Sahan R. Salpage,
Yuewen Xu,
Bozumeh Som,
Ammon J. Sindt,
Mark D. Smith and
Linda S. Shimizu
*
Department of Chemistry and Biochemistry, University of South Carolina, 631 Sumter St., Columbia, SC 29208, USA. E-mail: shimizuls@mailbox.sc.edu; Fax: +1-803-777-9521; Tel: +1-803-777-2066
First published on 6th October 2016
Porous organic crystalline materials were obtained by the self-assembly of pyridyl-phenylethynylene bis-urea macrocycles (1). In contrast to the typical columnar assembly of other bis-urea macrocycles, 1 assembled into interdigitated layers to afford a host with small 1D channels with a pore diameter of ∼4.5 Å. Herein, we discuss the origin between the expected and observed assembly and demonstrate the utility of these activated organic crystals to absorb a guest and maintain crystallinity during the reaction of the encapsulated guest and subsequent product isolation. Isoprene was chosen as a model monomer due to the small channel diameter of 1. The activated crystals were able to absorb isoprene and facilitate a photoinitiated and stereoselective oligomerization to produce trans-1,4-polyisoprene with low dispersity. The products were readily extracted from the crystals and analysis of the microstructure of the oligomer showed 97% trans-1,4 content and a dispersity (Đ) of 1.39. Despite the altered assembly pattern of this bis-urea macrocycle, powder X-ray diffraction studies demonstrated that the crystalline host was remarkably robust and stable throughout the activation, isoprene absorption, photoinduced polymerization, and product recovery processes. Our future investigations are focused on assessing the stability of the isoprene radicals within the host and evaluating the loading and reaction of other monomers.
Our group employs well-defined porous materials from self-assembled bis-urea macrocycles building blocks that consist of two urea groups and two C-shaped spacers (Fig. 1a). When the urea groups are preorganized approximately perpendicular to the plane of the macrocycle and in the absence of competing hydrogen bond acceptors, these macrocycles assemble into columnar structures.16 The phenylethynylene bis-urea 2 assembled into columns of ∼9 Å in diameter (Fig. 1c), affording functional crystals that were applied to the photodimerizations of coumarins, chromones and acenaphthylene.17–19 Here, we replace the central aryl group of 2 with the pyridyl unit to test the effects of the heterocycle on the subsequent assembly (Fig. 1b). We then demonstrate the utility of these porous crystals for guest absorption as well as for the subsequent photoreaction of isoprene within this confined nanoreactor.
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| Fig. 1 Heteroatoms, in the form of a pyridyl nitrogen in 1, altered the typically columnar assembly of bis-urea macrocycles. The interdigitated assembly of this new material afforded robust crystals with smaller 1D channels, which are used to polymerize isoprene to produce trans-1,4-polyisoprene. (a) Schematic representation of macrocycle 1 and 2. (b) Interdigitated assembly of 1 forms 1D channels with a diameter of 4.5 Å. (c) Columnar assembly of 2 forms 1D channels with a diameter of 9 Å.19 (d) Photo irradiation of isoprene in host crystals produces trans-1,4-polyisoprene in high selectivity. | ||
:
MeOH, 95
:
5). The product was further washed with water followed by hexane to remove excess TBAF and dried in vacuo to obtain the diol as pale yellow solid 1.3 g, (91%); mp 221 °C; 1H-NMR: (400 MHz, DMSO-d6 δ): 7.93–7.89 (t, 1H, J = 8.1 Hz, Ar-H), 7.65 (d, J = 7.8 Hz, 2H, Ar-H), 7.60 (d, 4H, J = 8.1 Hz, Ar-H), 7.41 (d, J = 8.1 Hz, 4H, Ar-H), 5.35 (t, J = 5.8 Hz, 2H, –OH), 4.55 (d, J = 5.7 Hz, 4H, –CH2); 13C-NMR: (100 MHz, DMSO-d6): δ 145.16, 143.48, 138.45, 132.30, 127.39, 127.33, 119.89, 89.82, 88.59, 63.13; IR (cm−1): 3340, 3315, 2214, 1440, 1244, 1163, 804; HRMS (EI+): [M+] calculated: 339.1259, found: 339.1260.
