3. Results and Discussions
In this study, porous silica particles were synthesized from emulsion droplets as
micro-reactors using sodium silicate as the precursor. Silica aerogel microparticles
with spherical morphologies could be synthesized by adjusting the mixing ratio of
silicic acid and ammonium hydroxide for the gelation of the silica precursor inside
the emulsion droplets. After removing the remaining reactants inside the particles
by washing, solvent exchanges using ethanol and toluene were applied to maintain the
porous structure of the aerogel particles, followed by surface modification with a
silane coupling agent like trichloromethylsilane for hydrophobic aerogel particles,
as depicted schematically in Fig 1(a). To compare oil adsorption capacity, silica microparticles with wrinkled surfaces
were also synthesized from emulsion droplets, without using ammonium hydroxide. In
this case, emulsion droplets containing silicic acid was heated for preferential gelation
on the droplets’ interface, causing crumpling and folding of the microparticles during
droplet shrinkage. The resulting wrinkled surface was also modified using the silane
coupling agent used for the hydrophobic particles, as described in Fig 1(b). For some samples, sacrificial templates such as polystyrene nanospheres were included
during synthesis of the silica microparticles with wrinkled surfaces, to create macroporous
structures inside the silica microparticles, as described in Fig 1(c). After surface modification of these porous silica particles with wrinkled surfaces,
the amount of adsorbed silicone oil was compared with the results for other types
of silica microparticles.
In this study, silane coupling agents with hydrocarbon groups were adopted to change
the surface property of silica microparticles. During surface modification, the hydroxyl
groups on the silica particle surface can be changed by the hydrocarbon chains in
the silane coupling agent by the alcoholysis reaction, as described schematically
in Fig 2(a). The change in functional groups during surface modification was confirmed by FT-IR
analysis shown in Fig 2(b). After treatment using a coupling agent like trichlorododecylsilane, characteristic
peaks near 3,000 cm-1 appeared due to dodecyl groups on the silica surface, indicating that a hydrophobic
property could be imposed on the silica aerogel particles. When heated from 300 to
600 °C, the characteristic peaks due to the dodecyl groups disappeared, leaving silica
aerogel particles with the FT-IR absorption spectrum of conventional silica, as shown
in the graph in Fig 2(b).
During the synthesis of the silica aerogel particles, the volume ratio of silicic
acid solution and ammonium hydroxide was adjusted from 5:1 to 10:1, and the morphologies
of the resulting particles are displayed in the SEM images of Fig 3. When the amount of ammonium hydroxide was a relatively small value, such as the
mixing ratio of 5:1, the morphologies of the silica aerogel particles were irregular
shapes, as shown in Fig 3(a), indicating that the gelation speed was not fast enough to maintain the spherical
morphologies of the original emulsion droplets. Thus, small silica particles aggregated
to form larger irregular particles. When the amount of ammonium hydroxide was increased
to a mixing ratio of 7:1, disk-shaped and spherical silica aerogel particles were
formed together, indicating that the rigidity of the aerogel particles may not be
strong enough to maintain the spherical morphologies, deforming the spherical microparticles
into oblate ellipsoids. In this case, the gelation of silica sol proceeded completely,
since microparticles could be formed from emulsion droplets as micro-reactors, as
displayed in SEM image of Fig 3(b).
Further increase in ammonium hydroxide to a mixing ratio of 9:1 resulted in the formation
of spherical aerogel particles, as shown in the SEM image of Fig 3(c). Since the amount of ammonia was sufficient to promote fast gelation inside the emulsion
droplets and produce strong rigidity, all of the aerogel particles exhibited a spherical
morphology. The pH of the dispersed phase according to the mixing ratio of silicic
acid and ammonium hydroxide is summarized in Table 1, implying that decreasing the pH value while increasing the amount of ammonia caused
more rapid gelation inside the emulsion droplets. The size distribution of the spherical
aerogel particles was polydisperse, since the original emulsion droplets generated
by the homogenizer showed broad size distribution. Although the results are not reproduced
here, the morphologies of the silica aerogel particles were also spherical when the
mixing ratio was 10:1.
