Natalia A Wojas1,2, Agne Swerin3, Viveca Wallqvist1, Mikael Järn1, Joachim Schoelkopf4, Patrick A C Gane5, Per M Claesson2. 1. Division of Bioeconomy and Health, Materials and Surface Design Department, RISE Research Institutes of Sweden, Box 5607, SE 114 86 Stockholm, Sweden. 2. School of Engineering Sciences in Chemistry, Biotechnology and Health, Department of Chemistry, Division of Surface and Corrosion Science, KTH Royal Institute of Technology, Drottning Kristinas väg 51, SE-100 44 Stockholm, Sweden. 3. Faculty of Health, Science and Technology, Department of Engineering and Chemical Sciences: Chemical Engineering, Karlstad University, SE-651 88 Karlstad, Sweden. 4. Omya International AG, Baslerstrasse 42, CH-4665 Oftringen, Switzerland. 5. School of Chemical Engineering, Department of Bioproducts and Biosystems, Aalto University, P.O. Box 16300, FI-00076 Aalto, Finland.
Abstract
A profound understanding of the properties of unmodified and saturated fatty acid-modified calcite surfaces is essential for elucidating their resistance and stability in the presence of water droplets. Additional insights can be obtained by also studying the effects of carboxylic acid-saturated aqueous solutions. We elucidate surface wettability, structure, and nanomechanical properties beneath and at the edge of a deposited droplet after its evaporation. When calcite was coated by a highly packed monolayer of stearic acid, a hydrophilic region was found at the three-phase contact line. In atomic force microscopy mapping, this region is characterized by low adhesion and a topographical hillock. The surface that previously was covered by the droplet demonstrated a patchy structure of about 6 nm height, implying stearic acid reorganization into a patchy bilayer-like structure. Our data suggest that during droplet reverse dispensing and droplet evaporation, pinning of the three-phase contact line leads to the transport of dissolved fatty carboxylic acid and possibly calcium bicarbonate Ca(HCO3)2 molecules to the contact line boundary. Compared to the surface of intrinsically hydrophobic materials, such as polystyrene, the changes in contact angle and base diameter during droplet evaporation on stearic acid-modified calcite are strikingly different. This difference is due to stearic acid reorganization on the surface and transport to the water-air interface of the droplet. An effect of the evaporating droplet is also observed on unmodified calcite due to dissolution and recrystallization of the calcite surface in the presence of water. In the case where a water droplet saturated with octanoic acid is used instead of water, the stearic acid-coated calcite remains considerably more stable. Our findings are discussed in terms of the coffee-ring effect.
A profound understanding of the properties of unmodified and saturated fatty acid-modified calcite surfaces is essential for elucidating their resistance and stability in the presence of water droplets. Additional insights can be obtained by also studying the effects of carboxylic acid-saturated aqueous solutions. We elucidate surface wettability, structure, and nanomechanical properties beneath and at the edge of a deposited droplet after its evaporation. When calcite was coated by a highly packed monolayer of stearic acid, a hydrophilic region was found at the three-phase contact line. In atomic force microscopy mapping, this region is characterized by low adhesion and a topographical hillock. The surface that previously was covered by the droplet demonstrated a patchy structure of about 6 nm height, implying stearic acid reorganization into a patchy bilayer-like structure. Our data suggest that during droplet reverse dispensing and droplet evaporation, pinning of the three-phase contact line leads to the transport of dissolved fatty carboxylic acid and possibly calcium bicarbonate Ca(HCO3)2 molecules to the contact line boundary. Compared to the surface of intrinsically hydrophobic materials, such as polystyrene, the changes in contact angle and base diameter during droplet evaporation on stearic acid-modified calcite are strikingly different. This difference is due to stearic acid reorganization on the surface and transport to the water-air interface of the droplet. An effect of the evaporating droplet is also observed on unmodified calcite due to dissolution and recrystallization of the calcite surface in the presence of water. In the case where a water droplet saturated with octanoic acid is used instead of water, the stearic acid-coated calcite remains considerably more stable. Our findings are discussed in terms of the coffee-ring effect.
Calcium
carbonate (CaCO3) is the most abundant inorganic
biomineral in nature, which is due to the predominance of limestone
over other carbonate rocks.[1] Calcium carbonate
is a polymorphous, variform compound, which nucleates into three different
crystal modifications: calcite, aragonite, and vaterite.[2−4] Most limestone sources consist essentially of calcite as it is the
thermodynamically most stable polymorph under ambient conditions.[1] The most common crystal system of calcite is
the rhombohedral one, which exposes {101̅4} faces, and is frequently
used in experimental and theoretical studies as a model structure.[2,5] With all their advantages, calcium carbonate rock, that is, limestone,
marble, and chalk, enjoy considerable industrial utilization.[2,6,7] They are important in the pharmaceutical,
paper, plastic, and food industries and are also used in water purification
as precipitates strengthening the soils and as a sorbent for exhaust
gasses.[2,8−13] Moreover, it is considered as a key mineral to build many organisms’
exoskeletons for protecting and supporting purposes, as well as tissues
for light perception and storage of calcium ions.[2,5,14,15] Understanding
the surface chemistry of calcium carbonates and their interactions
with other substances is thus essential. In particular, the dynamic
nature of the calcite surface is an important issue where much information
can be gained by use of scanning probe methods.[16−18]In many
industrial applications, CaCO3 particles act
as fillers embedded in an organic matrix. To achieve the desired product
properties, the synergy between the filler and matrix needs to be
optimized. Thus, it is essential to understand the interactions occurring
at organic–inorganic interfaces. Different classes of compounds
have been evaluated as surface modification agents for calcite, and
carboxylic acids are commonly used for this purpose.[19−26] The high surface energy and hydrophilic surface of CaCO3 are incompatible with a low-energy surface of, for example, a non-polar
polymer matrix. Therefore, surface treatment of calcite is needed.
