Natalia Pajares-Chamorro1, Xanthippi Chatzistavrou1. 1. Department of Chemical Engineering and Material Science, College of Engineering, Michigan State University, East Lansing, Michigan 48824, United States.
Abstract
Sol-gel-derived bioactive glass nanoparticles have attracted special interest due to their potential as novel therapeutic and regenerative agents. Significant challenges are yet to be addressed. The fabrication of sol-gel-derived nanoparticles in binary and ternary systems with an actual composition that meets the nominal has to be achieved. This work addresses this challenge and delivers nanoparticles in a ternary system with tailored composition and particle size. It also studies how specific steps in the fabrication process can affect the incorporation of the metallic ions, nanoparticle size, and mesoporosity. Sol-gel-derived bioactive glass nanoparticles in the 62 SiO2-34.5 CaO-3.2 P2O5 (mol %) system have been fabricated and characterized for their structural, morphological, and elemental characteristics using Fourier transform infrared spectroscopy, X-ray diffraction analysis, scanning electron microscopy associated with elemental analysis, transmission electron microscopy, and solid-state nuclear magnetic resonance. The fabricated nanoparticles were additionally observed to form the apatite phase when immersed in simulated body fluid. This work highlights the effect of the different processing variables, such as the nature of the solvent, the order in which reagents are added, stirring time, and the concentrations in the catalytic solution on the controlled incorporation of specific ions (e.g., P and Ca) in the nanoparticle network and particle size.
Sol-gel-derived bioactive glass nanoparticles have attracted special interest due to their potential as novel therapeutic and regenerative agents. Significant challenges are yet to be addressed. The fabrication of sol-gel-derived nanoparticles in binary and ternary systems with an actual composition that meets the nominal has to be achieved. This work addresses this challenge and delivers nanoparticles in a ternary system with tailored composition and particle size. It also studies how specific steps in the fabrication process can affect the incorporation of the metallic ions, nanoparticle size, and mesoporosity. Sol-gel-derived bioactive glass nanoparticles in the 62 SiO2-34.5 CaO-3.2 P2O5 (mol %) system have been fabricated and characterized for their structural, morphological, and elemental characteristics using Fourier transform infrared spectroscopy, X-ray diffraction analysis, scanning electron microscopy associated with elemental analysis, transmission electron microscopy, and solid-state nuclear magnetic resonance. The fabricated nanoparticles were additionally observed to form the apatite phase when immersed in simulated body fluid. This work highlights the effect of the different processing variables, such as the nature of the solvent, the order in which reagents are added, stirring time, and the concentrations in the catalytic solution on the controlled incorporation of specific ions (e.g., P and Ca) in the nanoparticle network and particle size.
Bioactive
glasses (BGs) are promising materials for tissue engineering
due to their controlled degradability and capability to stimulate
new tissue formation.[1−5] BGs are especially attractive for orthopedic applications as they
form a strong bond with the bone.[6−9] Additionally, their degradation promotes
osteogenesis by releasing ionic products that stimulate osteoinductivity.[10−14] Depending upon the type of ion released and its concentration, specific
properties can be achieved.[2,15−17] Thus, there is great interest to gain control over the incorporation
of each ion into the glass structure to achieve the desired performance.
In particular, BGosteogenic properties are mainly attributed to the
release of Si4+ and Ca2+ ions, which act as
triggers for the upregulation of osteogenic gene expression as well
as a spur for osteoblast metabolism and bone homeostasis.[10,18−21] Although these properties have been achieved in several BG compositions,
those containing CaO above 25 mol %, such as 45S5 Bioglass, S53P4,
or 58S, are probably the most commercially exploited for bone grafts
since a higher calcium content along with P provokes stronger cell
mineralization.[6,7]Tissue engineering and nanomaterials
science have been merged to
improve the material–cell interaction, presenting materials
that mimic host tissue nanofeatures.[22,23] Bioactive
glass nanoparticles (BGNs) can be synthesized, tailoring their characteristics
for the appropriate host response.[24] Their
small size favors cell uptake, granting an intracellular and localized
release of therapeutic ions.[15,25] The higher surface
reactivity of BGNs compared to their micrometer counterparts causes
faster network degradation, thereby advancing the bioactive properties
and accelerating the regenerative process.[26,27] Degradability, surface reactivity, and biological response depend
on the network connectivity and thus can be tailored by adjusting
the concentration of both network formers and network modifier ions
in the ultimate composition of the glass structure.[28,29] While addressing the desired composition in BG microparticles is
a well-standardized process, the incorporation of metallic ions in
BGNs is rarely achieved, challenging the ability to deliver the desired
set of properties for tissue regeneration.[30]Several techniques have been reported for the fabrication
of BGNs
such as microemulsion, flame spray, laser spinning, or post-modification.[31] However, this work focuses only on sol–gel-like
approaches, utilizing polymer-free one-step basic catalysis methods.
