Volume Reabsorption, Transepithelial Potential Differences, and Ionic Permeability Properties in Mammalian Superficial Proximal Straight Tubules

This paper describes experiments designed to evaluate Na⁺ and Cl^- transport in isolated proximal straight tubules from rabbit kidneys. When the perfusing solution was Krebs-Ringer buffer with 25 mM HCO₃^- (KRB) and the bath contained KRB plus 6% albumin, net volume reabsorption (J_v, nl min^-1 mm^-1 was -0.46 ± 0.03 (SEM); V_e, the spontaneous transepithelial potential difference, was -1.13 ± 0.05 mV, lumen negative. Both J_v, and V_e, were reduced to zero at 21°C or with 10^-4 M ouabain, but J_v, was not HCO₃^- dependent. Net Na⁺ reabsorption, measured as the difference between ²²Na⁺ fluxes, lumen to bath and bath to lumen, accounted quantitatively for volume reabsorption, assuming the latter to be an isotonic process, and was in agreement with the difference between lumen to bath ²²Na⁺ fluxes during volume reabsorption and at zero volume flow. The observed flux ratio for Na⁺ was 1.46, and that predicted for a passive process was 0.99; thus, Na⁺ reabsorption was rationalized in terms of an active transport process. The Cl^- concentration of tubular fluid rose from 113.6 to 132.3 mM during volume reabsorption. Since V_e, rose to +0.82 mV when tubules were perfused with 138.6 mM Cl^- solutions, V_e may become positive when tubular fluid Cl^- concentrations rise during volume reabsorption. The permeability coefficients P_Na and P_Cl computed from tracer fluxes were, respectively, 0.23 x 10^-4 and 0.73 x 10^-4 cm s^-1. A P_Na/P_Cl ratio of 0.3 described NaCl dilution potentials at zero volume flow. The magnitudes of the potentials were the same for a given NaCl gradient in either direction and P_Na/P_Cl was constant in the range 32–139 mM NaCl. We infer that the route of passive ion permeation was through symmetrical extracellular interfaces, presumably tight junctions, characterized by neutral polar sites in which electroneutrality is maintained by mobile counterions.     

Characterization of esophageal desalination in the seawater eel,Anguilla japonica

To characterize mechanisms of esophageal desalination, osmotic water permeability and ion fluxes were measured in the isolated esophagus of the seawater eel. The osmotic permeability coefficient in the seawater eel esophagus was 2·10^-4 cm·s^-1. This value was much lower than those in tight epithelial, although the eel esophagus is a leaky epithelium with a tissue resistance of 77 ohm·cm^-2. When the esophagus was bathed in normal Ringer solutions on both sides no net ion and water fluxes were observed. However, when mucosal NaCl concentration was increased by a factor of 3, Na⁺ und Cl^- ions were transferred from mucosa to serosa (desalination). If only Na⁺ or Cl^- concentration in the mucosal fluid was increased by a factor of 3, net Na⁺ and Cl^- fluxes were reduced to 30–40%, indicating that 60–70% of the net Na⁺ and Cl^- fluxes are coupled mutually. The coupled NaCl transport seems to be effective in desalting the luminal high NaCl. The remaining 30–40% of the total Na⁺ and Cl^- fluxes seems to be due to a simple diffusion, because these components are independent of each other and follow their electrochemical gradients, and also because these fluxes remain even after treatment with NaCN or ouabain. A half of the coupled NaCl transport could be explained by a Na⁺/H⁺–Cl^-/HCO ₃ ^- double exchanger on the apical membrane of the esophageal epithelium, because mucosal amiloride and 4.4-diisothiocyanatostilbene-2,2-disulphonic acid inhibited the net Na⁺ and Cl^- fluxes by approximately 30%. The other half of the coupled NaCl transport, which follows their electrochemical gradients, still remains to be explained.Abbreviations DIDS 4,4-diisothiocyanatostilbene-2,2-disulphonic acid - NMDG N-methyl-d-glucosamine - P _Cl Cl^- permeability coefficient - PD transepithelial potential difference - P _Na Na⁺ permeability coefficient - P _osm osinotic permeability coefficient - TALH thick ascending limb of Henle's loop     

Sodium, Potassium, and Chloride Fluxes in Intercostal Muscle from Normal Goats and Goats with Hereditary Myotonia

