RESEARCH PAPER
Flow field-flow fractionation and multi-angle light scattering
as a powerful tool for the characterization and stability evaluation
of drug-loaded metal
–organic framework nanoparticles
Barbara Roda
1,2
&
Valentina Marassi
1
&
Andrea Zattoni
1,2
&
Francesco Borghi
1
&
Resmi Anand
3
&
Valentina Agostoni
4
&
Ruxandra Gref
4
&
Pierluigi Reschiglian
1,2
&
Sandra Monti
3
Received: 15 March 2018 / Revised: 22 May 2018 / Accepted: 29 May 2018
# Springer-Verlag GmbH Germany, part of Springer Nature 2018
Abstract
Asymmetric flow field-flow fractionation (AF4) coupled with UV-Vis spectroscopy, multi-angle light scattering (MALS) and
refractive index (RI) detection has been applied for the characterization of MIL-100(Fe) nanoMOFs (metal
–organic frameworks)
loaded with nucleoside reverse transcriptase inhibitor (NRTI) drugs for the first time. Empty nanoMOFs and nanoMOFs loaded
with azidothymidine derivatives with three different degrees of phosphorylation were examined: azidothymidine (AZT, native
drug), azidothymidine monophosphate (AZT-MP), and azidothymidine triphosphate (AZT-TP). The particle size distribution and
the stability of the nanoparticles when interacting with drugs have been determined in a time frame of 24 h. Main achievements
include detection of aggregate formation in an early stage and monitoring nanoMOF morphological changes as indicators of their
interaction with guest molecules. AF4-MALS proved to be a useful methodology to analyze nanoparticles engineered for drug
delivery applications and gave fundamental data on their size distribution and stability.
Keywords Flow field-flow fractionation . Multi-angle light scattering . Metal
–organic frameworks . Azidothymidine . NRTI .
Metal
–organic framework nanoparticles characterization
Introduction
One of the most used strategies in HIV therapy is the inhibi-
tion of retrotranscription and synthesis of proviral DNA. The
class of drugs which exert such a function are the nucleoside
reverse transcriptase inhibitors (NRTIs), among which azido-
thymidine (AZT) is the most used. It has been demonstrated
that NRTIs exert their antiretroviral activity via metabolization
into their triphosphate derivatives [
1
]; however, the process,
which is actuated by intracellular kinases, has very low
efficiency [
2
]. On the other hand, the direct administration
of active triphosphorylated derivatives has important clini-
cal drawbacks, because the high hydrophilicity and poor
stability of such drugs in biological media severely limit
cellular uptake and therapeutic efficiency [
2
–
4
]. To over-
come this bottleneck, alternative strategies of administra-
tion of NRTIs, based on nanostructured carriers able to
improve drug stability, have been developed to optimize
delivery inside the cells and decrease toxicity effects
[
5
–
14
]. In this context, metal
–organic frameworks
(MOFs) have gained increasing attention in the recent
years. MOFs are hybrid crystals composed of metal ions
or clusters connected by multidentate organic ligands and
form structures with very high porosity and very large
surface area. Such unique features increased their interest
for a variety of scientific and technological areas, from
magnetic and electrooptical devices, gas storage, gas/
vapor separation, catalysis, and sensing [
15
]. In the bio-
logical field, they exhibited a promising potential for im-
aging and drug delivery [
16
,
17
]. In particular, they have
been proposed as valuable non-toxic nanocarriers for
* Barbara Roda
barbara.roda@unibo.it
1
Department of Chemistry
BG.Ciamician^, University of Bologna,
Via Selmi 2, 40126 Bologna, Italy
2
byFlow srl, Via Caduti della Via Fani, 11/B, 40127 Bologna, Italy
3
CNR-Istituto per la Sintesi Organica e la Fotoreattività, Via Piero
Gobetti, 40129 Bologna, Italy
4
Institut des Sciences Moléculaires d
’Orsay, UMR CNRS 8214,
Paris-Sud University, Paris Saclay, 91400 Orsay, France
Analytical and Bioanalytical Chemistry
https://doi.org/10.1007/s00216-018-1176-6
several anticancer and antiviral drugs, like busulfan [
14
,
18
–
20
], cidofovir [
14
,
18
], doxorubicin [
14
,
21
], and
NRTIs like AZT-TP [
22
] and gemcitabine [
22
–
24
].
