A combined surface treatment (i.e., surface grafting and a layer-by-layer (LbL) approach) is presented to create advanced biomaterials, i.e., 3D poly(l-lactide) (PLLA) microsphere scaffolds, at room temperature. The grafted surface plays a crucial role in assembling polyelectrolyte multilayers (PEMs) onto the surface of the microspheres, thus improving the physicochemical properties of the 3D microsphere scaffolds. The grafted surface of the PLLA microspheres demonstrates much better PEM adsorption, improved surface coverage at low pH, and smoother surfaces at high pH compared with those of nongrafted surfaces of PLLA microspheres during the assembly of PEMs. They induce more swelling than nongrafted surfaces after the assembly of the PEMs and exhibit blue emission after functionalization of the microsphere surface with a fluorescent dye molecule. The 3D scaffolds functionalized with and without nanosheets not only exhibit good mechanical performance similar to the compressive modulus of cancellous bone but also exhibit the porosity required for cancellous bone regeneration. The magnetic nanoparticle-functionalized 3D scaffolds result in an electrical conductivity in the high range of semiconducting materials (i.e., 1-250 S cm-1). Thus, these 3D microsphere scaffolds fabricated by surface grafting and the LbL approach are promising candidates for bone tissue engineering.
A combined surface treatment (i.e., surface grafting and a layer-by-layer (LbL) approach) is presented to create advanced biomaterials, i.e., 3D poly(l-lactide) (PLLA) microsphere scaffolds, at room temperature. The grafted surface plays a crucial role in assembling polyelectrolyte multilayers (PEMs) onto the surface of the microspheres, thus improving the physicochemical properties of the 3D microsphere scaffolds. The grafted surface of the PLLA microspheres demonstrates much better PEM adsorption, improved surface coverage at low pH, and smoother surfaces at high pH compared with those of nongrafted surfaces of PLLA microspheres during the assembly of PEMs. They induce more swelling than nongrafted surfaces after the assembly of the PEMs and exhibit blue emission after functionalization of the microsphere surface with a fluorescent dye molecule. The 3D scaffolds functionalized with and without nanosheets not only exhibit good mechanical performance similar to the compressive modulus of cancellous bone but also exhibit the porosity required for cancellous bone regeneration. The magnetic nanoparticle-functionalized 3D scaffolds result in an electrical conductivity in the high range of semiconducting materials (i.e., 1-250 S cm-1). Thus, these 3D microsphere scaffolds fabricated by surface grafting and the LbL approach are promising candidates for bone tissue engineering.
Polymer particles have
attracted much attention in many fields
(e.g., the chemical industry, biotechnology, pharmacology, and the
medical field). Their physicochemical properties, such as their electrical,
optical, and chemical properties, can be adjusted via alterations
in their composition, size, and structure.[1−4] The surface chemistry and morphology
of the particles play a critical role in their assembly, and the morphology
influences their physical interactions when they are utilized as new
types of material building blocks for self-assembly.[5,6] Alterations in surface morphology can be achieved via surface modification
to produce the desired properties, thereby controlling the subsequent
surface interactions and responses needed for any particular application.[7] Surface grafting via UV light, which is commonly
called photografting, is one of the surface modification techniques
that can be used to modify polymer surfaces.[8−10] It is a mild
reaction that selectively influences the sample surface,[9] and it is nondestructive.[11] The modified structure of particle surfaces offers a new
opportunity for tailoring biomaterials to improve the cellular functions
and interactions for tissue engineering for applications such as bone
tissue regeneration.[5,6,12]The three-dimensional (3D) scaffolds derived from polymeric materials
for human cancellous or trabecular bone require suitable mechanical
properties with a compressive modulus in the range of 10–2000
MPa,[13] and they require the appropriate
microstructure to perform their bone functions in vivo.[14] Additives are also sometimes required for improved
bone efficacy during bone tissue regeneration. However, the functionalization
of 3D scaffolds may reduce the mechanical performance required for
bone tissue regeneration.[15,16] The 3D bone scaffolds
can be made via a variety of techniques, such as solvent casting and
salt leaching,[17,18] chemical foaming,[19] foam gel,[20] freeze-drying,[21] 3D printing,[22,23] and 3D scaffolds
based on sintered microparticles.[14,24] Microsphere-based
3D scaffolds with a porous interconnected network were initially fabricated
using a sintering technique for bone tissue engineering. This approach
requires a temperature in the range of 70–120 °C or even
higher. The use of a high temperature during fabrication of the material
can lead to undesired side effects because several polymers are thermally
sensitive and the treatment causes detrimental effects on the surface
morphology. The compressive modulus of functional macromolecule-incorporated
and sintered microspheres has successfully been improved. However,
high molecular weight polymers are required to create strong 3D scaffolds
to enable the regeneration of cancellous bone, and only a single functional
species can be added.[14] The fabrication
of 3D microsphere scaffolds via a combined simple technique, the simultaneous
enhancement of the mechanical performance, and the inclusion of functional
additives to the 3D scaffolds remain challenging.The layer-by-layer
(LbL) technique is a simple, green, and highly
versatile process that is based on the alternating deposition of oppositely
charged polyelectrolytes.[25−27] The technique has been applied
in the field of biomedical applications.[28−30] This assembly
is fundamentally driven by not only electrostatic interactions[25,26] but also covalent,[31,32] hydrophobic,[33,34] and hydrogen-bonding interactions.[33,35] Microspheres
have been used as a template for assembling multilayer thin films
via a LbL approach, and the concept itself is an extension to produce
3D structures ranging from nano to micrometer scales.[36−38]Graphene oxide (GO) nanosheets have recently been exploited
to
enhance the mechanical performance of tissue engineering scaffolds[39,40] due to the high Young’s modulus of GO.[41] GO nanosheets have also been shown to accelerate the differentiation
mechanism of bone marrow-derived mesenchymal stem cells and myoblast
C2C12 cells.[42,43] The same increase in cell differentiation
has been demonstrated for Fe3O4 nanoparticles.[44,45] However, less attention has been given to a new basis that uses
grafted surfaces as a base layer onto which polyelectrolyte multilayers
(PEMs) can be physically adsorbed, and this combined surface treatment
can later be used to produce advanced 3D microsphere scaffolds at
room temperature. This constitutes an excellent surface treatment
combination to provide materials for 3D scaffolds for, e.g., cancellous
bone regeneration.Our main objective is here to stress the
importance of a grafted
surface as a base layer for the assembly of PEMs on polylactide (PLA)
microsphere surfaces and to introduce a straightforward method that
involves surface grafting and a LbL approach for fabricating advanced
3D scaffolding materials. Aiming for bone tissue regeneration, mechanical
properties of the scaffold should mimic the E-moduli of cancellous
bone. As model systems, nanosized particles can also be incorporated
into the 3D scaffolds to induce conductivity or to increase the mechanical
strength of the materials. The incorporation of functional additives,
i.e., nanomaterials, will create a so-called sandwich scaffold, thereby
altering the physicochemical properties of the 3D material. In addition,
any other additives can potentially be sandwiched, driven by entropic
gain, between polyelectrolyte layers in order to provide high-value
materials for certain applications. We hypothesize that surface grafting
onto microsphere surfaces improves the physicochemical properties
of the 3D microsphere scaffolds by ensuring strong interactions between
the particle and the formed PEMs. To achieve our aim, different types
of weak polyelectrolytes and neutral polymers, i.e., poly(acrylic
acid) (PAA), poly(allylamine hydrochloride) (PAH), and poly(acrylamide)
(PAAm), were utilized. Functional nanoadditives were used to increase
the scaffold conductivity or strength by alternative assembly on the
microsphere surfaces between the PEMs. This strategy should be applicable
to different polymers and could create highly functional materials
with tailored physicochemical properties for a wide range of applications.
