Determination of the affinities between heterotrimeric G protein subunits and their phospholipase C-beta effectors.

Phosphatidylinositide-specific phospholipase C-betas play a key role in Ca2+ signaling and are specifically activated by the alphaq family of heterotrimeric G proteins and as well as betagamma subunits. We have determined the affinity between Gbetagamma subunits and GTPgammaS and GDP-liganded Galphaq subunits on membrane surfaces, and their respective affinities to PLC-beta1, -beta2 and -beta3 effectors by fluorescence spectroscopy. We find that activation of Galphaq by GTPgammaS decreases its affinity for Gbetagamma subunits at least 36-fold compared to the GDP-liganded form, but increases its affinity for PLC-betas at least 40-200-fold depending on the PLC-beta isoform. The affinity of Galphaq(GTPgammaS) is similar for PLC-beta1 and -beta3 and 10-fold stronger for PLC-beta2, which corresponds to the reported relationship between the concentration of Galphaq(GTPgammaS) and PLC-beta activation on lipid bilayers. We find that a large portion of the PLC-beta-Galphaq association energy lies within the 400 residue C-terminal region of PLC-beta1 since truncating this region reduces its Galphaq affinity. In contrast, the isolated N-terminal region does not interact with Galphaq. Gbetagamma subunits interact with all three PLC-beta isotypes, but only showed strong binding to PLC-beta2, and activation of the three PLC-betas by Gbetagamma subunits parallels this behavior. We also tested the possibility that both Galphaq and Gbetagamma can simultaneously bind PLC-beta2. Our data argue against simultaneous binding and show that Galphaq and Gbetagamma independently regulate this effector.

Regulation of the rate and extent of phospholipase C beta 2 effector activation by the beta gamma subunits of heterotrimeric G proteins.

The activity of mammalian phosphoinositide-specific phospholipase C beta 2 (PLC-beta 2) is regulated by the alpha q family of G proteins and by beta gamma subunits. We measured the affinity between the laterally associating PLC-beta 2 and G beta gamma on membrane surfaces by fluorescence resonance energy transfer. Using a simple model, we translated this apparent affinity to a bulk or three-dimensional equilibrium constant (Kd) and obtained a value of 3.2 microM. We confirmed this Kd by separately measuring the on and off (kf and kr) rate constants. The kf was slower than a diffusion-limited value, suggesting that conformational changes occur when the two proteins interact. The off rate shows that the PLC-beta 2.G beta gamma complexes are long-lived ( approximately 123 s) and that activation of PLC-beta 2 by G beta gamma would be sustained without a deactivating factor. The addition of alpha i1(GDP) subunits failed to physically dissociate the complex as determined by fluorescence. However, enzyme activity studies performed under similar conditions show that the addition of G alpha i1(GDP) results in reversal of PLC-beta 2 activation by G beta gamma during the time of the assay (30 s). From these results, we propose that G alpha(GDP) subunits can bind to the PLC-beta 2.G beta gamma complex to allow for rapid deactivation without complex dissociation. In support of this model, we show by fluorescence that G alpha i1(GDP).G beta gamma.PLC-beta 2 can form.

Conformational changes of the insulin receptor upon insulin binding and activation as monitored by fluorescence spectroscopy.

We have characterized the changes in intrinsic fluorescence that the insulin receptor undergoes upon ligand binding and autophosphorylation. The binding of insulin to its receptor results in an increase in the receptor's fluorescence intensity, emission energy and anisotropy. We monitored the time course of the anisotropy change, and these data, coupled with studies monitoring the energy transfer from insulin receptor tryptophan donors to a fluorescent-labeled insulin, allowed us to conclude that the change in anisotropy is due to a conformational change in the receptor induced by hormone binding. Since insulin association is very fast, the time course also allowed us to estimate the slower rate of formation of this conformationally-altered state. The time course of receptor autophosphorylation was measured under similar conditions and was found to be similar to the ligand-induced anisotropy time course. The simultaneous use of two fluorescent-labeled insulin analogs also allowed us to assess the maximum distance between the two hormones bound to the receptor. Addition of ATP produces a large, seemingly instantaneous increase in anisotropy. Our observation that ATP binds to the insulin receptor in the presence and absence of insulin supports the idea that the conformational change produced by insulin binding increases the rate of autophosphorylation rather than increases ATP affinity. A suggested model for these changes is presented.

Effects of cholesterol on membrane surfaces as studied by high-pressure fluorescence spectroscopy.