Thus, acid-catalyzed, two-step catalysis methods and polymeric surfactant
methods will not be discussed. Silicate-based BGNs can be considered
as silica nanoparticles in which various network modifier ions are
introduced within the structure. The so-called Stöber method,[32] routinely applied for controlled silica nanoparticle
synthesis, is the most adapted basic catalysis methodology for BGN
fabrication.[30] In this method, alterations
in the pH, temperature, and reagent concentration can lead to silica
particles with submicrometer (100–1000 nm) or nano (<100
nm) sizes, with the simultaneous formation of aggregates for the latter.[33,34] The Stöber method has been previously adapted to attempt
the synthesis of BGNs but with limited success. The addition of network
modifying metallic ion precursors in the synthesis process may impair
the control over particle size, shape, and dispersity even at low
concentrations.[35,36] However, the main unsolved issue
is the persisting discrepancy between the nominal composition and
the actual one obtained after the fabrication process.[21,37,38] Specifically, the concentrations
of P and Ca2+ ions in BGNs, which are both key elements
for osteoconductivity and bone bonding, are consistently lower than
that aimed.[36]The most frequently
used precursors for the incorporation of calcium
and phosphorous ions during BG sol–gel synthesis are calciumnitrate and triethyl phosphate (TEP), respectively. The incorporation
of P ions depends on the hydrolysis of TEP, usually performed in a
solution already containing tetraethyl orthosilicate (TEOS) as the
main reagent for SiO2. The low amount of P2O5 (mol %) in the final BGN system has been attributed to the
different hydrolysis rates between these two precursors, TEOS and
TEP, under elevated pH, which causes the rapid condensation of SiO2 nanoparticles lacking P ions.[36] In the case of Ca2+ ion incorporation, the addition of
calcium nitrate takes place after hydrolysis and condensation of nanoparticles.
In this process, Ca2+ ions cover the particles’
surface by bonding to hydroxyl species and get diffused during calcination
above 400 °C, thus modifying the network.[39] This mechanism results in very low amounts of CaO (mol
%) in the final BGN system, resulting in a composition significantly
different in the nominal one. Different reasons explain this outcome,
such as the lack of sufficient hydroxyl groups at the nanoparticles’
surface to bond with elevated concentrations of Ca2+ ions
in solution or the low strength of these bonds, which cannot withstand
the washing steps before the calcination.[40] Additionally, Ca2+ ions are likely to form other species
such as carbonate groups or calcium-rich components, without being
properly incorporated into the amorphous structure.[35,37]Different approaches have been explored to overcome these
challenges.
For example, the addition of calcium nitrate during the early stages
of particle condensation allowed higher detection of calcium by EDS
but that resulted in a drop in the particle dispersity.[36] Additionally, it was unclear if the observed
calcium was modifying the silica network of the BGNs as modifier ions
or calcium was trapped as CaO molecules in BGNs or as calcium carbonate
molecules. Another approach reported the increase in the actual concentration
of calcium into the BGN network by increasing the Ca/Si ratio in the
synthesis protocol beyond the expected ratio of the nominal composition.[35] The Ca2+ ion supersaturated solution,
along with the absence of the washes before calcination, resulted
in the detection of the higher calcium content as well as the formation
of calcium-rich areas in the delivered BGNs.[35,37] However, once these calcium-rich areas were removed by applying
washes after the heat treatment, the measured amount of the CaO in
the BGNs was only around 10 mol %. Lately, Kesse et al. have shown
the effect of different concentrations of the CaO content in BGN by
adjusting their protocol to achieve 15.4 mol %, the maximum amount
reached up to date in monodispersed submicrometer BG particles by
a one-step base-catalyzed synthesis.[41]In this work, the challenges of incorporating P and Ca in amounts
equal to the nominal in BGNs were addressed. This work reports for
the first time a novel approach to synthesize nanoparticles in the
62 SiO2–34.5 CaO–3.2 P2O5 (in mol %) system where both nominal and actual compositions agree.
Initially, submicrometer particles (e.g., 400 nm) were reproduced
according to the protocol described by Zheng et al.,[36] and they were used as a reference for this study. Then,
systematic modifications were applied to the synthesis protocol in
terms of the utilized solvent, the stirring time, and the order in
which reagents were added to incorporate the desired concentrations
of P and Ca2+ ions. The solvent promoting hydrolysis of
TEP was used to allow the incorporation of P ions in the SiO2 network before the nucleation of nanoparticles. The processing protocol
was tailored so that the actual amount of CaO in the fabricated BGNs
was measured above 30 mol % and the particle size was below 100 nm.
This work also reports for the first time the impact that the stirring
time before catalysis has on controlling the size of the fabricated
nanoparticles. Moreover, it was showed that mesoporosity and particle
distribution can be further customized by modifying the concentrations
of the reagents in the catalyst (e.g., ammonium hydroxide and distilled
water). Overall, the changes introduced in the synthesis process not
only yielded BGNs with a composition that meets the nominal but also
revealed possible means of controlling particle size, particle dispersity,
and mesoporosity.
Results and Discussion
Morphology, Particle Size, and Distribution
The particle
size, dispersity, and composition of sol–gel-derived
BGNs were studied as a function of processing parameters. Particles
were synthesized following two main protocols: method 1 (M1) and method
2 (M2). Figure shows
the size, morphology, and distribution using the SEM and TEM images
and elemental analysis using the EDS spectrum of synthesized BGN.
