ATP-dependent calcium transport and its correlation with Ca2+-ATPase activity in basolateral plasma membranes of rat duodenum

Isolated basolateral plasmamembrane vesicles from rat duodenum epithelial cells exhibit ATP-dependent calcium-accumulation and Ca²⁺-dependent ATPase activity. Calcium accumulation stimulated by ATP is prevented by the calcium ionophore A23187, inhibited 80% by 0.1 mM orthovanadate but is not effected by oligomycin. Calcium accumulation is not observed with the substrate β-γ-(CH₂)-ATP, ADP and p-nitrophenyl phosphate. Kinetic studies reveal an apparent K_m of 0.2 μM Ca²⁺ and a V_max of 5.3 nmol Ca²⁺/min per mg protein for the ATP-dependent calcium-uptake system. Calmodulin and phenothiazines have no effect on calcium accumulation in freshly prepared membranes, but small effects are inducable after a wash with a 5 mM EGTA. The kinetic parameters of Ca²⁺-ATPase are: K_m = 0.25 μM Ca²⁺ and V_max = 19.2 nmol P_i/min per mg protein. Three techniques, osmotic shock, treatment with Triton X-100 or the channel-forming peptide alamethacin, reveal that about 40% of the vesicles are resealed. Assuming that half of the resealed vesicles have an inside-out orientation, the V_max of ATP-dependent calcium uptake amounts to 25 nmol Ca²⁺/min per mg protein and of the Ca²⁺-ATPase to 23 nmol P_i/min per mg protein. The close correlation between kinetic parameters of Ca²⁺-ATPase and ATP-dependent calcium-transport strongly suggests that both systems are expressions of a Ca²⁺-pump located in duodenal basolateral plasma membranes.     

Na+-coupled Cl− transport in the gastric mucosa of the guinea pig

The Cl^–/HCO ₃ ^– exchange mechanism usually postulated to occur in gastric mucosa cannot account for the Na⁺-dependent electrogenic serosal to mucosal Cl^– transport often observed. It was recently suggested that an additional Cl^– transport mechanism driven by the Na⁺ electrochemical potential gradient may be present on the serosal side of the tissue. To verify this, we have studied Cl^– transport in guinea pig gastric mucosa. Inhibiting the (Na⁺, K⁺) ATPase either by serosal addition of ouabain or by establishing K⁺-free mucosal and serosal conditions abolished net Cl^– transport. Depolarizing the cell membrane potential with triphenylmethylphosphonium (a lipid-soluble cation), and hence reducing both the Na⁺ and Cl^– electrochemical potential gradients, resulted in inhibition of net Cl^– flux. Reduction of short-circuit current on replacing Na⁺ by choline in the serosal bathing solution was shown to be due to inhibition of Cl^– transport. Serosal addition of diisothiocyanodisulfonic acid stilbene (an inhibitor of anion transport systems) abolished net Cl^– flux but not net Na⁺ flux. These results are compatible with the proposed model of a Cl^–/Na⁺ cotransport mechanism governing serosal Cl^– entry into the secreting cells. We suggest that the same mechanism may well facilitate both coupled Cl^–/Na⁺ entry and coupled HCO ₃ ^– /Na⁺ exit on the serosal side of the tissue.     

Head tube: a simple device for estimating velocity in running water

Construction and operation of a head tube are described. A head tube is an inexpensive, easily-built alternative to a current meter for measuring water velocity in streams and rivers. When water flowing in a channel is obstructed by an object, its depth increases at the point of zero velocity (stagnation zone). The difference between the flowing-water depth and depth in the stagnation zone is the head (h). A head tube consists of a clear, hollow, 2.5 cm diameter acrylic tube and a sliding sleeve made of clear plastic. The tube is placed vertically on the river bottom. The difference (head) between water level inside the tube and the height of water against the tube's upstream face is measured against a scale (cm s^–1) drawn on the sleeve, which provides a direct reading of velocity. Graduations of the scale are calculated from a hydrodynamic equation relating mean velocity () to head (h): = (2gh)^0.5, whereg is acceleration due to gravity. When tested in a laboratory flume, the head tube gave very precise estimates of velocity (R ² of relationship = 0.98), although the original calibration scale overestimated current meter-measured velocity by 22 percent. The relationship between head tube and current meter estimates of mean velocity determined in a river with stony substrate was less precise than the correspondence observed in the laboratory (R ² = 0.81). However, estimates of discharge based on head tube measurements were within 8 percent of estimates based on current meter readings.     

