Matteo Romio1,2, Benjamin Grob2, Lucca Trachsel3, Andrea Mattarei4, Giulia Morgese5, Shivaprakash N Ramakrishna6, Francesca Niccolai7, Elisa Guazzelli7, Cristina Paradisi8, Elisa Martinelli7, Nicholas D Spencer2, Edmondo M Benetti1,2,8. 1. Biointerfaces Lab, Swiss Federal Laboratories for Materials Science and Technology (Empa), Lerchenfeldstrasse 5, 9014 St. Gallen, Switzerland. 2. Laboratory for Surface Science and Technology, Department of Materials, ETH Zürich, Vladimir-Prelog-Weg 5, 8093 Zürich, Switzerland. 3. George & Josephine Butler Polymer Research Laboratory, Department of Chemistry, University of Florida, P.O. Box 117200, Gainesville, Florida 32611-7200, United States. 4. Department of Pharmaceutical and Pharmacological Sciences, University of Padova, Via Marzolo 5, 35131 Padova, Italy. 5. Institute of Materials and Process Engineering (IMPE), School of Engineering (SoE), Zürich University of Applied Sciences (ZHAW), Technikumstrasse 9, 8401 Winterthur, Switzerland. 6. Soft Materials and Interfaces, Department of Materials, ETH Zürich, Vladimir-Prelog-Weg 5, 8093 Zürich, Switzerland. 7. Department of Chemistry and Industrial Chemistry, University of Pisa, Via Moruzzi 13, 56124 Pisa, Italy. 8. Department of Chemical Sciences, University of Padova, Via Marzolo 1, 35122 Padova, Italy.
Abstract
Many synthetic polymers used to form polymer-brush films feature a main backbone with functional, oligomeric side chains. While the structure of such graft polymers mimics biomacromolecules to an extent, it lacks the monodispersity and structural purity present in nature. Here we demonstrate that side-chain heterogeneity within graft polymers significantly influences hydration and the occurrence of hydrophobic interactions in the subsequently formed brushes and consequently impacts fundamental interfacial properties. This is demonstrated for the case of poly(methacrylate)s (PMAs) presenting oligomeric side chains of different length (n) and dispersity. A precise tuning of brush structure was achieved by first synthesizing oligo(2-ethyl-2-oxazoline) methacrylates (OEOXMAs) by cationic ring-opening polymerization (CROP), subsequently purifying them into discrete macromonomers with distinct values of n by column chromatography, and finally obtaining poly[oligo(2-ethyl-2-oxazoline) methacrylate]s (POEOXMAs) by reversible addition-fragmentation chain-transfer (RAFT) polymerization. Assembly of POEOXMA on Au surfaces yielded graft polymer brushes with different side-chain dispersities and lengths, whose properties were thoroughly investigated by a combination of variable angle spectroscopic ellipsometry (VASE), quartz crystal microbalance with dissipation (QCMD), and atomic force microscopy (AFM) methods. Side-chain dispersity, or dispersity within brushes, leads to assemblies that are more hydrated, less adhesive, and more lubricious and biopassive compared to analogous films obtained from graft polymers characterized by a homogeneous structure.
Many synthetic polymers used to form polymer-brush films feature a main backbone with functional, oligomeric side chains. While the structure of such graft polymers mimics biomacromolecules to an extent, it lacks the monodispersity and structural purity present in nature. Here we demonstrate that side-chain heterogeneity within graft polymers significantly influences hydration and the occurrence of hydrophobic interactions in the subsequently formed brushes and consequently impacts fundamental interfacial properties. This is demonstrated for the case of poly(methacrylate)s (PMAs) presenting oligomeric side chains of different length (n) and dispersity. A precise tuning of brush structure was achieved by first synthesizing oligo(2-ethyl-2-oxazoline) methacrylates (OEOXMAs) by cationic ring-opening polymerization (CROP), subsequently purifying them into discrete macromonomers with distinct values of n by column chromatography, and finally obtaining poly[oligo(2-ethyl-2-oxazoline) methacrylate]s (POEOXMAs) by reversible addition-fragmentation chain-transfer (RAFT) polymerization. Assembly of POEOXMA on Au surfaces yielded graft polymer brushes with different side-chain dispersities and lengths, whose properties were thoroughly investigated by a combination of variable angle spectroscopic ellipsometry (VASE), quartz crystal microbalance with dissipation (QCMD), and atomic force microscopy (AFM) methods. Side-chain dispersity, or dispersity within brushes, leads to assemblies that are more hydrated, less adhesive, and more lubricious and biopassive compared to analogous films obtained from graft polymers characterized by a homogeneous structure.
Controlled
polymerization techniques, and especially reversible-deactivation
radical polymerizations (RDRPs), have progressively enabled the synthesis
of narrowly dispersed macromolecules under extremely accessible conditions.[1] Very recently, the fine-tuning of reaction conditions
during RDRP has additionally permitted the precise modulation of molecular
weight dispersity (Đ) over a relatively broad
range of values.[2,3]Besides this representing
a fundamental advance in the synthesis
of polymers, recent developments in the control over Đ are now revitalizing the interest of polymer and materials scientists,
who are trying to determine the impact that any heterogeneity in size
and/or molecular architecture of polymer components might have on
the physicochemical properties of derived materials.[4]Extensive work has been conducted in elucidating
the role that
dispersity plays in determining the morphology of nanostructured materials
obtained from self-assembly of block polymers, both in solution[5−7] and in bulk.[8−10] More recently, increased interest in the effects
that a variation of Đ could have on the properties
of oligomeric species has been developing because of the fundamental
studies by Hawker et al.[11−14] and Meijer et al.,[15−19] who have explored the morphological and structural
characteristics of a variety of self-assembled nanostructures derived
from block co-oligomers.Despite the evident blooming of research
in this particular field,
very little has been reported about the relationship between dispersity
and the properties of polymer interfaces, or polymer nanoassemblies
at solid surfaces.Focusing on polymer brushes, Matyjaszewski
and Bockstaller have
highlighted that when polymer brushes are grafted from silica nanoparticles
(NPs), their grafting density (σ) and Đ determine the morphology of the subsequently obtained hybrids. Narrowly
dispersed brushes enabled the formation of uniform films of NPs, while
broadly dispersed grafts generated anisotropic structures presenting
string-like NP aggregates.[20] These structural
differences were later demonstrated to affect the mechanical properties
of brush-particle-composite films.[21]Alternatively, while applying polymer brushes as biointerfaces,
Yadav et al. demonstrated that by increasing the molar mass and Đ of polyacid films on macroscopic surfaces, a fully
reversible attachment of bacteria could be achieved by switching pH
of the medium.[22]These initial studies
seem to suggest that in addition to polymer
composition, molar mass, and surface coverage, Đ could also represent an additional tuning parameter for modulating
the interfacial characteristics of polymer brushes.However,
these reports uniquely investigated a modulation in main-chain
dispersity and its effects on materials properties.
