Charge-to-substrate ratio during organic cation uptake by rat OCT2 is voltage dependent and altered by exchange of glutamate 448 with glutamine.

Uptake of substrate and electric charge was measured simultaneously in voltage-clamped Xenopus laevis oocytes expressing rat organic cation transporter 2 (rOCT2). At 0 mV, saturating substrate concentrations induced uptake of more positive elementary charges than monovalent organic cations, with charge-to-substrate ratios of 1.5 for guanidinium(+), 3.5 for tetraethylammonium(+), and 4.0 for 1-methyl-4-phenylpyridinium(+). At negative holding potentials, the charge-to-substrate ratios decreased toward unity. At 0 mV, charge-to-substrate ratios higher than unity were observed at different extracellular pH and after replacement of extracellular Na(+), K(+), Ca(2+), Mg(2+), and/or Cl(-). Charge-to-substrate ratios were not influenced by intracellular succinate(2-) or glutarate(2-). The effects of membrane potential and ion substitution strongly suggest that the surplus of transported positive charge is not generated by passive ion permeabilities. Rather, we hypothetize that small cations are taken up together with organic cation substrates whereas the outward reorientation of the empty transporter is electroneutral. Nonselective cotransport of small cations was supported by the three-dimensional structures of rOCT2 in its inward-facing and outward-facing conformations, which we determined by homology modeling based on known corresponding structures of H(+)-lactose permease of E. coli, and by functional analysis of OCT mutants. In our model, the innermost cavity of the outward-open binding cleft is negatively charged by Glu448 and Asp475, whereas the inward-open innermost cavity is electroneutral, containing Asp379, Asp475, Lys215, and Arg440. Substitution of Glu448 by glutamine reduced the charge-to-TEA(+) ratio at 0 mV to unity. The observed charge excess associated with organic cation uptake into depolarized cells may contribute to tubular damage in renal failure.

Reconstitution of depolarization and Ca2+-evoked secretion in Xenopus oocytes monitored by membrane capacitance.

The identity of the proteins that constitute the "minimal molecular machinery" required for depolarization-evoked neurotransmitter release at synapses is still not fully disclosed. Using capacitance monitoring combined with heterologous protein expression in Xenopus oocytes, we were able to reconstitute a fast (<.5 s) secretion that was triggered directly by membrane depolarization. The functional assembly of voltage-gated Ca2+ channel (Cav1.2 or Cav2.2) coexpressed with syntaxin 1A, synaptosome-associated protein of 25 kDa (SNAP-25), and synaptotagmin led to the reconstitution of depolarization-evoked secretion. Botulinum C1, botulinum A, and tetanus toxin were used to establish that this minimal set of proteins, named the excitosome complex, was necessary and sufficient for reconstituting depolarization-induced exocytosis. Similar to synaptic transmission, the capacitance changes were sensitive to neurotoxins, modulated by divalent cations (Ca2+, Ba2+, and Sr2+) or channels (Lc or N type; ionotropic glutamate GLUR3), and depended nonlinearly on extracellular divalent cation concentration. Expression of a recombinant intracellular domain of the calcium channel (Lc753-893) abolished evoked release in the reconstituted assay. Also, mutations at the synaptotagmin C2A polylysine motif, a channel interaction site, abolished depolarization-evoked capacitance transients, consistent with release studies in PC12 cells. Because of its improved speed, native trigger, and great experimental versatility, this reconstitution assay provides a novel, promising tool to study synaptic and nonsynaptic exocytosis and examine the role of other proteins implicated in these processes.

Identification of cysteines in rat organic cation transporters rOCT1 (C322, C451) and rOCT2 (C451) critical for transport activity and substrate affinity.

Effects of the sulfhydryl reagent methylmethanethiosulfonate (MMTS) on functions of organic cation transporters (OCTs) were investigated. Currents induced by 10 mM choline [I(max(choline))] in Xenopus laevis oocytes expressing rat OCT1 (rOCT1) were increased four- to ninefold after 30-s incubation with 5 mM MMTS whereas I(max(choline)) by rat OCT2 was 70% decreased. MMTS activated the rOCT1 transporter within the plasma membrane without changing stoichiometry between translocated charge and cation. After modification of oocytes expressing rOCT1 or rOCT2 with MMTS, I(0.5(choline)) values for choline-induced currents were increased. For rOCT1 it was shown that MMTS increased I(0.5) values for different cations by different degrees. Mutagenesis of individual cysteine residues in rOCT1 revealed that modification of cysteine 322 in the large intracellular loop, and of cysteine 451 at the transition of the transmembrane alpha-helix (TMH) 10 to the short intracellular loop between the TMH 10 and 11 is responsible for the observed effects of MMTS. After replacement of cysteine 451 by methionine, the IC(50(choline)) for choline to inhibit MPP uptake by rOCT1 was increased whereas the I(0.5(choline)) value for choline-induced current remained unchanged. At variance, in double mutant Cys322Ser, Cys451Met, I(0.5(choline)) was increased compared with rOCT1 wild-type whereas in the single mutant Cys322Ser I(0.5(choline)) was not changed. The data suggest that modification of rOCT1 at cysteines 322 and 451 leads to an increase in turnover. They indicate that cysteine 451 in rOCT1 interacts with the large intracellular loop and that cysteine 451 in both rOCT1 and rOCT2 is critical for the affinity of choline.