Fig 3(d) contains the pore size distribution of the silica aerogel particles synthesized using
the silicic acid solution and ammonium hydroxide at a mixing ratio of 9:1. Although
the N2 adsorption and desorption data is not reproduced here, the BET surface area of this
sample was measured to be 682.36 m2/g. Although the average pore size was measured to be 3.5 nm by the nitrogen adsorption
technique, it became difficult to detect pore size distribution after surface modification
using trichlorododecylsilane. Since the porous surface could be decorated with dodecyl
groups after modification, nitrogen adsorption may be hindered by hydrocarbon chains,
which block the bare surface of the porous structure of the silica aerogel, causing
a drastic change in pore size distribution before and after surface modification.
When the volume ratio of silicic acid to ammonium hydroxide solution was fixed at
9:1, the amount of trichlorododecylsilane was changed to investigate the effect on
the amount of adsorbed silicone oil (100 CS). As displayed in Fig 4(a), the amount of adsorbed oil increased ‘in overall’ with increasing amount of the
silane coupling agent, since enhanced hydrophobicity can be expected with increasing
number of hydrocarbon groups derived from the coupling agent. However, the amount
of adsorbed silicone oil declined as the concentration of silane coupling agent dissolved
in toluene was increased from 12 to 16%. Since the nanopores of the aerogel particles
can be blocked by chemisorption of the silane coupling agent, the amount of adsorbed
oil can be reduced by excessive addition of the coupling agent. However, a further
increase of the coupling agent concentration to higher than 16% may form a second
hydrophobic layer on the particle surface, which may increase the amount of adsorbed
oil again [22].
Unlike the effect of the silane coupling agent content on oil adsorption, there was
an optimal amount of precursors in the dispersed phase (emulsion droplets) to achieve
the maximum amount of adsorbed silicone oil (100 CS), as shown in Fig.4(b). When the
mixture of silicic acid and ammonium hydroxide was diluted using the same volume of
distilled water, the amount of adsorbed silicone oil was measured at its maximum value,
indicating that too diluted or concentrated precursors resulted in a decrease in the
amount of adsorbed oil. Accordingly, it is thought that an optimal value exists in
the void spaces to contain liquid oil in the solid silica phase modified with hydrophobic
silane coupling agent in aerogel particles.
In this study, trichloromethylsilane, with its shorter hydrocarbon group, was also
used to modify the aerogel particles to obtain a spherical hydrophobic powder, as
shown in Fig 5(a). The amount of silicic acid mixed with ammonium hydroxide solution was adjusted to
determine the composition of precursor solution for optimal oil adsorption capacity
after the modification using trichloromethylsilane, As shown in Fig 5(b), the surface area decreased from 733.46 to 246.19 m2/g after modification using the silane coupling agent, implying that chemisorption
of the trichloromethylsilane caused blocking of the nanopores in the aerogel particles.
As shown in the inset graph of Fig 5(b), the average pore size before surface modification was measured to be 88.23 Å, and
the very sharp distribution of the pore size disappeared after modification. However,
a new broad pore size distribution from 10 to 20 nm appeared after the surface modification,
similar to porous titania nanoparticles modified with 3-(2-aminoethylamino)propyldimethoxymethylsilane
[23]. Although the origin of the broad peak formation is not very clear, it is thought
that nanopores can be filled by the silane coupling agent, leading to the formation
of rough surfaces by successive chemisorption of the coupling agent, causing pore-like
structures on the particle surface.
Fig 5(c) contains the TGA results of the silica aerogel particles before and after surface
modification using trichloromethylsilane. Because the surface methyl groups originating
from the silane coupling agent can be removed by thermal degradation at temperatures
higher than about 250 °C, the mass of the aerogel powder modified with the silane
coupling agent was heavier than that of the bare aerogel particles, as shown in Fig 5(c). Materials remaining after the decomposition of hydrocarbon were recorded up to a
high temperature of 800 °C, implying that a carbon component may be coated on the
aerogel particles after heat treatment at high temperature.
To determine the optimum synthesis conditions for oil adsorption, the mixing ratio
of silicic acid to ammonium hydroxide solution was adjusted from 5:1 to 10:1 before
the emulsification step. As shown in Fig 6(a), an optimum value of the mixing ratio was found for maximum oil adsorption. Among
several samples, the aerogel powder with the 8:1 mixing ratio in the SEM image of
Fig 5(a) showed the maximum adsorption capacity, as displayed in the graph of Fig 6(a). Like the aerogel powder modified with trichlorododecylsilane, the optimal mixing
ratio of precursors was determined to be 8:1, implying that mixing ratios from 7:1
to 8:1 can result in the largest amount of oil adsorption regardless of the molecular
structure of the silane coupling agent. This indicates that oil adsorption can be
maximized using particles with a mixture of disk-shaped and spherical morphologies.