The average particle size for each fabrication protocol was calculated
by analyzing the TEM images, and the mean values are reported in Table . Dense, spherical,
and monodispersed particles with a diameter of around ∼400
nm were achieved in the M1 methodology (Figure A–C,E–G).
Figure 1
(A–X) Nanoparticle
(BGN) morphology, dispersity, and aggregation
size by SEM and TEM images and elemental analysis by SEM-EDS spectra
for protocols (A–D) M1-P1, (E–H) M1-P2, (I–L)
M2-P1, (M–P) M2-P2 A, (Q–T) M2-P2 B, and (U–X)
M2-P2 C. Scale bars indicate 200 nm for SEM images and 1000 and 40
nm for TEM images.
Table 1
Particle
Size of Synthesized BGN under
Different Fabrication Protocols Based on TEM Image Analysis
protocols
M1-P1
M1-P2
M2-P1
M2-P2 A
M2-P2 B
M2-P2 C
particle size (nm)
438 ± 17
425 ± 17
86 ± 14
70 ± 13
18 ± 2
18 ± 5
193 ± 51
495 ± 12
(A–X) Nanoparticle
(BGN) morphology, dispersity, and aggregation
size by SEM and TEM images and elemental analysis by SEM-EDS spectra
for protocols (A–D) M1-P1, (E–H) M1-P2, (I–L)
M2-P1, (M–P) M2-P2 A, (Q–T) M2-P2 B, and (U–X)
M2-P2 C. Scale bars indicate 200 nm for SEM images and 1000 and 40
nm for TEM images.The addition of CaNT before
catalysis in M2 (Figure I–K,M–O,Q–S,U–W)
led to a reduction in particle size below 100 nm and consequently
a decrease in particle dispersion. BGNs produced according to the
M2-P1 method were observed in a size of around ∼86 nm, forming
aggregates with an average size of around 1–2 μm (Figure J), and presented
mesoporosity (Figure K, inset). The surface characteristics of M2-P1 BGNs were determined
by the analysis of nitrogen adsorption and desorption isotherms (Figure S1). The Brunauer–Emmett–Teller
(BET) technique confirmed the mesoporosity of M2-P1 with an average
pore diameter of 18 nm, the presence of smaller pore size (around
1.7 and 3 nm), and a surface area of 21.95 m2/g (Figure S1).The decrease in H2O concentration in solution B that
was used in the M2-P2 A protocol (Figure M–O) yielded a trimodal distribution
with an average particle size of around ∼70 nm (52%), ∼190
nm (39%), and ∼500 nm (9%) (Table ) and loss of mesoporosity compared to M2-P1.
Particle size was also affected by increasing the stirring time before
catalysis as it was applied in M2-P2 B (increase in X1 stirring duration time before the addition of CaNT and
solution B, Figure Q–S) and M2-P2 C (increase in X2 stirring time after the addition of CaNT and before the addition
of solution B, Figure U–W) in which both protocols produced BGN of ∼20 nm
that form aggregates of a size of ∼1 μm. However, there
was no significant difference in the particle size and aggregation
size for nanoparticles formed by M2-P2 B and C protocols. This observation
indicates that the increase in stirring time before the addition of
solution B is critical. However, no dependence was observed with regard
to which step before catalysis in that the stirring time is prolonged
(before or after CaNT (X1 or X2)). DLS and zeta potential were also performed to confirm
the particle size and surface charge in M2BGNs (Table S1). DLS tended to overestimate the sizes of the BGNs
similarly to the effect observed by Greasley et al.[37] and gave measurements of aggregate sizes rather than individual
nanoparticles. However, most DLS measurements are within an acceptable
range from those obtained in TEM.
Elemental
Composition Analysis of BGNs
Control over the elemental composition
of BGNs following a Stöber-like
method has remained a challenge for years. The composition analysis
of BGN particles was performed by SEM-EDS spectra. The spectra collected
are presented in Figure D,H,L,P,T,X with the calculated values being summarized in Table . Nanoparticles fabricated
by the reference protocol M1-P1 presented a significantly low incorporation
of P and Ca in agreement with published data.[36] The lack of phosphorous was attributed to the unbalanced hydrolysis
rate between TEOS and TEP under basic conditions. The faster hydrolysis
of TEOS caused nanoparticles to condense before the TEP had hydrolyzed,
resulting in pure SiO2 nanoparticles. This effect was overcome
in the M1-P2 synthesis protocol by allowing both hydrolysis reactions
to happen at comparable rates. Methanol served as a solvent in solution
A for this purpose since shorter carbon chains were expected to allow
TEP to dissolve faster. This effect was observed by de Oliveria et
al. in whose work the P content significantly increased by applying
methanol in BGN synthesis, although the nominal composition was still
unmatched.[42] The same effect was observed
here in M1-P2 and M2BGNs. Although EDS confirmed the incorporation
of P within the desired range in the BGN structure and allows us to
assess the effectiveness of the applied protocol toward incorporation,
the errors associated with this technique challenge the ability to
determine its exact composition. Future work will be performed using
ICP analysis to measure accurately the composition.