Nanoscale iron trimesate metal
–organic frameworks (MIL-
100(Fe) nanoMOFs, MIL = Materials of Institut Lavoisier)
exhibit a biodegradable and biocompatible crystalline struc-
ture with high and regular porosity, formed by the spontane-
ous formation of iron(III) octahedral trimers in the presence of
trimesic acid [
14
,
25
,
26
]. The resulting 3D mesoporous sys-
tem presents smaller cages (24 Å) accessible through pentag-
onal microporous windows (5.6 Å) and larger cages (29 Å)
delimited by both pentagonal and hexagonal apertures (8.6 Å).
MIL-100(Fe) nanoMOFs showed very high AZT-TP loading
capability (up to 24 wt%) together with controlled release
abilities [
14
,
22
]. Due to the small size and flexible structure,
AZT-TP molecules are most likely adsorbed within the larger
mesoporous cages and interact through the phosphate groups
with the unsaturated iron(III) Lewis acid sites. This strong
binding further ensures a sustained in vitro delivery of the
AZT-TP ligand within HIV-infected cells, inhibiting up to
the 90% of the viral replication [
14
,
22
]. Such encouraging
perspectives have been further confirmed by an investigation
of the encapsulation process in the AZT-monophosphorylated
derivative (AZT-MP). Understanding of the impact of the
number of phosphate groups per nucleoside molecule on the
drug-nanocarrier association has direct relevance to the poten-
tial use of NRTIs monophosphorylated form as prodrug. It is
generally considered that the first phosphorylation step is the
rate-limiting reaction in the metabolic activation of nucleoside
analogues [
22
].
As nanostructured materials for biological applications,
nanoMOFs have to meet stability requirements. A certain de-
gree of chemical instability in the material is a desirable prop-
erty in physiological conditions, since the nanocarrier is expect-
ed to deliver and release the drug into the cell and once this
function is completed it should be able to degrade in situ. On
the other hand, for preparation and characterization purposes, a
good stability of the colloidal suspensions is required. For un-
derstanding the factors that govern the stability of the nanopar-
ticles (NPs) upon drug encapsulation and release, the charac-
terization of the suspensions as regards particle size and mor-
phology is crucial [
17
]. Such study is usually carried out by
techniques like atomic force microscopy and scanning or trans-
mission electron microscopy, and spectroscopic techniques like
dynamic light scattering (DLS) [
27
,
28
]. Electron microscopy
allows direct observation of the individual particles and allows
to assess their shape and size, but time-consuming analyses
have to be performed to provide significant data from a statis-
tical point of view, while DLS allows for the measurement of
average dimension over the entire population of particles but
does not provide information about morphology.
Field-flow fractionation is a family of separation tech-
niques suitable for the characterization of nanosized and
microsized systems. The separation is obtained as a combina-
tion of a parabolic flow of carrier solution and an external
field. Among the various sub-techniques, asymmetric flow
field-flow fractionation (AF4) is the one which experienced
the greatest success and development and is in fact the most
established and commercially available [
29
–
31
]. The separa-
tion results from the application of a flow stream of carrier
along a channel with a capillary dimension together with a
perpendicular, hydrodynamic flow. Since the separation de-
pends only upon the carrier flows applied and because of the
lack of a packed stationary phase, AF4 has a unique gentle
separation mechanism: issues like shear forces or particle al-
teration are therefore avoided. Retention times of particles are
inversely proportional to their diffusion coefficient (D), and
directly proportional to the hydrodynamic diameter [
32
]. The
two perpendicular flows are generated by splitting the longi-
tudinal (pump delivered) flow into a second one (namely the
cross-flow or x-flow) across the accumulation wall (the only
permeable wall of the channel).
Multi-angle light scattering (MALS) detection is an abso-
lute method for particle sizing and molar mass determination
and is able to work over a wide dimensional range without the
use of any standard [
33
]. The theory on size and mass calcu-
lation based on static light scattering had been extensively
explained [
34
]. Briefly, when refractive index increment (dn/
dc) and sample concentration are known, MALS can provide
the molecular weight (Mw), while, independently of concen-
tration or other sample specification and without assumptions
on particle conformation or shape, it provides the root mean
square (rms) radius, which represents the mass-averaged dis-
tance of each mass element of the NP from its center of grav-
ity. If both Mw and rms radius distributions are known, parti-
cle shape and density information are accessible (deriving
from the Mw-to-rms ratio). MALS detection is applicable in
the range 10 nm
–1 μm.
