Rat liver GTP-binding proteins mediate changes in mitochondrial membrane potential and organelle fusion.

The variety of mitochondrial morphology in healthy and diseased cells can be explained by regulated mitochondrial fusion. Previously, a mitochondrial outer membrane fraction containing fusogenic, aluminum fluoride (AlF4)-sensitive GTP-binding proteins (mtg) was separated from rat liver (J. D. Cortese, Exp. Cell Res. 240: 122-133, 1998). Quantitative confocal microscopy now reveals that mtg transiently increases mitochondrial membrane potential (DeltaPsi) when added to permeabilized rat hepatocytes (15%), rat fibroblasts (19%), and rabbit myocytes (10%). This large mtg-induced DeltaPsi increment is blocked by fusogenic GTPase-specific modulators such as guanosine 5'-O-(3-thiotriphosphate), excess GTP (>100 microM), and AlF4, suggesting a linkage between DeltaPsi and mitochondrial fusion. Accordingly, stereometric analysis shows that decreasing DeltaPsi or ATP synthesis with respiratory inhibitors limits mtg- and AlF4-induced mitochondrial fusion. Also, a specific G protein inhibitor (Bordetella pertussis toxin) hyperpolarizes mitochondria and leads to a loss of AlF4-dependent mitochondrial fusion. These results place mtg-induced DeltaPsi changes upstream of AlF4-induced mitochondrial fusion, suggesting that GTPases exert DeltaPsi-dependent control of the fusion process. Mammalian mitochondrial morphology thus can be modulated by cellular energetics.

Multiple conformations of physiological membrane-bound cytochrome c.

One-tenth of cytochrome c (cyt c) remains bound to the inner mitochondrial membrane (IMM) at physiological ionic strength (I; i.e. , I approximately 150 mM), exhibiting decreased electron transport (ET) activity. We now show that this form of membrane-bound cyt c (MB-cyt c) can be obtained in vitro and that binding to membranes at low I generates an additional conformation with higher ET activity. This low I bound form of MB-cyt c (MBL-cyt c) exhibited intrinsic ET rates similar to those of electrostatically bound cyt c (EB-cyt c). The ET activity of IMM-bound MB-cyt c approached slowly that of MBL-cyt c or EB-cyt c, suggesting that MB-cyt c converts to MBL-cyt c while bound to IMM. When maintained at physiological I, both forms of MB-cyt c were released from the membrane, indicating that they convert to an EB-cyt c-like form. This process may be very dynamic in cellular mitochondria, as binding and release for both MB-cyt c forms increased considerably with temperature. I-Dependent binding of MB-cyt c does not require IMM, and it can be reproduced using large or small unilamellar vesicles (SUV). Using SUV-cyt c complexes, we characterized the secondary structure of MB-cyt c and MBL-cyt c by circular dichroism. Conformational analysis revealed that cyt c binding as MB-cyt c decreases its alpha-helical content (70-79%) and increases its beta-sheet up to 135%. The secondary structure of MBL-cyt c was similar to that of EB-cyt c and soluble cyt c, with a modest increase in beta-sheet. Taken together, our experiments suggest that physiological cyt c exists in soluble and membrane-bound conformations with similar ET activity, which may exchange very rapidly, and that soluble hydrophilic proteins can bind transiently to biomembranes.

Novel fluorescence membrane fusion assays reveal GTP-dependent fusogenic properties of outer mitochondrial membrane-derived proteins.

