[2] in which IIl and IV are the time integrals of III and I-. The steady-state FA can be expressed by the time-resolved FA as s= J dtrtIt/ J dtIt, [3] in which the total fluorescence intensity It = I I I + 2Ij has been introduced. Since of x7 was consonant with the general concepts of membrane fluidity. The derivation of Eq. 4 proceeds from the following concept: The polarized light excites dipole moments of a certain orientation that emit light over their lifetime r. Initially the emitted light is polarized parallel, and rt is large. Due to rotational diffusion the orientation of the emitting dipoles becomes increasingly disordered, and rt decreases. Assuming the environment of the dipoles to be isotropic, their final distribution will also be isotropic, and rt decreases to zero (Fig. 1). The larger X and therefore 0, the longer the initially created anisotropy is preserved and consequently detected in steady-state measurements yielding a large rs.Recent time-resolved FA measurements with pure lipid membranes (2-4), lipid membranes containing cholesterol (5, 6), and cell membranes (7,8), as well as earlier measurements* with excitable membranes (9), have shown rt not to decrease to zero but to reach a finite level r. (Fig. 1)