Charge delocalization in proton channels, I: the aquaporin channels and proton blockage

The explicit contribution to the free energy barrier and proton conductance from the delocalized nature of the excess proton is examined in aquaporin channels using an accurate all-atom molecular dynamics computer simulation model. In particular, the channel permeation free energy profiles are calculated and compared for both a delocalized (fully Grotthuss shuttling) proton and a classical (nonshuttling) hydronium ion along two aquaporin channels, Aqp1 and GlpF. To elucidate the effects of the bipolar field thought to arise from two alpha-helical macrodipoles on proton blockage, free energy profiles were also calculated for computational mutants of the two channels where the bipolar field was eliminated by artificially discharging the backbone atoms. Comparison of the free energy profiles between the proton and hydronium cases indicates that the magnitude of the free energy barrier and position of the barrier peak for the fully delocalized and shuttling proton are somewhat different from the case of the (localized) classical hydronium. The proton conductance through the two aquaporin channels is also estimated using Poisson-Nernst-Planck theory for both the Grotthuss shuttling excess proton and the classical hydronium cation.     

Knockdown of aquaporin 3 is involved in intestinal barrier integrity impairment

AQP3 is a water/glycerol transporter expressed at the basolateral membrane of colonic epithelial cells. Although AQPs are expressed in the gastrointestinal tract, their effect on intestinal barrier has not been clear. Here, we showed that knockdown of AQP3 caused a dramatic, dose-dependent increase in E. coli C25 translocation, with the reduction of TEER and increasing LY permeability. Western blots revealed that expression of Claudin-1 and Occludin were significantly decreased in the AQP3 knockdown group, demonstrating that this treatment enhances paracellular permeability via an opening of the tight junction complex. These data not only describe the correlation between transcellular and paracellular pathways in human intestines, but also show that targeted knockdown of AQP3 might impair the intestinal barrier integrity.     

On the stimulation by insulin of tryptophan transport across the blood-brain barrier

Following previous studies showing that in vivo insulin administration increases brain tryptophan levels, we have tested the effect of insulin on tryptophan uptake by isolated bovine brain capillaries, which represent the in vitro equivalent of the blood-brain barrier. In the presence of insulin and Na+ ions, the uptake of 14C-labelled tryptophan was significantly increased with respect to controls, this increase being essentially due to a higher affinity of the transport system for the amino acid, while the Vmax was not affected. Insulin increased also, to a similar extent, the uptake of alpha-methylaminoisobutyrate in the presence of Na+ ions, while the uptake of beta-aminobicyclo(2.2.1)heptane carboxylic acid was not affected. Addition of phloretine, or of anti-insulin antibodies, as well as omission of Na+ ions from the buffer abolished the effect of insulin. Insulin appears therefore to increase specifically the substrate affinity of the A-system for neutral amino acid transport, without exerting any influence on the L-system. The absence of the A-system from the luminal side of the microvessels, and the high insulin concentrations needed, raise however some problems as to the physiological significance of this effect.     

Water transport in AQP0 aquaporin: molecular dynamics studies

A double lipid bilayer structure containing opposing tetramers of AQP0 aquaporin, in contact through extracellular face loop regions, was recently modeled using an intermediate-resolution map obtained by electron crystallographic methods. The pores of these water channels were found to be critically narrow in three regions and subsequently interpreted to be those of a closed state of the channel. The subsequent determination of a high-resolution AQP0 tetramer structure by X-ray crystallographic methods yielded a pore model featuring two of the three constrictions as noted in the EM work and water molecules within the channel pore. The extracellular-side constriction region of this AQP0 structure was significantly larger than that of the EM-based model and similar to that of the highly water permeable AQP1. The X-ray-based study of AQP0 however could not ascertain if the water molecules found in the pore were the result of water entering from one or both ends of the channel, nor whether water could freely pass through all constriction points. Additionally, this X-ray-based structure could not provide an answer to the question of whether the double lipid bilayer configuration of AQP0 could functionally maintain a water impermeable state of the channel. To address these questions we conducted molecular dynamics simulations to compare the time-dependent behavior of the AQP0 and AQP1 channels within lipid bilayers. The simulations demonstrate that AQP0, in single or double lipid bilayers, is not closed to water transport and that thermal motions of critical side-chains are sufficient to facilitate the movement of water past any of its constriction regions. These motional requirements do however lead to significant free energy barriers and help explain physiological observations that found water permeability in AQP0 to be substantially lower than in the AQP1 pore.     