It is often aimed to improve not only the adhesion and dispersibility
but also the mechanical properties, including tensile strength, stiffness
and elongation, abrasion resistance, viscosity, and so forth.[27−30] In order to achieve full benefits from modified mineral fillers,
especially for moisture curing applications, it is essential to minimize
pickup of undesired organic molecules and water. A water film initiates
undesired generation of hydrated calcium bicarbonate that alters the
adsorption of modifiers.[31,32] Calcium carbonate has
limited solubility (14 mg/L) in pure water.[2,33] However,
if carbon dioxide is present, the solubility increases by more than
a factor of 100, and the carbonate ion goes into solution as a hydrogen
carbonate ion[2]As calcium carbonate has a high surface energy
(about 500–600
mJ/m2 for the {101̅4} plane), it also readily adsorbs
organic molecules.[34,35] Therefore, for fundamental studies,
a clean, freshly fractured CaCO3 surface should be used
for effective surface modification, after which the modified surface
should be stored in the dry pure air (or preferably vacuum) environment.
This is, however, not realistically achievable in industrial processes.[36] The calcite surface itself is highly reactive
and readily undergoes recrystallization with time in air and particularly
at high relative humidity. When the calcite surface is modified with
fatty carboxylic acids, the adsorption and layer reorganization will
compete and combine with hydration, dissolution, and recrystallization,[6,17] especially under mechanical wear and humid conditions.[18]For a profound understanding of the properties
of fatty carboxylic
acid-modified calcite surfaces, it is essential to elucidate their
resistance to water droplets, both below the droplet and at the droplet
edge. In this work, we followed the evolution of the surface wettability,
structure, and nanomechanical properties of pure and stearic acid-modified
calcite surfaces when exposed to deposited droplets of pure water
and water saturated with octanoic acid. Our results highlight the
importance of desorption into the bulk, and at the edge of, the droplet
and layer reorganization. As a result, the hydrophobized calcite surface
shows strikingly different wetting properties compared to the surfaces
of intrinsically hydrophobic materials. We utilize atomic force microscopy
(AFM) topographical and nanomechanical imaging to elucidate the effects
of the water droplet on bare calcite and carboxylic acid-modified
calcite surfaces. Our data show that the presence of aqueous droplets
leads to uneven adsorption due to layer rearrangements, dissolution,
and capillary flow. Our results are discussed in light of the coffee-ring
effect (CRE),[37−40] where capillary flow transports non-volatile material to the edge
of the droplet. Experiments with octanoic acid-saturated aqueous droplets
show that the CRE can be suppressed to achieve higher stability of
the initially homogeneous fatty acid layer.
Experimental Section
Materials
The material used in the
experiments was of optical quality Iceland spar calcite (mined in
Madagascar and purchased from Geocity AB, Stockholm). A rhombohedral
crystal was fractured into smaller samples with a stainless steel
chisel and hammer[17] along the dominant
{101̅4} cleavage plane. This highly hydrophilic surface[34,41] was immediately purged with pressurized nitrogen (nitrogen ≥99.9
vol %, oxygen ≤20 ppm, water ≤10 ppm) to remove debris
and minimize adsorption of airborne molecules. At least three samples
(for each study) of about 3 mm thick, and with surface areas in the
range of 25–450 mm2 exhibiting no evidence of excessive
microcracks and steps, were chosen for the measurements. An epoxy
glue (Bostik) was utilized for the sample attachment to the magnetic
disc used in AFM experiments. The following saturated carboxylic acids
were utilized for the modification of the calcite surface: octanoic
acid (C8, known as caprylic acid) for synthesis ≥99.0%
(Sigma-Aldrich) and octadecanoic acid (C18, known as stearic
acid) for synthesis ≥97.0% (Sigma-Aldrich). Polystyrene, in
the form of a Petri dish, was used as a reference sample for studies
concerning intrinsically hydrophobic materials. Silica gel granulate
(Merck) was used in order to maintain low humidity conditions (below
2.5 %RH) during carboxylic acid vapor exposure at room temperature.
The relative humidity was measured with an external sensor (HMT317,
Vaisala), placed in close proximity to the samples. Ultrapure Milli-Q
water (type 1, ASTM D1193-91) was utilized as water medium in all
studies. The laboratory room temperature was set at 23 ± 0.5
°C, and the room relative humidity varied in the range 25–35%.
Calcite Surface Modification with Carboxylic
Acids
The CaCO3 surface was modified by exposure
to carboxylic acid vapor. Surface modification via carboxylic acid
vapor exposure is, however, efficient only at high enough vapor pressure
and thus strongly dependent on the surrounding temperature.[42] For this reason, modification has to be performed
above the melting temperature. The vapor pressures of the fatty acids
under the deposition conditions are presented in Table .
Table 1
Melting
Point and Vapor Pressure at
the Deposition Temperature and Aqueous Solubility of Octanoic and
Stearic Acid[33,42]
Acid
Melting point (°C)
Vapor pressure (Pa) at deposition temperature
Aqueous solubility (g/kg) at 25 °C
C8
16.5
0.49liq at 25 °C
0.800
C18
69.3
355liq at 105 °C
0.003
For modification of the calcite surface with octanoic
acid, the
samples were stored inside a closed desiccator (volume about 2.3 L)
for 4 h at room temperature (about 23 °C). The desiccator contained
40–50 mL of octanoic acid in a flat glass beaker (diameter
about 57 mm). Another beaker with silica granulates was placed below
the porcelain plate to stabilize the low humidity inside the desiccator
at room temperature, so that calcite recrystallization was retarded.[17]For modification by stearic acid, an oven
(UF 55, Memmert) was
used and set for 4 h at a temperature of 105 °C, and the relative
humidity was estimated to be below 2.5 %RH. The temperature and time
were chosen to achieve the full monolayer coverage as judged by the
high initial water contact angle (CA). The samples were kept in an
unsealed 1.5 L glass box containing a glass beaker filled with 20–25
g of stearic acid that was previously melted at the same temperature
for about 90 min.
