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Principles of Fluorescence Spectroscopy

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PRINCIPLES OF FLUORESCENCE SPECTROSCOPY 293<br />

Figure 8.20. Acrylamide Stern-Volmer plot for NATA (x), and three<br />

single-tryptophan mutants <strong>of</strong> the channel-forming peptide <strong>of</strong> Colicin<br />

E1 at pH 3.5, W-355 (!), W-460 (), and W-443 (O). Revised and<br />

reprinted with permission from [55]. Copyright © 1993, American<br />

Chemical Society.<br />

Figure 8.21. Emission maxima (top) and bimolecular quenching constants<br />

(bottom) <strong>of</strong> the twelve single-tryptophan mutants <strong>of</strong> the channel-forming<br />

peptide <strong>of</strong> Colicin E1 at pH 3.5. Revised and reprinted<br />

with permission from [55]. Copyright © 1993, American Chemical<br />

Society.<br />

The conformation <strong>of</strong> the membrane-bound form <strong>of</strong> the<br />

colicin E1 channel peptide was studied by acrylamide<br />

quenching. 55 Twelve single tryptophan mutants were<br />

formed by site-directed mutagenesis. The tryptophan<br />

residues were mostly conservative replacements, meaning<br />

the trp residues were placed in positions previously containing<br />

phenylalanine or tyrosine. Acrylamide Stern-Volmer<br />

plots <strong>of</strong> three <strong>of</strong> these mutant proteins are shown in Figure<br />

8.20. The accessibility to acrylamide quenching is strongly<br />

dependent on the location <strong>of</strong> the residue, and all residues<br />

are shielded relative to NATA. Depending on position, the<br />

trp residues also showed different emission maxima (Figure<br />

8.21, top). The acrylamide bimolecular quenching constants<br />

were found to closely follow the emission maxima,<br />

with lower values <strong>of</strong> k q for the shorter-wavelength tryptophans<br />

(bottom). Such data can be used to suggest a folding<br />

pattern for the channel-forming peptide, and to reveal conformational<br />

changes that occur upon pH activation <strong>of</strong> colicin<br />

E1.<br />

8.10. APPLICATION OF QUENCHING<br />

TO MEMBRANES<br />

8.10.1. Oxygen Diffusion in Membranes<br />

Quenching by oxygen has been used to determine the<br />

apparent diffusion coefficient <strong>of</strong> oxygen in membranes.<br />

This can be accomplished using probes that partition into<br />

the lipid bilayers or are covalently bound to the lipids. Figure<br />

8.22 shows oxygen Stern-Volmer plots for 2-methylanthracene<br />

in vesicles <strong>of</strong> DMPC and DPPC, which have<br />

phase-transition temperatures (T c ) near 24 and 37EC,<br />

respectively. 56 At the experimental temperature near 31EC<br />

the DPPC bilayers are below the phase transition, and the<br />

DMPC bilayers are above the phase transition. While<br />

anisotropy measurement on such a bilayer suggests a large<br />

change in viscosity at the transition temperature (Chapter<br />

10), the effect on oxygen diffusion is only modest: near<br />

tw<strong>of</strong>old. This surprisingly small change in the oxygen diffusion<br />

coefficient has been confirmed by other fluorescence<br />

57–59 and ESR experiments. 60 These experiments even<br />

suggest that cholesterol, which generally makes membranes<br />

more rigid, results in increased rates <strong>of</strong> oxygen transport.<br />

This can be seen by quenching <strong>of</strong> pyrene dodecanoic acid<br />

(PDA) in erythrocyte ghost membranes (Figure 8.23). In<br />

this case, the ghost membranes were modified by addition<br />

<strong>of</strong> endogenous cholesterol. The apparent bimolecular<br />

quenching constant increases with increasing amounts <strong>of</strong><br />

cholesterol, except for the highest membrane concentration

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