Myo-inositol transport through the blood-brain barrier

The unidirectional transport of [³H]myo-inositol across cerebral capillaries, the anatomical locus of the blood-brain barrier, was measured using an in situ rat brain perfusion technique. Myo-inositol was transported across the blood-brain barrier by a low capacity, saturable system with a one-half saturation concentration of 0.1 mM. The permeability surface-area product was 6.2×10^–5S^–1 with a myo-inositol concentration of 0.02 mM in the perfusate. The myo-inositol stereoisomer scyllo-inositol but not (+)-chiro-inositol (both 1 mM) inhibited myo-inositol transfer through the blood-brain barrier. These observations provide evidence that myo-inositol is transferred through the blood-brain barrier by simple diffusion and a stereospecific, saturable transport system.     

Hypoxanthine transport through the blood-brain barrier

The unidirectional influx of hypoxanthine across cerebral capillaries, the anatomical locus of the blood=brain barrier, was measured with an in situ rat brain perfusion technique employing [³H]hypoxanthine. Hypoxanthine was transported across the blood-brain barrier by a saturable system with a one-half saturation concentration of approximately 0.4 mM. The permeability-surface area product was 3×10^–4 sec^–1 with a hypoxanthine concentration of 0.02 M in the perfusate. Adenine (4 mM) and uracil and theophylline (both 10 mM), but not inosine (10 mM) or leucine (1 mM), inhibited hypoxanthine transfer through the blood-brain barrier. Thus, hypoxanthine is transported through the blood-brain barrier by a high-capacity, saturable transport system with a half-saturation concentration about 100 times the plasma hypoxanthine concentration. Although involved in the transport hypoxanthine from blood into brain, this system is not powerful enough to transfer important quantities of hypoxanthine from blood into brain.     

Niacinamide transport through the blood-brain barrier

The unidirectional influx of niacinamide across cerebral capillaries, the anatomical locus of the blood-brain barrier, was measured with an in situ rat brain perfusion technique employing [¹⁴C]niacinamide. Niacinamide was transported rapidly across the blood-brain barrier by a system that was not saturable with 10 mM niacinamide in the perfusate. However, with periods of perfusion longer than 30 seconds, there was substantial backflow of [¹⁴C]niacinamide into the perfusate. Niacinamide (1.7 M) transport through the blood-brain barrier was not significantly inhibited by 3-acetylpyridine. Thus, niacinamide is transported rapidly and bidirectionally through the blood-brain barrier by a high capacity transport system. Although involved in the transfer of niacinamide between blood and brain, this transport system does not play an important regulatory role in the synthesis of NMN, NAD, and NADP from niacinamide in brain.     

Annexin A4 reduces water and proton permeability of model membranes but does not alter aquaporin 2-mediated water transport in isolated endosomes

Annexin A4 (Anx4) belongs to a ubiquitous family of Ca2+-dependent membrane-binding proteins thought to be involved in membrane trafficking and membrane organization within cells. Anx4 localizes to the apical region in epithelia; however, its physiological role is unclear. We show that Anx4 exhibited binding to liposomes (phosphatidylcholine:phosphatidylserine, 1:1) in the presence of Ca2+ and binding was reversible with EDTA. Anx4 binding resulted in liposome aggregation and a reduction in membrane water permeability of 29% (P < 0.001) at 25 degrees C. These effects were not seen in the presence of Ca2+ or Anx4 alone and were reversible with EDTA. Measurements of membrane fluidity made by monitoring fluorescence anisotropy of 2-(12-(7-nitrobenz-2-oxa-1,3-diazol-4-yl)amino)dodecanoyl-1-hexadecanoyl-sn-glycero-3-phosphocholine (NBD-HPC) demonstrated that Anx4 binding rigidified the outer leaflet of the bilayer (P < 0.001), thus providing a molecular explanation for the inhibition of water flux. To determine whether Anx4 would produce similar effects on physiological membranes we constructed liposomes which recapitulated the lipid composition of the inner leaflet of the MDCK apical membrane. These membranes exhibited reductions to water permeability upon Anx4 binding (19.5% at 25 degrees C, 31% at 37 degrees C; P < 0.01 and P < 0.001, respectively) and to proton permeability (15% at 25 degrees C, 19.5% at 37 degrees C; P < 0.05). Since our in vitro experiments indicated an effect on membrane permeability, we examined localization of Anx4 in the kidney collecting duct, a region of the nephron responsible for concentrating urine through water reabsorbtion. Anx4 was shown to colocalize apically with aquaporin 2 (AQP2) in collecting duct epithelia. To test for the existence of a functional interaction between Anx4 and AQP2 we isolated AQP2-containing endosomes and exposed them to Anx4/Ca2+. Water flux rates were unchanged, indicating Anx4 does not directly regulate AQP2. We conclude that Anx4 can alter the physical properties of membranes by associating with them and regulate passive membrane permeability to water and protons. These properties represent important new functions for Anx4.     

