Oluwapelumi O.
Kareem
a,
Farzin
Rahmani
b,
Jason A.
Hyman
a,
Christopher B.
Keller
a,
Melissa A.
Pasquinelli
b,
Daniel A.
Savin
c and
Scott M.
Grayson
*a
aDepartment of Chemistry, Percival Stern Hall, Tulane University, New Orleans, Louisiana 70118, USA. E-mail: sgrayson@tulane.edu
bDepartment of Forest Biomaterials, Biltmore Hall, North Carolina State University, Raleigh, North Carolina 27695, USA
cDepartment of Chemistry, Leigh Hall, University of Florida, Gainesville, Florida 32611, USA
First published on 17th December 2020
Dendrimers are globular, multi-functional, monodisperse macromolecules with perfect structure fidelity. Their architecture is composed of a series of branched polymeric arms, composed within “wedges”, that emanate from a central core. Their structure contains a high density of functional groups located at their periphery, referred to as the “outer shell”. Due to their globular structure, it is assumed that the relative “size” of a dendrimer does not fluctuate greatly between solvents. This may be due to the inability of the branched arms, or wedges, to significantly expand or collapse (comparative to analogous linear polymers) owing to steric barriers from branching, especially at higher generations. In contrast, it is expected that a linear polymer, of similar molecular weight to a dendrimer analog, would have a greater degree of size variation dependent on solvent-polymer interactions. This stems from its innate flexibility and greater conformational flexibility. For this investigation, analogous dendritic and linear bis-MPA polyesters as well as poly(caprolactone) (PCL) were analyzed using size-measuring techniques including gel permeation chromatography (GPC) and diffusion ordered spectroscopy-nuclear magnetic resonance (DOSY-1H NMR).
Fig. 1 Drawing of a benzylidene-protected pentaerythritol-core [G3] bis-MPA dendrimer (Tetra[G3]Bnz16). |
In 1983, de Gennes and Hervert used a self-consistent field model to investigate the relationship between generation limit and spacer length.20 This is one of the earliest studies investigating this relationship as dendrimers were only discovered a few years prior in 1978. They found that every dendrimer has a theoretical growth limit where the polymer cannot be quantitatively functionalized at higher generations. This is driven by the increasing density of functional groups at the periphery and the length of the spacer molecules within each arm, assuming a fully extended structure. Generally, the longer the spacer length between branch points (e.g. poly(propylene imine) (PPI) dendrimers (–(CH2)3– spacer) vs. poly(amido amine) PAMAM dendrimers (–(CH2)2C(O)NH(CH2)2– spacer), the slower the peripheral functional density increases with subsequent functionalization, thus allowing for higher achievable generations. This means the generation limit is driven primarily by monomer (spacer) length but does not consider the effect solvent may have on dendrimer generation limit.
As dendrimer generation increases, each of the dendrimer wedges grow closer together as the rate of increasing dendrimer functional density exceeds the rate of increasing dendrimer volume. As such, there are likely several factors that contribute to the overall size of dendrimers, especially in solution. Backfolding of dendrimers was first highlighted by a kinetic growth model by Lescanec and Muthukumar in 1990.21 Their study suggested that the dendrimer terminal functional groups do not strictly populate the periphery of the dendrimer space, at any generation, but rather are distributed throughout the dendrimer volume.21 Further computational work done by Mansfield and Klushin with PAMAM dendrimers also supports this viewpoint.22 Since these early computational studies, there have been numerous experimental investigations into how dendrimers behave in solution, some with differing results.
