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Confined mesoporous silica membranes for albumin zero-order release
Nicola Gargiulo, Ilaria De Santo, Filippo Causa, Domenico Caputo, Paolo
Antonio Netti
PII: S1387-1811(12)00216-8
DOI: 10.1016/j.micromeso.2012.04.003
Reference: MICMAT 5470
To appear in: Microporous and Mesoporous Materials
Please cite this article as: N. Gargiulo, I. De Santo, F. Causa, D. Caputo, P.A. Netti, Confined mesoporous silica
membranes for albumin zero-order release, Microporous and Mesoporous Materials (2012), doi: 10.1016/
j.micromeso.2012.04.003
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Confined mesoporous silica membranes for
albumin zero-order release
Nicola Gargiuloa,*, Ilaria De Santoa,b,*, Filippo Causaa,c, Domenico Caputoc, Paolo
Antonio Nettia,b,c
a Centro di Ricerca Interdipartimentale sui Biomateriali, Università Federico II, P.le
Tecchio 80, 80125 Napoli, Italy
b Centre for Advanced Biomaterials for Health Care, Italian Institute of Technology,
Largo Barsanti, 80125 Napoli, Italy
c Dipartimento di Ingegneria dei Materiali e della Produzione, Università Federico II,
P.le Tecchio 80, 80125 Napoli, Italy
* These two authors contributed equally to this work.
Corresponding author: Domenico Caputo (e-mail: domenico.caputo@unina.it; address:
Dipartimento di Ingegneria dei Materiali e della Produzione, Università Federico II, P.le
Tecchio 80, 80125 Napoli, Italy; telephone: +397682396; fax: +397682394)
Abstract
In this work, the transport capabilities of anodic alumina membranes confining
SBA-15-like nanochannels in their pores were investigated. The mean pore size of the
confined mesophase was set around 7.0 nm, thus to achieve single passage of the
selected Bovine Serum Albumin (BSA) protein, having comparable hydrodynamic
diameter, through the nanochannels. Shape, size and orientation of the manufactured
mesophase were characterized by means of small-angle X-ray scattering, transmission
electron microscopy and N2 adsorption / desorption at 77 K. The usage of
mesostructure-containing samples having pore tuned over the size of the released BSA
allowed achieving a long-term zero-order release profile by single-file diffusion up to
several weeks, which delivers a constant amount of drug by unit time independently
from drug concentration and drug accessible area, while control anodic alumina
membranes showed a classic Fickian diffusion release. The attained BSA constant
release rate was about 2 μg/day. The possibility of rate tuning could be further exploited
by varying the length of the siliceous nanochannels inside the alumina pores, i.e.
through different amounts of mesostructure filling the host support.
Keywords: Mesoporous materials; Drug delivery; Confined diffusion; Zero-order
release
1. Introduction
The morphological control of porous systems on the nanoscale is a field of research that
recently turned out to be very active. In fact, the development of structures consisting in
ordered arrays of oriented nanochannels would allow to efficiently perform operations
such as the inclusion synthesis of a vast range of nanowire systems through hard
templating, the separation of large biomolecules, or the long-term and controlled
delivery of drugs. A shining example of such structures that is subject of many recent
research activities is represented by hierarchical systems made of mesoporous siliceous
materials confined in the channels of anodic alumina membranes (AAMs) [1, 2]. In
these systems the silica-surfactant nanocomposite is assembled at the alumina pore
walls to form the surfactant-templated silica-nanochannels which are typical of such
mesostructures. These materials can be synthesized by different methods, the most
investigated of which relies on the so-called evaporation-induced self-assembly (EISA)
[3]. In one of the first studies about mesoporous silica confined in AAMs by EISA,
different porous alumina membranes having distinct channel diameters (i.e., from 18 to
80 nm) were used as substrates and dip-coated with a synthesis solution containing
Pluronic P123 as templating agent. The development of different mesostructures (from
single chains of spherical mesopores to concentric or chiral helical mesopores) was
found to depend from the different diameters of the hosting alumina nanochannels [4].
