Open Access Article
Carlos E.
Gutierrez-Ulloa
ad,
Marina Yu.
Buyanova
b,
Evgeny K.
Apartsin
*b,
Alya G.
Venyaminova
b,
F. Javier
de la Mata
ad,
Mercedes
Valiente
*c and
Rafael
Gómez
*ad
aDepartamento de Química Inorgánica, Universidad de Alcalá, Campus Universitario, Alcalá de Henares, Madrid, Spain. E-mail: rafael.gomez@uah.es; Tel: (+34) 91 8854685
bInstitute of Chemical Biology and Fundamental Medicine SB RAS, Novosibirsk, Russia. E-mail: eka@niboch.nsc.ru; Tel: (+7) 383 3635129
cDepartamento de Química Analítica, Química Física e Ingeniería Química, Universidad de Alcalá, Campus Universitario, Alcalá de Henares, Madrid, Spain. E-mail: mercedes.valiente@uah.es; Tel: (+34) 91 8854670
dNetworking Research Center on Bioengineering, Biomaterials and Nanomedicine (CIBER-BBN), Madrid, Spain
First published on 22nd August 2017
A novel family of amphiphilic ionic carbosilane dendrons containing fatty acids at the focal point were synthesized and characterized. They spontaneously self-assembled in aqueous solution into micelles both in the absence and presence of salt, as confirmed by surface tension, conductivity, and DLS measurements. Dendron based micelles have spherical shapes and increase in size on decreasing dendron generation. These dendritic micelles have been demonstrated to be able to form complexes with therapeutic macromolecules such as siRNA and show a high loading capacity for drugs such as procaine, suggesting their potential use as nanocarriers for therapeutics.
A different dendritic typology is that based on the carbosilane structure which is hydrophobic, constituting interesting building blocks to be developed from a biomedical point of view.18,19 Silicon strongly increases the lipophilicity of the systems and facilitates their membrane crossing and bioavailability.20 Kim et al. reported on the behavior of amphiphilic linear block copolymers based on PEG and allyl-terminated carbosilane dendrons.21 For them, the formation of micellar aggregates highly depended on the size of the hydrophobic part (i.e. dendron generation). In the last few years, our research groups have been interested in the synthesis and biomedical applications of the dendritic carbosilane molecules. Cationic carbosilane dendrimers have been used as antibacterial22,23 and antiparasite24 agents and as carriers for short nucleic acids like siRNA or antisense oligonucleotides for transfection purposes.25,26 In the case of anionic dendrimers, these were applied as antiviral agents mainly for HIV infection.27,28 Recently, we also reported a synthetic platform of carbosilane dendrons29,30 able to dendronize nanostructured materials such as poly(D,L-lactide-co-glycolide) acid,31 mesoporous silica32 or gold33 NPs, as well as decorating their focal point with molecules of interest like ferrocene,34 DO3A (1,4,7,10-tetraazacyclodocecane-N,N′,N′′,N′′′-triacetic acid) chelator35 or drugs,36 among others.
In this study, we report on the synthesis of new amphiphilic systems formed from ionic-terminated carbosilane dendrons containing a hydrophobic tail at the focal point with two different lengths. In this particular case, the total hydrophobic contribution will be the result of the addition of both the tail and the dendritic structure, leaving only the terminal ionic groups of the dendrons as a major part for hydrophilicity. This situation gives rise to a different scenario within the dendritic amphiphile engineering towards the formation of new supramolecular assemblies for biomedical applications.
