Proteolytic degradation of ribonuclease A in the pretransition region of thermally and urea-induced unfolding.

The method of limited proteolysis has proven to be appropriate for the determination of unfolding rate constants (k(U)) of ribonuclease A in the transition region of thermal denaturation [Arnold, U. & Ulbrich-Hofmann, R. (1997) Biochemistry 36, 2166-2172]. The aim of the present paper was to extend this procedure to the pretransition region of thermally and urea-induced denaturation where spectroscopic methods do not allow direct measurement of k(U). The results show that the approach can be applied successfully to denaturing (free energy of unfolding Delta G < 10 kJ.mol(-1)) and to marginally native conditions (Delta G = 10-25 kJ.mol(-1)). Under moderately (Delta G = 25-30 kJ.mol(-1)) and strongly native conditions (Delta G > 30 kJ.mol(-1)), however, the determination of kU was not possible in this way as the proteolytic degradation of ribonuclease A by thermolysin or trypsin was no longer determined by global unfolding. Here, proteolysis proceeds via the native RNase A. In the presence of low concentrations of urea, the rate constants of proteolysis were, surprisingly, smaller than in the absence of urea. As the protease activity has been taken into account, this result points to a local stabilization of the RNase A molecule.     

The membrane dipole potential in a total membrane potential model. Applications to hydrophobic ion interactions with membranes.

The total potential energy profile for hydrophobic ion interactions with lipid bilayers can be written as the sum of four terms: the electrical Born, image and dipole contributions, and a neutral energy term. We introduce a specific model for the membrane dipole potential, treating it as a two-dimensional array of point dipoles located near each membrane-water interface. Together with specific theoretical models for the other energy terms, a total potential profile is developed that successfully describes the complete set of thermodynamic parameters for binding and translocation for the two hydrophobic ion structural analogues, tetraphenylphosphonium (TPP+) and tetraphenylboron (TPB-). A reasonable fit to the data is possible if the dipole potential energy has a magnitude of 5.5 + 0.5 kcal/mol (240 + 20 mV), positive inside, and if the neutral energy contribution for TPP+ and TPB- is -7.0 + 1.0 kcal/mol. These results may also have important implications for small ion interactions with membranes and the energetics of charged groups in membrane proteins.     

Membrane dipole potentials, hydration forces, and the ordering of water at membrane surfaces.

We have compared hydration forces, electrical dipole potentials, and structural parameters of dispersions of dipalmitoylphosphatidylcholine (DPPC) and dihexadecylphosphatidylcholine (DHPC) to evaluate the influence of fatty acid carbonyl groups on phospholipid bilayers. NMR and x-ray investigations performed over a wide range of water concentrations in the samples show, that in the liquid crystalline lamellar phase, the presence of carbonyl groups is not essential for lipid structure and hydration. Within experimental error, the two lipids have identical repulsive hydration forces between their bilayers. The higher transport rate of the negatively charged tetraphenylboron over the positively charged tetraphenylarsonium indicates that the dipole potential is positive inside the membranes of both lipids. However, the lack of fatty acid carbonyl groups in the ether lipid DHPC decreased the potential by (118 +/- 15) mV. By considering the sign of the potential and the orientation of carbonyl groups and headgroups, we conclude that the first layer of water molecules at the lipid water interface makes a major contribution to the dipole potential.     

Electric field strength of membrane lipids from vertebrate species: membrane lipid composition and Na+-K+-ATPase molecular activity

Intramembrane electric field strength is a very likely determinant of the activity of ion-transporting membrane proteins in living cells. In the absence of any transmembrane electrical potential or surface potential, its magnitude is determined by the dipole potential of the membrane's lipid components and their associated water of hydration. Here we have used a fluorometric method to quantify the dipole potential of vesicles formed from lipids extracted from kidney and brain of 11 different animal species from four different vertebrate classes. The dipole potential was compared with the fatty acid composition and with the Na(+)-K(+)-ATPase molecular activity of each preparation. The magnitude of the dipole potential was found to be relatively constant across all animal species, i.e., 236-334 mV for vesicles prepared from the total membrane lipids and 223-256 mV for phospholipids alone. The significantly lower value for phospholipids alone is potentially related to the removal of cholesterol and/or other common soluble lipid molecules from the membrane. Surprisingly, no significant dependence of the dipole potential on fatty acid composition was found. This may, however, be due to concomitant compensatory variations in lipid head group composition. The molecular activity of the Na(+)-K(+)-ATPase was found to increase with increasing dipole potential. The fact that the dipole potential is maintained at a relatively constant value over a wide range of animal species suggests that it may play a fundamental role in ensuring correct ion pump conformation and function within the membrane.     