More recently, Bein and coworkers conducted thorough experiments on the formation
of mesophases inside AAMs by means of two-dimensional small-angle X-ray scattering
(2D SAXS) and transmission electron microscopy (TEM) [5]. These studies were then
deepened by performing grazing incidence SAXS (GISAXS) measurements [6], by
formulating a possible formation mechanism for the confined mesostructure [7] and by
investigating the influence of the addition of inorganic salts on the orientation of the
channels in confined mesoporous silica templated by non-ionic triblock copolymer
surfactants [8].
Later on, Bein and coworkers also considered possible applications of confined silica
mesostructures as drug delivery systems (DDSs). These studies reported the adsorption
and the in vitro release kinetics of mesostructure-containing AAMs previously loaded
with vancomycin [9] or ibuprofen [10], showing that so-called hexagonal columnar
systems (i.e., systems in which the cylindrical pores of the confined phase are straight
and parallel to those of the hosting AAM [1]) attain a slower release over an extended
time period, and pointing that major parameters affecting drug release are pore shape,
accessibility, length, and diameter compared to that of the eluting molecule. Indeed, the
release or adsorption of bioactive agents from mesoporous materials depends in a
complex way from the physicochemical properties of both the biomolecule and the
device. Furthermore, the dynamic behavior of the transported molecules depends in turn
on the surface chemistry and size of the pores.
Although the reported works already tested mesostructure-containing AAMs as drug
carriers, none were devoted to the assessment of their transport properties as drug
delivery membranes. The most appropriate configuration of the confined mesophase for
this kind of application is represented by the hexagonal columnar orientation, which can
also be tailored in pore size on the nanometric scale by accurately choosing the
templating non-ionic tri-block copolymer surfactant (e.g., Brij 56 instead of Pluronic
P123 [8]). Indeed, the exploitation of mesostructure-containing AAMs as drug delivery
membranes could be advantageous for the long-term delivery of biomolecules, proteins
in particular. Among the diverse release mechanisms, the most fruitful for
pharmaceuticals applications consists in the zero order release mechanism, which
delivers a constant amount of drug by unit time independently from drug concentration
and drug accessible area [11]. Zero order release can be achieved through a single file
diffusion mechanism of molecules trafficking in a pore having similar size. Indeed, the
single-file diffusion of the released molecule is made possible when the diameter of the
constraining 2D geometry in the membrane is smaller than twice the size of the released
molecule, and, as a result, the effective release rate becomes constant with time due to
the single molecule passage [12].
Recent studies have already demonstrated single-file diffusion of protein drugs through
nanoprous membranes. In particular, membranes consisting of cylindrical block
copolymers nanochannels were developed and obtained single-file diffusion of proteins
through the fine-tuning of the pore membrane over the size of the bioactive agent to
release [13]. The pore size was indeed precisely modulated to that of the released agents
through Au deposition. Other groups showed the constant release rate of proteins
through nanoporous silicon membranes having a slit shaped pore nanometric in height,
although obtained through multiple steps of precision silicon fabrication techniques on
silicon-on-insulator substrates [14].
Here, we investigated the transport capabilities of AAMs confining SBA-15-like
columnar nanochannels in their pores (SBA-15-AAMs). The mean pore size of the
manufactured SBA-15-AAMs was set around 7.0 nm, and showed the long-term
capability of zero-order release of the fluorescent BSA proteins (molecular size 7.2 nm)
up to several weeks.