In isolated bundles of external intercostal muscle from normal goats and goats with hereditary myotonia the following were determined: concentrations and unidirectional fluxes of Na⁺, K⁺, and Cl^-, extracellular volume, water content, fiber geometry, and core-conductor constants. No significant difference between the two groups of preparations was found with respect to distribution of fiber size, intracellular concentrations of Na⁺ or Cl^-, fiber water, resting membrane potential, or overshoot of action potential. The intracellular Cl^- concentration in both groups of preparations was 4 to 7 times that expected if Cl^- were distributed passively between intracellular and extracellular water. The membrane permeability to K (P_K) calculated from efflux data was (a) at 38°C, 0.365 x 10^-6 cm sec^-1 for normal and 0.492 x 10^-6 for myotonic muscle, and (b) at 25°C, 0.219 x 10^-6 for normal and 0.199 x 10^-6 for myotonic muscle. From Cl^- washout curves of normal muscle usually only three exponential functions could be extracted, but in every experiment with myotonic muscle there was an additional, intermediate component. From these data PP_cl could be calculated; it was 0.413 x 10^-6 cm sec^-1 for myotonic fibers and was 0.815 x 10^-6 cm sec^-1 for normal fibers. The resting membrane resistance of myotonic fibers was 4 to 6 times greater than that of normal fibers.     

Decreased K+ conductance produced by Ba++ in frog sartorius fibers

The action of Ba⁺⁺ on membrane potential (E_m) and resistance (R_m) of frog (R. pipiens) sartorius fibers was studied. In normal Cl^- Ringer''s, Ba⁺⁺ (<9 mM) did not depolarize or induce contractions, but increased R_m slightly above the control value of 3.8 ± 0.6 KΩ-cm². In Cl^--free Ringer''s (methane sulfonate) R_m was 28.8 ± 2.8 KΩ-cm², and low concentrations of Ba⁺⁺ (0.05–5.0 mM) depolarized and induced spontaneous contractions (fibrillation), even in tetrodotoxin. To stop disturbance of the microelectrodes, contractions were prevented by using two Cl^--free solutions: (a) twice hypertonic with sucrose (230 mM), or (b) high K⁺ (83 mM) partially replacing Na⁺. In the hypertonic solution, the fiber diameters decreased, E_m increased slightly, and R_m decreased to 9.0 ± 0.6 KΩ-cm² (perhaps due to swelling of sarcotubules). Ba⁺⁺ (0.5 mM) rapidly increased R_m to 31.3 ± 3.8, decreased E_m (e.g., to -30 mv), and induced spontaneous "action potentials;" Sr⁺⁺ had no effect. In the high K⁺ solution, the fibers were nearly completely depolarized, and R_m was decreased markedly to 1.5 ± 0.2 KΩ-cm²; Ba⁺⁺ increased R_m to 6.7 ± 0.5 KΩ-cm². The Ba⁺⁺ actions usually began within 0.5 min and reached a maximum within 5 min. Addition of SO₄ ⁼, to precipitate the Ba⁺⁺, rapidly reversed the increase in R_m. Ba⁺⁺ must act by decreasing K⁺ conductance (g_K). In Cl^- Ringer''s, the high g_Cl/g_K ratio masked the effect of Ba⁺⁺ on g_K. Thus, small concentrations of Ba⁺⁺ specifically and rapidly decrease g_K.     

The effect of amphotericin B on the water and nonelectrolyte permeability of thin lipid membranes

This paper reports the effects of amphotericin B, a polyene antibiotic, on the water and nonelectrolyte permeability of optically black, thin lipid membranes formed from sheep red blood cell lipids dissolved in decane. The permeability coefficients for the diffusion of water and nonelectrolytes (P_DDi) were estimated from unidirectional tracer fluxes when net water flow (J_w) was zero. Alternatively, an osmotic water permeability coefficient (P_f) was computed from J_w when the two aqueous phases contained unequal solute concentrations. In the absence of amphotericin B, when the membrane solutions contained equimolar amounts of cholesterol and phospholipid, P_f was 22.9 ± 4.6 µsec^-1 and P _DDHDH2O was 10.8 ± 2.4 µsec^-1. Furthermore, P_DDi was < 0.05 µsec^-1 for urea, glycerol, ribose, arabinose, glucose, and sucrose, and σ_i, the reflection coefficient of each of these solutes was one. When amphotericin B (10^-6 M) was present in the aqueous phases and the membrane solutions contained equimolar amounts of cholesterol and phospholipid, P _DDHDH2O was 18.1 ± 2.4 µsec^-1; P_f was 549 ± 143 µsec^-1 when glucose, sucrose, and raffinose were the aqueous solutes. Concomitantly, P_DDi varied inversely, and σ_i directly, with the effective hydrodynamic radii of the solutes tested. These polyene-dependent phenomena required the presence of cholesterol in the membrane solutions. These data were analyzed in terms of restricted diffusion and filtration through uniform right circular cylinders, and were compatible with the hypothesis that the interactions of amphotericin B with membrane-bound cholesterol result in the formation of pores whose equivalent radii are in the range 7 to 10.5 A.     

