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Principles of Fluorescence Spectroscopy

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452 ENERGY TRANSFER<br />

safe for many proteins in the native state, particularly for<br />

single-domain proteins. For unfolded peptides or multidomain<br />

proteins a variety <strong>of</strong> conformations can exist, which<br />

results in a range <strong>of</strong> D–A distances. In this case calculation<br />

<strong>of</strong> a single distance using eq. 13.12 would result in an<br />

apparent distance, which would be weighted towards the<br />

shorter distances. Such systems are best analyzed in terms<br />

<strong>of</strong> a distance distribution using the time-resolved data<br />

(Chapter 14).<br />

13.3.2. Effects <strong>of</strong> Incomplete Labeling<br />

The largest source <strong>of</strong> error in calculating distance from the<br />

RET data is probably incomplete labeling with the acceptor.<br />

If melittin were incompletely labeled with acceptor, the<br />

measured value <strong>of</strong> F DA would be larger than the true value,<br />

and the calculated distance too large. We are less concerned<br />

with underlabeling by the donor because the protein molecules<br />

that do not contain donors do not contribute to the<br />

donor intensity, assuming the extent <strong>of</strong> donor labeling is the<br />

same for the donor-alone and donor–acceptor pair.<br />

If the fractional labeling with donor (f a ) is known then<br />

the relative intensities can be used to calculate the transfer<br />

efficiency. In this case eq. 13.14 becomes 13<br />

E 1 F DA F D(1 f A)<br />

F Df A<br />

( 1 FDA ) FD 1<br />

fA (13.17)<br />

For a high degree <strong>of</strong> RET donor quenching, (F DA /F D

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