The literature reports that AF4-MALS combination has
been successfully used for size analysis, study of stability,
and drug release of NPs of different composition, since it
allows for accurate size distribution determination, investiga-
tion of NPs aggregation in native conditions, separation of the
unbound constituents of the functional NPs, and determina-
tion of the optical features of the NPs (separated from other
dispersion components including free chromophores, or free
drugs) [
34
–
38
]. Some examples of use of AF4-MALS com-
bination on drug delivery NPs are relevant to the characteri-
zation of lipidic/liposome suspensions [
39
–
41
], organic poly-
mer particles like micelles (amphiphilic molecules),
polymerosomes, dendrimers, nanocapsules, and polymeric
NPs [
42
–
47
] and biopolymer particles [
48
–
52
].
In this work, we propose application of AF4 coupled with
MALS detection for the characterization of MIL-100(Fe)
nanoMOFs loaded with NRTI drugs for the first time. The
goal is to determine (a) the particle size distribution (PSD),
Roda B. et al.
(b) the stability of MOF NPs, and (c) the particle interaction
with the drug in a time frame of 24 h. To this aim, four types of
samples were examined: empty nanoMOFs and nanoMOFs
loaded with AZT derivatives with three different degrees of
phosphorylation: azidothymidine (AZT, native drug), azido-
thymidine monophosphate (AZT-MP), and azidothymidine
triphosphate (AZT-TP). It was also possible to relate the
MOF NP stability to the nature of the interaction with the drug
molecules.
Experimental part
Materials
Iron(III) chloride hexahydrate (Alfa Aesar, 98%) and 1,3,5-
benzenetricarboxylic acid (1,3,5-BTC; Aldrich, 95%) were
used as reactants for the nanoMOF synthesis and absolute
ethanol (Carlo Erba, 99%) for their activation. 3
′-azido-3′-
deoxythymidine (AZT, azido 3
′-deoxythymidine, Moravek),
3
′-azidothymidine monophosphate (AZT-MP, 3′-azido-3′-de-
oxy-
D
-thymidine 5
′-monophosphate sodium salt, Carbosinth),
and 3
′-azidothymidine triphosphate (AZT-TP, 3′-azido-2′,3′-
dideoxythymidine-5
′-triphosphate lithium salt, TriLink) were
used as received. Water was purified by passage through a
Millipore MilliQ system (Millipore SpA, Milan, Italy).
Water was used as dispersing medium.
Synthesis of the MIL-100(Fe) nanoMOFs was achieved by
means of a hydrothermal microwave-assisted reaction de-
scribed elsewhere [
22
,
53
], starting from a mixture of iron
chloride (8.97 mmol) and 1,3,5-benzenetricarboxylic acid
(4.02 mmol) in 20 ml of deionized water, heating 6 min at
130 °C under stirring. The as-synthesized nanoMOFs were
recovered by centrifugation (10 min, 10,000 g). To remove
the residual non-reacted organic acid, they were washed in
50 ml of absolute ethanol and recovered by centrifugation
(10 min, 10,000g). This activation step was repeated six times.
MIL-100(Fe) nanoMOF characterization was performed
by means of several techniques. Crystallinity was assessed
by X-ray powder diffraction (XRPD); NP diameter and mor-
phology were determined by dynamic light scattering (DLS)
and transmission electron microscopy (TEM). The porous sur-
face was measured by nitrogen adsorption analysis at
−
196 °C. The calculated BET surface was 1650 ± 100 m
2
g
−1
.
For any detail about application of the mentioned techniques,
see previous publications [
21
,
22
].
Samples
MIL-100(Fe) nanoMOFs were stored in the dark at room tem-
perature as EtOH wet material. An aliquot was suspended in a
few milliliters of ethanol, then centrifuged (10 min, 10,000g)
and subsequently washed two times with water to completely
remove ethanol. Four samples were prepared, one was empty
nanoMOFs and the other three were drug-loaded nanoMOFs.