We have shown that fusion of small unilamellar vesicles (SUV) with outer mitochondrial membranes occurs at physiological pH [Cortese et al., 1991, J. Cell Biol., Vol. 113, 1331-1340]. The proteins driving this process could be involved in mitochondrial membrane fusion, which is presently poorly understood. In this study, we release from rat liver mitochondria a soluble protein fraction (SF) that increases fusion at neutral pH measured by membrane fusion assays (MFAs). Since this fusogenic activity was specifically enhanced by GTP, we separate SF by GTP affinity chromatography into: i) a flow-through subfraction (G1) containing numerous proteins with low GTP affinity; and ii) a subfraction (G2) which may contain GTP-binding proteins. A novel array of MFAs is developed to study the fusogenic properties of these fractions, measuring the merging of membranes (membrane-mixing) or the mixing of intravesicular aqueous contents (content-mixing). The MFAs use: a) SUV/large unilamellar vesicles, lacking mitochondrial membranes; b) SUV/mitochondria, reconstituting membrane-mitochondrial interactions; and c) mitochondria/mitochondria, mimicking mitochondrial fusion. The results indicate that: i) G1 contains GTP-independent, in vitro fusogenic proteins that are not sufficient to induce mitochondrial fusion; and ii) G2 contains GTP-dependent proteins that stimulate mitochondrial fusion at neutral pH. The MFAs described here could be used to monitor the isolation of active proteins from these subfractions and to define the mechanism of intermitochondrial membrane fusion.

Stimulation of rat liver mitochondrial fusion by an outer membrane-derived aluminum fluoride-sensitive protein fraction.

In normal livers, hepatocytes contain a large number of spheroidal mitochondria. Mitochondrial morphology changes drastically in liver disease, but the underlying fusion-fission mechanisms are not known. We detected GTP- and aluminum fluoride-dependent membrane fusion events between rat liver mitochondria. Separation of outer mitochondrial membrane-derived proteins led to a subfraction containing a 60-kDa protein band that is detected by specific antibodies directed to common amino acid sequences of the GTP-binding site or carboxyl-terminus of eukaryotic heterotrimeric G-protein alpha subunits. Addition of this subfraction and aluminum fluoride to permeabilized rat hepatocytes triggered a substantial morphological change in hepatic mitochondria, giving them the three-dimensional appearance of a tubulovesicular network. Comparative stereology using electron and confocal microscopy showed that these morphological changes represent true mitochondrial fusion. Addition of aluminum fluoride alone induces a more limited change in mitochondrial morphology, from spheroidal organelles to short rods. Mitochondria maintained their normal membrane potential and overall membrane ultrastructure after all these morphological changes. Our results reveal that mammalian liver mitochondria contain proteins that stimulate mitochondrial fusion and suggest that members of the GTPase superfamily control the normalcy of mitochondrial morphology, which is closely linked to physiological cellular energetics.

Persistence of cytochrome c binding to membranes at physiological mitochondrial intermembrane space ionic strength.

We have shown that cytochrome c (cyt c) diffuses primarily in three dimensions in the intermembrane space (IMS) of intact mitochondria at physiological ionic strength (I). Recently, we found that a small percentage (11.2 +/- 2.1%) of endogenous cyt c remains bound to inner mitochondrial membranes (IMM) at high, physiological I (I = 150 mM), even after extensive washing with solutions at physiological I, overnight dialysis, changes in medium osmolarity, or further purification of IMM at high I using self-generating Percoll gradients. Measurements of heme c/heme a ratios, and electron transport (ET) reactions in which cyt c participates, confirmed the presence of a low amount of this I-resistant, membrane-bound form of cyt c (MB-cyt c), that had one third of the ET activity of electrostatically-bound cyt c (EB-cyt c), and which could not account for maximal ET rates. The amount of MB-cyt c was significantly increased above endogenous MB-cyt c by exposing KCl-washed IMM to increasing concentrations of exogenous cyt c. Also, subjecting large unilamellar vesicles (LUV) to successive cycles of cyt c binding/high I KCl-washes gave progressive increases in MB-cyt c. These protocols allowed in vitro characterization of MB-cyt c. The I at which binding takes place affects the affinity of cyt c for membranes, and oxidized cyt c had a greater intrinsic affinity for IMM or SUV than reduced cyt c. MB-cyt c appears to be bound partially by hydrophobic interactions since MB-cyt c was detected on negatively charged (asolectin) LUV and also on neutral, zwitterionic (phosphatidylcholine) LUV at high I. Consistent with the concentration-dependent changes in MB-cyt c, decreasing the IMS-volume of intact mitochondria (i.e., increasing th endogenous IMS-cyt c concentration) by metabolic or osmotic means increased the amount of MB-cyt c. After cyt c was delivered into the IMS by liposome-mediated low pH-induced fusion, resonance energy transfer showed a time-dependent cyt c-membrane proximity which was consistent with slow exchange of soluble IMS-entrapped cyt c molecules with a population bound to membranes at I = 150 mM. We conclude that, even though the majority of functional IMS-cyt c diffuses in three dimensions, a small portion remains firmly bound on the surface of the IMM under I conditions that are physiological for intact mitochondria. The occurrence of MB-cyt c may reflect an intrinsic conformational flexibility in cyt c, that allows a degree of membrane penetration and the formation of hydrophobic interactions which stabilize the membrane-bound form. The persistence of cyt c-membrane interactions under physiological I conditions indicates that cyt c-mediated ET in the IMS involves both fast (3D-diffusion) and slow (2D-diffusion) pathways for electron transfer.