Experimental Section
Materials
Poly(l-lactide) (PLLA) (Mn = 50 000
g mol–1; Đ = 1.32) was synthesized
via ring-opening polymerization
of l-lactide (LLA, Boehringer Ingelheim, Germany) at 110
°C for 72 h in bulk using ethylene glycol (Sigma-Aldrich, Germany)
as the initiator and stannous octoate (Sn(Oct)2) (Sigma-Aldrich,
Sweden) as the catalyst. The formed polymer was precipitated three
consecutive times in cold hexane (LabScan, Ireland)/methanol (general
purpose grade, Fisher Scientific, Germany) and used to fabricate the
microspheres. Benzophenone (99%, Sigma-Aldrich), ethanol (96%, VWR,
Sweden), sodium hydroxide (99%, Merck), hydrogen chloride (HCl) (2
M, Fisher Scientific), chloroform (>99%, Fisher Scientific), GO
(4–10%
edge oxidized, Sigma-Aldrich), 4′,6-diamidino-2-phenylindole
(DAPI) (Mw = 457.5; Life Technologies,
UK), hexadecylamine (90%, technical grade, Aldrich, Germany), FeCO5 (>99.9%, trace metal basis, Aldrich, Germany), oleic acid
(90%, technical grade, Aldrich, Germany), n-octanol
(≥99%, ACS reagent, Sigma-Aldrich), and sodium periodate (≥99.8%,
ACS reagent, Sigma-Aldrich) were used as received. Acrylic acid (AA)
(90%, Alfa Aesar) was purified by vacuum distillation at a temperature
of 40–50 °C prior to use. The three different weak polyelectrolytes,
PAA (99%, Sigma-Aldrich), PAH (99%, Alfa Aesar), and PAAm (99%, Polysciences),
were used as received.
Microsphere Fabrication
The PLLA
microspheres were
fabricated using a spray dryer (Mini Spray Dryer BUCHI B-290, Flawill,
Switzerland). Approximately 1 g of PLLA was dissolved in 100 mL of
chloroform. The following system parameters were used: an inlet temperature
(Tinlet) of 55–65 °C, an aspirator
at 100% (35 m3 min–1), a pump feed rate
of 20%, and a gas flow of 50 mm (750 NL h–1). The
PLLA microspheres were recovered from a collection vessel located
underneath the spray dryer cyclone. They were then surface-grafted
with 20% (v/v) AA under UV exposure, as previously described.[11] The PAA-grafted PLLA microspheres were subsequently
used as the main substrates to build-up PEMs.
Hydrophilic Fe3O4 Nanoparticle Synthesis
Magnetic Fe3O4 nanoparticles were synthesized
using a method similar to that described by Si.[46] Briefly, 3 mL of oleic acid and 0.22 g of hexadecylamine
were dissolved in 8.0 mL of n-octanol via stirring
and ultrasonication. Afterward, 2 mL of Fe(CO)5 was added
to the solution, and the blend was mixed for 5 min via stirring. The
mixture was then transferred into a 50 mL Teflon container and heated
at 200 °C for 12 h in an autoclave. The magnetic nanoparticles
were collected using a magnet after the autoclave reached room temperature.
The Fe3O4 nanoparticles were rinsed with ethanol
and distilled water three consecutive times, and they were dried under
vacuum overnight. To introduce hydrophilic groups onto the surface
of the nanoparticles, 100 mg of the synthesized magnetic nanoparticles,
which were dispersed in 15 mL of cyclohexane and 15 mL of 27 mg/mL
sodium periodate aqueous solution, was added into a 20 mL mixture
of ethyl acetate and acetonitrile with a volume ratio of 1:1 and stirred
vigorously for 2 h. After the reaction, the nanoparticles were again
collected using a magnet and rinsed with ethanol and distilled water
several times. Then, the magnetic nanoparticles were redispersed in
water.
