Literature DB >> 32356978

Single-Step Enantioselective Synthesis of Mechanically Planar Chiral [2]Rotaxanes Using a Chiral Leaving Group Strategy.

Chong Tian1, Stephen D P Fielden1, Borja Pérez-Saavedra1, Iñigo J Vitorica-Yrezabal1, David A Leigh1,2.   

Abstract

We report a one-step enantioselective synthesis of mechanically planar chiral [2]rotaxanes. Previous studies of such molecules have generally involved the separation of enantiomers from racemic mixtures or the preparation and separation of diastereomeric intermediates followed by post-assembly modification to remove other sources of chirality. Here, we demonstrate a simple asymmetric metal-free active template rotaxane synthesis using a primary amine, an activated ester with a chiral leaving group, and an achiral crown ether lacking rotational symmetry. Mechanically planar chiral rotaxanes are obtained directly in up to 50% enantiomeric excess. The rotaxanes were characterized by NMR spectroscopy, high-resolution mass spectrometry, chiral HPLC, single crystal X-ray diffraction, and circular dichroism. Either rotaxane enantiomer could be prepared selectively by incorporating pseudoenantiomeric cinchona alkaloids into the chiral leaving group.

Entities:  

Year:  2020        PMID: 32356978      PMCID: PMC7266371          DOI: 10.1021/jacs.0c03447

Source DB:  PubMed          Journal:  J Am Chem Soc        ISSN: 0002-7863            Impact factor:   15.419


Introduction

Mechanical planar chirality arises in rotaxanes with achiral components when an unsymmetrical axle is threaded through a macrocycle lacking rotational symmetry (Figure ).[1−4] Although lacking classical elements of chirality, studies on mechanically planar chiral rotaxanes suggest their asymmetry can be well expressed for applications.[5−7] However, despite mechanically planar chiral rotaxanes being known for nearly 50 years, their enantioselective synthesis remains challenging.[1d,8] Most studies on these systems rely on the separation of enantiomers from racemic mixtures by chiral stationary phase HPLC, limiting the scale of enantioenriched material that can readily be obtained.[9]
Figure 1

Enantioselective synthesis of mechanically planar chiral rotaxanes through metal-free active template N-acylation using a macrocycle lacking rotational symmetry and an electrophile with a point-chiral leaving group.

Enantioselective synthesis of mechanically planar chiral rotaxanes through metal-free active template N-acylation using a macrocycle lacking rotational symmetry and an electrophile with a point-chiral leaving group. Goldup et al. have addressed this synthetic problem through a chiral auxiliary approach that forms intermediate diastereomeric rotaxanes having both point chirality and mechanically planar chirality.[10,11] Separation of these diastereomeric intermediates by flash chromatography, followed by removal of the point chirality by either substitution[10] or symmetrization,[11] afforded enantioenriched mechanically planar chiral rotaxanes. The only single-step synthesis of enantioenriched mechanically planar chiral rotaxanes to date used a chiral catalyst to resolve the interconverting enantiomers of a crown ether-ammonium pseudorotaxane by capping.[12] Despite attempts to optimize this method, it produced rotaxanes in just 4% enantiomeric excess (e.e.). Here we report a simple, single-step, enantioselective synthesis of mechanically planar chiral rotaxanes that produces either enantiomer in up to 50% e.e. Metal-free active template reactions have recently been developed in which rotaxanes[13] are spontaneously assembled under kinetic control in a single step by combining a primary amine, electrophile, and crown ether[14] in apolar solvents. Crown ethers stabilize the transition states of various nucleophilic substitution reactions through the cavity by C–H hydrogen bonding, thereby favoring the formation of rotaxanes over the unthreaded axle. Different reactions, amines, and leaving groups result in different degrees of accelerated reaction through the ring, affording different rotaxane:thread selectivities. We chose crown ether-stabilized N-acylation for the present study (Scheme ), as this active template reaction often results in a particularly high ratio of rotaxane:thread.[14] This suggested the reaction might be tolerant of the additional functionality necessary in the macrocycle (to break rotational symmetry) and axle building blocks (to provide a chiral leaving group).
Scheme 1