Saturated Octanoic Acid
Solution
To study surface interactions with water, one should
not only consider
pure water but also saturated solutions of the carboxylic acids used
for modification of the calcite surface. Due to the low solubility
of stearic acid (Table ), we have chosen to investigate only solutions saturated with octanoic
acid. The C8-saturated solution was made by overnight magnetic
stirring of octanoic acid with Milli-Q water followed by sedimentation
of the heavier C8-saturated aqueous solution and decantation
of this liquid through separatory funnel drains. The pH of this solution
was initially around 4 and found to increase slowly with time in the
presence of calcite (see Supporting Information, Figure S1).The surface tension of octanoic acid and the
initial liquids was measured using two methods for accuracy. In the
pendant drop shape analysis method, the shape of the drop hanging
from a needle is determined from the balance of forces which include
gravitational pull and the surface tension of the liquid being investigated.
The droplet size was increased by 1 μL/s, and the droplet was
released from the needle when the volume reached 20–30 μL.The second method utilized a platinum Wilhelmy plate and a Force
Tensiometer-K100 (Krüss, Germany), where the force acting on
a vertically immersed plate is measured. The plate was removed from
the liquid at a speed of 10 mm/min, using an initial immersion depth
of 2 mm. The measurements were repeated about 20 times. The average
values for the surface tension from all measurements and density of
the studied solutions are reported in Table .
Table 2
Average Surface Tension
and Density
of Milli-Q Water, C8-Saturated Milli-Q Water, and Octanoic
Acid at 22 °Ca
Solution
Surface tension(mN/m)
Density(kg/m3)[33]
Milli-Q water
71.9 ± 0.4
0.997
C8-saturated Milli-Q water
31.5 ± 0.2
-
Octanoic
acid (liq)
28.3 ± 0.1
0.911
The density of
C8-saturated
Milli-Q water has not been measured.
The density of
C8-saturated
Milli-Q water has not been measured.
Surface Imaging and Nanomechanical Properties
The morphology and nanomechanical properties of carboxylic acid-modified
calcite surfaces exposed to liquid droplets were recorded by utilizing
a MultiMode 8 AFM (Bruker) with a standard holder and scanner (S/N:
10578JVLR, Bruker). Special wear-resistant HQ:NSC35/Hard/Al BS probes
(MikroMasch) with a nominal tip diameter of <20 nm, resonance frequency
of 330 kHz, and nominal spring constant, k, of 21 N/m were used as they are highly resistant
to wear. The actual value of k was determined using the thermal tune method within the Nanoscope
program.[43] The deflection sensitivity in
the normal direction was found to be 24.2 nm/V with the use of a sapphire
calibration sample (Bruker) in air. The modified calcite surfaces
were studied immediately after preparation. After locating a relatively
smooth area of the sample with a white-light microscope, the edge
of a deposited water droplet was found by utilizing a microscope equipped
with a camera, also under white light illumination. After removing
the water droplet, the edge region and the region previously below
the droplet were investigated by AFM. For these studies, the peak
force quantitative nanoscale mechanical characterization (QNM) mode
was used with the selected applied force of 20 nN. This force was
utilized since it deformed the surface sufficiently to allow measurements
of nanomechanical properties and yet was sufficiently low to not damage
the tip itself, as judged by imaging rough surfaces before and after
measurements. Nanomechanical properties were determined using 512
× 512 pixel images over a scanned area from 2 × 2 to 40
× 40 μm2 with a scanning frequency of 0.5–1.0
Hz. In all cases, no image enhancement was performed apart from plane
fit and flattening of height (second order) images in the NanoScope
Analysis program. We note that the exact values of nanomechanical
properties, such as adhesion and deformation, in general depend on
probe radius and applied force. For this reason, we focus on variations
in these properties observed in images taken by the same probe using
the same applied force, which remains consistently the case when considering
individual nanomechanical images.
Contact
Angle
The interactions between
modified calcite surfaces and liquids (Milli-Q water, saturated aqueous
octanoic acid solution) were measured using an optical CA device (OCA40,
Data Physics Instruments GmbH) equipped with an automated micro-pipette.
The droplet shape was recorded at the rate of 6 frames/s by a high-resolution
CCD camera and analyzed utilizing the ellipse fitting method in the
SCA20 software (DataPhysics Instruments GmbH). The average of the
CAs on the left and the right side of the droplet was calculated.
All CA measurements were carried out immediately after surface modification.
At least five samples were analyzed, where each could fit 2–4
independent 1 μL water droplets.The contact angle hysteresis
(CAH) was determined by measuring the advancing and receding CAs.
The advancing CA was determined when the droplet volume was increased
to 5 μL, after which the droplet was kept on the sample surface
for about 30 s. Next, the receding CA was determined when the droplet
volume was decreased again. In all these measurements, the speed of
the droplet change was set to 1 μL/s. Between measurements,
the syringe was cleaned from the concealed liquid by dispensing several
droplets (about 15–20 μL) outside the sample surface.