Table 2
Elemental Composition of BGN for Different
Processing Conditions (mol %)
However, the modification of solution A to use methanol
was still
insufficient to reach the intended CaO content in M1-P2. The compositional
gap observed for the calcium content is associated with their reported
mechanism of incorporation into the SiO2 structure. Calcination
above 400 °C is necessary to activate the diffusion of Ca2+ ions into the SiO2 network and consequently its
modification.[39] Because of this mechanism,
most protocols of BGNs suggest immersing previously developed SiO2 nanoparticles into a calcium nitrate bath in which Ca2+ ions would electrostatically attach to hydroxyl groups (OH–) at the nanoparticles’ surface. However, this
electrostatic interaction is weak and limited by the number of OH– available, which explains why CaO content has been
rarely above 10 mol % for BGNs.[36,37,40] The previously suggested approach to improve the incorporation of
calcium in this type of protocol[37] was
reproduced here in M1 where less than 7 mol % CaO was detected. Synthesizing
particles by the M2 protocol where CaNT has incorporated into solution
A prior to catalysis and stirring for a long enough time allows cation
interaction with SiO2 tetrahedra to increase the CaO content
up to 35 mol %. Particle size was also reduced below 100 nm.
Structure of BGNs
The structure of
BGNs was further assessed by FTIR, XRD, and NMR analysis. The FTIR
spectra in Figure show the evolution of the bond vibrations for the applied fabrication
protocols. All FTIR spectra present characteristic features of amorphous-like
structures. The spectra of M1 BGNs present a dominant SiO2 structure with vibration modes at 450, 805, 1000–1050, and
1200 cm–1 for Si–O–Si bending and
stretching. Additionally, the strong vibration of the Si–O–Si
stretching mode at 1000–1050 cm–1 overlaps
with the P–O bending at 1040 cm–1. The spectra
of M2BGNs present a modified SiO2 structure as indicated
by the development of a shoulder at the 900–1100 cm–1 region. This shoulder band at 900 cm–1, observed
in the spectra of all M2BGNs, is attributed to Si–O–nonbridging
oxygen (NBO) bonds, which confirm the presence of modifier ions (e.g.,
Ca2+) in the SiO2 network. The formation of
this vibration mode causes also the small shift of the peak at around
1050 cm–1 to lower wavenumber.
Figure 2
FTIR spectra presenting
nonmodified and modified SiO2 networks by Ca2+ ions for BGNs fabricated by M1 versus
M2 protocols, respectively.
FTIR spectra presenting
nonmodified and modified SiO2 networks by Ca2+ ions for BGNs fabricated by M1 versus
M2 protocols, respectively.Further structural analysis was performed by XRD. The BGNs fabricated
by M1 and M2 protocols present XRD patterns of amorphous structures
in agreement with FTIR spectra but with considerably different features
in the patterns among the different protocols (Figure a). These features were analyzed by fitting
the XRD patterns with Gaussian peaks for R2 = 0.99. Five Gaussian peaks were identified to fit the XRD patterns
with the maximum for each fitting peak at 2θ: 21.9° ±
0.6, 27.4° ± 0.5, 31.3° ± 0.2, 52.3° ±
3, and 70.3° ± 0.03 (Figure b). The area under each fitting curve was calculated,
and it was correlated with the evolution of the structure as ions
were incorporated into the SiO2 network (Figure c). As a general trend, the
peak with a maximum at 21.9° 2θ decreases significantly
in favor of the increase in the peak with a maximum at 27.4°
2θ. This trend was obvious when the XRD pattern of M1-P1BGNs
was compared to that of M1-P2BGNs where the only structural difference
was the incorporation of P ions in the structure. Finally, the fifth
peak with a maximum at 70.3° 2θ appears in the XRD patterns
of all M1 BGNs, while it disappears in the patterns of all M2BGNs,
and two other peaks appear with maxima at 31.1 and 52.3° 2θ
in the patterns of all M2-P2BGNs (Figure c). These changes in the XRD patterns could
be potentially assigned to the incorporation of Ca2+ ions
in M2BGNs that modified the SiO2 network compared to M1
BGNs where the network is barely modified due to the lack of calcium
content.
Figure 3
(a) XRD structural analysis, (b) Gaussian deconvolution, and (c)
evolution of the area in deconvoluted Gaussian peaks for M1-P1, M1-P2,
M2-P1, and M2-P2 A–C.