Patch Clamp on the Luminal Membrane of Exocrine Gland Acini from Frog Skin (Rana esculenta) Reveals the Presence of Cystic Fibrosis Transmembrane Conductance Regulator–like Cl? Channels Activated by Cyclic AMP

Chloride channels in the luminal membrane of exocrine gland acini from frog skin (Rana esculenta) constituted a single homogeneous population. In cell-attached patches, channels activated upon exposure to isoproterenol, forskolin, or dibutyryl-cAMP and isobutyl-1-methyl-xanthine rectified in the outward direction with a conductance of 10.0 ± 0.4 pS for outgoing currents. Channels in stimulated cells reversed at 0 mV applied potential, whereas channels in unstimulated cells reversed at depolarized potentials (28.1 ± 6.7 mV), indicating that Cl⁻ was above electrochemical equilibrium in unstimulated, but not in stimulated, cells. In excised inside-out patches with 25 mM Cl⁻ on the inside, activity of small (8-pS) linear Cl⁻-selective channels was dependent upon bath ATP (1.5 mM) and increased upon exposure to cAMP-dependent protein kinase. The channels displayed a single substate, located just below 2/3 of the full channel amplitude. Halide selectivity was identified as P_Br > P_I > P_Cl from the Goldman equation; however, the conductance sequence when either halide was permeating the channel was G_Cl > G_Br >> G_I. In inside-out patches, the channels were blocked reversibly by 5-nitro-2-(3-phenylpropylamino)benzoic acid, glibenclamide, and diphenylamine-2-carboxylic acid, whereas 4,4-diisothiocyanatostilbene-2,2-disulfonic acid blocked channel activity completely and irreversibly. Single-channel kinetics revealed one open state (mean lifetime = 158 ± 72 ms) and two closed states (lifetimes: 12 ± 4 and 224 ± 31 ms, respectively). Power density spectra had a double-Lorentzian form with corner frequencies 0.85 ± 0.11 and 27.9 ± 2.9 Hz, respectively. These channels are considered homologous to the cystic fibrosis transmembrane conductance regulator Cl⁻ channel, which has been localized to the submucosal skin glands in Xenopus by immunohistochemistry (Engelhardt, J.F., S.S. Smith, E. Allen, J.R. Yankaskas, D.C. Dawson, and J.M. Wilson. 1994. Am. J. Physiol. 267: C491–C500) and, when stimulated by cAMP-dependent phosphorylation, are suggested to function in chloride secretion.     

Halide Permeation in Wild-Type and Mutant Cystic Fibrosis Transmembrane Conductance Regulator Chloride Channels

Permeation of cystic fibrosis transmembrane conductance regulator (CFTR) Cl⁻ channels by halide ions was studied in stably transfected Chinese hamster ovary cells by using the patch clamp technique. In cell-attached patches with a high Cl⁻ pipette solution, the CFTR channel displayed outwardly rectifying currents and had a conductance near the membrane potential of 6.0 pS at 22°C or 8.7 pS at 37°C. The current–voltage relationship became linear when patches were excised into symmetrical, N-tris(hydroxymethyl)methyl-2-aminomethane sulfonate (TES)-buffered solutions. Under these conditions, conductance increased from 7.0 pS at 22°C to 10.9 pS at 37°C. The conductance at 22°C was ∼1.0 pS higher when TES and HEPES were omitted from the solution, suggesting weak, voltage-independent block by pH buffers. The relationship between conductance and Cl⁻ activity was hyperbolic and well fitted by a Michaelis-Menten–type function having a K _m of ∼38 mM and maximum conductance of 10 pS at 22°C. Dilution potentials measured with NaCl gradients indicated high anion selectivity (P_Na/P_Cl = 0.003–0.028). Biionic reversal potentials measured immediately after exposure of the cytoplasmic side to various test anions indicated P_I (1.8) > P_Br (1.3) > P_Cl (1.0) > P_F (0.17), consistent with a “weak field strength” selectivity site. The same sequence was obtained for external halides, although inward F⁻ flow was not observed. Iodide currents were protocol dependent and became blocked after 1–2 min. This coincided with a large shift in the (extrapolated) reversal potential to values indicating a greatly reduced I⁻/Cl⁻ permeability ratio (P_I/P_Cl < 0.4). The switch to low I⁻ permeability was enhanced at potentials that favored Cl⁻ entry into the pore and was not observed in the R347D mutant, which is thought to lack an anion binding site involved in multi-ion pore behavior. Interactions between Cl⁻ and I⁻ ions may influence I⁻ permeation and be responsible for the wide range of P_I/P_Cl ratios that have been reported for the CFTR channel. The low P_I/P_Cl ratio usually reported for CFTR only occurred after entry into an altered permeability state and thus may not be comparable with permeability ratios for other anions, which are obtained in the absence of iodide. We propose that CFTR displays a “weak field strength” anion selectivity sequence.     

