Rebecca Kaup1, Aldrik H Velders1,2,3. 1. Laboratory of BioNanoTechnology, Wageningen University. Bornse Weilanden 9, 6708 WG Wageningen, The Netherlands. 2. Interventional Molecular Imaging Laboratory, Department of Radiology, Leiden University Medical Center, 2300 RC Leiden, The Netherlands. 3. Instituto Regional de Investigacion Cientifica Aplicada (IRICA), Universidad de Castilla-La Mancha, Ciudad Real, 13071, Spain.
Abstract
Whereas the formation and overall stability of hierarchically organized self-assembled supramolecular structures have been extensively investigated, the mechanistic aspects of subcomponent dynamics are often poorly understood or controlled. Here we show that the dynamics of polyamidoamine (PAMAM) dendrimer based micelles can be manipulated by changes in dendrimer generation, pH, and stoichiometry, as proven by NMR and FRET. For this, dendrimers were functionalized with either fluorescein (donor) or rhodamine (acceptor) and encapsulated into separate micelles. Upon mixing, exchange of dendrimers is revealed by an increase in FRET. While dendrimicelles based on dendrimer generations 4 and 5 show a clear increase in FRET in time, revealing the dynamic exchange of dendrimers between micellar cores, generation 6 based micelles appear to be kinetically trapped systems. Interestingly, generation 6 based dendrimicelles prepared at a pH of 7.8 rather than 7.0 do show exchange dynamics, which can be attributed to about 25% less charge of the dendrimer, corresponding to the charge of a virtual generation 5.5 dendrimer at neutral pH. Changing the pH of dendrimicelle solutions prepared at a pH of 7.8 to 7.0 shows the activated release of dendrimers. High-resolution NMR spectra of the micellar core are obtained from a 1.2 GHz spectrometer with sub-micromolar sensitivity, with DOSY discriminating released dendrimers from dendrimers still present in the micellar core. This study shows that dendrimer generation, charge density, and stoichiometry are important mechanistic factors for controlling the dynamics of complex coacervate core micelles. This knowledge can be used to tune micelles between kinetically trapped and dynamic systems, with tuning of exchange and/or release speeds, to be tailored for applications in, e.g., material science, sensors, or drug delivery.
Whereas the formation and overall stability of hierarchically organized self-assembled supramolecular structures have been extensively investigated, the mechanistic aspects of subcomponent dynamics are often poorly understood or controlled. Here we show that the dynamics of polyamidoamine (PAMAM) dendrimer based micelles can be manipulated by changes in dendrimer generation, pH, and stoichiometry, as proven by NMR and FRET. For this, dendrimers were functionalized with either fluorescein (donor) or rhodamine (acceptor) and encapsulated into separate micelles. Upon mixing, exchange of dendrimers is revealed by an increase in FRET. While dendrimicelles based on dendrimer generations 4 and 5 show a clear increase in FRET in time, revealing the dynamic exchange of dendrimers between micellar cores, generation 6 based micelles appear to be kinetically trapped systems. Interestingly, generation 6 based dendrimicelles prepared at a pH of 7.8 rather than 7.0 do show exchange dynamics, which can be attributed to about 25% less charge of the dendrimer, corresponding to the charge of a virtual generation 5.5 dendrimer at neutral pH. Changing the pH of dendrimicelle solutions prepared at a pH of 7.8 to 7.0 shows the activated release of dendrimers. High-resolution NMR spectra of the micellar core are obtained from a 1.2 GHz spectrometer with sub-micromolar sensitivity, with DOSY discriminating released dendrimers from dendrimers still present in the micellar core. This study shows that dendrimer generation, charge density, and stoichiometry are important mechanistic factors for controlling the dynamics of complex coacervate core micelles. This knowledge can be used to tune micelles between kinetically trapped and dynamic systems, with tuning of exchange and/or release speeds, to be tailored for applications in, e.g., material science, sensors, or drug delivery.
Besides its ubiquitous importance
in biological systems and materials science,[1] self-assembly has proven to be an attractive and powerful strategy
to create a variety of molecular superstructures, by design of building
blocks allowing the tuning of physical–chemical parameters
such as structure, size, shape, stability and responsiveness.[2−6] However, the detailed characterization and understanding of the
dynamic properties of such subcomponents within structures remains
a great challenge, while this is important for the design, formation,
and control of nanomaterials and their applications.[7,8] Micelles coined complex coacervate core micelles or polyion complex
micelles (C3Ms and PICs, respectively) are well-defined self-assembled
systems formed by electrostatic interactions between a charged core
building block and an oppositely charged–neutral block copolymer.[9−11] Different core building blocks, from linear or branched polymers
to proteins and DNA have been exploited.[10] C3Ms are promising for nanomedical applications, including drug
delivery, gene transcription, and contrast agents.[12] For many applications the stability of micelles is an important
factor and has been extensively investigated, with bulk solution characteristics
such as critical micelle concentration (CMC) and critical salt concentration
(CSC) being representative parameters.[13,14] However, less
research has been done on the dynamics, i.e. the exchange between
core components of micelles, although both the exchange rate and the
nature of exchange is crucial for e.g. cargo protection, as exchange
of the material could lead to exposure of the cargo to the surrounding
environment.[15]In extremis, one would like to have spatial and temporal control, from kinetically
trapped systems, via controlled release, to dynamic exchange of subcomponents.
A few recent studies and simulations on the exchange of C3M subcomponents
show that the exchange rate is highly dependent on salt concentration
and polymer length.[15−19] However, it has not yet been shown that changing polymer lengths
(charges per core component) can not only be used to control exchange
rates but also can lead to kinetically trap micelles. Moreover, understanding
such parameters would allow moving between kinetically trapped systems,
controlled release, and exchange of subcomponents.Dendrimers,
and in particular polyamidoamine (PAMAM) dendrimers,
are highly symmetrical, branched polymers with a defined size and
number of surface groups.[20,21] The number of surface
groups doubles with increasing dendrimer generation, which in combination
with their highly defined structure makes them very suitable for systematic
studies. Furthermore, the voids of dendrimers can be used to encapsulate
small molecules: e.g., drugs or nanoparticles.[22−24] Dendrimers
and dendrons are often used as building blocks for nanomaterials based
on self-assembly and self-organization.[25,26] In the past,
we developed so-called dendrimicelles,[27] which are formed by electrostatic interactions between positively
charged PAMAM dendrimers and a neutral–negatively charged poly(methacrylic
acid)-b-poly(ethylene oxide), pMAA64-b-pEO885, block copolymer.[28] Encapsulation of dendrimer-encapsulated gold nanoparticles
(AuDENs) was used to reveal the shape and aggregation number of dendrimicelles
by cryo-transmission electron microscopy (cryoTEM).[28−31] Recently, we proved the formation
of multicompartment dendrimicelles with up to four different generation
6 dendrimers within one micellar core, by the combined use of cryoTEM
and FRET.[32]cryoTEM in particular
has proven fundamental for investigating
the stability of dendrimicelles in time, as the gold nanoparticles
provide single-micelle information, revealing micelles based on generation
7 or higher PAMAM dendrimers to be kinetically trapped.[28] We hypothesized that lower-generation dendrimers,
i.e. with fewer charged surface groups, could form more dynamic micelle
systems. Unfortunately, investigating the stability of dendrimicelles
based on lower-generation dendrimers by cryoTEM is not straightforward,
as PAMAM generations 5 and lower tend to form dendrimer-stabilized
nanoparticle systems rather than dendrimer-encapsulated nanoparticles,[30] inhibiting a systematic investigation of the
exchange of individual dendrimers between the cores of different micelles.