One of the earliest experimental studies on dendrimer solution size was conducted by Ihre et al. using pulsed field spin echo proton nuclear magnetic resonance (PGSE-1H NMR) looking at acetyl terminated bis-MPA dendrimers.23 They found that the estimated hydrodynamic radii did increase as generation size increased (from [G1] to [G4]) in chloroform (CHCl3), though this was not strictly linear. Lyulin et al. used small-angle neutron scattering (SANS) in their studies of [G5] and [G8] PAMAM dendrimers (–(CH2)2C(O)NH(CH2)2– spacer) to find that the overall solution size of each dendrimer did not change significantly as solvent quality was reduced. This suggests a relatively “rigid” structure where each of the arms must be restricted in its movement, at least for the [G5] and [G8] size range.24 However, when looking at poly(propylene imine) (PPI or DAB) (–(CH2)3– spacer) dendrimers, Chai et al. found using 2-D nuclear Overhauser effect spectroscopy (NOESY) NMR that the arms of a [G3] sample seem to have increased interaction between the terminal groups and interior methylenes in benzene (poor solvent quality) versus increased interaction between the terminal groups and solvent in CHCl3 (good solvent quality).25 This shows that the apparent size of PPI dendrimers may be impacted by the extent of backfolding depending on the solvent quality, despite still being soluble in a poor quality solvent such as benzene.
The extent of backfolding of dendrimers seems to be dependent on the analytical approach used and the dendritic family studied. Individual dendrimer family investigations are necessary to improve application design where dendrimers may be useful. Additionally, studies that include linear or branched analogs as points of comparison can provide context as to the significance of this backfolding. Unfortunately, this type of work has proven difficult since not all dendrimer families have linear equivalents to conduct such a study. Thus far, most experimental studies of dendrimers have been limited by examination in one or two solvents, or by looking solely at the dendrimer and no additional analog. PAMAM dendrimers are one of the most widely used commercially available dendrimers. However, a linear equivalent for these dendrimers does not yet exist for such a comparison. In contrast, poly(benzyl ether) dendrimers have been compared to other polymeric analogs,26–28 including their linear poly(benzyl ether) variant. These dendrimers have shown they can expand and contract quite readily depending on solvent but not to the same degree as their linear variant.26,27
Dendrimers are of interest since, theoretically, their hydrodynamic size variation or conformational flexibility may be more limited than a linear counterpart. They also have increased solubility across a wider range of solvents than linear polymers.29,30 However, as discussed earlier, the conclusions of previous studies are difficult to rely on when generalized for all other dendrimer families. Therefore, it is more appropriate to study each dendritic system, individually. Additional comparison to a linear analog would provide a clearer picture of how they behave. Though bis-MPA dendrimers have seen increased use, they have not had a true linear equivalent until Kareem et al. recently published a benzoyl-protected bis-MPA linear polyester, poly(3-(benzoyloxy)-2-(bromomethyl)-2-methylpropanoic acid) (PBBM).31 Though a linear bis-MPA polycarbonate has existed for some time,32–36 it is not the best linear analog to traditional bis-MPA dendrimers due to the lack of polyester linkages.31 With the advent of PBBM, it should now be possible to investigate the contribution the branched architecture a dendrimer provides to the overall “rigidness” of a bis-MPA dendrimer. With bis-MPA dendrimers already showing their worth as mass calibrants for MALDI-ToF MS2,8,9,12,19 and now having a true linear analog,31 an apparent size investigation on this dendrimer family would be of great importance.
As such, a study exploring solution size variation of bis-MPA dendrimers was performed. PBBM was used as the linear analog due to its similar atom composition and repeat unit mass (OC(O)C(CH3)(CH2OC(O)C6H5)(CH2Br)) (∼220 Da) to the terminal benzylidene-protected bis-MPA groups (C(O)C(CH3)(CH2O)2CHC6H5) (∼205 Da) at the dendrimer periphery. To provide more context to this investigation, linear poly(caprolactone) (PCL) was included as it is a common homopolyester that has a similar atom composition (C(O)(CH2)5O) and repeat unit mass (∼114 Da) to the bis-MPA subunit of bis-MPA dendrimers (C(O)C(CH3)(CH2)2O2) (∼115 Da). These two linear analogs are good comparative points for evaluating the size variation of these dendrimers. Herein, benzylidene-protected pentaerythritol (tetra)-core [G1–G4] dendrimers, PBBM, and PCL are analyzed using an observed mass versus apparent mass comparison via MALDI-ToF MS and GPC, respectively. Furthermore, diffusion ordered spectroscopy-nuclear magnetic resonance (DOSY-1H NMR) is used to measure diffusion coefficient, and subsequently the hydrodynamic (i.e., van der Waals) radii of each polymer in five deuterated solvents of varying solvent quality: tetrahydrofuran (THF-d8), chloroform (CDCl3), acetone (Ace-d6), dimethyl formamide (DMF-d7), and dimethyl sulfoxide (DMSO-d6). Molecular dynamics simulations were also performed to provide insight into the trends observed by DOSY-1H NMR. Though light scattering would be useful for this comparison, the dendrimers in question simply were too small to discern size changes from the inherent error in the measurement.