Motional dynamics of functional cytochrome c delivered by low pH fusion into the intermembrane space of intact mitochondria.

We have investigated the motional dynamics of cytochrome c in the intact, functional rat liver mitochondrion. To do this, functional, FITC-cytochrome c (fluorescein isothiocyanate monoderivatized cytochrome c) was incorporated into the intermembrane space (IMS) of intact mitochondria through encapsulation of cytochrome c into asolectin liposomes followed by low pH-induced fusion of the liposomes with the outer membranes of the mitochondria. A cytochrome c controlled enrichment of between 15%-50% (1800-7200 molecules incorporated per mitochondrion) was obtained. All cytochrome c incorporated, regardless of the quantity, participated in the function of electron transport, indicative of a functional, independent random diffusant. Resonance energy transfer was determined from the IMS-entrapped functional FITC-cytochrome c to octadecylrhodamine B incorporated into the mitochondrial membranes. Resonance energy transfer from FITC-cytochrome c to octadecylrhodamine B in isolated inner or outer mitochondrial membranes (IMM and OMM, respectively) was also measured. We found substantial differences in the effects of ionic strength (I) on the proximity of cytochrome c to isolated IMM and OMM. Interactions with isolated IMM were very dynamic, i.e., very I-dependent, and cytochrome c binding to IMM was significant only at very low I. I-dependent interactions of cytochrome c with isolated OMM were less I-dependent than those for the IMM. However, FITC-cytochrome c was essentially released from IMM and OMM at physiological I. The proximity of FITC-cytochrome c to each mitochondrial membrane after its incorporation into the IMS of intact mitochondria in the condensed configuration was estimated at different external, bulk I using: (a) resonance energy transfer from IMS-entrapped FITC-cytochrome c to octadecylrhodamine B-label evenly distributed in both mitochondrial membranes; and (b) resonance energy transfer from IMS-entrapped FITC-cytochrome c to octadecylrhodamine B-label concentrated in the OMM. Resonance energy transfer showed that the average distance between cytochrome c and the two IMS-membrane surfaces increased with increasing IMS-I, approaching a maximal measurable distance of 85 A at 150 mM I. This result is consistent with a dissociation of FITC-cytochrome c and both membranes of intact mitochondria at physiological I, i.e., when the activity of cytochrome c in electron transport is highest. Our findings reveal a primarily three-dimensional diffusion mode for IMS-cytochrome c during its function in electron transport in intact mitochondria at physiological I, and offer further evidence that mitochondrial electron transport is a process driven by random collisions between its independently diffusing electron transferring, redox components.

The ionic strength of the intermembrane space of intact mitochondria is not affected by the pH or volume of the intermembrane space.