Measurement of thermodynamic parameters for hydrophobic mismatch 2: intermembrane transfer of a transmembrane helix

Hydrophobic matching between proteins and lipids is essential for the thermodynamic stability of integral membrane proteins. However, there is no direct thermodynamic information available about the intermembrane transfer of proteins between membranes with different hydrophobic thicknesses, which is crucial for understanding hydrophobic mismatch. This article reports the complete set of thermodynamic parameters (DeltaG, DeltaH, DeltaS, and DeltaC(p)) for the intermembrane transfer of the inert hydrophobic model transmembrane helix NBD-(AALALAA)(3)-NH(2) (NBD: 7-nitro-2-1,3-benzoxadiazol-4-yl), which is exchangeable between vesicles, from 1-palmitoyl-2-oleoyl-sn-glycero-3-phosphocholine (POPC) to dimonounsaturated-phosphocholine lipid bilayers with different hydrophobic thicknesses (C14-C22) at 37-58 degrees C. The transfer free energies were calculated from equilibrium values of the extent of helix transfer from donor to acceptor lipid vesicles, as monitored by a decrease in fluorescence resonance energy transfer from the NBD group to a lipid-labeled Rhodamine in the donor upon transfer to the quencher-free acceptor. Under hydrophobic mismatch conditions up to approximately 7 A, the helix partitioning became unfavorable up to +7 kJ mol(-)(1), hampered by an increase in entropic (up to +20 kJ mol(-)(1)) and enthalpic (up to +66 kJ mol(-)(1)) terms in thinner and thicker membranes, respectively. Together with the results that H/D exchange at the membrane interface was accelerated in thinner membranes the obtained thermodynamic parameters were reasonably explained assuming that hydrophobic mismatch induces aqueous exposure or membrane burial of the helix termini, resulting in excess energies originating from the hydration of terminal hydrophobic residues or the unfavorable Born energy of terminal partial charges of the helix macrodipole.     

Quantification and characterization of P-glycoprotein-substrate interactions

It is generally accepted that P-glycoprotein binds its substrates in the lipid phase of the membrane. Quantification and characterization of the lipid-transporter binding step are, however, still a matter of debate. We therefore selected 15 structurally diverse drugs and measured the binding constants from water to the activating (inhibitory) binding region of P-glycoprotein, K(tw(1)) (K(tw(2))), as well as the lipid-water partition coefficients, K(lw). The former were obtained by measuring the concentrations of half-maximum activation (inhibition), K(1) (K(2)), in living NIH-MDR-G185 mouse embryo fibroblasts using a Cytosensor microphysiometer, and the latter were derived from surface activity measurements. This allowed determination of the membrane concentration of drugs at half-maximum P-glycoprotein activation (C(b(1)) = (0.02 to 67) mmol/L lipid), which is much higher than the corresponding aqueous concentration (K(1) = (0.02 to 376) microM). Moreover we determined the free energy of drug binding from water to the activating binding region of the transporter (DeltaG degrees (tw(1)) = (-30 to -54) kJ/mol), the free energy of drug partitioning into the lipid membrane (DeltaG degrees (lw) = (-23 to -34) kJ/mol), and, as the difference of the two, the free energy of drug binding from the lipid membrane to the activating binding region of the transporter (DeltaG degrees (tl(1)) = (-7 to -27) kJ/mol). For the compounds tested DeltaG degrees (tl(1)) was less negative than DeltaG degrees (lw) but varied more strongly. The free energies of substrate binding to the transporter within the lipid phase, DeltaG degrees (tl(1)), are consistent with a modular binding concept, where the energetically most efficient binding module comprises two hydrogen bond acceptor groups.     