Results and Discussion
In this section, we
first consider morphological and nanomechanical
changes that occur on calcite and carboxylic acid-modified calcite
surfaces, as a result of exposure to droplets of pure water and water
saturated with octanoic acid. Next, we consider the wetting characteristics
of carboxylic acid-modified calcite, including CAH and changes in
CAs and base diameter (BD) during droplet evaporation.
Morphological and Nanomechanical Changes
Droplets
on Unmodified Calcite
Pure Water
To
gain a clear understanding
of how the droplet affects the surface, the morphological and nanomechanical
changes were first elucidated. Figure a shows the topography, tip-sample adhesion, and surface
deformation of a calcite surface area. Here, the lower left part has
been covered by a microliter range water droplet for 30 s, while the
upper right part has been in contact with air. The border between
these two areas is most clearly seen in the adhesion image, and the
boarder is located at exactly the same position in the other images
as they were collected at exactly the same time and at exactly the
same spot on the surface. The calcite surface area that was located
under the water droplet and at the edge of the water droplet is different
from the area only exposed to air. This is evidently seen in the adhesion
and deformation images but less clearly in the topography image. In
the adhesion and deformation images, one can distinguish the position
of the droplet edge and non-spherical deposits with decreased adhesion
and increased deformation under the previously dispensed droplet.
The observed changes are due to more extensive dissolution and recrystallization
of the calcite surface in contact with water. As discussed in our
previous work,[17] these features are signs
of formation of a hydrated form of calcium carbonate, and apparently
this transformation occurs more rapidly below the droplet than outside
the region previously covered by the droplet. The solubility of calcite
in pure water is 14 mg/L,[33] but it increases
significantly in the presence of carbon dioxide due to the formation
of calcium bicarbonate Ca(HCO3)2 (solubility
166 g/L[33]). During prolonged exposure to
ambient air, further morphological changes occur also in the areas
not exposed to water, not clearly shown here but reported in detail
in our previous work.[17] This is due to
the hydrophilic nature of calcite that allows formation of a thin
adsorbed water layer on the surface, and we have previously shown
that the rate of change increases with increasing relative humidity.[17]
Figure 1
AFM topography and nanomechanical images of the calcite
surface
after contact with a water droplet (a) and C8-saturated
water droplet (b), prior and after exposure to 25–35 %RH air
overnight. Microscopic images illustrate the position of the droplet.
The edge of the aqueous droplet is marked by an arrow. Large features
(surface steps) seen in the topography image are due to the crystal
structure and not a result of the droplet edge. 40 × 40 μm2 images are provided in Figure S2 in Supporting Information.
AFM topography and nanomechanical images of the calcite
surface
after contact with a water droplet (a) and C8-saturated
water droplet (b), prior and after exposure to 25–35 %RH air
overnight. Microscopic images illustrate the position of the droplet.
The edge of the aqueous droplet is marked by an arrow. Large features
(surface steps) seen in the topography image are due to the crystal
structure and not a result of the droplet edge. 40 × 40 μm2 images are provided in Figure S2 in Supporting Information.
Octanoic
Acid-Saturated Water
As
shown in Figure b,
the surface area exposed to the octanoic acid-saturated water droplet
is at the lower part of the images. Here, the curved line shown in
all images represents the position of the droplet edge. By comparing Figure a,b, it is clear
that the surface below the droplet is less affected when C8-saturated water is added compared to when pure water droplets are
used. In particular, we observe a more homogeneous surface and no
deposits at the droplet edge, which implies that the calcite surface
is partly protected by C8 adsorption. Indeed, water CA
measurements on a calcite surface dipped into saturated octanoic acid
solution show an initial CA of 99° after removal from the solution,
demonstrating the formation of an octanoic acid monolayer. Interestingly,
we find no nanomechanical contrast between droplet-exposed and unexposed
areas. Recrystallization with growing patches on the terraces and
steps becomes evident in the adhesion image after overnight air exposure.
As before, the tip-surface adhesion is decreased in the recrystallized
areas.
Droplets on Octanoic Acid-Modified
Calcite
Data obtained for calcite
modified by exposure to octanoic acid vapor and then exposed to a
water droplet for 30 s are presented in Figure a. Here, the droplet covered the lower left
part in the images, and the droplet edge is seen clearly in adhesion
and deformation images. The border is distinguished by a curved line
of well-defined spherical deposits. However, the roughness of the
surface does not allow these features to appear evidently in the topography
image. They are apparently due to octanoic acid that partly dissolves
in the water droplet and accumulates at the air–water interface
before being partly deposited again as the water droplet is removed.
It is not clear if the deposits only contain octanoic acid or if also
dissolved and recrystallized calcium carbonate is included. However,
these deposits can be easily smeared out by scanning the AFM tip in
the contact mode over the surface (data not shown), even though they
remain for hours (images on the right are after 18 h exposure to air)
if left untouched in air. Compared to the bare calcite surface, Figure a, octanoic acid
deposition reduces the recrystallization of the surface upon water
exposure. However, due to the C8 solubility in water, a
structural change of the surface is still observed, but it is now
mainly due to the rearrangement of the adsorbed octanoic acid. Thus,
our hypothesis is that the solubilization of octanoic acid and redeposition
on the surface during droplet removal are the cause for the structural
changes, as observed in Figure a.
Figure 2
AFM topography and nanomechanical images of the C8-modified
calcite surface after contact with a water (a) and C8-saturated
water droplet (b), prior and after exposure to 25–35 %RH air
overnight. Microscopic images illustrate the position of the droplet.
The edge of the aqueous droplet is marked by an arrow. 40 × 40
μm2 images are illustrated in Figure S3 in Supporting Information.