For the synthesis of ionic carbosilane dendrons, thiol–ene reactions were used. In the case of formation of sulfonate-terminated dendrons, allyl-terminated dendrons (BrGnAm) were employed as the starting materials for the reaction with the thiol derivatives containing sulfonate groups. However, in the case of ammonium-terminated dendrons, more reactive vinyl-terminated dendrons (BrGnVm) were necessary in order to proceed with the corresponding thiol derivative. In addition, two different fatty acids such as hexanoic (caproic) and hexadecanoic (palmitic) acids were used to study the implications of the chain length in the self-assembly processes. The coupling reaction of fatty acids with the carbosilane dendrons to replace the bromine atom by this new aliphatic chain was performed by ester bond formation. This procedure afforded new families of dendrons, with palmitic acid, C16GnAm (n = 1, m = 2 (1); n = 2, m = 4 (2); n = 3, m = 8 (3)) and C16GnVm (n = 1, m = 2 (4); n = 2, m = 4 (5); n = 3, m = 8 (6)), and with hexanoic acid, C6GnAm (n = 1, m = 2 (7); n = 2, m = 4 (8); n = 3, m = 8 (9)) and C6GnVm (n = 1, m = 2 (10); n = 2, m = 4 (11); n = 3, m = 8 (12)), all of them obtained as yellow oils in high yields (see Scheme 1).
Once allyl-terminated dendrons with adequate focal points were obtained, modification of their periphery via thiol–ene addition was accomplished. Thus, solutions of dendrons of the type C16GnAm (1–3) and C6GnAm (7–9) and sodium 3-mercapto-1-propanesulfonate in THF/MeOH/H2O were stirred for 1 h under UV light to afford the new dendritic wedges C16Gn(SO3Na)m (n = 1, m = 2 (13); n = 2, m = 4 (14); n = 3, m = 8 (15)) and C6Gn(SO3Na)m (n = 1, m = 2 (16); n = 2, m = 4 (17); n = 3, m = 8 (18)) (Scheme 2). All compounds were obtained as white solids in high yields.
Analogously, solutions of dendrons C16GnVm (4–6) or C6GnVm (10–12) and 2-dimethylethylenethiol hydrochloride, HS(CH2)2NMe2·HCl, in THF/MeOH were stirred under UV irradiation to afford the dendrons C16Gn(NMe2HCl)m (n = 1, m = 2 (19); n = 2, m = 4 (20); n = 3, m = 8 (21)), and C6Gn(NMe2HCl)m (n = 1, m = 2 (22); n = 2, m = 4 (23); n = 3, m = 8 (24)) as white solids in high yields (Scheme 3). These systems were neutralized with Na2CO3 to give the amine-terminated dendrons C16Gn(NMe2)m (n = 1, m = 2 (25); n = 2, m = 4 (26); n = 3, m = 8 (27)) and C6Gn(NMe2)m (n = 1, m = 2 (28); n = 2, m = 4 (29); n = 3, m = 8 (30)). After that, the latter systems were quaternized with MeI to obtain the dendritic wedges C16Gn(NMe3+I)m (n = 1, m = 2 (31); n = 2, m = 4 (32); n = 3, m = 8 (33)), and C6Gn(NMe3+I)m (n = 1, m = 2 (34); n = 2, m = 4 (35); n = 3, m = 8 (36)) (see Scheme 3). For all these reactions, the presence of 2,2′-dimethoxy-2-phenylacetophenone (DMPA) as a photoinitiator was necessary. The addition of the thiol to the allyl or vinyl groups was regioselective at the β-position (vide infra). All the anionic dendrons 13–18 and the cationic ones 19–24 and 31–36 were soluble in water.
