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A new Ca intracellular store, the acidocalcisome, has been reported in trypanosomatids. It has been characterized physiologically as a Ca store sensitive to nigericin. The Ca/H-ATPase is the system responsible for Ca accumulation, which depends on a pH gradient formed by ATP- and PPi-dependent proton pumps. In this work we present physiological and morphological evidences for the presence of acidocalcisomes in Trypanosoma evansi . The parasites were purified and loaded with the fluorescent dye Fura 2-AM in order to detect the intracellular changes of Ca levels in individual cells. The simultaneous incubation of T. evansi cells with ionomycin and nigericin led to large release of Ca (ca. 200 nM) from intracellular stores, which was not observed with either agent alone. On the other hand, no enhancement of the nigericin-induced Ca release was observed in the presence of oligomycin. Additionally, the pretreatment with bafilomycin decreases the nigericin-induced Ca release. These results confirm the presence of an intracellular non-mitochondrial acidic Ca storage compartment. These results suggest that H-ATPase is involved in the process of Ca accumulation into the acidocalcisomes. Furthermore, the cells loaded with acridine orange exhibited abundant fluorescent vacuoles, which were sensitive to nigericin or bafilomycin A 1 . Electronic transmission microscopy observations demonstrated the presence of electron dense particles in the parasites. High levels of inorganic pyrophosphate and triphosphate were detected in perchloric acid extracts of T. evansi by high resolution 31 P NMR. Taken together, these results present the first evidence for the presence of acidocalcisomes in T. evansi .

Mendoza, M., Mijares, A., Rojas, H., Ramos, M., and DiPolo, R. 2001. Trypanosoma evansi:A convenient model for studying intracellular Ca2+homeostasis using fluorometric ratio imaging from single parasites. Experimental Parasitology99, 213–219. The aim of this work was to measure, for the first time, the basal cytosolic Ca2+levels of Trypanosoma evansiand to explore the possibility of observing changes in the intracellular Ca2+concentration ([Ca2+]i) using fluorescence ratio imaging techniques in single isolated parasites of this species. Under appropriate loading conditions, the high intracellular levels of the Ca2+fluorescence probe Fura-2 permits resolution, in real time, of single parasite [Ca2+]isignals. Measurements of the basal [Ca2+]iindicate that homeostatic mechanisms maintain [Ca2+]iat 106 ± 38 (n= 32) nM in the presence of 2 mM extracellular calcium. The resting [Ca2+]iwas unaffected by changes in extracellular Ca2+in the range from 0 to 10 mM. The Ca2+ionophore A23187 induced a large increase in [Ca2+]iwhich (i) reached a steady state value even in the simultaneous presence of both external calcium and ionophore and (ii) returned to base line upon removal of extracellular Ca2+. A dose-response curve of the protonophore nigericin shows that T. evansicontains an important pH-sensitive intracellular pool which may be released by this drug with a K1/2of 8 μM. These data demonstrate that this parasite contains highly efficient systems to control [Ca2+]i. Finally, our results, with the use of sera as source of an antibody-complement to induce Ca2+entry, demonstrate that it is possible to resolve fast [Ca2+]isignals in single parasites from T. evansi.