We have studied the effects of cholesterol on membrane surfaces using fluorescence spectroscopy at high pressure. At atmospheric pressure, the dissociation state of a pH-sensitive fluorophore (6-decanylnaphthol or DECNA) incorporated into several types of membranes showed an apparent increase in dissociation with cholesterol content coming somewhat closer to its dissociation state in solution. Previous studies have shown that when DECNA is free in solution, pressure induces proton dissociation due to the volume decrease that occurs when water electrostricts around the ions. But in phosphatidylcholine (PC) bilayers, proton dissociation is inhibited, either due to the inability of the surface to expand and allow for increased hydration, or other changes in lipid structure. The pressure behavior of DECNA in dioleoyl-PC, dioleoylphosphatidic acid and dioleylphosphatidylglycerol bilayers shows that incorporation of 5-10% cholesterol causes DECNA to behave like it is in a more unrestricted environment. This trend is reversed at higher cholesterol concentrations. These data, together with compressibility measurements, support the model of Sankaram and Thompson [M. Sankaram, T.E. Thompson, Biochemistry 29 (1990) 10676.] whereby in the disordered phase, cholesterol can span the two leaflets causing an increase in the area between the head groups; whereas in the ordered phase, no expansion occurs. Thus, the effect of cholesterol on membrane surfaces depends on its phase diagram.

Myristoylated alanine-rich C kinase substrate (MARCKS) produces reversible inhibition of phospholipase C by sequestering phosphatidylinositol 4,5-bisphosphate in lateral domains.

The myristoylated alanine-rich protein kinase C substrate (MARCKS) is a major protein kinase C (PKC) substrate in many different cell types. MARCKS is bound to the plasma membrane, and several recent studies suggest that this binding requires both hydrophobic insertion of its myristate chain into the bilayer and electrostatic interaction of its cluster of basic residues with acidic lipids. Phosphorylation of MARCKS by PKC introduces negative charges into the basic cluster, reducing its electrostatic interaction with acidic lipids and producing translocation of MARCKS from membrane to cytoplasm. The present study shows that physiological concentrations of MARCKS (<10 microM) inhibit phospholipase C (PLC)-catalyzed hydrolysis of phosphatidylinositol 4,5-bisphosphate (PIP2) in phospholipid vesicles. A peptide corresponding to the basic cluster, MARCKS(151-175), produces a similar inhibition, which was observed with both PLC-delta1 and -beta1. Direct fluorescence microscopy observations demonstrate that the MARCKS peptide forms lateral domains enriched in the acidic lipids phosphatidylserine and PIP2 but not PLC, which accounts for the observed inhibition of PIP2 hydrolysis. Phosphorylation of MARCKS(151-175) by PKC releases the inhibition and allows PLC to produce a burst of inositol 1,4, 5-trisphosphate and diacylglycerol.

Theory and application of fluorescence homotransfer to melittin oligomerization.

Fluorescence homotransfer (electronic energy transfer between identical fluorophores) has the potential to quantitate the number of subunits in membrane protein oligomers. Homotransfer strongly depolarizes fluorescence emission as a result of intermolecular excitation energy exchange between an initially excited, oriented molecule and a randomly oriented neighbor. We have theoretically treated fluorescein labeled subunits in an oligomer as a cluster of molecules that can exchange excitation energy back and forth among the subunits within that group. We find that the larger the number of subunits, the more depolarized is the emission. The general equations to calculate the expected anisotropy for complexes composed of varying numbers of labeled subunits are presented. Self-quenching of fluorophores, orientation, and changes in lifetime are also discussed and/or considered. To test this theory, we have specifically labeled melittin on its N-terminal with fluorescein and monitored its monomer to tetramer equilibrium both in solution and in lipid bilayers. The calculated anisotropies are close to the experimental values when non-fluorescent fluorescein dimers are taken into account. Our results show that homotransfer may be a promising method to study membrane-protein oligomerization.

Barbiturates inhibit hexose transport in cultured mammalian cells and human erythrocytes and interact directly with purified GLUT-1.