Ionic strength affects the electron transport activity of cytochrome c through its electrostatic interactions with redox partners and membrane lipids. We previously reported (Cortese, J.D., Voglino, A.L. and Hackenbrock, C.R. (1991) J. Cell Biol. 113, 1331-1340) that the ionic strength (I) of the intermembrane space (IMS-I) in isolated, intact condensed mitochondria is similar to the external, bulk I, over a wide range of bulk I. We now consider the possible effects of IMS-pH and IMS-volume, both variable parameters of mitochondrial function in situ, on IMS-I. IMS-pH and IMS-I were measured with pH- and I-sensitive fluorescent probes (highly fluorescent FITC-dextran for IMS-pH and FITC-BSA for IMS-I). These probes were delivered into the IMS of intact mitochondria via probe encapsulation into asolectin vesicles, followed by low pH-induced fusion of the vesicles with the outer membranes of intact mitochondria. IMS-pH was found to be 0.4-0.5 units lower than bulk pH over the pH range 6.0-8.5 for mitochondria with a large IMS-volume separating the two mitochondrial membranes (condensed configuration), and 0-0.2 units lower for mitochondria with a small IMS-volume and membranes closely opposed (orthodox configuration). This small pH difference between IMS-pM and bulk pH did not influence the similarity between IMS-I and bulk I. When the IMS-volume was osmotically decreased, bringing the two mitochondrial membranes in close proximity as in the orthodox configuration, IMS-I followed the bulk I above 10 mM but did not respond to changes in bulk I below 10 mM. The lack of response of the IMS-I below 10 mM indicates that the close proximity of the two mitochondrial membranes excludes ions only at low, nonphysiological I. Since the similarity of IMS-I and bulk I is unaffected by either IMS-pH or IMS-volume above a bulk I of 10 mM, at cytosolic physiological I (i.e., 100-150 mM) cytochrome c can be expected to be a free, three-dimensional diffusant in the IMS irrespective of the pH or volume of the IMS.

Ionic strength of the intermembrane space of intact mitochondria as estimated with fluorescein-BSA delivered by low pH fusion.

The electrostatic interactions of cytochrome c with its redox partners and membrane lipids, as well as other protein interactions and biochemical reactions, may be modulated by the ionic strength of the intermembrane space of the mitochondrion. FITC-BSA was used to determine the relative value of the mitochondrial intermembrane ionic strength with respect to bulk medium external to the mitochondrial outer membrane. FITC-BSA exhibited an ionic strength-dependent fluorescence change with an affinity in the mM range as opposed to its pH sensitivity in the microM range. A controlled, low pH-induced membrane fusion procedure was developed to transfer FITC-BSA encapsulated in asolectin liposomes, to the intermembrane space of intact mitochondria. The fusion procedure did not significantly affect mitochondrial ultrastructure, electron transport, or respiratory control ratios. The extent of fusion of liposomes with the mitochondrial outer membrane was monitored by fluorescence dequenching assays using a membrane fluorescent probe (octadecylrhodamine B) and the soluble FITC-BSA fluorescent probe, which report membrane and contents mixing, respectively. Assays were consistent with a rapid, low pH-induced vesicle-outer membrane fusion and delivery of FITC-BSA into the intermembrane space. Similar affinities for the ionic strength-dependent change in fluorescence were found for bulk medium, soluble (9.8 +/- 0.8 mM) and intermembrane space-entrapped FITC-BSA (10.2 +/- 0.6 mM). FITC-BSA consistently reported an ionic strength in the intermembrane space of the functionally and structurally intact mitochondria within +/- 20% of the external bulk solution. These findings reveal that the intermembrane ionic strength changes as does the external ionic strength and suggest that cytochrome c interactions, as well as other protein interactions and biochemical reactions, proceed in the intermembrane space of mitochondria in the intact cell at physiological ionic strength, i.e., 100-150 mM.

Effect of filamin and controlled linear shear on the microheterogeneity of F-actin/gelsolin gels.