: (a) Achiral Rotaxane Synthesis by Active Template N-Acylation Using Rotationally Symmetrical Crown Ethers; (b) Racemic and Unoptimized Enantioselective Synthesis of a Mechanically Planar Chiral Rotaxane

An example of an active template N-acylation is the reaction of 24-crown-8 1, primary amine 2, and electrophile 3 in toluene at room temperature, producing amide [2]rotaxane 4 in 84% yield (Scheme a).[14b] The rate-determining step of crown ether catalyzed N-acylation reactions is the collapse of the tetrahedral intermediate formed on addition of the amine to the activated ester.[15] The nitro-phenol ester used in the reaction of 1, 2, and 3 thus provides an opportunity for a chiral directing group to be incorporated into the leaving group that could interact with a rotationally unsymmetrical macrocycle in the transition state (Figure ).[16]

Results and Discussion

Development of an Enantioselective Rotaxane Synthesis

To establish that functionalized crown ethers could take part in the active template reaction, amine 2 and activated ester 3 were treated with commercially available dibenzo-24-crown-8 (5) in toluene, yielding the corresponding [2]rotaxane, 6, in 73% yield (Scheme a). However, although the rotaxane axle is unsymmetrical, dibenzo-24-crown-8 (5) is D2 symmetric and so rotaxane 6 is achiral.[1] Macrocycle 7, containing two different aromatic rings, lacks rotational symmetry (it has C1 symmetry, alternatively referred to as C). Reaction of 7 with 2 and 3 furnished racemic mechanically planar chiral rotaxane 8 in 78% yield (Scheme b). The enantiomers of 8 could be separated by chiral stationary phase HPLC (see Supporting Information). Next, we investigated the structure and location for an effective chiral leaving group in the electrophile. Preliminary screening studies identified nitrophenol ester 9, in which the chiral information stems from an O-alkylated cinchonidine unit adjacent to the nitro-group (Scheme b). This electrophile was reactive under the rotaxane-forming conditions despite the introduction of the deactivating electron-donating ether linkage. Combining 2, 7, and 9 in a 1:1:1 stoichiometry in toluene at room temperature afforded rotaxane 8 in 43% yield (Scheme b). Under similar conditions, electrophiles based on alkyl (thio)esters or with the cinchonidine unit positioned at the ortho position of the nitrophenol ring were either unreactive or generated less rotaxane (see Supporting Information). HPLC analysis of rotaxane 8 (isolated by flash chromatography) obtained from electrophile 9 revealed that the (+)-enantiomer (determined by polarimetry) had been formed in 12% e.e., confirming that a point-chiral leaving group was able to induce enantioselectivity of a mechanically planar rotaxane product. Increasing the electronic difference between the two aromatic substituents within the macrocycle improved the enantioselectivity of the active template reaction. Macrocycle 10, with a nitro group on the catechol unit (see Supporting Information for its synthesis), afforded rotaxane (+)-11 in 23% e.e. at room temperature, which increased to 40% e.e. (55% yield) when the rotaxane-forming reaction was performed at −40 °C (Figure a). Lowering the reaction temperature beyond −40 °C did not result in further improvements in enantioselectivity.[17]
Figure 2

(a) Enantioselective synthesis of mechanically planar chiral rotaxane 11. Reaction conditions: 2 equiv of amine 2, 1 equiv each of electrophile and crown ether 10, toluene, [0.14 M], –40 °C, 24 h. (b) Partial 1H NMR spectra (600 MHz, CDCl3, 295 K) of macrocycle 10 (top), rotaxane 11 (middle) and the corresponding unthreaded axle (bottom).

