Posts Tagged ‘Isomer’

Organocatalytic cyclopropanation of an enal: (computational) assignment of absolute configurations.

Saturday, September 1st, 2018

I am exploring the fascinating diverse facets of a recently published laboratory experiment for undergraduate students.[1] Previously I looked at a possible mechanistic route for the reaction between an enal (a conjugated aldehyde-alkene) and benzyl chloride catalysed by base and a chiral amine, followed by the use of NMR coupling constants to assign relative stereochemistries. Here I take a look at some chiroptical techniques which can be used to assign absolute stereochemistries (configurations).

I will focus on the compound 4a, the major stereochemical product of this student laboratory reaction, with the stereochemistry as represented in e.g. the abstract of the main article[1] and shown below with added CIP (Cahn-Ingold-Prelog) notation as (1S,2R,3R);

Its enantiomer (not shown in the article) is of course;

In the article supporting information[1]), the major diasteromer of 4a deriving from use of the S stereoisomer of the prolinol catalyst is reported as having an optical rotation (ORP) [α]D25 of -62.4°, p6 or -58.1°, p5), but the stereo-labels are not added there. On  p1 (“based on a student report”) 4a was however labelled as (1R,2S,3S) and the chirality (S) of the catalyst used was also noted in the adjacent experimental procedure. One might then reasonably match (1R,2S,3S)-4a to the S-catalyst and hence (1S,2R,3R)-4a to the R-catalyst.  However, in a laboratory environment where both S and R catalysts are in circulation, it is always useful to have procedures available for independent checks.

There are two methods of assigning absolute chirality, crystallography and chiroptical spectroscopy. The former does require crystalline samples; the latter can use solutions. To cut to the chase, the former method was used for a related compound where the n-heptyl group above is replaced by a p-chlorophenyl substituent (perhaps because the latter imparts suitable crystallinity). On p S123 of the SI of an earlier article[2] the assignment for the p-chlorophenyl derivative was as (1R,2S,3S)-4a for S-catalyst (see DOI: 10.5517/ccdc.csd.cc1mcqg5 OZAXEU). But this procedure is not entirely foolproof; the stereochemistry is decided by interactions between often bulky substituents at the transition state and it might be that here the p-chlorophenyl derivative has different properties from n-heptyl. Moreover bulk solutions may be different in their composition from single crystals. So it is useful to obtain independent proof.

An absolute assignment procedure based on chiroptical methods was first famously used by Kirkwood in 1951 (the Fischer convention is confirmed as a structurally correct representation of absolute configuration).[3] Such calculations need to take into account e.g. rotational conformers about the two bonds labelled in red above. In the previous post, I had noted variation of up to 2Hz in the calculated 3JHH coupling constants as a result of this mobility. This variation is probably too small to really influence any relative stereochemical interpretations, but is the same true for chiroptical assignments?

In Table 1 we can see whether this is still true for the predicted optical rotation of compound 4a, using two different functionals for the calculation (B3LYP and M062X respectively). The results rather surprised me; a simple bond rotation of an aryl or carbonyl group can invert the sign of the rotation. Clearly the observed optical rotation of -62.4° arises from a suitable combination of different Boltzmann populations of the individual bond rotamers, but to combine these accurately you would need to know the solution populations themselves very accurately and that is quite a challenge. So at this stage, we do not really have totally convincing independent evidence of whether the observed negative optical rotation corresponds to (1S,2R,3R)-4a or to its enantiomer (1R,2S,3S).

Table 1. Calculated Optical rotations for (1S,2R,3R)-4a. 

FAIR Data DOI: 10.14469/hpc/4678

Conformer

ORP [α]D, B3LYP+GD3BJ/Def2-TZVPP/SCRF=chloroform

ORP [α]D, M062X/Def2-TZVPP/SCRF=chloroform

4 +376 +238
3 -335 -301
2 -247 -223
1 +710 +522

Next, another chiroptical technique, electronic circular dichroism, or ECD. Here, the sign of the difference in absorption of polarized light (Δε), and known at the Cotton effect, characterises the specific enantiomer. The experimental Cotton effect for compound 4a obtained from S-catalyst (known as 3d in the SI, p S142[2]) can be simply summarised as +ve@315nm and -ve@275nm. Comparison with calculated spectra (Figure S17, p S146-7[2])  was performed using a Boltzmann-averaging (albeit based on enthalpies rather than the formally correct free energies), for three significant populations and this procedure matched to (1R,2S,3S).  Since the reported calculations were apparently for gas phase (and replacing n-heptyl with methyl) here I have repeated them in the actual solvent used (acetonitrile) and with the heptyl present. Although the ECD responses can still be severely dependent on the conformation, three of the spectra qualitatively agree that the responses at ~300nm and 260 nm are respectively -ve and +ve. This confirms that (1S,2R,3R)-4a is the wrong enantiomer for S-catalyst and that the correct assignment is therefore (1R,2S,3S), as was indeed reported.[2]