NMR spectroscopy confirmed the modification at the focal point from the –CH2Br group that showed one triplet at δ 3.40 in the 1H NMR spectra and one signal at δ 33.0 in the 13C NMR, to the new –CH2O– group that presented one triplet at δ 4.04 in the 1H NMR spectra and one signal at δ 63.8 in the 13C NMR (see the ESI† for spectra). One more signal at δ 173.9 in the 13C NMR corroborated the formation of the ester bond with respect to the –COOH group of the free fatty acids which appeared at δ 180.3. NMR spectroscopy, mass spectrometry (MS) and analytical data of all derivatives were consistent with their proposed structures. The presence of the new chain –Si(CH2)3S– in the anionic systems was confirmed by the presence of three multiplets at δ 0.53, 1.47 and 2.44 in the 1H NMR spectra. The outer chain –S(CH2)3SO3Na was observed as two multiplets at δ 2.52 and 2.85 for the protons of the –SCH2– and the –CH2SO3Na groups, respectively, and a multiplet at δ 1.89 for the inner methylene group of the chain (see Fig. S.4.3†). The –CH2– carbon atoms of the chain –Si(CH2)3S– were detected in the 13C NMR spectra at δ 12.8 for the –SiCH2– group, 23.9 for the middle –CH2– group, and δ 35.2 for the –CH2S– group. Those carbon atoms belonging to the chain –S(CH2)3SO3Na appeared at δ 30.3 for the –SCH2– group and δ 50.1 for the –CH2SO3Na group while the methylene group at the β position with respect to both S atoms was shown at δ 24.5 (see Fig. S.4.3 and S.4.4†). For the cationic compounds, the presence of the chain –Si(CH2)2S– was confirmed by 1H NMR, which showed two multiplets at δ 0.94 and 2.74, whereas the outer chain –S(CH2)2N– gave rise to two multiplets at δ 3.00 and 3.60 for the protons of the –SCH2– and –CH2N–, respectively. Furthermore, a singlet at δ 3.20 confirmed the presence of –NMe3+ (see Fig. S.4.9†). The carbon atoms of the –Si(CH2)2S– chain were observed in the 13C NMR spectra at δ 13.0 for the –SiCH2– group and at δ 29.4 for the –CH2S– group, whereas those belonging to the –S(CH2)2N– chain arose at δ 23.3 for the –SCH2– and δ 65.1 for the –CH2N– group. The –NMe3+ group was also detected at δ 53.6 by 13C NMR spectroscopy.
The structures of the new families of cationic and anionic carbosilane dendrons with fatty acids at the focal point are depicted in Fig. 2 and 3. To represent more clearly the structure–property relationship of these systems, the following notation was also used: CmGn+ or CmGn−, where Cm denotes the number of carbon atom of the aliphatic chain, Gn stands for the dendritic generation and + and − indicate the nature of the peripheral groups.
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| Fig. 2 Representative structures of anionic dendrons with palmitic or hexanoic acid at the focal points 13–18. | ||
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| Fig. 3 Representative structures of cationic dendrons with palmitic or hexanoic acid at the focal points 31–36. | ||
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| Fig. 4 Conductivity measurements of selected dendrons containing palmitic acid (13–15 (A) and 31–33 (B)) and hexanoic acid (36 and 18) (C) at the focal point. | ||
Both cationic and anionic systems of all generations containing palmitic acid at the focal point were able to form micelles with a CMC of around 240–110 μM. There were not big differences between the CMC of cationic and anionic amphiphiles with the same hydrophobic part (Table 1), indicating that the nature of the charged groups on the periphery appeared not to affect drastically the CMC values. However, among the ones bearing hexanoic acid at the focal point, only the third generation dendrons formed micelles. It should be noted that as a rule for amphiphilic dendrons, the amphiphilicity arises from the difference in hydrophilicity between the functional dendritic scaffold and the dendron tail. In this kind of dendron, the head groups are composed both for hydrophobic and hydrophilic parts. In amphiphilic carbosilane dendrons from the first to the third generation, the hydrophilicity increases due to the presence of a greater number of charged groups, but the lipophilicity also increases on increasing the carbosilane scaffold. Therefore, the behavior of the amphiphilic carbosilane dendrons in water medium is defined by the hydrophilic–lipophilic balance. In particular, the peculiarities of such balance in the dendrons C6G3 allow them to form micelles in water despite the short hydrophobic tail in the focal point.