We have previously established [Cortese and Frieden, J. Cell Biol. 107:1477-1487, 1988] that actin gels formed under shear are microheterogeneous. In this study, the effect of cross-linking (by chicken gizzard filamin), severing (by plasma gelsolin), and shear on actin microheterogeneity are investigated using fluorescence photobleaching recovery and video microscopy. We find that filamin and shear form microheterogeneous F-actin:gelsolin gels by different mechanisms. Bundling of actin:gelsolin filaments by filamin can be explained by an increase in the apparent length of the filaments due to interfilament binding, resulting in a decrease of the polymer number concentration at which filaments organize into anisotropic phases. Some intrafilament binding of filamin to actin filaments may also be present, and those filaments coated with filamin immobilize more slowly than actin under the same polymerization conditions. The length of F-actin/gelsolin filaments seems to be a major factor in controlling the extent of bundling relative to network formation. In contrast, the effect of shear on the microheterogeneity of actin:gelsolin filaments is consistent with our previous proposal that shear aligns actin filaments, allowing filament-filament interactions and phase formation to occur. Short filaments are unable to organize into branched actin networks, but they can create large aggregates under low shear. Longer actin filaments will exist as networks with variable levels of branching and are less sensitive to shear. The effect of the intensity of a shear field on the spatial distribution of actin may involve a progressively more random orientation of actin molecules and bundles. A regular pattern develops across the sample at low shear rates (0.04-1.39 s-1), and becomes very irregular at higher shear rates (greater than 10 s-1). We suggest here that actin-binding proteins and shear can control the transition between isotropic networks and anisotropic phases by their effect on apparent length and local filament concentration, and also that this transition can have substantial effects on the resistance of cells to mechanical stress.

Actin polymerization induces a shape change in actin-containing vesicles.

We have encapsulated actin filaments in the presence and absence of various actin-binding proteins into lipid vesicles. These vesicles are approximately the same size as animal cells and can be characterized by the same optical microscopic and mechanical techniques used to study cells. We demonstrate that the initially spherical vesicles can be forced into asymmetric, irregular shapes by polymerization of the actin that they contain. Deformation of the vesicles requires that the actin filaments be on average at least approximately 0.5 micron long as shown by the effects of gelsolin, an actin filament-nucleating protein. Filamin, a filament-crosslinking protein, caused the surfaces of the vesicles to have a smoother appearance. Heterogeneous distribution of actin filaments within the vesicles is caused by interfilament interactions and modulated by gelsolin and filamin. The vesicles provide a model system to study control of cell shape and cytoskeletal organization, membrane-cytoskeleton interactions, and cytomechanics.

Cooperativity in lipid activation of 3-hydroxybutyrate dehydrogenase: role of lecithin as an essential allosteric activator.

3-Hydroxybutyrate dehydrogenase (BDH) is a lecithin-requiring mitochondrial enzyme which catalyzes the interconversion of 3-hydroxybutyrate and acetoacetate with NAD(H) as coenzyme. The purified enzyme devoid of lipid (i.e., the apodehydrogenase or apoBDH) can be reactivated with soluble lecithin or by insertion into phospholipid vesicles containing lecithin. Two different models have been proposed to explain the sigmoidal lipid activation curves. For both models, activation of BDH is assumed to require the binding of two lecithin molecules per functional unit. Activation of soluble enzyme (dimeric form) by short-chain (soluble) lecithin is consistent with a model in which lecithin binding is noncooperative, whereas activation of the membrane-bound enzyme (tetrameric form) indicates cooperativity between the lecithin binding sites. A new comprehensive model is presented in which lecithin is considered to be an essential allosteric activator that shifts the equilibrium between conformational states of the enzyme. Resonance energy transfer data, reflecting NADH binding to membrane-bound and soluble apoBDH, are consistent with such a lecithin-induced conformational change. Apparent dissociation constants for binding of NADH to BDH are approximately 10 microM and approximately 37 microM for BDH activated by bilayer and soluble lecithin, respectively. The maximal fluorescence resonance energy transfer (delta F max) increases with higher mole fraction of lecithin in the bilayer. The largest changes occur between mole fractions 0 and 0.13, thereby correlating with enzymic function. Essentially no binding of NADH is observed in the absence of lecithin.(ABSTRACT TRUNCATED AT 250 WORDS)

Microheterogeneity of actin gels formed under controlled linear shear.