Fig. 3 Observed m/z by MALDI-ToF MS versus apparent Mn by GPC (calibrated against PS standards) using the Mn values from Table 1. |
Sample | M n | Đ | M n | Đ |
---|---|---|---|---|
a M n and Đ calculated by MALDI-ToF MS using DCTB with Na+ counterion calibrated against SpheriCal® standards. b M n and Đ calculated by GPC analysis calibrated against poly(styrene) (PS) standards. | ||||
Tetra[G1]Bnz4 | 975 | 1.00 | 900 | 1.00 |
Tetra[G2]Bnz8 | 2257 | 1.00 | 1600 | 1.00 |
Tetra[G3]Bnz16 | 4820 | 1.00 | 2900 | 1.01 |
Tetra[G4]Bnz32 | 9941 | 1.00 | 4800 | 1.04 |
1 kDa PBBM | 1200 | 1.03 | 1200 | 1.05 |
2.2 kDa PBBM | 2190 | 1.03 | 1900 | 1.05 |
4.8 kDa PBBM | 4830 | 1.01 | 4000 | 1.02 |
10 kDa PBBM | 10560 | 1.01 | 9400 | 1.04 |
1 kDa PCL | 1150 | 1.01 | 1500 | 1.03 |
2.2 kDa PCL | 2110 | 1.02 | 4400 | 1.08 |
4.8 kDa PCL | 4420 | 1.02 | 10600 | 1.04 |
10 kDa PCL | 10430 | 1.02 | 23400 | 1.12 |
As seen in Table 1 and Fig. 3, despite being of similar molecular weights according to MALDI-ToF MS, bis-MPA dendrimers consistently report lower GPC Mn values in THF than PBBM and PCL. Conceptually, this makes sense since in the case of the [G1–G4] dendrimers, molecular weight is spread out radially rather than linearly. Additionally, the terminal bis-MPA units are protected with benzylidene groups which add significantly to their observed mass (∼115 repeat unit mass vs. terminal unit mass ∼205 Da). PBBM contains a pendant benzoyl group that also adds significant mass to each repeat unit (repeat unit mass ∼220 Da). As a result, Tetra[G4]Bnz32 contains 60 bis-MPA units and an equivalent PBBM chain contains ∼45 bis-MPA units. Removal of these heavy protecting groups results in a molecular weight reduction for the dendrimer of 29% and 48% for PBBM. In contrast, though the PCL unit has a similar atom composition to the bis-MPA repeat unit, it lacks a heavy protecting group. Therefore, at the 10 kDa molecular weight range, PCL contains 87 repeat units compared to the 60 of the [G4] dendrimer. To provide a clearer example, in Fig. 2, Tetra[G2]Bnz8 is drawn along with the nearest molecular weight analog for PCL and PBBM. As shown in Fig. 2, the dendrimer contains twelve bis-MPA units while PBBM and PCL contain ten and twenty repeat units, respectively. These differences increase when looking at higher molecular weights and will be discussed later in this study.
Despite the [G1] dendrimer containing a “core” molecule, it still appears to be very similar in apparent mass to PBBM in THF. This similarity seems to continue even up to 2 kDa when following the trendline fits. Since both contain the same number of bis-MPA units up to this range, the observed overlap is not surprising. 1 kDa PCL also seems to be only marginally larger than the [G1] dendrimer despite having approximately double the number of repeat units. Thus far, it appears that at the 1 kDa range, there is not much difference in the apparent size of these analogs.