(a) Enantioselective synthesis of mechanically planar chiral rotaxane 11. Reaction conditions: 2 equiv of amine 2, 1 equiv each of electrophile and crown ether 10, toluene, [0.14 M], –40 °C, 24 h. (b) Partial 1H NMR spectra (600 MHz, CDCl3, 295 K) of macrocycle 10 (top), rotaxane 11 (middle) and the corresponding unthreaded axle (bottom). The opposite enantiomer of the rotaxane, (−)-11, could be selectively accessed using electrophile 12, derived from (+)-cinchonine, a pseudoenantiomer of cinchonidine (see Supporting Information for synthesis).[18] Combining 2, 10, and 12 at −40 °C gave rotaxane (−)-11 in 50% e.e. and 51% yield (Figure a). The difference in enantioenrichment is a consequence of electrophiles 9 and 12 being diastereomers rather than true enantiomers.

Characterization of Rotaxanes

Comparison of the 1H NMR spectra of macrocycle 10, rotaxane 11, and the unthreaded axle (see Supporting Information for synthesis) in CDCl3 at 298 K (Figure b) confirmed the interlocked structure of 11. The geminal protons of the crown ether display twice the number of environments in rotaxane 11 as in unthreaded 10 due to desymmetrization of the two macrocycle faces upon rotaxane formation, while H3 and H5 of the axle (hydrogen labeling shown in Figure a), which are situated either side of the amide group, display significant diastereotopic splitting (Δδ = 0.39 and 0.22 ppm respectively) within the chiral environment of rotaxane 11 which, as would be expected, is absent for the corresponding achiral noninterlocked axle. Upfield shifts of H6 and H7 (Δδ = −0.32 and −0.34 ppm) in the threaded axle and HA, HB, and HC (Δδ = −0.49, −0.21, and −0.37 ppm) of the nitrocatechol unit of the threaded macrocycle result from π–π interactions involving these moieties. These intercomponent interactions may play a role in rigidifying the transition state of the collapsing tetrahedral intermediate. The large downfield shift of the amide N–H proton H4 (Δδ = +1.74 ppm) in 11 is indicative of intercomponent hydrogen bonding between the amide and the glycol chain of the macrocycle. An upshield shift of HD (Δδ = −1.29 ppm) results from hydrogen bonding with the amide oxygen atom.[14b] Enantioenriched samples of rotaxane 11 (40% e.e. for the (+) enantiomer and 50% e.e. for the (−) enantiomer) were compared by circular dichroism (Figure a). The CD spectra of the mechanically planar chiral rotaxane enantiomers are symmetrical in terms of curve shape and have exciton couplings of opposite sign with maxima at 243 nm. The difference in intensity (normalized for absorption) of the spectra in Figure a corresponds to the difference in enantioenrichment of the samples.
Figure 3

(a) Circular dichroism spectra (1.0 × 10–4 M, CH2Cl2, 298 K) of (+)-11 (red) and (−)-11 (blue), baseline corrected. (b) Chemical structure of racemic rotaxane 13. (c) X-ray crystal structure of racemic rotaxane 13, side-on view showing intercomponent hydrogen bonds (in green). Hydrogen bond lengths: N47H—O16, 2.20 Å; O49—HC6, 2.63 Å. Hydrogen bond angles: N47—H–O16, 158.4°; O49—H–C6, 161.8°. (d) X-ray crystal structure of 13 viewed along the axle showing π-stacking between the macrocycle 1,2-dihydroxynaphthalene and axle bis(trifluoromethyl)phenyl rings. Centroid–centroid distance, 3.67 Å. Angle described by C40 and centroids, 97.6°. Solvate molecules and other hydrogen atoms omitted for clarity.