| Dendron | CMC (μM) | Ionization degree (α) | Gibbs energy of micellization (kJ mol−1) | |||
|---|---|---|---|---|---|---|
| CmGn− | CmGn+ | CmGn− | CmGn+ | CmGn− | CmGn+ | |
| C16G1 | 240 ± 26 | 120 ± 10 | 0.69 ± 0.02 | 0.37 ± 0.02 | −41 | −65 |
| C16G2 | 140 ± 8 | 110 ± 10 | 0.78 ± 0.01 | 0.20 ± 0.02 | −127 | −130 |
| C16G3 | 140 ± 10 | 190 ± 6 | 0.79 ± 0.01 | 0.49 ± 0.01 | −255 | −250 |
| C6G3 | 200 ± 20 | 120 ± 20 | 0.53 ± 0.02 | 0.33 ± 0.01 | −202 | −258 |
The ionization degrees (α) of the micelles obtained from the ratio of slopes method of specific conductivity measurements along with the Gibbs energy estimation of micelle formation for the pseudo-phase separation model as ΔmicG° ≈ iRT
ln
XCMC are presented in Table 1. Anionic micelles of palmitic dendrons were highly ionized in water media (α = 0.7–0.8). In contrast, the ionization degrees were considerably lower (α = 0.2–0.5) for analogous cationic micelles indicating that these cationic dendrons assembled into micelles with smaller charge density than the homologous micelles consisting of anionic dendrons. The smaller values for cationic micelles could be related to the nature of counterion. The counterions used in these cases were I− for cationic micelles and Na+ for anionic micelles. Larger ions (I−) are more polarizable tending to be less hydrated, and subsequently binding more effectively on the micellar surface. In addition, the values of micellization Gibbs energy were negative indicating spontaneous micelle formation and more favorable on increasing the dendron generation.
The strong electrostatic repulsion between head groups in both types of micelles can be reduced by increasing the ionic strength. One of the factors known to affect the CMC in aqueous solution is the presence of added electrolyte. It is a general rule that the addition of salt decreases the CMC and increases the micelle aggregation number in ionic micelles.38,39 In solutions of increasing ionic strength, the forces of electrostatic repulsion between the head groups in a micelle are considerably reduced, enabling micelles to form more easily, that is, at lower concentration. The electrostatic screening effect decreases the ionic head group repulsion to assist self-assembly formation with increasing aggregation number of micelles. Electrical conductivity measurements were not sensitive enough to evaluate CMC in the presence of salt; therefore surface tension curves of the dendrons with and without salts were generated. The ionic strength effect on the CMC and adsorption properties at the air/water interface are depicted in Fig. 5 and 6. NaCl addition facilitated the formation of micelle-like structures as was observed by decreasing the corresponding CMC values (see Table 2).
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| Fig. 6 Surface tension measurements of selected dendrons containing palmitic acid (13–15 (B) and 31–33 (C)) and hexanoic acid (17–18 (A)) at the focal point at a fixed salt concentration of 20 mM. | ||
| Dendron | CMC (μM) | 106Γ (mol m−2) | σ CMC (mN m−1) | A (nm2 per molecule) |
|---|---|---|---|---|
| a Salt concentration equal to 2 mM. | ||||
| Anionic dendrons (CmGn−) | ||||
| C16G1− (13)a | 50 ± 10 | 0.77 | 40 | 2.1 |
| C16G1− (13) | 6 ± 1 | 2.7 | 39 | 0.61 |
| C16G2− (14) | 6 ± 1 | 2.2 | 50 | 0.75 |
| C16G3− (15) | 8 ± 1 | 1.7 | 49 | 0.98 |
| C6G2− (17) | 50 ± 5 | 1.5 | 43 | 1.1 |
| C6G3− (18) | 1.5 ± 0.2 | 0.68 | 50 | 2.4 |
| Cationic dendrons (CmGn+) | ||||
| C16G1+ (31) | 25 ± 1 | 1.0 | 39 | 1.7 |
| C16G2+ (32) | 19 ± 1 | 0.77 | 45 | 2.1 |
| C16G3+ (33) | 17 ± 1 | 0.69 | 51 | 2.4 |
| C6G3+ (36) | 12 ± 1 | 0.83 | 50 | 2.0 |
Based on the surface tension data, the geometrical parameters of the dendron packaging in micelles were estimated. The required area per head group, A, at the interface can be calculated using the Gibbs equation
log
c can be obtained from the slope of the plot surface tension versus the logarithm of the concentration at concentrations below the CMC. The reciprocal of Γ gives the area of surface occupied by a mole of adsorbed molecules. The values of CMC, Γ, A, and the surface tension at CMC (σCMC) for micelles formed from anionic and cationic dendrons are listed in Table 2.