The diffusion coefficients and fluorescence polarization properties of actin subjected to a known shear have been determined both during and after polymerization, using a modification of a cone-plate Wells-Brookfield rheometer that allows monitoring of samples with an epifluorescence microscope. Fluorescence polarization and fluorescence photobleaching recovery experiments using rhodamine-labeled actin as a tracer showed that under conditions of low shear (shear rates of 0.05 s-1), a spatial heterogeneity of polymerized actin was observed with respect to fluorescence intensity and the diffusion coefficients with actin mobility becoming quite variable in different regions of the sample. In addition, complex changes in fluorescence polarization were noted after stopping the shear. Actin filaments of controlled length were obtained using plasma gelsolin (gelsolin/actin molar ratios of 1:50 to 1:300). At ratios of 1:50, neither spatial heterogeneity nor changes in polarization were observed on subjecting the polymerized actin to shear. At ratios of approximately 1:100, a decrease on the intensity of fluorescence polarization occurs on stopping the shear. Longer filaments exhibit spatial micro-heterogeneity and complex changes in fluorescence polarization. In addition, at ratios of 1:100 or 1:300, the diffusion coefficient decreases as the total applied shear increased. This behavior is interpreted as bundling of filaments aligned under shear. We also find that the F-actin translational diffusion coefficients decrease as the total applied shear increases (shear rates between 0.05 and 12.66 s-1), as expected for a cumulative process. When chicken gizzard filamin was added to gelsolin-actin filaments (at filamin/actin molar ratios of 1:300 to 1:10), a similar decrease in the diffusion coefficients was observed for unsheared samples. Spatial microheterogeneity might be related to the effects of the shear field in the alignment of filaments, and the balance between a three-dimensional network and a microheterogeneous system (containing bundles or anisotropic phases) appears related to both shear and the presence of actin-binding proteins.

Noncooperative vs. cooperative reactivation of D-beta-hydroxybutyrate dehydrogenase: multiple equilibria for lecithin binding are determined by the physical state (soluble vs. bilayer) and composition of the phospholipids.

D-beta-Hydroxybutyrate dehydrogenase (BDH) is a lecithin-requiring mitochondrial enzyme that catalyzes the interconversion of beta-hydroxybutyrate and acetoacetate. The purified soluble enzyme devoid of lipid (i.e., the apodehydrogenase) can be reactivated with soluble lecithin or by insertion into phospholipid vesicles containing lecithin. Lipid activation curves have a sigmoidal shape, and two models have been proposed to explain them. We have previously reported that the kinetics of reactivation with short-chain lecithins in the soluble state is consistent with a model in which the enzyme enzyme contains two identical, noninteracting lecithin binding sites, both of which must be occupied to activate the enzyme [noncooperative mechanism; Cortese, J.D., Vidal, J.C., Churchill, P., McIntyre, J.O., & Fleischer, S. (1982) Biochemistry 21, 3899-3908]. More recently a kinetic model involving cooperative interactions between lecithin binding sites was proposed for the reactivation of the membrane-bound enzyme [Sandermann, H., Jr., McIntyre, J.O., & Fleischer, S. (1986) J. Biol. Chem. 261, 6201-6208]. This study reinvestigates the basis for the different conclusions in these two studies. The previous study with soluble lecithins was limited to about 34% of maximal activation compared with mitochondrial phospholipid, due to inactivation of the enzyme at the critical micellar concentration. We could now extend this study to 91% activation by increasing the ethanol concentration. This experimental evidence confirms that the soluble system follows a noncooperative equation. We provide a new kinetic approach to test the cooperative model. A velocity equation is derived for a Hill-type cooperative ligand binding system interacting with a mixture of ligands. This equation predicts a proportionality between an overall weighted cooperative dissociation constant [Kcoop(w)] and a dissociation constant for a single lecithin (PC) species from interacting sites (KPC), regulated by the PC molar fraction (XPC): 1/Kcoop(w) = XPC/KPC. The equation was applied to the data of Sandermann et al. [Sandermann, H., Jr., McIntyre, J.O., & Fleischer, S. (1986) J. Biol. Chem. 261, 6201-6208] as well as to newly obtained data. The results obtained over a wide range of PC molar fractions and different mixtures of bilayer phospholipids fit this equation, confirming the cooperative behavior. We conclude that BDH has a different mode of reactivation depending on the nature of the lipid environment. With soluble lecithin, the activation is noncooperative, whereas in the bilayer, mixtures of phospholipids give cooperative behavior that fits a Hill equation.(ABSTRACT TRUNCATED AT 400 WORDS)

