3.1. Physicochemical Properties of the Chit-g-PNIPAM+DNA Polyplexes
A series of DLS and ELS measurements were conducted in order to examine the physicochemical properties of the Chit-
g-PNIPAM+DNA polyplexes formed at different N/P ratios for both DNA samples (50 and 2000 bp) under study. The obtained results regarding the scattered intensity, the values of the hydrodynamic radius (
Rh) of the various scattering populations discerned, evidenced by the different peaks of the corresponding size distribution functions (SDFs), with the SDFs for the pure components are also included for comparison, along with the zeta potential of the polyplexes are shown in
Figure 1, as a function of the N/P ratio. As mentioned in the description of the preparation of the polyplexes (see
Section 2.3), the dispersion at N/P = 0.5 for the short DNA series (50 bp) and the one at N/P = 1 for the long one (2000 bp) exhibited precipitation after equilibration, which of course is a direct indication of extended aggregation. For these samples the measurements were conducted on the supernatant and the corresponding obtained data are denoted appropriately.
As seen in
Figure 1a, the mass (which is directly proportional to the scattered intensity) of the polyplexes formed between the Chit-
g-PNIPAM graft copolymer and either the short or the long DNA exhibits its highest values for N/P ratios below 1 (i.e., estimated charge neutralization point). Please note that for the precipitated dispersions the measured intensity values correspond to only a small fraction of the total mass (since most of the polyplexes/aggregates have precipitated), otherwise they would have been much higher. Therefore, it can be deduced with relative certainty that, for N/P ≤ 1, the interaction between the two components is extremely strong or, in other words, the excess of DNA related to the available amino groups of Chit-
g-PNIPAM leads to the formation of large/massive polyplexes or aggregates. These formations are most probably colloidally unstable due to charge neutralization, along with their increased mass, thus undergoing secondary aggregation and eventually precipitating. As far as the comparison between the two DNAs is concerned, it seems that at N/P = 1 the polyplexes formed with the short DNA do not reach the stoichiometry (no precipitation observed) of those formed with the long one which already precipitated at this ratio. Apparently, the long DNA enables to a greater extent the secondary aggregation of the polyplexes, probably acting as a bridging agent between them. At the same time, when the DNA2000 sample is in excess at N/P = 0.5, it looks like it provides additional charges and thus the formed polyplexes/aggregates are still stable although very massive and/or compact, as evidenced by the extremely high scattered intensity. By the same reasoning, the fact that the short DNA forms stable polyplexes close to the nominal charge neutralization point (N/P = 1) could be an indication of its greater ability to be incorporated and efficiently accommodated into the formed polyplexes, due to its smaller size. Nevertheless, as the content of the DNA50 sample increases further (N/P = 0.5), extensive aggregation (leading to precipitation) is also induced, likely as a result of the large-scale charge neutralization. When the Chit-
g-PNIPAM copolymer is in excess and thus there is a surplus of positive charges, that is, for N/P > 1, the resulting polyplexes are less massive/dense and colloidally stable. This is directly correlated to the solubility of the graft copolymer (due also to the contribution of soluble non-interacting PNIPAM chains) and the fact that the formed polyplexes comprise an increased number of Chit-
g-PNIPAM chains, especially in comparison to the ones formed at lower N/P ratios. Lastly, it is worth mentioning that for the same N/P values the polyplexes formed with the long DNA have a higher mass or are more compact than the ones with the short DNA, possibly indicating a higher degree of interaction with the graft copolymer.