(a) Circular dichroism spectra (1.0 × 10–4 M, CH2Cl2, 298 K) of (+)-11 (red) and (−)-11 (blue), baseline corrected. (b) Chemical structure of racemic rotaxane 13. (c) X-ray crystal structure of racemic rotaxane 13, side-on view showing intercomponent hydrogen bonds (in green). Hydrogen bond lengths: N47H—O16, 2.20 Å; O49—HC6, 2.63 Å. Hydrogen bond angles: N47—H–O16, 158.4°; O49—H–C6, 161.8°. (d) X-ray crystal structure of 13 viewed along the axle showing π-stacking between the macrocycle 1,2-dihydroxynaphthalene and axle bis(trifluoromethyl)phenyl rings. Centroid–centroid distance, 3.67 Å. Angle described by C40 and centroids, 97.6°. Solvate molecules and other hydrogen atoms omitted for clarity. Although we were unable to obtain high quality single crystals of 11, single crystals of a racemic sample of 13 suitable for analysis by X-ray diffraction were grown by slow evaporation of an isopropanol/hexane solution of 13 (Figure b). Rotaxane 13 contains the same macrocycle as 11 and an axle derived from amine 2 and a different acyl stopper. The X-ray crystal structure of 13 (Figure c), containing both rotaxane enantiomers in the unit cell, shows similar intercomponent interactions to those observed by 1H NMR for 11 in solution (Figure b). Hydrogen bonds are present between an oxygen of the macrocycle glycol chain and the amide hydrogen atom of the axle and between the amide oxygen and a macrocycle C–H hydrogen atom (analogous to HD in 11).[14] The di(alkoxyl)naphthalene ring of the macrocycle and bis(trifluoromethyl)benzene unit of the axle π-stack (Figure d, closest centroid-centroid distance = 3.67 Å),[19] with the nitro-catechol moiety positioned so as to cover one face of the amide group. A similar arrangement in the transition state of the active template reaction would orient the macrocycle with respect to the axle building blocks such that one mechanically planar chiral enantiomer would be favored over the other.

Origin of Enantioselectivity

A preliminary indication of the origin of chiral transduction in these systems comes from the relative energies of the tetrahedral intermediates preceding (+)- and (−)-11, calculated at the PM6 level[20] using the Gaussian 09 software package[21] (Supporting Information and Figure ). The collapse of similar tetrahedral intermediates has previously been shown[15a] to be the rate-determining step for the glyme catalysis of ester aminolysis. Following the Hammond postulate, the differences between the diastereomeric tetrahedral intermediates to (+)- and (−)-11 from 9 and 12 may resemble those between the transition states. The lowest energy intermediate calculated for both pseudoenantiomeric leaving groups featured an (S) stereocenter adjacent to the ammonium unit, but with the macrocycle orientation inverted for the two pseudoenantiomers (Figure ), meaning changing between the leaving groups of 9 and 12 favors the formation of a different enantiomer of 11, as observed experimentally. The somewhat surprising indication that the two chiral leaving groups both favor an (S)-tetrahedral intermediate may reflect why the pseudoenantiomers do not generate equal and opposite e.e.’s in the active template reaction. The noncovalent interactions in the intermediate (e.g., the stacking of the electron-rich naphthalene unit with the electron-poor aryl group of the nucleophile, and the hydrogen bonding of the glycol oxygens to the H–N atoms) are reminiscent of those present in the X-ray crystal structure of rotaxane 13.
Figure 4

Tentative rationale for the transfer of chirality from Euclidean point-chirality (of the leaving group) to mechanical planar chirality (of the rotaxane). The lowest energy tetrahedral intermediates were modeled (see Supporting Information) using (a) electrophile 9 or (b) electrophile 12. The di(alkoxyl)naphthalene ring of the macrocycle and bis(trifluoromethyl)benzene unit originating from the nucleophile π-stack, causing the nitro-catechol ring to be positioned so as to cover one face of the tetrahedral center of the intermediate. This thermodynamically favored arrangement of components ensures the different handedness of the pseudoenantiomeric leaving groups is well-expressed in the diastereomeric transition states, resulting in enantioselectivity in the mechanically planar chiral rotaxane product. Hydrogen bonds are indicated by black dotted lines.