Thermodynamics of insertion and self-association of a transmembrane helix: a lipophobic interaction by phosphatidylethanolamine

Thermodynamic parameters for the insertion and self-association of transmembrane helices are important for understanding the folding of helical membrane proteins. The lipid composition of bilayers would significantly affect these fundamental processes, although how is not well understood. Experimental systems using model transmembrane helices and lipid bilayers are useful for measuring and interpreting thermodynamic parameters (ΔG, ΔH, ΔS, and ΔC(p)) for the processes. In this study, the effect of the charge, phase, acyl chain unsaturation, and lateral pressure profile of bilayers on the membrane partitioning of the transmembrane helix (AALALAA)(3) was examined. Furthermore, the effect of 1-palmitoyl-2-oleoyl-sn-glycero-3-phosphatidylethanolamine (POPE) on the thermodynamics for insertion and self-association of the helix in host membranes composed of 1-palmitoyl-2-oleoyl-sn-glycero-3-phosphatidylcholine (POPC) was investigated in detail. Interbilayer transfer of the helix monomer from POPC to POPC/POPE (1/1) bilayers was unfavorable (ΔG = +4.5 ± 2.9 kJ mol(-1) at 35 °C) due to an increase in enthalpy (ΔH = +31.1 ± 2.1 kJ mol(-1)). On the other hand, antiparallel dimerization of the helices in POPC/POPE (1/1) bilayers was enhanced compared with that in POPC bilayers (ΔΔG = -4.9 ± 0.2 kJ mol(-1) at 35 °C) due to a decrease in enthalpy (ΔΔH = -33.2 ± 1.5 kJ mol(-1)). A greater thickness of POPC/POPE bilayers only partially explained the observed effects. The residual effects could be related to changes in other physical properties such as higher lateral pressure in the hydrocarbon core in the PE-containing membrane. The origin of the enthalpy-driven "lipophobic" force that modulates the insertion and association of transmembrane helices will be discussed.     

Thermodynamic properties of nucleotide reductase reactions

Recent thermodynamic measurements have made it possible to calculate the apparent equilibrium constants of the ribonucleoside diphosphate reductase reaction and the ribonucleoside triphosphate reductase reaction with various reducing agents. Third law heat capacity measurements on crystals of d-ribose and other calorimetric measurements make it possible to calculate Delta(f)G degrees for D-ribose and two species of D-ribose 5-phosphate. The experimental value of the apparent equilibrium constant K' for the deoxyribose-phosphate aldolase reaction makes it possible to calculate the standard Gibbs energies of formation Delta(f)G degrees for two protonation states of 2'-deoxy-D-ribose 5-phosphate. This shows that Delta(f)G degrees (2'-deoxy-D-ribose 5-phosphate(2)(-)) - Delta(f)G degrees (D-ribose 5-phosphate(2)(-)) = 147.86 kJ mol(-1) at 298.15 K and zero ionic strength in dilute aqueous solutions. This difference between reduced and oxidized forms is expected to apply to D-ribose, D-ribose 1-phosphate, ribonucleosides, and ribonucleotides in general. This expectation is supported by two other enzyme-catalyzed reactions for which apparent equilibrium constants have been determined. The availability of Delta(f)G degrees values for the species of 2'-deoxy-D-ribose and its derivatives makes it possible to calculate standard transformed Gibbs energies of formation of these reactants, apparent equilibrium constants for their reactions, changes in the binding of hydrogen ions in these reactions, and standard apparent reduction potentials of the half reactions involved as a function of pH and ionic strength at 298.15 K. The apparent equilibrium constant for ADP + thioredoxin(red) = 2'-deoxyADP + H(2)O + thioredoxin(ox) is 1.4 x 10(11) at 298.15 K, pH 7, and 0.25 M ionic strength.     

Electrostatic modeling of ion pores. II. Effects attributable to the membrane dipole potential.