However, at the 10 kDa range significant differences can be observed. Despite containing fewer bis-MPA units in this 10 kDa mass range, linear PBBM still has a higher apparent mass by GPC in THF. 10 kDa PCL contains approximately 87 repeat units. Though this is ∼1.5 times as many repeat units as the [G4] dendrimer, this results in an almost five-fold higher apparent mass. At this mass range, linear polymers can appear much larger than dendrimers by GPC even if they have similar molecular weights by MALDI-ToF MS.
To reach the same apparent mass of linear polymers, dendrimers of much higher molecular weights would need to be used. However, this is not feasible, since traditional dendrimers all have a growth limit, as discussed earlier. In this example, the tetra-core bis-MPA dendrimers appear to have a generation limit of [G5]. The differences in apparent mass shown in this preliminary size comparison suggests apparent size variation will be greater for the linear analogs, though more data outside of THF would be needed to confirm this.
DOSY-1H NMR measures the decay of 1H signal intensity with decreasing gradient strength. This decay was used to calculate a self-diffusion constant (D) using ESI eqn (1)† for each sample. DOSY-1H NMR spectra of each sample in each solvent are shown in Fig. S11–69.† The calculated D values were then used in the Stokes–Einstein equation (ESI eqn (2)†) to calculate the corresponding hydrodynamic radius (Rh). Though these calculations assume an ideal spherical shape for each sample and are not a direct measurement of molecular size, they should still be able to yield good insight into how each polymer is behaving in each solvent. As solvent quality changes for each molecular weight and sample, compounds that are less “rigid” should see greater size variation.
Table 2 shows the calculated D and Rh of each sample in the respective solvent. Additionally, average Rh across all five solvents and calculated variation values are shown in Fig. 4. The variation value was calculated by taking the average of Rh across all five solvents for each sample and molecular weight range and then calculating a variation value of each experiment from this average. These variation values were then averaged to attain the average size variation.
Fig. 4 Average Rh and size variation of each polymer across all tested molecular weight ranges using data from DOSY-1H NMR. |
Sample | Solvent | Avg Db (m2 s−1) | R h (nm) | Sample | Solvent | Avg Db (m2 s−1) | R h (nm) | Sample | Solvent | Avg Db (m2 S−1) | R h (nm) |
---|---|---|---|---|---|---|---|---|---|---|---|
a Each sample was analyzed in duplicate using DOSY-1H NMR at 5 mg ml−1 at 298 K in all five solvents. b Within each DOSY-1H NMR spectrum, D for four separate peaks were calculated using eqn (1). This was done for each of the duplicate spectra. All eight of these calculated D values were then averaged to give the D values shown in the above table. Peaks used for this analysis are shown in Fig. S71–S73.† c R h value was calculated from the average D from two separate runs of each sample using ESI eqn (2).† d 10 kDa PCL was not sufficiently soluble in DMSO at 298 K to complete the experiment. | |||||||||||
Tetra[G1]Bnz4 | THF | 8.44 × 10−10 | 0.54 ± 0.03 | 1 kDa PBBM | THF | 7.53 × 10−10 | 0.60 ± 0.00 | 1 kDa PCL | THF | 4.45 × 10−10 | 1.02 ± 0.04 |
CHCl3 | 6.95 × 10−10 | 0.59 ± 0.08 | CHCl3 | 7.20 × 10−10 | 0.56 ± 0.00 | CHCl3 | 5.31 × 10−10 | 0.76 ± 0.06 | |||