Table 2. Calculated electronic circular dichroism for

 (1S,2R,3R)-4a. FAIR Data DOI: 10.14469/hpc/4678

Conformer

ECD calculation, ωB97XD/Def2-TZVPP

4
3
2
1

It is still true that the overall the fit between chiroptical experiment and theory can be sensitive to the Boltzmann population, as obtained from e.g. ΔΔG = -RT ln [1]/[2]), where 1 and 2 are two different conformers. ΔΔG is a difficult energy difference to compute accurately. Here is a suggested exercise in the statistics of error propagation. How does an error in ΔΔG propagate to the ratio of concentrations of two conformers [1]/[2]? Or, how accurately must ΔΔG be calculated in order to predict conformer populations to say better than 5%.

One more go at chiroptics, this time Vibrational Circular Dichroism, or VCD. The nature of the chromophore is different, but the principle is the same as ECD. I have deliberately truncated the spectrum to cut off all vibrations below 1000 cm-1 (these being the modes associated with group rotations) but to no avail, the four conformations all still look too different to avoid doing a Boltzmann averaging.

Table 3. Calculated VCD spectra for (1S,2R,3R)-4a. 

Conformer Spectrum
4
3
2
1

A modern VCD instrument does have one trick up its sleeve for coping with the conformer problem. The sample (as a thin-film) can be annealed down to very low temperatures before the spectrum is recorded. This effectively removes all higher energy forms, leaving just the most stable conformation as the only species present. However, that is an expensive experiment (and instrument!) to use.

There are perhaps some 2 million scalemic molecules (substances where one chiral form is in excess over the mirror image) for which chiroptical properties have been reported, but probably <50,000 crystal structures where absolute configurations have been assigned. Thus the vast majority of absolute configuration assignments have been done either chiroptically or by synthetic correlations (chemical transformations from molecules of known absolute configuration, with the assumption that you know how each transformation affects the chiral centres present). Given some of the difficulties and challenges noted above, it is tempting to conclude that a significant proportion of those 2 million molecules may have been mis-assigned (I once estimated up to 20%). However, we may conclude that the molecules discussed here are safely assigned correctly! 


No CIP-stereolabels appear in the article itself.[1] Perhaps this assignment is omitted in order to provide a student exercise? There are many errors in stereochemical assignments in the literature. A good many of them may be the result of simple sample mis-labelling.[4] The caption to Figure S17 states All the simulations are for the 1R,2R,3S absolute configuration. This is probably an error and should read 1R,2S,3SA correction of ~+15nm is sometimes applied to these values, but not done here.

 

References

  1. M. Meazza, A. Kowalczuk, S. Watkins, S. Holland, T.A. Logothetis, and R. Rios, "Organocatalytic Cyclopropanation of (<i>E</i>)-Dec-2-enal: Synthesis, Spectral Analysis and Mechanistic Understanding", Journal of Chemical Education, vol. 95, pp. 1832-1839, 2018. https://doi.org/10.1021/acs.jchemed.7b00566
  2. M. Meazza, M. Ashe, H.Y. Shin, H.S. Yang, A. Mazzanti, J.W. Yang, and R. Rios, "Enantioselective Organocatalytic Cyclopropanation of Enals Using Benzyl Chlorides", The Journal of Organic Chemistry, vol. 81, pp. 3488-3500, 2016. https://doi.org/10.1021/acs.joc.5b02801
  3. W.W. Wood, W. Fickett, and J.G. Kirkwood, "The Absolute Configuration of Optically Active Molecules", The Journal of Chemical Physics, vol. 20, pp. 561-568, 1952. https://doi.org/10.1063/1.1700491
  4. H.S. Rzepa, "The Chiro-optical Properties of a Lemniscular Octaphyrin", Organic Letters, vol. 11, 2009. https://doi.org/10.1021/ol901172g

Bond stretch isomerism. Did this idea first surface 100 years ago?

Tuesday, February 9th, 2016

The phenomenon of bond stretch isomerism, two isomers of a compound differing predominantly in just one bond length, is one of those chemical concepts that wax and occasionally wane.[1] Here I explore such isomerism for the elements Ge, Sn and Pb.