1. Dialysed giant axons from the squid have been used to study some of the properties of the Na+ fluxes when the Na+ pump is fully inhibited by strophanthidin. 2. In axons which had been depleted of ATP, strophanthidin had no effect on Na+ efflux. Similar negative results were obtained in axons dialysed with and without internal or external K+, and with or without 100 microM‐internal Ca2+. 3. In the presence of 60 mM‐internal Na+, 440 mM‐external Na+ and strophanthidin, the fluxes of Na+ had the following characteristics. (i) ATP stimulated an efflux and an influx of Na+ of similar magnitude. The K1/2 for ATP, measured from its effect on Na+ efflux, was about 200 microM. (ii) The non‐hydrolysable ATP analogue adenylyl(beta, gamma‐methylene)‐diphosphonate (AMP‐PCP), at 2 mM concentration, either alone or in combination with 2 mM‐internal phosphate, failed to stimulate any efflux of Na+. (iii) The ATP‐dependent Na+ efflux was not affected by removal of internal or external K+, or external Mg2+ or Ca2+, and was not dependent on internal Ca2+. (iv) within the resolution of the method, all the ATP‐dependent Na+ influx required internal Na+, and all the ATP‐dependent Na+ efflux required external Na+. From the magnitude of the unidirectional Na+ fluxes the stoichiometry seemed to be a 1 to 1 Na+‐‐Na+ exchange. 4. The ATP‐internal Na+‐dependent influx of Na+ in the presence of strophanthidin was not affected by 1 mM‐vandate in the dialysis solution, a concentration which fully inhibits the Na+ efflux through the Na+ pump that is activated by external K+. 5. In the presence of external Na+, the external K+ sites of the Na+ pump are completely saturated with 100 mM‐external K+. In unpoisoned axons incubated with 100 mM‐external K+, replacement of external Na+ with Tris+ produced no change in the efflux of Na+. However, in axons poisoned with 50 microM‐strophanthidin, replacement of external Na+ with Tris+ resulted in a reversible inhibition of Na+ efflux. This could suggest that strophanthidin poisoning might induce Na+ (cations?) fluxes which are not present in normal conditions.

A combination of the voltage-clamp and the intracellular dialysis techniques has been used to study the membrane potential dependence of the Nao-dependent Ca efflux in squid giant axons. In order to improve axon survival, experiments were carried out using internal solutions prepared with large impermeant organic anions and cations, which did not affect the operation of the Na/Ca exchange mechanism. In axons dialyzed with solutions prepared without internal Na, the Nao-dependent Ca efflux had a small sensitivity to membrane potential changes. For a 25-mV membrane displacement in the hyperpolarizing direction, the basal Ca efflux increased by only 7.4% (n = 13). When the dialysis medium contained Na (from 20 to 55 mM), the efflux increased 32.3% (n = 25) for the same membrane potential change. The K1/2 for this effect is approximately 5 mM Na, and saturation appears to occur at a Na concentration above 20 mM. Adding ATP to the dialysis medium increased the magnitude of the Nao-dependent Ca efflux without changing its voltage sensitivity. Wide changes in the intracellular ionized Ca concentration (from 0.1 to 230 microM) did not modify the voltage sensitivity of the exchange system. Elimination of the reversal of Na/Ca exchange (Nai-dependent Ca influx) by removing Cao did not modify the voltage sensitivity of the Nao-dependent Ca efflux. When the axon membrane potential was submitted to prolonged changes, the corresponding changes in the Ca efflux were not sustained, but declined exponentially to intermediate values. This effect may indicate a slow inactivation process in the Na/Ca exchange mechanism. Voltage-clamp pulse experiments revealed: (a) the absence of a fast inactivation process in the Na/Ca exchange, and (b) that the activation of the carrier for hyperpolarizing pulses occurs as rapidly as 1 ms.

We have studied the interaction of physiological ligands other than Nai and Cai with the Ca pump and Na/Ca exchange in internally dialyzed squid axons. The results show the following. (a) Internal Mg2+ is an inhibitor of the Nao-dependent Ca efflux. At physiological Mg2+i (4 mM), the inhibition amounts to approximately 50%. The inhibition is partial and noncompetitive with Cai, and is not affected by Nai or ATP. The ATP-dependent uncoupled efflux is unaffected by Mgi up to 20 mM. Both components of the Ca efflux require Mg2+i for their activation by ATP. (b) At constant membrane potential, Ki is an important cofactor for the uncoupled Ca efflux. (c) Orthophosphate (Pi) activates the Nao-dependent Ca efflux without affecting the uncoupled component. Activation by Pi occurs only in the presence of Mg-ATP or hydrolyzable ATP analogues. Pi under physiological conditions has no effect on the uncoupled component; nevertheless, at alkaline pH, it inhibits the Ca pump, probably by product inhibition. (d) ADP is a potent inhibitor of the uncoupled Ca efflux. The Nao-dependent component is inhibited by ADP only at much higher ADP concentrations. These results indicate that (a) depending on the concentration of Ca2+i, Na+i Mg2+i, and Pi, the Na/Ca carrier can operate under a low- or high-rate regime; (b) the interactions of Mg2+i, Pi, Na+i, and ATP with the carrier are not interdependent; (c) the effect of Pi on the carrier-mediated Ca efflux resembles the stimulation of the Nao-dependent Ca efflux by internal vanadate; (d) the ligand effects on the uncoupled Ca efflux are of the type seen in the Ca pump in red cells and the sarcoplasmic reticulum.