AFM topography and nanomechanical images of the C8-modified
calcite surface after contact with a water (a) and C8-saturated
water droplet (b), prior and after exposure to 25–35 %RH air
overnight. Microscopic images illustrate the position of the droplet.
The edge of the aqueous droplet is marked by an arrow. 40 × 40
μm2 images are illustrated in Figure S3 in Supporting Information.
Octanoic Acid-Saturated Water
In
case the mentioned hypothesis is correct, no similar changes should
be observed if the (partial) solubilization of the adsorbed octanoic
acid was prevented. This situation can be achieved using a saturated
aqueous C8 solution instead of pure water. In this case,
exchange of octanoic acid in solution and on the surface can occur,
but the overall octanoic acid concentration in the droplet cannot
be increased. The data in Figure b report on this situation. One can still clearly distinguish
the droplet edge in the adhesion and deformation images, but the surface
area exposed to the saturated aqueous octanoic acid solution looks
homogeneous but with higher adhesion and lower deformation than the
unexposed area, suggesting additional adsorption of octanoic acid.
In contrast to the case with a water droplet, no spherical deposits
are observed at the droplet edge. Apparently, the deposited octanoic
acid monolayer is more stable in contact with a saturated octanoic
acid solution than that in contact with pure water, which would be
expected if solubilization of octanoic acid was the main reason for
the structural changes, as observed in Figure a. With increasing time in air, the difference
in nanomechanical properties between the exposed and unexposed area
decreases, suggesting surface diffusion aided by adsorbed water vapor
that evens out the initial packing density contrast. We note that
in Figure b, we see
small surface features on the air side. They are distinguished by
lower adhesion than the surrounding, which distinguishes them from
the C8 deposits found on the area covered by the droplet,
as shown in Figure a. The features, as seen in Figure b, are likely debris from the cleavage in the form
of hydrated calcite, which is dissolved and/or removed when exposed
to the droplet and during droplet removal.
Droplets on Stearic Acid-Modified Calcite
Pure
Water
Stearic acid is much
less soluble in water than octanoic acid (Table ). Thus, one would not expect that dissolution
of the C18 layer would be of equal importance as for C8 layers. However, rearrangements of the layer can still occur.
Calcite modified with stearic acid vapor has a very hydrophobic nature
(Table ), resulting
from the hydrocarbon chains being exposed outward, while the carboxylic
acid groups are attached to the calcite surface. From surface energy
considerations, this remains a favorable situation when the surface
is in contact with air but not when in contact with water. Thus, one
could expect that surface energy minimization would drive a reorientation
of the pre-adsorbed stearic acid layer when exposed to a water droplet.
This indeed occurs and is shown in Figures and 4a where the
water droplet covered the lower left part of the image of the C18-modified calcite. The thin irregular line, as seen in the
topography image in Figure , is due to stearic acid deposition at the pinned contact
line. Just below this line follows an area with increased adhesion
and decreased deformation that suggests depletion of the stearic acid
layer on the water side of the applied droplet edge. Further inside
the droplet, the initially homogeneous adsorbed acid layer has been
converted into a patchy array over the calcite surface. The height
of the patches seen in the topography images in the region exposed
to the droplet is about 4.4–6.7 nm, which indeed suggests transformation
of the initial monolayer into at least bilayer patches. In comparison,
the extended length of the stearic acid molecule is 2.4–2.6
nm.[20,22]
Table 3
Initial Contact Angle of Milli-Q Water
and C8-Saturated Milli-Q Water Droplets on Calcite and
Carboxylic Acid-Modified Calcite
Solution
Freshly fractured
CaCO3
C8-modified
CaCO3
C18-modified
CaCO3
Milli-Q water
<5°
105° ± 3°
108° ± 5°
C8-saturated Milli-Q water
70° ± 5°
68° ± 2°
69° ± 2°
Figure 3
AFM topography and nanomechanical images of
the C18-modified
calcite surface after contact with a water droplet prior and after
exposure to 25–35 %RH air overnight. Microscopic images illustrate
the position of the droplet. The edge of the aqueous droplet is marked
by an arrow. Note the large accumulation of the material at the droplet
edge, which is due to the CRE.
Figure 4
AFM topography
and nanomechanical images of the C18-modified
calcite surface after contact with a water (a) and a C8-saturated water droplet (b) prior and after exposure to 25–35
%RH air overnight. Microscopic images illustrate the position of the
droplet. The edge of the aqueous droplet is marked by an arrow. The
two images with scale bar 2 μm in (a) are focused on areas at
the droplet edge (upper one) and below the droplet (lower one). Corresponding
5 × 5 μm2 images to those in panel (b) are reported
in Figure S4 in Supporting Information.
Note the different scale bars in Figure a,b.
AFM topography and nanomechanical images of
the C18-modified
calcite surface after contact with a water droplet prior and after
exposure to 25–35 %RH air overnight. Microscopic images illustrate
the position of the droplet. The edge of the aqueous droplet is marked
by an arrow. Note the large accumulation of the material at the droplet
edge, which is due to the CRE.AFM topography
and nanomechanical images of the C18-modified
calcite surface after contact with a water (a) and a C8-saturated water droplet (b) prior and after exposure to 25–35
%RH air overnight. Microscopic images illustrate the position of the
droplet. The edge of the aqueous droplet is marked by an arrow. The
two images with scale bar 2 μm in (a) are focused on areas at
the droplet edge (upper one) and below the droplet (lower one). Corresponding
5 × 5 μm2 images to those in panel (b) are reported
in Figure S4 in Supporting Information.
Note the different scale bars in Figure a,b.A more pronounced accumulation of material at the
droplet edge
occurs for stearic acid-modified calcite, as observed in Figure , compared to the
C8-modified surface, as illustrated in Figure a, which is related to the
CRE, discussed later, and the solubility of the carboxylic acids.