When irregular-shaped or spherical particles were solely used, oil adsorption was
less effective than the adsorption capacity of aerogel particles.
The random packing of the mixture of spherical aerogel particles and disk-shaped aerogel
particles can be modeled as a mixture of spheres and rod-like particles with a small
aspect ratio (L/D). Since the random packing fraction of this mixture is higher than
that of pure spheres (0.634), more compact packing of the mixed particles can be expected,
causing enhanced oil adsorption per unit volume of powder [24]. Thus, it is advantageous to use aerogel particles prepared at mixing ratios from
7:1 to 8:1 (aqueous silicic acid : ammonia solution).
The amount of trichloromethylsilane was also changed to investigate the effect on
oil adsorption capacity after surface modification of the aerogel powder, as displayed
in Fig 6(b). When the amount of hydrophobizing agent, trichloromethylsilane was too small,
the amount of adsorbed silicone oil was smaller than 200% due to insufficient coverage
of the methyl groups on the surface of the aerogel particles, which means the resulting
silica aerogel particles adsorbed silicone oil (100 CS) equal to almost 2 times the
mass of the porous particles. Because the nanopores contained in the aerogel particles
can be blocked to prevent liquid oil from being absorbed into the particles, an excessive
amount of trichloromethylsilane also resulted in a decrease in the amount of silicone
oil adsorbed. Thus, there was an optimal amount of trichloromethylsilane needed to
achieve the maximum amount of oil adsorption, 250%, as displayed in Fig 6(b).
The specific surface area of the silica aerogel particles fabricated and modified
under optimal conditions was measured by BET method, and the nitrogen adsorption and
desorption results are shown for samples before and after modification using trichloromethylsilane.
In this study, silicone oils with various viscosities were used to measure the amount
of oil adsorbed by silica aerogel particles synthesized by silicic acid solution and
ammonium hydroxide at an 8:1 mixing ratio and subsequent modification using trichloromethylsilane.
Overall, the amount of oil adsorbed decreased as the viscosity of the silicone oil
increased, as shown in Fig 6(c). Since viscous oil is difficult to infiltrate through the porous structure of the
aerogel, a highly viscous liquid resulted in less adsorption by aerogel particles.
This can be explained by the following Washburn equation [25].
Here, h and reff indicate the infiltration height through pores and the effective radius of the pore,
respectively. ΔP stands for the pressure difference between the applied and critical pressure, whereas
t and η are the infiltration time and the viscosity of the liquid, respectively. Thus, infiltration
height decreases with increasing liquid viscosity, causing a decrease in amount of
adsorbed silicone oil, since the infiltration of a viscous liquid through the nanopores
of the aerogel particle is difficult due to the existence of surface anchoring groups
originating from the silane coupling agent.
In this study, various kinds of silane coupling agents with alkyl groups having different
length of hydrocarbon chains were adopted for surface modification of the silica aerogel
particles. Fig 7(a) contains the FT-IR spectra of the silica aerogel particles after modification with
trichloromethylsilane, trichlorohexylsilane, trichlorododecylsilane, and trichlorooctadecylsilane.
When the modification was performed using trichloromethylsilane, the FT-IR spectrum
of the resulting aerogel particles was similar to PDMS (polydimethylsiloxane), indicating
that the characteristic peaks appeared at about 790 and 1,030 cm-1 due to the Si-C stretching of S-CH3. The peak that appeared at about 1,260 cm-1 was derived from the CH3 deformation of Si-CH3. [26]. Although similar characteristic peaks appeared in the FT-IR spectra of the silica
aerogel particles treated with trichlorohexylsilane and trichlorododecylsilane, the
peak intensity from trichlorododecylsilane was stronger compared to that of trichlorohexylsilane,
indicating that long-chain hydrocarbon resulted in a more intensive absorption peak.