In contrast, a large variety of synthetic polymer brushes includes
a polymer backbone and functional, oligomeric (or polymeric) side
chains, with a design that is reminiscent of the structure of biopolymers,
such as proteoglycans,[23] which, it should
be noted, are intrinsically characterized by discrete, monodisperse structures[24] and provide distinctive
properties and functions to different tissues within our body.[25]Hence, dispersity of side chains (or side-chain heterogeneity) within polymer brushes emerges
as a possible tuning parameter for
an array of technologically relevant, interfacial physicochemical
properties and lies at the focus of the present study (Scheme ).
Scheme 1
While in previous work the
effect of main-chain dispersity of (co)polymers on the properties
of subsequently derived materials was investigated, side-chain dispersity
lies in the focus of the present study.
While in previous work the
effect of main-chain dispersity of (co)polymers on the properties
of subsequently derived materials was investigated, side-chain dispersity
lies in the focus of the present study.More
generally, the impact of variation in the degree of heterogeneity
of grafted polymer architectures on essential properties such as steric
stabilization of the substrate and amount of coupled solvent has yet
to be demonstrated. These parameters directly determine fundamental
characteristics of brush coatings, such as their resistance toward
nonspecific biological contamination,[26] their lubricious properties,[27,28] or colloidal stabilization,[29,30] when they are grafted from NPs.In this study, the effect
of side-chain dispersity of polymer brushes assembled
on flat substrates is specifically
investigated for the case of graft polymers constituted by poly(methacrylate)s
(PMAs) presenting oligomeric side chains. Here, these are based on
poly[oligo(2-ethyl-2-oxazoline) methacrylate]s (POEOXMAs),[31−36] which were synthesized by reversible addition–fragmentation
chain transfer (RAFT) polymerization of oligo(2-ethyl-2-oxazoline)
methacrylates (OEOXMAs), previously obtained by cationic ring-opening
polymerization (CROP) of 2-ethyl-2-oxazoline (EOX).Graft polymers
with similar structures, such as poly[oligo(ethylene
glycol) methacrylate] (POEGMA), are widely applied in materials science
for the functionalization of biomaterials,[37,38] the fabrication of biosensors[39] and thermoresponsive
coatings,[40,41] and in a broad range of other applications.[42−45] In addition, they are considered to be “standards”
for performing RDRPs in aqueous media.[46−50] However, despite their widespread use, POEGMAs usually
feature a distribution of OEG side-chain
lengths (n), which is typically centered at n ≈ 10,[42] although this
value might vary across different monomer batches and sources. In
other words, POEGMA brushes applied in some of the most common materials
formulations and coatings are characterized by an intrinsic dispersity
in their side-chain length, or a certain degree of heterogeneity in
their structure, with side chains that do not feature a well-defined n.In order to investigate how the side-chain length
and dispersity
in the brush structure influence their interfacial properties, we
concentrated on POEOXMA, as 2-oxazoline-based polymers represent some
of the most promising replacements for PEG and its derivatives in
biomaterials and biotechnology.[51−54] Precise tuning of graft polymer brush structure was
achieved by first synthesizing OEOXMAs, which are intrinsically polydisperse,
and subsequently purifying them into discrete macromonomers with distinct n by column chromatography.[11−13]Polydisperse OEOXMA
and monodisperse macromonomers with different n values
were subsequently polymerized by RAFT polymerization,
and the obtained POEOXMAs were finally derivatized with a disulfide-based
anchor, enabling their assembly on Au surfaces to yield brush nanofilms.The properties of chemically similar but structurally different
POEOXMA brushes were characterized by a variety of surface-analytical
methods. Assembly of brushes, their hydration, steric stabilization,
nanotribological and antifouling properties were investigated by a
combination of quartz crystal microbalance with dissipation (QCMD),
variable-angle spectroscopic ellipsometry (VASE), and atomic force
microscopy (AFM)-based methods.Results from these approaches
demonstrate how the presence of polydisperse
side chains leads to an increase in hydration, in comparison to graft
polymer brushes incorporating monodisperse oligomers within each monomer
unit. Enhanced hydration simultaneously leads to an improvement in
several relevant properties, including lubrication and biopassivity.
In contrast, the presence of side chains with a well-defined length
within brushes with a homogeneous structure favors the occurrence
of hydrophobic interactions, markedly degrading both lubricious properties
and resistance toward nonspecific protein contamination.Overall, side-chain dispersity within nanofilms
of graft polymer brushes emerges as a major factor in their propensity
to hydrate, in addition to well-known parameters, such as composition
and molar mass. Especially in the case of brushes presenting oligomeric
side chains, or graft polymer brushes, which are commonly applied
in myriad formulations, this parameter is revealed to have significant
impact on interfacial physicochemical properties.
Results and Discussion
Structurally different POEOXMAs were molecularly designed starting
from their monomeric constituents. OEOXMAs were initially synthesized
by CROP using methyl p-toluenesulfonate (MeOTs) as
initiator and methacrylic acid (MA) as terminator agents (Figure a). The resulting
OEOXMA featured an average n of 3.3, as measured by 1H nuclear magnetic resonance
(1H NMR) spectroscopy (Figure a). However, n was intrinsically
characterized by a rather broad distribution of values, as evidenced
by high-performance liquid chromatography (HPLC) (Figure b). Polydisperse OEOXMA (which is identified as OEOXPMA) could
be purified into monodisperse fractions presenting a well-defined n by flash column chromatography (Figure b and Methods). This
process gave access to OEOXMA presenting n = 3, 4, and 5 (OEOX3MA, OEOX4MA
and OEOX5MA, respectively), which are the most abundant
fractions present within OEOXPMA (Figure b–f).
Figure 1
CROP using MeOTs as initiator and MA as
terminator agent provided
unfractionated OEOXPMA (a), which could be subsequently
purified by flash column chromatography yielding monodisperse OEOXMA (b). OEOXMA, with n = 3, 4, and 5, and unfractionated OEOXPMA were subsequently polymerized by RAFT (c), using AIBN as
radical initiator and CDPA as chain-transfer agent, finally obtaining
POEOXMAs-COOH with different dispersity and length n of side chains (d). Coupling of ANPIS to POEOXMAs-COOH provided
graft polymer adsorbates that could be assembled (e) from ethanolic
solution onto Au substrates forming brushes (f).