Regarding the size of the formed polyplexes, the obtained SDFs shown in
Figure 1c,d reveal the presence of various peaks providing valuable insights. First of all, the pure Chit-
g-PNIPAM solution exhibits two peaks indicating two scattering populations in solution, with corresponding
Rh values in the range of 10 to 20 nm for the small one and about 600 or 300 nm for the large one. This difference in the size of the second peak between the two SDFs is attributed to the fact that they correspond to different prepared stock Chit-
g-PNIPAM solutions. Still, the presence of the second large peak indicates that the graft copolymer exhibits some degree of self-assembly forming multi-chain aggregates, most probably due to hydrophobic interactions stemming from the chitosan backbone or intra-polyelectrolyte interactions of the copolymer. Hence, most probably both single Chit-
g-PNIPAM copolymer chains and multi-chain aggregates coexist in the solution. The same stands for the two DNA samples as well, since they also exhibit two peaks, with
Rh values about 20 and 100 nm for the short DNA or about 70 and 700 nm for the long one, in direct proportion to the respective lengths of the two nucleic acids. As far as the polyplexes of the Chit-
g-PNIPAM+DNA50 system are concerned, at high N/P values (i.e., 2 and 4) the SDFs are similar to that of the pure copolymer, or in other words the sizes of the two populations of polyplexes are dictated by the corresponding populations of the graft copolymer which is in excess. More specifically, the smaller population has an
Rh of about 20 nm (
Figure 1b), somewhat larger both in size and overall intensity compared to that of the pure Chit-
g-PNIPAM, which is additional confirmation of the formation of polyplexes. Note that this population most likely indicates polyplexes formed between the original single copolymer chains and DNA molecules. In parallel, the second peak denotes an
Rh of about 400 nm, which is somewhat smaller than the size of the multi-chain aggregates of the copolymer. So, it seems that there is some shrinking of the Chit-
g-PNIPAM aggregates upon binding of the DNA50 molecules, probably due to the reduction of electrostatic repulsions caused by charge neuralization and screening. This effect is even more pronounced at N/P = 1, where only one peak with an intermediate size around 75 nm is observed, indicating the formation of compact/dense polyplexes (also evidenced by the increased scattered intensity), possibly incorporating a large number of Chit-
g-PNIPAM copolymer chains and short DNA molecules. For the precipitated dispersion at N/P = 0.5 an additional population of very large aggregates (
Rh ≈ 2 μm) can still be detected in the supernatant, denoting the occurring extended secondary aggregation. Quite interestingly, for the Chit-
g-PNIPAM+DNA2000 system the SDFs show only one peak/population, with a rather similar size of about 75 nm for all three stable dispersions. This signifies the formation of compact and/or dense polyplexes regardless of the aggregation state and content of the graft copolymer, which is obviously a direct consequence of the length of the specific DNA sample. This means that the long DNA molecules cannot be incorporated in the pre-existing multi-chain aggregates of the Chit-
g-PNIPAM copolymer without changing their structure much (as in the case of the short DNA sample). Again, in the case of the dispersion showing precipitation (N/P = 1) a relatively larger population (
Rh ≈ 600 nm) compared to the rest can be discerned, indicative of the secondary aggregation.
The information about the effective charge of the formed polyplexes, derived from the acquired zeta potential values shown in
Figure 1e, are in line with the assumptions made so far. Starting at the highest N/P value, both Chit-
g-PNIPAM+DNA50/2000 systems exhibit relatively strong positive values, close to the corresponding one measured for the pure copolymer, which is about +50 mV. This observation confirms that when the graft Chit-
g-PNIPAM copolymer is in excess, the overall properties and conformation of the formed polyplexes are mostly dictated by the copolymer’s intrinsic conformational/aggregation state and characteristics. As the N/P ratio decreases (by increasing the DNA content), a gradual decrease in the zeta potential of the polyplexes can be observed, reaching values close to zero for the short DNA sample, or even negative values (i.e., charge reversal) in the case of the long one. It is thus confirmed that the polyplexes formed at N/P ratios close to 1 are characterized by reduced overall charge, as a result of the charge neutralization that takes place upon the electrostatic interaction of the two components. Of course, a reduction of the overall charge of the polyplexes (or in other words zeta potential values close to zero) also entails colloidal instability, which leads to the observed precipitation. Apparently, the presence of PNIPAM soluble chains cannot prevent precipitation of the formed polyplexes. One final point worth noting is that for the long DNA, the polyplexes formed at N/P = 0.5 show negative zeta potential as a result of the excess of DNA, which also imparts additional stability to the system. It seems that the increased conformational constraints of the longer DNA chains prevent them from being fully incorporated into the formed polyplexes, in contrast to the shorter DNA macromolecules.
