Posts Tagged ‘calixarene’

Computational “reality checks” for mechanistic speculations.

Thursday, September 1st, 2011

I have mentioned Lewis a number of times in these posts; his suggestion of the shared electron covalent bond still underpins much chemical thinking. Take for example mechanistic speculations on the course of a reaction, a very common indulgence in almost all articles reporting such, and largely based on informed  arrow pushing. This process is bound to follow the rules of reasonable Lewis structures for any putative intermediates. Here, I suggest that we are now firmly in an era where such speculations must of necessity be backed up by quantum mechanical estimates of the energies and structures. I would propose that journals routinely encourage referees to insist on such (additional) checks. Let me give one specific example of the need to do this (part of a follow up to an earlier article I blogged on previously).

Scheme 1 (reproduced from 10.1002/chem.201100693 )

The example is found as scheme 1 of an article written by Legrand, Gilles, Petit, van der Lee and Barboiu entitled “Unprecedented Synthesis of 1,3-Dimethylcyclobutadiene in the Solid State and Aqueous Solution” (DOI: 10.1002/chem.201100693;  Scheme 1 reproduced here  with the permission of the publishers). Structures 1 – 3 are my additions, and are not present in scheme 1 of the above article.

Possible species involved in the mechanism for photochemical irradiation of dimethyl pyrone.

The scientific problem is to identify what the products are of photolysis of Me21. The species is contained as a guest inside a calixarene host, the whole assembly being dissolved in water (D2O). This was photolysed and the products characterised by (inter alia) their 1H NMR spectra, Figure 7. Focus in particular on 7b, which shows a set of five spectra that are claimed to identify the consecutive species Me21, Me22, (Me23 or 1), Me2CBDS/CO2, Me2CBDR and Me24 as the outcomes of photolysis at “different irradiation times at l=320–500 nm or at l=190–500 nm“.

Figure 7 (taken from 10.1002/chem.201100693, reproduced with permission of publisher )

How might one apply a computational reality check to this scheme? Lewis himself might have ventured to suggest that representation Me23 does not adhere to his rules; a modern chemistry student would draw it instead as 2, a vinyl zwitterion. This species in turn could either eliminate carbon monoxide (red arrow) or ring close to give the unusual ylid 3 (blue arrow). In fact DFT calculations on the isolated molecules in water (ωB97XD/6-311G(d,p)/SCRF=water) indicate that the C-O bond in an isolated molecule of Me2does not persist and fragments to carbon monoxide and an alkoxy zwitterion, making it around ~36.5 kcal/mol higher in free energy than the alternative zwitterion 1. The third species 3 is somewhat more stable, being ~20 kcal/mol above 1. Calculations also reveal that whilst rectangular Me2CBDR is obtained on the singlet surface, the square Me2CBDS/CO2 can only be obtained on the triplet surface. This state however is ~8-10 kcal/mol higher in energy and unlikely to have a long lifetime before it decays down to the singlet surface. One could study all the species in the scheme above in this manner, but that analysis is for another place and time.

Until relatively recently, such reality checks would be all one might attempt computationally. But these experiments were NOT conducted on isolated molecules in solution, they were done in the presence of a calixarene host. Could that change things? Zwitterion 1 can be placed inside this cavity and the calculation repeated (again simulating solvent water), as can 2. In fact the latter spontaneously collapses to 3, and now has an energy ~ 27 kcal/mol higher than 1. Whether 1 itself (or indeed Me2CBDR) has any persistent lifetime is another issue, and one not addressed in this blog post.

In fact, the reality check has another purpose, which is to stimulate other ideas. In this case for example one could regard 3 as a carbene, in which case one might ask if coordination of the carbene to a suitable metal might be a stabilizing mode. Amazingly, a number of such systems are known! I show just one below.

SCHXFe structure diagram.


SCHXFe. Click for 3D structure.

There is a lot more that could be said (and written) about this article, including discussion of the 1H NMR spectra, but I will stop at this point. Hopefully, I have shown how simple computational reality checks on a proposed mechanism can easily result in both unexpected outcomes and ideas for new chemistry!