Figure 2
(a) 1H NMR spectrum of polydisperse OEOXMA obtained
by CROP. (b) HPLC elugram of polydisperse OEOXMA highlighting the
different OEOXMA fractions. Liquid chromatography–mass
spectrometry (LC–MS) spectra of (c) polydisperse OEOXMA, (d)
OEOX3MA, (e) OEOX4MA, and (f) OEOX5MA.
CROP using MeOTs as initiator and MA as
terminator agent provided
unfractionated OEOXPMA (a), which could be subsequently
purified by flash column chromatography yielding monodisperse OEOXMA (b). OEOXMA, with n = 3, 4, and 5, and unfractionated OEOXPMA were subsequently polymerized by RAFT (c), using AIBN as
radical initiator and CDPA as chain-transfer agent, finally obtaining
POEOXMAs-COOH with different dispersity and length n of side chains (d). Coupling of ANPIS to POEOXMAs-COOH provided
graft polymer adsorbates that could be assembled (e) from ethanolic
solution onto Au substrates forming brushes (f).(a) 1H NMR spectrum of polydisperse OEOXMA obtained
by CROP. (b) HPLC elugram of polydisperse OEOXMA highlighting the
different OEOXMA fractions. Liquid chromatography–mass
spectrometry (LC–MS) spectra of (c) polydisperse OEOXMA, (d)
OEOX3MA, (e) OEOX4MA, and (f) OEOX5MA.Subsequent RAFT polymerization
of OEOXMAs provided POEOXMA species
with different degrees of heterogeneity and lengths of oligomeric
side chains (Figure c,d).As reported in Table , using 4-cyano-4-[(dodecylsulfanylthiocarbonyl)sulfanyl]pentanoic
acid (CDPA) as a RAFT agent and azobisisobutyronitrile (AIBN)
as a radical initiator, all the different OEOXMAs could be polymerized,
reaching conversions higher than 90% in 24 h and yielding carboxylic
acid-terminated POEOXMAs (POEOXMAs-COOH, Figure c) with Đ lying between
1.15 and 1.35 (Table ).
Table 1
Characterization of POEOXMA Adsorbates
and The Corresponding Brushes
polymer
Mn (SEC) [kDa]
Đ
Mn (NMR) [kDa]
Tdry (VASE) [nm]
Twet (QCM) [nm]
W [%]
σa [nm-2]
θS [deg]
θA [deg]
θR [deg]
POEOXPMA
10.8
1.21
22.8
3.0 ± 0.1
7.1 ± 0.1
58 ± 3
0.10 ± 0.01
39.6 ± 0.6
41.3 ± 0.5
23.3 ± 0.7
POEOX3MA
11.5
1.35
25.1
3.1 ± 0.1
6.2 ± 0.3
49 ± 8
0.09 ± 0.01
42.9 ± 2.1
44.0 ± 0.8
28.5 ± 1.7
POEOX4MA
15.6
1.32
24.9
3.2 ± 0.2
6.4 ± 0.1
51 ± 5
0.09 ± 0.01
44.8 ± 1.0
46.4 ± 1.1
25.5 ± 1.6
POEOX5MA
20.9
1.15
16.1
2.7 ± 0.1
5.7 ± 0.1
52 ± 4
0.11 ± 0.01
41.9 ± 2.2
44.3 ± 1.8
25.6 ± 1.7
Grafting density
(σ), expressed
as [chains nm–2], was calculated using the equation
σ = ρTdryNAMn–1 where
ρ is the density of the dry polymer layer (1.14 g cm–3), Tdry is the dry thickness measured
by VASE, NA is the Avogadro number, and Mn is the average molar mass of the adsorbate
measured by 1H NMR.
Grafting density
(σ), expressed
as [chains nm–2], was calculated using the equation
σ = ρTdryNAMn–1 where
ρ is the density of the dry polymer layer (1.14 g cm–3), Tdry is the dry thickness measured
by VASE, NA is the Avogadro number, and Mn is the average molar mass of the adsorbate
measured by 1H NMR.Subsequent conjugation of POEOXMAs-COOH with N-(4-(aminomethyl)benzyl)-5-(1,2-dithiolan-3-yl)pentanamide
(ANPIS) provided graft polymer adsorbates with a disulfide end group
(named as POEOXPMA-, POEOX3MA-, POEOX4MA-, and POEOX5MA-ANPIS) that could function as an anchor
for their subsequent assembly on Au surfaces (Figure e,f).Assembly of POEOXMAs-ANPIS on
Au and the formation of the corresponding
brushes were performed by incubation of freshly cleaned Au-coated
silicon substrates in 1 mg mL–1 ethanolic solutions
of the different polymer adsorbates, followed by extensive rinsing
with ethanol and ultrapure water.The properties of POEOXMA
brushes in the dry state were monitored
by ex situ VASE and in the swollen state by in situ QCMD.As
shown in Table , following
1 h of adsorption, the different POEOXMA-based adsorbates
formed brush layers with dry thicknesses (Tdry) ranging from 2.7 to 3.2 nm, as measured by VASE, corresponding
to grafting densities (σ) that are similar for the different
assemblies, lying in the range of 0.09–0.11 chains nm–2.Despite their very similar values of Tdry and σ, interestingly, different POEOXMAs-ANPIS generated
brushes
with diverse swelling properties, which could be evaluated by QCMD.It is particularly instructive to compare assembly and hydration
of brushes obtained via chemisorption of POEOX3MA-ANPIS
and POEOXPMA-ANPIS onto Au surfaces. These two graft polymer
adsorbates present very similar values of Mn and comparable, as obtained by size-exclusion chromatography (SEC)
and confirmed by 1H NMR (Table ), and thus they feature similar values of
both number average degree of polymerization and main-chain dispersity.
However, POEOX3MA-ANPIS and POEOXPMA-ANPIS are
characterized by side OEOX chains with markedly different length distributions.
POEOX3MA presents monodisperse, oligomeric side chains
with n = 3, whereas POEOXPMA is characterized
by broadly dispersed side chains with a maximum in the distribution
of n lying between 3 and 4, as inferred by HPLC and 1H NMR (Figure a,b). Hence POEOX3MA and POEOXPMA are illustrative
of two polymers presenting similar main-chain characteristics but
a dissimilar degree of structural heterogeneity because of a markedly
different dispersity of their side chains.Typical QCMD sensograms
reporting the variation in frequency (ΔF) for
three different overtones (f-3rd, f-5th, and f-7th)
while assembling POEOX3MA-ANPIS and POEOXPMA-ANPIS
on Au are reported in Figure a.