2. Experimental
2.1 Synthesis of AAM-confined mesoporous silica
The confinement of mesoporous silica in AAMs was performed following the procedure
reported in [8]. First, 2.08 g of tetraethyl orthosilicate (Aldrich) were mixed with 3.00 g
of a 0.2 M HCl (J. T. Baker) aqueous solution, 1.80 g of H2O and 4.00 g of ethanol
(Fluka). This mixture was then heated at 60 °C for 1 h to achieve acid-catalyzed
hydrolysis-condensation of the silica precursor. The pre-hydrolyzed silica was then
mixed with 0.75 g of the non-ionic triblock copolymer surfactant Pluronic P123
(Aldrich) that was preliminarily dissolved in 11.85 g of ethanol. In order to achieve the
hexagonal columnar orientation of the mesoporous siliceous channels, 0.085 g of LiCl
(Aldrich) were added to the resulting mixture [8]. The AAMs used (Anodisc, Whatman)
have a diameter of 13 mm and an average pore size of 200 nm. Two drops of the
precursor mixture were homogeneously spread on the membrane surface and let to
evaporate at 30 °C at about 50% relative humidity. Mesostructure-containing
membranes were then calcined using a heating rate of 0.5 °C/min with annealing
periods of 10 h at 120 °C, and 5 h at 200, 300 and 500 °C, respectively. Because the
confined phase may be thought to resemble SBA-15 mesoporous silica in both its
structure and textural properties [15], the final product was labeled as SBA-15-AAM.
2.2 Characterization of SBA-15-AAM
SBA-15-AAM samples were characterized with SAXS by means of an Anton Paar
SAXSess instrument operating in point-collimation mode with a Genix Microsource
X-ray generator (CuKα radiation) at 50 kV and 1 mA. The experimental setup is similar
to that reported in [8]: in detail, SBA-15-AAM samples were stuck onto a Variostage
X-Rotation cell using a small amount of vacuum grease; the tilting angle was set to 10°
and the data collection was performed in 5 exposures of 120 s each that were
successively averaged into one image.
Moreover, TEM images of SBA-15-AAM samples were collected by means of a Philips
EM 208 instrument equipped with a MegaView camera. Prior to the observation,
membrane samples were embedded within resin and then ultramicrotomied.
In order to analyze the pore structure of the synthesized hierarchical structure, partially
ground samples of SBA-15-AAM were submitted to nitrogen adsorption/desorption at
77 K by means of a Micromeritics ASAP 2020 apparatus. The density functional theory
(DFT) pore size distribution was determined modeling experimental adsorption data
with a kernel function for oxide materials having cylindrical pore geometry.
2.3 Release experiments
In order to assess protein release through nanochannels, SBA-15-AAMs were glued by
a cyanoacrylate solution onto Transwell support, in place of the original membrane,
and between two reservoirs. Control Anodisc membranes, having 200 nm pore size,
were attached to a Transwell support in the same way. The proposed experimental
system envisages the uniaxial flow of biomolecules through the mesoporous membrane.
The membrane separates an initially filled biomolecules-containing reservoir from a
phosphate buffered saline (PBS) solution environment where biomolecules are depleted.
Before loading, membranes were preconditioned in 30% ethanol solution for thirty
minutes and then put in water for about ten days. After preconditioning, the volume
above the membranes was filled with 0.5 ml of 2.5 M fluorescent
BSA-TetraMethylRhodamine protein solution (Molecular Probes, MW 67 kDa),
whereas the lower volume contained 2 ml of PBS plus 0.03% sodium azide. The release
system was kept at 23 °C on a 50 rpm shaking plate. Protein concentration in the lower
reservoir was measured by means of a Perkin-Elmer Spectrofluorimeter (485-535 nm).
The BSA concentration was determined from a 100 L solution aliquot removed from
the sink reservoir and replaced with an equal amount of fresh PBS plus 0.03% sodium
azide at intervals of approximately 48 h and followed up to two months.
3. Results and discussion
3.1. Characterization of SBA-15-AAM
Fig. 1 shows the SAXS pattern of a SBA-15-AAM sample: as reported in the literature
[8], SAXS measurements on siliceous mesostructures confined in AAMs usually result
in diffraction patterns with two or four visible first-order reflections that can be
correlated to the orientation of the mesoporous channels with respect to the
macroporous ones of the hosting AAM. The reflections in the horizontal plane of the
primary beam are called in-plane (ip) reflections, and are detectable when the hexagonal
columnar orientation occurs, but also when the mesophase assumes a closed,
donut-shaped circular configuration [1]. The reflections out of the horizontal plane are
called oop reflections and occur only in correspondence of the circular orientation.