Computational "reality checks" for mechanistic speculations.

Thursday, September 1st, 2011

I have mentioned Lewis a number of times in these posts; his suggestion of the shared electron covalent bond still underpins much chemical thinking. Take for example mechanistic speculations on the course of a reaction, a very common indulgence in almost all articles reporting such, and largely based on informed  arrow pushing. This process is bound to follow the rules of reasonable Lewis structures for any putative intermediates. Here, I suggest that we are now firmly in an era where such speculations must of necessity be backed up by quantum mechanical estimates of the energies and structures. I would propose that journals routinely encourage referees to insist on such (additional) checks. Let me give one specific example of the need to do this (part of a follow up to an earlier article I blogged on previously).

Scheme 1 (reproduced from 10.1002/chem.201100693 )

The example is found as scheme 1 of an article written by Legrand, Gilles, Petit, van der Lee and Barboiu entitled “Unprecedented Synthesis of 1,3-Dimethylcyclobutadiene in the Solid State and Aqueous Solution” (DOI: 10.1002/chem.201100693;  Scheme 1 reproduced here  with the permission of the publishers). Structures 1 – 3 are my additions, and are not present in scheme 1 of the above article.

Possible species involved in the mechanism for photochemical irradiation of dimethyl pyrone.

The scientific problem is to identify what the products are of photolysis of Me21. The species is contained as a guest inside a calixarene host, the whole assembly being dissolved in water (D2O). This was photolysed and the products characterised by (inter alia) their 1H NMR spectra, Figure 7. Focus in particular on 7b, which shows a set of five spectra that are claimed to identify the consecutive species Me21, Me22, (Me23 or 1), Me2CBDS/CO2, Me2CBDR and Me24 as the outcomes of photolysis at “different irradiation times at l=320–500 nm or at l=190–500 nm“.

Figure 7 (taken from 10.1002/chem.201100693, reproduced with permission of publisher )

How might one apply a computational reality check to this scheme? Lewis himself might have ventured to suggest that representation Me23 does not adhere to his rules; a modern chemistry student would draw it instead as 2, a vinyl zwitterion. This species in turn could either eliminate carbon monoxide (red arrow) or ring close to give the unusual ylid 3 (blue arrow). In fact DFT calculations on the isolated molecules in water (ωB97XD/6-311G(d,p)/SCRF=water) indicate that the C-O bond in an isolated molecule of Me2does not persist and fragments to carbon monoxide and an alkoxy zwitterion, making it around ~36.5 kcal/mol higher in free energy than the alternative zwitterion 1. The third species 3 is somewhat more stable, being ~20 kcal/mol above 1. Calculations also reveal that whilst rectangular Me2CBDR is obtained on the singlet surface, the square Me2CBDS/CO2 can only be obtained on the triplet surface. This state however is ~8-10 kcal/mol higher in energy and unlikely to have a long lifetime before it decays down to the singlet surface. One could study all the species in the scheme above in this manner, but that analysis is for another place and time.

Until relatively recently, such reality checks would be all one might attempt computationally. But these experiments were NOT conducted on isolated molecules in solution, they were done in the presence of a calixarene host. Could that change things? Zwitterion 1 can be placed inside this cavity and the calculation repeated (again simulating solvent water), as can 2. In fact the latter spontaneously collapses to 3, and now has an energy ~ 27 kcal/mol higher than 1. Whether 1 itself (or indeed Me2CBDR) has any persistent lifetime is another issue, and one not addressed in this blog post.

In fact, the reality check has another purpose, which is to stimulate other ideas. In this case for example one could regard 3 as a carbene, in which case one might ask if coordination of the carbene to a suitable metal might be a stabilizing mode. Amazingly, a number of such systems are known! I show just one below.

SCHXFe structure diagram.


SCHXFe. Click for 3D structure.

There is a lot more that could be said (and written) about this article, including discussion of the 1H NMR spectra, but I will stop at this point. Hopefully, I have shown how simple computational reality checks on a proposed mechanism can easily result in both unexpected outcomes and ideas for new chemistry!