Ace | 1.17 × 10−09 | 0.59 ± 0.05 | Ace | 1.13 × 10−09 | 0.61 ± 0.01 | Ace | 9.49 × 10−10 | 0.74 ± 0.10 | |||
DMF | 4.80 × 10−10 | 0.57 ± 0.02 | DMF | 4.12 × 10−10 | 0.67 ± 0.01 | DMF | 2.93 × 10−10 | 0.94 ± 0.01 | |||
DMSO | 1.65 × 10−10 | 0.67 ± 0.03 | DMSO | 1.84 × 10−10 | 0.60 ± 0.02 | DMSO | 1.15 × 10−10 | 0.96 ± 0.03 | |||
Tetra[G2]Bnz8 | THF | 5.39 × 10−10 | 0.84 ± 0.02 | 2.2 kDa PBBM | THF | 5.36 × 10−10 | 0.85 ± 0.03 | 2.2 kDa PCL | THF | 3.92 × 10−10 | 1.16 ± 0.06 |
CHCl3 | 5.07 × 10−10 | 0.80 ± 0.07 | CHCl3 | 5.51 × 10−10 | 0.73 ± 0.01 | CHCl3 | 2.67 × 10−10 | 1.51 ± 0.02 | |||
Ace | 8.46 × 10−10 | 0.82 ± 0.02 | Ace | 8.99 × 10−10 | 0.77 ± 0.08 | Ace | 5.55 × 10−10 | 1.25 ± 0.02 | |||
DMF | 3.22 × 10−10 | 0.85 ± 0.02 | DMF | 3.12 × 10−10 | 0.88 ± 0.01 | DMF | 2.30 × 10−10 | 1.19 ± 0.00 | |||
DMSO | 1.20 × 10−10 | 0.92 ± 0.04 | DMSO | 1.21 × 10−10 | 0.91 ± 0.03 | DMSO | 8.40 × 10−11 | 1.31 ± 0.05 | |||
Tetra[G3]Bnz16 | THF | 3.91 × 10−10 | 1.17 ± 0.10 | 4.8 kDa PBBM | THF | 2.98 × 10−10 | 1.53 ± 0.01 | 4.8 kDa PCL | THF | 2.68 × 10−10 | 1.70 ± 0.06 |
CHCl3 | 3.61 × 10−10 | 1.12 ± 0.04 | CHCl3 | 3.06 × 10−10 | 1.32 ± 0.10 | CHCl3 | 2.12 × 10−10 | 1.90 ± 0.05 | |||
Ace | 6.34 × 10−10 | 1.09 ± 0.03 | Ace | 5.56 × 10−10 | 1.24 ± 0.01 | Ace | 4.06 × 10−10 | 1.71 ± 0.03 | |||
DMF | 2.76 × 10−10 | 1.00 ± 0.10 | DMF | 1.96 × 10−10 | 1.40 ± 0.07 | DMF | 1.57 × 10−10 | 1.75 ± 0.05 | |||
DMSO | 9.21 × 10−11 | 1.20 ± 0.02 | DMSO | 8.05 × 10−11 | 1.37 ± 0.10 | DMSO | 8.85 × 10−11 | 1.25 ± 0.06 | |||
Tetra[G4]Bnz32 | THF | 3.37 × 10−10 | 1.35 ± 0.01 | 10 kDa PBBM | THF | 2.51 × 10−10 | 1.81 ± 0.08 | 10 kDa PCL | THF | 1.75 × 10−10 | 2.60 ± 0.06 |
CHCl3 | 2.94 × 10−10 | 1.37 ± 0.09 | CHCl3 | 2.55 × 10−10 | 1.58 ± 0.03 | CHCl3 | 1.55 × 10−10 | 2.61 ± 0.11 | |||
Ace | 5.44 × 10−10 | 1.28 ± 0.09 | Ace | 3.73 × 10−10 | 1.86 ± 0.08 | Ace | 2.70 × 10−10 | 2.56 ± 0.08 | |||
DMF | 2.65 × 10−10 | 1.39 ± 0.06 | DMF | 1.47 × 10−10 | 1.87 ± 0.01 | DMF | 1.12 × 10−10 | 2.46 ± 0.04 | |||
DMSO | 1.98 × 10−10 | 1.40 ± 0.09 | DMSO | 5.67 × 10−11 | 1.95 ± 0.05 | DMSOd | — | — |
Fig. 5 Calculated average Rh values, from DOSY-1H NMR, for Tetra[G1]Bnz4, 1 kDa PCL, and 1 kDa PBBM in all tested solvents. aSolvent polarity values from Reichardt were used to determine order of polarity.39 |
When comparing the variation values of the [G1] dendrimer and equivalent PBBM (Fig. 4), it appears that the dendrimer may exhibit slightly more size variation (0.07 Å more). However, this difference is miniscule (less than the length of a carbon–carbon bond) and when looking at Rh calculations they are quite similar (Fig. 4 and 5). This minimal difference between the [G1] dendrimer and 1 kDa PBBM suggests they have similar conformational flexibility. The size variability of 1 kDa PCL on the other hand is much higher than the other analogs (∼4.5 times more than PBBM and ∼3.5 times more than Tetra[G1]Bnz4) (Fig. 4). This may be due to the 1 kDa PCL containing 10 repeat units compared to four bis-MPA units of the [G1] dendrimer and four bis-MPA units of 1 kDa PBBM, thus being larger. The differences here are now at the angstrom scale and may be due to a lack of stabilizing intramolecular interactions of PCL compared to the benzyl rings in PBBM and the dendrimer. Though all three analogs appeared to be similar in our GPC comparison at 1 kDa, differences already exist when looking at multiple solvents though some of these differences are on the sub-Angstrom scale.