Characteristic peaks at similar wavenumber appeared from the silica aerogel powder
modified with trichlorooctadecylsilane, as shown in Fig 7(a). The FT-IR spectrum of the silica aerogel powder modified with trichloropheylsilane
was also measured, and the result is shown as a blue line in Fig 7(a), indicating the characteristic peaks appeared at 1427, 696, and 727 cm-1 due to the Si-C6H5 bond [27].
Fig 7(b) contains the change in the amount of silicone oil (100 CS) adsorbed by the silica
aerogel particles as a function of the number of carbon atoms in the silane coupling
agent used for surface modification of the particles. From the graph in Fig 7(b), it is evident that the adsorbed amount of oil increased with increasing number of
carbon atoms in the silane coupling agent, except for the result from trichloromethylsilane,
since larger alkyl groups can enhance the hydrophobicity of the aerogel particles.
However, silica aerogel particles modified with trichlorooctadecylsilane revealed
less oil adsorption compared to the sample modified with trichlorododecylsilane, because
bulky hydrocarbon chains may block the nanopores in the aerogel particles, causing
a decreased in oil adsorption. When trichloromethylsilane was used for surface modification,
the amount of silicone oil adsorbed was larger than that of trichlorobutylsilane,
since the blocking of nanopores can be avoided by using trichloromethylsilane with
an alkyl chain shorter than the other types of silane coupling agent. Though the result
is not included in Fig 7(b), silica aerogel particles modified with trichlorophenylsilane showed an adsorption
capacity of 131.7%, which is a larger value than that of the aerogel powder treated
with trichlorohexylsilane, 72%. It is thought that this large discrepancy was caused
by the difference in the molecular structures of trichlorophenylsilane and trichlorohexylsilane,
implying that aromatic groups can be more advantageous than aliphatic groups for the
adsorption of oil.
In the photograph in Fig 7(c), silica aerogel particles adsorbing the silicone oil can be seen to be a solid-like
phase, indicating that the saturated state was achieved without an unadsorbed liquid-phase
oil. For better visualization, the oil was stained red using Sudan III dye. Since
the aerogel particles are lighter than water because of their porous and hydrophobic
nature after surface modification, the particles floated on the water-air interface,
as shown in the photograph in Fig 7(c). The degree of hydrophobicity of the aerogel particles was assessed by measuring
the contact angle of a water droplet coating a film composed of the particles, as
displayed in the photograph in Fig 7(d). As the number of carbon atoms in the hydrocarbon chain of the silane coupling agent
used during surface modification increased from 4 to 18, the contact angle increased
from 125.02 to 141.66 °, indicating that more hydrophobic particles could be prepared
using the silane coupling agent with longer alkyl chains. However, the contact angle
of the trichloroalkyl silane was higher than those of the coupling agent with butyl,
hexyl, and octyl groups, because the larger pore volume of the aerogel particles may
remain after modification with the short methyl groups, unlike the other types of
silane coupling agents with longer alkyl chains.
Fig 8(a) shows the change in oil adsorption capacity of the silica aerogel particles modified
with trichloromethylsilane as a function of the heating temperature of the particles
before oil adsorption. When the heating temperature was lower than 300 °C, the adsorption
of silicone oil was enhanced, growing with increasing heat treatment temperature.
This indicates that carbon elements derived from the coupling agents may remain on
the surface of the aerogel particles after the heat treatment, to maintain the hydrophobicity
of the particles. Though oil adsorption should be enhanced with increasing temperature,
it decreased again at higher temperature, since the short hydrocarbon chains derived
from the trichloromethylsilane were easily decomposed by applying larger thermal energy.
In this way, the optimal heating temperature was determined to be about 300 °C for
aerogel particles modified with trichloromethylsilane.
Fig 8(b) illustrates the change in the oil adsorption capacity as a function of heating time
after oil adsorption. The measurement was carried out using silica aerogel particles
synthesized under optimal conditions and modified using trichloromethylsilane. Due
to the diffusion of silicone oil adsorbed by the aerogel particles, oil adsorption
capacity decreased with increasing heating time at a relatively high temperature.
However, the amount of oil adsorption decreased and became negligible after 2 hours
of heating at 50 °C, indicating that a prolonged heating time at a higher temperature
like 70 °C is necessary to remove adsorbed oil from the particles.