LbL Formation
The PEMs were formed similar to those
that are alternately assembled on a film substrate, as described elsewhere.[47] This technique involves hydrogen-bonding interactions
between an anionic (PAA) and a neutral polymer (PAAm) polyelectrolyte
at pH 2.5 (abbreviated PAA/PAAm) or electrostatic interactions between
an anionic (PAA) and a cationic polymeric (PAH) polyelectrolyte at
pH 2.5 and 5 (abbreviated as PAA/PAH). Both systems were alternately
deposited onto PAA-grafted PLLA microspheres. Briefly, immersion into
a 0.3 M polyelectrolyte solution (based on the repeating unit of molecular
weight) in 18.2 MΩ cm Millipore water was performed for approximately
15 min under mechanical stirring, followed by centrifugation at 4000
rpm for 3 min. Water was added to physically remove the unabsorbed
polyelectrolyte in the solution between each deposition step. The
water volume was two times that of the polyelectrolyte solutions.The rinsing step was carried under vigorous stirring and was subsequently
followed by centrifugation. Thus, a deposition/centrifugation/rinse/centrifugation
cycle was performed to obtain the PEMs and to remove free polyelectrolytes
from the solution. The pH of the rinsing water was adjusted to be
the same as the polyelectrolyte solution, i.e., pH 2.5 and 5. The
pH of the PAH and PAA dipping solutions was experimentally adjusted
to 2.5 and 5, respectively, whereas a pH of only 2.5 was used to create
the PAA and PAAm multilayers. To the system with the outermost layer
of PAAm or PAH at pH 2.5 was deposited 0.002 wt % of a functional
additive as a model nanomaterial (i.e., GO or Fe3O4) onto the microsphere surfaces. The nanomaterial, i.e., GO
or Fe3O4, acted as a third component after sequential
adsorption of polyanions and polycations/neutral polymers onto grafted
surfaces, meaning that the sequential adsorption of these nanomaterials
was carried out an equal number of times as the number of formed bilayers
following the desired layer of polyanions and polycations/neutral
polymers. Nongrafted PLLA microspheres were also prepared using the
same procedure to build-up PEMs as reference (Table ).
Table 1
Surface-Grafted Microspheres
Used
during the Assembly of PEMs and Their Nongrafted Microspheres
microspheres
type of multilayer
build-up
pH
name
nongrafted
PLLA
PAA/PAAm
2.5
PAMn
PAA/PAH
2.5
PAH2.5n
PAA/PAH
5
PAH5n
PAA-grafted PLLA
PAA/PAAm
2.5
PAMg
PAA/PAH
2.5
PAH2.5g
PAA/PAH
5
PAH5g
PAA/PAAm/GO
2.5
PAMgGO
PAA/PAH/GO
2.5
PAHgGO
PAA/PAAm/Fe3O4
2.5
PAMgFeO
PAA/PAH/Fe3O4
2.5
PAHgFeO
3D Scaffold Fabrication
After rinsing
with water, the
PEM-coated PLLA microspheres whose outermost layers consisted of carboxylates
were mixed with amide layers that contained microspheres in one batch.
Later, they were rinsed with water and centrifuged. This procedure
was similarly performed for the electrostatic-driven interaction with
the PAA and PAH outermost layers. They were packed into a cylindrical
cutoff plastic syringe with a diameter of 8–10 mm and a height
of 4–8 mm (Figure ). The 3D microsphere scaffolds were subsequently dried for
1 week prior to characterization.
Figure 2
Schematic illustration of the surface grafting and build up of
PEMs onto the grafted surface of PLLA microspheres.
Characterization
Size Exclusion
Chromatography (SEC)
The molar mass
of the PLLA microspheres was determined using a Waters 717 plus autosampler
and a Waters model 510 apparatus equipped with two PL gel 10 μm
mixed B columns (300 × 7.5 mm; Polymer Laboratories, UK). The
instrument was calibrated using narrow molar mass distribution polystyrene
standards with molar masses in the range 580–400 000
g mol–1.
Fourier Transform Infrared Spectroscopy (FTIR)
The formation of PEMs
that were
attached to the PLLA-based microspheres was characterized using FTIR.
Spectra were recorded in the range 4000–600 cm–1 on a Spectrum 2000 PerkinElmer spectrometer using an attenuated
total reflectance (ATR) accessory (Golden Gate).
X-ray Diffraction
(XRD)
The crystalline structure of
the GO-functionalized materials and their respective references was
evaluated using XRD on a PANalytical XPert Pro instrument with Cu
Kα radiation at a wavelength (λ) of 1.54 Å and a
voltage and electric current of 45 kV and 45 mA, respectively. The
diffractograms were recorded at 25 °C using a silicon monocrystal
sample holder at a step size angle of 0.017°. The intensity of
the diffractogram was measured as a function of 2θ ranging between
5 and 60°.
Scanning Electron Microscopy (SEM)
The surface morphology
of the microsphere-based samples was determined using a Hitachi S-4800
scanning electron microscope at an acceleration of 1 kV. The samples
were mounted on adhesive carbon black and were sputter-coated.
Compression
Test
The mechanical testing was conducted
on an Instron 5566 instrument (Instron, UK) with a load cell of 10
kN and a compressive rate of 10% thickness min–1. The 3D microsphere scaffolds had a height between 5 and 8 mm and
a diameter between 8 and 10 mm.
Particle Size Distribution
(PSD)
A predetermined amount
of microspheres (approximately 600 mg) was prepared. The PSDs of neat
PLLA, PLLA-g-PAA microspheres, and PEM-coated microspheres
were determined at a distance of 10 mm from the spray outlet via a
laser diffraction spectrometer with a He–Ne laser at a wavelength
of 632.8 nm as the laser source (model HELOS/KR-H3522, Sympatec GmbH,
Clausthal-Zellerfeld, Germany), according to ISO 13320:2009. The microspheres
were previously dispersed using a RODOS dispersing unit at a reduced
pressure of 2 bar. The HELOS was operated with a focal distance of
fR3 = 100 mm to span a distance between 0.5 and 175 μm.
The measurement was performed for 1.5 s for each sample. The PSD was
then evaluated using the Fraunhofer diffraction model.