When ionic surfactants (such as cetyltrimethylammonium bromide) are used as
templates for the assembly of the confined phase, the process spontaneously leads to the
hexagonal columnar arrangement of the mesostructure [5]. On the contrary, when using
non-ionic triblock copolymer surfactants (e.g., Pluronic P123) as templates, the
assembly evolves towards the circular phase. The addition of an inorganic salt (LiCl) to
the P123-based sol allows to mimic the behavior of a sol based on an ionic surfactant:
by this way, the resulting confined mesostructure will be characterized by a high
accessible porosity due to its columnar orientation, and also by a high pore size due to
the usage of a long-chain, non-ionic surfactant as template. These observations are
confirmed by the analysis of Fig.1, in which the scattering pattern of the SBA-15-AAM
sample shows distinct ip reflections at a value of the scattering vector q of about
0.51 nm-1 (corresponding to a d-spacing of 12.3 nm), and only weak oop reflections
with almost the same d-spacing (~12.7 nm). As a consequence, the mesophase is mainly
hexagonal columnar, with only a small fraction of hexagonal circular domains: this
result is well comparable with others reported in the literature [8].
[Figure 1]
Fig. 2 shows a TEM image of a SBA-15-AAM sample, in which one of the
200 nm-wide pores of the AAM is filled with the siliceous mesostructure. In previous
papers dealing with similar topics [8], TEM observations consisted in top views of the
membranes, and the samples were prepared by dimple grinding and successive ion
milling. On the contrary, in this case, the sample was embedded within resin and then
ultramicrotomied: this approach, though basically more destructive than the
aforementioned one, allowed to directly observe a cross section of the membrane. In
Fig. 2, the hexagonal columnar orientation of the mesoporous siliceous channels is
clearly visible, confirming what already pointed out from SAXS experiments.
Moreover, the adherence of the confined phase to the AAM channel surface is plainly
demonstrated: as reported in the literature [8], when the confinement of the
P123-templated mesostructure is performed without the addition of inorganic salts to
the precursor sol, the resulting circularly oriented phase turns out to be significantly
detached from part of the wall of the hosting macropores after the assembly process;
such phenomenon is further stressed after the calcination treatment. On the contrary, the
presence of LiCl in the synthesis environment, apart from promoting the columnar
orientation of the siliceous channels, aids to protect the confined phase from such
detachment during both the gelation and the template removal steps.
[Figure 2]
Fig. 3 shows the N2 adsorption/desorption isotherm at 77 K on partially ground samples
of SBA-15-AAM: the shape of the isotherm is coherent with what reported in the
literature [8]. In particular, it is classifiable as IUPAC type IV, which is typical of
mesoporous materials [16]; moreover, a H1-type hysteresis loop is highlighted. The
BET specific surface area turned out to be about 40 m2/g, in fair accordance with the
literature: such result seems odd if compared with those (one order of magnitude higher)
usually associated to bulk mesoporous silica particles, but becomes plausible when
considering that the mesophase content inside the composite membrane may be as low
as 10 wt% [8].
[Figure 3]
Fig. 4 shows the DFT pore size distribution of partially ground samples of
SBA-15-AAM obtained from modeling of experimental data reported in Fig. 3. Again,
the results are coherent with those reported in the literature [8]: the distribution has a
main peak at about 7.0 nm, that actually corresponds to the pore size of the confined
mesostructured phase. The tail that follows such peak in Fig. 4 may be related to defects
originated during the grinding process, but also by the occasional merging of silica
pores. This phenomenon may be considered as a side effect of the increased interactions
of the mesophase with the alumina channel walls due to the addition of an inorganic salt
to the synthesis system. In fact, while in the absence of LiCl the mechanical stress
caused to the circularly oriented siliceous channels during the calcination process leads
to the detachment from the alumina pore walls, the columnar phase originated in the
presence of the inorganic salt remains attached to the alumina, and the mechanical stress
related to the thermal treatment propagate to the silica structure, causing the rupture of a
small fractions of its pore walls [8].