Octanoic acid can be partly solubilized in the water droplet, whereas
C18 hardly dissolves but can be transported to the edge
via the air–water interface. Compared to the C8 case,
the border between the exposed and unexposed areas is less regular,
which is due to more severe droplet pinning (Figure ). This, in turn, is due to a larger difference
in hydrophobicity between the area under the droplet and at the edge
where stearic acid is removed to the air–water interface. The
droplet edge region remains clearly seen also after 15–16 h,
suggesting high stability of the stearic acid layer in air, and we
also note recrystallization of calcite in exposed bare calcite areas
(close to the droplet edge), most evidently seen in the nanomechanical
images of Figures and 4a.We note that the images, as
shown in Figure ,
cover a significantly larger area than
those reported in Figures and 2. The reason for this is that
the surface area affected by the water droplet is so large for stearic
acid-modified calcite that it cannot be captured fully at higher resolutions.
Nevertheless, higher resolution images of the droplet edge region
for stearic acid-modified calcite are provided in Figure a to facilitate direct comparison
with the images reported in Figures and 2.When
a droplet of C8-saturated aqueous solution is used (Figure b), a much smaller
effect on the surface morphology and nanomechanical properties is
observed than with pure water. In fact, in order to see clearly any
effect at all, we needed to image small surface areas (note the scale
bar in Figure b),
and here slight differences in adhesion and deformation of the area
exposed and not exposed to the droplet can be distinguished. The reason
for this is that there is now another mechanism than C18 reorientation that can reduce the surface energy between the modified
calcite surface and the aqueous solution. This is adsorption of octanoic
acid on top of the C18 layer, which has the energetic advantage
that the strong bond between calcite and the carboxylic acid group
is retained, while the interfacial energy between the surface and
the aqueous phase is reduced. As a result of predominance of octanoic
acid adsorption hardly any contrast or spherical deposits are seen
in any of the images in Figure b. This also suggests that the outer layer of octanoic acid
adsorbed on top of the stearic acid layer by hydrophobic interactions
is removed together with the water droplet. By comparing the data
reported in Figure a,b it is clear that our results demonstrate that the presence of
C8 in the aqueous solution stabilizes the C18 layer significantly.
Surface Wettability Hysteresis
The structural changes
observed under the deposited droplets and at the edge of the droplet
should also be evident in the wetting behavior. Thus, to gain further
understanding, experiments focused on water CAH were performed. Here,
the three-phase contact line was advanced during the first 5 s by
increasing the droplet volume, then kept at rest for 30 s, and finally
withdrawn by reducing the droplet volume. Thus, the surface was in
contact with the droplet under the same conditions as analyzed after
droplet removal in the previous sections. The initial CAs measured
at 1.2 s after droplet deposition for all mentioned samples are stated
in Table .Droplets
of Milli-Q water spread on freshly cleaved calcite, whereas C8- and C18-modified surfaces are initially hydrophobic
with CAs close to 110°. However, with time, the carboxylic acid
layer under the droplet and at the droplet edge changes, as demonstrated
previously in Figures –4. As illustrated here in Figure , this results in
a decrease in the CA and increase in droplet BD with time. The changes
occur much more rapidly for the more soluble C8 compared
to the less soluble C18. Quantitatively, the droplet BD
increases by 35% on octanoic acid-modified calcite and by 5% on stearic
acid-modified calcite. The water droplet is initially pinned when
retracted, which is due to the hydrophilic region created at the droplet
edge.
Figure 5
CAH and normalized droplet BD of water droplet on (a) octanoic
acid-modified, (b) stearic acid-modified calcite surfaces; and octanoic
acid-saturated water droplet on (c) freshly fractured calcite surface,
(d) octanoic acid-modified, (e) and stearic acid-modified calcite
surfaces.
CAH and normalized droplet BD of water droplet on (a) octanoic
acid-modified, (b) stearic acid-modified calcite surfaces; and octanoic
acid-saturated water droplet on (c) freshly fractured calcite surface,
(d) octanoic acid-modified, (e) and stearic acid-modified calcite
surfaces.The
CA measured with a saturated aqueous C8 solution is in
all cases initially around 70°. This means that both for bare
calcite and carboxylic acid-modified calcite, we end up with a similar
situation, suggesting a monolayer coverage just outside the droplet
edge and a full or partial bilayer exposing carboxylic acid groups
toward the solution under the droplet due to C8 adsorption.
When the octanoic acid-saturated droplet is at rest, the CA and BD
are much more stable as compared to the case of pure water droplets.
This is due to the higher stability of the initial carboxylic acid
layer, as demonstrated in Figures –4. Quantitatively, we
find that the BD increased by less than 2% of the initial values for
C8-saturated droplets. As the droplet volume was reduced,
the BD decreased more readily, that is, in a shorter time after starting
the droplet volume reduction process, compared to when a pure water
droplet was used. This correlates with the smaller edge effects seen
in the AFM images, Figures –4. However, the data suggest
some pinning also when aqueous-saturated octanoic acid solutions are
used.
Wettability of Drying Droplets
In our discussion above,
we have emphasized dynamic changes in the adsorbed carboxylic acid
layer to rationalize the wetting behavior and found support for this
in the structural changes observed by AFM. One would thus expect a
different wetting behavior of stearic acid-modified calcite and the
surface of an intrinsically hydrophobic material, such as polystyrene.
