Association dynamics and lateral transport in biological membranes

Dances with Membranes: Breakthroughs from Super-resolution Imaging

Biological membrane organization mediates numerous cellular functions and has also been connected with an immense number of human diseases. However, until recently, experimental methodologies have been unable to directly visualize the nanoscale details of biological membranes, particularly in intact living cells. Numerous models explaining membrane organization have been proposed, but testing those models has required indirect methods; the desire to directly image proteins and lipids in living cell membranes is a strong motivation for the advancement of technology. The development of super-resolution microscopy has provided powerful tools for quantification of membrane organization at the level of individual proteins and lipids, and many of these tools are compatible with living cells. Previously inaccessible questions are now being addressed, and the field of membrane biology is developing rapidly. This chapter discusses how the development of super-resolution microscopy has led to fundamental advances in the field of biological membrane organization. We summarize the history and some models explaining how proteins are organized in cell membranes, and give an overview of various super-resolution techniques and methods of quantifying super-resolution data. We discuss the application of super-resolution techniques to membrane biology in general, and also with specific reference to the fields of actin and actin-binding proteins, virus infection, mitochondria, immune cell biology, and phosphoinositide signaling. Finally, we present our hopes and expectations for the future of super-resolution microscopy in the field of membrane biology.

The influence of diffusion on the rate of a reversible quasi-unimolecular reaction in one, two or three dimensions

The role of diffusion in the kinetics of a reversible quasi-unimolecular reaction is considered. Equations that couple diffusion and reversible reaction are defined. From these equations are derived expressions for the concentrations of the reacting species, as a function of time, after a perturbation from their equilibrium concentrations. These expressions demonstrate how the time-dependent approach by a concentration to its equilibrium value is determined by the binding rate of adjacent molecules, the dissociation rate, the diffusion coefficients, the distance of closest approach of the reactants, the concentrations of the reactants, and the dimensionality. The expressions are applicable to perturbation-relaxation experiments in one, two, and three dimensions. The formalism is compared with previously existing theories.

Barriers to diffusion of plasma membrane proteins form early during guinea pig spermiogenesis

The plasma membrane of the mature guinea pig sperm is segregated into at least four domains of different composition. Previous studies have shown that some proteins localized within these domains are free to diffuse laterally, suggesting that barriers to protein diffusion are responsible for maintaining the nonuniform distribution of at least some surface proteins in mature sperm. The different membrane domains appear sequentially during sperm morphogenesis in the testis and during later passage through the epididymis. To determine when diffusion barriers become functional during sperm development, we examined the diffusion of two proteins that are expressed on the cell surface of developing spermatids and become segregated to different plasma membrane domains during the course of spermiogenesis. Both proteins exhibited rapid lateral diffusion throughout spermiogenesis, even after they become localized to specific regions of the surface membrane. These results suggest that barriers to membrane diffusion form concomitantly with membrane domains during spermiogenesis.

Computer simulation of lipid diffusion in a two-component bilayer. The effect of adsorbing macromolecules

We have modelled the effects of macromolecular adsorption upon lipid lateral diffusion in a two-component lipid bilayer or monolayer, which is at a temperature above both of the main transition temperatures. One set of lipids (binders, b) can bind to the macromolecules with a free energy of binding, FB, while the other set does not bind (non-binders, nb). We assumed that no phase separation of the lipids occurs in the absence of adsorbed macromolecules. We represented the lipid bilayer/monolayer by a triangular lattice, each site of which is occupied by a lipid molecule. Adsorbed macromolecules were represented by hexagons covering nH sites, and we defined a probability per unit of time, p, that a hexagon attempts to adsorb onto the lattice. We considered two sizes of hexagons, nH = 7 (Size-1) and nH = 19 (Size-2) and disallowed or permitted adsorbed hexagons to move laterally on the lattice. We calculate the lipid relative diffusion coefficients, Dnb, and Db, for three characteristic time-regimes, (i) tau c << tau a, (ii) tau c approximately tau a and (iii) tau c >> tau a, where tau c and tau a are the times for proteins to adsorb/desorb or for lipids to move from site to site, respectively. We obtain analytical expressions for Dnb and Db in the first case and calculate them using computer simulation in the other two cases. We found that (i) D alpha (iii) < or = D alpha (ii) < or = D alpha (i) (alpha = nb, b); (ii) D alpha could display a shoulder as a function of FB for low values of p; (iii) compared to cases in which lateral diffusion was disallowed, the lateral diffusion of absorbed hexagons appeared to have little effect on Dnb, but could cause Db to increase by 50%. (iv) Scatter in the calculated values of D via simulation appeared to be largest for Size-1 hexagons, and could be understood as a consequence of the large interfacial region between areas free of hexagons and areas 'covered' by hexagons. Our results suggest that it is advisable to measure Db, since Dnb might show little change from 1.0 for the values of F and p appropriate to the system being studied.

