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At least 19 recordsLinked to original sources
PubMed1999

Cooling-induced bronchoconstriction: the role of ion-pumps and ion-carrier systems.

The mechanism of cold-induced bronchoconstriction is poorly understood. Our previous results show that cooling-induced contractions (CIC) do not involve activation of cell surface receptor systems nor innervation nor Ca2+ uptake. However, the results show that CIC is mainly dependent on intracellular Ca2+ [32]. Isolated tracheal strips and bronchiolar segments were suspended in organ baths containing Krebs' solution for isometric tension recording. Tissue responses during stepwise cooling from 37 to 5 degrees C were examined. Cooling ovine tracheal strips and bronchiolar ring segments to 20 degrees C caused a rapid contraction which decreased slowly until it reached the basal level in approximately 30 min. There is a significant inhibition of 45Ca2+ efflux at 20 degrees C to those incubated at 37 degrees C. This prompted this study whose aim was to determine the role of ion-pump and ion-carrier systems on cooling mechanisms. Inhibition of the Na+/K+ pump with ouabain (10 micrometer) evoked contraction in tracheal and bronchiolar preparations. When cooling was superimposed on this contraction the cooling-induced contractions were reduced in the bronchiolar segments. In the tracheal strips, at temperatures down to 15 degrees C ouabain converted the contractions to a relaxation, but further cooling to 10 and 5 degrees C resulted in contractions that were similar to control at 5 degrees C. Staurosporine, a protein kinase inhibitor (1 micrometer) enhanced CIC in trachea and bronchiole. Vanadate, a Ca2+-ATPase pump inhibitor (1 mm) potentiated CIC in the two preparations. Trifluoperazine and W-7, calmodulin antagonists (10 and 100 micrometer) enhanced CIC in tracheal preparations but not in the bronchiolar segments. Thapsigargin and cyclopiazonic acid (CPA), inhibitors of sarcoplasmic reticulum (SR) Ca2+-ATPase pump (1 and 10 micrometer) potentiated CIC in tracheal but not in bronchiolar preparations. Amiloride, Na+/H+ and Na+/Ca2+ exchange system inhibitor (1 mm) abolished CIC in both trachea and bronchiole. These results show a strong relationship between cooling and the activity of ion transport systems and indicate that CIC is due to inhibition of calcium removal mechanisms as a result of inhibition of these ion-pump and ion carrier systems.

Animals↗
PubMed1991

Reversible mechanosensitive ion pumping as a part of mechanoelectrical transduction.

To explain the ability of some mechanosensitive cells to reverse the process of mechanotransduction and to generate mechanical oscillations and emit sound, a piezo-conformational coupling model (PCC model) is proposed. The model includes a transport protein which changes either its volume (PV-coupling) or its area in the membrane (gamma A-coupling) when undergoing conformational transitions. Such a protein can interact with an oscillating pressure to pump ions and create a transmembrane gradient if the affinities of the protein for ions are different at the two sides of membrane. The frequency and concentration windows for mechanical energy transduction were determined. Under optimal conditions, the efficiency of energy transduction can approach the theoretical maximum of 100%. If the concentration gradient exceeds the static head value (quasi-equilibrium which can be built up and maintained by this transport system), the energy transduction reverses and the transporter becomes a generator of mechanical oscillations at the expense of a concentration gradient. Estimation of thermodynamic parameters of the pump shows that the PV-coupling model would require large pressure oscillations to work while the gamma A-coupling model could work in physiological conditions. The gamma A-coupling mechanism may be used by cells for two purposes. In the reverse mode, it can be a force generator for various applications. In the direct mode, it may serve bioenergetic purposes by harvesting the energy of mechanical oscillations and storing it in the form of a concentration gradient. This pump has an unusual thermodynamic feature: it can distinguish the two components of the electrochemical potential gradient,i.e., the concentration gradient and the electrical potential, the latter serving as a permissive switch to open, or close, the pump when the potential reaches the threshold value.Predictions of the PCC model and its probable involvement in biological mechanotransduction are dicussed.

Biological Transport, Active↗
PubMed2003

Crystal structure of the bromide-bound D85S mutant of bacteriorhodopsin: principles of ion pumping.

We report the crystal structure of a bromide-bound form of the D85S mutant of bacteriorhodopsin, bR(D85S), a protein that uses light energy rather than ATP to pump halide ions across the cell membrane. Comparison of the structure of the halide-bound and halide-free states reveals that both displacements of individual side-chain positions and concerted helical movements occur on the extracellular side of the protein. Analysis of these structural changes reveals how this ion pump first facilitates ion uptake deep within the cell membrane and then prevents the backward escape of ions later in the pumping cycle. Together with the information provided by structures of intermediate states in the bacteriorhodopsin photocycle, this study also suggests the overall design principles that are necessary for ion pumping.