Values for ionized [Ca] in squid axons were obtained by measuring the light emission from a 0.1-mul drop of aequorin confined to a plastic dialysis tube of 140-mum diameter located axially. Ionized Ca had a mean value of 20 x 10(-9) M as judged by the subsequent introduction of CaEGTA/EGTA buffer (ratio ca. 0.1) into the axoplasm, and light measurement on a second aequorin drop. Ionized Ca in axoplasma was also measured by introducing arsenazo dye into an axon by injection and measuring the Ca complex of such a dye by multichannel spectrophotometry. Values so obtained were ca. 50 x 10(-9) M as calibrated against CaEGTA/EGTA buffer mixtures. Wth a freshly isolated axon in 10 mM Ca seawater, the aequorin glow invariably increased with time; a seawater [Ca] of 2-3 mM allowed a steady state with respect to [Ca]. Replacement of Na+ in seawater with choline led to a large increase in light emission from aequorin. Li seawater partially reversed this change and the reintroduction of Na+ brought light levels back to their initial value. Stimulation at 60/s for 2-5 min produced an increase in aequorin glow about 0.1% of that represented by the known Ca influx, suggesting operationally the presence of substantial Ca buffering. Treatment of an axon with CN produced a very large increase in aequorin glow and in Ca arsenazo formation only if the external seawater contained Ca.

In squid axons, internally applied ATP potentiates the magnitude of the potassium conductance and slows down its activation kinetics. This effect was characterized using internally dialyzed axons under voltage-clamp conditions. Both amplitude potentiation and kinetic slow-down effects are very selective towards ATP, other nucleotides like GTP and ITP are ineffective in millimolar concentrations. The current potentiation Km for ATP is near 10 microM with no further effects for concentrations greater than 100 microM. ATP effect is most likely produced via a phosphorylative reaction because Mg ion is an obligatory requirement and nonhydrolyzable ATP analogues are without effect. In the presence of ATP, the K current presents more delay, resembling a Cole-Moore effect due to local hyperpolarization of the channel. ATP effect induces a 10-20 mV shift in both activation and inactivation parameters towards more depolarized potentials. As a consequence of this shift, conductance-voltage curves with and without ATP cross at approximately -40 mV. This result is consistent with the hyperpolarization observed with ATP depletion, which is reversed by ATP addition. At potentials around the resting value, addition of ATP removes almost completely K current slow inactivation. It is suggested that a change in the amount of the slow inactivation is responsible for the differences in current amplitude with and without ATP, possibly as a consequence of the additional negative charge carried by the phosphate group. However, a modification of the local potential is not enough to explain completely the differences under the two conditions.

We have used dialyzed squid axons to characterize the ouabain- and bumetanide-insensitive Na efflux components and their relation to the operation of the Na/Ca exchange mechanism. In axons dialyzed with solutions containing nearly physiological concentrations of K, Na, and Mg, three components of the Na efflux can be distinguished: Cai-activated, Cao-dependent Na efflux ("reverse" Na/Ca exchange); Cai-activated, Nao-dependent Na efflux; and Cai-independent, ATP-activated, Nao-dependent Na efflux. We have studied the effects of internal alkalinization, Mgi, Cao, and the ATP analogue [gamma-thio]ATP (ATP gamma S) on the different components of the Na efflux. The results show the following: (a) internal alkalinization activates both Cao- and Nao-dependent Na efflux components provided that Cai is present; (b) Mgi inhibits both the Cai-activated, Cao- and Nao-dependent Na efflux components; (c) Cao inhibits the Nao-dependent component by competition for a common site; (d) ATP gamma S activates both Nao- and Cao-dependent Na efflux components only in the presence of Cai; and (e) ATP activates the Nai/Nao and Nai/Cao exchanges, causing a 10-fold increase in the affinity of the reverse Na/Ca exchange toward Cai. In the absence of Cai, ATP stimulates an Nao-dependent Na efflux that is not affected either by internal alkalinization or high Cao. The ATP analogue does not activate the Cai-independent Na/Na exchange system. These experiments demonstrate that the Cai-activated Na/Na exchange is a mode of operation of the Na/Ca exchange mechanism that substantially contributes to Na movement during the activation of the Na/Ca antiporter. The experimental evidence obtained on the Cai-independent Na/Na exchange component shows that this system is not part of the Na/Ca exchange.

