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Peptide-Based Drug Design

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100 Westermann and Craik<br />

times and can change from positive, to zero, to negative values depending on<br />

the size of the peptide being studied. The correlation time at which a molecule<br />

displays negative NOEs depends on the temperature and the field strength of the<br />

spectrometer used. As a guideline, peptides around 1 kDa display only weak or<br />

no NOEs on a 500 MHz spectrometer, and ROESY experiments (60) may be<br />

necessary for peptides of this size. Notwithstanding this complication, NOEs are<br />

extremely useful.<br />

4.4.1. Transferred NOE<br />

In this method the different correlation times and NOE build-up rates of free<br />

and bound states of a ligand are used to detect NOEs on the free ligand that<br />

reflect its bound conformation. This class of experiment usually is conducted by<br />

performing transient NOE experiments by means of 2D NOESY spectra. The<br />

basis of the technique is that small molecules show positive NOEs while macromolecules<br />

show negative NOEs and that NOEs build up/decay quickly in macromolecules<br />

but slowly in small molecules. Upon binding of a small molecule to<br />

a macromolecule, the motional characteristics of the small molecule change and<br />

it shows negative NOEs. After dissociation from the complex, information on<br />

the negative NOE is transferred back to the free ligand, which is usually in large<br />

excess and readily detectable (12).<br />

Besides intramolecular transferred NOEs, intermolecular transferred NOEs<br />

are of interest when studying molecular interactions (61,62). In this case NOEs<br />

build up between protons of the ligand during its residence time in the binding<br />

pocket. This gives information on the orientation and conformation of the ligand<br />

in the binding site. The transferred NOE approach for structural characterisation<br />

of the bound conformation of a ligand is schematically illustrated in Fig. 8<br />

Fig. 8. Schematic representation of the trNOE effect. On the left the conformation of<br />

the unbound ligand does not allow the buildup of a NOE because the two protons are too<br />

far away. In the middle representation the bound conformation orients the two protons at<br />

a distance that allows the buildup of a NOE. After dissociation of the complex the information<br />

of spatial proximity of the two protons in the bound conformation is transferred<br />

back into the solution conformation (right), where the NOE still is observable.

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