Chapter 7. Conclusions.

7.1. Summary

One goal of our research is determine what are the conformations and configurations of the tetrahedral intermediates in carnitine acyl transfers. So far, the approach has been experimental, by designing conformationally constrained analogues of the tetrahedral intermediates. To make the approach cost-effective, we need reliable modeling methods to guide the choice of the next generation of inhibitors. The modeling methods developed in this dissertation fulfill that need for the most part.

This dissertation addressed two additional questions:

Acetylcarnitine reaches its high energy of hydrolysis by drawing from the solvation energy. The coupling between solvation energy, dipole moment and conformational change, supplies the necessary energy from the solvation term to yield a free energy of hydrolysis that compares to that of AcCoA. The high-energy status of acylcarnitine makes possible an exchange equilibrium with CoA (Keq = 0.6), that minimizes the energy consumed by processes other than the transport through the cell membrane.

From the preliminary results for the modeling of the tetrahedral intermediate, [shown in the table in chapter 3,] we see the RMS fits of the dioxazaphosphacinium rings to the intermediate. The most promising candidates are both boat-boat conformers that correspond to the R,S diastereomer of the tetrahedral intermediate. The cis-substituted ring and the dimethyl-substituted ring yield the closest fit to the R,S tetrahedral intermediate. These fits should be considered as one parameter in a quantitative structure-activity relationship for the inhibitory potency of the inhibitors already developed by our group. This will help in the prediction of the next generation of inhibitors. The morpholinium rings should receive a similar treatment.

7.2. Future work.

Based on the results obtained from the acetylcarnitine hydrolysis, the aqueous modeling of the heterocycles including a methylenecarboxylate should pay attention to the influence of the dipole moments. In the dioxazaphosphacinium rings, there will be two sources of polarity: the dipoles due to the C-O-P=O torsions, and the dipole due to the zwitterion. How will the conformational preference of the rings be affected by the presence of the zwitterion?. Answering such question will require careful attention to the charge set used in the calculation. It may be desirable to determine a new charge set for the methylenecarboxylate-substituted ring, at the HF/6-31+G* level of theory using the CHelpG scheme, to ensure that the charge set found in this dissertation is still applicable (see the file BondPC.txt for the output from the CHelpG calculation). After all, changing from a cation to a neutral species will likely affect the charge distribution in the molecule. In addition, unless newer versions of MacroModel provide utilities for the calculation of the dipole moment, it will be necessary to supplement the MacroModel results with some other modeling package. Single-point calculations on the AMBER*-optimized geometries, using the AM1 Hamiltonian in MOPAC93, would provide an appropriate starting point.


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