Determinants of the translational mobility of a small solute in cell cytoplasm

The purposes of this study were: (a) to measure the translational mobility of a small solute in cell cytoplasm; (b) to define quantitatively the factors that determine solute translation; and (c) to compare and contrast solute rotation and translation. A small fluorescent probe, 2,7-bis-(2-carboxyethyl)-5-(and 6-)-carboxyfluorescein (BCECF), was introduced into the cytoplasm of Swiss 3T3 fibroblasts. BCECF translation was measured by fluorescence recovery after photo-bleaching; rotation was measured by Fourier transform polarization microscopy. Diffusion coefficients relative to those in water (D/D0) were determined by comparing mobility in cytoplasm with mobility in standard solutions of known viscosity. At isosmotic cell volume, the relative diffusion coefficients for BCECF translation and rotation in cytoplasm were 0.27 +/- 0.01 (SEM, n = 24, 23 degrees C) and 0.78 +/- 0.03 (n = 4), respectively. As cell volume increased from 0.33 to 2 times isosmotic volume, the relative translational diffusion coefficient increased from 0.047 to 0.32, while the relative rotational diffusion coefficient remained constant. The factors determining BCECF translation were evaluated by comparing rotation and translation in cytoplasm, and in artificial solutions containing dextrans (mobile barriers) and agarose gels (immobile barriers). It was concluded that the hindrance of BCECF translation in cytoplasm could be quantitatively attributed to three independent factors: (a) fluid-phase cytoplasmic viscosity is 28% greater than the viscosity of water (factor 1 = 0.78); (b) 19% of BCECF is transiently bound to intracellular components of low mobility (factor 2 = 0.81); and most importantly, (c) translation of unbound BCECF is hindered 2.5-fold by collisions with cell solids comprising 13% of isosmotic cell volume (factor 3 = 0.40). The product of the 3 factors is 0.25 +/- 0.03, in good agreement with the measured D/D0 of 0.27 +/- 0.01. These results provide the first measurement of the translational mobility of a small solute in cell cytoplasm and define quantitatively the factors that slow solute translation.

In vitro measurement and screening of monoclonal antibody affinity using fluorescence photobleaching

Antibody screening is a routine in vitro assay in monoclonal antibody development and production. We have recently adapted the fluorescence photobleaching method to quantify antibody mass transport and binding parameters in bulk solution (Kaufman and Jain, 1990, 1991). The present study uses this in vitro method to screen a series of monoclonal antibodies (IgG) developed against the rabbit VX2 carcinoma tumor line. These experiments indicate that the three antibodies recognize distinct epitopes on the tumor, with equilibrium binding constants of 1.3 +/- 0.5, 5.1 +/- 3.6 and 2.0 +/- 1.1 x 10(7) M-1 for the antibodies RVC-184, RVC-626 and RVC-779, respectively. The antibody diffusion coefficient revealed no dependent upon protein concentration or antigen bead volume fraction within the ranges investigated. It was demonstrated experimentally that the interactions conformed to a reaction limited binding model of fluorescence recovery, that the system was at equilibrium, and that non-specific binding due to the fluorescein probe was not significant. Once the non-reactive fraction of antibody is determined, this photobleaching technique does not require perturbation or physical separation of the unbound species. As such, it has many potential applications including in vivo investigation of binding parameters.