Fig. 6 Calculated average Rh values, from DOSY-1H NMR, for Tetra[G2]Bnz8, 2.2 kDa PCL, and 2.2 kDa PBBM in all tested solvents. aSolvent polarity values from Reichardt were used to determine order of polarity.39 |
Sample | Avg Rha (nm) | Size fluctuation valueb (Å) |
---|---|---|
a Each of the calculated Rh values from each DOSY-1H NMR spectrum was used to calculate the average Rh of each sample across all five tested solvents. b Size variation was calculated by taking the average Rh values and calculating the deviation of each Rh value, in each respective solvent, from the average Rh in all five solvents. These deviations were then averaged to give a size variation value. | ||
Tetra[G1]Bnz4 | 0.59 ± (0.05) | 0.32 |
Tetra[G2]Bnz8 | 0.87 ± (0.05) | 0.32 |
Tetra[G3]Bnz16 | 1.13 ± (0.05) | 0.42 |
Tetra[G4]Bnz32 | 1.36 ± (0.05) | 0.37 |
1 kDa PBBM | 0.61 ± (0.04) | 0.25 |
2.2 kDa PBBM | 0.83 ± (0.07) | 0.61 |
4.8 kDa PBBM | 1.37 ± (0.11) | 0.73 |
10 kDa PBBM | 1.78 ± (0.14) | 1.14 |
1 kDa PCL | 0.87 ± (0.13) | 1.11 |
2.2 kDa PCL | 1.29 ± (0.14) | 1.01 |
4.8 kDa PCL | 1.74 ± (0.10) | 0.69 |
10 kDa PCL | 2.56 ± (0.07) | 0.48 |
In the GPC analysis (Fig. 3), 2.2 kDa PCL appears to be significantly larger than the [G2] dendrimer and 2.2 kDa PBBM. This remains consistent in the DOSY-1H NMR data as it is ∼51% larger (4.3 Å larger), on average, than the [G2] dendrimer (Fig. 4). Its variation value is also 1.0 Å which is ∼3 times higher than the [G2]. This is likely due to 2.2 kDa PCL containing ∼20 repeat units. As can be seen in Fig. 6, the apparent size of 2.2 kDa PCL is significantly larger than the other two analogs: a trend that will continue for the rest of this study.