Figure 3
(a) QCMD sensograms reporting the variation of ΔF during the assembly of POEOX3MA and POEOXPMA brushes on Au-coated sensors. Three different overtones (f-3rd, f-5th, and f-7th) were reported for each sample. Point 1
corresponds to injection of polymer solutions. At point 2 the formed
brushes were rinsed by injecting pure ethanol, and at point 3 flushing
with ultrapure water was carried out. Fitting of the f-3rd, f-5th, and f-7th overtones by an extended viscoelastic model provided
the values of Twet for POEOX3MA and POEOXPMA brushes. (b, c) Illustrations highlighting
the less hydrated assembly of POEOX3MA grafts (b), in which
hydrophobic interactions between chains are taking place, and the
enhanced hydration of POEOXPMA brushes (c).
(a) QCMD sensograms reporting the variation of ΔF during the assembly of POEOX3MA and POEOXPMA brushes on Au-coated sensors. Three different overtones (f-3rd, f-5th, and f-7th) were reported for each sample. Point 1
corresponds to injection of polymer solutions. At point 2 the formed
brushes were rinsed by injecting pure ethanol, and at point 3 flushing
with ultrapure water was carried out. Fitting of the f-3rd, f-5th, and f-7th overtones by an extended viscoelastic model provided
the values of Twet for POEOX3MA and POEOXPMA brushes. (b, c) Illustrations highlighting
the less hydrated assembly of POEOX3MA grafts (b), in which
hydrophobic interactions between chains are taking place, and the
enhanced hydration of POEOXPMA brushes (c).In both cases, the polymers readily assembled on Au, showing
a
rapid chemisorption until a plateau was reached, a few minutes after
the injection of the polymer solutions.Although the two different
brushes presented similar values of Tdry, the assembly of POEOXPMA-ANPIS
on Au was mirrored by a larger ΔF, compared
to that recorded during the assembly of POEOX3MA-ANPIS.
A larger value of ΔF at similar Tdry necessarily implies a higher amount of coupled water.[55,56]The values of swollen thickness (Twet) could be obtained by fitting the ΔF and
dissipation data (ΔD) with an extended viscoelastic
model,[56,57] yielding Twet = 6.2 ± 0.5 and 7.1 ± 0.1 nm for POEOX3MA and
POEOXPMA brushes, respectively. These values were used
to estimate the water content (calculated as W %
= [(Twet – Tdry)/Twet] ×100 for each brush
type, which yielded ∼49% for POEOX3MA and ∼58%
for POEOXPMA brushes. Hence, polymer brushes presenting
polydisperse side chains showed higher hydration when compared to
chemically identical grafts of similar grafting densities, featuring
dicrete oligomers in their monomer units (Figure b,c).When comparing POEOXMA brushes
with monodisperse OEOX side chains of different lengths,
an increment in n from 3 to 5 was mirrored by a slight
but progressive increase in W % (Table ). However, even POEOX5MA brushes (featuring the
longest OEOX segments among the studied assemblies) showed a lower
swelling with respect to brushes presenting a high degree of heterogeneity
in their side-chain length, which averaged only 3.3.These results
suggested that the surface concentration of hydrophilic
units[58] is not the only parameter controlling
hydration of brushes and that side-chain dispersity appears to be
a major factor.The higher hydration tendency of POEOXPMA brushes was
further confirmed by static and dynamic contact angle (CA) measurements.As reported in Table , POEOXPMA brushes were characterized by the lowest value
of static contact angle (θS), which was 39 ±
0.6°. For monodisperse side chains, higher contact angles were
observed, with θS = 43 ± 2°, 45 ±
1°, and 42 ± 2° for POEOX3MA, POEOX4MA, and POEOX5MA brushes, respectively. Dynamic
wettability analysis confirmed the higher affinity of POEOXPMA brushes toward water. Advancing and receding contact angle (θA and θR, respectively) values recorded on
POEOXPMA brushes were 41 ± 1° and 23 ± 1°,
respectively. In contrast, θA values were included
between 44° and 46° for POEOXMA brushes with monodisperse
OEOX, whereas the corresponding θR were in all cases
≥26° (Table ).The different tendency to hydrate by POEOXMA adsorbates
featuring
diverse side chain-dispersity was further confirmed by analyzing their
thermoresponsive properties in water (Figure ).
Figure 4
(a) POEOXMA adsorbates form micellar dispersions
in aqueous media
due to the presence of hydrophobic ANPIS anchors. (b) Turbidity curves
recorded by UV/vis on 5 mg mL–1 dispersions of POEOXMA
in ultrapure water. (c) Dispersions of the different POEOXMA adsorbates
at ∼25 °C and after heating at ∼80 °C.
(a) POEOXMA adsorbates form micellar dispersions
in aqueous media
due to the presence of hydrophobic ANPIS anchors. (b) Turbidity curves
recorded by UV/vis on 5 mg mL–1 dispersions of POEOXMA
in ultrapure water. (c) Dispersions of the different POEOXMA adsorbates
at ∼25 °C and after heating at ∼80 °C.Due to the presence of hydrophobic ANPIS anchor
groups, all POEOXMA
adsorbates formed stable micellar dispersions in solution (Figure a). However, the
obtained dispersions were all characterized by a lower critical solution
temperature (LCST), in accordance to previous studies focusing on
compositionally similar OEOX-based graft polymers.[31] Relevantly, turbidity measurements performed by UV/vis
spectroscopy highlighted a significantly higher value of cloud point
temperature (CP) for POEOXPMA dispersions, which was centered
at ∼85 °C (Figure b,c). In contrast, analogous dispersions of POEOXMA adsorbates
with side chains of discrete length showed significantly lower values
of CP, which were 67°, 59°, and 55 °C, for POEOX5MA, POEOX4MA, and POEOX3MA, respectively.Hence, enhanced hydration by POEOXPMA adsorbates, which
was clearly significant in the case of micellar dispersions, translated
into an increment in water uptake by analogous surface-grafted assemblies
that was less remarkable. However, the differences in hydration that
could be visualized by QCMD/VASE, and the intrinsically different
structure of POEOXPMA brushes with respect to POEOXMA brush
analogues presenting monodisperse side segments translated into significant
variations in an array of technologically relevant interfacial properties
(vide infra).The increased hydration capability
by POEOXMA adsorbates with polydisperse
side chains could be generally explained by considering the effect
of intramolecular and intermolecular side-chain interactions (hydrophobic/van
der Waals) when amphiphilic grafts are confined to flat, macroscopic
surfaces within a densely grafted brush assembly (Figure b,c) (or when these form the
shell of a micellar structure, as displayed in Figure ).An increase in hydrophobic effects
within amphiphilic brushes as
a function of surface coverage was previously described by Schwartz et al. in the case of linear PEG grafts.[59] Generally, an increase in σ leads to two distinct
effects on the interfacial properties of PEG brushes. On the one hand,
an increment in surface density leads to an increase in steric stabilization
of the surface through osmotic and entropic effects.[26,60] On the other hand, an increase in grafted-chain crowding favors
the occurrence of hydrophobic interactions between nonionic, amphiphilic
segments.[59,61]POEOXMA brushes present amphiphilic
side chains at each monomer