Measurement of mass transport and reaction parameters in bulk solution using photobleaching. Reaction limited binding regime

Fluorescence recovery after photobleaching (FRAP) has been used previously to investigate the kinetics of binding to biological surfaces. The present study adapts and further develops this technique for the quantification of mass transport and reaction parameters in bulk media. The technique's ability to obtain the bulk diffusion coefficient, concentration of binding sites, and equilibrium binding constant for ligand/receptor interactions in the reaction limited binding regime is assessed using the B72.3/TAG-72 monoclonal antibody/tumor associated antigen interaction as a model in vitro system. Measurements were independently verified using fluorometry. The bulk diffusion coefficient, concentration of binding sites and equilibrium binding constant for the system investigated were 6.1 +/- 1.1 x 10(-7) cm2/s, 4.4 +/- 0.6 x 10(-7) M, and 2.5 +/- 1.6 x 10(7) M-1, respectively. Model robustness and the applicability of the technique for in vivo quantification of mass transport and reaction parameters are addressed. With a suitable animal model, it is believed that this technique is capable of quantifying mass transport and reaction parameters in vivo.

Normal band 3-cytoskeletal interactions are maintained on tanktreading erythrocytes

Normal nonnucleated erythrocytes subjected to continuous hydrodynamic shear exhibit membrane deformation or "tanktreading," a process important for reduction of the bulk viscosity of circulating blood. To characterize the effect of this unique process on the erythrocyte membrane we have measured the lateral diffusion of band 3 during tanktreading. Band 3 is normally constrained through interactions with the spectrin-actin cytoskeleton, therefore, any significant disruption of these interactions would result in alterations in band 3 dynamics. Band 3 of human erythrocytes was labeled with dichlorotriazinyl amino fluorescein. After laser photobleaching of an equatorial stripe, fluorescence images were recorded from cells in the presence or absence of shear. The amplitude of induced nonuniformity in the surface distribution of fluorescence was calculated directly from images of unsheared cells. In shear the bleached line rotated with the tanktreading motion of the cells. The surface integral of fluorescence oscillated with this motion. For this case, the amplitude of photobleaching-induced nonuniformity was defined as the amplitude at the fundamental frequency of fast Fourier transforms in time of the oscillations. Shear stress-induced membrane flow did not interrupt the linkage of band 3 with the erythrocyte cytoskeleton. Diffusion coefficient and mobile fraction (1.5 +/- 0.5 x 10(-10) cm2/s and 54 +/- 11%, respectively) were unaffected by shear. The rate of fluorescence recovery of cells in shear was also similar at the centers and at the edges, where in-plane shear forces are maximal.

Lateral diffusion in a mixture of mobile and immobile particles. A Monte Carlo study

The lateral diffusion coefficient for mixtures of mobile and immobile particles is obtained from Monte Carlo calculations of random walks by mobile tracers in the presence of immobile obstacles on a triangular lattice. The diffusion coefficient of the mobile species is obtained as a function of the area fractions of mobile and immobile species. The results are applied to diffusion of band 3 in the erythrocyte membrane, and indicate that obstruction of diffusion of mobile band 3 by band 3 and glycophorin attached to the membrane skeleton is not sufficient to explain the observed diffusion coefficient.

Quantification of transport and binding parameters using fluorescence recovery after photobleaching. Potential for in vivo applications

Fluorescence Recovery After Photobleaching (FRAP) has been used extensively in the study of transport and binding in biological media in vitro. The present study adapts and further develops FRAP so that it may be utilized for the in vivo quantification of binding parameters. The technique is validated in vitro by measuring mass transport and binding parameters for the Concanavalin A/Mannose binding system (a diffusion-limited system). The pseudo-equilibrium constant (the product of the equilibrium constant and the total concentration of binding sites) for this system was determined to be 26 +/- 15 which compares favorably with literature values ranging between 16 and 32. The applicability of this technique to measure parameters for monoclonal antibody/antigen interactions in a thin tissue preparation such as the rabbit ear chamber tissue preparation is also examined. Unlike other methods for measuring binding parameters, this is the only technique which has the potential to measure parameters relevant to antibody delivery in vivo. The proposed technique is noninvasive and does not require a priori knowledge of, independent measurement of, or variation in the concentration of binding sites or total concentration of binding species.