[Figure 4]
3.2. Release experiments
Bovine Serum Albumin (BSA) protein was selected for the evaluation of the transport
properties of the manufactured membrane. Indeed, BSA is characterized by a molecular
weight of 67000 Da and a hydrodynamic diameter of around 7.2 nm [17], which is close
to the main peak value of the mesopore size distribution of SBA-15-AAM samples. The
quality of BSA release profile through SBA-15-AAM was assessed through the
evaluation of the time-dependent transport of proteins across a membrane mounted in a
Transwell support. Fig. 5 shows the release profile of BSA through SBA-15-AAM,
and through the control alumina membrane. Open circles represent the released BSA
amount from the control AAM having nominal pore size of 200 nm, while full stars the
quantity released from a SBA-15-AAM with a mean pore size of around 7.0 nm. No
significant time lags are recognized in Fig. 5, which were instead present in absence of
membranes preconditioning (data not shown).
[Figure 5]
The constant release profile of BSA is obtained in SBA-15-AAM, whereas a classic
Fickian diffusion release profile is obtained for the AAM. In the case of AAM, the
release profile has been adjusted following the mass balance, which applies under the
assumption of Fickian diffusion for a quasi-stationary process [18] reported below:
ln 1− C(t) /C(∞)[ ] = − DnAp /L( )× 1/V1 +1/V2( )× t (1)
In Eq. (1), C(t) is the protein concentration in the sink reservoir at a time t, C(∞) is the
concentration of the system at infinite time, D is the protein diffusion coefficient in the
pores, n and Ap are the number of pores and their section respectively, L represents the
membrane thickness, V1 and V2 are the source and sink volumes.
The BSA diffusion coefficient in AAM could be roughly esteemed from Eq. (1),
attaining 3.5E-9 cm2/s, which is around two orders of magnitude smaller than in bulk,
6E-7 cm2/s. Since the ratio of molecule diameter over pore size is in this case 0.04, such
a reduction of diffusion coefficient cannot be uniquely ascribed to constrained diffusion,
and could be rather due to an over esteem of the pore number in AAMs, which are
declared having a broad pore density range.
On the other hand, in the case of SBA-15-AAM the BSA release profile exhibits a clear
zero order release, which follows the equation
Qt = Q0 + K0 × t (2)
where Qt is the protein amount dissolved at time t, Q0 is the initial amount of drug in the
solution, and K0 is the zero order release constant independent of the solvent accessible
area.
In particular, since during the first two days of observation, the release curve of
SBA-15-AAM shows a higher slope compared to the longer times, probably ascribable
to low sensitivity of the reading apparatus, the linear fit of the profile in Fig. 5 is
evaluated from day three of release attaining a 0.990 r-square, which suggests a zero
order release rate of 1.83 μg/day, and the total released quantity is around 70% of the
protein loaded in the source. Indeed, BSA proteins have comparable size of membrane
pores, of about 7.0 nm. This condition justifies a zero order release rate by the single
file passage of molecules through the nanochannel. This size effect has to be coupled to
considerations regarding surface interactions, which of course cannot be neglected in
the case of high surface to volume ratios accomplished by nanoporous geometries [19].
Indeed, since BSA isoelectric point is 4.7, albumin shows a net negative charge of about
-17e at pH 7. This would suggest that also electrostatic repulsion between a negative
charged SBA-15 inner surface [20] and BSA, avoiding adsorption [21], could play a
determinant role in the zero order release shown.
Zero order release is highly desired in pharmaceuticals applications, since guarantees
constant release rate independently from reservoirs concentrations. Our formulation
attained a constant rate of about 2 μg/day, which is on the same order of magnitude of
what obtained in nanofluidic membranes [22]. This rate could be tuned to satisfy the
small dosages required for long term therapies such as growth factor delivery, useful in
tissue engineering applications for different tissues repair aims, such as vascularization
and bone regeneration. Growth factors as vascular endothelial VEGF and bone
morphogenetic proteins BMPs, control self-renewal, migration, differentiation as well
as other cell fate processes of progenitor cells. In vascularization as well as osteo-
regenerative processes, the release rates are indeed preferably around 100 ng - 10
µg/day/cm3 of injured tissue [23].