To elucidate this, we followed the change in CA and normalized BD,
where the BD at any time, t, is normalized by the
initial BD, evaluated at t = 1.2 s, during droplet
evaporation, and quoted as %, that is (BD(t)/BD(t = 1.2)) × 100 (Figure ). Note the extended time of these experiments (30
min) compared to those reported in previous sections (30 s). The CA
of the water droplet on the polystyrene sample (Figure a) decreased slowly with time during the
first 5 min, from 98 to 81°. This suggests reorientation of surface
groups to expose less hydrophobic sites toward water.[44,45] The BD was seen to be initially fixed, such that the reduction of
the droplet volume due to evaporation was compensated by the decrease
in CA. However, after the point where apparently no further rearrangements
at the polystyrene surface can occur, the decrease in the CA terminated,
and the BD became significantly reduced due to evaporation, that is,
at this stage, we encounter the receding CA that is about 80°.
About 2 min prior to complete evaporation, the CA decreased again
as the droplet contracted to a very small size.
Figure 6
CA and normalized BD
as a function of time on stearic acid-modified
calcite and polystyrene. Measurements were carried out with (a) water
and (b) octanoic acid-saturated water droplets.
CA and normalized BD
as a function of time on stearic acid-modified
calcite and polystyrene. Measurements were carried out with (a) water
and (b) octanoic acid-saturated water droplets.The stearic acid-modified calcite surface is, as discussed above,
more complex than polystyrene since in this case, our AFM data show
that the stearic acid layer rearranges. Stearic acid can also be partly
transferred to the water–air interface of the droplet and to
a very limited degree desorbs into the bulk of the droplet. This is
reflected in the wetting behavior, as illustrated in Figure a,b. We find, thus, that the
evaporating droplet also behaves very differently on stearic acid-modified
calcite than that on polystyrene. The water CA on stearic acid-modified
calcite was found to decrease continuously with time (CA decreased
from 107° to about 17° within 17.5 min) as the layer under
the droplet became restructured (Figures and 4). In contrast,
the BD first increased up to 118% of its initial value during the
first 5 min as stearic acid molecules at the interface were removed
to the air–water interface, and then, the BD stabilized. This
is opposite to the case of the droplet on polystyrene where the CA
remained constant, but the BD was shrinking during droplet evaporation.
Thus, on stearic acid-modified calcite, the droplet becomes pinned,
which is due to the hydrophilic region generated at the droplet edge
observed in the AFM image (Figures and 4a) caused by stearic acid
desorption at the three phase contact line (TPCL).A
different behavior was observed for the CA of the octanoic acid-saturated
water droplets (Figure b). Here, the CA decreased by only 2° during the first 21 min
for polystyrene, while the BD was continuously reduced in response
to evaporation. About 8 min prior to complete evaporation, the CA
started to decrease again as octanoic acid was deposited, and the
droplet contracted to very small size.Just as for polystyrene,
the BD of the evaporating C8-saturated water droplet was
seen to shrink continuously on C18-modified calcite. Thus,
the presence of C8 counteracts removal of stearic acid
at the edge of the droplet, and no pinning occurs. The CA was initially
stable at around 70°, in accordance with Figure . However, after this initial period, the
CA decreased continuously with time (CA decreased from 73° to
about 32° within 9 min) at the same time as the BD decreased.
This is lower than the receding CA, as shown in Table . From this, we conclude that C8 stabilizes the C18 layer for a limited time only. It
appears that entropic effects with time lead to some displacement
of C18 with C8 at the calcite surface.
Table 4
Advancing and Receding Contact Angle
of Milli-Q Water and C8-Saturated Milli-Q Water Droplets
on Calcite and Carboxylic Acid-Modified Calcitea
Droplet
Surface
Advancing CA, θa
Receding CA 1, θr
Receding CA 2, θr
Fp 1 (mN m–1)
Fp 2 (mN m–1)
H2O
C8-modified
109 ± 3°
41°
15°
4.9
6.8
C18-modified
106 ± 4°
69°
-
2.7
-
C8-saturated H2O
Freshly fractured calcite
70 ± 1°
58°
47°
0.38
0.35
C8-modified
71 ± 2°
62°
53°
0.28
0.28
C18-modified
74 ± 1°
60°
55°
0.44
0.16
The advancing
CA is an average value
obtained during the first 5 s when the contact line starts to advance.
Receding CA 1 reflects the CA when the droplet BD starts to decrease,
while receding CA 2 is evaluated when the droplet BD stabilizes and
remains constant for some time. The resulting pinning force, Fp, values were calculated as: Fp = γLV(cos θa –
cos θr), where the liquid–vapor surface tension
γLV can be found in Table , and θa and θr are the advancing and retreating CAs, respectively.
The advancing
CA is an average value
obtained during the first 5 s when the contact line starts to advance.
Receding CA 1 reflects the CA when the droplet BD starts to decrease,
while receding CA 2 is evaluated when the droplet BD stabilizes and
remains constant for some time. The resulting pinning force, Fp, values were calculated as: Fp = γLV(cos θa –
cos θr), where the liquid–vapor surface tension
γLV can be found in Table , and θa and θr are the advancing and retreating CAs, respectively.
Coffee-Ring
Effect
Evaporation of
volatile species combined with pinning of the TPCL results in capillary
flow that transports non-volatile solutes to the contact line, giving
rise to a CRE. This flow arises from liquid evaporation at the droplet
edge that is replenished by liquid flow from the bulk to the edge.[37] A large CAH appearing as the outcome of droplet
pinning at the three-phase contact line can thus result in a CRE during
droplet evaporation.[38,46] In our particular case, this
could lead to the transport of carboxylic acids and species dissolved
from the calcite surface to the droplet edge. With increasing magnitude
of the capillary flow during droplet retraction, the deposition at
the contact line has been reported to become more ordered.[47] The mechanism of this type of CRE development
is represented schematically in Figure .