Porosity
Measurement
The porosity of the scaffolds
was measured using a μCT device (SkyScan 1172 Scanner, Belgium)
at 40 keV with a 2.4 μm voxel. Samples were randomly selected
and characterized via CTan (CT analyzer, ver. 1.5.0, SkyScan) and
CTvol (CT Vol Realistic, ver. 1.9.4, SkyScan) software. Three-dimensional
models were later reconstructed using NRecon (ver.1.6.9, SkyScan)
and CTan (v.1.14.4, SkyScan) software.
Electrical Conductivity
Measurement
The 3D scaffolds
were doped with 1 mol L–1 HCl for 24 h. Nondoped
3D scaffolds were also prepared as a reference. After Cl– doping, the scaffolds were dried in a vacuum oven for 48 h. Thus,
the conductivity was not influenced by the water content. Microsphere
pellets with diameters of 0.6–0.9 cm and thicknesses of 0.3–0.4
mm were made via compression molding using a pressure of 150 kN m–2 at 100 °C for 10 min. The pellets were placed
between two stainless steel plates, and an electric current of 1 mA
was then passed through the plates. The voltage of the nondoped and
doped 3D microsphere scaffolds was measured using symmetrical cylindrical
cells. The recorded voltage was later used to calculate the electrical
conductivity according to Pouillet’s law.[48]
Tunneling Electron Microscopy (TEM)
The structure of
the nanomaterials was determined using a Hitachi HT7700 transmission
electron microscope at a voltage of 100 kV. The samples were deposited
on 400 mesh copper grids that were coated with carbon (Ted Pella,
Inc., USA) from ultrasonicated water suspensions of the nanomaterials.
Zeta Potential Measurement
The zeta potential of the
PEMs that were attached to the grafted microspheres was determined
using a Nanozetasizer with a He–Ne laser source at a wavelength
of 633 nm (Zetasizer ZEN 3600, Malvern Instruments, UK). The microspheres
were injected into the zeta potential cell and allowed to equilibrate
for 2 min. Duplicate samples were measured. During the measurement,
the Slomuchowski method was selected to obtain the zeta potential.
Fluorescence Microscopy
Fluorescence measurements were
performed using a Nikon Ti–S spectrometer. Prior to the surface
fluorescence tests, the PEM-coated microspheres were kept in the oven
after drying at a temperature of 55–65 °C for 1 week to
create strong interactions and good stability for the particulate
samples at a high pH of 7.4. Approximately 10–20 mg of the
particulate samples was placed in glass vials and immersed in 0.5
mL of 3 mM DAPI (pH 7.4) at room temperature for 30 min. The vials
containing DAPI solution and the microsphere-based samples were protected
from light. The PEM-coated microspheres were pipetted onto a microscopic
glass slide and covered with a coverslip.
Swelling Test
The swelling ratio (SR) of the particulate
scaffolds was determined by immersing dry 3D microsphere scaffolds
in water at pH 2.5 and 5. The weight at different time points of the
swollen-state samples (ms,t) was recorded
after removing excess water with tissue paper. Then, the SR was calculated
from the following equationand the equilibrium
swelling, Q∞, is given bywhere md and m∞ are defined
as the weight of the samples
in the dry state and at equilibrium, respectively.
X-ray Microtomography
A volume of 1 mm (diameter) ×
1 mm (length) for the 3D microsphere scaffolds was acquired using
microtomography (Xradia MicroXCT-200). The distances from the X-ray
source and the detector were 40 and 7 mm, respectively. The following
scanning conditions were then set up: a power of 6 W, an X-ray source
voltage of 60 kV, 1105 projections, and an exposition time of 25 s
projection–1. The magnification was 20× with
a pixel resolution of 1.1519 μm.
Results and Discussion
Here, we show the importance of an AA-grafted PLA surface as a
microsphere base layer for alternately assembled PEMs for the fabrication
of strong and functional 3D microsphere scaffolds that can be made
to be conductive and/or stronger.After surface grafting and
PEM assembly (polyanionic/polycationic
layers or polyanionic/neutral polymer layers) onto the surfaces of
the PLLA microspheres, the microspheres were molded at room temperature
in a form (Figure , left, and Figure ), resulting in 3D scaffolds held together
by intermolecular forces through electrostatic and/or hydrogen-bonding
interactions. For the electrostatic interactions, strong attractive
forces were created between oppositely charged surfaces. Interpenetration
of polyelectrolytes could also occur to form polyelectrolyte complexes
during this interaction, resulting in strong adhesive forces. The
3D scaffolds exhibited strong resistance to high-shear mixing (Video S1). Without adsorption of the PEMs, the
PLLA microspheres could not be shaped into a permanent cylindrical
3D shape and could be very easily ruptured after 3D template removal.
In addition, PLLA microspheres without any polyelectrolytes or grafted
chains sintered at 55–65 °C were also easily ruptured
under high ultrasonication or high-shear mixing.
Figure 1
Comparison of the fabricated
3D microsphere scaffolds to 10 cent
Euro coins: (left) PAH2.5g, (middle) PAHgGO,
and (right) PAHgFeO. All 3D microsphere scaffolds were
assembled at pH 2.5.
Comparison of the fabricated
3D microsphere scaffolds to 10 cent
Euro coins: (left) PAH2.5g, (middle) PAHgGO,
and (right) PAHgFeO. All 3D microsphere scaffolds were
assembled at pH 2.5.Schematic illustration of the surface grafting and build up of
PEMs onto the grafted surface of PLLA microspheres.The 3D scaffolds were also functionalized with
model additives
i.e., GO, Fe3O4, and DAPI, to illustrate the
versatility of the technique. Functionalization of GO nanosheets into
a 3D microsphere scaffold that was assembled via the LbL technique
resulted in a darker gray color (Figure , middle) compared with that of the Fe3O4-functionalized 3D scaffold (Figure , right).Thus, 3D microsphere
scaffolds were successfully fabricated and
functionalized with different functional additives, i.e., GO, Fe3O4, and DAPI (Figure S5).
Functionalities of the PEMs on the Surface of PLLA Microspheres
The presence of PAA-grafted PLLA surfaces as a base layer significantly
affected the physical adsorption of weak polyelectrolytes, resulting
in denser absorption bands for the functionalities than with the nongrafted
surfaces. The surface chemistry of the grafted microspheres after
the assembly of the PEMs was evaluated using FTIR (Figure ) and compared with that of
the nongrafted microspheres (Figure S3).