Apparent cooperativity of Ca2+ binding associated with crystallization of Ca2+-binding protein from sarcoplasmic reticulum.

Needle-shaped crystals of the Ca2+-binding protein (CBP) isolated from rabbit skeletal muscle sarcoplasmic reticulum were studied with regard to the influence of Ca2+, K+, and H+ on its solubility and cation binding. The solubility of CBP is sharply decreased with concentration of Ca2+, whereas K+ increased it. Aggregation of the CBP and crystal formation is correlated with the binding of Ca2+. The Ca2+ bound to the crystalline CBP is two to three times higher than that of the soluble form. A strong apparent positive cooperative behavior of Ca2+ binding by CBP was observed concomitant with the shift in equilibrium from the soluble to the crystalline form. From the steepest Hill slope we obtained Hill coefficients of 3.3 for soluble CBP and 14 for the transition between soluble and crystalline forms of CBP. A detailed treatment is presented to validate the applicability of Hill plots for the combined binding and crystallization process. Two-thirds of the Ca2+-binding sites were K+ sensitive and one-third were K+ insensitive. An increase in H+ concentration decreased the Ca2+ binding by crystalline CBP without affecting its solubility, with a pK value of 6.2 determined for this process. These results indicate that the equilibrium between the soluble and crystalline forms of CBP is determined by the amount and nature of the bound cations, Ca2+, K+, and H+. They suggest the possibility that a cycle of aggregation and solubilization of CBP attends the uptake and release of Ca2+ in the sarcoplasmic reticulum, respectively.

Pseudocooperative effects in reactivation of membrane-bound enzymes with phospholipids.

The kinetic mechanism for reactivation of membrane-bound enzymes by lipids is analyzed on the basis of multiple equilibriums between the enzyme (which is assumed to contain n identical, non-interacting binding sites) and the lipid. The rate equations derived when only the fully occupied enzyme species ELn (or ELn and the next most highly occupied species ELn-1, ELn-2,..., ELn-i) is catalytically active can fully account for the apparent positive cooperativity observed in the plots of enzyme activity as a function of phospholipid concentration. A general equation for the cases in which more than one lipid species are simultaneously present in the reaction medium is presented which allows to test whether the binding sites are indeed non-interacting, as well as whether the active species have the same catalytic constant (kcat), regardless the nature of the lipid bound to the binding sites. This analysis demonstrates that, in addition to apparent positive cooperativity, more complex curves resembling mixed cooperativity may be obtained with simple systems when interaction between protein subunits (i.e., association-dissociation equilibriums) are present. Finally, some theoretical problems and pitfalls in the interpretation of the experimental results will be discussed.

Pseudocooperative effects in reactivation of membrane-bound enzymes with phospholipids.