(a) XRD structural analysis, (b) Gaussian deconvolution, and (c)
evolution of the area in deconvoluted Gaussian peaks for M1-P1, M1-P2,
M2-P1, and M2-P2 A–C.The features observed in XRD revealed the presence of different
SiO2 coordinations being formed in the BGN structure. The
network connectivity was evaluated in terms of Q speciation for two
representative samples (M1-P2 and M2-P2 A) using 29Si MAS-NMR. Figure shows the chemical
shift (−δ) for Q4 (109–112 ppm), Q3 (100–102 ppm), Q2 (85–93 ppm), and
Q1 (76–79 ppm). Two different signals were identified
for Q2 species related to (1) silicon associated with hydrogen
(∼93 ppm) and (2) silicon associated with network modifiers
(∼85 ppm), in this case, calcium.[43] The structure of M1 BGNs that was dominated by the presence of Q4 and Q3 species represents most of the intensity
areas of the spectrum. However, M2BGNs were dominated by Q3 species and showed a significant increase in the total Q2 speciation compared to M1 BGNs. Building on these facts and considering
the composition in mol % detected in the synthesized BGNs, the network
connectivity (NC) was calculated from theoretical and experimental
models. While phosphorous can appear in both orthophosphate and forming
Si–O–P bridges, the most common status is the former.
To account for the exact influence of the phosphorous status in the
silicate network connectivity, 31P MAS-NMR studies would
be required to determine the number of orthophosphate (Q0) and Si–O–P bridges (Q1) in the BGNs. Orthophosphates
are associated with an increase in silicatepolymerization,[44] whereas Si–O–P bridges are known
to decrease the network connectivity of the glass.[45] Therefore, orthophosphates are accounted for the “no.
of BO”, while Si–O–P bridges would contribute
to the “no. of NBO” portion of eq . Because of the low level of P contained
in the synthesized BGNs (62 Si/3 P) and its preferable chemical bonding
to form orthophosphate units, the overall effect of Si–O–P
bridges in the presented BGN system would be minimum. Thus, the theoretical
model based on eq assumed
that phosphorous was present only as orthophosphate, neglecting the
small percentage of phosphorous in Si–O–P bridges.[46−52] Experimental network connectivity was obtained from the proportion
Q2/Q3 for M1-P2 and M2-P2BGNs, where Q2 = Q2H + Q2Ca.[53] The network connectivity values obtained from
the theoretical and experimental models are summarized in Table .
Figure 4
(a, b) Solid-state 29Si CP MAS-NMR
spectra for (a) M1-P2
and (b) M2-P2 A. Deconvoluted signal components are represented by
lighter color lines, with peak assignments displayed at the top of
the column.
Table 3
Network Connectivity
(NC) Based on
Theoretical and Experimental Models
protocol
theoretical
NC
experimental
NC
M1-P1
3.9
N.Aa
M1-P2
4
0.73
M2-P1
3.2
N.Aa
M2-P2
3.3
0.36
N.A, not applicable.
(a, b) Solid-state 29Si CP MAS-NMR
spectra for (a) M1-P2
and (b) M2-P2 A. Deconvoluted signal components are represented by
lighter color lines, with peak assignments displayed at the top of
the column.N.A, not applicable.These results allowed the correlation
of the Q speciation observed
in NMR and the amorphous structures observed in FTIR and XRD. The
BGNs fabricated by any M1 protocol presented XRD patterns with a higher
intensity at around 21.9° 2θ, while all M2BGNs showed
XRD patterns with a maximum intensity at around 27.4° 2θ.
Thus, a highly connective SiO2 network, with mainly Q4 species, could be correlated with the highest intensity XRD
peak at 21.9° 2θ in M1 BGNs, while less connectivity in
the SiO2 network, with significantly higher Q2 species, is correlated with an increase in the XRD peak at 27.4°
2θ, as observed in M2BGNs’ patterns.
Mechanism of Ion Incorporation
In
this work, the sol–gel process with one-step basic catalysis
was applied to synthesize BGNs in a ternary system without using polymeric
templates. Previously reported protocols showed that the collected
BGNs presented a significant drop in the incorporated P and Ca2+ ions compared to the nominal composition.[36] Here, P was incorporated in the M1-P2 synthesis protocol
by allowing the hydrolysis reactions of both TEOS and TEP to happen
at comparable rates. In this work, extended stirring was the key to
allow the incorporation of P into the silicate structure and achieve
the nominal concentration for P. Modifying the stirring time X1 (after the addition of TEP) from 4 to 24 h
proved that the nominal composition was only met in the latter, probably
because the hydrolysis of all TEP was not completed after 24 h (Figure S2). Figure shows the proposed mechanism of ion incorporation
during particle formation. Monodispersed BGNs were obtained by providing
a basic pH above the isoelectric point of the structure.[34] This approach offered the ability of P ion incorporation
without compromising particle size or dispersity. Particle diameter
became slightly smaller (from 437 to 425 nm) by utilizing methanol
as a solvent due to the shorter chain of alcohol.[42] The chemical modification introduced in this protocol was
insufficient to affect the surface charges caused by the increase
in pH. Thus, particle size and dispersity will be still controllable
by precisely tailoring water and ammonium hydroxide concentrations
as reported in other Stöber-like protocols.[37,54]
Figure 5
Proposed
mechanisms for P (light blue circle) and Ca2+ (red circle)
ions position within BGNs when M1-P2 and M2 protocols
are applied. Tetrahedra are formed by Si (green circle) and O (white
circle) ions in both protocols. In the case of protocol M1-P2, pure
silica nanoparticles are formed, and Ca ions remain on their surface
prior to calcination, while in protocol Μ2 prior to calcination,
Ca ions are already present within the nanoparticles. Calcination
in both protocols allows Ca ion incorporation into the glass structure
bridging oxygens (BO) and nonbridging oxygens (NBO) marked in purple.