unit and hydrophobic backbones based on PMA chains. Hence, hydrophobic
effects involving OEOX segments and PMA backbones are likely to arise
both intramolecularly, within the same graft, and intermolecularly, i.e., between neighboring POEOXMA chains. The extent of
such hydrophobic effects and how they interfere with the association
of water molecules within POEOXMA brushes must be correlated to the
length and dispersity of their side OEOX chains, as these two parameters
are expected to determine interactions within the polymer structure
(between neighboring side segments or involving side segments and
PMA backbone) and between neighboring surface-grafted chains.Besides wettability, the occurrence of hydrophobic interactions
influences several interfacial properties of polymer brushes, including
adhesion, lubrication, and resistance toward nonspecific contamination
by serum proteins.[52,62]In order to elucidate the
relationship among interfacial properties,
hydrophobic effects, and side-chain dispersity, we analyzed the different
POEOXMA brushes by colloidal probe microscopy (CPM) and lateral force
microscopy (LFM). During CPM and LFM, 20 μm diameter Au-coated
silica particles, which were previously functionalized with the same
POEOXMA brushes that were assembled on Au substrates, were used as
probes.For all POEOXMA brushes, force-vs-separation (FS) profiles
were
characterized by approach curves showing “snapping in”
at separations of ≤20 nm, due to net attractive forces between
opposing brush surfaces (Figure a). Simultaneously, retract curves were characterized
by adhesive interactions, which were generally due to van der Waals
forces taking place between POEOXMA brush surfaces compressed against
each other (Figure b).[52] However, adhesion was relatively
low in the cases of POEOXPMA and POEOX5MA brushes,
whereas significantly higher values were recorded for POEOX4MA and especially POEOX3MA (Figure c).
Figure 5
(a) Representative approach curves from FS profiles
recorded by
CPM on POEOXMA brushes and (b) the corresponding retract FS curves.
As depicted in the insets, in each experiment an AFM colloidal probe
bearing a POEOXMA brush identical to that deposited on the Au surface
was employed. (c) Measured pull-off force distributions recorded by
compressing the different POEOXMA brushes with identical brush countersurfaces.
(a) Representative approach curves from FS profiles
recorded by
CPM on POEOXMA brushes and (b) the corresponding retract FS curves.
As depicted in the insets, in each experiment an AFM colloidal probe
bearing a POEOXMA brush identical to that deposited on the Au surface
was employed. (c) Measured pull-off force distributions recorded by
compressing the different POEOXMA brushes with identical brush countersurfaces.Generally, adhesion between opposing POEOXMA brush
films was determined
by hydrophobic interactions and hydration. As previously mentioned,
hydrophobic interactions could occur both intramolecularly, between
neighboring OEOX side chains as well as involving PMA backbones, and
intermolecularly between side segments and main chains by polymers
that are grafted close to each other on the Au surface.In the
case of POEOX5MA brushes, the presence of longer,
OEOX side chains favored hydration and reduced the occurrence of hydrophobic
interactions between PMA backbones. In contrast, within POEOXPMA brushes side-chain dispersity appeared to be an additional,
major factor in determining adhesion, as the presence of polydisperse
side chains determined an increment in hydration and simultaneously
hindered hydrophobic interactions within brushes. As a result of the
combination of both these effects, POEOXPMA brushes showed
the lowest values of pull-off force among the studied samples.A similar trend was recorded while comparing the nanotribological
properties of POEOXMA brushes. These were analyzed by LFM, shearing
an Au-coated colloidal AFM probe functionalized with POEOXMA brushes
over an Au substrate presenting identical grafts (Figure a). As highlighted in the friction
force-vs-applied load profiles (FfL) reported in Figure b, POEOXPMA brushes demonstrated the most lubricious assemblies among the
studied brushes, with a coefficient of friction (μ) approximating
0.02. In contrast, POEOX3MA and POEOX4MA grafts
were characterized by significantly higher friction, with an order
of magnitude higher values of μ, which were 0.25 and 0.35, respectively,
while just a slight increase in lubrication was attained for POEOX5MA brushes, which showed μ = 0.17.
Figure 6
(a) LFM was performed
by shearing a POEOXMA brush-functionalized
colloidal AFM probe against an identical brush countersurface. (b)
FfL profiles recorded for the different POEOXMA brush tribopairs.
(c) Thickness of FHS recorded by VASE after 1 h of incubation of POEOXMA
brushes, where the bare Au surface was used as control. * and ** indicate
statistically significant differences between the set of data (*p < 0.01; **p < 0.05).
(a) LFM was performed
by shearing a POEOXMA brush-functionalized
colloidal AFM probe against an identical brush countersurface. (b)
FfL profiles recorded for the different POEOXMA brush tribopairs.
(c) Thickness of FHS recorded by VASE after 1 h of incubation of POEOXMA
brushes, where the bare Au surface was used as control. * and ** indicate
statistically significant differences between the set of data (*p < 0.01; **p < 0.05).Hence, CPM and LFM analyses showed that POEOXPMA brushes,
incorporating heterogeneous side chains, are more hydrated, less adhesive,
and significantly more lubricious with respect to analogous graft
polymer brushes comprising monodisperse OEOX segments. An increase
in side-chain length, as in the case of POEOX5MA brushes,
also led to a suppression of van der Waals interactions and a decrease
in friction. Nevertheless, side-chain dispersity appeared as a crucial
parameter in determining nanomechanical and nanotribological properties
of POEOXMA brushes.Enhanced hydration by graft polymer brushes
featuring polydisperse
side chains also influenced their resistance toward nonspecific protein
contamination. In particular, the different POEOXMA brushes were incubated
for 1 h in full human serum (FHS), and the amount of physisorbed proteins
was subsequently evaluated by VASE (Figure c).When comparing brushes incorporating
monodisperse OEOX side segments,
the lowest amount of adsorbed proteins was recorded on POEOX5MA brushes, which present the longest side OEOX chains. This result
agreed well with the typical biopassive behavior of PAOXA and PEG
brush surfaces, according to which a significant increase in surface
concentration of ethylene glycol (EG) or alkyloxazoline (AOX) units
was mirrored by a concomitant, relevant decrease in the mass of adsorbed
serum proteins.[58,63]The unexpected and somewhat
counterintuitive properties of POEOX4MA brushes are worth
pointing out, since this polymer showed
the highest thickness of physisorbed proteins and the highest values
of μ, compared to both POEOX3MA and POEOX5MA analogues. This results from the combination of two effects, side-chain/main-chain
and side-chain/side-chain hydrophobic interactions, only one of which
is dominant for POEOX3MA and POEOX5MA, respectively.
