Rs. Brown et al., SELF-QUENCHING OF NITROBENZOXADIAZOLE LABELED PHOSPHOLIPIDS IN LIPID-MEMBRANES, The Journal of chemical physics, 100(8), 1994, pp. 6019-6027
The emission intensity, wavelength, and lifetime of the fluorophore ni
trobenzoxadiazole dipalmitoylphosphatidylethanolamine (NBD-PE) are sen
sitive to the local environmental structure when this species is prese
nt as a component of an amphiphilic membrane. Alterations of the physi
cal and electrostatic structure of a membrane can result in changes in
the fluorescence signal owing to changes in the extent of self-quench
ing of the probe. To investigate self-quenching, NBD-PE was incorporat
ed into monolayers and vesicles composed of Egg phosphatidylcholine at
concentrations of 0.1 to 50 mol %. Monolayer samples were dipcast ont
o glass slides at a pressure of 35 mN m-1. Both the integrated intensi
ty per fluorophore (quantum yield) from vesicles and dipcast monolayer
s, and the mean fluorescence lifetime from vesicles decreased as the c
oncentration of fluorophore in the membranes was increased. At all con
centrations studied the decay of NBD-PE fluorescence was fitted to two
discrete exponentials, and both lifetime components were observed to
change with concentration. The complexity of the fluorescence decay di
d not permit the use of standard theoretical models such as the Klafte
r-Blumen or Stern-Volmer equations which are normally employed to desc
ribe changes in fluorescence lifetime with changes in quencher concent
ration. Instead, a phenomenological approach was used to develop an em
pirical model of fluorescence self-quenching which could describe the
observed alterations in the fluorescence lifetime and intensity. The m
odel was based on a combination of Perrin quenching and Forster energy
transfer. The fluorescence data was fit by a model wherein NBD-PE for
med nonemissive trap sites with a critical radius of R(c) = 1.0 +/- 0.
1 nm (Perrin quenching), with Forster energy transfer occurring to the
trap sites with an R(0) value of 2.55 +/- 0.10 nm as determined from
spectral overlap integrals.