Osmosis in Cortical Collecting Tubules : ADH-Independent Osmotic Flow Rectification

The present experiments were designed to evaluate the effects of varying the osmolality of luminal solutions on the antidiuretic hormone (ADH)-independent water and solute permeability properties of isolated rabbit cortical collecting tubules. In the absence of ADH, the osmotic water permeability coefficient (cm s^–1) P_f^l→b, computed from volume flows from hypotonic lumen to isotonic bath, was 20 ± 4 x 10^–4 (SEM); the value of P_f^b→l in the absence of ADH, computed from volume flows from isotonic bath to hypertonic lumen, was 88 ± 15 x 10^–4 cm s^–1. We also measured apparent urea permeability coefficients (cm s^–1) from ¹⁴C-urea fluxes from lumen to bath (P_DDurea^l→b) and from bath to lumen (P_DDurea^b→l). For hypotonic luminal solutions and isotonic bathing solutions, P_DDurea^l→b was 0.045 ± 0.004 x 10^–4 and was unaffected by ADH. The ADH-independent values of P_DDurea^l→b and P_urea^b→l were, respectively, 0.216 ± 0.022 x 10^–4 cm s^–1 and 0.033 ± 0.002 x 10^–4 cm s^–1 for isotonic bathing solutions and luminal solutions made hypertonic with urea, i.e., there was an absolute increase in urea permeability and asymmetry of urea fluxes. Significantly, P_DDurea^l→b did not rise when luminal hypertonicity was produced by sucrose; and, bathing fluid hypertonicity did not alter tubular permeability to water or to urea. We interpret these data to indicate that luminal hypertonicity increased the leakiness of tight junctions to water and urea but not sucrose. Since the value of P_f^b→l in the absence of ADH, when tight junctions were open to urea, was approximately half of the value of P_f^l→b in the presence of ADH, when tight junctions were closed to urea, we conclude that tight junctions are negligible paracellular shunts for lumen to bath osmosis with ADH. These findings, together with those in the preceding paper, are discussed in terms of a solubility-diffusion model for water permeation in which ADH increases water solubility in luminal plasma membranes.     

The Interaction of Polyene Antibiotics with Thin Lipid Membranes

Optically black, thin lipid membranes prepared from sheep erythrocyte lipids have a high dc resistance (R_m ≅ 10⁸ ohm-cm²) when the bathing solutions contain NaCl or KCl. The ionic transference numbers (T_i) indicate that these membranes are cation-selective (T _Na ≅ 0.85; T _Cl ≅ 0.15). These electrical properties are independent of the cholesterol content of the lipid solutions from which the membranes are formed. Nystatin, and probably amphotericin B, are cyclic polyene antibiotics containing ≈36 ring atoms and a free amino and carboxyl group. When the lipid solutions used to form membranes contained equimolar amounts of cholesterol and phospholipid, these antibiotics reduced R_m to ≈10² ohm-cm²; concomitantly, T _Cl became ≅0.92. The slope of the line relating log R_m and log antibiotic concentration was ≅4.5. Neither nystatin (2 x 10^-5 M) nor amphotericin B (2 x 10^-7 M) had any effect on membrane stability. The antibiotics had no effect on R_m or membrane permselectivity when the lipids used to form membranes were cholesterol-depleted. Filipin (10^-5 M), an uncharged polyene with 28 ring atoms, produced striking membrane instability, but did not affect R_m or membrane ionic selectivity. These data suggest that amphotericin B or nystatin may interact with membrane-bound sterols to produce multimolecular complexes which greatly enhance the permeability of such membranes for anions (Cl^-, acetate), and, to a lesser degree, cations (Na⁺, K⁺, Li⁺).     

