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Principles of Fluorescence Spectroscopy

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304 QUENCHING OF FLUORESCENCE<br />

Figure 8.42. Stern-Volmer plots for the iodide quenching <strong>of</strong> E. coli tet<br />

repressor (wild type, WT) and its mutants (W75F and W43F). Revised<br />

from [108].<br />

quenching <strong>of</strong> the wild-type protein is intermediate between<br />

the two single-tryptophan mutants. These results are consistent<br />

with those obtained from the quenching-resolved emission<br />

spectra. While the same information is available from<br />

the mutant proteins, the use <strong>of</strong> quenching provided the<br />

resolved spectra using only the wild-type protein.<br />

It is valuable to notice a difference in the method <strong>of</strong><br />

data analysis for the modified Stern-Volmer plots (Section<br />

Figure 8.43. Emission spectra <strong>of</strong> a four α-helix bundle in water in the<br />

presence <strong>of</strong> halothane. Each peptide chain contains one tryptophan<br />

residue. Revised from [114].<br />

8.8.1) and for the quenching-resolved emission spectra. In<br />

a modified Stern-Volmer plot one assumes that a fraction <strong>of</strong><br />

the fluorescence is totally inaccessible to quenchers. This<br />

may not be completely true because one component can be<br />

more weakly quenched, but still quenched to some extent.<br />

If possible, it is preferable to analyze the Stern-Volmer plots<br />

by nonlinear least squares, when the f i and K i values are<br />

variable. This approach allows each component to contribute<br />

to the data according to its fractional accessibility,<br />

instead <strong>of</strong> forcing one to be an inaccessible fraction. Of<br />

course, such an analysis is more complex, and the data may<br />

not be adequate to recover the values <strong>of</strong> f i and K i at each<br />

wavelength.<br />

8.13. QUENCHING AND ASSOCIATION<br />

REACTIONS<br />

8.13.1. Quenching Due to Specific Binding<br />

Interactions<br />

In the preceding sections we considered quenchers that<br />

were in solution with the macromolecule but did not display<br />

any specific interactions. Such interactions can occur, and<br />

<strong>of</strong>ten appear to be <strong>of</strong> static quenching. 110–115 One example is<br />

provided by a synthetic peptide which spontaneously forms<br />

a four α-helical bundle in aqueous solution (Figure 8.43).<br />

The bundle consists <strong>of</strong> two peptide chains. Each peptide<br />

chain contains two α-helical regions and a single tryptophan<br />

residue. 114 The general anesthetics are nonpolar and<br />

were expected to bind to the central nonpolar region <strong>of</strong> the<br />

four helix bundles.<br />

The effects <strong>of</strong> halothane on the emission intensity <strong>of</strong><br />

the four-helix bundle are shown in Figure 8.43. The emission<br />

is strongly quenched by even low concentrations <strong>of</strong><br />

halothane. Quenching <strong>of</strong> the trp residues was also examined<br />

in the presence <strong>of</strong> 50% trifluoroethanol (TFE). Halothane<br />

quenching is much less efficient in this solvent (Figure<br />

8.44). TFE is known to disrupt hydrophobic interactions but<br />

to enhance helix formation in peptides. In 50% TFE the<br />

peptide is expected to exist as two separate α-helical peptides<br />

that are not bound to each other. These results show<br />

that the trp residues are buried in a nonpolar region in the<br />

four-helix bundle and become exposed to the solvent phase<br />

when the two peptides dissociate.<br />

How can one determine whether the quenching seen<br />

for the helix bundle in water is due to halothane binding, or<br />

to collisional quenching? One method is to calculate the<br />

apparent bimolecular quenching constant (k q app). Assume<br />

the decay time <strong>of</strong> trp residues in the bundle is near 5 ns. The

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