During FTIR measurement, the higher intensity of the functional groups
located on the grafted surfaces (Figure A,B) than on nongrafted surfaces (Figure S3A,B) confirmed the 2D coverage of PEMs
and highlighted the importance of surface grafting to achieve dense
multilayer films. These functional groups were primarily observed
in two wavenumber (υ) regions, i.e., υ ∼ 1680–1500
cm–1 (the area where the carboxylic acid group and
the ionizedcarboxylate groups of PAA and the amide I and II groups
of PAAm exists) and υ ∼ 3800–2300 cm–1 (the absorption bands of the amine and methylene).
Figure 3
ATR-FTIR spectra of neat
PLLA microspheres (black) and PEMs alternately
assembled onto the surface of PLLA-g-PAA microspheres
with PAMg (red), PAMgGO (magenta), PAMgFeO (orange), PAH2.5g (green), PAHgGO (violet),
PAHgFeO (gray), and PAH5g (blue) in the region
of (A) 1680–1500 cm–1 and (B) 3800–2300
cm–1. (C) XRD patterns of the 3D microsphere scaffolds
with and without GO functionalization.
ATR-FTIR spectra of neat
PLLA microspheres (black) and PEMs alternately
assembled onto the surface of PLLA-g-PAA microspheres
with PAMg (red), PAMgGO (magenta), PAMgFeO (orange), PAH2.5g (green), PAHgGO (violet),
PAHgFeO (gray), and PAH5g (blue) in the region
of (A) 1680–1500 cm–1 and (B) 3800–2300
cm–1. (C) XRD patterns of the 3D microsphere scaffolds
with and without GO functionalization.As expected, the neat PLLA microspheres exhibited an absorption
band representing ester groups at 1747 cm–1 (Figure A). The FTIR spectra
confirmed the growth from the first to the sixth PEM bilayer on the
PAA-grafted surfaces (Figure A,B) and nongrafted analogues (Figure S3A,B) by the increase in the intensities of the corresponding
functional groups. The zeta potential also confirmed the stepwise
growth of the PEMs onto the grafted surfaces via charge reversal (Figure S2). The surface grafting had a strong
affect on the peak area of the PEMs in the 1680–1500 and 3800–2300
cm–1 regions relative to the nongrafted microspheres
(Table ). The physical
adsorption of the PEMs on the surfaces of both the PAA-grafted and
nongrafted PLLA microspheres is a complex process, and it could influence
the conformational entropy of the acrylic acid groups of PAA and the
amine-methylene groups of PAH during PEM assembly.
Table 2
Peak Areas of Nongrafted and Grafted
PLLA Microspheres after Assembly of the Sixth PEM Bilayer
peak
area (A cm–1)a
nongrafted
grafted
materials
υ ∼ 1680–1500 cm–1
υ ∼ 3800–2300 cm–1
υ ∼ 1680–1500 cm–1
υ ∼ 3800–2300 cm–1
PAMn
18
8
PAMg
20
15
PAH2.5n
20
15
PAH2.5g
20
19
PAH5n
15
5
PAH5g
15
13
PAMgGO
23
12
PAHgGO
19
12
PAMgFeO
17
13
PAHgFeO
19
18
Calibrated by subtracting
the peak
area of PEM-coated microspheres from the peak area of neat PLLA, which
was approximately 0.3 at 1680–1500 cm–1 and
0.2 at 3800–2300 cm–1. The results of the
peak area were subsequently rounded.
Calibrated by subtracting
the peak
area of PEM-coated microspheres from the peak area of neat PLLA, which
was approximately 0.3 at 1680–1500 cm–1 and
0.2 at 3800–2300 cm–1. The results of the
peak area were subsequently rounded.For the GO-functionalized particles (Figure S1A), the peak area in the 1680–1550 cm–1 region differed between PAH2.5g and PAMg,
whereas Fe3O4 nanomaterials (Figure S1B) impacted the peak area in two different regions,
i.e., 1680–1500 and 3800–2300 cm–1, for those two materials (Table ). The absorption peak for the Fe–O stretching
bond[46] in the range of 600–580 cm–1 was difficult to detect using FTIR spectroscopy (Figure S3C), suggesting that the IR penetration
depth and the concentration may have influenced the detection of the
functionalities of the material.XRD measurements of the two
GO-functionalized materials and their
respective references showed a low intensity of 12.3° for the
detection of the GO stacking layer at 2θ in the PAHgGO material, which corresponded to an interlayer spacing of 0.72
nm for the GO nanosheets that was calculated from Bragg’s law
(arrow, Figure C).
This result confirmed the existence of stacked GO layers[49] between the PEM films. The XRD pattern of GO
was quite low, which could be related to the very small amount of
GO incorporated in the PEMs.The XRD pattern of GO was observed
in PAHgGO and not
in PAMgGO. This might be related to the primary or secondary
physical adsorption of nanomaterials interpenetrated through the PEM
network. Primary physical adsorption (deep adsorption) might have
occurred during GO functionalization into PAA/PAAm multilayers, whereas
GO nanomaterials might have attached to the outermost layers of polyelectrolytes
through secondary physical adsorption for PAA/PAH multilayers; thus,
XRD could detect the existence of GO nanomaterials located at the
outermost surface of the PEM rather than the ones adsorbed deeper
in the material. Three sharp peaks were located at 2θ values
of 16.9, 18.9, and 22.3°, which are characteristic of PLLA[50] (Figure C). Hence, grafting of the AA monomer on the surface of the
PLLA microspheres provided a denser PEM assembly; thus, the grafted
surfaces constitute a crucial factor for alternately assembling (PAA/PAAm)6 and (PAA/PAH)6 multilayers. Similar to the surface
chemistry, the grafted surfaces also influenced the swelling behavior
of the PEMs. It is worth noting that (PAA/PAH)6 multilayers
demonstrated a larger swelling effect than (PAA/PAAm)6 multilayers
at pH 2.5 (Figure S6).