Fig. 7 Calculated average Rh values, from DOSY-1H NMR, for Tetra[G3]Bnz16, 4.8 kDa PCL, and 4.8 kDa PBBM in all tested solvents. aSolvent polarity values from Reichardt were used to determine order of polarity.39 |
4.8 kDa PCL not only has a larger average Rh (6.1 Å larger) than the [G3] dendrimer, its variation value is also ∼64% higher (higher by 0.28 Å) (Fig. 4). Interestingly, despite being the largest analog thus far, its size variability appears to be lower than it was at both the 1 kDa and 2.2 kDa range. This was unexpected since at this mass range, PCL contains ∼42 repeat units which is 1.5 times the number of repeat units for the [G3] dendrimer despite having similar molecular weights (Table 1). Thus, a higher size variability was expected. However, this may be explained by the introduction of local constraints due to intramolecular chain entanglements or interactions. It should be noted that this trend is in opposition of the PBBM analog. As molecular weight is increasing the PBBM analogs have a growing level of size variability whereas the PCL is becoming more size stable. This trend continues into the 10 kDa range which may suggest a more sphere-like structure than random coil. Despite both materials being linear homopolyesters, their trends in size variability do not mirror each other meaning there are more size influencing factors involved other than just linear vs. branched architecture.
Fig. 8 Calculated average Rh values, from DOSY-1H NMR, for Tetra[G4]Bnz32, 10 kDa PCL, and 10 kDa PBBM in all tested solvents. aSolvent polarity values from Reichardt were used to determine order of polarity.39 |
Following the same trend from the 2.2 kDa range, 10 kDa PCL has the largest average Rh value across these tested solvents. Its average Rh is 7.8 Å higher than the equivalent PBBM and 12 Å higher than the equivalent [G4] (Fig. 8). Though the 10 kDa PCL is 8.2 Å larger than the 4.8 kDa PCL, another drop in size variability is observed: a reduction of ∼69% (0.2 Å reduction) following the trend starting from the 2.2 kDa range. This again supports the notion of the PCL adopting a more “globular” structure. 10 kDa PCL may not be as size stable as the [G4] dendrimer but its variation value is only 0.1 Å higher. This is much lower than was expected, especially considering that 10 kDa PCL contains ∼27 more repeat units than the [G4] dendrimer.
Fig. 9 Average Rh and variation values for apparent 5 kDa Tetra[G4]Bnz32, 4.8 kDa PBBM, and 2.2 kDa PCL. |
The similarities observed in THF also carry over when looking at the other solvents using DOSY-1H NMR. Despite having ∼39 more bis-MPA units than 4.8 kDa PBBM and ∼40 more repeat units than 2.2 kDa PCL, the [G4] has a similar Rh value to these analogs. Though they are of similar sizes, the fluctuation behavior between these analogs is different. The [G4] dendrimer has a variation value (0.37 Å) that is ∼97% (0.36 Å) less than the 4.8 kDa PBBM (0.73 Å) and ∼172% (0.64 Å) less than the 2.2 kDa PCL (1.01 Å). This supports the notion of dendrimers being globular molecules that have limited size variability compared to linear polymers. However, when comparing the [G4] to its PCL apparent mass analog, 2.2 kDa PCL, the difference is substantially more significant. The observed MALDI mass comparison reveals that PCL must reach a GPC Mn that is ∼five times that of an equivalent bis-MPA dendrimer to exhibit a similar level of size stability. Therefore, the bis-MPA dendrimers are indeed more size stable than both linear analogs when comparing both observed mass and apparent mass, as hypothesized.
As explained in the computational details section in the ESI,† a series of MD simulations were performed on the 10 kDa analogs to determine their Hansen Solubility Parameters (HSPs). In Table 4, the value of HSP component are shown for the Tetra[G4]Bnz32, 45-mer PBBM, and 87-mer PCL. As seen in this table, the value of the van der Waals and electrostatic components for PCL are 17.31 MPa0.5 and 10.32 MPa0.5, respectively, which closely match the values shown in literature.40 While these results reveal that the δvdW values for all three analogs are similar, the δele values for PBBM and [G4] are significantly higher than the PCL. Therefore, the PBBM and [G4] tend to exhibit greater solvent-polymer interaction in more polar solvents such as DMSO and DMF which is shown in higher Rh values in Table 5.