In order to gain further insight regarding the morphology of the polyplexes, STEM imaging was performed on the polyplexes formed at N/P = 4 for both Chit-
g-PNIPAM+DNA50/2000 systems, as shown in
Figure 2. In both cases spherical homogeneous nanostructures of various sizes and rather loose, urchin-like structures are observed. Obviously, the density of the polyplexes decreases close to their periphery and rather straight or slightly curved bundles of complexed copolymer/DNA chains are visible in the outer parts of the formed nanostructures (especially in the DNA50 case). The latter characteristic may be a result of the semirigid nature of DNA and chitosan backbone and hint towards a ladder-like coassembly of the primary DNA/graft copolymer complexes. However, DNA2000 may be more well condensed in the primary complexes due to its longer length that gives it high conformational adaptability upon complexation. Notably, for the Chit-
g-PNIPAM+DNA50 system there is a better distinction between populations of different sizes (i.e., small vs. large particles), while quite the opposite stands for the Chit-
g-PNIPAM+DNA2000 system, where a broader distribution of sizes is observed. Nevertheless, the overall size of the polyplexes formed between the graft Chit-
g-PNIPAM copolymer and the short DNA sample is bigger than that of the ones formed with the long DNA, in accordance with the corresponding DLS results. As seen more clearly in the higher-magnification images (
Figure 2c,d), the large polyplexes corresponding to the DNA50 or DNA2000 sample have a diameter of about 1 μm or 500 nm, respectively. In general, the size derived from the STEM images is somewhat larger than the hydrodynamic size measured by means of DLS, because nanostructures of loose morphology like the ones under study are expected to adopt a more flattened conformation upon surface deposition and after solvent evaporation. Still, there seems to be a greater inconsistency between the two methods for the Chit-
g-PNIPAM+DNA2000 system, with the STEM size of the polyplexes (radius about 250 nm) being significantly larger than the corresponding
Rh value (~75 nm). One possible explanation for this is that since the distribution of sizes is broader in this case, the DLS technique is not able to fully distinguish between different populations and thus underestimates to some extent the size of the larger polyplexes.
3.2. Temperature Response of the Chit-g-PNIPAM+DNA Polyplexes
As anticipated, the presence of the PNIPAM side chains imparts a thermoresponsive character to the Chit-
g-PNIPAM graft copolymer [
26], which can be exploited in potential bioapplications like gene delivery. More specifically, the temperature-induced increase in hydrophobic interactions (due to the phase transition of PNIPAM chains) could potentially facilitate the interaction with cell membranes and thus enhance cellular uptake. Therefore, the investigation of the thermal response of the already formed Chit-
g-PNIPAM+DNA50/2000 polyplexes is of particular interest. For this reason, DLS measurements of representative polyplex stable dispersions from both systems at a range of temperatures from 25 to 45 °C, i.e., within the biologically relevant temperature range, were performed.
Figure 3 presents the obtained results in regard to the increase in the scattered intensity (i.e., the initial values have been shifted to zero for clarity), and the
Rh values of the different peaks discerned in the corresponding SDFs, as a function of temperature, for the stable polyplexes formed at N/P = 4 of both Chit-
g-PNIPAM+DNA50/2000 systems. Similar measurements were also performed for the non-precipitated dispersions at the lowest N/P values of each system (i.e., N/P = 1 or 0.5 for the DNA50 or DNA2000 samples, respectively), as well as the pure Chit-
g-PNIPAM copolymer solution for comparison, and the results can be found in the
Supplementary Materials (see
Figures S1 and S2). Note that in all cases after the gradual increase in temperature up to 45 °C, the sample was cooled back to 25 °C and remeasured in order to examine the reversibility of any occurring changes. These measurements are marked as AH, which stands for “after heating”, and the corresponding values in
Figure 3a,b are separated by a dashed line.