Moreover, TEM only allows visualization of snapshots at different
time points, and the dynamics cannot be closely monitored over time.
To allow investigation of this intriguingly well-defined and versatile
class of dendrimicelles, we envisioned to exploit Förster resonance
energy transfer (FRET) to study the exchange of dendrimers from the
core of one dendrimicelle with dendrimers in the core of other micelles,
as depicted in Scheme . Fluorescence and FRET are powerful techniques to study the thermodynamic
properties and/or kinetics of self-assembled systems, including micelles.[33] For FRET systems, solutions containing nanoassemblies
with either a donor or an acceptor fluorophore are mixed, an increase
in FRET efficiency revealing exchange of the building blocks or guest
molecules.[16,17,34−36] For the dendrimicelles, we show that the exchange
is different for different dendrimer generations. Moreover, the exchange
dynamics can be tuned by varying the generation of dendrimers used,
by varying the pH, or by affecting the stoichiometry of the subcomponents.
Scheme 1
PAMAM Dendrimers Functionalized with either FITC (Green) or RITC
(Red) and Consequently Used to Form Dendrimicelles by Mixing the Positively
Charged Dendrimer Generation 4, 5, or 6 with a Neutral–Negatively
Charged pMAA64-b-pEO885 Block Copolymer under
Charge Stoichiometric Conditions
To measure the exchange
of
dendrimers, micelles containing only the donor (FITC) or only the
acceptor (RITC) are mixed at a 1:1 ratio. Exchange will result in
micelles containing both donor and acceptor molecules, bringing them
into close proximity and resulting in FRET. A premixed control sample
containing the donor and acceptor gives the maximum FRET value corresponding
to complete exchange. In this study different dendrimer generations
and generation 6 at two different pH values or slightly off-stoichiometric
conditions were tested and show control over exchange dynamics and
trapping as well as activated release of dendrimers. For reasons of
clarity, only generation 6 dendrimers are depicted in this scheme.
PAMAM Dendrimers Functionalized with either FITC (Green) or RITC
(Red) and Consequently Used to Form Dendrimicelles by Mixing the Positively
Charged Dendrimer Generation 4, 5, or 6 with a Neutral–Negatively
Charged pMAA64-b-pEO885 Block Copolymer under
Charge Stoichiometric Conditions
To measure the exchange
of
dendrimers, micelles containing only the donor (FITC) or only the
acceptor (RITC) are mixed at a 1:1 ratio. Exchange will result in
micelles containing both donor and acceptor molecules, bringing them
into close proximity and resulting in FRET. A premixed control sample
containing the donor and acceptor gives the maximum FRET value corresponding
to complete exchange. In this study different dendrimer generations
and generation 6 at two different pH values or slightly off-stoichiometric
conditions were tested and show control over exchange dynamics and
trapping as well as activated release of dendrimers. For reasons of
clarity, only generation 6 dendrimers are depicted in this scheme.In a systematic approach, PAMAM dendrimers were
functionalized
with either fluorescein isothiocyanate (FITC) as a donor or with rhodamine
B isothiocyanate (RITC) as an acceptor. As shown in Scheme , micelle solutions containing
only the donor fluorophore or only the acceptor fluorophore were mixed,
resulting in an increase in energy transfer upon exchange of dendrimers
between micelles over time. FRET is an ideal methodology to prove
exchange between micellar core components, as energy transfer is only
possible when the donor and acceptor are in close proximity: i.e.,
within the same micelle core.[32] In four
different kinds of experiments we reveal the exchange properties of
dendrimicelles based on dendrimer generations 4, 5, and 6, with, respectively,
64, 128, and 256 positive charges based on the theoretical maximum
number of amine end groups. First, the formation of dendrimicelles
is proven with DLS and nuclear magnetic resonance (NMR) spectroscopy.
Consecutively, FRET reveals the exchange of donor- and acceptor-labeled
dendrimers between the cores of micelles based on generations 4 and
5, but not for 6. Third, preparing dendrimicelles based on generation
6 at a higher pH, so that there is a lower overall charge per dendrimer,
results in a G6-based dendrimicelle that rather than a kinetically
trapped system that now is dynamic. In a final experiment, the surface
charge of micellar core-dendrimers is altered by changing in situ the pH of the micelle solution, resulting in the
release of dendrimers from the core. Whereas commonly micelles are
investigated and characterized by light-scattering techniques, we
here additionally introduce high-resolution solution NMR spectroscopy
as an highly informative and powerful technique. Notwithstanding the
enormous size and very low sub-micromolar concentrations of the micelles,
aspects that normally preclude or strongly limit the use of NMR in
micelle studies, the sensitivity of a 1.2 GHz spectrometer allows
discriminative signals from dendrimers as micellar core subcomponents
as well as free dendrimers. This work provides qualitative and quantitative
tools to control the dynamics of subcomponents in complex hierarchically
organized self-assembled structures, which is of use for the design
of responsive materials with spatial and temporal control over the
subcomponent dynamic properties.
Results and Discussion
Here below, we first describe
the formation and characterization
of dendrimicelles based on three different generations of PAMAM dendrimers
with a pMAA64-b-pEO885 block
copolymer. Although the data are similar for dendrimicelles of generations
4, 5, and 6, the focus in this first part is on generation 6 alone
for purposes of clarity. Importantly, we prove the invaluable use
of high-field NMR spectroscopy, revealing the presence of dendrimers
inside micellar cores. Second, based on a time-lapse FRET experiment
we show that the use of generation 4 and 5 PAMAM dendrimers results
in the formation of dendrimicelles that have dynamic core properties:
i.e., the dendrimers can exchange between cores of different micelles.
Differently, the G6-based system appears to be kinetically inert.
Next, preparing dendrimicelles at a pH of 7.8 rather than 7 results
in G6-based micelles that do show dynamic exchange of the dendrimers.
Finally, the responsive release capabilities of the versatile dendrimicelle
concept is proven by lowering the pH of a G6-based dendrimicelle prepared
at high pH. Here again, NMR spectroscopy, and in particular diffusion-ordered
NMR spectroscopy (DOSY), provides detailed and unambiguous insights.