This paper presents calculations of the shielded dipole potential in the interior of a pore piercing a lipid membrane that is at a potential V0 with respect to the aqueous solution. Except in the case of long narrow pores, there is substantial shielding of the membrane dipole potential. The associated dipole field never extends a significant distance into the aqueous region. The fact that the single-channel conductance of gramicidin B is only twice as large in glyceryl monooleate membranes as in phosphatidyl choline (PC) membranes, even though PC is approximately 120 mV more positive with respect to water, is interpreted in terms of the potential energy profile calculated for a gramicidin-like channel. It is demonstrated that the membrane dipole potential can significantly affect channel conductance only if the pore is narrow and if the peak in the potential energy profile occurs in the pore interior.     

Voltage-dependent depolarization of bacterial membranes and artificial lipid bilayers by the peptide antibiotic nisin

The peptide antibiotic nisin is shown to disrupt valinomycin-induced potassium diffusion potentials imposed on intact cells of Staphylococcus cohnii 22. Membrane depolarization occurred rapidly at high diffusion potentials while at low potentials nisin-induced depolarization was slower suggesting that nisin requires a membrane potential for activity. This assumption was proven in experiments with planar lipid bilayers (black lipid membranes). Macroscopic conductivity measurements indicated a voltage-dependent action of nisin. The potential must have a trans-negative orientation with respect to the addition of nisin (added to the cis-side) and a sufficient magnitude (ca. -100 mV). With intact cells the threshold potential was lower (-50 to -80 mV at pH 7.5 and below -50 mV at pH 5.5). Single channel recordings resolved transient multistate pores, strongly resembling those introduced by melittin into artificial bilayers. The pores had diameters in the range of 0.2–1 nm, and lifetimes of few to several hundred milliseconds. The results indicate that nisin has to be regarded as a membrane-depolarizing agent which acts in a voltage-dependent fashion.Abbreviations BLM Black lipid membranes - CCCP carbonyl cyanide m-chlorophenylhydrazone - DOPC dioleoyl phosphatidylcholine - PS phosphatidylserine - TPP⁺ tetraphenylphosphonium cation     

P-glycoprotein senses its substrates and the lateral membrane packing density: consequences for the catalytic cycle

P-glycoprotein (ABCB1) prevents absorption (e.g., blood-brain barrier) or enhances excretion (e.g., kidney) by moving substrates from the cytosolic to the extracellular membrane leaflet at the expense of ATP hydrolysis. It translocates various drugs and functions in membranes exhibiting different lateral packing densities. To gain more functional insight, we measured the temperature dependence of the P-glycoprotein ATPase activity in NIH-MDR1-G185 cell membranes in the absence and presence of three drugs (promazine, verapamil, and PSC833), exhibiting significantly different transporter affinities. Activation enthalpies (Delta H(++)) and entropies ( TDelta S(++)) were derived from Eyring plots. In the absence of drugs, the activation enthalpy and the free energy of activation for P-glycoprotein ATPase activity was determined as Delta H(++) = 92.6 +/- 4.2 kJ/mol and Delta G(++) = 73.1 +/- 7.2 kJ/mol, respectively. Increasing the drug concentration reduced the activation enthalpy, whereby the drug with the highest transporter affinity had the strongest effect (DeltaDelta H(++) = -21%). The free energy of activation decreased for activating (DeltaDelta G(++) = approximately -3.8%) and increased for inhibitory compounds (DeltaDelta G(++) = approximately +0.7%). The drug-specific changes of the free energy of activation are thus barely above thermal energy. A comparison with literature data revealed that a decrease of the lateral membrane packing density reduces the enthalpic and the entropic contribution to the free energy of activation. Although the P-glycoprotein ATPase activity increases only slightly with decreasing lateral membrane packing density, the mode of action changes from strongly entropy-driven at high, to essentially enthalpy-driven at low packing densities. This suggests that the transporter and the membrane form a functional entity.     

Mode of action of the staphylococcinlike peptide Pep 5: voltage-dependent depolarization of bacterial and artificial membranes.