However, in the case of the intermediate-length POEOX4MA
both effects are apparently in operation.In good agreement
with the results from the adhesion and friction
tests, the best protein repellency was recorded in the case of POEOXPMA brushes, on which a protein layer with a thickness of just
∼0.2 nm was formed, nearly 4-fold thinner than that recorded
on POEOX3MA and 8-fold thinner than that formed on POEOX4MA.Hence, the capability to associate water molecules
and thus to
provide an energetic barrier against nonspecific interactions with
proteins depends not only on the surface density of biopassive units
within polymer brushes but also on their side-chain dispersity. This
parameter strongly influences the occurrence of hydrophobic interactions
between surface-grafted chains, especially in the case of bioinert
but amphiphilic brushes. In other words, side-chain dispersity of
brushes seems to be acting in a similar way to surface dilution[59] or brush mixing,[61] which were both previously demonstrated to enhance water uptake.
Conclusions
In this study, the impact of side-chain dispersity within graft polymer brushes on a set of interfacial properties
was investigated through a variety of surface analytics.Generally,
the presence of polydisperse OEOX side chains within
POEOXMA brushes prevents the occurrence of hydrophobic van der Waals
interactions and favors association with water molecules. This phenomenon
regulates interfacial physicochemical properties that are highly relevant
for technological applications and for the design of nanobiointerfaces,
including hydration of brushes, adhesion, lubrication, and biopassivity.More generally, dispersity within brushes appears
to be a major factor in determining their properties when swollen
in aqueous media, in addition to their composition, molar mass, and
surface coverage.This represents a fundamental result especially
in the case of
brushes comprising a PMA backbone and oligomeric side segments, which
are already broadly employed in materials science and nanotechnology
and feature a structure reminiscent of a large array of biomacromolecules.In contrast to their natural “analogues”, which are
intrinsically characterized by high purity and structural discreteness,
synthetic brushes are often polydisperse, and side-chain dispersity
emerges as one of the main tuning parameters for their properties.These findings open up previously unknown possibilities in the
design of polymer adsorbates for the functionalization of biomaterials,
whose main-chain and side-chain dispersities can nowadays be precisely
tailored by employing controlled-polymerization techniques.
Methods
Materials
2-Ethyl-2-oxazoline
(EOX, 99%, Sigma-Aldrich)
was distilled over KOH to remove traces of water. Methyl p-toluenesulfonate (MeOTs, 98%, Sigma-Aldrich) was purified by distillation
under reduced pressure over CaH2, and methacrylic acid
(MA, 99%, Sigma-Aldrich) was purified by filtration on a basic alumina
column before use. Triethylamine (TEA, ≥99.5% Sigma-Aldrich)
was purified by distillation over KOH. 4-Cyano-4-[(dodecylsulfanylthiocarbonyl)sulfanyl]pentanoic
acid (CDPA, 97%, Sigma-Aldrich) was used as received. Azobisisobutyronitrile
(AIBN, 98%, Sigma-Aldrich) was recrystallized from methanol. Toluene
was refluxed over CaH2 for 4 h under nitrogen atmosphere
and distilled. Sodium carbonate (NaHCO3, ≥99.5%),
magnesium sulfate (MgSO4, anhydrous, ≥99.5%), potassium
hydroxide (KOH, ≥98.5%), calcium hydride (CaH2,
95%), acetonitrile (ACN, 99.9+% dry with molecular sieves), methanol
(MeOH, >99.9% HPLC grade), and N,N-dimethylformamide (DMF, >99%) were purchased from Sigma-Aldrich
and used as received. (±)-α-Lipoic acid (>98%) was purchased
from Acros Organics.
Synthesis of OEOXPMA
To an oven-dried 100
mL Schlenk flask were added dry ACN (20 mL) and EOX (10 g, 101 mmol,
4 equiv) under nitrogen. Then MeOTs (4.7 g, 25 mmol, 1 equiv) was
added at 0 °C under nitrogen and stirred for another 15 min before
the polymerization mixture was heated to 70 °C and stirred for
15 h under argon. After this time, the polymerization was terminated
by adding a solution of MAA (4.3 g, 50 mmol, 2 equiv) and TEA (5.1
g, 50 mmol, 2 equiv) in dry ACN (10 mL) at room temperature and left
stirring for another 24 h under argon at 60 °C. MAA was previously
filtered through a basic alumina plug before use. The solvent was
removed under reduced pressure, and the residue was redissolved in
chloroform (250 mL). The organic solution was washed with a saturated
solution of NaHCO3 (2 × 200 mL) and finally with brine
(1 × 200 mL). The organic phase was dried over MgSO4, filtered, and the solvent was evaporated under reduced pressure
prior to addition of a point of spatula of hydroquinone in order to
prevent the possible self-polymerization. The residue was then dissolved
in water and freeze-dried in order to obtain a white and very hygroscopic
yellowish solid (11.5 g, 92% yield).The chemical structure
and the purity of the synthesized monomer were determined by 1H NMR (400 MHz) (Figure S1) by
LC–MS and HPLC (Figure ).
Purification of OEOXPMA into Discrete
OEOXMA
OEOXPMA was
dissolved in the
minimum amount of DCM. The obtained viscous solution was then purified
by flash silica gel column chromatography (proportion between sample
and SiO2 should lie between 1:70 to 1:100 w/w) using a
manually performed gradient of mobile phase from 100% DCM to 90%/10%
DCM/MeOH. Single-fraction detection was performed using SiO2-coated TLC sheets stained with KMnO4 solution. Each fraction
was isolated by solvent evaporation under reduced pressure, redissolution
in water, freeze-drying, and finally storage below −20 °C
prior to use. All fractions were finally characterized by 1H NMR (Figures S2–S4) and by LC–MS
(Figure ).
RAFT Polymerization
POEOXPMA and POEOXMAs with n = 3, 4, and 5
were synthesized by RAFT polymerization with 60:1:0.2 monomer:CDPA:AIBN
molar ratio in toluene solution (0.5 M monomer concentration). In
a typical procedure, OEOX3MA (0.328 g, 0.825 mmol), CDPA
(5.55 mg, 0.014 mmol), AIBN (0.45 mg, 0.0027 mmol), and anhydrous
toluene (1.65 mL) were loaded in a 10 mL Carius tube, and the mixture
was degassed with five freeze–pump–thaw cycles. The
polymerization was carried out under vacuum at 70 °C. After 24
h, the reaction was stopped by exposure to air, and the crude product
was precipitated into a large excess of n-hexane.