An analysis of unstirred layers in series with "tight" and "porous" lipid bilayer membranes

The present experiments were designed to evaluate the effective thickness of the unstirred layers in series with native and porous (i.e., in the presence of amphotericin B) lipid bilayer membranes and, concomitantly, the respective contributions of membranes and unstirred layers to the observed resistances to the diffusion of water and nonelectrolytes between aqueous phases. The method depended on measuring the tracer permeability coefficients for the diffusion of water and nonelectrolytes (P_DDi, cm sec^-1) when the aqueous phase viscosity (η) was increased with solutes having a unity reflection coefficient, such as sucrose or dextran. The effective thickness of the unstirred layers (α^t, cm) and the true, or membrane, permeability coefficients for diffusion of water and nonelectrolytes (P_mmi, cm sec^-1) were computed from, respectively, the slope and intercept of the linear regression of 1/P_DDi on η. In both the native and porous membranes, α^t was approximately 110 x 10^-4 cm. The ratio of P_f, the osmotic water permeability coefficient (cm sec^-1) to P_mmH2O was 1.22 in the native membranes and 3.75 in the porous membranes. For the latter, the effective pore radius, computed from Poiseuille's law, was approximately 5.6 A. A comparison of P_mmi and P_DDi, indicated that the porous membranes accounted for 16, 25, and 66% of the total resistance to the diffusion of, respectively, H₂O, urea, and glycerol, while the remainder was referable to the unstirred layers.     

A study of lipid bilayer membrane stability using precise measurements of specific capacitance

A method is described for measuring the specific capacitance (C_m) of lipid bilayer membranes with an estimated experimental error of only 1%. The gross capacitance was measured with an AC Wheatstone bridge and a photographic technique was used to determine the area of thin membrane. The results of measurements on oxidized cholesterol-decane membranes formed in 1 × 10^-2 M KCl show that C_m depends upon temperature, voltage, time, and the age of the bulk membrane solutions. For a freshly thinned membrane (from 5 week old solution), C_m increases exponentially from an initial value of 0.432 ±0.021 (SD) μF/cm² with a time constant of ~15 min. A 100 mv potential applied across the membrane for 10-20 min prior to making measurements eliminated this time dependence and produced final-state membranes. C_m of final-state membranes depends upon applied voltage (V_a) and obeys the equation C_m = C₀ + βV_a² where V_a V_DC + V^rms_AC. C₀ and β depend upon temperature; C₀ decreases linearly with temperature while β increases linearly. At 20°C, C₀ = 0.559 ±0.01 (SD) μF/cm² and β = 0.0123 ±0.0036 (SD) (μF/cm²)/(mv²) and at 34°C, C₀ = 0.472 ±0.01 and β = 0.0382 ±0.0039. These variations in C_m are interpreted as resulting from thickness changes. The possibility that they result from diffuse layer and/or membrane dielectric phenomena is discussed and found to be unlikely. The results are discussed in terms of membrane stability by constructing hypothetical potential energy vs. thickness curves.     

Electrodiffusion,Barrier, and Gating Analysis of DIDS-insensitive Chloride Conductance in Human Red Blood Cells Treated with Valinomycin or Gramicidin

Current-voltage curves for DIDS-insensitive Cl⁻ conductance have been determined in human red blood cells from five donors. Currents were estimated from the rate of cell shrinkage using flow cytometry and differential laser light scattering. Membrane potentials were estimated from the extracellular pH of unbuffered suspensions using the proton ionophore FCCP. The width of the Gaussian distribution of cell volumes remained invariant during cell shrinkage, indicating a homogeneous Cl⁻ conductance among the cells. After pretreatment for 30 min with DIDS, net effluxes of K⁺ and Cl⁻ were induced by valinomycin and were measured in the continued presence of DIDS; inhibition was maximal at ∼65% above 1 μM DIDS at both 25°C and 37°C. The nonlinear current-voltage curves for DIDS-insensitive net Cl⁻ effluxes, induced by valinomycin or gramicidin at varied [K⁺]_o, were compared with predictions based on (1) the theory of electrodiffusion, (2) a single barrier model, (3) single occupancy, multiple barrier models, and (4) a voltage-gated mechanism. Electrodiffusion precisely describes the relationship between the measured transmembrane voltage and [K⁺]_o. Under our experimental conditions (pH 7.5, 23°C, 1–3 μM valinomycin or 60 ng/ml gramicidin, 1.2% hematocrit), the constant field permeability ratio P_K/P_Cl is 74 ± 9 with 10 μM DIDS, corresponding to 73% inhibition of P_Cl. Fitting the constant field current-voltage equation to the measured Cl⁻ currents yields P _Cl = 0.13 h⁻¹ with DIDS, compared to 0.49 h⁻¹ without DIDS, in good agreement with most previous studies. The inward rectifying DIDS-insensitive Cl⁻ current, however, is inconsistent with electrodiffusion and with certain single-occupancy multiple barrier models. The data are well described either by a single barrier located near the center of the transmembrane electric field, or, alternatively, by a voltage-gated channel mechanism according to which the maximal conductance is 0.055 ± 0.005 S/g Hb, half the channels are open at −27 ± 2 mV, and the equivalent gating charge is −1.2 ± 0.3.     