A significant increase in the scattered intensity is observed above 35 °C for both systems, as seen in
Figure 3a, with the change being even more pronounced in the case of the polyplexes formed with the short DNA sample. This behavior is also evidenced by the pure Chit-
g-PNIPAM graft copolymer (see
Figure S2), which is attributed to the increase in the hydrophobic interactions and is considered a characteristic trait of the thermoresponsive nature of PNIPAM. At the same time, the size of the DNA2000-based polyplexes seems to be rather unaffected by the increase in temperature, with only a slight broadening of the
Rh peak being discerned in the corresponding SDFs (
Figure 3d). On the contrary, for the DNA50 system a considerable decrease in the size of the larger population is witnessed (
Figure 3c), while for the size of the smaller population there is a much slighter decrease mostly observed at 35 °C. Note that the Chit-
g-PNIPAM copolymer demonstrates an analogous decrease in size (
Figure S2c). Taking all these observations into account, it seems that the large population of polyplexes formed with the short DNA sample have a rather loose conformation/structure, resembling to a large degree that of the multi-chain aggregates of the graft copolymer (see also the corresponding images in
Figure 2a,c). Thus, upon heating they transition to more compact/collapsed configurations (also evidenced by the drastic increase in scattered intensity) due to the increase in the hydrophobic interactions between the PNIPAM side chains (either with one another or with the chitosan backbone). This effect appears less intense in the case of the smaller in size population, probably meaning that they are characterized by a more compact initial conformation that does not really allow for further shrinking upon heating. This also applies for the Chit-
g-PNIPAM+DNA2000 polyplexes whose size exhibits no significant changes, again indicating an increased level of initial compactness. However, it is possible that a small degree of secondary aggregation between the polyplexes occurs, as indicated by the broadening of the
Rh peak and the not so drastic, yet observable, increase in the scattered intensity, owing to the increase in the hydrophobic interactions as temperature rises. Likewise, secondary aggregation upon heating is possibly taking place in the case of the polyplexes formed at N/P = 1 of the Chit-
g-PNIPAM+DNA50 system, according to the observed increase in both the scattered intensity (which is particularly intense) and the corresponding size (see
Figure S1). On the contrary, the polyplexes corresponding to N/P = 0.5 for the DNA2000 sample are practically uninfluenced by the increase in temperature (see
Figure S1), most probably because of the excess of DNA that imparts additional colloidal stability to the system. Overall, the thermal response of the formed polyplexes is closely linked to their conformation/structure, which in turn is a direct consequence of the N/P ratio and the DNA length. Nevertheless, the observed changes are essentially fully reversible in all cases, showcasing the adaptability and resilience of the formed polyplexes.
3.3. Stability of the Chit-g-PNIPAM+DNA Polyplexes
Another important factor for the successful application of potential gene carrier systems, like the ones under consideration, is their stability in various environments. On these grounds, the effect of the increase in the ionic strength on the stable polyplexes of both systems was examined by means of appropriate DLS measurements and the results are shown in
Figure 4. Namely, the change in the scattered intensity (i.e., the initial values have been normalized to one for clarity) and the
Rh values of the different peaks from the corresponding SDFs, for the polyplex dispersions at N/P = 4 of both Chit-
g-PNIPAM+DNA50/2000 systems, are plotted against the ionic strength. The same experimental protocol was also applied on the pure Chit-
g-PNIPAM copolymer solution for comparison and the obtained results are presented in a similar manner in
Figure S3.