Aliquots of the centrifugate were taken and re-dispersed in
water or aqueous solution of drug to achieve a final concen-
tration of 0.2 mg/ml of the starting solid MOF material and
0.2 mg/ml of MOFs and 0.1 mM of drug for the drug-
conjugated particles. NanoMOFs were loaded with drugs sim-
ply by impregnation. Nanoparticles were incubated with the
aqueous solution of drug, stirring the mixture at room temper-
ature in the dark for either 15 min (freshly prepared samples)
or 24 h. With freshly prepared samples, all the measurements
were performed within 1 h from preparation. The 24-h delay
was chosen to evaluate the stability of the MOF NP conjugat-
ed with the phosphorylated AZT derivatives, because no sig-
nificant release of the drugs was assessed by HPLC analysis
over 3 days in water [
22
].
Measured pH value of dispersed MOF NPs was slightly
acidic.
The zeta potential (ZP) of NPs was measured with a
Zetasizer 4 equipment (Malvern Instruments, UK) on suspen-
sions containing 0.2 mg/mL of MOF NPs.
AF4-MALS analysis
AF4-MALS was performed by using a 1100 Series HPLC
system (Agilent Technologies, Palo Alto, CA), connected to
a control module to control AF4 flow rates and operations
(Eclipse 3, Wyatt Technology Europe, Dernbach, Germany).
On-line detection of the eluted species was performed with an
Agilent 1100 DAD UV/Vis spectrophotometer, a MALS
DAWN HELEOS detector (Wyatt Technology Corporation,
Santa Barbara, CA), and an Optilab rEX refractive index de-
tector (Wyatt Technology Corporation). Carrier solutions were
degassed using an on-line vacuum degasser Agilent, 1100
series (Agilent Technologies).
The separation device is constituted by a flat channel with a
trapezoidal shape and capillary height. For the sample analy-
sis, particles are introduced in the channel and focused,
allowing the sample to concentrate on a narrow band. When
the elution starts, the separation is gained by the combination
of a longitudinal and a perpendicular hydrodynamic field. The
channel was 152 mm long (Wyatt Technology Europe),
equipped with a polyethersulfone membrane (Nadir), with a
molecular weight cutoff of 10 kDa. The channel spacer was
350
μm thick, with trapezoidal shape (upstream width b0 =
16 mm; downstream width bL = 4 mm).
The flow rate program was set up as follows: 2 min of
elution (crossflow 0.2 ml/min) was applied to equilibrate the
baselines on the detectors; then 1-min focus flow (0.5 ml/min)
was applied to equilibrate the flows in the channel. Then 2-
min injection (at a flow rate of 0.2 ml/min) in focus mode was
applied in order to allow the sample to reach the channel, and
2 further minutes of focus was used to allow for a complete
Flow field-flow fractionation and multi-angle light scattering as a powerful tool for the characterization...
relaxation. After the focus step, the elution starts with an
isocratic cross-flow step of 0.2 ml/min for 30 min. Elution
medium was pure water. The method reproducibility was ver-
ified in the method development step to ensure robustness and
the effective correspondence between retention time and sam-
ple properties depending on time and storage conditions.
Results and discussion
AF4-MALS characterization of empty nanoMOFs
MIL-100(Fe) nanoMOFs were successfully prepared and
characterized as described in
B
Materials
^ section. DLS and
TEM showed particle diameters around 200
–240 nm and
facetted-type architecture [
21
,
22
].
Figure
1
reports the light scattering signal and the rms radius
distribution obtained by the AF4-MALS analysis of empty
nanoMOF particles in the freshly prepared sample (measure-
ment performed within 1 h from preparation). The fractionation
profiles constituted by a monomodal but relatively large distri-
bution band, with a maximum at retention time (tR) of 18 min
and a tail at higher retention times (up until 22
–23 min). The
particle size distribution (PSD) obtained by the AF4-MALS
fractionation indicates that the sample is fairly homogenous
with rms radius values of ca. 81 nm (see Table
1
).
As for the fractionation method, the absence of peak at the
field release (tR = 37 min) indicates a complete fractionation
process with no retained sample into the channel. In addition,
the profile has a sharp peak at tR = 8 min which is the void
peak corresponding to the flow change effect together with a
negligible part of non-retained sample; this is a constant for all
injections.