Bicarbonate-Chloride Exchange in Erythrocyte Suspensions: Stopped-Flow pH Electrode Measurements

A pH-sensitive glass electrode was used in a temperature-controlled stopped-flow rapid reaction apparatus to determine rates of pH equilibration in red cell suspensions. The apparatus requires less than 2 ml of reactants. The electrode is insensitive to pressure and flow variations, and has a response time of < 5 ms. A 20% suspension of washed fresh human erythrocytes in saline at pH 7.7 containing NaHCO₃ and extracellular carbonic anhydrase is mixed with an equal volume of 30 mM phosphate buffer at pH 6.7. Within a few milliseconds after mixing, extracellular HCO₃^- reacts with H⁺ to form CO₂, which enters the red cells and rehydrates to form HCO₃^-, producing an electrochemical potential gradient for HCO₃^- from inside to outside the cells. HCO₃^- then leaves the cells in exchange for Cl^-, and extracellular pH increases as the HCO₃^- flowing out of the cells reacts with H⁺. Flux of HCO₃^- is calculated from the dpH/dt during HCO₃^--Cl^- exchange, and a velocity constant is computed from the flux and the calculated intracellular and extracellular [HCO₃^-]. The activation energy for the exchange process is 18.6 kcal/mol between 5°C and 17°C (transition temperature), and 11.4 kcal/mol from 17°C to 40°C. The activation energies and transition temperature are not significantly altered in the presence of a potent anion exchange inhibitor (SITS), although the fluxes are markedly decreased. These findings suggest that the rate-limiting step in red cell anion exchange changes at 17°C, either because of an alteration in the nature of the transport site or because of a transition in the physical state of membrane lipids affecting protein-lipid interactions.     

Electrical Properties and Acetylcholine Sensitivity of Singly and Multiply Innervated Avian Muscle Fibers

Membrane constants and distribution of acetylcholine (ACh) receptors were determined for multiply innervated fibers of the anterior latissimus dorsi (ALD) and singly innervated fibers of the posterior latissimus dorsi (PLD) muscles of 3–6 month old chickens. The values of the various membrane constants were: length constant, 1.78 mm (mean) in ALD, 0.68 mm in PLD; time constant, 35 msec in ALD, 3.7 msec in PLD; transverse membrane resistance, 4388 Ω cm² in ALD, 561 Ω cm² in PLD; and membrane capacitance, 8.2 µF/cm² in ALD, 7.0 µF/cm² in PLD. Peaks of ACh sensitivity occurred at intervals of ca. 740 µ on ALD fibers with a low sensitivity remaining between peaks. Only one peak of ACh sensitivity was detected on PLD fibers. The maximum ACh sensitivity found was 5 ± 4 mv/ncoul for fibers of the ALD and 77 ± 60 mv/ncoul for fibers of the PLD. The distance over which this sensitivity fell to 0.1 was ca. 225 µ in the ALD and 140 µ in the PLD. The membranes of these two muscle fiber types differ widely regarding some electrical properties and the disposition of ACh-sensitive receptor sites.     

The Influence of the Intracellular Potential on Potassium Uptake by Beetroot Tissue

Intracellular potentials were measured in beetroot tissue during the steady-state uptake of K⁺ from various solutions. In solutions containing bicarbonate, the membrane potential becomes up to 70 mv more negative than the estimated equilibrium potential for K⁺. The uptake of K⁺ from such solutions is correlated with variations in the potential, both when the bicarbonate concentration is changed and also when the metabolic activity of the tissue is changed by washing in water for various periods. However, the estimated permeability to K⁺ varies from 0.4 x 10^-7 to 1.5 x 10^-7 cm·sec^-1. It is postulated that the change of potential arises from the metabolic transport of HCO₃^- into the cell or H⁺ outwards, and that the associated uptake of K⁺ is partly or entirely by passive diffusion across the cell membrane. In contrast, K⁺ uptake from KCl solutions is not accompanied by any significant change in the membrane potential, which remains relatively close to the K⁺ equilibrium potential. In solutions containing both KHCO₃ and KCl, it appears that an amount of K⁺ equal to the influx of Cl^- is taken up independently of the potential, while the component of K⁺ uptake which is not balanced by Cl^- uptake is related to the potential in the manner described. These results suggest that K⁺ uptake is linked to Cl^- uptake in an electrically neutral active transport process.     