Formation and Characterization of Dendrimer-Based Micelles
First, different generations of PAMAM-based dendrimicelles were
formed at pH 7 by mixing the dendrimers in a stoichiometric ratio
with pMAA64-b-pEO885. Generations
4, 5, and 6 were chosen, because previous work already showed that
generation 7 dendrimers form kinetically trapped dendrimicelles.[28] We hypothesized that lower-generation dendrimers,
i.e. with fewer charged surface groups, form more dynamic micelle
systems. The micelles were characterized with dynamic light scattering
(DLS), showing a hydrodynamic diameter of 40–60 nm, with generation
4 forming slightly larger micelles than generations 5 and 6 (Figure A and Figure S1). The critical micelle concentration
(CMC) of the dendrimicelles was also determined with DLS. The CMC
is <10 mg/L of the total polymer concentration for all three G4-,
G5- and G6-based dendrimicelles (Figure S2).
Figure 1
(A) DLS plot of dendrimer generation 6 based micelles. (B) 1H NMR 1D-DOSY spectrum of G6-based dendrimicelles with gradient
strengths of 5% (lower spectrum) and 50% (upper spectrum). The peaks
marked with an asterisk are from MOPS buffer. The peak at 3.6 ppm
is from the PEG part of the block copolymer. The dendrimer peaks are
highlighted by the blue bars in the two spectra, showing the dramatic
improvement in spectral features of the dendrimers inside the micelle
core when higher pulsed-field gradient strengths are applied. (C)
Pseudo-2D DOSY overlay plots of generation 6 dendrimers encapsulated
in micelles (blue) or free in solution (red), showing only the dendrimer
signals. The 1D spectrum used on top of the 2D plot was taken with
30% gradient strength and shows the signals of the dendrimers inside
the micelle core. The dashed lines are an aid to the eye, showing
which peaks belong to the free dendrimers or to the dendrimers in
the micelles (note that here the DOSY plot is an overlay of two separate
pseudo-2D DOSY plots from two different samples).
(A) DLS plot of dendrimer generation 6 based micelles. (B) 1H NMR 1D-DOSY spectrum of G6-based dendrimicelles with gradient
strengths of 5% (lower spectrum) and 50% (upper spectrum). The peaks
marked with an asterisk are from MOPS buffer. The peak at 3.6 ppm
is from the PEG part of the block copolymer. The dendrimer peaks are
highlighted by the blue bars in the two spectra, showing the dramatic
improvement in spectral features of the dendrimers inside the micelle
core when higher pulsed-field gradient strengths are applied. (C)
Pseudo-2D DOSY overlay plots of generation 6 dendrimers encapsulated
in micelles (blue) or free in solution (red), showing only the dendrimer
signals. The 1D spectrum used on top of the 2D plot was taken with
30% gradient strength and shows the signals of the dendrimers inside
the micelle core. The dashed lines are an aid to the eye, showing
which peaks belong to the free dendrimers or to the dendrimers in
the micelles (note that here the DOSY plot is an overlay of two separate
pseudo-2D DOSY plots from two different samples).Due to the micelle size (low tumbling times) as
well as because
of the very low (μM) concentrations, we had no high expectations
of making the dendrimers residing inside the micelle core visible
with NMR spectroscopy. However, with a state-of-the-art 28.2 T (1200
MHz 1H Larmor frequency) spectrometer, it appears possible to observe
the dendrimers at sub-micromolar concentrations, even when they reside
inside the micellar core (Figure B,C and Figures S3–S6). Clearly the mobility of the dendrimers inside the micellar core
is high enough to allow sharp lines in NMR, and this is the case for
micelles based on each of the three generations used. In particular,
DOSY is a most useful technique and was used previously by us to investigate
covalently functionalized dendrimers as well as a dendrimer-encapsulated-nanoparticle
system.[37−39] DOSY experiments are typically executed as a series
of 1D echo experiments with an increasing pulsed-field gradient (PFG)
strength.[40−43] A single 1D DOSY spectrum acquired with a relatively high PFG strength
acts as a kind of filter that selectively attenuates signals of small
molecules more than the signals of larger components.[44]Figure B shows the spectra of generation 6 based micelles recorded with
gradient strengths of 5% and 50%. At 50% gradient strength signals
deriving from smaller molecules such as the buffer components present
at high concentrations (20 mM of MOPS) are dramatically attenuated,
while the peaks of larger particles (present at orders of magnitude
lower concentrations, i.e. 2 μM of G6 PAMAM) remain visible.
Therefore, at the rightly chosen gradient parameters, predominantly
peaks of the block copolymer and the (micellar-core) dendrimers are
observed. The fact that the dendrimers are detectable means that they
can still move relatively freely or circulate inside the micelle core.
In a cross-linked system such as dendroids,[45] no dendrimer peaks could be detected. This shows that dendrimicelles
are highly dynamic systems regarding the mutual movements and interactions
of the subcomponents.Figure C is a pseudo-2D
DOSY plot showing the overlap of two different experiments, with the
peaks of generation 6 dendrimers free in solution (red) compared to
the dendrimers residing inside micelle cores (blue) (full DOSY plot
of G6-based micelles is given in Figure S7). In comparison with free dendrimers, the peaks of encapsulated
dendrimers shifted downfield, indicating the different environment
inside micelle cores. In fact, the dendrimers are expected to be close
in proximity to the negatively charged carboxylic acid groups of the
block copolymer. Diffusion coefficients were obtained by fitting the
attenuated signals of the series of 1D DOSY spectra, giving 5.25 ×
10–11 and 1.02 × 10–11 m2/s for free dendrimers and dendrimers encapsulated in micelles,
respectively. The higher diffusion coefficient for free dendrimers
clearly corroborates that the other dendrimer peaks derive from dendrimers
in a larger complex. The diffusion coefficients were further used
to determine the micelle size. This was done by using the Stokes–Einstein
equation (, which shows
an inversely proportional correlation between the diffusion coefficient
and hydrodynamic radiuswith kB, T, η, and R being the Boltzmann constant,
the absolute temperature, the viscosity, and the hydrodynamic radius,
respectively. The self-diffusion and consequently the DOSY measurements
are very susceptible to experimental parameters such as solvent, temperature,
and hence viscosity, which can lead to relatively large errors in
the determined diffusion coefficients in running absolute DOSY experiments
or on comparing separate measurements.[37,46] However, working
under identical conditions or, even better, by measuring components
in one and the same NMR tube, the exact calibration of the gradient
coil, as well as temperature or viscosity control, is not of importance.