In one earlier post, I noted a form of bond stretch isomerism that can arise from a Jahn-Teller distortion ending in two different geometries in which one or more pairs of bonds swap short/long lengths. Examples include substituted cyclo-octatetraenes[2] and octahedral d9-Cu(II) complexes.[3] A more interesting seminal possibility was implied by G. N. Lewis a century ago when discussing the arrangement of electrons in a (carbon-carbon) triple bond.[4]

lewis1
*It took ~50 years to prove this assertion wrong.[5]

In a commentary, I reported the results of a search of the crystal structure database for the geometries associated with RX≡XR systems (X= C, Si, Ge, Sn, Pb). Here I focus the search[6] specifically for X=Sn,Ge; this version of bond stretch isomerism also allows angles to change (= rehybridisation at atoms) in order to provide a mechanism for a barrier separating the two forms.

For X=Sn, note the presence of up to three clusters, although the relatively low number of hits makes the statistics less certain.

  1. The hotspot cluster centered around angles of 125° and a Sn-Sn distance of ~2.6Å.
  2. Another with angles of <100° and Sn-Sn distances of ~3.3Å.
  3. A third with angles of <100° and Sn-Sn distances of 2.8Å, which may or may not be a genuine unique form of bonding.

This pattern was commented on in 2010 by Power[7], whose group synthesized most of the examples in the hits above. A plot of compounds with Ge-Ge bonds reveals both similarity with (two, possibly three clusters) and difference from (the clusters are closely spaced in terms of the Ge-Ge bond length, but separated in terms of angle) Sn.

GeGe

Time for some computations (which at least will remove random errors in the geometry). I selected the only known example of an RPb-PbR compound[8] as a seed and put it through a B3LYP+D3/Def2-TZVPP calculation (with 172 atoms and 2920 basis functions, this is a relatively large calculation!), which reproduces the known structure pretty well (table).

QIMQUY

So what about another bond stretch isomers? The Pb=Pb variation is indeed a stable minimum around 28.0 kcal/mol above the known structure, which seems to put this form out of experimental reach (with this ligand/aryl group at least). With Sn for the same aryl ligand, the energy difference is smaller (~15.8 kcal/mol for this ligand; Powers reports other systems where the energy difference may be only ~5 kcal/mol). Judging by the distribution of the 13 hits recovered from the CSD search, both bond stretch isomers may be accessible experimentally. The calculations show that the GeGe bond isomers are much closer in energy than SnSn (for this ligand). For all three metals however, the calculated difference in the metal-metal length for the two isomers is ~0.45 – 0.52Å. This strongly suggests that whereas the SnSn plot above is demonstrating bond length isomerism, the GeGe plot may not be; at least not of the same type that the calculations here are revealing (via the Wiberg bond orders).

System Relative energy XX distance RXX angle Wiberg bond order DataDOI
Pb=Pb +28.0 2.767 118.7 1.666 [9]
Pb-Pb 0.0 3.215 (3.188)[8] 93.7 (94.3)[8] 0.889 [10]
Sn=Sn +15.8 2.640 123.1 1.911 [11]
Sn-Sn 0.0 3.126 95.5 0.892 [12]
Ge=Ge +0.5 2.263 125.2 2.138 [13]
Ge-Ge 0.0   2.777 99.7 0.866 [14]

No doubt the particular bond length form is being facilitated by the nature of the ligand and the steric interactions therein imparted, both repulsive AND attractive. These interactions can be visualised via NCI (non-covalent-interaction) plots (click on the image to obtain a rotatable 3D model). First Pb-Pb followed by Pb=Pb. Note how in both cases, the PbPb region is enclosed in regions of weak attractive dispersion interactions, which however avoid the "hemidirected" inert Pb lone pairs.[15]

Pb-Pb Pb=Pb

So in the end we have something of a mystery. There is evidence from crystal structures that at least two bond-stretch isomers of RSnSnR compounds can form, but the calculations indicate that the Sn=Sn form is significantly higher in energy (although not impossibly so for thermal accessibility). Conversely, the Ge=Ge equivalent is very similar in energy to a Ge-Ge form with a significantly longer bond length, but there seems no crystallographic evidence for such a big difference in bond lengths. Perhaps the answer lies with the ligands?

It seems particularly appropriate on the centenary of G. N. Lewis' famous paper in which he clearly notes the possibility of three isomeric forms for the triple bond, to pay tribute to the impact his suggestions continue to make to chemistry.