Molecular identification and reconstitution of depolarization-induced exocytosis monitored by membrane capacitance.

Regulated exocytosis of neurotransmitters at synapses is fast and tightly regulated. It is unclear which proteins constitute the "minimal molecular machinery" for this process. Here, we show that a novel technique of capacitance monitoring combined with heterologous protein expression can be used to reconstitute exocytosis that is fast (<0.5 s) and triggered directly by membrane depolarization in Xenopus oocytes. Testing synaptic proteins, voltage-gated Ca2+ channels, and using botulinum and tetanus neurotoxins established that the expression of a Ca2+ channel together with syntaxin 1A, SNAP-25, and synaptotagmin was sufficient and necessary for the reconstitution of depolarization-induced exocytosis. Similar to synaptic exocytosis, the reconstituted release was sensitive to neurotoxins, modulated by divalent cations (Ca2+, Ba2+, and Sr2+) or channel (Lc-, N-type), and depended nonlinearly on divalent cation concentration. Because of its improved speed, native trigger, and great experimental versatility, this reconstitution assay provides a novel, promising tool to study synaptic exocytosis.

Alkali cation binding and permeation in the rat organic cation transporter rOCT2.

Organic cation transporters of the OCT family mediate downhill transport of organic cations, compatible with carrier, pore, or gate-lumen-gate mechanisms. We studied rat OCT2 expressed in Xenopus oocytes by the two-electrode voltage-clamp technique, including membrane capacitance (C(m)) monitoring. Choline, a transported cationic substrate, elicited the expected inward currents but also elicited decreases of C(m). Similar C(m) decreases were caused by the non-transported inhibitors tetrabutylammonium (a cation) and corticosterone (uncharged). Effects on C(m) were voltage-dependent, with a maximum at -140 mV. These findings suggest that the empty rOCT2 protein can undergo an electrogenic conformation change, with one conformation highly favored at physiological voltage. Moreover, alkali cations elicited considerable inward currents and inhibited uptake of [(14)C]tetraethylammonium with a sequence Cs(+) > Rb(+) > K(+) > Na(+) approximately Li(+). Cs(+) affected current and capacitance with similar affinity (K(0.5) approximately 50 mm). Tetraethylammonium inhibited Cs(+) currents in a concentration-dependent manner. Conversely, Cs(+) inhibited tetraethylammonium uptake by a competitive mechanism. Activation energy of the currents estimated from measurements between 12 degrees C and 32 degrees C was approximately 81 kJ/mol for Cs(+) and 39 kJ/mol for tetramethylammonium, compatible with permeation of Cs(+) through rOCT2 along the same path as organic substrates and by a mechanism different from simple electrodiffusion. Rationalization of Cs(+) selectivity in terms of a pore pointed to a pore diameter of approximately 4 A. Intriguingly, that value matches the known selectivity of rOCT2 for organic compounds. Our data show that selective permeability of rOCT2 is not determined by ligand affinity but might rather be understood in terms of the ion channel concept of a distinct "selectivity filter."

The quantitation of buffering action I. A formal & general approach.