Water transport in the midrib tissue of maize leaves : direct measurement of the propagation of changes in cell turgor across a plant tissue

Water movement across plant tissues occurs along two paths: from cell-to-cell and in the apoplasm. We examined the contribution of these two paths to the kinetics of water transport across the parenchymatous midrib tissue of the maize (Zea mays L.) leaf. Water relations parameters (hydraulic conductivity, Lp; cell elastic coefficient, ε; half-time of water exchange for individual cells, T_½) of individual parenchyma cells determined with the pressure probe varied in different regions of the midrib. In the adaxial region, Lp = (0.3 ± 0.3)·10⁻⁵ centimeters per second per bar, ε = 103 ± 72 bar, and T_½ = 7.9 ± 4.8 seconds (n = seven cells); whereas, in the abaxial region, Lp = (2.5 ± 0.9)·10⁻⁵ centimeters per second per bar, ε = 41 ± 9 bar, and T_½ = 1.3 ± 0.5 seconds (n = 7). This zonal variation in Lp, ε, and T_½ indicates that tissue inhomogeneities exist for these parameters and could have an effect on the kinetics of water transport across the tissue.

The diffusivity of the tissue to water (D_t) obtained from the sorption kinetics of rehydrating tissue was D_t = (1.1 ± 0.4)·10⁻⁶ square centimeters per second (n = 6). The diffusivity of the cell-to-cell path (D_c) calculated from pressure probe data ranged from D_c = 0.4·10⁻⁶ square centimeters per second in the adaxial region to D_c = 6.1·10⁻⁶ square centimeters per second in the abaxial region of the tissue. D_t D_c suggests substantial cell-to-cell transport of water occurred during rehydration. However, the tissue diffusivity calculated from the kinetics of pressure-propagation across the tissue (D_t′) was D_t′ = (33.1 ± 8.0)·10⁻⁶ square centimeters per second (n = 8) and more than 1 order of magnitude larger than D_t. Also, the hydraulic conductance of the midrib tissue (Lp_m per square centimeter of surface) estimated from pressure-induced flows across several parenchyma cell layers was Lp_m = (8.9 ± 5.6)·10⁻⁵ centimeters per second per bar (n = 5) and much larger than Lp.

These results indicate that the preferential path for water transport across the midrib tissue depends on the nature of the driving forces present within the tissue. Under osmotic conditions, the cell-to-cell path dominates, whereas under hydrostatic conditions water moves primarily in the apoplasm.

     

Hydroxyl ion movements across the human erythrocyte membrane. Measurement of rapid pH changes in red cell suspensions

A stopped flow rapid reaction apparatus capable of following changes of ±0.02 pH unit in 0.1 ml of solution in less than 0.005 sec has been developed, utilizing a commercially available pH-sensitive glass electrode. Using this instrument, extracellular pH at 37°C was followed from less than 0.025 sec to 300 sec after mixing equal volumes of the following CO₂-free solutions: (A) normal human red cells, washed three times and resuspended in 150 mM NaCl at pH 7.2 with a hematocrit of 18%; and, (B) 150 mM NaCl adjusted with HCl or NaOH to pH 2.1 to pH 10.3. A minimum of 2 ml of mixture had to flow through the electrode chamber to ensure complete washout. The mixing process produced a step change in the pH of the extracellular fluid, after which exchanges across the red cell membrane and buffering by intracellular hemoglobin caused it to return toward pH 7.2 with an approximately exponential time course. Under the assumption that pH changes after mixing represent exchanges of hydroxyl for chloride ions across the cell membrane, hydroxyl ion permeabilities (P _OH ^- in cm/sec) were calculated and found to vary from 2 x 10^-4 at pH 9 to 4 x 10^-1 at pH 4 according to the empirical relationship P _OH ^- = 170 exp (-1.51 pH). The form of the dependence of P _OH ^- on extracellular pH does not appear compatible with a simple fixed charge theory of membrane permselectivity.     