Morphology
of the PEMs on the Grafted Surfaces
The
change in morphology between neat PLLA and PLLA-g-PAA microspheres demonstrated significant surface texture differences.
Neat PLLA microspheres with an average diameter of 2 μm (Table ) had a rough surface
(Figure A), whereas
PLLA-g-PAA microspheres had a “crystal”-like
structure (Figure B). The crystal structure might be a consequence of the benzophenone
that terminates the free-radical polymerization under UV irradiation[51] or a solvent-induced crystallization process.[52] The difference in the morphology of these two
base substrates subsequently influences the sequential adsorption
of PEMs since the growth of PEMs consists of three main zones, where
zone I is a function of the substrate surface and zone III demonstrates
that excess charge affects the final structure of the PEMs.[53] PAMg also had a rough morphology
(Figure C), whereas
a smooth surface was observed for PAMn (i.e., the nongrafted
surface) after PEM assembly (Figure S4A). A significant change in the morphology was observed for PAH2.5g because the polyelectrolyte charge induced the conformational
transition directly[54] (Figure D). In other words, the polyanion/polycation
multilayers provided a rough surface at low pH because of the low
charge density and because the formation of segmental loops and tails
is more favored than at high pH, resulting in thicker PEMs than those
from sequential adsorption at high pH. Additionally, the grafted surfaces
demonstrated large polyanion/polycation multilayer surface coverage
at low pH (Figure D) compared to that of the nongrafted analogues (Figure S4B). In contrast to the surface morphology, no significant
change in emission color was observed for a fluorescent dye molecule
that was functionalized into the PEMs and physically adsorbed on the
grafted and nongrafted surfaces (Figure S5).
Table 3
Microsphere Characteristics, Layer
Thickness of the Microsphere-Based Samples, and Porosity Data for
the 3D Scaffolds
microsphere
properties
material
mean diameter,ad (μm)
Smb
layer thicknessc (μm)
porosity of 3D scaffold
in air (%)
PLLA
2
1.2
d
PLLA-g-PAA
3.5 ± 0.7
0.6
1.5 ± 0.7
d
PAH2.5g
11.5 ± 0.7
0.2
9.5 ± 0.7
48
PAMg
7
0.3
5
58
PAHgGO
4
0.6
2
50
PAMgGO
12
0.2
10
50
Calculated based on Sauter’s
method. This diameter may be calculated from single or aggregated
microspheres.
Sm =
specific surface area per unit mass.
The layer thickness of the PEMs
was calculated by subtracting the diameter of PEM-coated microspheres
from that of neat PLLA microspheres. The diameter was measured using
laser diffraction.
Not possible
to produce 3D scaffolds.
Figure 4
Surface morphologies of the microspheres of (A) neat PLLA, (B)
PLLA-g-PAA, (C) PAMg, (D) PAH2.5g, (E) PAH5g, (F) PAMgGO, (G) PAHgGO, (H) PAMgFeO, and (I) PAHgFeO.
Surface morphologies of the microspheres of (A) neat PLLA, (B)
PLLA-g-PAA, (C) PAMg, (D) PAH2.5g, (E) PAH5g, (F) PAMgGO, (G) PAHgGO, (H) PAMgFeO, and (I) PAHgFeO.Calculated based on Sauter’s
method. This diameter may be calculated from single or aggregated
microspheres.Sm =
specific surface area per unit mass.The layer thickness of the PEMs
was calculated by subtracting the diameter of PEM-coated microspheres
from that of neat PLLA microspheres. The diameter was measured using
laser diffraction.Not possible
to produce 3D scaffolds.A smoother surface morphology was observed for PAH5g compared
to that for PAH2.5g after the adsorption of
the PEMs (Figure E).
This is believed to be caused by a conformational transition in the
(PAA/PAH)6 multilayers when the pH of the solution was
increased to 5. At higher pH, the enthalpy required to maintain the
charged polymer in a stretched conformation is able to overcome the
entropic penalty of the globule conformational transition at a certain
critical charge density. The result is that the polyelectrolyte chains
that were adsorbed on the grafted microsphere surfaces may have formed
a larger number of trains, resulting in stretched conformations.[47] Thus, the surface of the nongrafted PLLA microspheres
remained rough after increasing the pH of the solution, in contrast
with the grafted PLLA microspheres (Figure S4C).At low pH, functionalization with GO or Fe3O4 nanomaterials improved the surface coverage of the grafted
microspheres
and altered their morphology after the adsorption of the (PAA/PAAm)6 (Figure F,H)
and (PAA/PAH)6 (Figure G,I) multilayers, whereas no significant alteration
in the surface morphology of the (PAA/PAAm)6 and (PAA/PAH)6 multilayers occurred after GO functionalization at low pH
(Figure F,G). In summary,
the surface grafting influenced the morphology of the microsphere
surfaces during the assembly of the PEMs. Additionally, the grafted
surfaces also demonstrated an improved surface coverage of the PEMs
compared with that of the nongrafted analogues.
Mechanical
Properties of the 3D Microsphere Scaffolds and Their
Comparison to the Cancellous Bone
The 3D microsphere scaffolds
(Figure A) were mechanically
compressed under a load cell of 10 kN to evaluate their mechanical
performance in comparison to that of natural materials, such as cancellous
or trabecular bone. PAH2.5g had an E-modulus of 141 ±
19 MPa, whereas PAMg had a lower E-modulus of 115 ±
5 MPa. These two 3D microsphere scaffolds demonstrated a higher Young’s
modulus than PAH5g (Figure B). The PAMg and PAH2.5g 3D scaffolds
were selected, and new scaffolds, previously functionalized with GO
nanosheets, were created, namely, PAMgGO and PAHgGO. After GO functionalization, the E-modulus of PAMgGO
improved significantly to 146 ± 6 MPa, whereas PAH2.5gGO decreased significantly to a very low E-modulus of 16 ± 2
MPa.