The cationic staphylococcinlike peptide Pep 5 is shown to depolarize bacterial and planar lipid membranes in a voltage-dependent manner. An artificial valinomycin-induced potassium diffusion potential across the cytoplasmic membrane of Staphylococcus cohnii 22 was sufficient to promote Pep 5 action. Thus, evidence is provided that a membrane potential of sufficient magnitude is the only prerequisite for Pep 5 activity. The voltage dependence was elucidated by macroscopic conductance measurements with black lipid membranes. A threshold potential of about -90 to -100 mV, which was deduced from experiments with bacterial cells, could be confirmed. Single pores were resolved which often occur as short-lived bursts and fluctuate among different conductance levels. Pore diameters were calculated ranging from 0.1 to 1 nm. Succinylation of the lysine residues of Pep 5 resulted in prolonged pore lifetimes and maintenance of distinct conductance levels. However, the succinylated peptide required a higher threshold potential, approximately -150 mV, than the native peptide, which is probably the reason for the reduced activity of the modified peptide against intact gram-positive bacteria.     

Cholesterol effect on the dipole potential of lipid membranes

The effect of cholesterol removal by methyl-beta-cyclodextrin on the dipole potential, psi(d), of membrane vesicles composed of natural membrane lipids extracted from the kidney and brain of eight vertebrate species was investigated using the voltage-sensitive fluorescent probe di-8-ANEPPS. Cyclodextrin treatment reduced cholesterol levels by on average 80% and this was associated with an average reduction in psi(d) of 50 mV. Measurements of the effect of a range of cholesterol derivatives on the psi(d) of DMPC lipid vesicles showed that the magnitude of the effect correlated with the component of the sterol's dipole moment perpendicular to the membrane surface. The changes in psi(d) observed could not be accounted for solely by the electric field originating from the sterols' dipole moments. Additional factors must arise from sterol-induced changes in lipid packing, which changes the density of dipoles in the membrane, and changes in water penetration into the membrane, which changes the effective dielectric constant of the interfacial region. In DMPC membranes, the cholesterol-induced change in psi(d) was biphasic, i.e., a maximum in psi(d) was observed at approximately 35-45 mol %, after which psi(d) started to decrease. We suggest that this could be associated with a maximum in the strength of DMPC-cholesterol intermolecular forces at this composition.     

The determination of the membrane ptoential of Chlorella vulgaris. Evidence for electrogenic sugar transport.

From data on the accumulation of tetraphenylphosphonium within Chlorella vulgaris cells, it can be estimated that these cells possess a membrane potential of --120 to --150 mV (inside negative). Under anaerobic conditions as well as in the presence of uncoupling agents the membrane potential drops to about -60 to -80 mV. Nystatin (50 mug/ml) abolishes it almost completely. Since it took more than 1 h before the tetraphenylphosphonium equilibrium was reached, this method could not be used to measure relatively fast transient changes in membrane potential. However, the rate of influx of tetraphenylphosphonium is also directly dependent on membrane potential and can be followed within minutes. Using this phenomenon as an indicator for membrane potential a brief transient depolarisation was detected after the addition of sugars taken up by Chlorella via the proton cotransport system. The depolarisation was absent from cells not induced for sugar uptake and induced cells did not show it with substances not transported, like mannitol. The maximal depolarisation observed amounted to about 70 mV; after 1 min, however, the membrane potential returned to a value about 25 mV less negative than the one before sugars was added. The results demonstrate that sugar uptake in Chlorella is electrogenic. The delta pH plus membrane potential measured for Chlorella completely cover the energy required to explain the 1600-fold accumulation of 6-deoxyglucose experimentally observed.     

Depolarization increases the single-channel conductance and the open probability of crayfish glutamate channels.

We have studied the voltage sensitivity of glutamate receptors in outside-out patches taken from crayfish muscles. We found that single-channel conductance, measured directly at the single-channel level, increases as depolarization rises. At holding potentials from -90 mV to approximately 20 mV, the conductance is 109 pS. At holding potentials positive to 20 mV, the conductance is 213 pS. This increase in single-channel conductance was also observed in cell-attached patches. In addition, desensitization, rise time, and the dose-response curve were all affected by depolarization. To further clarify these multifaceted effects, we evaluated the kinetic properties of single-channel activity recorded from cell-attached patches in hyperpolarization (membrane potential around -75 mV) and depolarization (membrane potential approximately 105 mV). We found that the glutamate dissociation rate constant (k_) was affected most significantly by membrane potential; it declined 6.5-fold under depolarization. The rate constant of channel closing (k(c)) was also significantly affected; it declined 1.8-fold. The rate constant of channel opening (k(o)) declined only 1.2-fold. The possible physiological significance of the depolarization-mediated changes in the above rate constants is discussed.     