Barbiturates reduce cerebral blood flow, metabolism, and Glc transfer across the blood-brain barrier. The effect of barbiturates on hexose transport in cultured mammalian cell lines and human erythrocytes was studied. Pentobarbital inhibits [3H]-2-dGlc uptake in 3T3-C2 murine fibroblasts by approximately 95% and approximately 50% at 10 and 0.5 mM, respectively. Uptake of [3H]-2-dGlc is linear with time in the presence or absence of pentobarbital, and the percent inhibition is constant. This suggests that hexose transport, not phosphorylation, is inhibited by barbiturates. Inhibition by pentobarbital of hexose transport in 3T3-C2 cells is rapid (< 1 min), is not readily reversible, is not altered by the presence of albumin [1% (w/v)], and is independent of temperature (4-37 degrees C) and the level of cell surface GLUT-1. The IC50's for inhibition of hexose transport in 3T3-C2 cells by pentobarbital, thiobutabarbital, and barbital are 0.8, 1.0, and 4 mM, respectively. This is consistent with both the Meyer-Overton rule and the pharmacology of barbiturates. Neither halothane (< or = 10 mM) nor ethanol [< or = 0.4% (v/v)] significantly inhibits hexose transport. Inhibition by pentobarbital (0.5 mM) of [3H]-2-dGlc uptake by 3T3-C2 cells decreases the apparent Vmax (approximately 50%) but does not alter the apparent Km (approximately 0.5 mM). Inhibition of hexose transport by barbiturates, but not ethanol [< or = 0.4% (v/v)], is also observed in human erythrocytes and four other cultured mammalian cell lines. Pentobarbital quenches (Qmax approximately 75%) the intrinsic fluorescence of purified and reconstituted GLUT-1 (Kd approximately 3 mM). Quenching is independent of Glc occupancy, is unchanged by mild proteolytic inactivation, and does not appear to directly involve perturbations of the lipid bilayer. We propose that barbiturates can interact directly with GLUT-1 and inhibit the intrinsic activity of the carrier. Glc crosses the blood-brain barrier primarily via the GLUT-1 of the endothelial cells of cerebral capillaries. Partial inhibition of this process by barbiturates may be of significance to cerebral protection.

Stability of a potential blood substitute, HbXL99 alpha, under high pressure.

One important criteria for a plasma circulating hemoglobin blood substitute is resistance to subunit dissociation. For this reason, cross-linked hemoglobins (with low oxygen affinities) are being specifically designed to serve as potential blood substitutes. An example is HbXL99 alpha, cross-linked between the alpha-subunits [PNAS (1987) 84:7280]. In the study presented here, the effects of up to 2 kilobars of pressure on the intrinsic fluorescence of HbXL99 alpha, HbA, and myoglobin were compared. Hemoglobin solutions were studied between 0.01-0.1g% in potassium phosphate or Hepes buffers, pH 7.4. Results show HbA exhibits a decrease in fluorescence intensity as a function of pressure. In contrast, HbXL99 alpha as well myoglobin (a monomer) show essentially no significant intrinsic fluorescence changes as a function of pressure. These results suggest that HbXL99 alpha is stable as a tetramer up to approximately 2 kilobars of pressure. In addition, high pressure intrinsic fluorescence studies provide a suitable technique for determining the subunit stability of hemoglobins.

The differential effects of carbon monoxide and oxygen on the pressure dissociation of Lumbricus terrestris hemoglobin.

We have explored the subunit affinities of Lumbricus terrestris hemoglobin (LtHb) under a variety of conditions using high-pressure spectroscopy. While only small changes were observed for LtHb-oxy below 1.0 kbar, higher pressures resulted in a 1000 cm-1 red shift and 2-fold increase in fluorescence intensity with a concomitant 12-fold decrease in scattering intensity, all of which reached completion by approx. 2.2 kbar. In the presence of 1 M MgCl2 or at acidic pH (4.2), the curves shifted by 400 and 1000 bar corresponding to significant destabilization. At pH 9.1, the initial spectral parameters were almost equal to the final endpoints and were unaffected by pressure. While the pressure curve of the CO form was similar to the oxy form at pH 7.2, the midpoints of the other samples were shifted to higher pressures relative to their oxy counterpart, indicating tighter subunit contacts. This stabilization was unexpected based upon the sequence homology to vertebrate hemoglobins, and the minimal structural differences between these two liganded forms of human hemoglobin. These data indicate that the differences are the result of the additive nature of the interactions involved in subunit packing whose effects become significant in larger aggregates.

Solution studies of the interactions between the histone core proteins and DNA using fluorescence spectroscopy.