Bacteriorhodopsins↗
PubMed1984

Current noise generated by electrogenic ion pumps.

Active ion transport by ATP- or light-driven pumps involves a sequence of elementary steps such as binding and release of ions, as well as conformational transitions of the pump protein. At the microscopic level the individual reaction steps occur at random intervals, and therefore the current generated by electrogenic pumps fluctuates around a mean value. In this paper, a theoretical treatment of the electrical noise associated with active ion transport is given. The analysis, which is based on the calculation of the correlation function, yields the spectral intensity S1 of current noise as a function of frequency, f. The shape of S1(f) contains information on the rate constants as well as on the magnitude of the charge displacements occurring during single reaction steps. The contribution of electrogenic pumps to the total voltage noise of the cell may be estimated from S1(f) and from the frequency-dependent impedance of the cell membrane.

Adenosine Triphosphate↗
PubMed1992

Regulation of the calcium ion pump of sarcoplasmic reticulum: reversible inhibition by phospholamban and by the calmodulin binding domain of the plasma membrane calcium ion pump.

A 45 amino acid peptide (A45) corresponding to the phospholamban (PLN) binding domain of the sarcoplasmic reticulum (SR) ATPase was synthesized. Circular dichroism experiments have shown that the peptide had a predominantly random-coil conformation but adopted a higher proportion of secondary structure in the presence of a synthetic 32 amino acid peptide corresponding to the hydrophilic portion of PLN. A similar conformational change was induced by the synthetic calmodulin binding domain of the plasma membrane Ca2+ pump (peptide C28W), which acts as an endogenous inhibitor of the pump and is homologous to PLN. Cross-linking experiments have shown that peptide C28W interacted with peptide A45. The Ca(2+)-pumping activity of cardiac SR, which contains endogenous PLN, was stimulated about 30% by peptide A45. The stimulation was maximal at submicromolar Ca2+ levels and tended to disappear at higher Ca2+ concentrations. By contrast, the Ca(2+)-pumping activity of skeletal muscle SR, which lacks endogenous PLN, was unaffected. Peptide C28W strongly inhibited the pumping activity of skeletal muscle SR, and peptide A45 reversed the inhibition. The results suggest that peptide A45 competed with the ATPase for phospholamban or for peptide C28W, removing the inhibition of the pump. Thus, the exogenous inhibitor of the SR Ca(2+)-ATPase, PLN, and the internal inhibitor of the plasma membrane Ca(2+)-ATPase, peptide C28W, are functionally analogous.

Amino Acid Sequence↗
PubMed2004

Energy transduction in transmembrane ion pumps.

Recent crystallographic structures of three different ion pumps provide a first view of the mechanisms by which these molecular machines transfer ions across cell membranes against an electrochemical gradient. Each of the structures reinforces the concept that several buried counter ions have central roles in substrate recruitment, substrate binding and energy transduction during ion pumping. The spatial organization of the counter ions suggests that, initially, one or more counter ions lowers the Born energy cost of binding a substrate ion in the low-dielectric interior of the membrane. Subsequently, a ligand-induced conformational change seems to close a charged access gate to prevent backflow from a subsequent, low-affinity state of the pump. A final role of the buried counter ions might be to couple the input of external energy to a small charge separation between the substrate ion and the buried counter ions, thereby decreasing the binding affinity for the substrate ion in preparation for its release on the high-energy side of the membrane.

Animals↗
PubMed1991

Australian Halobacteria and their retinal-protein ion pumps.

Halophiles collected in Western Australia have been found to be examples of extremely halophilic rod-shaped archaebacteria, members of the genus Halobacterium. Most of them contain retinal proteins, and these proteins differ from one another and also from both bacteriorhodopsin (bR) and halorhodopsin [and sensory rhodopsins (sR)] isolated from Halobacterium salinarium (halobium), as revealed by their peptide maps and amino acid sequences. However, these retinal proteins still have the ability to pump protons or chloride ions in the light. These new ion pumps, designated archaerhodopsins (aR) [Mukohata et al. (1988) Biochem. Biophys. Res. Commun. 151, 1339-1345], are almost identical in terms of their molecular sizes and transient photochemical properties to the ion pumps identified previously. Differences are found in the: (1) apparent extinction coefficient of dark/light-adapted aR-2; (2) titration profiles at acidic pH of the absorption spectra of all aRs; and (3) circular dichroism spectra, which are influenced by the coexistent isoprenoid bacterioruberin. The amino acid sequences of two proton pumps from the Australian halobacteria, namely aR and aR-2, are approximately 90% homologous and both sequences are about 60% homologous with that of bR. Hydropathy plots suggest that these pumps also have a seven-helical structure similar to that of bR. The amino acid residues are highly conserved in the helical regions, in particular in the case of helices C and G (91 and 84%, respectively), among the three proton pumps.