However, the obtained rate could be further optimized and adjusted on the specific drug
dosage required for the considered application by fine-tuning the exposed membrane
surface. Otherwise, the amount of silica precursor solution used in the initial sol
quantities, could be lowered thus attaining higher release rates by decreasing the length
of the siliceous nanochannels inside the alumina pores, i.e. filling less alumina
membrane thickness. Indeed, it would be ideally possible to tune the release slope, thus
release velocity, by confining less mesostructure inside the alumina pore in order to
change the effective thickness of the mesoporous channel system.
Since zero order release induced by single molecule passage can be achieved as soon as
the diameter of the constraining 2D geometry in the membrane is smaller than twice the
size of the released molecule, the manufactured pore size of SBA-15-AAM could be
used to perform zero order release of several other proteins, including hemoglobin and
human insulin (hydrodynamic diameters 7.0 and 5.4 nm, respectively). Indeed, the
dimensional range explored covers most of large proteins of pharmaceutical interest,
which the tested BSA belongs to. In addition, it was shown already the achievement of
confined mesoporous silica membranes of about 5.0 nm pore size in the presence of
ionic surfactants (i.e. cetyltrimethylammonium bromide [8-10]). These membranes
could be tested to obtain single passage of smaller proteins, such as lysozyme and
chymotrypsinogen (hydrodynamic diameters 3.8 and 4.8 nm, respectively).
Moreover, it would be interesting to explore the possibility to expand the pores of
SBA-15-AAM by modifying the starting sol, for applying the manufactured membrane
to even larger proteins such as apoferritin and thyroglobulin (hydrodynamic diameters
16.4 and 20.2 nm, respectively).
Different works already demonstrated zero order release for BSA diffusing in
nanochannel of nanometric height, though this result was never achieved so far for
mesoporous membranes produced by EISA. The major advantage in this configuration
is the relatively ease of manufacturing compared to costly and time-consuming
production schemes developed for the microprocessor industry.
4. Conclusions
Samples of anodic alumina membranes confining SBA-15-like nanochannels in their
pores were successfully synthesized and characterized by means of small-angle X-ray
scattering, transmission electron microscopy and N2 adsorption / desorption at 77 K.
SAXS and TEM measurements confirmed the hexagonal columnar orientation of the
mesoporous siliceous channels hosted by the 200 nm-wide alumina pores. The mean
pore size of SBA-15-AAMs, as confirmed by microporosimetric analysis, was set
around 7.0 nm, which is comparable with the hydrodynamic diameter of the Bovine
Serum Albumin protein selected for release testing.
Long-term zero order release of BSA through SBA-15-AAM samples was demonstrated
up to several weeks, obtaining a release rate of about 2 μg/day. The possibility of tuning
the release rate through different amounts of AAM-filling mesostructure could be
exploited. Further investigations are needed in order to test protein biological activity
intactness after several weeks of protein-mesostructure interaction. These findings claim
a deeper insight into transport phenomena through confined silica mesopores in order to
better design drug delivery systems.
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Figure captions
Figure 1. SAXS pattern of SBA-15-AAM evidencing in-plane (ip) and out-of-plane
(oop) reflections.
Figure 2. TEM image of SBA-15-AAM.
Figure 3. N2 adsorption (solid symbols) / desorption (open symbols) isotherm at 77 K
on partially ground SBA-15-AAM samples.
Figure 4. DFT differential pore size distribution of partially ground SBA-15-AAM
samples.
Figure 5. Release profiles of BSA through SBA-15-AAM (full stars) with a pore size of
7.0 nm, and through the supporting AAM with a nominal pore size of 200 nm (open
circles).
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