The equilibrium interactions between histone H2A-H2B and H3/H4 subunits with 200 base pair chicken erythrocyte DNA have been studied by monitoring the fluorescence polarization of a long-lived fluorescence probe covalently bound to the histone subunits. These studies have brought to light the formation of highly asymmetric complexes exhibiting very high histone/DNA stoichiometries as well as very high apparent affinities. The stoichiometries observed for these non-nucleosome complexes depended both upon the concentration of the histones and the concentration of the DNA 200mer. The observed stoichiometries varied approximately between 4 and 16 histone octamers/DNA 200mer and the affinities were in the nanomolar range. These results are discussed in terms of their in vitro as well as their possible in vivo significance.

Effect of increased chain packing on gramicidin-lipid interactions.

To study the effect of lipid packing on the dynamics of membrane proteins, the changes in the rotational motion of gramicidin tryptophans with increased packing brought about by high hydrostatic pressure through fluorescence spectroscopy were determined. In fluid phase dimyristoylphosphatidylcholine, the rotational motion of the residues decreased slightly with increased packing, but in the gel phase a significant reversible increase was observed. The magnitude of this increase was temperature dependent and much greater at lower temperatures. Quenching studies show that the increase in rotational motion is not due to a change in the location of the peptide in the membrane under pressure. Aromatic ring stacking between residues 9 and 15 appears to be stabilized under pressure, and there is no evidence of pressure-induced changes in peptide aggregation. The increase in rotational motion could be caused by a destabilization of hydrogen bonds between the indole hydrogens and the lipid head group oxygens due to an increase in the thickness of the compressible lipid bilayer with pressure without a concomitant lengthening of the peptide. These results indicate that specific interactions between lipids and proteins may play a major role of regulating the dynamics of membrane proteins.

Compression of lipid membranes as observed at varying membrane positions.

We have measured the microscopic isothermal compressibility of dioleoyl- and dimyristyl-phosphatidylcholine multilayers and bilayers as a function of membrane depth by the pressure dependence of the polarization of a series of anthroyloxy fatty acids. In both systems, within experimental error, the compressibility did not change with membrane depth. The magnitudes of the compressibilities matched those of organic solids and those reported for dipalmitoylphosphatidylcholine multilayers from neutron diffraction measurements (Braganza, L. F., and D. L. Worcester. 1986. Biochemistry, 25:7484-7488). The bilayer compressibility decreased with temperature and this decrease was similar with membrane depth consistent with the isotropic thermal expansion of membranes previously observed (Scarlata, S. 1989. Biophys. J. 55:1215-1223). The vertical compressibility in the z direction is much lower than the horizontal (xy planes) for probes that lie parallel to the hydrocarbon chains which is consistent with an increase in bilayer thickness. The compressibility for probes that lie perpendicular to the hydrocarbon chains is more isotropic due to their limited spatial access to the z plane.

Effect of salt and membrane fluidity on fluorophore motions of a gramicidin C derivative.

We have used fluorescence spectroscopy to investigate the effect of salt and membrane fluidity on the rotational motion of a 5-(dimethylamino)naphthalene-1-sulfonyl (dansyl) derivative of gramicidin C (dansyl-gC) in dimyristoylphosphatidylcholine bilayers, under conditions where the peptide is a formyl-NH to formyl-NH terminal dimer, and in octyl glucoside micelles, where the peptide is an intertwined helical dimer. Energy-transfer experiments showed no changes in either conformation or dimer aggregation under the conditions explored here (15-40 degrees C, 1-350 bar, 0-0.33 M Mg2+, and 0-1 M Na+). The addition of permeable (Na+) or nonpermeable (Mg2+) ions did not affect the temperature or pressure behavior of dansyl rotation. However, fluorescence lifetime measurements indicated an increase in solvent accessibility in the presence of sodium. In bilayers, the temperature dependence of the fluorescence polarization and lifetime shows strong interactions between the dansyl residue and the peptide, and at no time did the dansyl motions become solvent controlled as has been observed for aqueous solvent peptides [Scarlata, S. F., Rholam, M., & Weber, G. (1984) Biochemistry 23, 6789]. In micelles, the change in rotational motion with temperature followed solvent expansion, showing that in this case the dansyl residue does not associate extensively with the peptide. Our results indicate that because of the extensive coupling between the dansyl residue and the rest of the peptide, membrane fluidity does not play a major role in controlling side-chain motions.

Effect of increased lipid packing on the surface charge of micelles and membranes.

