityto unveil the structural origin of lithium-ion
mobility. The softness distribution of lithium ions is highly spatially
correlated: that is, the “soft” (high mobility) lithium
ions are predominantly found around PS43– units, while the “hard”
(low mobility) ions are found around P2S64– units. We also show that
soft lithium-ion migration requires a smaller energy barrier to be
overcome relative to that observed for hard lithium-ion migration
Accessing a Forbidden Disordered State of a Zeolitic Imidazolate Framework with Higher Stiffness and Toughness through Irradiation
Metal–organic frameworks (MOFs) with nanoscale
porosity
have numerous potential applications, for example, within catalysis,
shock absorption, ion transportation, gas sorption, and separation.
Recently, the disordered state of MOFs has also attracted significant
attention, since some MOF crystals can melt and be quenched into bulk
glasses, as first discovered for zeolitic imidazolate frameworks (ZIFs,
a subset of MOFs). Another potential route to disorder in MOFsthat
so far remains unexploredis irradiation, e.g., silicate minerals
are well-known to rearrange into a disordered state upon irradiation.
Here, we investigate the structural disordering of both ZIF-4 crystals
and glasses under irradiation using reactive molecular dynamics simulations.
Our results show that the two phases converge toward a new “forbidden”
disordered state that is not accessible through any thermal path.
The evolution of the structure upon irradiation allows us to establish
a relationship between structural disorder and mechanical properties
to explain why the irradiated ZIF-4 state is both stiffer and tougher
than that of both the parent ZIF-4 crystal and glass
Electronic Origin of Doping-Induced Enhancements of Reactivity: Case Study of Tricalcium Silicate
Systematic manipulation of the reactivity
of silicate materials
in aqueous environment remains a challenging topic. Herein, by combining
first-principles and reactive molecular dynamics simulations, we present
a complete picture of the influence of impurity species on hydration
reactivity, using the reactive triclinic tricalcium silicate phase
as an example. We show that although initial hydration is influenced
by the surface’s chemistry and structure, longer-term hydration
is primarily controlled by proton transport through the bulk solid.
Both shorter- and longer-term hydration processes are noted as being
intrinsically correlated with electronic features. These outcomes
provide the first direct evidence of the linkages between electronic
structure and the longer-term (i.e., on the order of several nanoseconds)
hydration behavior and sensitivity of hydrophilic crystalline materials
and also offer a pathway to efficient compositional design for similar
materials
Predicting Fracture Propensity in Amorphous Alumina from Its Static Structure Using Machine Learning
Thin
films of amorphous alumina (a-Al2O3)
have recently been found to deform permanently up to 100% elongation
without fracture at room temperature. If the underlying ductile deformation
mechanism can be understood at the nanoscale and exploited in bulk
samples, it could help to facilitate the design of damage-tolerant
glassy materials, the holy grail within glass science. Here, based
on atomistic simulations and classification-based machine learning,
we reveal that the propensity of a-Al2O3 to
exhibit nanoscale ductility is encoded in its static (nonstrained)
structure. By considering the fracture response of a series of a-Al2O3 systems quenched under varying pressure, we
demonstrate that the degree of nanoductility is correlated with the
number of bond switching events, specifically the fraction of 5- and
6-fold coordinated Al atoms, which are able to decrease their coordination
numbers under stress. In turn, we find that the tendency for bond
switching can be predicted based on a nonintuitive structural descriptor
calculated based on the static structure, namely, the recently developed
“softness” metric as determined from machine learning.