Tentative rationale for the transfer of chirality from Euclidean point-chirality (of the leaving group) to mechanical planar chirality (of the rotaxane). The lowest energy tetrahedral intermediates were modeled (see Supporting Information) using (a) electrophile 9 or (b) electrophile 12. The di(alkoxyl)naphthalene ring of the macrocycle and bis(trifluoromethyl)benzene unit originating from the nucleophile π-stack, causing the nitro-catechol ring to be positioned so as to cover one face of the tetrahedral center of the intermediate. This thermodynamically favored arrangement of components ensures the different handedness of the pseudoenantiomeric leaving groups is well-expressed in the diastereomeric transition states, resulting in enantioselectivity in the mechanically planar chiral rotaxane product. Hydrogen bonds are indicated by black dotted lines. Also consistent with the stacking of the electron-rich naphthalene unit with the electron-poor aryl group of the nucleophile providing the driving force for organization of the transition state is the experimental evidence that decreasing the electron density of the other aromatic ring of the macrocycle increases the enantioselectivity of rotaxane formation (i.e., 12% e.e. for (+)-8; 40% e.e. for (+)-11). The less electron-rich the catechol ring is, the less it competes with the naphthalene group for π-stacking with the bis(trifluoromethyl)benzylamine and so the greater the enantiodiscrimination in the transition state.

Conclusions

The examples presented demonstrate that mechanically planar chiral rotaxanes can be directly accessed in up to 50% e.e. in a single synthetic step. The chirality of the point-chiral leaving group is transferred into mechanically planar chirality in the rotaxane through metal-free active template N-acylation. Pseudoenantiomeric cinchona alkaloids allow either rotaxane enantiomer to be accessed. X-ray crystallography and molecular modeling suggest that the origin of the enantioselectivity lies in π-stacking of an electron-rich aromatic ring on the macrocycle with an electron-poor aryl group originating from the nucleophilic axle building block. This positions the second aromatic ring of the macrocycle in an orientation that blocks one face of the electrophile. Simple methods for accessing enantioenriched mechanically planar chiral rotaxanes should improve their availability for investigation in applications such as asymmetric catalysis,[7] chiral (bio)molecule sensing,[1,6,22] and novel designs[23] of molecular machinery.
  35 in total

Review 1.  On the way to rotaxane-based molecular motors: studies in molecular mobility and topological chirality.

Authors:  C A Schalley; K Beizai; F Vögtle
Journal:  Acc Chem Res       Date:  2001-06       Impact factor: 22.384

2.  A novel synthesis of chiral rotaxanes via covalent bond formation.

Authors:  Naohiro Kameta; Kazuhisa Hiratani; Yoshinobu Nagawa
Journal:  Chem Commun (Camb)       Date:  2004-01-28       Impact factor: 6.222

3.  Dynamic Control of Chiral Space Through Local Symmetry Breaking in a Rotaxane Organocatalyst.

Authors:  Marcel Dommaschk; Javier Echavarren; David A Leigh; Vanesa Marcos; Thomas A Singleton
Journal:  Angew Chem Int Ed Engl       Date:  2019-09-10       Impact factor: 15.336

4.  Synthesis of Mechanically Planar Chiral rac-[2]Rotaxanes by Partitioning of an Achiral [2]Rotaxane: Stereoinversion Induced by Shuttling.

Authors:  Yuta Mochizuki; Katsuhiko Ikeyatsu; Yuichiro Mutoh; Shoichi Hosoya; Shinichi Saito
Journal:  Org Lett       Date:  2017-08-07       Impact factor: 6.005

5.  [2]Rotaxane Formation by Transition State Stabilization.