For normalization of two components measured under the same conditions,
all of the constants and parameters can be eliminated on equalizing
the respective Stokes–Einstein equation, which results in eq , where the known diameter
of the free dendrimer multiplied by the ratio of the diffusion coefficients
of the dendrimers free in solution and inside the core yields the
micelle dimension.For our system, first the apparent
hydrodynamic diameter of generation
6 PAMAM dendrimers (amine-terminated) was determined by using generation
6 PAMAM-OH dendrimers as an internal standard (Figure S8). The hydrodynamic diameter of the PAMAM-OH was
used, as it is expected not to be affected by salt (double) layers;
this is in contrast to the positively charged amine-terminated end
groups of the regular PAMAM. Taking a size of 7.0 nm for generation
6 PAMAM-OH, the diffusion coefficient of the generation 6 PAMAM-NH2 dendrimer corresponds to a hydrodynamic diameter of 8.3 nm.
When the diffusion coefficients of free generation 6 PAMAM dendrimers
and generation 6 dendrimers inside a micelle core are consecutively
compared, the ratio is 5.2. Using eq , this results in a micelle size of 43 nm in diameter,
which corresponds well with the diameter found with DLS for generation
6 based micelles. So, in other words, the NMR signals of the G6 dendrimer,
which apparently is highly mobile inside the micellar core, are clearly
observable, and its diffusion coefficient then correlates to the hydrodynamic
radius of the whole micelle in whose core it is residing. The micelle
appears to be 5.2× larger in diameter than the dendrimer itself
and corresponds with the dimensions obtained with DLS. In volume the
micelle is then 140× larger than the PAMAM G6.The diffusion
coefficients of the free dendrimers of generations
4, 5, and 6 increase with decreasing dendrimer generation, as the
dendrimer size is proportionally increasing with each generation.
In contrast to this, the diffusion coefficient of the dendrimers is
about the same for all three dendrimer generations in their respective
dendrimicelle solutions, and moreover that small they indicate the
dendrimers are residing inside the micelles (Figure S9). Also, the pseudo-2D DOSY plots corroborate that the micelle
size is independent of dendrimer generation, in agreement with the
DLS results and previous research.[27] DOSY
measurements have been used in micelle studies, e.g., to determine
the critical micelle concentration (CMC) by detecting the core components
free in solution while they were not visible once encapsulated in
micelles[47] or to study drug encapsulation
in micelles.[48] However, to the best of
our knowledge, micellar core components of complex coacervate core
micelles have not yet been detected and identified as residing inside
the micellar core. For free dendrimers in solution typically eight
signals can be discriminated, attributable to one set of four methylene
groups from the repeating units of the dendrimer branches and one
set of four methylene groups from the end ethyleneamide-ethylenamino
group. Due to the high symmetry and branching nature of the PAMAM
dendrimers, the intensities of these eight discernible methylene groups
are close to identical,[37] as can be seen
also from the peaks in Figures S3 and S9. Interestingly, the methylene groups of the dendrimers residing
inside the micellar core are not all equally well discernible. The
peaks of interior methylene groups are more attenuated/broader than
the terminal methylene groups (see Figure C, Figure S26,
and the assignment of dendrimer peaks in Figure S22). This indicates a higher mobility of the terminal dendrimer
parts while the interior parts are less mobile.
Exchange of Dendrimers between Dendrimicelles
For the
fluorescence measurements, amine-terminated PAMAM dendrimers of generations
4, 5, and 6 were functionalized as described previously,[32] by reacting either FITC or RITC with dendrimers.
A low functionalization degree, about 2–4 fluorophores per
dendrimer, was chosen to keep a high charge density on the dendrimers
to avoid interference with micelle formation and to minimize intramolecular
quenching (see Table S1 and Figures S10 and S11). Dendrimicelles were then
formed with each dendrimer generation at a ratio of 1:1 between FITC-
and RITC-functionalized dendrimers. DLS showed sizes of 40–60
nm for all micelles (Figure S12), comparable
to micelles formed with nonfunctionalized dendrimers (Figure A and Figure S1). Likewise, optical spectral properties are not significantly
influenced by micelle formation and no intermolecular quenching was
observed (Figures S13–15).In order to measure the exchange of dendrimers, micelles containing
either only FITC-functionalized dendrimers (donor) or only RITC-functionalized
dendrimers (acceptor) were formed. Micelle solutions were left overnight
to make sure that the systems were at equilibrium and subsequently
mixed at a 1:1 ratio between donor and acceptor micelles. Thus, only
the exchange was studied, not the micelle formation process. The emission
of the donor and acceptor upon donor excitation at 480 nm was measured
every 1 min for 2 h. The ratio between acceptor and donor emissions
(575–615 nm:500–540 nm) was followed to study the exchange.
An increase in the acceptor:donor (A/D) ratio indicates more energy
transfer and therefore an increase in proximity of donors and acceptors,
indicating that the exchange of dendrimers between micelles occurs.
As shown above in the NMR discussion, dendrimers can still freely
move despite encapsulation into micelle cores, meaning that fluorescence
measurements represent an average distance between donor and acceptor
fluorophores.First, two separate samples were measured: i.e.
dendrimicelles
based on only donor-labeled dendrimers and dendrimicelles based on
only acceptor-labeled micelles. The sum of the emission spectra of
these two reference samples was taken as a starting point for the
exchange experiments (0% FRET). Likewise, a premixed sample containing
the donor and acceptor within the same micelle core in a 1:1 ratio
was used as a reference for complete exchange (100% FRET). The fraction
of maximal FRET, αA/D, was determined by normalizing
the measured A/D ratio in the exchange sample to the three reference
samples, using eq with αA/D being a dimensionless
parameter[6] and (A/D)min, (A/D)max, and (A/D) being the acceptor/donor
ratio before mixing (sum of only donor and only acceptor sample),
that of complete exchange (premixed sample), and that from the exchange
sample at time t, respectively.Micelles were
formed containing generation 4, 5, or 6 dendrimers
labeled with either donor or acceptor fluorophores and were consecutively
mixed and monitored over time (Figure A). For generation 6 based micelles, αA/D hardly changes within 2 h (Figure B), indicating a kinetically trapped system or at least
very slow exchange. This is probably due to the high amount of charged
surface groups in higher generations: i.e., theoretically 256 for
generation 6. In contrast to that, in generation 4 based systems FRET
increases rapidly (Figure B). A sharp increase takes place in the first 5 min, followed
by a slow increase reaching the maximum value, and therefore close
to complete exchange, after about 90 min. Generation 5 shows an exchange
efficiency between generations 6 and 4. Again, a fast increase in
the first 20 min can be seen. After that it is increasing slowly,
reaching about 50% exchange after 2 h. A longer measurement shows
that, also after 12 h, only about 50% of maximum exchange was reached
(Figure S16). However, when a control sample
was measured for 12 h, with premixed donor and acceptor present in
the same micellar core, a bleaching effect could be detected after
about 4 h (Figure S17). Therefore, it is
important not to overinterpret the FRET data after the first 4 h in Figure S16, as they can be affected by the bleaching
process.