Proposed
mechanisms for P (light blue circle) and Ca2+ (red circle)
ions position within BGNs when M1-P2 and M2 protocols
are applied. Tetrahedra are formed by Si (green circle) and O (white
circle) ions in both protocols. In the case of protocol M1-P2, pure
silica nanoparticles are formed, and Ca ions remain on their surface
prior to calcination, while in protocol Μ2 prior to calcination,
Ca ions are already present within the nanoparticles. Calcination
in both protocols allows Ca ion incorporation into the glass structure
bridging oxygens (BO) and nonbridging oxygens (NBO) marked in purple.The incorporation of calcium was also achieved
by introducing a
major change in the synthesis process. Calcium nitrate was added into
the solution and stirred for a long enough time to allow cation interaction
with SiO2 tetrahedra. Catalysis of the solution after 24
h not only caused nanoparticle formation but also allowed trapping
of Ca2+ ions within the structure. BGNs before calcination
at 400 °C presented 35 mol % CaO content in SEM-EDS and lacked
the Si–O–NBO vibration at 900 cm–1 in FTIR (Figure S3), demonstrating that
Ca2+ ions were only trapped within the BGNs. After calcination,
these trapped ions form Si–O–Ca NBO, modifying the SiO2 network, as observed in the FTIR and NMR spectra of M2BGNs.
Although the concentration of CaO was achieved at both stages, before
and after calcination, their status in the silica network was different
and leads to different behavior. For example, trapped Ca2+ will leach at an uncontrollable rate, while Si–O–Ca
NBO not only allows the controlled release of Ca2+ but
also accelerates the degradation of a silicate network since it is
less interconnected. Following our approach, not only the CaO content
was increased to the desired amount (35 mol %) but also the particle
size was also reduced. It is also worth noting that although the concentrations
of water and ammonium in the catalytic solution have previously shown
a critical effect on the final particle size,[37,54] here, the early addition of calcium nitrate before catalysis seemed
to neutralize their overall effect on nanoparticles’ size.
In fact, BGNs were collected after different stirring times X3 (after catalysis) from 5 min to 6 h, and all
presented similar sizes and composition (Figure S4).This study also indicates a significant effect of
stirring time
prior to catalysis and condensation in both the composition and size
of BGNs. Increasing the stirring time before catalysis allowed P and
Ca2+ ions to position around SiO2 tetrahedra.
The time allowed for solution homogenization was at least 24 h, and
further experiments would be required to determine the minimum time
for optimal ion incorporation. In this regard, the significance of
stirring time has been noticed in other works, although never highlighted
before. In particular, Lukowiak et al. achieved 28 wt % CaO in europium-doped
BGN in a two-step catalysis method by homogenizing the solution for
20 h,[38] whereas only 12 wt % was obtained
after 8 h.[55] Stirring solutions for a total
of 72 h before catalysis (as in M2-P2 B and C) yielded a significant
reduction in particle size. In this case, the long stirring not only
allowed ion incorporation but also affected the network connectivity.
The hydrolysis in the methanol solvent for an extended period made
Si–O–Sibonds more susceptible to chain breakdown during
catalysis. Furthermore, the additional stirring time allowed maximum
utilization of TEOS, TEP, and CaNT precursors, as proved by the higher
mass of material collected after calcination.
Bioactive
Behavior
The osteoconductive
potential of nanoparticles was assessed through in vitro biomineralization studies. The formation of the biological apatite
phase served as an indicator of bioactive glass behavior in a body
simulated scenario. The capability of the BGNs to form this apatite
phase was evaluated for M1, M2-P1, and M2-P2 ABGNs. Particles were
immersed in SBF at 37 °C under constant agitation to reproduce
body conditions. After 7 days, the formation of an apatite phase was
observed by FTIR (Figure , solid line) and compared to that before SBF (Figure , dashed like). For both M1
BGNs, the vibration peaks that confirm the presence of a calcium phosphate
phase after immersion in SBF are significantly lower than the respective
peaks for the spectra of M2BGNs. Nevertheless, the formation of this
deposition was evidenced in both M1 BGNs by the development of a broad
peak in the region of 575–620 cm–1 commonly
attributed to P–O bending. Particles fabricated by M2 protocols
presented the characteristic dual peak for P–O bending at 575
and 620 cm–1 that together with the carbonate group
bands at ∼873 and ∼1450 cm–1 confirmed
the formation of a carbonated calcium phosphate phase. The band at
∼1050 cm–1 was also slightly different in
M2BGNs before and after SBF, showing a better formed shoulder at
∼950 and ∼1200 cm–1 and an increase
in the sharpness of the peak at 1050 cm–1. These
features are attributed to a stronger P–O bending vibration
in the structure caused by the increase in P–O bonds during
apatite deposition.
