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Principles of Fluorescence Spectroscopy

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896 ANSWERS TO PROBLEMS<br />

Energy transfer can also be used to detect protein<br />

binding. Neither DNA nor model membranes possess<br />

chromophores that can serve as acceptors for<br />

the tryptophan fluorescence. Hence it is necessary<br />

to add extrinsic probes. Suitable acceptors would<br />

be probes that absorb near 350 nm, the emission<br />

maximum <strong>of</strong> most proteins. Numerous membranes<br />

and nucleic-acid probes absorb near 350 nm. The<br />

membranes could be labeled with DPH (Figure<br />

1.18), which absorbs near 350 nm. If the protein is<br />

bound to DPH-labeled membranes, its emission<br />

would be quenched by resonance energy transfer to<br />

DPH. Similarly, DNA could be labeled with DAPI<br />

(Figure 3.23). An advantage <strong>of</strong> using RET is that<br />

through-space quenching occurs irrespective <strong>of</strong> the<br />

details <strong>of</strong> the binding interactions. Even if there<br />

were no change in the intrinsic tryptophan emission<br />

upon binding to lipids or nucleic acids, one still<br />

expects quenching <strong>of</strong> the tryptophan when bound to<br />

acceptor-labeled membranes or nucleic acids.<br />

A3.2. A. The data in Figure 3.48 can be used to determine<br />

the value <strong>of</strong> F 0/F at each [Cl – ], where F 0 = 1.0 is<br />

the SPQ fluorescence intensity in the absence <strong>of</strong><br />

Cl – , and F is the intensity at each Cl – concentration.<br />

These values are plotted in Figure 3.49.<br />

Using Stern-Volmer eq. 1.6, one obtains K = 124<br />

M –1 , which is in good agreement with the literature<br />

value 182 <strong>of</strong> 118 M –1 .<br />

B. The value <strong>of</strong> F 0 /F and τ 0 /τ for 0.103 M Cl –<br />

can be found from eq. 1.6. Using K = 118 M –1 ,<br />

one obtains F 0 /F = τ 0 /τ = 13.15. Hence the<br />

intensity <strong>of</strong> SPQ is F = 0.076, relative to the<br />

intensity in the absence <strong>of</strong> Cl – ,F 0 = 1.0. The<br />

Figure 3.49. Stern-Volmer plot for the quenching <strong>of</strong> SPQ by chloride.<br />

lifetime is expected to be τ = 26.3/13.15 = 2.0<br />

ns.<br />

C. At [Cl – ] = 0.075 M, F = 0.102 and τ = 2.67.<br />

D. The Stern-Volmer quenching constant <strong>of</strong> SPQ<br />

was determined in the absence <strong>of</strong> macromolecules.<br />

It is possible that SPQ binds to proteins<br />

or membranes in blood serum. This could<br />

change the Stern-Volmer quenching constant<br />

by protecting SPQ from collisional quenching.<br />

Also, binding to macromolecules could<br />

alter τ 0 , the unquenched lifetime. Hence it is<br />

necessary to determine whether the quenching<br />

constant <strong>of</strong> SPQ is the same in blood serum as<br />

in protein-free solutions.<br />

A3.3. A. The dissociation reaction <strong>of</strong> the probe (P B )<br />

and analyte (A) is given by<br />

P B = A + P B , (3.3)<br />

where B and F refer to the free and bound forms <strong>of</strong> the<br />

probe. The fraction <strong>of</strong> free and bound probe is related<br />

to the dissociation constant by<br />

K D P F<br />

P B A<br />

(3.4)<br />

For the non-ratiometric probe Calcium Green, the fluorescein<br />

intensity is given by<br />

F = q F C F + q B C B , (3.5)<br />

where q i are the relative quantum yields, C i the molecular<br />

fraction in each form, and C F + C B = 1.0. The fluorescent<br />

intensities when all the probe is free is F min =<br />

kq FC, and then all the probe is bound in F max = kq BC,<br />

where k is an instrumental constant.<br />

Equation 3.5 can be used to derive expressions<br />

for C B and C F in terms <strong>of</strong> the relative intensities:<br />

F B F F min<br />

F max F min<br />

F F F max F<br />

F max F min<br />

(3.6)<br />

(3.7)<br />

The fractions C B and C F can be substituted for the<br />

probe concentration in (3.4), yielding

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