Figure 7
Schematic representation of the rearrangement of the C18 stearic acid monolayer on the calcite surface, forming a
patchy
array of multi-molecular thickness while being in contact with the
bulk water droplet, the formation of deposits at the droplet edge
due to the CRE during droplet evaporation, and the subsequent pinning
of the TPCL.
Schematic representation of the rearrangement of the C18 stearic acid monolayer on the calcite surface, forming a
patchy
array of multi-molecular thickness while being in contact with the
bulk water droplet, the formation of deposits at the droplet edge
due to the CRE during droplet evaporation, and the subsequent pinning
of the TPCL.For all cases illustrated in Figures –4, we note
specifically from adhesion and deformation images an accumulation
of material at the drop edges. This effect is apparently already for
pure water on calcite (Figure a), in which case the deposited material is most likely hydrated
calcium carbonate. Figure a,b shows two cases with C8-modified calcite, where
exposure to a pure water droplet leads to more accumulation than exposure
to a C8-saturated aqueous drop. Figure a shows the case with pure water on C18-modified calcite and the strongest material accumulation
at the droplet edge of all cases. In contrast, when the drop is saturated
with C8 acid (Figure b), there is hardly any noticeable effect at the drop
edge. A further observation is that results from CA and CAH measurements,
as shown in Figures and 6, can be closely related to topographical
and nanomechanical images. As one example, Table shows that CA values and CAH are lower for
the C8 drop on C18-modified calcite compared
to when pure water is used, which relates to less topographical and
nanomechanical effects, as seen in Figure b compared to Figure a.We suggest that these observations
are typical of the CRE[37,38] and that it represents a novel
case for its occurrence, namely,
one containing calcite and fatty acids exposed to a water droplet.
The major factor relevant for this type of CRE as a result of hydrophobization
is the pinning force estimated from surface tension and CAH.[38]Table shows that the pinning force can be estimated to decrease
ten-fold or more for the combinations using C8-saturated
water compared to pure water on C8- or C18-modified
calcite.We can clearly suppress the CRE by lowering the pinning
force and
thereby the capillary flow[37] by lowering
the liquid surface tension in combination with additional C8-adsorption that reduces the CAH. The AFM results support these suggestions
by demonstrating less material accumulation at the droplet edge, as
most apparently seen in the nanomechanical images. Although these
experiments are in a model-type situation, we suggest that the findings
are of technical importance during carboxylic fatty acid modification
of calcium carbonate for the purpose of increased homogeneity in the
fatty acid surface layers during deposition and storage of the final
product under humid conditions.
Conclusions
This work has elucidated the stability of bare and fatty carboxylic
acid-modified calcite surfaces in the presence of water droplets and
droplets of saturated aqueous octanoic acid solutions. AFM was used
to follow the structural changes in the unmodified and modified calcite
surfaces during short-term (30 s) exposure to the water and saturated
octanoic acid droplets. In all cases, more stable surfaces were found
in the presence of droplets of saturated aqueous solutions of octanoic
acid than that in the presence of pure water droplets. For the bare
calcite surface, this is due to adsorption of octanoic acid that retards
dissolution and recrystallization of calcite. Adsorption of octanoic
acid also occurs on the carboxylic acid-modified surface, and this
retards structural rearrangements in the initial monolayer of stearic
acid and octanoic acid on the modified calcite surfaces. It also reduces
the CAH, which results in smaller pinning force and reduced capillary
flow.The AFM data also allow us to distinguish events occurring
at the
three-phase surface–liquid–air interface at the water
droplet edge and events occurring below the droplet surface. Below
the water droplet, the initially hydrophobic stearic acid monolayer
is converted into a patchy array in order to reduce the solid–water
interfacial energy. We observe clear differences between calcite surfaces
modified with octanoic acid and stearic acid. These differences are
related to the much higher aqueous solubility of octanoic acid compared
to stearic acid. Thus, octanoic acid can dissolve in the bulk of the
water droplet, whereas this hardly occurs for stearic acid. However,
both types of carboxylic acids can move to the air–water interface,
and this results in the creation of a hydrophilic region close to
the droplet edge.The presence of the hydrophilic region at
the droplet edge gives
rise to significant CAH as the droplet edge becomes pinned, which
is the fundamental reason for capillary flow that results in the CRE.
The dynamic nature of the carboxylic acid-modified calcite surface
results in dramatically different wetting properties during droplet
evaporation compared to surfaces of intrinsic hydrophobic materials
such as polystyrene where only reorientation of surface groups occurs.To summarize, this work emphasized the importance of understanding
the properties of carboxylic acid layers adsorbed on calcite surfaces
with focus on their resistance during exposure to liquid solutions.
Such phenomena may arise during industrial processing of modified
calcite surfaces and are important to consider during material treatments,
storage, and in applications.
Authors: Natalia A Wojas; Agne Swerin; Viveca Wallqvist; Mikael Järn; Joachim Schoelkopf; Patrick A C Gane; Per M Claesson Journal: J Colloid Interface Sci Date: 2019-01-14 Impact factor: 8.128
Authors: Maria Ricci; Juan José Segura; Blake W Erickson; Georg Fantner; Francesco Stellacci; Kislon Voïtchovsky Journal: Langmuir Date: 2015-06-30 Impact factor: 3.882
Authors: Natalia A Wojas; Illia Dobryden; Viveca Wallqvist; Agne Swerin; Mikael Järn; Joachim Schoelkopf; Patrick A C Gane; Per M Claesson Journal: Langmuir Date: 2021-08-06 Impact factor: 3.882