With respect to anionic micelles, the CMC for C16G1− (13) changed from 240 μM without salt to 50 μM with 2 mM of salt, and 6 μM with 20 mM of salt. Salt concentrations above 20 mM almost did not affect the CMC value, suggesting that the results obtained are applicable under physiological conditions. It seems that this amount of salt was high enough to reduce the electrostatic repulsions between the head groups. In this case, the CMC showed very poor sensitivity to the generation of palmitic dendrons. For hexanoic dendrons, the presence of salt permitted the formation of micelles even for the second generation above 50 μM, while the third generation formed micelles at a lower CMC value than those for palmitic dendrons. With respect to cationic micelles, the salt effect produced a decrease in CMC as well, ranging from 17 to 25 μM for all the generations of palmitic dendrons. Again, the third generation for hexanoic dendrons showed a lower CMC value than those observed for palmitic dendrons. Comparing the CMC data of the anionic and cationic systems, the latter afforded slightly higher values. It is worth noting that the lower CMC values obtained for the third generation dendrons containing hexanoic acids suggest the important role of the hydrophobic character of the dendritic scaffold in the amphiphilic behavior toward micelle formation.
With respect to the air/water interface, the hydrophilic charge of the head groups should be introduced in the water phase while the hydrophobic alkyl chain should be oriented to the air. From Table 2, the molecular area (A) occupied of C16Gn− (13–15) increased from n = 1 (0.61 nm2 per molecule) to n = 3 (0.98 nm2), suggesting that the volume of the head group was responsible for this increase. There was also observed an increase in σCMC with increasing generation.40 Regarding the salt effect, for the dendron C16G1− (13) with 2 and 20 mM of salt, the molecular area of the head group decreased as the salt concentration increased. This can be explained by a decrease in the strong electrostatic repulsion forces between the head groups due to the salt addition. Comparing the results for dendrons of the same generation with palmitic or hexanoic tails, the area occupied per molecule of dendron into the surface was clearly smaller for palmitic dendrons. The higher hydrophobic part of these systems can form an oriented monolayer in the interface allowing the molecule to be in closer packing than for hexanoic dendrons. For cationic micelles in the presence of salt, the amphiphilic dendrons were closer packing when generation decreased as it occurs with the anionic micelles; however, in this case, there was no difference between palmitic and hexanoic dendrons.
Hydrodynamic radii were determined by DLS for anionic and cationic micelles in the presence of salt (see Table 3) showing diameters between 3.8 and 6.4 nm for all of them, although no significant differences between anionic and cationic micelles were observed, taking the standard deviation into consideration. Hydrodynamic radii obtained were independent of dendron concentrations in the micellar regime at least for concentrations three fold higher than CMC. The increase in dendron concentrations appeared to increase the number of micelles and not their size, which showed the typical behavior of spherical ionic micelles. At low ionic dendron concentrations, we can assume that the dendritic micelles were spherical structures as is usual for conventional ionic surfactants.