Figure 2
(A) Cartoon showing three different dendrimicelle samples. Generation
4, 5, and 6 dendrimers are encapsulated in either only donor (green)
or only acceptor (red) micelles. The number of dendrimers per micelle
increases with decreasing dendrimer generation. Different dendrimer
generations are indicated by different sizes. Upon mixing, exchange
of dendrimers between micelles leads to mixed micelles containing
both donor and acceptor. For generation 6 almost no exchange could
be observed and therefore the donor and acceptor stay in separate
micelles. (B) αA/D over time forgeneration 4 (light
gray, circles), generation 5 (dark gray, triangles), and generation
6 (black, squares) based micelles. The first point of each line at
αA/D = 0 corresponds to the combined donor only and
acceptor only spectrum measured for the respective dendrimer generation
system. The dashed line at αA/D = 1 corresponds to
the spectrum of micelles containing both donor and acceptor, representing
complete exchange; also here, for each dendrimer generation system
the respective control samples were measured with the corresponding
generation of dendrimer. Excitation was at 480 nm.
(A) Cartoon showing three different dendrimicelle samples. Generation
4, 5, and 6 dendrimers are encapsulated in either only donor (green)
or only acceptor (red) micelles. The number of dendrimers per micelle
increases with decreasing dendrimer generation. Different dendrimer
generations are indicated by different sizes. Upon mixing, exchange
of dendrimers between micelles leads to mixed micelles containing
both donor and acceptor. For generation 6 almost no exchange could
be observed and therefore the donor and acceptor stay in separate
micelles. (B) αA/D over time forgeneration 4 (light
gray, circles), generation 5 (dark gray, triangles), and generation
6 (black, squares) based micelles. The first point of each line at
αA/D = 0 corresponds to the combined donor only and
acceptor only spectrum measured for the respective dendrimer generation
system. The dashed line at αA/D = 1 corresponds to
the spectrum of micelles containing both donor and acceptor, representing
complete exchange; also here, for each dendrimer generation system
the respective control samples were measured with the corresponding
generation of dendrimer. Excitation was at 480 nm.For generation 5, in total three different micelle
concentrations
were tested: i.e., with 0.9, 0.45, and 0.23 μM of G5 concentration
(Figure S18). As the exchange seems to
be independent of concentration, the main exchange mechanism is probably
expulsion and insertion, meaning that single polymers or small neutral
clusters are expulsed from one micelle followed by insertion into
another micelle.[16] Still, this does not
explain the two observed exchange rates: i.e., the initial fast increase
in αA/D and the following slower increase. So, whereas
expulsion and insertion seems to be the main exchange process, other
processes can also take place. Hollapa et al. got similar results
for polyelectrolyte complexes; they identified the fast exchange as
expulsion and insertion and the slower exchange as fusion and fission,
which is the splitting and consequent merging of micelles.[49] However, as we see a logarithmic increase over
time (Figure S19), according to Lund et
al. this cannot be attributed to only two exchange mechanisms but
is better explained by a broad distribution of many different exchange
rates.[50] They showed that defects in the
polymer structure as well as differences in activation energy and
hierarchical constrained dynamics could play a role. Hierarchical
constrained dynamics could imply for dendrimicelles that dendrimers
positioned at the outer side of the micellar core exchange faster
and more often than dendrimers in the center of the core structure,
as more rearrangements are needed for that to happen. Therefore, the
exchange process of dendrimicelles remains a very complex process
but according to our data consisting of predominantly expulsion and
insertion pathways, yet other processes might play minor roles as
well.A first-order reasoning to explain the difference between
the exchange
dynamics of micelles based on the three different generations is the
number of charges per dendrimer. Generation 4 and the block copolymer
pMAA64-b-pEO885 have the same
number of charges at the tested pH 7.0 (theoretically 64). So, in
theory, only one block copolymer can be attached to one G4 dendrimer,
making it relatively easy for the dendrimer–block copolymer
system to leave a micelle as a small neutral complex. For C3Ms in
fact this is more favorable than exchange of single polyelectrolyte
unimers.[19] Generation 6, in contrast, has
256 charges, meaning that in theory at least four block copolymers
should bind to one dendrimer to compensate for all the positive charges.
As this would probably require more rearrangements of electrostatic
bonds, the expulsion rate is decreased, making it more difficult to
leave the micelle.[19] Generation 5 has 128
charges and is an intermediate between G6 and G4 and indeed behaves
accordingly. This suggests that the surface charge and multivalent
charge interactions are important for the exchange rate of dendrimers
between micelles. However, this is not a complete description, as
between generations of dendrimers not only the number of end groups
is changing but also the charge density: i.e., the charges per dendrimer
surface and volume.[51] As a rough estimate,
considering the diameter of the dendrimers, the dendrimer surface
increases by a factor of 2 on going from G4 to G6 PAMAM, while the
charge quadruples. Thus, the charge density becomes higher on moving
to higher generations, which will have its effects on the efficiency
of interactions of the block copolymer with the dendrimer. Such discussions
need to be taken with caution, as for higher generations defects are
also more commonly found, such as missing or back-folding of part
of the branches,[52] obviously affecting
the charge density.Next, a mixture of different dendrimer generations
within one micelle
core was prepared. Generations 4 + 5, 4 + 6, and 5 + 6 were studied
(Figure S21A). For each experiment, both
generations are present within the same micelle, meaning that e.g.
FITC-functionalized G4 and G5 are present in the donor micelle and
RITC-functionalized G4 and G5 are present in the acceptor micelle.
Micelle formation was confirmed by DLS for all three combinations
(Figure S20) and the exchange monitored
(Figure S21B). The combination G4 + G5
shows a fast exchange, reaching about 80% exchange after 2 h. This
is close to what was seen for only G4, although the initial rapid
increase is slower for the mixture than for only G4-based dendrimicelles,
finished after 15 min and after 5 min, respectively. The mixtures
of generations 4 and 6 as well as of 5 and 6 show an intermediate
between the exchange rates for the respective single generations seen
in Figure B. Generations
4 and 5 are still exchanging between micelles, leading to an increased
αA/D, but the exchange rate is slower compared to
only generation 4 or 5 micelles. The data from a previous section
and this section show that the exchange rate and hence the stability
of dendrimicelles can be tuned by using different single-dendrimer
generations or a mix thereof. At the same time, these data also prove
that different dendrimer generations can be encapsulated within one
micelle core, in line with our previous work in which differently
functionalized dendrimers of the same generation were incorporated
inside a single micelle core.[32]
Exchange of G6 Dendrimers between Micelles Prepared at pH 7.8
In the experiments described thus far, dendrimicelles were formed
at pH 7.0 as the dendrimers and the carboxyl groups of the block copolymer
are positively and negatively, respectively, charged at this pH value.