:
hexanes, 1
:
1) to obtain the dibromide as pale yellow solid 0.9 g, (66%); mp 183 °C; 1H-NMR: (400 MHz, CD3Cl δ): 7.75–7.64 (t, J = 8.2 Hz, 1H, Ar-H), 7.58 (d, J = 7.2 Hz, 4H, Ar-H), 7.48 (d, 2H, J = 7.8 Hz, Ar-H), 7.39 (d, J = 8.2 Hz, 4H, Ar-H), 4.49 (s, 4H, –CH2); 13C-NMR: (100 MHz, CD3Cl) δ: 143.88, 138.91, 136.75, 132.72, 129.36, 126.66, 122.42, 89.32, 89.20, 33.04; IR (cm−1): 3315, 2214, 1440, 1244, 1163, 804; HRMS (EI+): [M+] calculated: 462.9571, found: 462.9590.
:
ethyl ether
:
MeOH, 4
:
4
:
0.5) to obtain the product as pale yellow solid 0.19 g (19%); 1H-NMR: (300 MHz, CDCl3 δ): 7.70–7.61 (m, 2H, Ar-H), 7.63–7.57 (m, 8H, Ar-H), 7.47–7.45 (m, 4H, Ar-H), 7.36–7.34 (m, 8H, Ar-H), 4.59 (s, 8H, –CH2–), 4.25 (s, 8H, –CH2–), 0.96 (s, 18H, –CH3); 13C-NMR: (100 MHz, CDCl3 δ): 155.87, 143.87, 139.46, 136.40, 132.50, 128.15, 125.96, 121.16, 89.45, 88.49, 61.82, 54.38, 48.59, 28.24; IR (cm−1): 3315, 2214, 1630, 1440, 1244, 1163, 804; HRMS (ES+): [M + H]+ calculated: 921.4604, found: 921.4582.
:
1 mixture of 20% [NH(CH2CH2OH)2/H2O, adjusted with HCl to pH ∼ 2]: MeOH and heated to reflux for 48 h. A pale yellow precipitate formed after 24 h. The solution was cooled in an ice bath for 30 min. The product was suction filtered, washed with H2O (30 mL) and MeOH (30 mL), and dried in vacuo to obtain the final product as pale yellow powder 0.14 g (90%). 1H-NMR: (400 MHz, DMSO-d6 δ): 7.91–7.87 (m, 2H, Ar-H), 7.64–7.60 (m, 12H, Ar-H), 7.33–7.31 (m, 8H, Ar-H), 6.69 (t, J = 6.2 Hz, 4H, –NH), 4.30 (d, J = 6.1 Hz, 8H, –CH2); 13C-NMR: (100 MHz, DMSO-d6 δ): 158.54, 143.84, 143.29, 138.07, 132.28, 127.53, 127.09, 119.60, 89.48, 88.50, 43.01; IR (cm−1): 3315, 2214, 1630, 1554, 1440, 1244, 1163, 804; HRMS (ES+): [M + H]+ calculated: 727.2821, found: 727.2795.| 1 | 3 | |
|---|---|---|
| Empirical formula | C48H34N6O2 | C61H58Cl2N8O2 |
| Formula weight | 726.81 | 1006.05 |
| Temperature/K | 100(2) | 150(2) |
| Crystal system | Orthorhombic | Monoclinic |
| Space group | Pbcn | P21/m |
| a/Å | 19.711(5) | 9.6662(4) |
| b/Å | 8.983(2) | 18.8900(8) |
| c/Å | 26.520(6) | 14.4567(6) |
| α/° | 90 | 90 |
| β/° | 90 | 91.464(1) |
| γ/° | 90 | 90 |
| Volume/Å3 | 4695.7(18) | 2638.85(19) |
| Z | 4 | 2 |
| ρcalc (g cm−3) | 1.028 | 1.266 |
| μ/mm−1 | 0.064 | 0.175 |
| F(000) | 1520 | 1060 |
| Crystal size/mm3 | 0.48 × 0.20 × 0.08 | 0.28 × 0.20 × 0.08 |
| 2θ range/° | 3.072–45.078 | 1.41–23.26 |
| Index ranges | −21 ≤ h ≤ 21 | −10 ≤ h ≤ 10 |
| −9 ≤ k ≤ 9 | −20 ≤ k ≤ 20 | |
| −28 ≤ l ≤ 28 | −16 ≤ l ≤ 16 | |
| Reflections collected | 45 741 |
28 637 |
| Independent reflections | 3087 | 3930 |
| Rint | 0.1417 | 0.0615 |
| Parameters | 261 | 379 |
| GoF on F2 | 1.080 | 1.017 |
| Final R1 [I > 2σ(I)] | 0.0596 | 0.0750 |
| Final wR2 [I > 2σ(I)] | 0.1732 | 0.2161 |
| Final R1 [all data] | 0.0909 | 0.1066 |
| Final wR2 [all data] | 0.1868 | 0.2410 |
| Δρmin,max/e Å−3 | 0.20/−0.15 | 0.822/−0.321 |
Following deprotection of 3, host 1 (20 mg/4 mL DMSO) was crystallized by vapor diffusion of methanol affording pale yellow needle crystals suitable for single crystal X-ray diffraction. The crystal structure revealed the expected bis-urea macrocycle as a solvate; however, 1 was not planar but folded into a bowl or saddle conformation with C2 point symmetry (Fig. 2a). Here, the two urea groups remain oriented in the same direction. This folded architecture assembles through typical bifurcated urea hydrogen bonds (N(H)⋯O distances of 2.81–2.87 Å) with four neighboring macrocycles to afford 2D assemblies of interdigitated cycles (Fig. 2b). The packing of the layers creates tubular channels of ∼4.5 Å in diameter along the crystallographic b axis (Fig. 2c). The channels are occupied by disordered solvent molecules (DMSO and/or MeOH). Adjacent layers alternate ureas in an anti-parallel fashion resulting in a cancellation of the dipoles. The assembly is further stabilized by aryl stacking and CH-pi interactions. The crystalline structures have regular and aligned 1D pores with diameters of ∼4.5 Å (Fig. S9, ESI†).