| Anionic dendron | R H (nm) | Cationic dendron | R H (nm) |
|---|---|---|---|
| C16G1− (13) | 3.4 ± 0.1 | C16G1+ (31) | 3.2 ± 0.2 |
| C16G2− (14) | 2.9 ± 0.1 | C16G2+ (32) | 2.3 ± 0.1 |
| C16G3− (15) | 2.5 ± 0.1 | C16G3+ (33) | 2.3 ± 0.2 |
| C6G2− (17) | 2.3 ± 0.2 | ||
| C6G3− (18) | 2.2 ± 0.1 | C6G3+ (36) | 1.9 ± 0.1 |
A theory of micellar structure based on the geometry of various micellar shapes and the space occupied by the hydrophilic and hydrophobic groups of the surfactant molecules was developed by Israelachvili, Mitchell and Ninham.41 The volume occupied by the hydrophobic groups in the micellar core (V), the length of the hydrophobic groups in the core (L) and the cross-sectional area occupied by the hydrophilic groups in the micelle–solution interface (a0) have been used to calculate a “molecular packing parameter”, P = V/a0L, which determine the shape of micelles. P ≤ 1/3 accounts for spherical micelles, 1/3 < P < 1/2 for cylindrical ones, and 1/2 < P < 1 for bilayer structures such as vesicles. For ionic charged head groups at low concentrations, P must be lower than 1/3 due to the high value of a0. However, a0 decreases with salt addition due to a decrease in ionic repulsions between the head groups, which results in an increase of P and in the size of the micelles. With respect to dendron generation, although the RH values were close to each other, the tendency of the micelle size was detected to increase on decreasing the generation (see Fig. 7). The palmitic dendrons showed a systematic trend; the larger the head group the smaller the micelles. The change in generation affects a0 and also affects V and L values. The effect is more important in the cross-sectional area occupied by the hydrophilic groups in the micelle–solution interface. The salt addition permits us not to consider the increase in the number of charges with the generation. Basically, geometrical considerations can explain the decrease in hydrodynamic radius when the generation increases due to an increase in a0. The same effect was also observed in the cross-sectional area (A) occupied by the hydrophilic groups in the water–air interface (planar interface) (see Table 2).
As a preliminary work to demonstrate the capability of the family of carbosilane dendritic micelles to bind and carry therapeutic nucleic acids, complexes obtained by mixing nucleic acids with cationic micelles have been studied. The ability of cationic dendrons 31–36 to bind nucleic acids was tested using pro-apoptotic siRNA Mcl-143 as a model. The siRNA was mixed with cationic dendrons at different charge ratios. Such ratios correspond to dendron concentrations both below and above their CMC, and the amount of free siRNA in samples estimated from agarose gel electrophoregrams (Fig. 8A). The dendrons were found to bind siRNA in a different manner depending on the length of the fatty acid moiety at the focal point. Among the hexanoic acid-bearing dendrons 34–36, the siRNA binding efficiency increased with the dendron generation as G1 ≪ G2 < G3, indicating the positive dendritic effect on the complexation. Only the dendron C6G3+ (36) was able to form complexes with siRNA at a charge ratio of 1
:
1. In the case of dendrons with palmitic acid at the focal point C16Gn+ (31–33), no dendritic effect was observed, all of them efficiently binding the siRNA at the charge ratio of 1
:
2. These observations correlated with the dynamics of CMC values found and suggested that the siRNA binding by dendrons was the result of micelle formation. Hexanoic acid moieties for the first and second generations did not cause micelle formation as efficiently as the palmitic ones, thus affording an inefficient siRNA binding by dendrons 34 and 35 at charge ratio <5. Zeta potential profiles obtained by mixing siRNA with dendrons 31–36 at different charge ratios corroborated the effects observed (Fig. 8B).
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| Fig. 8 (A) Agarose gel electrophoresis and (B) zeta potential profiles of complexes of Mcl-1 siRNA with cationic dendrons 31–36 at different charge ratios. An siRNA concentration of 4 μM in PBS. | ||
The results suggested an interesting regularity of siRNA binding. As it has been shown in several works devoted to the physico-chemical studies of the formation of dendriplexes prepared from nucleic acids and cationic dendrimers, the charge ratios corresponding to the full binding obtained using agarose gel electrophoresis or using other methods (ethidium bromide intercalation assay, fluorescence polarization measurements) were usually lower than those corresponding to the plateau in the zeta potential profiles.44–46 As we have observed, this phenomenon did not depend on the number of positive charges per molecule or the dendrimer architecture.46 One can assume that the interaction of nucleic acids with pre-organized supramolecular assemblies was more favourable than with individual macromolecules. Alternatively, siRNA can facilitate the formation of micelles by stabilizing them via electrostatic interactions. Earlier, Liu et al. have demonstrated14 that the amphiphilic PAMAM dendrons bound siRNA completely at an N
:
P ratio of 1
:
2.5, whereas its cationic part (8 cationic groups on the periphery) without a lipid tail was not able to bind siRNA even at 10-fold excess of cations. Recently, the formation of nano-sized dendrimer aggregates has been shown to increase the efficiency of nucleic acid delivery.47 This is in agreement with the data on the comparison of the behaviour of the hexanoic and palmitic acid-bearing carbosilane dendrons presented here and support the above mentioned assumption. Thus, the organization of dendritic molecules into soft nanoparticles was essential for efficient nucleic acid binding.