We have investigated the responsiveness of micelle and bilayer surfaces to changes in bulk pH through titrations, and to changes in lipid packing through the application of high hydrostatic pressure using two fluorescent, pH-sensitive surface probes. In micelles, the surface is very sensitive to bulk pH while in phosphatidylcholine and phosphatidic acid bilayers the surface charge changed little through a large pH region. Application of pressure on micelles causes proton dissociation due to the volume reduction achieved from the contraction of water around the charges (electrostriction). However, in bilayers, the effect of electrostriction is greatly reduced, most likely due to the energy needed to expand and hydrate the surface. The sign and amount of change in dissociation the probe undergoes with pressure depend on the initial degree of probe dissociation, which is in turn dependent on the particular surface rather than the charge of the lipid head groups comprising the bilayer. This finding may limit the use of fluorescent probes to determine the exact surface potential. By assuming the change in delta V for proton dissociation from the probe is constant for a given pH, we can calculate the changes in local pH that occur under pressure relative to a neutral or uncharged system. In doing so, we find that the local pH around the probe in bilayers changes very little (approximately 0.1 pH unit or less) in the first 2000 bars. Also, if pressure data are coupled with titration curves, we can determine the change that the bulk pH must undergo to produce the observed change in dissociation seen under pressure.(ABSTRACT TRUNCATED AT 250 WORDS)

Salt effects on histone subunit interactions as studied by fluorescence spectroscopy.

The salt concentration dependence of the aggregation properties of calf thymus and chicken erythrocyte histones has been investigated by using fluorescence spectroscopy. The isolated H2A/H2B and H3/H4 subunit preparations were labeled with 5-(dimethylamino)naphthalene-1- sulfonyl (dansyl). This long-lived fluorescence probe allows for the observation of rotations due to tumbling of the particle and thus is a probe for changes in the size of macromolecular assemblies. The fluorescence polarization and lifetime were measured as a function of salt concentration for these isolated preparations. Next, each labeled preparation was reconstituted with its unlabeled complement, and the salt concentration dependence of histone core octamer interactions was investigated in the same manner. Salt-induced core particle formation was observed by monitoring the dansyl-labeled dimers for both the calf thymus and chicken erythrocyte preparations. Evidence for subunit dissociation of the isolated H2A-H2B preparations was also found, as well as aggregation of the isolated H3/H4 subunits to at least dimers of tetramers. The calf thymus H3/H4 preparation was in aggregated form under all conditions studied, whereas the chicken erythrocyte H3/H4 only formed aggregates at high protein or salt concentrations. We have found evidence that the dimer can displace the tetramer from the higher order aggregate in order to form core particles. Such competition between the subunit interfaces in the histone system suggests that they may play a regulatory role in histone-DNA interactions.

Histone subunit interactions as investigated by high pressure.

High-pressure fluorescence polarization was used to investigate subunit interactions of the histone H2A-H2B dimer and the H3/H4 tetramer isolated from calf thymus (CT) and chicken erythrocyte (CE) chromatin. The proteins were individually labeled with the fluorescent probe 5-(dimethylamino)-naphthalene-1-sulfonate (dansyl or DNS), and the fluorescence polarization was measured as a function of pressure. The long fluorescence lifetime of the probe allows for the observation of global rotations of the protein, the rate of which is dependent upon the aggregation state. From the pressure dependence of the dansyl polarization, the Kd of H2A-H2B dissociation of the CE dimer was found to be approximately 1 X 10(-7) M at 2.0 M NaCl. Lowering the salt concentration to 200 mM slightly stabilized the protein to 6 X 10(-8) M. Our data indicate a small negative volume change for the dissociation of the core particle octamer. The (H3)2(H4)2 tetramer, as was shown in the previous paper (Royer et al., 1989), also formed predominantly dimers of tetramers at higher protein or salt concentrations. In the study presented here, we found the dissociation constant for the H3/H4 octamer to dimer transition to be 1 X 10(-21) M3 (C1/2 = 4 X 10(-8) M) at 2 M NaCl for the CT preparation. Decreasing the salt concentration to 200 mM reduced the stability of the CT H3/H4 octamer to 9 X 10(-21) M3 (C1/2 = 8 X 10(-8) M). The dimer of the CE tetramer also dissociated upon application of pressure in 2 M salt.(ABSTRACT TRUNCATED AT 250 WORDS)

Evaluation of the thermal coefficient of the resistance to fluorophore rotation in model membranes.