Figure 5
(A) Illustration of the 3D microsphere scaffold. (B) Summary of
the compressive Young’s modulus (E-modulus) of the 3D microsphere
scaffolds (nongrafted microspheres resulted in irreproducible data).
(C) Ashby plot of E-modulus vs the density of natural materials and
the 3D microsphere scaffolds. (D) X-ray microtomography of the 3D
microsphere scaffold.
(A) Illustration of the 3D microsphere scaffold. (B) Summary of
the compressive Young’s modulus (E-modulus) of the 3D microsphere
scaffolds (nongrafted microspheres resulted in irreproducible data).
(C) Ashby plot of E-modulus vs the density of natural materials and
the 3D microsphere scaffolds. (D) X-ray microtomography of the 3D
microsphere scaffold.The mechanical properties of the scaffold increased (or decrease)
for PAMg (or PAH2.5g) after alternatingly adsorbing
GO to the particles, which could be related to an increase (or decrease)
in the thickness of the PEM layer of PAMg (or PAH2.5g). Low pH generally results in GO nanosheet agglomeration.[55] At pH 2.5, PAHgGO demonstrated thicker
layers than PAMgGO (Table ). The thickness of the charged polymers depends on
the surface charge density and the charge density of the adsorbing
polymer.[47] The PAA/PAH multilayers (polyanionic/polycationic
combination) may have demonstrated a higher surface charge density
than the PAA/PAAm multilayers (polyanionic/neutral polymer), resulting
in more GO nanosheets binding to these charged polymers per unit area.
The interpenetration of GO nanomaterials during LbL assembly, then,
might have interrupted the chain conformations of the PAA/PAH multilayers,
thus physically suppressing the thickness of the PEMs. When the thickness
decreased, weaker mechanical performance was observed. The E-modulus
of the nongrafted 3D scaffolds could not be evaluated due to the weak
3D scaffolds. More specifically, the 3D scaffold fabricated from (PAA/PAH)6 multilayers on nongrafted surfaces at pH 2.5 cracked after
the 3D template was removed. The 3D scaffolds of PAMg,
PAH2.5g, and PAMgGO demonstrated similar mechanical
performances to those of sintered microspheres of diameters between
100 and 600 μm when they were sintered between 60 and 70 °C,[56] at 100 °C for 4 h,[14] and at 160 °C for 2 h.[57] However,
these 3D microsphere scaffolds had a higher mechanical performance
compared with that of solvent/nonsolvent sintered microsphere scaffolds.[58] As previously noted, an increase in the temperature
and sintering time resulted in a detrimental effect on the surface
morphology. Additionally, the porosity was decreased after the sintering
process.[14,56] Furthermore, the E-moduli of all of the
3D microsphere scaffolds that were fabricated via surface grafting
and LbL assembly were in the range of cancellous bone from a low to
high E-modulus, i.e., 10–2000 MPa. However, the cancellous
human bone described in the Ashby plot database[59] demonstrated a high range for the E-modulus (>100 MPa)[60] at medium density, and three of our 3D microsphere
scaffolds closely matched natural human bone, namely, PAH2.5g, PAMg, and PAMgGO (Figure C). Similar to the XRD analysis, X-ray microtomography
of the 3D scaffold, i.e., PAMgGO, did not detect a signal
for GO inside the 3D scaffold. Thus, the distribution of GO could
not be calculated, but it showed that the 3D biomaterial was homogenous
(Figure D and Video S2). However, the 3D microsphere scaffolds
fabricated via LbL assembly were successfully functionalized with
GO and retained good mechanical performance from a low to high Young’s
modulus.
Physical Properties of the Microspheres
Combined surface
treatments (surface grafting and physical adsorption of PEMs) on the
PLLA microspheres had a large impact on the diameter and thickness
of the PEMs (Table ). The particle diameter was evaluated using Sauter’s method
since this method is commonly used to evaluate the diameter of a particle
when the surface is active. Such a substantial increase in layer thickness
would, at first glance, indicate particle aggregation. However, a
shape factor equivalent to 1, referring to a spherical geometry, was
observed for all of the particulate samples during particle size measurement,
indicating single particles rather than spherical aggregates. An aggregated
spherical complex of particles would be substantially larger than
the measured values in Table .It is worth noting that traditional LbL assembly is
generally used to create ultrathin PEMs (from several tenths to a
hundred nanometers in thickness),[47,61] and several
hundred-nanometer-thick layers were achieved after numerous bilayers
were assembled, which depended on parameters such as pH.[62] For a specific application, such as 3D biomaterials,
micrometer-thick PEMs might be favored over nanometer-thick PEMs since
the mechanical stability can be enhanced. Thick PEMs, i.e., in the
micrometer range, could also be obtained after the addition of numerous
bilayers.[63,64] Here, micrometer-thick films were obtained
on the particulate surfaces after grafting due to exponential growth
of the PEMs and due to the conditions used during LbL assembly, i.e.,
the stirring rate and polymer concentration in the solution. The mechanism
of an exponential growth regime is not well understood.[65] It is speculated that exponential growth of
PEMs can be obtained through a complexation process of polyanions/polycations[66] or diffusion “in and out” of the
polyanions/polycations, which subsequently forms polyelectrolyte complexes
at the outermost layer of the physically adsorbed film.[65,67] At one-tenth of the polyelectrolyte concentration used, the 3D scaffold
ruptured under the high-shear mixing that was used as a pretest for
mechanical stability, which could be due to the presence of a linear
growth regime at a concentration that is lower than the actual concentration
we used. Thus, the concentration of polymer in the solution and the
stirring process used in this work might have accelerated the exponential
growth process to support the integrity and mechanical performance
of the 3D scaffold. Surface grafting on PLLA microspheres yielded
a polymer graft thickness of 800 nm to 2.2 μm in the dry state.