At higher pH values the dendrimer surface charge decreases as fewer
primary amines are protonated. As from the previous experiments it
was clear that the charge and probably charge density play an important
role in the exchange dynamics, we envisioned to use this to stimulate
the exchange of higher-generation dendrimers. Dendrimicelles are stable
in a pH range of ∼6 to ∼8;[28] thus, we decided to measure the exchange of generation 6 dendrimers
in dendrimicelles prepared at a pH of 7.8 (Figure A). Importantly, at this pH not all of the
primary amines of a dendrimer are protonated and actually the overall
charge is about 25% lower than that of a completely charged generation
6 dendrimer.[53] A generation 6 dendrimer
with only 75% of its maximum charges has about 192 charges, which
corresponds to a virtual kind of generation 5.5 PAMAM at pH 7.0, considering
only the surface charges. The increase in pH is not expected to influence
the charge of the block copolymer, with the pKa of the carboxylic acid groups being ∼4.5. In order
to avoid effects related to changing the pH during or after mixing,
the dendrimicelles were formed already at pH 7.8, at the theoretical
charge stoichiometric conditions at that pH. Figure B shows that the size is similar to that
of a G6-based dendrimicelle formed at pH 7.0, but more dendrimers
are present per micelle, as we have less charge per dendrimer at this
higher pH value.[54,55]Figure C shows the exchange dynamics of generation
6 at pH 7.0 and 7.8. The initial absence of FRET at pH 7.8 indicates
a kinetically trapped G6 system, similar to what is observed for generation
6 dendrimicelles at pH 7.0. However, in contrast to the pH 7.0 data
(see Figures B and 3C), at pH 7.8 an eventual clear increase in FRET
is seen, about 20% after 2 h. Apparently, the G6 at pH 7.8, which
correpsonds to a virtual generation 5.5 at pH 7, forms dendrimicelles
at the borderline between kinetically trapped and (slow) exchanging.
This is highlighted in the cartoon in Figure A, with the resulting dendrimicelles showing
a mix of differntly labeled dendrimers in the core, but still a clear
excess of either the donor- or acceptor-labeled dendrimers.
Figure 3
G6-based dendrimicelles
formed at either pH 7.0 or pH 7.8 under
stoichiometric conditions. (A) Cartoon showing the two different micelle
samples. Micelles containing either a donor or acceptor were mixed
in a 1:1 ratio. Exchange of dendrimers leads to mixed micelles containing
donor as well as acceptor fluorophores. As previously observed, generation
6 at pH 7.0 does not exchange. (B) DLS plot of G6-based micelles at
pH 7.0 (black) and 7.8 (dark gray) containing both donor and acceptor
in a 1:1 ratio. (C) αA/D over time for generation
6 at pH 7.8 (gray, triangles) and generation 6 at pH 7.0 (black, squares).
The data points from generation 6 at pH 7.0 are repeated from Figure B for comparison.
The first point of each line at αA/D = 0 corresponds
to the sum of a donor-only and an acceptor-only spectrum. The dashed
line at αA/D = 1 corresponds to the spectrum of micelles
containing both a donor and acceptor, representing the maximum exchange.
The excitation wavelength was 480 nm.
G6-based dendrimicelles
formed at either pH 7.0 or pH 7.8 under
stoichiometric conditions. (A) Cartoon showing the two different micelle
samples. Micelles containing either a donor or acceptor were mixed
in a 1:1 ratio. Exchange of dendrimers leads to mixed micelles containing
donor as well as acceptor fluorophores. As previously observed, generation
6 at pH 7.0 does not exchange. (B) DLS plot of G6-based micelles at
pH 7.0 (black) and 7.8 (dark gray) containing both donor and acceptor
in a 1:1 ratio. (C) αA/D over time for generation
6 at pH 7.8 (gray, triangles) and generation 6 at pH 7.0 (black, squares).
The data points from generation 6 at pH 7.0 are repeated from Figure B for comparison.
The first point of each line at αA/D = 0 corresponds
to the sum of a donor-only and an acceptor-only spectrum. The dashed
line at αA/D = 1 corresponds to the spectrum of micelles
containing both a donor and acceptor, representing the maximum exchange.
The excitation wavelength was 480 nm.
pH-Responsive Release and Exchange of G6-Dendrimers from Dendrimicelles
Following up on the data obtained in the previous section, we hypothesized
we could exploit the G6 dendrimer properties at different pH values
to investigate the responsive release of dendrimers from a micelle
core. After G6-based dendrimicelle formation at pH 7.8 under charge
stoichiometric conditions, the pH was subsequently decreased to 7.0.
This lowering of the pH results in an increase in the degree of protonation
of the primary amine groups of the dendrimer and therefore results
in an excess of positive charges in the micelle core with respect
to the block copolymer charge. We hypothesized that this would lead
to a rearrangement of the micelles aiming for charge stoichiometry.
During this process dendrimers should then be released (Figure A, left part).
Figure 4
(A) G6-based micelles
formed at pH 7.8 under stoichiometric conditions.
Before mixing donor and acceptor micelles, the pH was decreased to
7.0, resulting in a nonstoichiometric condition leading to the realease
of dendrimers. (B) αA/D over time after changing
the pH to 7.0. The first point at αA/D = 0 corresponds
to the sum of a donor-only and an acceptor-only spectrum. The dashed
line at αA/D = 1 corresponds to the spectrum of micelles
containing both donor and acceptor, representing the maximum exchange.
The excitation wavelength was 480 nm. (C) DOSY spectrum of an aged
sample of nonfunctionalized G6-based dendrimicelles after changing
the pH from 7.8 (stoichiometric) to 7.0. Only the dendrimer signals
are shown. The 1D spectrum at the top part was taken with 30% gradient
strength. Note: in contrast to the DOSY plot in Figure , here the free dendrimer and the dendrimer-inside-micelle
are both present in the same NMR tube and this is a single DOSY experiment
proving the release of dendrimers from micelle cores. (D) G6-based
micelles formed at pH 7.0 under stoichiometric conditions. Before
mixing donor–and acceptor micelles, 25% of unlabeled G6 dendrimers
were additionally added, resulting in a nonstoichiometric condition.
(E) αA/D over time after addition of free dendrimers.
The first point at αA/D = 0 corresponds to the sum
of a donor-only and an acceptor-only spectrum. The dashed line at
αA/D = 1 corresponds to the spectrum of micelles
containing both donor and acceptor, representing the maximum exchange.
The excitation wavelength was 480 nm.
(A) G6-based micelles
formed at pH 7.8 under stoichiometric conditions.
Before mixing donor and acceptor micelles, the pH was decreased to
7.0, resulting in a nonstoichiometric condition leading to the realease
of dendrimers. (B) αA/D over time after changing
the pH to 7.0. The first point at αA/D = 0 corresponds
to the sum of a donor-only and an acceptor-only spectrum. The dashed
line at αA/D = 1 corresponds to the spectrum of micelles
containing both donor and acceptor, representing the maximum exchange.