The thermal coefficient of the frictional resistance to fluorophore rotation (b), a parameter related to the change in the local viscosity with temperature, was determined for anthroyloxy-fatty acid probes in micelles and dimyristoyl lecithin (DMPC) and dioleoyl lecithin (DOPC) unilamellar and multilamellar vesicles. The value of b and the percent change in anisotropy with temperature (%dA/dT) remained constant with membrane depth and only depended on composition. These parameters were also the same when either in-plane, or in-plane and out-of-plane fluorophore motions were observed. This result indicates that the membranes expand isotropically. The magnitude of b was found to be primarily dependent on the packing of the hydrocarbon chains with higher b values relating to more closely-packed chains. b was responsive to the gel to liquid crystal phase transition of DMPC and the bilayer to hexagonal phase transition of egg-phosphatidylethanolamine. When the enthalpy values for the fluorophore transfer from one phase to another are calculated, the values are larger than those measured by calorimetry and reflect a discrepancy between the microscopic enthalpy experienced by the fluorophore due to a change in environment versus the macroscopic enthalpy of the system as a whole.

The effects of viscosity on gramicidin tryptophan rotational motion.

The rotational amplitude of gramicidin tryptophans was investigated as a function of temperature and viscosity in a variety of solvents using fluorescence spectroscopy. In 80% glycerol-ethanol, gramicidin behavior was similar to that of alpha helical globular proteins. In dioleoyl-phosphatidylcholine (DOPC) and egg-phosphatidylcholine bilayers, the rotational amplitude of the tryptophans remained constant from 5 degrees to 40 degrees C due to the large number of tryptophans participating in intermolecular aromatic ring stacking. In gel phase dimyristoyl-phosphatidylcholine (DMPC), the tryptophan rotations likewise do not respond to temperature and viscosity changes, presumably because of a combination of Trp 9 and 15 stacking and the high viscosity of the membrane. In fluid phase DMPC, stacking becomes disrupted as the temperature increases causing the change in tryptophan amplitude with temperature to be greater than allowed by the membrane. In n-octylglucoside micelles, ring interactions are also broken with heat. We conclude that membrane viscosity regulates both inter- and intramolecular gramicidin interactions but not in a straightforward manner.

The lateral fluidity of erythrocyte membranes. Temperature and pressure dependence.

The pressure and temperature dependence of the lateral and rotational fluidity of erythrocyte membranes was investigated by inserting the excimeric membrane probe 1'-pyrenedodecanoic acid (PDA) into the membranes of intact cells and measuring the probe excimer formation rate and the steady-state polarization of the monomer at pressures up to 2000 atm (2 kbar). At that pressure the lateral diffusivity of PDA was found to decrease by a factor of 10 and its emission anisotropy by a factor of 5 at 22 degrees C. At atmospheric pressure, the local lateral diffusion coefficient of PDA at 2 and 33 degrees C is 1.5 and 4.3 x 10(-8) cm2 s-1, respectively. The activation energy for probe translation was found to decrease from 6 to 3 kcal M-1 in going from atmospheric pressure to 2 kbar, while the entropy decreased by approx. 15 cal M-1 K-1, indicating greater lipid order at the high pressure. The experimental data are consistent with a 'free-area' model for the membrane, analogous to the free-volume model for nonassociated liquids. The lateral diffusivity of PDA was found to be proportional to the free membrane area and linear extrapolation to zero diffusivity indicates that at atmospheric pressure, the fractional free area of the erythrocyte membrane is 6%.

Ligand-induced asymmetry as observed through fluorophore rotations and free energy couplings: application to neurophysin.

Changes that occur in subunit neurophysin structure upon ligand binding were explored by two methods. First, the thermal coefficient of the viscosity around the subunit tyrosine was monitored, which yields information on the environmental flexibility and free rotational space of the fluorophore. Initially, it was determined that the environmental flexibility and the free space around each subunit tyrosine are unperturbed upon dimerization. Binding of the tripeptide analogue of oxytocin causes the once homologous environments of the subunit tyrosines to become drastically different such that one moves onto a closely packed environment whereas the other moves into a region of larger free space. Even though the subunits as seen by each tyrosine are very different, the specific binding sites as seen by the ligands are similar. It was also found that ligand binding is stabilized by ring stacking and that energy transfer occurs between the tyrosine of the ligand and the neurophysin subunit tyrosine. Second, changes in subunit structure upon ligation were also followed by the determination of the order of free energy coupling between ligand binding and oligomerization, which tells how each ligand affects the subunit affinity. Since the binding of ligand is cooperative and induces dimer formation, there is second-order coupling between ligand binding and dimerization and the binding of the second ligand is responsible for the increase in subunit affinity.