The individual entries can be inspected via the following dois: [16],[17],[18],[19],[20],[21],[22],[23],[24],[25]

You can view individual entries via the following DOIs: [26],[27],[28],[29],[30],[31],[32],[33],[34],[35]

References

  1. J.A. Labinger, "Bond-stretch isomerism: a case study of a quiet controversy", Comptes Rendus. Chimie, vol. 5, pp. 235-244, 2002. https://doi.org/10.1016/s1631-0748(02)01380-2
  2. J.E. Anderson, and P.A. Kirsch, "Structural equilibria determined by attractive steric interactions. 1,6-Dialkylcyclooctatetraenes and their bond-shift and ring inversion investigated by dynamic NMR spectroscopy and molecular mechanics calculations", Journal of the Chemical Society, Perkin Transactions 2, pp. 1951, 1992. https://doi.org/10.1039/p29920001951
  3. W. Zhang, L. Chen, R. Xiong, T. Nakamura, and S.D. Huang, "New Ferroelectrics Based on Divalent Metal Ion Alum", Journal of the American Chemical Society, vol. 131, pp. 12544-12545, 2009. https://doi.org/10.1021/ja905399x
  4. G.N. Lewis, "THE ATOM AND THE MOLECULE.", Journal of the American Chemical Society, vol. 38, pp. 762-785, 1916. https://doi.org/10.1021/ja02261a002
  5. F.A. Cotton, "Metal-Metal Bonding in [Re<sub>2</sub>X<sub>8</sub>]<sup>2-</sup> Ions and Other Metal Atom Clusters", Inorganic Chemistry, vol. 4, pp. 334-336, 1965. https://doi.org/10.1021/ic50025a016
  6. H. Rzepa, "Crystal structures containing Sn...Sn bonds", 2016. https://doi.org/10.14469/hpc/249
  7. Y. Peng, R.C. Fischer, W.A. Merrill, J. Fischer, L. Pu, B.D. Ellis, J.C. Fettinger, R.H. Herber, and P.P. Power, "Substituent effects in ditetrel alkyne analogues: multiple vs. single bonded isomers", Chemical Science, vol. 1, pp. 461, 2010. https://doi.org/10.1039/c0sc00240b
  8. L. Pu, B. Twamley, and P.P. Power, "Synthesis and Characterization of 2,6-Trip<sub>2</sub>H<sub>3</sub>C<sub>6</sub>PbPbC<sub>6</sub>H<sub>3</sub>-2,6-Trip<sub>2</sub> (Trip = C<sub>6</sub>H<sub>2</sub>-2,4,6-<i>i</i>-Pr<sub>3</sub>):  A Stable Heavier Group 14 Element Analogue of an Alkyne", Journal of the American Chemical Society, vol. 122, pp. 3524-3525, 2000. https://doi.org/10.1021/ja993346m
  9. H.S. Rzepa, "C 72 H 98 Pb 2", 2016. https://doi.org/10.14469/ch/191856
  10. H.S. Rzepa, "C 72 H 98 Pb 2", 2016. https://doi.org/10.14469/ch/191873
  11. https://doi.org/
  12. H.S. Rzepa, "C 72 H 98 Sn 2", 2016. https://doi.org/10.14469/ch/191881
  13. H.S. Rzepa, "C 72 H 98 Ge 2", 2016. https://doi.org/10.14469/ch/191882
  14. H.S. Rzepa, "C 72 H 98 Ge 2", 2016. https://doi.org/10.14469/ch/191883
  15. M. Imran, A. Mix, B. Neumann, H. Stammler, U. Monkowius, P. Gründlinger, and N.W. Mitzel, "Hemi- and holo-directed lead(<scp>ii</scp>) complexes in a soft ligand environment", Dalton Transactions, vol. 44, pp. 924-937, 2015. https://doi.org/10.1039/c4dt01406e
  16. Jones, C.., Sidiropoulos, A.., Holzmann, N.., Frenking, G.., and Stasch, A.., "CCDC 892557: Experimental Crystal Structure Determination", 2012. https://doi.org/10.5517/ccyys5t
  17. Phillips, A.D.., Wright, R.J.., Olmstead, M.M.., and Power, P.P.., "CCDC 187521: Experimental Crystal Structure Determination", 2002. https://doi.org/10.5517/cc6942p
  18. Peng, Yang., Fischer, R.C.., Merrill, W.A.., Fischer, J.., Pu, Lihung., Ellis, B.D.., Fettinger, J.C.., Herber, R.H.., and Power, P.P.., "CCDC 771267: Experimental Crystal Structure Determination", 2010. https://doi.org/10.5517/cctwklt