Amino Acid Sequence↗
PubMed1985

Incorporation of membrane potential into theoretical analysis of electrogenic ion pumps.

The transport rate of an electrogenic ion pump, and therefore also the current generated by the pump, depends on the potential difference (delta psi) between the two sides of the membrane. This dependence arises from at least three sources: (i) charges carried across the membrane by the transported ions; (ii) protein charges in the ion binding sites that alternate between exposure to (and therefore electrical contact with) the two sides of the membrane; (iii) protein charges or dipoles that move within the domain of the membrane as a result of conformational changes linked to the transport cycle. Quantitative prediction of these separate effects requires presently unavailable molecular information, so that there is great freedom in assigning voltage dependence to individual steps of a transport cycle when one attempts to make theoretical calculations of physiological behavior for an ion pump for which biochemical data (mechanism, rate constants, etc.) are already established. The need to make kinetic behavior consistent with thermodynamic laws, however, limits this freedom, and in most cases two points on a curve of rate versus delta psi will be fixed points independent of how voltage dependence is assigned. Theoretical discussion of these principles is illustrated by reference to ATP-driven Na,K pumps. Physiological data for this system suggest that all three of the possible mechanisms for generating voltage dependence do in fact make significant contributions.

Biological Transport, Active↗
PubMed1991

Direct comparison of in-vitro and in-vivo Photofrin-II mediated photosensitization using a pulsed KTP pumped dye laser and a continuous wave argon ion pumped dye laser.

A pulsed KTP pumped dye laser (25 kHz repetition rate and 470 nsec pulse width) has been compared to a continuous wave argon ion pumped dye laser as the source of 630 nm light during in-vitro and in-vivo Photofrin-II mediated photosensitization studies. Individual experiments documented the effectiveness of each laser system on a) photosensitizer induced cytotoxicity and induction of stress protein synthesis using Chinese hamster fibroblasts; b) photobleaching of Photofrin-II in aqueous solution; c) Photofrin II mediated photosensitization of normal mouse skin; d) Photofrin II mediated photodynamic therapy of a mouse mammary carcinoma; and e) tumor temperature levels generated during laser exposure. Comparable results were obtained for both laser systems in all experiments.

Animals↗
PubMed2002

Halorhodopsin: light-driven ion pumping made simple?

Halorhodopsin, a light-driven halide pump, is the second archaeal rhodopsin involved in ion pumping to be studied at high resolution by X-ray crystallography. Like its cousin bacteriorhodopsin, halorhodopsin couples vectorial ion transport to the isomerisation state of a covalently linked retinal. Given the similarity and interconvertability of these two ion pumps, a unified mechanism for ion translocation by archaeal rhodopsins is now emerging.

Biological Transport, Active↗
PubMed1994

Inhibitory effects of Microcystis aeruginosa toxin on ion pumps of the gill of freshwater fish.

A microsomal fraction enriched in ion pump enzymes was isolated from the gill of the carp (Cyprinus carpio Linneo). Mg(2+)-dependent (Na+ + K+), Na+, HCO3- and Ca(2+)-stimulated ATPase activities were studied following treatment with microcystin-LR-like toxin, the major toxic component isolated from Microcystis aeruginosa culture. These enzyme activities were inhibited in a dose-dependent manner. The maximum inhibition of each enzyme, induced with nM concentration of the toxin, was similar to that produced by inhibitors specific for each ATPase activity. The Mg(2+)-ATPase activity and non-specific hydrolysis of ATP were unaffected. These results strongly suggest that the massive fish death during M. aeruginosa blooms may result from the loss of ion homeostatic processes produced by the inhibitory action of microcystin on the ion pumps of gill chloride cells.

Animals↗
PubMed1986

Inhibition of ion pump ATPase activity by 3'-O-(4-benzoyl)benzoyl-ATP (BzATP): assessment of BzATP as an active site-directed probe.

The interaction of 3'-O-(4-benzoyl)benzoyl-ATP (BzATP) with the renal (Na+ + K+)-ATPase, the sarcoplasmic reticulum Ca-transport ATPase, and the gastric (H+ + K+)-ATPase has been investigated in order to determine whether BzATP is a suitable probe for the labeling and identification of a peptide from the ATP binding sites of these ion pumps. After ultraviolet irradiation BzATP inhibited the enzymatic hydrolysis of ATP by each of the ion pumps, and also was covalently incorporated into the 100 000 dalton polypeptides of each protein. The presence of excess ATP in the reaction solution did not prevent either the inactivation of ATPase activity or the labeling of the catalytic polypeptides by BzATP. Prior modification of the ATPases with fluorescein-5'-isothiocyanate (FITC), however, prevented much of the labeling of the 100 000 dalton polypeptides by BzATP. BzATP competitively inhibited the high-affinity binding of ATP to the ion pumps, but ATP did not block the high-affinity binding of BzATP by the enzymes. BzATP binds to the membrane-bound ATPases at a high-affinity site with a Kd of 0.8-1.2 microM and a Bmax of 2-3 nmol/mg, and also binds to at least one low-affinity, high-capacity site on the membranes. HPLC separation of the soluble peptides from a tryptic digest of BzATP-labeled (Na+ + K+)-ATPase revealed the presence of several labeled peptides, none of which was protected by either ATP or FITC. Although BzATP can displace ATP from a high-affinity binding site on the ion pumps, it appears, therefore, that inactivation of enzymatic activity is the result of reactions between BzATP and the proteins at locations outside this site. Thus, it is concluded from these experiments that BzATP is not likely to be a useful probe for the ATP binding sites on the ion transport ATPases.