Do electrons prefer to move in packs of 4, 6 or 8 during proton exchange in a calixarene?

Friday, January 7th, 2011

This story starts with a calixarene, a molecule (suitably adorned with substituents) frequently used as a host to entrap a guest and perchance make the guest do something interesting. Such a calixarene was at the heart of a recent story where an attempt was made to induce it to capture cyclobutadiene in its cavity.

The basic skeleton of a calixarene

At the base of the calixarene are four hydroxyl groups, arranged in either a left or right handed manner. The molecule, in other words is chiral (C4 symmetry to be precise). As a chiral molecule, it might trap left and right-handed guests in a slightly different manner (forming two possible diastereomeric host-guest complexes).  As it happens, the guest in the cyclobutadiene story was just such a chiral molecule. But an essential question to ask is what the barrier to enantiomerization of such a calixarene might be?  One can envisage several ways of accomplishing such a conversion.

Enantiomerization pathways for a chiral calixarene

All four hydrogens can be moved in a single step, one might move two at a time in two steps, or one might move one at a time in four steps. These processes would involve respectively 8, 6 or 4 electrons in each step. There is a fundamental difference between the first pathway and the last two;  the latter involve  ionic intermediates (zwitterions) whereas the first is neutral. As such one might imagine the process would depend on the ability of the solvent to stabilize any such zwitterion.

Let us start with a gas phase model (ωB97XD/6-311G(d,p)), and a transition state with one negative force constant is indeed found with  C4v symmetry. The free energy barrier ΔG for the process is 14.0 kcal/mol, which means the reaction will occur rapidly, even at lower temperatures of  ~200K. A pack size of 8 seems preferred for this model. This is hardly a surprise since the formation of ionic intermediates would not be expected. One might however speculate thus. In the schematic above, n=1 and one might be tempted to ask if higher values of n (lets say  n=2, a pack size of 10, or n=3, a pack size of 12, etc ) might exhibit similar behaviour. Is there any limit to the ring/pack size for this type of proton exchange?

Transition state for enantiomerization of a calixarene in the gas phase. Click for 3D.

What about in solution? Well, let us apply the mildest of solvents, benzene as a so-called continuum field. This has a very low dielectric (2.3) and you might imagine it would have hardly any effect. Well click on the below. The C4v geometry now has three computed negative force constants; the two additional ones are shown below (they are degenerate with a wavenumber of 101i cm-1).

C4v symmetric geometry for calixarene in benzene solvent, with three negative force constants. Click for animation of E mode.

C4v geometry for calixarene in benzene. Click for animation of second E mode.

Each of these additional two negative force constants shows a displacement heading towards the zwitterion shown in the scheme below. As one increases the polarity of the solvent, so the force constant becomes more negative. Thus for dichloromethane, it is now 322i cm-1 and with water it is 376i cm-1

So now the question is what happens when either of the two additional negative force constants is followed downhill? Will it form a true zwitterion (which would have Cs symmetry), in which case it would be (two) 6 electron processes to enantiomerize the calixarene instead of one 8 electron one.

True transition state for proton exchange in solution phase calixarene

In fact this geometry of Cs symmetry, which does resemble the zwitterion shown in the scheme above, is NOT a minimum but a true transition state itself (the free energy barrier hardly changed from the value for the gas phase). So the answer seems to be that a calixarene enantiomerizes via transition state not of C4v but of Cs symmetry, and which resembles a zwitterion but is not actually one. The 8-packof electrons was tempted to take a short rest-break on their way to shifting the four protons, but in the end did it in a single journey! So we have an unusual zwitterionic but nevertheless concerted transition state for the process.

Still unresolved is whether such cyclic transfer of four protons between four oxygen atoms continues to be concerted for larger rings, or whether the system is finally tempted to break up the transfer by resting with one or more discrete intermediates along the way. I finally note that in the calixarene reported which catalysed the thoughts above, the four oxygens are capped with a guanidinium cation sitting just above them, and this too may have an interesting effect on the proton transfer process.