As seen in
Figure 4a, the initial addition of salt (0.05 M) in the dispersion of the polyplexes prepared with the short DNA causes a noticeable drop in the scattered intensity, as well as the size of the larger population discerned from the relative SDFs (note that there is also an evident change in the relative intensities of the two peaks). A similar transition is observed for the pure Chit-
g-PNIPAM copolymer as well (see
Figure S3), strengthening the assumption that at low ionic strength values the solubility of the graft copolymer increases due to the reduction in the hydrophobic interactions, thus leading to some degree of dissociation of the initial multi-chain copolymer aggregates. Most probably, this is also the case for the corresponding polyplexes formed between the copolymer aggregates and the DNA molecules. A further increase in the ionic strength up to 0.33 M appears to have no significant effect either on the conformation or the size of the formed polyplexes, which is a good indication of their stability. Even so, when reaching high ionic strength (above 0.43 M) an abrupt increase in the scattered intensity is observed, accompanied by a transition from two to one peak in the corresponding SDFs. It seems that at high salt content the Chit-
g-PNIPAM+DNA50 polyplexes collapse to more compact/dense structures due to the increase in the hydrophobic interactions associated with the worsening of the solubility of the copolymer (see
Figure S3) and the extended charge screening. Moving on to the Chit-
g-PNIPAM+DNA2000 system, analogous transitions of the scattered intensity and the size of the polyplexes are taking place (i.e., initial drop followed by small fluctuations and eventual increase) but to a much smaller variation range. This behavior probably stems from the already more compact initial conformation of these polyplexes that apparently prevents them from adopting more collapsed structures. On the whole, although some conformational rearrangements are inflicted, the polyplexes of both systems exhibit remarkable stability, especially at intermediate ionic strength values that are relevant to biological applications (i.e., about 0.15 M for blood plasma or cell cytoplasm).
Apart from the stability against the ionic strength, it is equally important to test the behavior of the polyplexes when interacting with biological fluids, as a means of simulating their response upon introduction into the human body. For this purpose, parts from the stable polyplex dispersions of both systems were mixed (in equal volumes) with FBS solutions of two different concentrations, i.e., 10 and 50%
v/
v in PBS, and the final equilibrated mixtures were measured by DLS first at room temperature (25 °C) and subsequently at body temperature (37 °C) after incubation for 30 min.
Figure 5 presents the obtained results regarding the increase in the scattered intensity (i.e., the initial values have been shifted to zero for clarity), and the
Rh values of the different peaks from the corresponding SDFs (which are also shown in
Table S1 for better clarity), for the polyplexes at N/P = 4 of both Chit-
g-PNIPAM+DNA50/2000 systems, after mixing with FBS solutions of different contents (10 and 50%
v/
v). Note that values at zero FBS content denote the initial state of the dispersions. Moreover, the small peaks with sizes below 20 nm seen in the SDFs are attributed to FBS (see
Figure S5) and have been excluded from
Figure 5b for clarity reasons. The interaction of the pure Chit-
g-PNIPAM copolymer with FBS was also examined in a similar manner and the corresponding results are shown in
Figure S4, while
Figure S5 displays relevant DLS results for the neat FBS solutions.
The DLS results reveal an increase mainly in the scattered intensity and to a lesser extent the size of the stable polyplexes of the DNA50 sample after mixing with the FBS solutions, with the differences being more pronounced for the high FBS content. Even after incubation at 37 °C small changes are observed. Therefore, it can be assumed that although the polyplexes interact with the components of the FBS solution (mostly proteins and enzymes), a fact that cannot be disputed since there is a considerable increase in the scattered intensity, their size does not increase much most probably due to their initial loose structure that allows for appropriate conformational rearrangements. Of course, at higher FBS content each polyplex binds more proteins/enzymes, resulting in a noticeable increase in both their mass and size. Still, no extended secondary aggregation that could lead to precipitation is observed in any case, or in other words, the resulting mixed particles are essentially stable. To some extent this should be attributed to the presence of the soluble not interacting with PNIPAM grafted chains of the copolymer component. Moreover, they seem to have a rather compact/dense configuration that is mostly unaffected by the increase in temperature and the consequent increase in hydrophobic interactions. Roughly the same narrative stands for the polyplexes of the Chit-
g-PNIPAM+DNA2000 system as well, the main difference in this case being that these polyplexes are already characterized by an initial compact conformation, thus upon binding of the FBS components a significant increase in their mass and size occurs, especially at high FBS content, where the possibility of secondary aggregation is rather likely. Nevertheless, they also exhibit remarkable stability against biological fluids (no precipitation or phase separation observed), even after incubation at body temperature. Surely, the behavior of the polyplexes originates to some degree from the precursor Chit-
g-PNIPAM copolymer, which demonstrates similar properties (see
Supplementary Materials).