Azide reduces the hydrophobic barrier of the bacteriorhodopsin proton channel

The sensitivity of a nitroxide spin label to the polarity of its environment has been used to estimate the hydrophobic barrier of the proton channel of the transmembrane proton pump bacteriorhodopsin. By means of site-specific mutagenesis, single cysteine residues were introduced at 10 positions located at the protein surface, in the protein interior, and along the proton pathway. After reaction with a methanethiosulfonate spin label, the principle values of the hyperfine tensor A and the g-tensor were determined from electron paramagnetic resonance spectra measured at 170 K. The shape of the hydrophobic barrier of the proton channel is characterized in terms of a polarity index, DeltaA, determined from the variation of the hyperfine coupling constant Azz. The maximum of the hydrophobic barrier is found to be close to the retinal chromophore in the proton uptake pathway. The effect of the asymmetric distribution of charged and polar residues in the proton release and uptake pathways is clearly reflected in the behavior of the hydrophobic barrier. The presence of azide reduces the barrier height of both the cytoplasmic and extracellular channels. This finding supports the view of azide and other weakly acidic anions as catalysts for the formation of hydrogen-bonded networks in proton pathways of proteins.     

On the mechanism of proton transport by the neuronal excitatory amino acid carrier 1

Uptake of glutamate from the synaptic cleft is mediated by high affinity transporters and is driven by Na(+), K(+), and H(+) concentration gradients across the membrane. Here, we characterize the molecular mechanism of the intracellular pH change associated with glutamate transport by combining current recordings from excitatory amino acid carrier 1 (EAAC1)-expressing HEK293 cells with a rapid kinetic technique with a 100-micros time resolution. Under conditions of steady state transport, the affinity of EAAC1 for glutamate in both the forward and reverse modes is strongly dependent on the pH on the cis-side of the membrane, whereas the currents at saturating glutamate concentrations are hardly affected by the pH. Consistent with this, the kinetics of the pre-steady state currents, measured after saturating glutamate concentration jumps, are not a function of the pH. In addition, we determined the deuterium isotope effect on EAAC1 kinetics, which is in agreement with proton cotransport but not OH(-) countertransport. The results can be quantitatively explained with an ordered binding model that includes a rapid proton binding step to the empty transporter followed by glutamate binding and translocation of the proton-glutamate-transporter complex. The apparent pK of the extracellular proton binding site is approximately 8. This value is shifted to approximately 6.5 when the substrate binding site is exposed to the cytoplasm.     