Comparison of the AF4-MALS rms radius value with di-
ameter obtained from DLS (200
–250 nm, see ref. [
21
]) indi-
cates a fair agreement. More in detail, the parameter that
MALS measures is the root mean square (rms) radius, the
measure of a particle
’s size weighted by the mass distribution
about its center of mass, while DLS and nanoparticle tracking
analysis (NTA) give a measure of the hydrodynamic radius
(Rh). The ratio between rms and Rh (shape factor) gives in-
sight into the actual shape of the particles. For example, a ratio
of 1.7 (rms/Rh) corresponds to rods or chain aggregates, while
a ratio of about 0.7
–0.8 corresponds to more compact spher-
ical objects [
54
]. NanoMOFs show a MALS-calculated diam-
eter and a DLS-calculated diameter of 162 and 210 nm respec-
tively; the ratio would be 0.77. This is in line with a globular
compact mesoporous material, in agreement with TEM and
XRDP findings [
23
] indicating a facetted and crystalline struc-
ture, and with N2 absorption findings showing an important
porous structure [
22
].
By correlating the characterization data with the AF4-
MALS results, we can conclude that the AF4-MALS system
appears suitable for the characterization of nanoMOF suspen-
sions and can allow to obtain fundamental data on their size
and stability over time as it could detect even minor size
evolutions.
AF4-MALS characterization of drug-loaded nanoMOFs
The PSD in the nanoMOFs loaded with AZT, AZT-MP, and
AZT-TP was measured in the freshly prepared suspensions
and in the suspensions stored 24 h in the dark at room tem-
perature with the developed AF4-MALS method used for
empty nanoMOFs. In Fig.
2
, the fractographic profiles of the
three freshly prepared, drug-loaded nanoMOF suspensions
Fig. 1 Fractograms (LS signal at
90°) and calculated gyration radii
of empty nanoMOF; freshly
prepared sample: 0.2 mg/mL of
solid MOF material, in water
Table 1 rms radius
values (nm) of
nanoMOFs immediately
after preparation and af-
ter 24 h. All samples
were at a concentration
of 0.2 mg/mL of
nanoMOF in water
Sample
rms radius (nm)
Fresh
24 h
Empty nanoMOF
81 ± 2
–
NanoMOF-AZT
81 ± 2
80 ± 3
NanoMOF-AZT-MP
90 ± 2
90 ± 2
NanoMOF-AZT-TP
97 ± 2
97 ± 2
Roda B. et al.
(nanoMOF 0.2 mg/mL + AZT 1 × 10
−4
M, nanoMOF 0.2 mg/
mL + AZT-MP 1 × 10
−4
M, nanoMOF 0.2 mg/mL + AZT-TP
1 × 10
−4
M) were compared with those of the corresponding
empty nanoMOF (0.2 mg/mL) suspension. Results of PSD
analysis by AF4-MALS are reported in Table
1
.
It can be noted that empty nanoMOF and MOF-AZT sam-
ples have identical PSD. The MOF-AZT-MP NP exhibits a
rms radius of 90.0 ± 2.0 nm with an increase of ca. 10 nm with
respect to the empty nanoMOFs. This fact can be rationalized
with the prompt binding of the drug to the nanoMOFs and to
bridging effects leading to a slight increase of the size. The
interaction of the triphosphorylated drug with the MOF NP
frame is also established promptly. The MOF-AZT-TP sample
shows a further increase of NP radius with a measured value
of 96.8 ± 2.3 nm. On the contrary, no increase of the
nanoMOF size is observed with AZT.
These findings clearly (i) confirm the prompt binding of
both AZT-MP and AZT-TP to the nanoMOF frame; (ii) are in
agreement with the known lack of appreciable interaction of the
native drug with the nanoMOFs, assessed by means of drug
loading and release studies combined with UV-vis spectrosco-
py, ITC, and molecular modeling [
22
]; (iii) highlight the key
role of the phosphate groups for effective encapsulation of AZT
derivatives within the MIL-100(Fe) nanoMOF cages, also tes-
tified by the very high maximum loadings observed, as report-
ed in a previous work (36 and 24 wt% for AZT-MP and AZT-
TP, respectively) [
22
]; and (iv) support the idea of a different
MOF interplay with the mono- or triphosphorylated drug, al-
ready suggested by UV-Vis absorption spectroscopy, circular
dichroism, isothermal titration calorimetry, and molecular
modeling data [
22
,
24
]. On the basis of these techniques, the
binding mechanism has been assigned to the formation of
strong iono-covalent links of the phosphate groups with the
Lewis iron(III) acid sites [
22
]. Due to the stronger complexing
capability, the triphosphorylated drug was proposed to possess
higher tendency than AZT-MP to occupy the nanoMOF cages
by replacing coordinated trimesic acid bound to iron metal
sites. With this respect, it has been also shown that the number
of phosphate groups has a direct impact on the binding constant
which is lower for AZT-MP than for AZT-TP (K = 1340 vs.