BACKGROUND: Although "buffering" as a homeostatic mechanism is a universal phenomenon, the quantitation of buffering action remains controversial and problematic. Major shortcomings are: lack of a buffering strength unit for some buffering phenomena, multiple and mutually incommensurable units for others, and lack of a genuine ratio scale for buffering strength. Here, I present a concept of buffering that overcomes these shortcomings. THEORY: Briefly, when, for instance, some "free" H+ ions are added to a solution (e.g. in the form of strong acid), buffering is said to be present when not all H+ ions remain "free" (i.e., bound to H2O), but some become "bound" (i.e., bound to molecules other than H2O). The greater the number of H+ ions that become "bound" in this process, the greater the buffering action. This number can be expressed in two ways: 1) With respect to the number of total free ions added as "buffering coefficient b", defined in differential form as b = d(bound)/d(total). This measure expresses buffering action from nil to complete by a dimensionless number between 0 and 1, analogous to probabilites. 2) With respect to the complementary number of added ions that remain free as "buffering ratio B", defined as the differential B = d(bound)/d(free). The buffering ratio B provides an absolute ratio scale, where buffering action from nil to perfect corresponds to dimensionless numbers between 0 and infinity, and where equal differences of buffering action result in equal intervals on the scale. Formulated in purely mathematical, axiomatic form, the concept reveals striking overlap with the mathematical concept of probability. However, the concept also allows one to devise simple physical models capable of visualizing buffered systems and their behavior in an exact yet intuitive way. CONCLUSION: These two measures of buffering action can be generalized easily to any arbitrary quantity that partitions into two compartments or states, and are thus suited to serve as standard units for buffering action. Some exemplary treatments of classical and non-classical buffering phenomena are presented in the accompanying paper.

The quantitation of buffering action II. Applications of the formal & general approach.

BACKGROUND: The paradigm of "buffering" originated in acid-base physiology, but was subsequently extended to other fields and is now used for a wide and diverse set of phenomena. In the preceding article, we have presented a formal and general approach to the quantitation of buffering action. Here, we use that buffering concept for a systematic treatment of selected classical and other buffering phenomena. RESULTS: H+ buffering by weak acids and "self-buffering" in pure water represent "conservative buffered systems" whose analysis reveals buffering properties that contrast in important aspects from classical textbook descriptions. The buffering of organ perfusion in the face of variable perfusion pressure (also termed "autoregulation") can be treated in terms of "non-conservative buffered systems", the general form of the concept. For the analysis of cytoplasmic Ca++ concentration transients (also termed "muffling"), we develop a related unit that is able to faithfully reflect the time-dependent quantitative aspect of buffering during the pre-steady state period. Steady-state buffering is shown to represent the limiting case of time-dependent muffling, namely for infinitely long time intervals and infinitely small perturbations. Finally, our buffering concept provides a stringent definition of "buffering" on the level of systems and control theory, resulting in four absolute ratio scales for control performance that are suited to measure disturbance rejection and setpoint tracking, and both their static and dynamic aspects. CONCLUSION: Our concept of buffering provides a powerful mathematical tool for the quantitation of buffering action in all its appearances.

The concept of "buffering" in systems and control theory: from metaphor to math.

The paradigm of "buffering" is used increasingly for the description of diverse "systemic" phenomena encountered in evolutionary genetics, ecology, integrative physiology, and other areas. However, in this new context, the paradigm has not yet matured into a truly quantitative concept inasmuch as it lacks a corresponding quantitative measure of "systems-level buffering strength". Here, I develop such measures on the basis of a formal and general approach to the quantitation of buffering action. "Systems-level buffering" is shown to be synonymous with "disturbance rejection" in feedback-control systems, and can be quantitated by means of dimensionless proportions between partial flows in two-partitioned systems. The units allow either the time-independent, "static" buffering properties or the time-dependent, "dynamic" ones to be measured. Analogous to this "resistance to change", one can define and measure the "conductance to change"; this quantity corresponds to "set-point tracking" in feedback-control systems. Together, these units provide a systematic framework for the quantitation of buffering action in systems biology, and reveal the common principle behind systems-level buffering, classical acid-base buffering, and multiple other manifestations of buffering.

Role of glycosylation in the renal electrogenic Na+-HCO3- cotransporter (NBCe1).

The electrogenic Na(+)-HCO(3)(-) cotransporter NBCe1 is important for the regulation of intracellular pH (pH(i)) and for epithelial HCO(3)(-) transport in many tissues, including kidney, pancreas, and brain. In the present study, we investigate glycosylation sites in NBCe1. Treatment of rat kidney membrane extracts with peptide N-glycosidase F (PNGase F) shifted the apparent molecular weight (MW) of NBCe1 from 130 to 116, the MW predicted from the deduced amino acid sequence. Treatment with endoglycosidase F(2) or H or O-glycosidase did not affect the MW of NBCe1. Lectin-binding studies, together with the enzyme data, suggest that the N-linked carbohydrates are of tri- or tetra-antennary type. To localize glycosylation sites, we individually mutated the seven consensus N-glycosylation sites by replacing asparagine (N) with glutamine (Q) and assessing mutant transporters in Xenopus laevis oocytes. Immunoblotting of oocyte membrane extracts treated with PNGase F indicates that NBCe1 is normally glycosylated at N597 and N617 (both on the third extracellular loop). However, N592 (on the same loop) is glycosylated when the other two sites are mutated. The triple mutant (N592Q/N597Q/N617Q) is completely unglycosylated but, based on microelectrode measurements of membrane potential and pH(i) in oocytes, preserves the Na(+) and HCO(3)(-) dependence and electrogenicity of wild-type NBCe1.