Structural transitions in short-chain lipid assemblies studied by (31)P-NMR spectroscopy

The self-assembled supramolecular structures of diacylphosphatidylcholine (diC(n)PC), diacylphosphatidylethanolamine (diC(n)PE), diacylphosphatidyglycerol (diC(n)PG), and diacylphosphatidylserine (diC(n)PS) were investigated by (31)P nuclear magnetic resonance (NMR) spectroscopy as a function of the hydrophobic acyl chain length. Short-chain homologs of these lipids formed micelles, and longer-chain homologs formed bilayers. The shortest acyl chain lengths that supported bilayer structures depended on the headgroup of the lipids. They increased in the order PE (C(6)) < PC (C(9)) < or = PS (C(9) or C(10)) < PG (C(11) or C(12)). This order correlated with the effective headgroup area, which is a function of the physical size, charge, hydration, and hydrogen-bonding capacity of the four headgroups. Electrostatic screening of the headgroup charge with NaCl reduced the effective headgroup area of PS and PG and thereby decreased the micelle-to-bilayer transition of these lipid classes to shorter chain lengths. The experimentally determined supramolecular structures were compared to the assembly states predicted by packing constraints that were calculated from the hydrocarbon-chain volume and effective headgroup area of each lipid. The model accurately predicted the chain-length threshold for bilayer formation if the relative displacement of the acyl chains of the phospholipid were taken into account. The model also predicted cylindrical rather than spherical micelles for all four diacylphospholipid classes and the (31)P-NMR spectra provided evidence for a tubular network that appeared as an intermediate phase at the micelle-to-bilayer transition. The free energy of micellization per methylene group was independent of the structure of the supramolecular assembly, but was -0.95 kJ/mol (-0.23 kcal/mol) for the PGs compared to -2.5 kJ/mol (-0.60 kcal/mol) for the PCs. The integral membrane protein OmpA did not change the bilayer structure of thin (diC(10)PC) bilayers.     

Cholesterol depletion with (2-hydroxypropyl)- β-cyclodextrin modifies the gating of membrane electroporation-induced inward current in pituitary tumor GH3 cells: experimental and analytical studies

The effects of (2-hydroxypropyl)-β-cyclodextrin (HPβCD), a cyclic oligomer, on membrane electroporation-induced inward current (I(MEP)) in pituitary tumor (GH(3)) cells were experimentally and analytically characterized. Depletion of membrane cholesterol by exposing cells to HPβCD (2 mM) increased the activation time constant of delayed rectifier K(+) current. Such maneuver resulted in a significant reduction of I(MEP) density. 2,2'-Azo-bis(2-amidinopropane) dihydrochloride (AAPH), an initiator of free radicals, increased the magnitude of I(MEP). AAPH-stimulated I(MEP) was not reversed by the blockers of Ca(2+)-activated K(+) channels, but by LaCl(3) or MnCl(2). However, in HPβCD-treated cells, the ability of AAPH to enhance I(MEP) was abolished. Under such maneuver, the gating charge of I(MEP) activation was increased by 2 fold, along with a hyperpolarized shift of the activation curve by 30 mV. No change in single-channel conductance of MEP-induced channels during cell exposure to HPβCD was demonstrated. The energy change of I(MEP) in untreated and HPβCD-treated cells was estimated to be -17.7 and -44.8 kJ/mol, respectively, and the perturbation of free energy following HPβCD treatment was -27.1 kJ/mol. Based on an MEP model, cell exposure to HPβCD increased the edge energy of the electropore size. By use of a two barrier-one site barrier model, HPβCD treatment can increase both the peak height and well depth of the barrier profile. Taken together, depletion of membrane cholesterol by HPβCD can elevate the edge energy of pore formation, thereby decreasing the I(MEP) magnitude. The channel-suppressing properties during membrane cholesterol depletion with HPβCD might thus contribute to the underlying mechanisms by which such maneuver alters neuronal or neuroendocrine function.     