The membrane skeleton of erythrocytes: models of its effect on lateral diffusion

The membrane skeleton, a network of structural proteins attached to the cytoplasmic surface of the plasma membrane, hinders lateral diffusion of integral proteins. 2. In some types of cells, such as epithelial cells and nerve cells, the obstruction of lateral diffusion by the membrane skeleton is one of the mechanisms by which proteins are localized to domains on the cell surface. 3. The effect of the membrane skeleton on lateral diffusion may involve steric hindrance, transient binding or both. Three pictures of the effect are reviewed, the discrete barrier model, the continuous barrier model and the transient binding model. 4. Experiments to distinguish the models are discussed.

Interpretation of fluorescence correlation spectroscopy and photobleaching recovery in terms of molecular interactions

The theoretical basis and experimental implementation of FCS and FPR measurements are now well established. Because of the requirements for system stability and long data acquisition times FCS is relatively rarely used. But FCS can provide unique information, especially about extents of aggregation or polymerization and therefore is a useful supplement to FPR for certain applications. FPR measurements are now carried out routinely in many laboratories in a variety of formats using different beam profiles, optical systems, and analytical schemes. A particular version may be better adapted to a specific application. The spot photobleaching approach, however, seems simplest and most versatile for cellular studies and is now most often used. Important experimental considerations in setting up a spot photobleaching instrument are discussed in detail in Chapter 10 by Wolf (this volume) and elsewhere (Petersen et al., 1986a). In interpreting FPR measurements it is also important to take into account the possibility of systematic errors from a number of sources. In Chapter 10 in this volume, Wolf discusses many factors that must be properly controlled in carrying out FPR measurements. Additional consideration of some of these points is presented by Petersen et al. (1986a). One potentially troublesome type of error arises from the possibility that chemical reactions initiated by the photobleaching pulse or during the measurement of recovery could significantly perturb the system. Evidence from a variety of sources [summarized, for example, in Petersen et al. (1986a)] indicates that photobleaching fluorophores can induce chemical cross-linking of cellular proteins under some conditions. But measurements in a number of different systems have demonstrated that, even if these types of reactions occur in FPR measurements, nevertheless they do not perturb the measured mobilities. If possible, however, this point should be checked for each new system because variations in structure or environmental conditions could enhance the chemical cross-linking reactions mediated by photogenerated free radicals. In practice, the principal difficulty in carrying out FPR measurements on cells is frequently the low intensity of the fluorescent signal which can be obtained from specifically labeled cell surface ligands or microinjected components. This low intensity results from the typically low capacity of an individual cell for the specifically labeled macromolecule. Even in the absence of systematic errors, low emission intensity will reduce the accuracy of measurements due to shot noise. This is an important practical limitation on measuring accuracy. Low measurement accuracy severely limits the extent to which the data can be interpreted mechanistically. Precision can be improved by averaging many recovery experiments.(ABSTRACT TRUNCATED AT 400 WORDS)

Inhomogeneous translational diffusion of monoclonal antibodies on phospholipid Langmuir-Blodgett films

The translational mobility of fluorescent-labeled monoclonal antibodies specifically bound to supported phospholipid bilayers containing hapten-conjugated phospholipids has been measured as a function of the surface concentration of bound antibodies using fluorescence recovery after photobleaching. Fluorescence recovery curves are fit well by a model that assumes the presence of two populations of antibodies with different lateral diffusion coefficients. The larger diffusion coefficient equals 3.5 x 10(-9) cm2/s, the smaller diffusion coefficient ranges from 1.5 x 10(-9) cm2/s to 2.5 x 10(-10) cm2/s, and the fractional fluorescence recovery associated with the smaller coefficient increases from approximately 0 to approximately 0.7 with increasing concentration of bound antibody. These results suggest that complexes of haptenated phospholipids and antibodies in phospholipid Langmuir-Blodgett films form clusters or domains in a concentration-dependent fashion.