Upregulation of the transport system for TNFalpha at the blood-brain barrier

The transport system for the cytokine tumor necrosis factor-alpha (TNFalpha) at the blood-brain barrier (BBB) enables an enhanced yet saturable entry of TNFalpha from blood to the CNS. This review focuses on the selective upregulation of the transport system for TNFalpha at the BBB that is specific for type of pathology, region, and time. The upregulation is reflected by increased CNS tissue uptake of radiolabeled TNFalpha after iv injection in mice and by inhibition of this increase with excess non-radiolabeled TNFalpha. (1) Spinal cord injury (SCI): upregulation of TNFalpha uptake after thoracic transection is seen in the delayed phase of BBB disruption at the lumbar spinal cord. Thoracic SCI by compression, however, has a longer lasting impact on TNFalpha transport that involves thoracic and lumbar spinal cord, in contrast to the upregulation confined to the lumbar region in lumbar SCI by compression. Regardless, the uptake of TNFalpha by spinal cord does not parallel BBB disruption as measured by the leakage of radiolabeled albumin. (2) Experimental autoimmune encephalomyelitis (EAE): the increase in the differential permeability to TNFalpha is seen in all CNS regions (brain and cervical, thoracic, and lumbar spinal cord) and has a distinct time course and reversibility. Exogenous TNFalpha has biphasic effects in modulating functional scores. The BBB, a dynamically regulated barrier, is actively involved in disease processes.     

Electrogenic proton transport in epithelial membranes

Summary Certain polar epithelial cells have strong transport capacities for protons and can be examinedin vitro as part of an intact epithelial preparation. Recent studies in the isolated turtle bladder and other tight urinary epithelia indicate that the apical membranes of the carbonic anhydrase-containing cell population of these tissues contain an electrogenic proton pump which has the characteristics of a proton-translocating ATPase. The translocation of protons is tightly coupled to the energy of ATP hydrolysis. Since the pump translocates protons without coupling to the movement of other ions, it may be regarded as an ideal electrogenic pump. The apparent simplicity of the functional properties has led to extensive studies of the characteristics of this pump and of the cellular organization of the secondary acid-base flows in the turtle bladder. Over a rather wide range of electrochemical potential gradients for protons ( ) across the epithelium, the rate of H⁺ transport is nearly linear with . The formalisms of equivalent circuit analysis and nonequilibrium thermodynamics have been useful in describing the behavior of the pump, but these approaches have obvious limitations. We have attempted to overcome some of these limitations by developing a more detailed set of assumptions about each of the transport steps across the pump complex and to formulate a working model for proton transport in the turtle bladder that can account for several otherwise unexplained experimental results. The model suggests that the real pump is neither a simple electromotive force nor a constant current source. Depending on the conditions, it may behave as one or the other.     

Mechanism of proton transport by plant plasma membrane proton ATPases

The mechanism of proton translocation by P-type proton ATPases is poorly defined. Asp684 in transmembrane segment M6 of the Arabidopsis thaliana AHA2 plasma membrane P-type proton pump is suggested to act as an essential proton acceptor during proton translocation. Arg655 in transmembrane segment M5 seems to be involved in this proton translocation too, but in contrast to Asp684, is not essential for transport. Asp684 may participate in defining the E₁ proton-binding site, which could possibly exist as a hydronium ion coordination center. A model of proton translocation of AHA2 involving the side chains of amino acids Asp684 and Arg655 is discussed.     

Inhibitors of proton pumping: effect on passive proton transport

Reported inhibitors of the Characean plasmalemma proton pump were tested for their ability to inhibit the passive H⁺ conductance which develops in Chara corallina Klein ex Willd. at high pH. Diethylstilbestrol inhibits the proton pump and the passive H⁺ conductance with about the same time course, at concentrations that have no effect on cytoplasmic streaming. N-Ethylmaleimide, a sulfhydryl reagent which is small and relatively nonpolar, also inhibits both pumping and passive conductance of H⁺. However, it also inhibits cytoplasmic streaming with about the same time course, and therefore could not be considered a specific ATPase inhibitor. p-Chloromercuribenzene sulfonate (PCMBS), a sulfhydryl reagent which is large and charged and hence less able to penetrate the membrane, does not inhibit pumping or conductance at low concentration. At high concentration, PCMBS sometimes inhibits pumping without affecting H⁺ conductance, but since streaming is also inhibited, the effect on the pump cannot be said to be specific. 1-Ethyl-3-(3-dimethylaminopropyl)carbodiimide, a water soluble carbodiimide, weakly inhibits both pump and conductance, apparently specifically.     