Electrophysiology of flounder intestinal mucosa. I. Conductance properties of the cellular and paracellular pathways

We evaluated the conductances for ion flow across the cellular and paracellular pathways of flounder intestine using microelectrode techniques and ion-replacement studies. Apical membrane conductance properties are dominated by the presence of Ba-sensitive K channels. An elevated mucosal solution K concentration, [K]m, depolarized the apical membrane potential (psi a) and, at [K]m less than 40 mM, the K dependence of psi a was abolished by 1-2 mM mucosal Ba. The basolateral membrane displayed Cl conductance behavior, as evidenced by depolarization of the basolateral membrane potential (psi b) with reduced serosal Cl concentrations, [Cl]s. psi b was unaffected by changes in [K]s or [Na]s. From the effect of mucosal Ba on transepithelial K selectivity, we estimated that paracellular conductance (Gp) normally accounts for 96% of transepithelial conductance (Gt). The high Gp attenuates the contribution of the cellular pathway to psi t while permitting the apical K and basolateral Cl conductances to influence the electrical potential differences across both membranes. Thus, psi a and psi b (approximately 60 mV, inside negative) lie between the equilibrium potentials for K (76 mV) and Cl (40 mV), thereby establishing driving forces for K secretion across the apical membrane and Cl absorption across the basolateral membrane. Equivalent circuit analysis suggests that apical conductance (Ga approximately equal to 5 mS/cm2) is sufficient to account for the observed rate of K secretion, but that basolateral conductance (Gb approximately equal to 1.5 mS/cm2) would account for only 50% of net Cl absorption. This, together with our failure to detect a basolateral K conductance, suggests that Cl absorption across this barrier involves KCl co-transport.     

The Intracellular pH of Clostridium paradoxum, an Anaerobic, Alkaliphilic, and Thermophilic Bacterium

When the extracellular pH was increased from 7.6 to 9.8, Clostridium paradoxum, a novel alkalithermophile, increased its pH gradient across the cell membrane ((Delta)pH, pH(infin) - pH(infout)) by as much as 1.3 U. At higher pH values (>10.0), the (Delta)pH and membrane potential ((Delta)(psi)) eventually declined, and the intracellular pH increased significantly. Growth ceased when the extracellular pH was greater than 10.2 and the intracellular pH increased to above 9.8. The membrane potential increased to 110 (plusmn) 8.6 mV at pH 9.1, but the total proton motive force ((Delta)p) declined from about 65 mV at pH 7.6 to 25 mV at pH 9.8. Between the extracellular pH of 8.0 and 10.3, the intracellular ATP concentration was around 1 mM and decreased at lower and higher pH values concomitantly with a decrease in growth rate.     

The major outer membrane protein of Fusobacterium nucleatum (FomA) folds and inserts into lipid bilayers via parallel folding pathways

Membrane protein insertion and folding was studied for the major outer membrane protein of Fusobacterium nucleatum (FomA), which is a voltage-dependent general diffusion porin. The transmembrane domain of FomA forms a beta-barrel that is predicted to consist of 14 beta-strands. Here, unfolded FomA is shown to insert and fold spontaneously and quantitatively into phospholipid bilayers upon dilution of the denaturant urea, which was shown previously only for outer membrane protein A (OmpA) of Escherichia coli. Folding of FomA is demonstrated by circular dichroism and fluorescence spectroscopy, by SDS-polyacrylamide gel electrophoresis, and by single-channel recordings. Refolded FomA had a single-channel conductance of 1.1 nS at 1 M KCl, in agreement with the conductance of FomA isolated from membranes in native form. In contrast to OmpA, which forms a smaller eight-stranded beta-barrel domain, folding kinetics of the larger FomA were slower and provided evidence for parallel folding pathways of FomA into lipid bilayers. Two pathways were observed independent of membrane thickness with two different lipid bilayers, which were either composed of dicapryl phosphatidylcholine or dioleoyl phosphatidylcholine. This is the first observation of parallel membrane insertion and folding pathways of a beta-barrel membrane protein from an unfolded state in urea into lipid bilayers. The kinetics of both folding pathways depended on the chain length of the lipid and on temperature with estimated activation energies of 19 kJ/mol (dicapryl phosphatidylcholine) and 70 kJ/mol (dioleoyl phosphatidylcholine) for the faster pathways.