3.5. DNA Structure Within the Chit-g-PNIPAM+DNA Polyplexes
Extremely useful and detailed information concerning the conformation of the DNA molecules after their incorporation in the polyplexes can be gained through FTIR spectroscopy, which constitutes an invaluable tool for studying DNA structure [
32,
33,
34,
35,
36,
37,
38]. To this end, FTIR-ATR spectroscopic measurements of the stable polyplexes at N/P = 2 for both Chit-
g-PNIPAM+DNA50/2000 systems were performed by drying a small aliquot of the dispersion directly on the ATR crystal. For comparison reasons the corresponding solutions of the pure Chit-
g-PNIPAM copolymer, along with the two DNA samples, were also measured in a similar manner. By examining the obtained spectra for the polyplexes of the two systems in contrast to the corresponding DNAs, the effect of the interaction with the graft copolymer on the structure of the DNA molecules can be derived.
Figure 7 presents the FTIR-ATR spectra in the characteristic spectral region from 1800 to 900 cm
−1, where the position of the peaks and spectral regions indicating characteristic changes are noted accordingly. Moreover,
Table 2 summarizes the assignment of the discerned peaks, along with the interpretation of the observed changes according to the literature [
32,
33,
34]. It should be noted that the spectral contribution of the Chit-
g-PNIPAM copolymer has been appropriately subtracted from the spectra of the polyplexes.
Upon inspection of the spectra in
Figure 7a, it is rather clear that for the DNA50 sample there are only a few differences observed between the neat molecules and those incorporated into the polyplexes. More specifically, the position of the peak attributed to the asymmetric
stretching (i.e., 1225–1245 cm
−1) is the main marker for distinguishing between the A- and B-form of the DNA helical conformation. Thus, in this case it seems that the neat short DNA chains adopt the A-form, while the ones incorporated into the polyplexes are in the B-form. This difference in conformation is directly correlated to the degree of hydration of the DNA molecule, since fully hydrated chains are in the B-form [
33,
34]. These changes in the hydration degree of the DNA are also evidenced through shifts (like the one seen in
Figure 7a) or intensity variations of the peak located in the 1475–1480 cm
−1 region, which is related to the conformation of the major groove [
32]. Apparently, due to the specific measuring protocol that entails the drying of the liquid sample on the ATR crystal, the neat DNA chains become dehydrated, while the ones incorporated into the polyplexes are protected against dehydration, as a result of the presence of the graft copolymer. In other words, the interaction with the Chit-
g-PNIPAM copolymer protects the innate conformation and hydration of the short DNA chains.
As far as the long DNA sample is concerned, there are even more spectral markers, suggesting that the neat DNA2000 molecule adopts the A-form of the helical structure, i.e., the peaks discerned at 1243, 1176, and 961 cm
−1. The additional spectral characteristics could be attributed to the longer length of the sample that probably enables a more well-defined conformation. On the other hand, the DNA2000 chains within the polyplexes are mainly in the B-form (according to the position of the corresponding peaks), indicating a more hydrated structure, a fact that is also evidenced by the variations in intensity and position of the 1480/1484 cm
−1 band. Furthermore, the differences in intensity of the peaks located at about 1650, 1603, 1531, and 1095 cm
−1 observed in this case suggest some degree of single- to double-strand transition between the neat DNA2000 chains and the ones incorporated into the polyplexes [
32,
33,
34]. One possible explanation for this observation is that as the longer DNA chains are bound to additional conformational constraints, the neat chains are more susceptible to structural changes upon drying. Nevertheless, the interaction of the long DNA with the graft copolymer preserves it not only from dehydration but also from possible structural changes upon drying, thus strengthening its native structure.