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| Fig. 9 Absorption profiles in water of procaine hydrochloride in the presence of the dendron C16G1 (13) in the range of dendron concentrations of 1–80 μM. | ||
CH2), 1.61 (m, 4H, OCH2CH2CH2CH2Si, CH3(CH2)12CH2CH2CO2), 2.26 (t, 2H, CH3(CH2)12CH2CH2CO2), 4.04 (t, 2H, OCH2CH2CH2CH2Si), 4.85 (m, 4H, SiCH2CH
CH2), 5.75 (m, 2H, SiCH2CH
CH2). 13C NMR (CDCl3) δ −5.29 (SiMe), 12.5 (OCH2CH2CH2CH2Si), 14.1 (CH3CH2CH2(CH2)10CH2CH2CO2), 20.7 (OCH2CH2CH2CH2Si), 21.2 (SiCH2CH
CH2), 22.6 (CH3CH2CH2(CH2)10CH2CH2CO2), 24.6 (CH3CH2CH2(CH2)10CH2CH2CO2), 29.42 (CH3CH2CH2(CH2)10CH2CH2CO2), 31.9 (CH3CH2CH2(CH2)10CH2CH2CO2), 32.3 (OCH2CH2CH2CH2Si), 34.3 (CH3CH2CH2(CH2)10CH2CH2CO2), 63.8 (OCH2CH2CH2CH2Si), 113.2 (SiCH2CH
CH2), 134.6 (SiCH2CH
CH2), 173.9 (CH3CH2CH2(CH2)10CH2CH2CO2). MS: [M + H]+ = 437.43 Da. Anal. calculated for C27H52O2Si (436.78 g mol−1) %: C, 74.24, H, 12.00. Exp. %: C, 74.13, H, 11.86.
:
25) and a 0.5 mL aqueous solution containing sodium 3-mercapto-1-propanesulfonate (0.45 g, 2.51 mmol) was prepared. Over the dendron solution, one fourth of the aqueous solution and of the photoinitiator 2,2 dimethoxy-2-phenylactenophenone (DMPA) (0.06 g, 0.25 mmol) were added. The mixture was deoxygenized and stirred under UV light for 1 h. The aqueous solution was added stepwise each 1 h with the photoinitiator. The total irradiation time was 4 h. Afterwards, solvents were removed under vacuum and the products were dissolved in distilled water and purified by nanofiltration with cellulose membranes with a cutoff limit MWCO = 500–1000 Da. Finally, water was removed to obtain 13 as a white powder with a high yield (0.82 g, 91%). Data for 13 are as follows. NMR (D2O): 1H NMR δ −0.13 (m, 3H, SiMe), 0.53 (m, 6H, OCH2CH2CH2CH2Si, SiCH2CH2CH2S), 0.75 (m, 3H, CH3(CH2)14CO2), 1.15 (m, 26H, CH3(CH2)12(CH2)2CO2, OCH2CH2CH2CH2Si), 1.47 (m, 8H, CH3(CH2)12CH2CH2CO2, OCH2CH2CH2CH2Si, SiCH2CH2CH2S), 1.89 (m, 4H, SCH2CH2CH2SO3,), 2.14 (m, 2H, CH3(CH2)12CH2CH2CO2), 2.44 (m, 4H, SiCH2CH2CH2S), 2.52 (m, 4H, SCH2CH2CH2SO3), 2.85 (m, 4H, SCH2CH2CH2SO3), 3.92 (m, 2H, OCH2CH2CH2CH2Si). 13C NMR (D2O) δ −5.35 (SiMe), 12.8 (SiCH2CH2CH2S), 13.2 (OCH2CH2CH2CH2Si), 13.92 (CH3 (CH2)12CH2CH2CO2), 20.1 (OCH2CH2CH2CH2Si), 23.9 (SiCH2CH2CH2S), 24.5 (SCH2CH2CH2SO3), 24.9 (CH3(CH2)10CH2CH2CO2), 29.3–29.9 (CH3(CH2)12CH2CH2CO2), 30.29 (SCH2CH2CH2SO3), 32.3 (OCH2CH2CH2CH2Si), 34.1 (CH3(CH2)12CH2CH2CO2), 35.2 (SiCH2CH2CH2S), 50.1 (SCH2CH2CH2SO3), 63.9 (OCH2CH2CH2CH2Si), 173.3 (CH3CH2CH2(CH2)10CH2CH2CO2). Anal. calculated for C33H66Na2O8S4Si (793.20 g mol−1) %: C, 49.97, H, 8.39. Exp. %: C, 49.95, H, 8.35.
