In the previous post, I showed how modelling of unbranched alkenes depended on dispersion forces. When these are included, a bent (single-hairpin) form of C58H118 becomes lower in free energy than the fully extended linear form. Here I try to optimise these dispersion forces by adding further folds to see what happens.
Posts Tagged ‘energy’
What is the best way of folding a straight chain alkane?
Sunday, April 6th, 2014Modelling the geometry of unbranched alkanes.
Saturday, March 29th, 2014By about C17H36, the geometry of “cold-isolated” unbranched saturated alkenes is supposed not to contain any fully anti-periplanar conformations. [cite]10.1002/anie.201202894[/cite] Indeed, a (co-crystal) of C16H34 shows it to have two-gauche bends.[cite]10.1002/chem.200801428[/cite]. Surprisingly, the longest linear alkane I was able to find a crystal structure for, C28H58 appears to be fully extended[cite]10.1107/S0108768191011059[/cite],[cite]10.1107/S0567740876005025[/cite] (an early report of a low quality structure for C36H74[cite]10.1107/S0365110X5600111X[/cite] also appears to show it as linear).‡ Here I explore how standard DFT theories cope with these structures.
Patterns of behaviour: serendipity in action for enantiomerisation of F-S-S-Cl
Thursday, September 19th, 2013Paul Schleyer sent me an email about a pattern he had spotted, between my post on F3SSF and some work he and Michael Mauksch had done 13 years ago with the intriguing title “Demonstration of Chiral Enantiomerization in a Four-Atom Molecule“.[cite]http://doi.org/d8g2nw[/cite] Let me explain the connection, but also to follow-up further on what I discovered in that post and how a new connection evolved.
Molecule-sized pixels.
Sunday, August 11th, 2013The ultimate reduction in size for an engineer is to a single molecule. It’s been done for a car; now it has been reported for the pixel (picture-element).[cite]10.1021/ja404256s[/cite]
Woodward’s symmetry considerations applied to electrocyclic reactions.
Monday, May 20th, 2013Sometimes the originators of seminal theories in chemistry write a personal and anecdotal account of their work. Niels Bohr[cite]10.1007/BF01326955[/cite] was one such and four decades later Robert Woodward wrote “The conservation of orbital symmetry” (Chem. Soc. Special Publications (Aromaticity), 1967, 21, 217-249; it is not online and so no doi can be given). Much interesting chemistry is described there, but (like Bohr in his article), Woodward lists no citations at the end, merely giving attributions by name. Thus the following chemistry (p 236 of this article) is attributed to a Professor Fonken, and goes as follows (excluding the structure in red):
Why diphenyl peroxide does not exist.
Monday, April 29th, 2013A few posts back, I explored the “benzidine rearrangement” of diphenyl hydrazine. This reaction requires diprotonation to proceed readily, but we then discovered that replacing one NH by an O as in N,O-diphenyl hydroxylamine required only monoprotonation to undergo an equivalent facile rearrangement. So replacing both NHs by O to form diphenyl peroxide (Ph-O-O-Ph) completes this homologous series. I had speculated that PhNHOPh might exist if all traces of catalytic acid were removed, but could the same be done to PhOOPh? Not if it continues the trend and requires no prior protonation at all!
How to predict the regioselectivity of epoxide ring opening.
Sunday, April 28th, 2013I recently got an email from a student asking about the best way of rationalising epoxide ring opening using some form of molecule orbitals. This reminded me of the famous experiment involving propene epoxide.[cite]10.1021/ja01208a047[/cite]