The final product POEOX3MA (conversion 95%) was characterized
by 1H NMR (1H NMR (CDCl3) 4.4–3.9
(CH2COO), 3.9–3.25 (CH2CH2N), 3.1–2.9 (CH3N), 2.7–2.25 (CH3CH2CO), 2.20–0.70 (CH3CH2CO, CH2CCH3)) and size exclusion chromatography
(SEC) (Figure S5).
Synthesis of N-(4-(Aminomethyl)benzyl)-5-(1,2-dithiolan-3-yl)pentanamide
(ANPIS)
(±)-α-Lipoic acid (2.00 g, 9.70 mmol,
1 equiv) was dissolved in 12 mL of anhydrous chloroform. 1,1-Carbonyldiimidazole
(2.00 g, 12.3 mmol, 1.3 equiv) was added to the lipoic acid solution
and stirred for 5 min at room temperature. The resultant solution
was added dropwise into a 1,4-benzenedimethanamine suspension (6.6
g, 48.5 mmol, 5 equiv) in dry chloroform (8 mL) and stirred for 40
min in an ice bath and for another 3 h at room temperature. The crude
product was washed three times with 20 mL of 10% NaCl aqueous solution
and once with 20 mL of water. It was dried with sodium sulfate and
the solvent removed using a rotary evaporator. The residue was purified
by flash silica gel chromatography using 80/20 CHCl3/MeOH
+ 1% TEA as mobile phase. The product (ANPIS) was obtained as a beige
solid (2.3 g, 7.3 mmol, 75% yield). 1H NMR (Figure S6, 400 MHz, DMSO-d6) δ = 8.34–8.24 (m, 1H), 7.34–7.10 (m,
4H), 4.22 (d, J = 5.9 Hz, 2H), 3.73 (s, 2H), 3.59
(dq, J = 8.6, 6.2 Hz, 1H), 3.25–3.04 (m, 2H),
2.40 (dq, J = 12.4, 6.1, 5.6 Hz, 1H), 2.13 (t, J = 7.3 Hz, 2H), 1.85 (dq, J = 13.4, 6.8
Hz, 1H), 1.76–1.58 (m, 1H), 1.54 (qd, J =
9.5, 8.0, 3.1 Hz, 3H), 1.45–1.21 (m, 2H) ppm. 13C NMR (100 MHz, DMSO-d6) δ = 171.85,
140.62, 138.03, 127.26, 127.03, 56.10, 44.70, 41.74, 38.08, 35.13,
34.09, 28.29, 25.04 ppm.
Synthesis of POEOXMA-ANPIS Conjugates
The synthesis
of POEOX3MA-ANPIS conjugate was exemplarily reported. POEOX3MA (227 mg, 0.02 mmol of free acid group), ANPIS (65 mg, 0.2
mmol, 10 equiv), and 1-[(1-(cyano-2-ethoxy-2-oxoethylideneaminooxy)dimethylaminomorpholino)]uronium
hexafluorophosphate (COMU) (85 mg, 0.2 mmol, 10 equiv) were dissolved
in 4 mL of DCM in a 10 mL Schlenk flask. The flask was purged with
a stream of nitrogen, and DIPEA (100 mL, 0.3 mmol, 30 equiv) was finally
added and the reaction mixture stirred at RT for 48 h under argon.
Then 7 mL of MeOH was added to the reaction mixture, and the flask
was washed with a further 8 mL of MeOH and finally purified by dialysis
(1 kDa MWCO) in MeOH for 48 h. The solvent was removed to yield POEOX3MA-ANPIS as a yellow, viscous polymer. The chemical structure
and the purity of POEOXPMA-, POEOX3MA-, POEOX4MA-, and POEOX5MA-ANPIS were determined by 1H NMR (400 MHz) (Figures S7–S10).
Surface Assembly of POEOXMA-ANPIS Adsorbates on Au
Silicon wafers coated with a 100 nm thick Au layer were prepared
by reactive magnetron sputtering (Paul Scherrer Institute, Villigen,
Switzerland). The substrates (10 × 20 mm2) were cleaned
for 1 min in piranha solution (3:1 mixture of concentrated H2SO4 and H2O2) and later were extensively
washed with ultrapure water and absolute ethanol. Surface assembly
of POEOXMA-ANPIS adsorbates was performed by immersing the Au-coated
substrates for 2 h in 1 mg mL–1 methanolic solutions
at room temperature (RT). The functionalized samples were subsequently
rinsed with ultrapure water and absolute ethanol to remove physisorbed
species and finally dried under a stream of N2.
NMR Spectroscopy
1H and 13C NMR
spectra were recorded on a Bruker Avance III HD 400 MHz spectrometer
at room temperature using D2O, CDCl3, or DMSO-d6 as solvents.
Size Exclusion Chromatography
(SEC)
SEC was performed
by using a Viscotek gel permeation chromatography (GPC) system (Malvern,
Worcs, U.K.) equipped with a pump and degasser (GPCmax VE2001, 1.0
mL min–1 flow rate), a detector module (Viscotek
302 TDA), and three columns (2× PLGel Mix-C and 1× ViscoGEL
GMHHRN 18055, dimensions 7.5 mm × 300 mm for each column) using
THF as eluent. Each sample was prepared dissolving the polymer at
a defined concentration of 1 mg mL–1 in THF containing
0.3% of toluene.
Contact Angle (CA) Measurements
Surface wettability
was determined by static and dynamic CA (DSA 100, Krüss, Hamburg,
Germany) in an automated procedure.Static CA measurements were
performed using the sessile drop technique. A sessile drop was deposited
onto the brush-functionalized Au surfaces with the aid of an automated
syringe, and the drop contour was fit by the Young–Laplace
method. Twenty measurements were recorded for each type of sample.In order to record the values of θA and θR, the volume of ultrapure water drops dispensed on the brush-functionalized
substrates was progressively increased and decreased from 4 to 10
μL at a speed of 15 μL min–1. Three
different locations were measured on each sample.
Variable-Angle
Spectroscopic Ellipsometry (VASE)
Ex
situ VASE measurements were carried by using a variable-angle spectroscopic
ellipsometer (M-2000F, Woollam Co., Inc., Lincoln, NE, USA) to determine
the values of Tdry of the polymer brushes
assembled on Au. The measurements were performed in the spectral range
of 290–900 nm using focusing lenses at three different angles
of incidence (60°, 65°, and 70°) from the surface normal.