An improved method for real-time monitoring of membrane capacitance in Xenopus laevis oocytes.

Measurements of membrane capacitance (C(m)) in Xenopus laevis oocytes offer unique experimental possibilities but are difficult to perform with current methods. To improve C(m) measurements in the two-electrode voltage clamp (TEVC) mode, we developed a paired-ramp protocol and tested its performance in a model circuit (with tunable C(m), membrane resistance R(m), and series resistance R(s)) and in Xenopus oocytes. In the cell model and with R(s) = 0 Omega, inaccuracy of C(m) estimates was <1% under widely varying conditions (R(m) ranging from 100 to 2000 kOmega, and C(m) from 50 to 1000 nF). With R(s) > 0 Omega, C(m) was underestimated by a relative error epsilon closely approximated as epsilon approximate 2 x R(s)/(R(s) + R(m)), in keeping with the theoretical prediction. Thus, epsilon may be neglected under standard conditions or, under extreme conditions, corrected for if R(s) is known. Relative imprecision of C(m) estimates was small, independent of R(s), and inversely related to C(m) (<1.5% at 50 nF, <0.4% at 200 nF). Averaging allowed reliable detection of C(m) deviations from 200 nF of 0.1 nF, i.e., 0.05%. In Xenopus oocytes, we could resolve C(m) changes that were small (e.g., DeltaC(m) approximate 2 nF upon 100 muM 8-Br-cAMP), fast (e.g., DeltaC(m)/Deltat approximate 20nF/30s upon 1 muM phorbol myristate acetate (PMA)) or extended and complex (e.g., fast increase, followed by prolonged C(m) decrease upon 1 muM PMA). Rapidly alternating between paired ramps and a second, step protocol allowed quasi-simultaneous monitoring of additional electrical parameters such as R(m), slope conductance g(m), and reversal potential E(rev). Taken together, our method is suited to monitor C(m) in Xenopus oocytes conveniently, with high temporal resolution, accuracy and precision, and in parallel with other electrical parameters. Thus, it may be useful for the study of endo- and exocytosis and of membrane protein regulation and for electrophysiological high-throughput screening.

Immunoelectron microscopic localization of the electrogenic Na/HCO(3) cotransporter in rat and ambystoma kidney.

Immunofluorescence analysis has revealed that electrogenic Na(+)/HCO(3)(-) (NBC1) is expressed in the proximal tubule of rat kidney and in the proximal and distal tubules of the salamander AMBYSTOMA: tigrinum kidney. The present study was undertaken to define the detailed subcellular localization of the NBC1 in rat and AMBYSTOMA: kidney using high-resolution immunoelectron microscopy. For this purpose, two rabbit polyclonal antibodies raised against amino acids 928 to 1035 and amino acids 1021 to 1035 of the C-terminus of rat kidney (rkNBC1) were developed. The affinity-purified antibodies revealed a strong band of approximately 140 kD in immunoblots of membranes from rat kidney cortex but no signal in membranes isolated from outer and inner medulla. Deglycosylation reduced the apparent molecular weight to approximately 120 kD, corresponding to the predicted molecular weight. A similar but weaker band was also present in membranes isolated from the lateral part of Ambystoma: kidney. In rat kidney, immunohistochemistry confirmed the presence of rkNBC1 in convoluted segments of the proximal tubules. In ultrathin cryosections or Lowicryl HM20 sections from rat kidney cortex, distinct immunogold labeling was associated with the basolateral plasma membrane of segments S1 and S2 of proximal tubules, whereas in S3 no labeling was observed. The labeling density was similar at the basal and lateral plasma membrane and was specifically associated with the inner surface of the membrane consistent with the internal position of the C-terminus of the transporter. In contrast, rkNBC1 was absent from the apical plasma membrane and not observed in intracellular vesicles, including those closely associated with basolateral plasma membrane. In Ambystoma: kidney, a weak labeling was present in the basolateral membrane of the proximal tubule and stronger labeling was observed in the late distal segment. The results demonstrate that rkNBC1 is expressed only in segment S1 and segment S2 of rat proximal tubule as well as Ambystoma: proximal and late distal tubule and that rkNBC1 is present in both basal and lateral plasma membranes and absent in intracellular vesicles of the apical plasma membrane.