Identification of Low Molecular Mass GTP-Binding Proteins in Membranes of the Halotolerant Alga Dunaliella salina

A family of specific guanine nucleotide-binding proteins in Dunaliella salina was studied. Polypeptides of different subcellular fractions were separated by electrophoresis and transferred to nitrocellulose or Immobilon membranes. Incubation of the transfer blots with [³⁵S]GTPγS or [α-³²P]GTP showed no evidence for GTP-binding proteins in the chloroplast and cytosol fractions. However, two GTP-binding proteins with molecular masses of 28 and 30 kilodaltons were present in the plasma membrane and microsomal fractions. An additional 29 kilodalton GTP-binding protein was detected in the plasma membrane. The mitochondrial fraction contained significant amounts of only the 28 kilodalton GTP-binding protein. Binding of [³²P]GTP to the protein blots was completely prevented by 10 micromolar GTP or guanosine 5′-O-(2-thiodiphosphate) (added in 3 × 10⁴-fold excess), whereas ATP or CTP had no effect on the binding. The 28 kilodalton GTP-binding protein was recognized by polyclonal antibodies to the ras-related YPT1 protein of yeast but not by the anti-ras Y13-259 monoclonal antibody. GTP-binding proteins present in the microsomal fraction could not be solubilized by incubation of microsomes with 1 molar NaCl or 0.2 molar Na₂CO₃, but some GTP-binding activity was solubilized when microsomes were treated with 6 molar urea. These results indicate that D. salina GTP-binding proteins are tightly associated with the membranes. The covalent attachment of fatty acids to these proteins was also investigated. Electrophoresis followed by fluorography of delipidated microsomal proteins extracted from [³H]myristic acid-labeled cells showed an intense labeling of a 28 kilodalton protein. We conclude that D. salina contains proteins resembling the ras-related proteins found in animal cells and higher plants.     

Dynamic Light-Scattering Evidence for the Flexibility of Native Muscle Thin Filaments

We have obtained clear evidence for the flexibility of native scallop adductor thin filaments by studying the temperature and ionic strength dependence of the average decay constants obtained from intensity fluctuation spectroscopic (IFS) measurements. The low-angle (10-25°), average decay constants obtained from time autocorrelation functions of scattered light were independent of concentration (0.08-1.3 mg/ml), scaled with the ratio of temperature to solvent viscosity, T/η, over a range of 4-45°C, and yielded a value for the translational diffusion coefficient of D_T^5°C = (1.24 ± 0.06) × 10^-8 cm²/s. From this value and the Broersma relation for rigid rods, we find an average filament length of 1.06 ± 0.06 μm. Quantitative sodium dodecyl sulfate polyacrylamide gel electrophoresis showed that at high temperatures (> 35°C) or in 0.6 M NaCl, tropomyosin completely dissociates from native thin filaments. Decay constants from high-angle (60-150°C) IFS temperature dependence measurements do not scale with T/η and hence do not show the temperature dependence expected for rigid rods. The differences are not due to any change in length distribution of filaments with temperature or to the free tropomyosin in solution, but are attributed to nonrigid motions of the filaments. Similar experiments on samples in high- and low-salt solvents gave results consistent with this interpretation.     

Function and Expression of Cystic Fibrosis Transmembrane Conductance Regulator after Small Intestinal Transplantation in Mice

The secretion function of intestinal graft is one of the most important factors for successful intestinal transplantation. Cystic fibrosis transmembrane conductance regulator (CFTR) mediates HCO₃ ^- and Cl^- secretions in intestinal epithelial cells. In this study, we made investigation on the expression and function of CFTR in an experimental model of murine small intestinal transplantation. Heterotopic intestinal transplantations were performed in syngeneic mice. The mRNA and protein expressions of CFTR were analyzed by real time PCR and western blot. Murine intestinal mucosal HCO₃ ^- and Cl^- secretions were examined in vitro in Ussing chambers by the pH stat and short circuit current (I_sc) techniques. The results showed that forskolin, an activator of CFTR, stimulated jejunal mucosal epithelial HCO₃ ^- and Cl^- secretions in mice, but forskolin-stimulated HCO₃ ^- and Cl^- secretions in donor and recipient jejunal mucosae of mice after heterotopic jejunal transplantation were markedly decreased, compared with controls (P<0.001). The mRNA and protein expression levels of CFTR in donor and recipient jejunal mucosae of mice were also markedly lower than those in controls (P<0.001), and the mRNA and protein expression levels of tumor necrosis factor α (TNFα) were markedly increased in donor jejunal mucosae of mice (P<0.001), compared with controls. Further experiments showed that TNFα down-regulated the expression of CFTR mRNA in murine jejunal mucosa. In conclusion, after intestinal transplantation, the function of CFTR was impaired, and its mRNA and protein expressions were down-regulated, which may be induced by TNFα.