Each data point resulted from the average of 20 measurements, and
the obtained raw ellipsometric data were fitted with a bilayer model
(Au and organic adlayer) using the analysis software WVASE32. The
thickness of Au layer (100 nm) was assumed to be constant. The n and k values for Au were fitted by measuring
a freshly cleaned Au substrate (without brushes), and the organic
adlayer (polymer brush) was fitted using the Cauchy model (A = 1.45 and B =
0.01, C = 0). A homogeneous mass distribution
of the organic adlayer perpendicular to the Au surface was assumed
with a density of 1.14 g cm–3 for the polymer brush.[64]
Quartz Crystal Microbalance with Dissipation
(QCMD)
QCMD experiments were performed at ambient temperature,
using a Q-Sense
E4 (Q-Sense AB, Göteborg, Sweden) equipped with dedicated Q-Sense
AB software. Au-coated crystals (LOT-Oriel AG) with a fundamental
resonance frequency of 5 MHz were used as substrates. Before the experiment,
the substrates were sonicated twice in toluene and twice in isopropanol
and finally subjected to UV–ozone (UV Clean model 135500 from
Boekel Industries, Inc.) for 30 min. Au-coated crystals were first
exposed to ultrapure water until a stable baseline was recorded (Figure S11). Water was subsequently replaced
with methanol until a new baseline was reached. A 1 mg mL–1 ethanolic solution of POEOXMA-ANPIS was then injected until complete
formation of POEOXMA brushes was accomplished. Removal of physisorbed
polymer adsorbates was performed by rinsing with ethanol and finally
with ultrapure water. The values of Twet of POEOXMA brushes were obtained by applying an extended viscoelastic
model (Qtools 3 software), fitting the frequency (ΔF) and dissipation shifts (ΔD) recorded after
the formation of POEOXMA brush layers and their swelling in ultrapure
water, using four different overtones (3rd, 5th, 7th, and 9th) for each sample (see Supporting Information). Two crystals for each
film were used to calculate the mean values of Twet and standard deviations. Fixed parameters for the fitting
were fluid density (997 kg m–3), layer density (1100
kg m–3), and fluid viscosity (0.009 kg m–1 s–1). The parameters that were fitted (while being
constrained to physically meaningful boundaries) were the layer’s
viscosity (0.009–0.05 kg m–1 s–1), shear modulus (104–108 Pa), Twet (10–9–10–8 m), and hydrated mass.All QCMD experiments were conducted
at ambient temperature, which oscillated between 20 and 22 °C.
UV/Visible Spectroscopy
Thermoresponsive behavior of
POEOXMAs in solution was analyzed by performing turbidity measurements
using a Shimadzu (Kyoto, Japan) 2450 UV/vis spectrometer equipped
with a S-1700 thermoelectric single cell holder. 5 mg mL–1 aqueous solution of the POEOXMAs was analyzed in quartz cuvettes
with a 10 mm optical path. Transmittance was measured at a fixed wavelength
of 700 nm. Turbidity measurement were carried out in the temperature
range 25–95 °C. Cloud point temperatures (Tcp) were assigned at temperatures that showed a 50% decrease
in transmittance with respect to the value recorded at 25 °C.
Atomic Force Microscopy (AFM)
Lateral and normal force
measurements were performed by using MFP3D AFM (Asylum Research, Oxford
Instruments, Santa Barbara, USA) under 1 mM (4-(2-hydroxyethyl)-1-piperazineethanesulfonic
acid) (HEPES) buffer solution at pH = 7.4. Colloidal AFM probes were
prepared by attaching a ∼20 μm diameter silica bead (EKA
Chemicals AB, Kromasil R, Sweden) onto tipless cantilevers (CSC38-C/tipless/Cr-Au,
Mikromasch, Bulgaria). Colloidal AFM probes were subsequently covered
by a 3 nm thick W layer, followed by a 20 nm thick layer of Au by
a metal evaporator (MED020 coating system, BAL-TEC, Balzers, Lichtenstein).
POEOXMA brushes with different side-chain dispersity and length were
later grafted to the colloidal probes following the same procedures
applied for the flat Au-coated substrates. Four different cantilevers
having nearly identical normal and lateral spring constant values
were selected for preparing colloidal probes with four different side-chain
dispersity.The normal (KN) and
torsional (KT) spring constant values
for all the cantilevers were obtained by thermal noise[65] and Sader’s method[66] prior to the attachment of the colloids. The obtained KN and KT values
for four different cantilevers were reported in Table S3.In all the AFM measurements, the diameter
of the Au-coated, silica
colloidal probe was ∼20 μm. Friction measurements were
performed by obtaining 5–6 “friction loops” along
the same line for each applied load over 3 different positions on
each sample (scan rate of 0.5 Hz, sliding distance of 5 μm),
from which the average friction forces and the standard deviations
were calculated. The friction force calibration was carried out by
using the method following Cannara et al.[67] Each set of FS curves was obtained over 3 different positions for
each sample. A scanning distance of 1 μm and a scanning rate
of 0.5 Hz were used.All AFM experiments were conducted at ambient
temperature, which
oscillated between 20 and 22 °C.
Authors: Daniel Y Joh; Angus M Hucknall; Qingshan Wei; Kelly A Mason; Margaret L Lund; Cassio M Fontes; Ryan T Hill; Rebecca Blair; Zackary Zimmers; Rohan K Achar; Derek Tseng; Raluca Gordan; Michael Freemark; Aydogan Ozcan; Ashutosh Chilkoti Journal: Proc Natl Acad Sci U S A Date: 2017-08-07 Impact factor: 11.205
Authors: Jimmy Lawrence; Sang-Ho Lee; Allison Abdilla; Mitchell D Nothling; Jing M Ren; Abigail S Knight; Carolin Fleischmann; Youli Li; Austin S Abrams; Bernhard V K J Schmidt; Michael C Hawker; Luke A Connal; Alaina J McGrath; Paul G Clark; Will R Gutekunst; Craig J Hawker Journal: J Am Chem Soc Date: 2016-05-06 Impact factor: 15.419
Authors: Jacob T Heggestad; Cassio M Fontes; Daniel Y Joh; Angus M Hucknall; Ashutosh Chilkoti Journal: Adv Mater Date: 2019-11-29 Impact factor: 30.849
Authors: Anindita Das; Katja Petkau-Milroy; Gilian Klerks; Bas van Genabeek; René P M Lafleur; Anja R A Palmans; E W Meijer Journal: ACS Macro Lett Date: 2018-04-16 Impact factor: 6.903
Authors: Bas van Genabeek; Brigitte A G Lamers; Bas F M de Waal; Martin H C van Son; Anja R A Palmans; E W Meijer Journal: J Am Chem Soc Date: 2017-10-17 Impact factor: 15.419