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Principles of Fluorescence Spectroscopy

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916 ANSWERS TO PROBLEMS<br />

Figure 17.49. Arrhenius plot for the rotational correlation times <strong>of</strong><br />

RNase T 1 . Data from [54].<br />

total anisotropy. The fractional contribution <strong>of</strong> the<br />

long correlation time (t L ) is given by<br />

f L r 01<br />

r 01 r 02<br />

(17.7)<br />

This fraction can be related to the displacement <strong>of</strong> the<br />

transition dipole according to the definition <strong>of</strong><br />

anisotropy:<br />

cos 2 β 2f L 1<br />

3<br />

(17.8)<br />

Alternatively, this fraction can be related to the angle<br />

(θ c ) through which the tryptophan rotates before striking<br />

an energy barrier:<br />

f L [ 1<br />

2 cos θ c (1 cos θ c) ] 2<br />

(17.9)<br />

Application <strong>of</strong> these expressions to the data in Table<br />

17.4 yields the following results in Table 17.9.<br />

A17.3. The time-zero anisotropy, r(0), for RNase T 1 in Table<br />

17.7 is derived from the time-domain data and is lower<br />

than from other reports. One possible origin <strong>of</strong> the difference<br />

is the shorter excitation wavelength (295 nm)<br />

for the time-domain data and the possibility <strong>of</strong> a small<br />

error in the reported excitation wavelength. Another<br />

difference is that r(0) was a variable parameter in the<br />

analysis <strong>of</strong> the time-domain data. It is possible that a<br />

short component in the anisotropy decay was missed<br />

by limited time resolution, as suggested by molecular<br />

dynamics simulations or RNase T 1. 149<br />

A17.4. A. The intensity decays more slowly at longer<br />

emission wavelengths. This indicates that the<br />

mean decay time is increasing. In this case the<br />

effect is due to an increasing fractional contribution<br />

<strong>of</strong> the long-lived component (9.8 ns).<br />

B. The decay-associated spectra are calculated<br />

using the data in Table 17.8 and eq. 17.3, resulting<br />

in the DAS shown in Figure 17.50. In order<br />

to interpret the DAS one has to assume that each<br />

decay time (3.8 or 9.8 ns) is associated with one<br />

<strong>of</strong> the tryptophan residues. Using this assumption<br />

the 3.8 ns decay time is associated with a<br />

blue-shifted emission and a lower quantum yield<br />

than the red-shifted 9.8 ns residue.<br />

C. The most rigorous way to confirm assignment <strong>of</strong><br />

the DAS is to create the single tryptophan<br />

mutants. Each mutant should display one <strong>of</strong> the<br />

calculated DAS. One could also use quenching<br />

by iodide or acrylamide with the two tryptophan<br />

Table 17.9. Angular Freedom <strong>of</strong> NATA and Tryptophan Residues in Single-Tryptophan<br />

Peptides and Proteins at 20°C<br />

Proteins r 0 = r 01 + r 02 f L β (deg) θ c (deg)<br />

RNase T 1 , 20°C 0.310 1.00 0.0 0.0<br />

Staph. nuclease 0.321 0.944 11.1 11.2<br />

Monellin 0.315 0.768 23.2 23.8<br />

ACTH 0.308 0.386 39.8 43.8<br />

Gly-trp-gly 0.325 0.323 42.2 47.3<br />

NATA 0.323 1.00 0.00 0.00<br />

Melittin monomer 0.323 0.421 38.4 41.9<br />

Melittin tetramer 0.326 0.638 29.4 30.8

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