  19. Peng, Yang., Fischer, R.C.., Merrill, W.A.., Fischer, J.., Pu, Lihung., Ellis, B.D.., Fettinger, J.C.., Herber, R.H.., and Power, P.P.., "CCDC 771268: Experimental Crystal Structure Determination", 2010. https://doi.org/10.5517/cctwkmv
  20. Peng, Yang., Fischer, R.C.., Merrill, W.A.., Fischer, J.., Pu, Lihung., Ellis, B.D.., Fettinger, J.C.., Herber, R.H.., and Power, P.P.., "CCDC 771270: Experimental Crystal Structure Determination", 2010. https://doi.org/10.5517/cctwkpx
  21. Peng, Yang., Fischer, R.C.., Merrill, W.A.., Fischer, J.., Pu, Lihung., Ellis, B.D.., Fettinger, J.C.., Herber, R.H.., and Power, P.P.., "CCDC 771271: Experimental Crystal Structure Determination", 2010. https://doi.org/10.5517/cctwkqy
  22. Peng, Yang., Fischer, R.C.., Merrill, W.A.., Fischer, J.., Pu, Lihung., Ellis, B.D.., Fettinger, J.C.., Herber, R.H.., and Power, P.P.., "CCDC 771272: Experimental Crystal Structure Determination", 2010. https://doi.org/10.5517/cctwkrz
  23. Peng, Yang., Fischer, R.C.., Merrill, W.A.., Fischer, J.., Pu, Lihung., Ellis, B.D.., Fettinger, J.C.., Herber, R.H.., and Power, P.P.., "CCDC 771274: Experimental Crystal Structure Determination", 2010. https://doi.org/10.5517/cctwkt1
  24. Fischer, R.C.., Pu, Lihung., Fettinger, J.C.., Brynda, M.A.., and Power, P.P.., "CCDC 624216: Experimental Crystal Structure Determination", 2007. https://doi.org/10.5517/ccnyk04
  25. Pu, Lihung., Phillips, A.D.., Richards, A.F.., Stender, M.., Simons, R.S.., Olmstead, M.M.., and Power, P.P.., "CCDC 221953: Experimental Crystal Structure Determination", 2004. https://doi.org/10.5517/cc7fysc
  26. Sasamori, Takahiro., Sugahara, Tomohiro., Agou, Tomohiro., Guo, Jing-Dong., Nagase, Shigeru., Streubel, Rainer., and Tokitoh, Norihiro., "CCDC 1035078: Experimental Crystal Structure Determination", 2014. https://doi.org/10.5517/cc13r2mk
  27. Sidiropoulos, A.., Jones, C.., Stasch, A.., Klein, S.., and Frenking, G.., "CCDC 749451: Experimental Crystal Structure Determination", 2010. https://doi.org/10.5517/cct4vvm
  28. Shan, Yu-Liang., Yim, Wai-Leung., and So, Cheuk-Wai., "CCDC 1019495: Experimental Crystal Structure Determination", 2015. https://doi.org/10.5517/cc136vy3
  29. Sugiyama, Y.., Sasamori, T.., Hosoi, Y.., Furukawa, Y.., Takagi, N.., Nagase, S.., and Tokitoh, N.., "CCDC 297827: Experimental Crystal Structure Determination", 2006. https://doi.org/10.5517/cc9zxbh
  30. Stender, M.., Phillips, A.D.., Wright, R.J.., and Power, P.P.., "CCDC 180660: Experimental Crystal Structure Determination", 2002. https://doi.org/10.5517/cc61zry
  31. Peng, Yang., Fischer, R.C.., Merrill, W.A.., Fischer, J.., Pu, Lihung., Ellis, B.D.., Fettinger, J.C.., Herber, R.H.., and Power, P.P.., "CCDC 771273: Experimental Crystal Structure Determination", 2010. https://doi.org/10.5517/cctwks0
  32. Peng, Yang., Fischer, R.C.., Merrill, W.A.., Fischer, J.., Pu, Lihung., Ellis, B.D.., Fettinger, J.C.., Herber, R.H.., and Power, P.P.., "CCDC 771269: Experimental Crystal Structure Determination", 2010. https://doi.org/10.5517/cctwknw
  33. Peng, Yang., Fischer, R.C.., Merrill, W.A.., Fischer, J.., Pu, Lihung., Ellis, B.D.., Fettinger, J.C.., Herber, R.H.., and Power, P.P.., "CCDC 771266: Experimental Crystal Structure Determination", 2010. https://doi.org/10.5517/cctwkks
  34. Jones, C.., Sidiropoulos, A.., Holzmann, N.., Frenking, G.., and Stasch, A.., "CCDC 892556: Experimental Crystal Structure Determination", 2012. https://doi.org/10.5517/ccyys4s
  35. Jones, C.., Sidiropoulos, A.., Holzmann, N.., Frenking, G.., and Stasch, A.., "CCDC 892555: Experimental Crystal Structure Determination", 2012. https://doi.org/10.5517/ccyys3r