In this study, silica aerogel particles synthesized from emulsion droplets were applied
as an oil adsorber to prepare composite films containing lubricant oil to avoid ice
adhesion to the film surface. In winter season, ice can be formed on construction
surfaces under humid air. Because this may reduce the generation rate of electricity
by depressing the motion of blades in a wind power system, an adequate coating technique
is essential to detach the adhered ice layer. Since our hydrophobic aerogel particles
containing a large amount of oil can be mixed with polymer films like PDMS, they can
be applied as an icephobic coating.
Icephobicity can be quantitatively discussed using ice adhesion strength, τice, which can be defined as the shear stress needed to detach an adhered ice layer from
a surface. Fig 9(a) shows the change in the ice adhesion strength (τice) of composite films made of PDMS, silica aerogel particles, and silicone oil as a
function of the amount of particle-oil mixture. The viscosity of the oil was 100 cSt,
and the mixing ratio of the oil and the aerogel particles modified with trichloromethyl
silane was maintained at 1:0.3. Because the oil functions as a lubricant it can be
enhanced by increasing the amount of particle-oil mixture, and τice could be reduced with increasing amount of the particle-oil mixture in the film,
implying that adhered ice layer cannot be maintained on the surface for long time.
Fig 9(b) shows the change in ice adhesion strength as a function of the viscosity of the silicone
oil mixed with silica aerogel particles. When the weight percent of the particle-oil
mixture was 70%, τice increased as the viscosity of oil increased, indicating that solid particles embedded
in the composite film may increase the surface roughness of the film, causing strong
attachment of the ice layer to the film surface. However, τice decreased for the composite film with a 50% particle-oil mixture with increasing
oil viscosity, due to the slow elution of viscous oil from the particles.
Fig 10(a), 10(b), and 10(c) contain SEM images of the silica microparticles with wrinkled surfaces, synthesized
using silicic acid solution and distilled water at different mixing ratios of 6:1,
4:3, and 1:6, respectively. As the amount of water in the dispersed phase (emulsion
droplets) increased, the volume occupied by the silica material in the final particles
decreased, due to decrease in silica precursor during the synthesis step, whereas
a high concentration of silicic acid resulted in more compact particles, as displayed
in the SEM images in Fig 10(a) to 10(c).
As shown in the graph in Fig 10(d), the adsorbed amount of silicone oil (100 CS) increased with the increasing concentration
of silicic acid, indicating that a greater amount of oil molecules could be adhered
more strongly to the compact silica particles with wrinkled surfaces shown in Fig 10(a), compared to the crumpled silica microparticles with less dense structure in Fig 10(b) or 10(c). Unlike the aerogel particles with a nanoporous structure, the porous nature of the
silica microparticles shown in Fig 10(a) to 10(c) can be considered ‘macroporous’ particles with irregular-shaped pores. Since macropores
are much larger than nanopores, huge amounts of liquid oil may not be contained in
the macropores due to the difference in the specific surface areas of the aerogel
and macroporous particles. To confirm this, the BET surface area of the silica microparticles
in Fig 10(b) was measured to be 148.93 m2/g, which is much smaller than that of the silica aerogel particles shown in Fig 3 or Fig 7, indicating that the specific surface area strongly affects the amount of adsorbed
oil.Table 2.
Porous structures can be expected to have enhanced properties including mechanical
properties [29]. In this study, the morphologies as well as porous structure of the silica microparticles
with wrinkled surfaces could be changed by the addition of PS nanospheres as templating
materials in a dispersed phase during synthesis. After calcination, porous silica
microparticles with hollow interior structures were fabricated after removal of the
PS nanospheres, due to removal of the polymeric beads, as shown in the SEM images
of Fig 11(a) and 11(b). For comparison, the amount of silicone oil adsorbed (100 CS) was measured using
the porous silica microparticles shown in Fig 11(a) and 11(b), as contained in the graph of Fig 11(d). Since the porous structures derived from the PS templates provide more space for
oil adsorption, the amount of adsorbed oil increased when the PS nanospheres were
included inside the emulsion droplets. However, the oil adsorption capacity of the
porous silica particles was inferior to that of silica aerogel particles, because
the aerogel particles contained smaller nanopores [28]. The BET surface area of porous silica particles in Fig 11(b) was measured to be 608.3 m2/g, which is smaller than that of the silica aerogel particles, and therefore the
adsorption capacity was inferior to the results of the aerogel particles.