Intracellular free zinc and zinc buffering in human red blood cells

Summary The effect of vasopressin on voltage-sensitive Ca²⁺ currents in the rat insulinoma cell line RINm5F has been investigated in patch-clamp whole-cell and single-channel current recording experiments. In the whole-cell recording configuration the dominant inward current in the presence of tetrodotoxin was noninactivating and had a high voltage threshold. This current was much enhanced when external Ca²⁺ was replaced by Ba²⁺ and was blocked by 1 m nifedipine. It can therefore be classified as an L-current. Vasopressin enhanced the L-current without changing the voltage threshold of activation or the voltage at which the peak current was observed. Vasopressin effects were seen at concentrations as low as 0.01nm, and the maximal effect was observed at about 1nm. In higher concentrations the vasopressin effects were weaker, with effects at 50nm of about the same magnitude as at 0.01nm. In single-channel current recording experiments carried out with the cell-attached configuration there were no effects on single L-channel currents when vasopressin was added to the bath solution, but in experiments in which vasopressin (5nm) was infused into the patch pipette a marked increase in the apparent channel open state probability was observed. We conclude that vasopressin, a peptide that is known to markedly enhance glucose-evoked insulin secretion, stimulates opening of the voltage-sensitive Ca²⁺ channels in insulin-secreting cells.     

Developmental changes in the calcium currents in embryonic chick ventricular myocytes

Summary Using the patch-clamp technique, we recorded whole-cell calcium current from isolated cardiac myocytes dissociated from the apical ventricles of 7-day and 14-day chick embryos. In 70% of 14-day cells after 24 hr in culture, two component currents could be separated from totalI _Ca activated from a holding potential (V _h) of –80 mV. L-type current (I _L) was activated by depolarizing steps fromV _h –30 or –40 mV. The difference current (I _T) was obtained by subtractingI _L, fromI _Ca.I _T could also be distinguished pharmacologically fromI _L in these cells.I _T was selectively blocked by 40–160 m Ni²⁺, whereasI _L was suppressed by 1 m D600 or 2 m nifedipine. The Ni²⁺-resistant and D600-resistant currents had activation thresholds and peak voltages that were near those ofI _T andI _L defined by voltage threshold, and resembled those in adult mammalian heart. In 7-day cells,I _T andI _L could be distinguished by voltage threshold in 45% (S cells), while an additional 45% of 7-day cells were nonseparable (NS) by activation voltage threshold. Nonetheless, in mostNS cells,I _Ca was partly blocked by Ni²⁺ and by D600 given separately, and the effects were additive when these agents were given together. Differences among the cells in the ability to separateI _T andI _L by voltage threshold resulted largely from differences in the position of the steady-state inactivation and activation curves along the voltage axis. In all cells at both ages in which the steady-state inactivation relation was determined with a double-pulse protocol, the half-inactivation potential (V _1/2) of the Ni²⁺-resistant currentI _L averaged –18 mV. In contrast,V _1/2 of the Ni²⁺-sensitiveI _T was –60 mV in 14-day cells, –52 mV in 7-dayS cells, and –43 mV in 7-day NS cells. The half-activation potential was near –2 mV forI _L at both ages, but that ofI _T was –38 mV in 14-day and –29 mV in 7-day cells. Maximal current density was highly variable from cell to cell, but showed no systematic differences between 7-day and 14-day cells. These results indicate that the main developmental change that occurs in the components ofI _Ca is a negative shift with, embryonic age in the activation and inactivation relationships ofI _T along the voltage axis.     

Interpretation of sedimentation data measured in a former tidal channel Lake Volkerak

In Lake Volkerak, situated in the southwest of the Netherlands, downward settling fluxes are related to external inputs of suspended solids and wind action. The settling fluxes, measured using sediment traps, were 55 g (dw) m ^–2 d ^–1 on average. The ratio of metal concentration to scandium concentration was used to discriminate between external (polluted) suspended solids and internal (relatively clean) suspended solids. Generally, the contribution of the river suspended solids was small compared to that of resuspended material; the river-transported material was mainly deposited in the centre and to the east of the lake. The amount of material trapped increased substantially with increasing wind velocity.A simple model was used to interpretate the data. This model does not have a predictive capacity, but can be used to interpret and assess the significance of material retained in the sediment traps. Erosion was related to the wind velocity, using an empirical relationship between the orbital velocity of the wind-generated waves at the bottom and the wind velocity. The critical wind velocity for erosion to occur was estimated to be 5.5 m s^–1. The extremely high amounts retained in the sediment traps in shallow areas during storms emphasised the importance of these wind conditions for the transport of fine sediments.     