The conformational difference between the saddle structure of 1 (X = N) with the relatively planar conformation of the carbon derivative 2 (X = CH), reported previously,19 is striking and appears to drive the interdigitated assembly of 1 over the columnar assembly of 2. The density of 1, calculated in the absence of the disordered guests, is 1.028 mg mm−3 (orthorhombic, space group Pbcn) with a solvent accessible volume per unit cell estimated as 1341.4 Å3 (28.6% of the total unit cell volume). In comparison columnar assembled 2 (monoclinic, space group P21/n) has a calculated solvent-free density of 1.061 mg mm−3 with a solvent-accessible volume of the unit cell estimated as 491.1 Å3 (21.6% of the total unit cell volume).19 We further compared the assemblies using Hirshfeld analysis.22–24 Interestingly, the two assembly motifs show similar contributions of key interactions including hydrogen bonding (1: 5.5% vs. 2: 6.1% O⋯H), and CH-aryl interactions (1: 26.5% vs. 2: 26.4% C⋯H contacts) but displayed small differences in aryl stacking interactions (1: 7% vs. 2: 11.7% C⋯C) and in contacts to nitrogen (1: 4.3% vs. 2: 1.4% N⋯H) (Fig. S11–S12, ESI†). A screen of crystallization conditions has not yet yielded other crystal forms of 1.
The smaller diameter channels of 1 versus 2 (4.5 vs. 9 Å) are comparable to channels that encapsulate isoprene in inclusion complexes with dipeptides or cyclotriphosphazenes.25,26 Isoprene and its polymers are widely used in industry to synthesize block copolymers,27–29 as compatibilizers for natural rubber and acrylic polymer blends,30,31 as nanocomposites,32,33 and to produce macromolecular core shell nano architectures.34,35 These materials can have low glass transition temperatures and unsaturated backbone or side chains that allow further functionalization.36 Thus, isoprene provides an interesting model monomer to evaluate the stability of host 1 as a container to reversibly absorb a guest and to remain stable over the course of the reaction of the encapsulated material. Conventional polymerization of isoprene provides isomeric polymers through different addition modes (cis-1,4-, trans-1,4, 1,2- or 3,4-) depending upon how the C–C double bonds react (Fig. 3a). Anionic polymerization is the technique of choice but requires stringent reaction conditions and leads to low trans-1,4-selectivity (Table S1, ESI†).37 The trans-1,4 (Balata) is produced by plants using enzymatic synthesis. It exhibits excellent thermoplastic characteristics, high tensile strength, abrasion resistance, and is free from odor and taste.38,39 Yet, stereoselective synthesis of trans-1,4-polyisoprene remains challenging. Confined environments have been applied for the selective radical polymerization of isoprene trapped within the controlled pores, a process that typically requires high energy gamma irradiation necessitating careful handling and specialized reactors.15
Our goal was to evaluate if encapsulation in the small channels of 1 could modulate the reactivity of isoprene and enable polymerization under mild conditions. Initially, the channels of 1 are filled with solvent, which was removed prior to the introduction of isoprene. Thermogravimetric analysis (TGA) showed a two step desorption from rt to 250 °C with a 9.98% weight loss. The crystals were also heated at 120 °C for 3 h resulting in a similar weight loss (Fig. S13, ESI†). Powder X-ray diffraction (PXRD) was used to compare the solvated and activated structures before and after solvent removal (Fig. 3c, patterns ii and iii). Comparison of the two PXRD patterns show they are nearly identical suggesting that the material still maintains its crystallinity after solvent evacuation. Indeed, removal of the disordered solvent did not change the morphology of the crystals.