Figure 6
FTIR spectra of BGNs fabricated by M1-P1, M1-P2, M2-P1,
and M2-P2
A protocols after 7 days of immersion in SBF (solid line) compared
to the respective spectra before SBF (dashed line).
FTIR spectra of BGNs fabricated by M1-P1, M1-P2, M2-P1,
and M2-P2
A protocols after 7 days of immersion in SBF (solid line) compared
to the respective spectra before SBF (dashed line).The ability to develop the biological apatite phase was found
weaker
for M1 BGNs than for M2BGNs as a consequence of nanoparticles’
composition and size. The mechanism of apatite formation in BG is
attributed to the accumulation of dissolution products.[56] Initially, P and Ca2+ ions are exchanged
in solution, leaving an increased concentration of silanolbonds (Si–OH)
at the surface of nanoparticles. Then, silanols are repolymerized,
creating a silica-rich layer. Further ion migration of P and Ca species
takes place from the core of the particle toward the surface and reacts
to create an amorphous calcium phosphate layer. The supersaturated
solution causes the deposition of hydroxyl and carbonate groups as
well as more P and Ca2+ ions and later the crystallization
of the calcium phosphate phase to hydroxycarbonate apatite (HCA).[56−58] The rate of HCA layer formation was greatly influenced by BG composition.
The substitution of Si by other ions such as P and the modification
of the network by Ca2+ ions created a less connected network
in which hydrolysis of Si–O–Si is not necessary for
the dissolution of silicate chains.[7] BGNs
fabricated by M2 protocols exhibited half network connectivity (NC)
than M1 BGNs protocols as a consequence of higher calcium incorporation,
and thus, they undergo a faster bioactive response. The NC was below
the ideal reported by Edén (2 < NC < 2.6) and insufficient
to generate a dense apatite phase after 7 days in SBF.[59] Despite the low calcium content in M1 BGNs,
a calcium phosphate deposition was observed. This result is in agreement
with previous reports that proved bioactive behavior of sol–gel
glasses with up to 90 mol % SiO2.[60] The bioactive response is also affected by the particle size.[61,62] A lower particle size induces a higher ion dissolution rate due
to the higher surface to volume ratio. Thus, ion release in M2BGNs
(particle size, <100 nm) is intrinsically higher than that in M1
protocols (∼400 nm).
Conclusions
In this study, a sol–gel method was optimized to incorporate
P and Ca2+ ions in the structure of BGNs, achieving for
the first time the nominal composition. The role of the order in which
reagents were added, the concentrations in the catalytic solution,
and the stirring time before catalysis were evaluated in terms of
the final particle size, composition, and structure. The incorporation
of P ions was achieved by utilizing methanol for the hydrolysis of
TEP and long stirring time. The incorporation of calcium in amounts
higher than 20 mol % was accomplished by adding calcium before catalysis
and the SiO2 condensation reaction. This process also causes
particle size reduction below 100 nm. Long stirring times were required
to ensure the reaction between ionic species and SiO2 tetrahedra.
Despite their aggregation in microsized clusters, BGNs below 100 nm
proved nanoscale properties as evidenced by the faster bioactive response.
This faster reactivity, a consequence of the high surface area, and
the bioactive properties emphasize the potential of these particles
for tissue engineering application.
Experimental
Procedure
Materials
Particle synthesis was
performed with analytical grade tetraethyl orthosilicate (TEOS), triethyl
phosphate (TEP), calcium nitrate tetrahydrate (CaNT), and 28–30%
ammonium hydroxide (NH4OH) solution purchased from Sigma-Aldrich.
The solvents used were distilled water, 200 proof ethyl alcohol, and
methanol. All reagents were used as received without further purification.
Preparation of Bioactive Glass Nanoparticles
(BGNs)
Bioactive glass nanoparticles with a nominal composition
of 62 SiO2–34.5 CaO–3.2 P2O5 (in mol %) were prepared using the sol–gel process
with one-step basic catalysis. Various experiments were conducted
to investigate how different processing parameters, such as (1) the
type of solvent, (2) the addition order of the CaNT, and (3) the relative
concentrations of the components in the catalytic solution (solution
B), affect the fabricated nanoparticles. The layout of the synthesis
protocols is illustrated in Figure . Initially, two solutions were prepared. Solution
A containing 41.6 mL of solvent (ethanol (M1-P1) or methanol (M1-P2
and M2)), 5.55 mL of TEOS, and 0.5 mL of TEP in a Teflon beaker was
stirred for a specific time (X1). The
catalytic solution was named as “solution B” and prepared
by mixing distilled water and 28–30% ammonium hydroxide in
ethanol. The ratios of the concentrations (in molarity, M) of the
reagents (H2O and NH4OH in ethanol) used for
solution B are summarized in Table . All processes were performed at room temperature
under vigorous stirring (∼500 rpm). All solutions were covered
in beakers with parafilm.
Figure 7
Layout of the fabrication methodologies M1 and
M2 where CaNT is
added after or before solution B, respectively.