Effects of mutations in three domains of the vesicular stomatitis viral glycoprotein on its lateral diffusion in the plasma membrane

The lateral mobility of the vesicular stomatitis virus spike glycoprotein (G protein) and various mutant G proteins produced by site-directed mutagenesis of the G cDNA has been measured. Fluorescence recovery after photobleaching results for the wild type G protein in transfected COS-1 cells yielded a mean diffusion coefficient (D) of 8.5 (+/- 1.3) X 10(-11) cm2/s and a mean mobile fraction of 75% (+/- 3%). Eight mutant proteins were also examined: dTM14, lacking six amino acids from the transmembrane domain; TA2, lacking an oligosaccharide in the extracellular domain; QN2, possessing an extra N-linked oligosaccharide in the extracellular domain; CS2, possessing a serine instead of a cysteine at residue 489 in the cytoplasmic domain, preventing palmitate addition to the glycoprotein; TMR-stop, lacking the entire cytoplasmic domain except an arginine at residue 483; and three chimeric proteins, G mu, G23, and GHA, containing in place of the 29 amino acid wild type cytoplasmic domain the cytoplasmic domains from the surface IgM from the spike protein of the infectious bronchitis virus or from the hemagglutinin protein of the influenza virus, respectively. The mean D for the mutant proteins varied over a relatively small range, with the slowest mutant, G23, exhibiting a value of 11.3 (+/- 1.4) X 10(-11) cm2/s and the fastest mutant, GHA, having a D of 28.6 (+/- 4.5) X 10(-11) cm2/s. The mean mobile fraction similarly varied over a small range, extending from 55 to 68%. None of the mutations resulted in the more rapid diffusion characteristic of membrane proteins embedded in artificial bilayers. Therefore, it appears that the cytoplasmic and transmembrane domains themselves contribute little to restraining the lateral mobility of this integral membrane protein when expressed in transfected cells.

Lateral diffusion of the PH-20 protein on guinea pig sperm: evidence that barriers to diffusion maintain plasma membrane domains in mammalian sperm

PH-20 protein on the plasma membrane (PH-20PM) is restricted to the posterior head of acrosome-intact guinea pig sperm. During the exocytotic acrosome reaction the inner acrosomal membrane (IAM) becomes continuous with the posterior head plasma membrane, and PH-20PM migrates to the IAM. There it joins a second population of PH-20 protein localized to this region of the acrosomal membrane (PH-20AM) (Cowan, A.E., P. Primakoff, and D.G. Myles, 1986, J. Cell Biol. 103:1289-1297). To investigate how the localized distributions of PH-20 protein are maintained, the lateral mobility of PH-20 protein on these different membrane domains was determined using fluorescence redistribution after photobleaching. PH-20PM on the posterior head of acrosome-intact sperm was found to be mobile, with a diffusion coefficient and percent recovery typical of integral membrane proteins (D = 1.8 X 10(-10) cm2/s; %R = 73). This value of D was some 50-fold lower than that found for the lipid probe 1,1-ditetradecyl 3,3,3',3'-tetramethylindocarbocyanine perchlorate (C14diI) in the same region (D = 8.9 X 10(-9) cm2/s). After migration to the IAM of acrosome-reacted sperm, this same population of molecules (PH-20PM) exhibited a 30-fold increase in diffusion rate (D = 4.9 X 10(-9) cm2/s; %R = 78). This rate was similar to diffusion of the lipid probe C14diI in the IAM (D = 5.4 X 10(-9) cm2/s). The finding of free diffusion of PH-20PM in the IAM of acrosome-reacted sperm supports the proposal that PH-20 is maintained within the IAM by a barrier to diffusion at the domain boundary. The slower diffusion of PH-20PM on the posterior head of acrosome-intact sperm is also consistent with localization by barriers to diffusion, but does not rule out alternative mechanisms.