2930 M
−1
). These findings are also in agreement with the pre-
viously reported data from XRDP measurements, which shows
that the encapsulation of the phosphorylated drug into the
nanoMOF structure does not affect the crystalline structure
[
22
,
23
], and is performed through pore filling.
The fractograms in Fig.
2
also indicate that, despite FFF
theory suggesting that smaller particles elute first, the reten-
tion times of the loaded vs. unloaded MOF NPs are inverted:
MOF-AZT-MP and MOF-AZT-TP particles have lower reten-
tion time than empty nanoMOF and MOF-AZT particles. This
reflects a change in the zeta potential of the MOF NPs. Zeta
potential plays indeed a key role in the retention time of the
nanoparticles because it influences the elution process inside
the channel. In Table
2
, the measured values of the zeta po-
tential for the MOF-AZT-MP and MOF-AZT-TP are com-
pared to those of empty nanoMOFs (AZT-loaded particles
exhibit a surface charge quite similar to that of the empty
ones). The loaded MOF NPs show negative surface charge
with absolute values that are higher when compared to those
of empty ones. Since the channel membrane is negatively
charged, negative conjugated particles are repelled away from
the membrane and travel at a higher position compared to the
unconjugated ones: thus, their position corresponds to a
higher flow stream. The repeatability of these results has been
confirmed in more than seven repetitions under same condi-
tions showing a CV% < 5%: this behavior confirms that AZT-
MP and AZT-TP actually bind to the nanoMOF and are pres-
ent in the porous cores as well as in the top layers influencing
the overall particle potential.
Another indirect indication of drug-nanoparticle complex-
ation comes from the relative intensity of the LS signals. The
higher scattering intensity for the MOF-AZT-MP and MOF-
Fig. 2 Fractograms (LS signal at 90°) and calculated gyration radii of
freshly prepared MOF samples. Light gray dotted line: MOF-AZT-TP.
Gray dotted line: MOF-AZT-MP; Black line: MOF-AZT. Gray line: emp-
ty nanoMOF. Samples: 0.2 mg/ml of the solid MOF material for the
empty nanoMOFs and 0.2 mg/ml of the solid material plus 0.1 mM of
drug for the drug-loaded particles, in water
Table 2
Zeta potential of empty nanoMOF, MOF-AZT-MP, and MOF-
AZT-TP NPs, measured in water at 0.2 mg/ml MOF material
concentration
Sample
Zeta potential (mV)
Empty nanoMOF
+ 10 ± 3
NanoMOF-AZT-MP
− 15 ± 2
NanoMOF-AZT-TP
− 40 ± 2
Flow field-flow fractionation and multi-angle light scattering as a powerful tool for the characterization...
AZT-TP with respect to the signal of the unloaded particles is
not simply justified by the increase in PSD of just 10 and
16 nm, respectively, since the size difference is too small.
Actually, the LS signal is proportional to the mass, concentra-
tion, and derivative of the refractive index vs. concentration,
dn/dc [
33
]. The different scattering power can be then ex-
plained by taking into consideration the last two parameters.
The dn/dc values are expected to be bigger for the loaded
MOF with respect to the unloaded MOF particles, the formers
being more polarizable and therefore able to give a more in-
tense signal. Indeed, opposed to AZT which has practically no
interaction with the nanoMOFs, AZT-MP and AZT-TP fill
completely their large cages as previously reported [
22
].
Moreover, the actual concentration of nude and AZT-
nanoMOFs could lower, due to precipitation of macro-aggre-
gates, thereby reducing the scattering intensity. The colloidal
instability of the suspensions is most evident for nude
nanoMOFs, but also noticeable for AZT-nanoMOF (see also
B
AF4-MALS study of drug-loaded nanoMOF stability
^ sec-
tion), further proving the lack of interaction between the
nanoMOF and a non-phosphorylated drug.
In conclusion, differences in PSD, particles surface charge,
and polarizability between empty particles and drug-loaded par-
ticles give a strong indication of MOF surface and core modi-
fication, and, together with the signal intensity, may contribute
to the elucidation of the stability features of these systems.