Regulation of a potassium-selective current in rabbit corneal epithelium by cyclic GMP,carbachol and diltiazem

Summary The effects of cyclic GMP (cGMP), carbachol and diltiazem on a potassium-selective, delayed-rectifier current in freshly dissociated rabbit corneal epithelial cells were studied using a modified perforated-patch-clamp technique. The current was stimulated by both 500 m cGMP (2.3–4.5-fold, mean = 2.9) and 250 nm carbachol, a muscarinic agonist (1.12–7.04-fold, mean = 3.8), and the stimulated current was totally blocked by diltiazem (10 m). The effects of cGMP appeared to be, at least in part, different from those of carbachol as they required the presence of external calcium. Single-channel data suggest that cGMP and carbachol activate the potassium current by increasing the open probability of the channel via a second-messenger system and that the action of diltiazem is probably through a direct blocking effect on the open channel.We are grateful to Erika Wohlfiel for secretarial help, Helen Hendrickson for cell preparation, and Joan Rae for software development. The work was supported by NIH grants EY06005 and EY03282 and an unrestricted award from Research to Prevent Blindness.     

K+ current stimulation by Cl- in the midgut epithelium of tobacco hornworm (Manduca sexta)

Summary Chloride-stimulated K⁺ secretion by Manduca sexta midgut (5th-instar larvae) was measured as K⁺-carried short-circuit current of the tissue mounted in an Ussing chamber. Microscopic parameters, such as single-channel current and channel density for the rate-determining passive transport step across the basolateral goblet cell membrane (i.e. K⁺ channels), were estimated by means of current-fluctuation analysis of the K⁺ channel blockade by haemolymph-side Ba²⁺ ions. Ba²⁺ was equally effective with Cl^- or gluconate (Glu^-) as the principal ambient anion. The Ba²⁺-induced K⁺ channel conduction noise is reflected by a Lorentzian, or relaxation, noise component in the power spectrum of the K⁺ current fluctuations. A reduced Lorentzian plateau value, but an unchanged corner frequency, were observed when Cl^- was replaced by Glu^-. The results from the analysis of a two-state model of K⁺ channel block by Ba²⁺, with respect to the anion-replacement effects, suggest that the observed changes in K⁺ current and Lorentzian plateau value mirror a complex change of the underlying parameters: Cl^- omission reduces single channel current but increases channel density so that the product of single channel current and channel density is smaller in Glu^- than in Cl^-. It seems likely that basolateral K⁺ channels (1) are subject to anionic gating ligands, and (2) depend on anions with respect to the rate of K⁺ transfer through and open K⁺ channel.Abbreviations a.c. alternating current - single-channel conductance - E _K K⁺ Nernst potential - f frequency contained in current noise - f _c corner frequency - Glu^- gluconate - G _t transepithelial conductance - I _sc short-circuit current - I _K K⁺ current - I _K(max) maximal K⁺ current - i single-channel current - K _Ba barium inhibition constant - K _m Michaelis constant of saturating K⁺ current - k ₀₁ and k ₁₀ barium association and dissociation rate constant, respectively - M K⁺ channel density - S _f power density - S _o Lorentzian plateau value - P _o channel-open probability - P _K K⁺ permeability - V _sc cellular potential at short-circuit These results have already been presented in part, at the 1989 joint meeting of the German and Israel Physiological Societies in Jerusalem (Zeiske et al. 1990).     

Determination of electric current distributions in animals and humans exposed to a uniform 60-Hz high-intensity electric field

The thermographic method for determining specific absorption rate (SAR) in animals and models of tissues or bodies exposed to electromagnetic fields was applied to the problem of quantifying the current distribution in homogeneous bodies of arbitrary shape exposed to 60-Hz electric fields. The 60-Hz field exposures were simulated by exposing scale models of high electrical conductivity to 57.3-MHz VHF fields of high strength in a large 3.66 × 3.66 × 2.44-m TE₁₀₁ mode resonant cavity. After exposure periods of 2–30 s, the models were quickly disassembled so that the temperature distribution (maximum value up to 7 °C) along internal cross-sectional planes of the model could be recorded thermographically. The SAR, W′, calculated from the temperature changes at any point in the scale model was used to determine the SAR, W, for a full-scale model exposed to a 60-Hz electric field of the same strength by the relation W = (60/ f² · (σ′/σ) · W′ where f′ is the model exposure frequency, σ′ is the conductivity of the scale model at the VHF exposure frequency, and σ is the conductivity of the full-scale subject at 60 Hz. The SAR was used to calculate either the electric field strength or the current density for the full-scale subject. The models were used to simulate the exposure of the full-scale subject located either in free space or in contact with a conducting ground plane. Measurements made on a number of spheroidal models with axial ratios from 1 to 10 and conductivity from 1 to 10 s/m agreed well with theoretical predictions. Maximum current densities of 200 nA/cm² predicted in the ankles of man models and 50 nA/cm² predicted in the legs of pig models exposed to 60-Hz fields at 1kV/m agreed well with independent measurements on full-scale models.