Effects of cell density and extracellular matrix on the lateral diffusion of major histocompatibility antigens in cultured fibroblasts

We have studied the effect of cell density on the lateral diffusion of major histocompatibility (MHC) antigens in the plasma membranes of fibroblasts using fluorescence recovery after photobleaching. The percent recovery of fluorescence was decreased in fibroblasts grown in confluent cultures. While recovery of fluorescence was measurable in greater than 90% of the cells from sparse cultures, measurable recovery was detected in only 60-80% of the cells from dense cultures; no mobile antigens were detectable in 20-40% of cells examined. The diffusion coefficient on human skin fibroblast cells that did show recovery was the same for cells grown in sparse or dense conditions. In WI-38, VA-2, and c1 1d cultures the diffusion coefficients of mobile antigens were smaller in cells from dense cultures. Changes in lateral diffusion occurred with increased cell-cell contact and with age of cell culture but were not observed in growth-arrested cells or in sparse cells cultured in medium conditioned by confluent cells. Decreased mobile fractions of MHC antigens were observed when cells were plated on extracellular matrix materials derived from confluent cultures. Treatment of the extracellular matrix materials with a combination of proteolytic enzymes or by enzymes that degrade proteoglycans abolished this effect. Matrices produced by cells from other cell lines were less effective in inducing changes in mobile fractions and purified matrix components alone did not induce changes in lateral diffusion. Finally, there were no differences in the proportion of MHC antigens that were resistant to Triton X-100 extraction in sparse and dense cells. These results suggest that cell-cell interactions mediated through extracellular matrix materials can influence the lateral diffusion of at least part of the population of MHC antigens.

Probing the structure of cytoplasm

We have used size-fractionated, fluorescent dextrans to probe the structure of the cytoplasmic ground substance of living Swiss 3T3 cells by fluorescence recovery after photobleaching and video image processing. The data indicate that the cytoplasm of living cells has a fluid phase viscosity four times greater than water and contains structural barriers that restrict free diffusion of dissolved macromolecules in a size-dependent manner. Assuming these structural barriers comprise a filamentous meshwork, the combined fluorescence recovery after photobleaching and imaging data suggest that the average pore size of the meshwork is in the range of 300 to 400 A, but may be as small as 200 A in some cytoplasmic domains.

Behavior of a fluorescent analogue of calmodulin in living 3T3 cells

We have prepared and partially characterized a lissamine-rhodamine B fluorescent analogue of calmodulin, LRB-CM. The analogue had a dye/protein ratio of approximately 1.0 and contained no free dye or contaminating labeled proteins. LRB-CM was indistinguishable from native calmodulin upon SDS PAGE and in assays of phosphodiesterase and myosin light chain kinase. The emission spectrum of LRB-CM was insensitive to changes in pH, ionic strength, and temperature over the physiological range, but the apparent quantum yield was influenced somewhat by divalent cation concentration. LRB-CM injected into living Swiss 3T3 fibroblasts became associated with nitrobenzoxadiazole-phallacidin staining stress fibers in some interphase cells. LRB-CM and acetamidofluorescein-labeled actin co-injected into the same cell both became associated with fibers in some cells, but in most cases association of the two analogues with fibers was mutually exclusive. This suggests that calmodulin may differ from actin in the timing of incorporation into stress fibers or that we have distinguished distinct populations of stress fibers. We were able to detect no direct interaction of LRB-CM with actin by fluorescence photobleaching recovery (FRAP) of aqueous solutions. Interaction of LRB-CM with myosin light chain kinase also was not detected by FRAP. This suggests that the mean lifetime of the calmodulin-myosin light chain kinase complex is too short to affect the diffusion coefficient of calmodulin. We examined various fluorescent derivatives of proteins and dextrans as suitable control molecules for quantitative fluorescent analogue cytochemistry in living cells. Fluorescein isothiocyanate-dextrans were found to be preferable to all the proteins tested, since their mobilities in cytoplasm were inversely dependent on molecular size and there was no evidence of binding to intracellular components. In contrast, FRAP of LRB-CM in the cytoplasm of living 3T3 cells suggested that the analogue interacts with intracellular components with a range of affinities. The mobility of LRB-CM in the cytoplasm was sensitive to treatment of the cells with trifluoperazine, which suggests that at least some of the intracellular binding sites are specific for calmodulin in the calcium-bound form. FRAP of LRB-CM in the nuclei of living 3T3 cells indicated that the analogue was highly mobile within the nucleus but entered the nucleus from the cytoplasm much more slowly than fluorescein isothiocyanate-dextran of comparable molecular size and much more slowly than predicted from its mobility in cytoplasm.