The (PAA/PAH)6 multilayers adsorbed onto the PAA-grafted
PLLA microspheres had a diameter of 11.5 ± 0.7 μm, which
was 4–5 μm thicker than that of the (PAA/PAAm)6 multilayers. This could be due to the formation of a loop conformation
on the PLLA surface (Figure C). Functionalization of the GO nanosheets resulted in an
alteration of the properties of the microsphere material. The (PAA/PAAm)6 multilayers showed an increase in the diameter and thickness
and a decrease in the surface area of PLLA microspheres compared to
those of the (PAA/PAH)6 multilayers assembled on grafted
PLLA microspheres at low pH. The higher E-moduli of two of the 3D
microsphere scaffolds, PAH2.5g and PAMg (Figure B), may also be related
to the microsphere properties because of their thicker layer (Table ), which improves
the mechanical performance. Importantly, the porosity of PAMg and PAMgGO in air matched that of human cancellous bone
(50–90%),[60] whereas the porosity
of PAH2.5g (48%) was comparable to that of porous scaffolds
that have been used to regenerate femoral defects in rabbits.[68]During bone regeneration, an electric
field can exogenously stimulate
new bone formation at a minimum frequency between 10 and 30 Hz. The
bone tissue will later respond to a minimum electrical signal in the
range of 1–10 μV cm–1.[69] Thus, the conductivity of the scaffolds also plays a critical
role in electrical signaling. The conductivity of the 3D scaffolds
consisting of different nanomaterials was measured, and neither the
nonfunctionalized materials nor the GO-functionalized scaffolds were
conductive. GO itself is an electrically insulating material, but
an electrical conductivity of approximately 2.58 × 10–6 S cm–1 was previously observed.[70] It could also be that the GO-functionalized scaffolds were
not conductive because of the very low concentration of GO nanomaterials,
which are required to pass the electric current, in the scaffolds.
In contrast to the GO-functionalized scaffolds, the Fe3O4-functionalized scaffolds resulted in a high electrical
conductivity, which could be due to the regular organization of Fe3O4 nanoparticles between layers after sequential
adsorption. In addition, Fe3O4 nanomaterials
can transfer electric current through their aligned electron domains
in parallel, a phenomenon called electronic conduction. The hot press
PAHgFeO and PAMgFeO films had electrical conductivity
values of approximately 180 and 130 S cm–1, respectively,
after 1 mA electric current was passed through 0.3–0.4 mm thick
films, although only 0.002 wt % of Fe3O4 nanomaterials
was functionalized on the surface of the 3D scaffolds. After doping,
the electrical conductivity of PAH2.5g decreased approximately
60 times, i.e., 3 S cm–1, compared with that of
the nondoped microparticle-based scaffolds. In contrast to PAHgFeO, PAMgFeO exhibited a much higher electrical
conductivity of approximately 240 S cm–1 compared
with that of nondoped PAMgFeO. Humidity has been known
to affect electronic conductivity,[71] but
humidity was not controlled during conductivity measurements in this
work. A possible explanation for this phenomenon might be related
to the swelling effect of PAA/PAH multilayers during HCl doping. In
addition, PAA/PAH multilayers seemed to demonstrate more swelling
than PAA/PAAm multilayers, causing an extension of the chain conformations.
As a consequence, the orientation of iron nanoparticles was also altered,
causing a large gap between these nanoparticles in the PAA/PAH multilayers.
The pathways of unconnected nanoparticles seemed to be constant in
the PAA/PAH multilayers, even after they were dried and hot pressed.
The tunnelling probability of electrons will then decrease when the
electric current is passed through this material in air. Thus, the
electronic conductivity of PAHgFeO, where iron nanoparticles
were located between PAA/PAH multilayers, decreased dramatically more
than PAMgFeO, which consisted of iron nanoparticles sandwiched
in PAA/PAAm multilayers. The functionalization of Fe3O4 nanoparticles interpenetrated into (PAA/PAAm)6 multilayers had a stronger impact on the magnetic field than that
of the (PAA/PAH)6 multilayers when a magnetic source was
located 4–5 mm on top of the surface of the 3D scaffolds (Video S3).The success of the 3D microsphere
scaffolds fabricated via surface
grafting in combination with the LbL approach at room temperature
demonstrates that these scaffolds can be functionalized with inorganic
nanomaterial or biofunctional species between different layers while
retaining porosities and mechanical performances that are similar
to those of human cancellous bone.
Conclusions
Surface
grafting was shown to be a crucial technique to create
a base layer for the alternating assembly of weak polyelectrolytes
onto the surface of PLLA microspheres. This simple method can be used
to fabricate advanced 3D scaffolding materials that are strong, functional,
and/or highly conductive. Conformational changes in the PEMs at different
pH values resulted in variations in the layer thickness, thus affecting
the mechanical performance of the 3D microsphere scaffolds. Grafted
surfaces of PLLA microspheres exhibited a larger peak area for the
absorption bands of PEMs compared with that of nongrafted surfaces.
Alteration of the morphology produced an improved surface coverage
for the PEMs assembled at low pH on the grafted surfaces compared
with that of the nongrafted surfaces. A blue emission color indicated
the success of the functionalization of a fluorescent dye onto two
different substrate surfaces. The PEMs that were physically adsorbed
on the grafted surfaces had more pronounced swelling behaviors than
those of nongrafted surfaces. The 3D microsphere scaffolds were within
the compressive range of human cancellous bone, in addition to having
a similar porosity. The functionalization of magnetic nanoparticles
at low concentration into the PEMs resulted in a high electrical conductivity.
The 3D scaffolds of polyanionic and polycationic systems reduced their
electrical conductivity after doping, in contrast to the polyanionic
and neutral polymers. Thus, surface grafting of PLLA microspheres
in combination with the LbL approach and functionalization with nanomaterials
created 3D scaffolds that are suitable for bone tissue engineering.
Authors: C Picart; J Mutterer; L Richert; Y Luo; G D Prestwich; P Schaaf; J-C Voegel; P Lavalle Journal: Proc Natl Acad Sci U S A Date: 2002-09-17 Impact factor: 11.205
Authors: Robertus Wahyu N Nugroho; Karin Odelius; Anders Höglund; Ann-Christine Albertsson Journal: ACS Appl Mater Interfaces Date: 2012-05-24 Impact factor: 9.229