The excitation wavelength was 480 nm. (C) DOSY spectrum of an aged
sample of nonfunctionalized G6-based dendrimicelles after changing
the pH from 7.8 (stoichiometric) to 7.0. Only the dendrimer signals
are shown. The 1D spectrum at the top part was taken with 30% gradient
strength. Note: in contrast to the DOSY plot in Figure , here the free dendrimer and the dendrimer-inside-micelle
are both present in the same NMR tube and this is a single DOSY experiment
proving the release of dendrimers from micelle cores. (D) G6-based
micelles formed at pH 7.0 under stoichiometric conditions. Before
mixing donor–and acceptor micelles, 25% of unlabeled G6 dendrimers
were additionally added, resulting in a nonstoichiometric condition.
(E) αA/D over time after addition of free dendrimers.
The first point at αA/D = 0 corresponds to the sum
of a donor-only and an acceptor-only spectrum. The dashed line at
αA/D = 1 corresponds to the spectrum of micelles
containing both donor and acceptor, representing the maximum exchange.
The excitation wavelength was 480 nm.First, NMR measurements show that dendrimers are
indeed released
from the micelles after lowering the pH from 7.8 to 7.0 (Figure C). The DOSY plot
clearly shows two types of dendrimers: i.e. dendrimers still encapsulated
in micelle cores and released dendrimers free in solution. The released
dendrimers show a higher diffusion coefficient and slightly upfield
shifted signals. In theory, approximately 25% of the dendrimers could
be pushed out of the micelles after decreasing the pH, corresponding
to a free dendrimer concentration of about 0.6 μM. Additional
proton and DOSY-filtered NMR spectra from the same sample before (Figures S23 and S24) and after (Figures S25 and S26) changing the pH to 7.0 confirm the release
of dendrimers. At pH 7.0, extra peaks appear with a slight upfield
shift, corresponding to released dendrimers, whereas these are not
visible at pH 7.8. The peaks of the released dendrimers overlay with
the peaks from dendrimers free in solution. Mostly the peaks labeled
as C, c and D (highlighted by the black box in Figures S23–S26) are illustrative, as the other dendrimer
peaks are influenced by overlapping residual MOPS buffer peaks. By
comparing the peak height of dendrimers inside micelles and released
dendrimers, a release of about 10–15% is estimated (peak at
3.47 ppm to 3.44 ppm, respectively). Furthermore, DLS measurements
of the same micelle sample show a discrete decrease in scattering
intensity after changing the pH from 7.8 to 7.0, additionally corroborating
the release of dendrimers from micelles (Table S2). The observation of free G6 in solution proves that dendrimers
are pushed out of the micellar core when the pH is changed from 7.8
to 7.0. This lowering of the pH causes an excess of positive charges
inside the core, and the charge stoichiometry is then restored by
the release of part of the dendrimers. By releasing part of the dendrimers
into solution, the aggregation number of the dendrimicelles is then
back to the “normal” one at pH of 7.0: i.e., 30 dendrimers
per micelle for G6.[29]Interestingly,
complementary to the NMR data shown above that were
obtained from a several days old sample, i.e. when dendrimers have
been released from the micelles, the FRET experiment in Figure B shows an increase in time
of the FRET in the first hours after lowering the pH. The FRET data
indicate that there is exchange of the G6 dendrimers between micelle
cores taking place now also at pH 7.0, whereas freshly prepared G6
dendrimicelles do not show such an exchange (Figure B). The exchange after 2 h is about 15–20%
of the maximum FRET. Combining the conclusions from the NMR and FRET
experiment, we can state that release of dendrimers is taking place;
moreover, the excess of about 25% of dendrimers in solution with respect
to the charge stoichiometry at pH 7.0 also results in the G6 dendrimers
exchanging between micellar cores. To corroborate this, exchange between
generation 6 based dendrimers was measured at pH 7.0 after adding
25% of (unlabeled) generation 6 dendrimers (Figure D). Again a change corresponding to an exchange
of about 15–20% was visible after 2 h (Figure E), confirming that the addition of dendrimers
can influence the kinetic stability of the cores of dendrimicelles
and initiate slow exchange of dendrimers between generation 6 based
dendrimicelles. As unlabeled dendrimer is added, the overall exchange
is slightly higher than the corresponding 15–20% shown in the
exchange described in the earlier experiments. On the one hand, from
earlier FRET experiments it is known that the FRET efficiency remains
unaltered when mixing in up to 30% of nonlabeled dendrimers into the
core containing a mix of donor- and acceptor-labeled dendrimers.[32] On the other hand, the release of also fluorophore-labeled
dendrimers from micelle cores results in an overall lower αA/D.
Conclusion
We have presented the formation of dendrimicelles
containing generation
4, 5, and 6 PAMAM dendrimers. NMR and especially DOSY measurements
unambiguously prove that the dendrimers are residing inside the micelles
for all tested generations and are still moving and/or rotating fast
enough on the NMR time scale to allow high-resolution spectra. Dendrimers
functionalized with either FITC or RITC were used to study the exchange
of dendrimers between the cores of micelles by monitoring the change
in FRET signal. The results showed that generation 6 based dendrimicelles
are kinetically trapped, whereas generation 5 and 4 based micelles
do show exchange of the dendrimers between micelles. The exchange
rate of smaller generations is faster than that for larger dendrimer
generations, meaning that probably the number of charges plays a major
role in determining the speed of exchange events. Thus, the exchange
rate can be tuned from kinetically trapped systems to fast dynamics
using different dendrimer generations, and further also by mixing
two different generations within the same micelle core. So far only
mixtures of two different generations and a mixing ratio of 1:1 between
generations based on the number of dendrimers have been studied. Different
ratios could even lead to more control of exchange rates. As the exchange
rate is independent of concentration, expulsion and insertion are
the dominant exchange mechanisms for dendrimicelles. Furthermore,
exchange rates can also be tuned by forming micelles at higher pH
values and therefore de facto changing the number of charges per dendrimer.
Forming generation 6 based micelles at pH 7.8 and thereby decreasing
the charge per G6 dendrimer by about 25% results in borderline micelles
with very slow exchange kinetics, whereas no dynamics were detected
at pH 7.0. It is likely that not only the number of charges but also
the charge density, i.e. the charge per volume, influences the exchange
rate. Current efforts are under way to corroborate the dynamics with
computational models linking the charge density of the dendrimers
with that of the block copolymers. By changing the pH after micelle
formation from 7.8 to 7.0, thereby increasing the charge per dendrimer,
micelle rearrangements are induced in which dendrimers are released
from the micelle cores, which has been unambiguously proven by DOSY
NMR measurements. This dendrimer release at the same time initiated
exchange of generation 6 dendrimers between micelles. In fact, exchange
of kinetically trapped generation 6 dendrimers from micelle cores
can also be initiated by addition of free dendrimer to a micelle solution.