10 kDa analog | Total | δ vdW(MPa0.5) | δ ele(MPa0.5) |
---|---|---|---|
Tetra[G4]Bnz32 | 25.35 | 18.22 | 17.63 |
45-mer PBBM | 25.51 | 17.86 | 18.22 |
87-mer PCL | 20.10 | 17.31 | 10.22 |
Tetra[G4]Bnz32 | 45-mer PBBM | 87-mer PCL | ||||||
---|---|---|---|---|---|---|---|---|
Solventa | R a(A–B) | R h (nm) | Solventa | R a(A–B) | R h (nm) | Solventa | R a(A–B) | R h (nm) |
a The solvent column for each analog is ordered by increasing Ra(A–B) from top to bottom. b R a(A–B) was determined using MD calculations for each analog and literature values for each solvent. Ra(A–B) was also determined using experimental values for each solvent and that data can be seen in Table S2.† | ||||||||
DMF | 1.65 | 1.39 | DMF | 1.03 | 1.87 | THF | 1.09 | 2.60 |
DMSO | 1.72 | 1.40 | DMSO | 1.54 | 1.95 | CHCl3 | 3.86 | 2.61 |
Ace | 7.45 | 1.28 | Ace | 7.39 | 1.86 | Ace | 4.30 | 2.56 |
THF | 8.31 | 1.35 | THF | 8.66 | 1.81 | DMF | 7.54 | 2.46 |
CHCl3 | 11.17 | 1.37 | CHCl3 | 11.73 | 1.58 | DMSO | 9.35 | N/A |
In order to determine solvent quality for each analog, the solubility parameter distance (Ra(A–B)) was determined using eqn (1).
Solubility parameter distance (Ra(A–B) equation:40
(1) |
The solubility parameter distance represents the HSP distance from each analog to each solvent. As a result, a smaller Ra(A–B) value means the HSPs are closer and therefore they should have better compatibility. In Table 5, the calculated Ra(A–B) values are given for all solvent-analog combinations. According to the molecular dynamics’ calculations in Table 4, DMF and DMSO are the best solvents for the [G4] dendrimer. This agrees with the DOSY-1H NMR data as those solvents showed the highest average Rh values. Much like the dendrimer, DMF and DMSO appear to be the best solvents for PBBM. This is mirrored in the Rh values and shows very good agreement between Ra(A–B) and the diffusion experiments. Additionally, the Ra(A–B) trends for the dendrimer and PBBM are the same further supporting that PBBM is a good linear analog for these bis-MPA dendrimers. For PCL, good agreement between the Ra(A–B) and Rh trends are observed. However, though it is also a homopolyester, DMF and DMSO do not appear to be good solvents for PCL. Interestingly, the Ra(A–B) trends for PCL are almost opposite to that of PBBM and the dendrimer. This may point to the reason why the size variation trend for PCL was so different from PBBM and the dendrimers. Though some differences in some of the previous comparisons were minimal, the close agreement of Ra(A–B) and Rh trends support many of the aforementioned claims.
According to this data, bis-MPA dendrimers do exhibit more solution size stability than their direct linear analog, PBBM, and potentially other linear polymers such as PCL given the same apparent mass or nominal mass. Despite all tested analogs being polyesters, there is greater similarity between the bis-MPA dendrimers and PBBM and less so between those and PCL. As shown in the MALDI vs. GPC comparison, the branch complexity of the bis-MPA dendrimers leads to a more size stable structure compared to PBBM. Though these differences exist on the Å scale, it is important to note that Å scale differences on Rh value can have a significant impact on the overall size and shape of a molecule. Additionally, the data here supports the idea of using dendrimers as small apparent mass calibrants for techniques like GPC from 0 up to at least 5 kDa. Though dendrimers cannot practically reach the same apparent size as, and will not replace, linear calibrants (100 kDa to 1 MDa), they do have added benefits such as increased solubility in a wider range of solvents than linear polymers. This means that dendrimers may prove to be good calibrants for apparent size measuring techniques especially when looking at non-linear architectures or switching between solvents. From the results of this study, the branch architecture of the dendrimers has a measurable effect on the size stability of dendrimers when compared to their linear analog.
Footnote |
† Electronic supplementary information (ESI) available: Experimental materials, methods, and characterization data of bis-MPA dendrimers, PBBM, and PCL. See DOI: 10.1039/d0py01070g |
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