Importantly, the softness metric is here trained from the spontaneous
dynamics of the system (i.e., under
zero strain) but, interestingly, is able to readily predict the fracture
behavior of the glass (i.e., under
strain). That is, lower softness facilitates Al bond switching and
the local accumulation of high-softness regions leads to rapid crack
propagation. These results are helpful for designing glass formulations
with improved resistance to fracture
Table_1_Glass Fracture Upon Ballistic Impact: New Insights From Peridynamics Simulations.DOCX
Most glasses are often exposed to impact loading during their service life, which may lead to the failure of the structure. While in situ experimental studies on impact-induced damage are challenging due to the short timescales involved, continuum-based computational studies are complicated by the discontinuity in the displacement field arising from the propagation of cracks. Here, using peridynamics simulations, we investigate the role of the mechanical properties and geometry in determining the overall damage on a glass plate subjected to ballistic impact. In particular, we analyze the role of bullet velocity, bullet material, and elastic modulus, fracture energy, and radius of the plate. Interestingly, we observe a power-law dependence between the total damage and the fracture energy of the glass plate. Through an auto-regressive analysis of the evolution of cracks, we demonstrate that the self-affine growth of cracks leads to this power-law dependence. Overall, the present study illustrates how peridynamic simulations can offer new insights into the fracture mechanics of glasses subjected to ballistic impacts. This improved understanding can pave way to the design and development of glasses with improved impact-resistance for applications ranging from windshields and smart-phone screens to ballistics.</p
Electrosteric Control of the Aggregation and Yielding Behavior of Concentrated Portlandite Suspensions
Portlandite (calcium hydroxide: CH: Ca(OH)2) suspensions
aggregate spontaneously and form percolated fractal aggregate networks
when dispersed in water. Consequently, the viscosity and yield stress
of portlandite suspensions diverge at low particle loadings, adversely
affecting their processability. Even though polycarboxylate ether
(PCE)-based comb polyelectrolytes are routinely used to alter the
particle dispersion state, water demand, and rheology of similar suspensions
(e.g., ordinary portland cement suspensions) that feature a high pH
and high ionic strength, their use to control portlandite suspension
rheology has not been elucidated. This study combines adsorption isotherms
and rheological measurements to elucidate the role of PCE composition
(i.e., charge density, side chain length, and grafting density) in
controlling the extent of PCE adsorption, particle flocculation, suspension
yield stress, and thermal response of portlandite suspensions. We
show that longer side-chain PCEs are more effective in affecting suspension
viscosity and yield stress, in spite of their lower adsorption saturation
limit and fractional adsorption. The superior steric hindrance induced
by the longer side chain PCEs results in better efficacy in mitigating
particle aggregation even at low dosages. However, when dosed at optimal
dosages (i.e., a dosage that induces a dynamically equilibrated dispersion
state of particle aggregates), different PCE-dosed portlandite suspensions
exhibit identical fractal structuring and rheological behavior regardless
of the side chain length. Furthermore, it is shown that the unusual
evolution of the rheological response of portlandite suspensions with
temperature can be tailored by adjusting the PCE dosage. The ability
of PCEs to modulate the rheology of aggregating charged particle suspensions
can be generally extended to any colloidal suspension with a strong
screening of repulsive electrostatic interactions
Resolving the Conflict between Strength and Toughness in Bioactive Silica–Polymer Hybrid Materials
Simultaneously
improving the strength and toughness of materials
is a major challenge. Inorganic–polymer hybrids offer the potential
to combine mechanical properties of a stiff inorganic glass with a
flexible organic polymer. However, the toughening mechanism at the
atomic scale remains largely unknown. Based on combined experimental
and molecular dynamics simulation results, we find that the deformation
and fracture behavior of hybrids are governed by noncovalent intermolecular
interactions between polymer and silica networks rather than the breakage
of covalent bonds. We then attempt three methods to improve the balance
between strength and toughness of hybrids, namely the total inorganic/organic
(I/O) weight ratio, the size of silica nanoparticles, and the ratio
of −C–O vs −C–C bonds
in the polymer chains. Specifically, for a hybrid with matched silica
size and I/O ratio, we demonstrate optimized mechanical properties
in terms of strength (1.75 MPa at breakage), degree of elongation
at the fracture point (31%), toughness (219 kPa), hardness (1.08 MPa),
as well as Young’s modulus (3.0 MPa). We also demonstrate that
this hybrid material shows excellent biocompatibility and ability
to support cell attachment as well as proliferation. This supports
the possible application of this material as a strong yet tough bone
scaffold material