Adenosine Triphosphatases↗
PubMed1992

Electrostatic coupling of ion pumps.

In this paper the electrostatic interactions between membrane-embedded ion-pumps and their consequences for the kinetics of pump-mediated transport processes have been examined. We show that the time course of an intrinsically monomolecular transport reaction can become distinctly nonexponential, if the reaction is associated with charge translocation and takes place in an aggregate of pump molecules. First we consider the electrostatic coupling of a single dimer of ion-pumps embedded in the membrane. Then we apply the treatment to the kinetic analysis of light-driven proton transport by bacteriorhodopsin which forms two-dimensional hexagonal lattices. Finally, for the case of nonordered molecules, we also consider a model in which the pumps are randomly distributed over the nodes of a lattice. Here the average distance is equal to that deduced experimentally and the elemental size of the lattice is the effective diameter of one single pump. This latter model is applied to an aggregate of membrane-embedded Na, K- and Ca-pumps. In all these cases the electrostatic potential considered is the exact solution calculated from the method of electrical images for a plane membrane of finite thickness immersed in an infinite aqueous solution environment. The distributions of charges (ions or charged binding sites) are considered homogeneous or discrete in the membrane and/or in the external solution. In the case of discrete distributions we compare the results from a mean field approximation and a stochastic simulation.

Electrophysiology↗
PubMed1976

The bicarbonate ion pump in the endothelium which regulates the hydration of rabbit cornea.

1. Studies were made on the short-circuit current (s.c.c.) and fluid transport across rabbit corneal endothelium. 2. Normal s.c.c. of 27 muA.cm-2 is reduced to 19 muA.cm-2 in CO2-free Ringer, to 9 muA. cm-2 in HCO-3 -free Ringer and to zero in CO2 and HCO-3 -free Ringer. 3. Carbonic anhydrase inhibitors reduce s.c.c. from 27 to 19 muA.cm-2. Removal of exogenous CO2 causes no further reduction in s.c.c. 4. In CO2-free Ringer, net exogenous bicarbonate translocation is equal to s.c.c. 5. In all cases studied, net fluid transport across the endothelium in open circuit is directly proportional to s.c.c. 6. It is concluded that the endothelial 'pump' which regulates corneal hydration operates by 'pumping' bicarbonate ions into the aqueous humour. 7. Under physiological conditions, two thirds of the substrate is supplied by exogenous bicarbonate ions and one third is supplied by conversion of exogenous CO2 by intracellular carbonic anhydrase. 8. Metabolic CO2 does not participate significantly in the process, probably because it is at too low a concentration to compete effectively with exogenous CO2. 9. Electron histochemical studies suggest that carbonic anhydrase is located immediately underneath the posterior membrane of the endothelium, across which the active bicarbonate ion flux passes.

Animals↗
PubMed1992

Structural modelling of P-type ion pumps.

Over forty sequences of P-type ion pumps have been determined. They fall into five families showing between 20% and 50% identity in sequence. The conserved residues are concentrated in several regions which are found in all the pumps. All the defined functional sites are associated with conserved segments and provide a basis for subdivision into domains, to which tentative secondary and tertiary structures can be assigned. The domains have been assembled into a structure consisting of a conserved core with variable loops and deletions on the surface, which accommodates site mutants, affinity labels and known epitopes. This model has been correlated with the results of an electron crystallographic study of the Ca++ pump. Two types of crystal have been examined in negative stain and in amorphous ice; thin plates which diffract to 4A and long helical tubes which diffract to 15A. The plates have given a 6A projection map, some of which can be interpreted by difference from the map of the negatively stained crystal, as transmembrane helices. Three dimensional interpretation will require a tilt series. In the meantime, analysis of the tubes has given a 14A 3D map which clearly defines the cytoplasmic domains and their relation to the transmembrane region (Stokes and Toyoshima in preparation). Although it is not yet possible to assign specific functions to the cytoplasmic lobes, the structure at this resolution is consistent with the model.

Animals↗