MDS |
Studying nanoscale
wettability
of different rock surfaces for ore flotation and oil recovery |
Condensed-phase Optimized
Molecular Potentials for Atomistic Simulation Studies (COMPASS) force-field,
Andersen thermostat, and Ewald summation methods |
Rock wettability ranks as
gypsum > calcite > halite > silica > graphite |
(58) |
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Silica’s water contact
angles change with oil polarity, ranging from 58° in hexane to
118° in toluene |
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To utilize MDS for simulating
some phenomena at a molecular level (oil/brine/rock system) and develop
a model that correlates free energies with contact angles |
Forcite module in Materials
Studio, incorporating the COMPASS force field and Nosé–Hoover
thermostat |
The model
accurately predicts
experimental results (R2 ∼ 0.98) |
(228) |
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MDS effectively and economically
assesses sandstone wettability changes |
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Analyzing shale organic
matter’s wettability under reservoir conditions |
COMPASS force field |
Water becomes more wettable
with rising temperature under certain pressures |
(203) |
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Water wettability drops
with higher salinity; Mg2+ and Ca2+ ions affect
wetting more than Na+
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Studying how interface wettability
affects Lennard-Jones fluid flow in nanochannels via molecular dynamic
simulations |
Non-Equilibrium
Molecular
Dynamics (NEMD) simulation with a modified Lennard-Jones potential |
Wettability greatly affects
interfacial hydrodynamic resistance |
(229) |
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Near solid walls, temperature
and pressure profiles vary due to wettability, with higher interfacial
friction increasing temperatures |
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Assessing wetting properties
and adsorption capacities of surfactants (ALES, SLES, TD, SDS) on
coal dust, by using MD simulations and quantum calculations |
Amorphous cell module |
Wetting performance is mainly
influenced by surfactants’ molecular structure, EO groups,
and hydrolytic cations |
(230) |
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NH4+ in ALES
and the combined hydrophilicity of EO groups and SO4– in ALES and SLES greatly improve their wetting and adsorption on
coal dust |
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To simulate nano water droplets’
wetting behavior on flat and pillar surfaces using molecular dynamics |
Large-scale Atomic/Molecular
Massively Parallel Simulator (LAMMPS) with Lennard-Jones potential
and SPC/E water model |
Higher surface energy on
flat surfaces reduces the contact angle, indicating better wettability |
(231) |
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Nanostructured pillar surfaces
are more hydrophobic than flat ones, with sparser pillars increasing
the contact angle |
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To assess how reservoir
temperature and kerogen structure affect shale kerogen wettability |
LAMMPS with Lennard-Jones
potential and SPC/E water model |
Kerogen contact angles vary
by type and maturity, with Type II being more water-wet and Type III
the least |
(232) |
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Rising reservoir
temperatures
decrease contactangles by 62%, increasing water-wettability |
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CFD |
To study the dynamic wetting
and wrapping process of coal dust by spray droplets |
A numerical simulation study
focusing on the dynamic wetting and wrapping process of coal dust
particles |
The study
found that a particle
size ratio (θ) over 2 between droplets and dust allows droplets
to fully cover and wet coal dust, while a ratio under 1 results in
ineffective wetting |
(233) |
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To determine the optimal
conditions for effectively wetting and settling respirable dust in
mining environments |
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Droplet velocity
is key
to wetting efficiency; lower velocities cause poor coverage, but at
around 20 m/s, wetting becomes faster
and more effective |
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To evaluate how surfactant-based
nanofluids change wettability and their impact on enhancing oil recovery |
multicomponent multiphase,
compositional model |
Surfactant-enhanced nanofluids
can shift rock wettability in tight oil reservoirs from oil-wet to
water-wet; this change improves capillary pressure and permeability,
aiding in increased oil extraction |
(234) |
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To understand how self-propelled
droplets on superhydrophobic surfaces with varying wettability control
their jumping direction |
The interFoam solver in
OpenFOAM which is based on the VOF model |
Surface energy gradients,
influenced by wettability, direct droplet movement toward smaller
contact angles |
(235) |
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To examine how reservoir
wettability, pore geometry, and fluid viscosity ratios impact relative
permeability |
LBM
for simulating two-fluid
flow in porous media |
Increasing reservoir rock
wettability from neutral to strong reduces the wetting fluid’s
relative permeability |
(236) |
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This effect on
the wetting
fluid’s permeability diminishes at higher viscosity ratios,
while the nonwetting fluid’s permeability is significantly
higher in strongly wet conditions compared to neutral wettability |