Protein transport across the lung epithelial barrier

Alveolar lining fluid normally contains proteins of important physiological, antioxidant, and mucosal defense functions [such as albumin, immunoglobulin G (IgG), secretory IgA, transferrin, and ceruloplasmin]. Because concentrations of plasma proteins in alveolar fluid can increase in injured lungs (such as with permeability edema and inflammation), understanding how alveolar epithelium handles protein transport is needed to develop therapeutic measures to restore alveolar homeostasis. This review provides an update on recent findings on protein transport across the alveolar epithelial barrier. The use of primary cultured rat alveolar epithelial cell monolayers (that exhibit phenotypic and morphological traits of in vivo alveolar epithelial type I cells) has shown that albumin and IgG are absorbed via saturable processes at rates greater than those predicted by passive diffusional mechanisms. In contrast, secretory component, the extracellular portion of the polymeric immunoglobulin receptor, is secreted into alveolar fluid. Transcytosis involving caveolae and clathrin-coated pits is likely the main route of alveolar epithelial protein transport, although relative contributions of these internalization steps to overall protein handling of alveolar epithelium remain to be determined. The specific pathways and regulatory mechanisms responsible for translocation of proteins across lung alveolar epithelium and regulation of the cognate receptors (e.g., 60-kDa albumin binding protein and IgG binding FcRn) expressed in alveolar epithelium need to be elucidated.     

Nutrient transport and the blood-brain barrier in developing animals

Structural alterations in the development of the blood-brain barrier (BBB) can be seen in capillary profiles from the rat cortex. The neonatal luminal membrane is amplified with irregular folds, a possible adaptation to reduced cerebral blood flow rates. By 21 days the capillaries have resolved to a smooth-surfaced, adult-like appearance. Developmental alterations in the basement membrane, tight junctions, capillary seams, Golgi, pinocytotic vesicles, and cytoplasmic thickness are observed. Two studies have addressed developmental modulations in BBB polarity; both indicate that brain-to-blood transport mechanisms that were inoperative in the early neonatal rat become functional in weanlings. Six of the seven major independent BBB nutrient transport systems that regulate plasma-to-brain uptake have been kinetically characterized in the newborn rabbit, and comparisons have been made in the weanling (28-day-old) rabbit. All of these saturable transport systems are operative at birth, which suggests that the immature rabbit has a mature BBB with respect to regulation of nutrients. Purine base permeability, affinity, and uptake velocities are virtually unchanged during postnatal development. Subtle alterations in amino acid and amine transport were suggested by the lower-affinity (high-capacity) transport mechanisms characterized in the newborn as compared to the 28-day-old BBB. Under conditions of elevated plasma levels (typical of the neonate), these higher-capacity mechanisms would facilitate a relative increase in metabolite influx to the developing brain. Significant differences in kinetics were also observed for the monocarboxylic acid and hexose transport systems in the absence of developmental changes in permeability times surface area products. A low-affinity, high-capacity monocarboxylic acid transport system operates at birth. It supplies the developing brain with increased quantities of ketone bodies, but is seen as a high-affinity, low-capacity mechanism in the 28-day-old rabbit. Concomitantly, the higher-affinity glucose carrier defined in newborn rabbits modulates, and by 28 days becomes a lower-affinity, high-capacity mechanism capable of delivering about 2 mumol X min-1 X g-1 of glucose to the (anesthetized) brain.     

The influence of hydrophobic ions and dipolar molecules on the electrostatic barrier in biomembranes

To calculate the electric field inside a membrane the aqueous phase can be approximated by a conductor since the dielectric constant of water is much larger than that of the membrane. Then, using the method of image charges, ions adsorbed inside the membrane can be considered as dipoles and dipolar molecules adsorbed inside the membrane may similarly be regarded as sets of two similarly oriented dipoles. The microscopic interactions and, therefore, the spatial correlations of the adsorbed species can then be obtained. Together with the Gouy theory for the diffuse double layer these results allow the determination of the adsorbed phase—aqueous phase equilibrium. From the densities and spatial correlations of the adsorbed ions and dipolar species, their influence upon the electrostatic barrier as experienced by an ion translocating the membrane can be calculated. Changes observed in the relaxation time and initial conductance of translocating hydrophobic ions in voltage-pulse experiments on bilayer membranes are predicted using this model of the electrostatic barrier. In addition, an equation giving the surface tension as a function of the (non-ideal) adsorption of hydrophobic ions and dipoles is derived.