Authors:  Guillaume De Bo; Guillaume Dolphijn; Charlie T McTernan; David A Leigh
Journal:  J Am Chem Soc       Date:  2017-06-19       Impact factor: 15.419

6.  An Artificial Molecular Shuttle Operates in Lipid Bilayers for Ion Transport.

Authors:  Sujun Chen; Yichuan Wang; Ting Nie; Chunyan Bao; Chenxi Wang; Tianyi Xu; Qiuning Lin; Da-Hui Qu; Xueqing Gong; Yi Yang; Linyong Zhu; He Tian
Journal:  J Am Chem Soc       Date:  2018-11-28       Impact factor: 15.419

Review 7.  Biomimetic Synchronized Motion of Two Interacting Macrocycles in [3]Rotaxane-Based Molecular Shuttles.

Authors:  Li-Shuo Zheng; Jie-Shun Cui; Wei Jiang
Journal:  Angew Chem Int Ed Engl       Date:  2019-09-09       Impact factor: 15.336

Review 8.  Radial Hetero[5]catenanes: Peripheral Isomer Sequences of the Interlocked Macrocycles.

Authors:  Antony Wing Hung Ng; Chi-Chung Yee; Ho Yu Au-Yeung
Journal:  Angew Chem Int Ed Engl       Date:  2019-10-17       Impact factor: 15.336

9.  Weak functional group interactions revealed through metal-free active template rotaxane synthesis.

Authors:  Chong Tian; Stephen D P Fielden; George F S Whitehead; Iñigo J Vitorica-Yrezabal; David A Leigh
Journal:  Nat Commun       Date:  2020-02-06       Impact factor: 14.919

10.  Asymmetric Catalysis with a Mechanically Point-Chiral Rotaxane.

Authors:  Yusuf Cakmak; Sundus Erbas-Cakmak; David A Leigh
Journal:  J Am Chem Soc       Date:  2016-02-04       Impact factor: 15.419

View more
  7 in total

1.  Mechanically axially chiral catenanes and noncanonical mechanically axially chiral rotaxanes.

Authors:  John R J Maynard; Peter Gallagher; David Lozano; Patrick Butler; Stephen M Goldup
Journal:  Nat Chem       Date:  2022-06-27       Impact factor: 24.274

2.  A Co-conformationally "Topologically" Chiral Catenane.

Authors:  Arnau Rodríguez-Rubio; Andrea Savoini; Florian Modicom; Patrick Butler; Stephen M Goldup
Journal:  J Am Chem Soc       Date:  2022-06-28       Impact factor: 16.383

3.  Phototriggered Complex Motion by Programmable Construction of Light-Driven Molecular Motors in Liquid Crystal Networks.

Authors:  Jiaxin Hou; Guiying Long; Wei Zhao; Guofu Zhou; Danqing Liu; Dirk J Broer; Ben L Feringa; Jiawen Chen
Journal:  J Am Chem Soc       Date:  2022-04-05       Impact factor: 16.383

Review 4.  Planar Chirality: A Mine for Catalysis and Structure Discovery.

Authors:  Rosa López; Claudio Palomo
Journal:  Angew Chem Int Ed Engl       Date:  2022-01-27       Impact factor: 16.823

5.  Transamidation-Driven Molecular Pumps.

Authors:  Lorna Binks; Chong Tian; Stephen D P Fielden; Iñigo J Vitorica-Yrezabal; David A Leigh
Journal:  J Am Chem Soc       Date:  2022-08-18       Impact factor: 16.383

6.  Diastereoselective synthesis of [1]rotaxanes via an active metal template strategy.

Authors:  Noël Pairault; Adrien Bessaguet; Romain Barat; Lucas Frédéric; Grégory Pieters; Jeanne Crassous; Isabelle Opalinski; Sébastien Papot
Journal:  Chem Sci       Date:  2020-12-29       Impact factor: 9.825

7.  Diastereoselective Amplification of a Mechanically Chiral [2]Catenane.

Authors:  Kenji Caprice; Dávid Pál; Céline Besnard; Bartomeu Galmés; Antonio Frontera; Fabien B L Cougnon
Journal:  J Am Chem Soc       Date:  2021-07-29       Impact factor: 15.419

  7 in total

北京卡尤迪生物科技股份有限公司 © 2022-2023.