Having a detailed understanding and control of the dendrimer exchange
is important for e.g. drug delivery applications, and we believe that
this is an important step forward toward the designs of responsive
materials. For example, various strategies can be designed that allow
for different time scales for release and/or exchange by playing with
the various relevant parameters of the toolbox.
Experimental Section
Materials
Amine-terminated polyamidoamino dendrimers,
generations 4, 5, 6, were purchased from Dendritech Inc., MI, USA,
as a 5 wt % methanolic solution and used as a 2.89 mM aqueous solution
based on primary amine content. pMAA64-b-pEO885 (Mw/Mn = 1.15) was obtained from Polymer Sources Inc., Canada,
and used as a 5 mM aqueous solution based on carboxylic acid content.
Fluorescein isothiocyanate, rhodamine B isothiocyanate, 3-(N-morpholino)propanesulfonic acid (MOPS) sodium salt, and
1 M NaOH solutions were obtained from Sigma-Aldrich.
Characterization
DLS was done on a Malvern Zetasizer
Nano S instrument equipped with a laser operating at 633 nm. NMR spectra
of the mixture of generation 6 PAMAM-NH2 and PAMAM-OH in
D2O were obtained on a Bruker Avance III spectrometer operating
at 500 MHz for 1 H, equipped with a 5 mm TXI probe. NMR spectra of
generation 6 PAMAM-NH2 in MOPS buffer and D2O were obtained on a Bruker Avance III spectrometer operating at
600 MHz for 1 H, equipped with a 2.5 mm SEI probe. All other NMR spectra,
of nonfunctionalized free dendrimers and micelles in D2O, were obtained on a Bruker NEO spectrometer operating at 28.2 T
(1200 MHz 1H-Larmor frequency), equipped with a 3 mm room-temperature
probe. All NMR spectra were analyzed using Topspin. Diffusion coefficients
were obtained by fitting the attenuated signals of the series of 1D
DOSY spectra. Fluorescence emission spectra were acquired on a Cary
Eclipse spectrophotometer. Absorbance spectra were obtained on a Shimadzu
UV-1900 UV–vis spectrophotometer.
Dendrimer Functionalization
Functionalization was done
as described previously.[32] Briefly, 2 mg
of PAMAM dendrimers of generation 4, 5, or 6 in methanol were added
to a vial. Amounts of 4–6 mol equiv of fluorescein isothiocyanate
(FITC) or rhodamine B isothiocyanate (RITC) with respect to the dendrimers
were dissolved in 1 mL of methanol and added dropwise to the dendrimer
solution, with mixing. The mixture was stirred at room temperature
for several hours and covered with aluminum foil. Afterward, the solvent
was evaporated under reduced pressure and the dried product was dissolved
in demineralized water. Unreacted FITC or RITC was removed by dialysis
against demineralized water using a dialysis membrane with a molecular
cutoff of 3.5–5 kDa, covered with aluminum foil. The purified
functionalized dendrimers were again dried under reduced pressure
and dissolved in D2O for NMR analysis. The dendrimer concentration
was determined with NMR using the internal standard TMSP-D4, and the
functionalization degree was calculated using UV–vis.
Dendrimicelle Formation
Dendrimicelles were formed
under charge stoichiometric conditions following an established protocol.[45] For this, 20 μL of an aqueous 2.89 mM
PAMAM dendrimer solution (charge concentration based on surface groups)
was added to 20 μL of 0.2 M MOPS buffer at pH 7. This solution
was dissolved in 149 μL of demineralized water. Afterward, 11
μL of an aqueous 5 mM pMAA64-b-pEO885 solution (charge concentration based on −COO−)
was added during sonication for 2 min. Samples were left to equilibrate
overnight before characterization and exchange experiments. To make
stoichiometric micelles at pH 7.8, only 8.25 μL of the block
copolymer solution was added to compensate for fewer positive charges
on the dendrimers.
Determination of Critical Micelle Concentration
The
critical micelle concentration was determined with dynamic light scattering
by measuring micelles at different concentrations. The scattering
intensity was converted to the excess Rayleigh ratio according to
the equationwith Rθ being the excess Rayleigh ratio at scattering angle
θ, Rtoluene the known Rayleigh scattering
ratio of toluene (1.35 × 10–3 m–1), nsolvent and ntoluene the refractive indices of water and toluene (1.333
and 1.497, respectively), and Isample, Isolvent, and Itoluene the scattering intensities of the sample, water and toluene, respectively.By plotting the excess Rayleigh ratio versus the total polymer
concentration (block copolymer + dendrimer) and a linear fitting,
the CMC is determined from the intersection with the x axis.
Exchange Experiment
For exchange experiments, dendrimicelles
containing only the donor (dendrimers functionalized with FITC) or
only the acceptor (dendrimers functionalized with RITC) were prepared
according to the aforementioned protocol. For all samples the charge
concentration of the dendrimers was kept the same. The next day, the
samples were diluted five times to avoid an inner filter effect. To
measure the exchange, half of the only-donor and half of the only-acceptor
samples were mixed at a 1:1 ratio (500 μL each) and measured
immediately after mixing every 1 min for 2 h. The excitation wavelength
was 480 nm, and the emission range was 490–700 nm. To calculate
the A/D ratio, integrals from 500 to 540 nm (donor, D) and from 575
to 615 nm (acceptor, A) were taken.As reference sample 1 for
the starting point, the other half of each sample (500 μL) was
mixed with 500 μL of a dendrimicelle solution containing nonfunctionalized
dendrimers. This was done to keep the total volume and the micelle
concentration the same. The fluorescence emission spectra of both
samples, only-donor and only-acceptor mixed with nonfunctionalized
dendrimicelles, were measured separately with an excitation wavelength
of 480 nm. The sum of these two spectra was used to calculate the
starting A/D ratio for the exchange experiment.Reference sample
2, containing both the donor and the acceptor
within one micelle at a 1:1 ratio, was prepared to determine the maximum
A/D ratio showing complete exchange. The fluorescence emission spectrum
of this sample was recorded with an excitation wavelength of 480 nm.To get the αA/D value, the A/D ratios for the
exchange sample were then normalized to the A/D ratios from the two
reference samples, using eq .For the mixed-generation micelles, both generations
are always
present in all micelles. The ratio between the two generations is
always 1:1, based on the number of dendrimers.
Authors: Denis Dorokhin; Nikodem Tomczak; Mingyong Han; David N Reinhoudt; Aldrik H Velders; G Julius Vancso Journal: ACS Nano Date: 2009-03-24 Impact factor: 15.881
Authors: Jan Bart Ten Hove; Junyou Wang; Matthias N van Oosterom; Fijs W B van Leeuwen; Aldrik H Velders Journal: ACS Nano Date: 2017-11-07 Impact factor: 15.881