Freshly recrystallized 1 (20 mg) was heated at 120 °C to remove the disordered solvent and further evacuated under high vacuum before exposure to isoprene under reduced pressure at room temperature for 3 h. A custom made loading apparatus was used to absorb isoprene from its vapor phase under reduced pressure at room temperature for 24 h, conditions in order to approach equilibrium (Fig. 3b). A sample of the crystals (2 mg) was dissolved in DMSO-d6 and analysed by 1H NMR. Comparison of the integrated peaks suggests that isoprene had been absorbed in a 1
:
1 host
:
guest ratio (Fig. S19†). The host 1·isoprene material was frozen in liquid N2, vacuum, sealed, and UV-irradiated in a Rayonet RPR-200 UV reactor equipped with 350 nm lamps for 24 h at rt. The irradiated material showed similar PXRD pattern suggesting that the crystal form was not altered during the loading process and the subsequent reaction (Fig. 3c, patterns iii and iv). The polymer was then extracted from the host by sonication with CHCl3 (10 mL). The suspension of host 1 and polymer was filtered to recover the host and the filtrate concentrated in vacuo. Polyisoprene was precipitated by the dropwise addition of ice-cold methanol.
The products displayed the simple 1H NMR spectra shown in Fig. 4a. The polymer microstructure consists mainly of trans-1,4-polyisoprene in 96.7% with 3.3% cis-1,4-isomer. The absence of signals at ∼5.9 ppm and ∼4.7 ppm indicated that no significant amount of the branched 1,2- or 3,4-structures had been formed. Gel permeation chromatography was used to analyse the molar mass of the resulting polymer. The polymer shows a Mn = 4400 g mol−1 with a dispersity (Đ) of 1.39 (Fig. 4b). The average length of the channels in the bulk material was estimated from dark field microscope images as ∼212.8 μm. Assuming isoprene is fully absorbed in channels of 1, the rough maximum Mw is ∼3.02 × 107 g mol−1. Studies are underway to optimize conditions for the polymerization. Evacuated host 2 (20 mg) was exposed to isoprene and similarly UV-irradiated; however, no oligomers or polymers were formed, which suggests that isoprene either has a low affinity for the larger channels of 2 or is not reactive within these channels.
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| Fig. 4 Characterization of the isolated polyisoprene. (a) 1H NMR (CDCl3, 400 MHz) of the polyisoprene. (b) GPC trace of polyisoprene in THF. | ||
Isoprene has a low boiling point and likely desorbs from these hosts at room temperature over the 24 h irradiation period. Thus, full characterization of the host·isoprene material was not possible and one cannot rule out the possibility that this is a simple mixture. However, the reasonably high molecular weight polymer and low dispersity for a free radical polymerization process induced by UV-irradiation of host 1·isoprene material is a strong indication that isoprene is bound within the channels of 1 and that the reaction proceeds relatively quickly before isoprene has a chance to desorb. Recent work from Kitagawa and co-workers on the radical polymerization of 2,3-dimethyl-1,3-butadiene in a porous coordination polymer suggests that their confined environment stabilizes the propagating radicals and inhibits radical termination.40
Footnote |
| † Electronic supplementary information (ESI) available: NMR spectra, PXRD, TGA, isoprene loading studies, characterization of the polymer and crystallographic data CCDC. CCDC 1457935 and 1463771. For ESI and crystallographic data in CIF or other electronic format see DOI: 10.1039/c6ra18681e |
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