The kinetic mechanism for reactivation of membrane-bound enzymes by lipids is analyzed on the basis of multiple equilibriums between the enzyme (which is assumed to contain n identical, non-interacting binding sites) and the lipid. The rate equations derived when only the fully occupied enzyme species ELn (or ELn and the next most highly occupied species ELn-1, ELn-2,..., ELn-i) is catalytically active can fully account for the apparent positive cooperativity observed in the plots of enzyme activity as a function of phospholipid concentration. A general equation for the cases in which more than one lipid species are simultaneously present in the reaction medium is presented which allows to test whether the binding sites are indeed non-interacting, as well as whether the active species have the same catalytic constant (kcat), regardless the nature of the lipid bound to the binding sites. This analysis demonstrates that, in addition to apparent positive cooperativity, more complex curves resembling mixed cooperativity may be obtained with simple systems when interaction between protein subunits (i.e., association-dissociation equilibriums) are present. Finally, some theoretical problems and pitfalls in the interpretation of the experimental results will be discussed.

Kinetic studies on the reactivation of D-beta-hydroxybutyrate dehydrogenase with mixtures of short-chain lecithins.

D-beta-hydroxybutyrate dehydrogenase, purified as soluble, lipid-free apoenzyme (inactive) from rat liver mitochondria can be reactivated by the short-chain dihexanoyl, diheptanoyl, and dioctanoyl lecithins at the monomeric state, upon formation of a reversible enzyme-lecithin complex. Previous studies with these lecithins suggested that reactivation of the apoenzyme requires the simultaneous occupation of two identical, noninteracting lecithin binding sites via a rapid equilibrium random mechanism. The short-chain lecithins exhibited similar reactivating capacities, differing only in their affinities towards the enzyme. In order to further test that model, the reactivation of the apoenzyme was studied when two or three short-chain lecithins were simultaneously present in the reaction medium. The initial velocities were measured either as a function of the concentration of one lecithin while the other(s) were kept constant, or as a function of the total phospholipid concentration with mixtures of different lecithins at a constant molar ratio. The pertinent equations were derived on the principles of multiple equilibria with identical, noninteracting sites able to be occupied by any of the different lecithins present in the reaction medium, with the doubly occupied enzyme as the only active species. In agreement with the above-proposed model, the results obtained indicates that the molar fraction of the doubly occupied (active) enzyme species can be calculated from equilibrium considerations and that the maximal attainable with the different short-chain lecithins are similar.

Reactivation of D-beta-hydroxybutyrate dehydrogenase with short-chain lecithins: stoichiometry and kinetic mechanism.

D-beta-Hydroxybutyrate dehydrogenase (BDH), purified as soluble, lipid-free apoenzyme (inactive) from either beef heart or rat liver mitochondria, can be reactivated by short-chain lecithins in the monomeric state. The enzyme was reactivated with dihexanoyl- [PC(6:0)], diheptanoyl- [PC(7:0)], and dioctanoyllecithins [PC(8:0)]. The titration curves of enzyme activity as a function of the phospholipid concentration are consistent with a model in which the enzyme contains two identical, noninteracting lecithin binding sites. The simultaneous occupation of these sites (via an equilibrium random mechanism) is required to activate the apoenzyme. Similar results were obtained with both rat liver and beef heart apoenzymes. The maximal velocities obtained with the different lecithins were similar [110-140 mumol of NAD+ reduced min-1 (mg of protein)-1]. The KL values (the apparent dissociation constants of the lecithin-site complexes) were 1.2 X 10(-4) M [PC(8:0)], 1.5 X 10(-3) M [PC(7:0)], and 4.5 X 10(-3) M [PC(6:0)] at 37 degrees C. This was confirmed by using phospholipase A2 to compete with the dehydrogenase for the lecithin monomers. Comparison of the delta G degrees values for complex formation with the different lecithins shows an average contribution of approximately 2.4 kJ/mol (0.9RT) per CH2 group. The interaction of the apolar moiety of lecithin with the protein seems to be essential for effective binding of phosphatidylcholine to apoBDH. The delta G degrees values, when combined with the estimated delta H degrees values, suggest that the binding of lecithin to the apoenzyme is approximately 60% enthalpy and approximately 40% entropy driven.