Table 4
Applied Protocols with the Type of
Solvent Used in Solution A and the Components with the Ratios Used
in Solution B
Layout of the fabrication methodologies M1 and
M2 where CaNT is
added after or before solution B, respectively.Method 1 (M1)
has been previously reported by Zheng et al.[36] and is utilized here as a reference for the
later systematic modifications. Briefly, solution B was incorporated
into solution A and stirred for 30 min before the addition of 3.14
g of CaNT. Particles were collected after 2 h of stirring duration.
The effect of the type of the solvent was also investigated by using
ethanol (M1-P1 as described by the Zheng et al. protocol) or methanol
(M1-P2) as an alternative solvent in solution A.Method 2 (M2)
studies the effect of changing the order in which
CaNT is added in solution A by incorporating this reagent before the
incorporation of solution B. Methanol was used as the solvent constantly
in M2 because of the advances shown in M1-P2. After the addition of
3.14 g of CaNT into solution A, the solution was under stirring duration
for X2 amount of time and then, the collection
of particles was happening 24 h after solution B was incorporated
into solution A.The effect of the catalyst (solution B) was
studied by modifying
the concentration (in M) of H2O and consequently the relevant
ratios of H2O/TEOS and H2O/ethanol in all M2-P2
protocols from that of M1, as reported in Table . Additionally, the effects of the stirring
durations (X1 and X2) before the addition of solution B in the size of the collected
particles were evaluated for M2-P2 protocols as it is presented in Figure . The effect of the
stirring duration time after catalysis on particle composition and
size for M1 protocols is not reported in this work as it has been
previously explored by other research groups,[36,63] while no effect on particle size and composition was observed for
all M2 protocols with different stirring duration times after catalysis
(data presented for M2-P1 in the Supporting Information).All particles were collected by centrifugation at 3000 rpm
for
3 min. The collected particles were then heat-treated at 60 °C
for 6 h, calcinated at 700 °C for 2 h with a 2 °C/min heating
rate, and cooled down to room temperature with 5 °C/min. The
collected powder was additionally mortar pulverized, washed with ethanol
twice to remove calcium-rich areas, and air-dried before characterization.[37]All fabrication protocols were applied
three times, and the number
of samples under characterization from each group was three.
Morphological and Elemental Evaluation
The morphology
of the BGN was observed using a scanning electron
microscope (ZEISS FIB-SEM) operated at 3 kV. Elemental analysis was
performed at 15 kV using another SEM instrument (MIRA3 TESCAN FEG-SEM)
equipped with an EDS detector. Powder samples were spread on carbon
tape to avoid interference from the substrate in the elemental analysis.
All SEM samples were Pt sputter coated for 30 s. The compositions
reported here are the average result of three scans at different regions
of the samples.
Particle Size and Distribution
The
particle size and the size of distribution were investigated using
transmission electron microscopy (JEOL 100 TEM) operated at 100 kV.
Ethanol was used to disperse the BGNs through sonication, and 5 μL
of the solution was pipetted in a 200 mesh C-coated Cu grid.
Structural Assessment and Surface Charge
Structural
analysis was performed with Fourier transform infrared
(FTIR) spectroscopy for wavenumbers in the range of 400–2000
cm–1 in the transmittance mode. Additionally, the
microstructure of the BGNs was examined by X-ray diffraction analysis
(Rigaku Smartlab XRD) using Cu Kα radiation at 40 kV/40 mA.
Data were collected in the 2θ range of 15–70° with
a stepsize of 0.1°. The evolution of the amorphous structure
was approached by curve fitting the experimental spectra with Gaussian
peaks for an R2 value of 0.99. The coordination
of silicon in the synthesized samples was evaluated with 1H → 29Si magic angle-spinning (MAS) solid-state
nuclear magnetic resonance (NMR). The NMR spectra were recorded on
a Varian Infinity Plus 400 spectrometer. Samples were spun in a 5
mm probe at 5 kHz for a spectrometer frequency set to 79.49 MHz. All
spectra were collected using a proton-enhanced cross-polarization
(CP) method with a contact time of 1 ms. The recycle time between
successive accumulations was 5 s, and the total number of scans was
17,000 for all spectra.
In Vitro Formation of an
Apatite Phase
The bioactive behavior of the particles was
assessed in terms of the apatite-forming ability with an immersion
test in Kokubo’s simulated body fluid (SBF).[64] Samples were prepared with a BGN/SBF weight ratio of 3.33:1
and then placed in an incubator at 37 °C under constant shaking
(175 rpm). After 7 days, the solution was centrifuged, and particles
were rinsed with 100% ethanol, dried at 37 °C, and stored for
analysis. The presence of the hydroxycarbonate apatite (HCA) layer
was evaluated using FTIR.
Authors: Olga Tsigkou; Sheyda Labbaf; Molly M Stevens; Alexandra E Porter; Julian R Jones Journal: Adv Healthc Mater Date: 2013-07-05 Impact factor: 9.933
Authors: Agda Aline Rocha de Oliveira; Dickson Alves de Souza; Luisa Lima Silveira Dias; Sandhra Maria de Carvalho; Herman Sander Mansur; Marivalda de Magalhães Pereira Journal: Biomed Mater Date: 2013-03-15 Impact factor: 3.715