Lateral diffusion of an 80,000-dalton glycoprotein in the plasma membrane of murine fibroblasts: relationships to cell structure and function

The lateral diffusion of an 80,000-dalton major cell surface glycoprotein of murine fibroblasts has been measured. This antigen, identified through the use of monoclonal antibodies, is an integral glycoprotein distributed through the plasma membrane as judged by immunofluorescence and immunoelectron microscopy (see preceding paper). Measurements of fluorescence recovery after photobleaching were performed on the antigen-antibody complex within the plasma membrane of C3H/10T1/2 and NIH/3T3 cells after labeling the monoclonal antibody with fluorescein. Measurements were performed as a function of temperature, for interphase, mitotic, and G0 C3H/10T1/2 cells. The mean lateral diffusion coefficients (D) for the antibody-protein complex in interphase cells were in the range of 0.7-3.5 X 10(-10) cm2/s between 9 degrees and 37 degrees C, while that for the lipid analog probe, dihexadecylindocarbocyanine was about two orders of magnitude greater. This comparison indicates that peripheral interactions other than bilayer fluidity limit the lateral mobility of the antigen. The mobile fraction of mitotic, G0, and interphase cells showed a monotonic increase with temperature with most of the antibody-antigen complexes being free to move about 25 degrees C. Semi-quantitative interpretations of both the slow glycoprotein diffusion and the immobile fraction are offered. Comparison of diffusion coefficients for cells in different phases of the cell cycle does not reveal striking differences. Mobile fractions for G0 cells at 25 degrees C or less are substantially lower than in interphase cells. In all cases, there was a remarkably broad range of the fluorescence recovery data between different cells, resulting in up to a 10-fold variation in diffusion coefficients, which is far greater than the precision limits of the experiment. Diffusion values and mobile fractions were generally well within a factor of two when measured at several arbitrary points on a single cell. The origins of this cellular heterogenity remain to be elucidated. Lateral mobility in cell fragments and specific regions of single cells was also examined. The glycoprotein was mobile in ventral surface cell fragments. Its mobility was not altered in regions of cell-cell underlapping. However, the diffusion coefficient was threefold higher near the leading edge of motile cells compared to the trailing region. This difference may reflect weaker coupling of the glycoprotein to the underlying cytoskeleton in the dynamic leading edge region.

A localized pattern photobleaching method for the concurrent analysis of rapid and slow diffusion processes

A scanning pattern photobleaching method for the analysis of lateral transport is described and discussed. Fluorescence bleaching with a localized pattern allows for the concurrent analysis of motions over two very different characteristic distances: xi 0(-1), the repeat distance of the pattern, and W, the linear dimension of the illuminated region. The former motion is deduced from the decay of the modulation amplitude (of period xi 0(-1) of fluorescence scans with the attenuated pattern, the latter from the recovery of the average fluorescence intensity. Such analysis should prove useful for the study of samples with a wide range of diffusion coefficients, and for the separation of effects arising from lateral diffusion and association dynamics. Theoretical analyses are presented for three related problems: (a) the effect of pattern localization on the decay of the modulation amplitude, (b) the effect of the pattern modulation on the recovery of the average local fluorescence intensity, and (c) the effect of a limited diffusion space (with linear dimensions of only a few pattern periods) on the decay of the modulation amplitude.