:
25) solution (5 ml) were mixed. The reaction mixture was deoxygenated and irradiated for 2 h. Another 5% mol of DMPA was added, and the reaction mixture was irradiated for 2 h again and monitored by 1H NMR. The products were dissolved in distilled water and purified by nanofiltration with cellulose membranes with a cutoff limit MWCO = 500–1000 Da. Finally, water was removed to obtain 19 as a white powder with a high yield (1.5 g, 88%). Data for 19 are as follows. NMR (D2O): 1H NMR δ 0.00 (s, 3H, SiMe), 0.54 (t, 2H, OCH2CH2CH2CH2Si), 0.84 (t, 3H, CH3(CH2)14CO2), 0.90, (t, 4H, SiCH2CH2S), 1.25 (s, 24H, CH3(CH2)12(CH2)2CO2), 1.30 (m, 2H, OCH2CH2CH2CH2Si), 1.58 (m, 4H, OCH2CH2CH2CH2Si, CH3(CH2)12CH2CH2CO2), 2.24 (t, 2H, CH3(CH2)12CH2CH2CO2), 2.62 (t, 4H, SiCH2CH2S), 2.87 (s, 12H, SCH2CH2NMe2HCl), 3.0 (m, 4H, SCH2CH2NMe2HCl), 3.27 (m, 4H, SCH2CH2NMe2HCl), 4.00 (t, 2H, OCH2CH2CH2CH2Si). 13C NMR (D2O) δ −5.4 (SiMe), 12.5 (OCH2CH2CH2CH2Si), 13.4 (SiCH2CH2S), 14.0 (CH3CH2CH2(CH2)10CH2CH2CO2), 20.0 (OCH2CH2CH2CH2Si), 22.6 (CH3CH2CH2(CH2)10CH2CH2CO2), 24.3 (SCH2CH2NMe2HCl), 24.9 (CH3CH2CH2(CH2)10CH2CH2CO2), 26.0 (SiCH2CH2S), 29.0–29.6 (CH3CH2CH2(CH2)10CH2CH2CO2), 31.8 (CH3CH2CH2(CH2)10CH2CH2CO2), 32.2 (OCH2CH2CH2CH2Si), 34.2 (CH3CH2CH2 (CH2)10CH2CH2CO2), 41.4 (SCH2CH2NMe2HCl), 55.3 (SCH2CH2NMe2HCl), 63.7 (OCH2CH2CH2CH2Si), 173.7 (CH3CH2CH2(CH2)10CH2CH2CO2). Anal. calculated for C33H72Cl2N2O2S2Si (692.05 g mol−1) %: C, 57.27, H, 10.49, N, 4.51. Exp. %: C, 57.15, H, 10.35, N, 4.39.
Footnote |
| † Electronic supplementary information (ESI) available. See DOI: 10.1039/c7ob01331k |
| This journal is © The Royal Society of Chemistry 2017 |