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To assess how silicon oxide
nanoparticles, affect wettability in glass micromodels to boost oil
recovery |
CFD (with
method performed
using Ansys Fluent software) |
Initial wettability significantly
affects oil saturation and recovery |
(197) |
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Nanofluid-induced wettability
alteration is time-dependent |
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Silica nanoparticles form
a nanotexture coating on solid surfaces, changing the wettability
from oil-wet to intermediate-wet, enhancing oil recovery |
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To explore microtexture
lubrication mechanisms through the lens of interface wettability |
CFD |
Isotropic textures with
low skewness and high kurtosis improve wettability and spreading |
(237) |
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Groove-shaped textures cause
anisotropic spreading through continuous triple contact lines, improving
wettability |
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To evaluate the wettability
of silicon microstructures made |
CFD with VOF model |
The VOF model accurately
simulates macroscopic contact-angle characteristics on complex surfaces |
(238) |
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To analyze and understand
discrepancies between experimental and theoretical contact angles
of these surfaces complex surfaces |
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A 2D CFD model with an equivalent
triangular waveform precisely predicts contact angles |
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To examine how surface wettability,
inclination, liquid properties, and impact velocity affect drop impact
and spreading dynamics |
VOF model |
The Static
Contact Angle
(SCA) model is precise for less wettable surfaces (SCA > 90°),
matching experimental results |
(239) |
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For more wettable surfaces
(SCA < 90°), the dynamic contact
angle (DCA) is higher initially, requiring the DCA model for accurate
predictions |
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ML |
To employ ML tools to efficiently
determine the contact angle, is crucial for assessing shale wettability
in CO2-enhanced oil recovery, CO2 sequestration in saline
aquifers, and hydraulic fracturing |
LR and RF |
The operating pressure,
temperature, total organic content (TOC), and mineral matter significantly
affect shale wettability |
(240) |
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The RF model proved
reliable
for predicting contact angles, offering an alternative to complex
experimental methods in CO2 sequestration applications |
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To improve carbon capture,
utilization, and storage by leveraging ANN and ANFIS for estimating
the contact angle in coal-water-CO2 systems. |
ANN and ANFIS |
The ANN and ANFIS models
demonstrated high accuracy in predicting contact angles in coal formations |
(222) |
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A new empirical equation
derived from the ANN model showed high accuracy, confirming the reliability
of machine learning in accurately predicting contact angles |
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To estimate shale wettability,
a key factor in CO2-EOR and CO2 storage in shale
formations |
Decision
tree, RF, function
networks, and gradient boosting regressor |
The operating pressure,
temperature, rock mineralogy, and TOC as significant factors affecting
shale wettability |
(241) |
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Machine learning
models,
especially the gradient boosting regressor, were effective in predicting
contact angles |
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To explore how rock mineral
composition and properties of oil-based drilling fluids affect the
wettability of tight gas sandstone formations |
General Regression Neural
Network (GRNN) |
The
mineral compositions
of quartz, feldspar, carbonate, and clay significantly affect the
wettability of tight sandstone |
(242) |
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The GRNN model accurately
predicted wettability |
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To evaluate shale wettability
based on formation pressure, temperature, salinity, TOC, and theta
zero |
Multilayer perceptron
(MLP)
and radial basis function neural networks (RBFNN) |
The Radial Basis Function
Neural Network-Many-Objective Optimization (RBFNN-MVO) emerged as
the most accurate |
(243) |
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Sensitivity analysis
identified
theta zero, TOC, pressure, temperature, and salinity as key factors
influencing shale wettability |
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To assess shale wettability
by analyzing critical factors such as formation pressure, temperature,
salinity, TOC, and theta zero |
MLP and RBFNN |
The RBFNN-MVO model was
the most accurate among tested ML models for predicting shale wettability |
(225) |
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The RBFNN-MVO model was
validated as an efficient and cost-effective tool for shale wettability
prediction |
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To assess the wettability
of CO2/brine/rock minerals (quartz and mica) in geological
formations |
Fully
connected feedforward
neural networks, extreme gradient boosting, k-nearest neighbors, decision
trees, adaptive boosting, and RF |
FCFNN model was more effective
than other machine learning techniques in predicting the wettability
of the mineral/CO2/brine system, achieving an R2 above 0.98 and an error below 3% |
(224) |