AF4-MALS study of drug-loaded nanoMOF stability
The AF4-MALS method was applied to control the morpho-
logical stability of the drug-loaded nanoparticles after 24 h
(Fig.
3
a
–c).
The fractograms relevant to the MOF-AZT system are re-
ported in Fig.
3
a. The profiles indicate that immediately after
Fig. 3 AF4-MALS profiles of
nanoMOF particles immediately
after preparation (gray line) and
after 24 h (black line) incubated
with
a MOF-AZT, b MOF-AZT-
MP, and
c MOF-AZT-TP.
Samples: 0.2 mg/ml of the solid
material plus 0.1 mM of drug for
the drug-loaded particles, in water
Roda B. et al.
preparation there is a Gaussian and symmetric band, which
becomes bimodal and less intense after 24 h. This fact high-
lights how the MOF-AZT nanoparticles tend to aggregate
with elapsing time. The particle size distribution does not
change so much. A very poor interaction of AZT with the
MOF frame is confirmed also after 24 h. However, the big
decrease in LS signal intensity suggests a decrease in particle
concentration in the sample. Most probably, precipitation of
aggregates and sedimentation could explain such effects, as
mentioned above.
Figure
3
b shows the fractograms of the MOF-AZT-MP
system. After 24 h, there is only a little variation in the LS
signal intensity and in the band profile, and the PSD given by
the rms radius does not change (Table
1
).
Figure
3
c shows the fractograms of the MOF-AZT-TP
system. Also in this case, the signal intensity and band
profile do not change much over the 24 h and the rms
radius keeps the same.
From the comparison between PSD distributions in Fig.
3
a
–c
and from data in Table
1
, it can be inferred that all the drug-
loaded systems are fairly stable over the time frame of the ob-
servations. AZT does not modify the nude particle scattering
behavior, thus confirming the lack of appreciable interaction,
whereas the phosphorylated derivatives strongly modify the
scattering behavior due to efficient interaction with the
nanoMOF frame. Comparison of the MOF-AZT-MP system
with the MOF-AZT-TP one indicates the latter is more stable.
This fact could be explained with the magnitude of the apparent
binding constant of the drug to the MOF frame, which is higher
for AZT-TP than for AZT-MP and points to a role of the strength
of the interaction controlled by the number of phosphate groups,
in the system stability [
22
]. However, the changes in rms radius
over 24 h are negligible for both MOF-AZT-MP and MOF-
AZT-TP, so it can be concluded that the interaction with both
phosphorylated drugs was maintained during storage.
Conclusions
AF4-MALS was for the first time applied to the characteriza-
tion of a nanosized MOF material, MIL-100(Fe) nanoMOFs,
loaded with NRTI drugs of interest for anti-HIV therapy. The
method provided important information on size, stability, and
aggregation behavior of the MOF NPs and clearly evidenced
surface/core modification on the drug-loaded nanoMOF.
AF4-MALS was shown here to be a useful methodology to
analyze particles intended for drug delivery applications. The
size separation together with the unique gentle separation
mechanism is crucial to avoid loss of aggregates and to detect
them, allowing for their identification even when they are
present in such a small amount that they do not affect signif-
icantly the particle size distribution (e.g., when the aggrega-
tion process is at its early stage). The online coupling with
MALS detection allowed for particle size distribution deter-
mination and early-stage aggregation detection. Insights were
obtained on drug location which greatly influenced the dn/dc
parameters of the nanoMOFs.
Acknowledgments
This work has been carried out in the frame of the European
ITN network CYCLON (no. 237962).
Compliance with ethical standards
Conflict of interest
Andrea Zattoni, Barbara Roda, and Pierluigi
Reschiglian are associates of the academic spinoff company byFlow Srl
(Bologna, Italy). The company mission includes know-how transfer, de-
velopment, and application of novel technologies and methodologies for
the analysis and characterization of samples of nanobiotechnological in-
terest. Valentina Marassi, Francesco Borghi, Resmi Anand, Valentina
Agostoni, Ruxandra Gref, and Sandra Monti declare no conflicts of
interest.
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Document Outline - Flow...
- Abstract
- Introduction
- Experimental part
- Materials
- Samples
- AF4-MALS analysis
- Results and discussion
- Conclusions
- Acknowledgments
- References
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