A method has been developed to measure Ca influx in internally dialyzed squid axons. This was achieved by controlling the dialyzed segment of the axon exposed to the external radioactive medium. The capacity of EGTA to buffer all the Ca entering the fiber was explored by changing the free EGTA at constant [Ca++]i. At a free [EGTA]i greater than 200 microM, the measured resting Ca influx and the expected increment in Ca entry during electrical stimulation were independent of the axoplasmic free [EGTA]. To avoid Ca uptake by the mitochondrial system, cyanide, oligomycin, and FCCP were included in the perfusate. Axons dialyzed with a standard medium containing: [ATP] = 2 mM, [Ca++]i = 0.06 microM, [Ca++]o = 10 mM, [Na+]i = 70 mM, and [Na+]o = 465 mM, gave a mean Ca influx of 0.14 +/- 0.012 pmol.cm-2.s-1 (n = 12. Removal of ATP drops the Ca influx to 0.085 +/- 0.007 pmol.cm-2.s-1 (n = 12). Ca influx increased to 0.35 pmol.cm-2,s-1 when Nao was removed. The increment was completely abolished by removing Nai+ and (or) ATP from the dialysis medium. At nominal zero [Ca++]i, no Nai-dependent Ca influx was observed. In the presence of ATP and Nai [Ca++]i activates the Ca influx along a sigmoid curve without saturation up to 1 microM [Ca++]i. Removal of Nai+ always reduced the Ca influx to a value similar to that observed in the absence of [Ca++]i (0.087 +/- 0.008 pmol.cm-2.s-1; n = 11). Under the above standard conditions, 50-60% of the total Ca influx was found to be insensitive to Nai+, Cai++, and ATP, sensitive to membrane potential, and partially inhibited by external Co++.

Tension development in voltage-clamped barnacle muscle fibers occurs with depolarizing pulses so small as not to activate the potassium and calcium conductance systems. Peak tension and the tension time integral appear to be graded by both amplitude and duration of the depolarizing pulses. Subthreshold depolarizing conditioning pulses shorter than 500 ms potentiate the response to a given test pulse. This effect diminishes and reverts when the duration of the conditioning pulse is increasingly prolonged. The relationship between fiber membrane potential and tension developed in response to depolarizing pulses is described by an S-shaped curve. The tension saturates at a membrane potential of about +10 mV (inside positive). For a given pulse duration the saturation value remains constant even when the fiber interior reaches a value of +230 mV, which is well above what may be estimated to be the equilibrium potential of calcium ions (Eca = +120). In the presence of 5 mM external procaine, the shape of the tension-potential curve changes; the maximum value tension besides being diminished is not sustained by falls when the potential approaches the estimated value for Eca. These results suggest that under physiological conditions the contractile activator is probably released from an internal store, and that the calcium entering the fiber as inward current does not play a direct major role in contractile activation.

The magnitude of the activating effect of ATP on the Ca efflux was explored at different [Ca++]i in squid axons previously exposed to cyanide seawater and internally dialyzed with a medium free of ATP and containing p-trifluoro methoxy carbonyl cyanide phenyl hydrazine. At the lowest [Ca++]i used (0.06 micron more than 95% of the Ca efflux depends on ATP. At high [Ca++]i (100 micron), 50-60% of the Ca efflux still depends on ATP. The apparant affinity constant for ATP was not significantly affected in the range of [Ca++]i from 0.06 to 1 micron. Axons dialyzed to reduce their internal magnesium failed to show the usual activation of the Ca efflux when the Tris or the sodium salt of ATP was used. Only in the presence of internal magnesium is ATP able to stimulate the Ca efflux. Nine naturally occurring high-energy phosphate compounds were ineffective in supporting calcium efflux. These compounds were: UTP, GTP, CTP, UDP, CDP, ADP, AMP, CAMP, and acetyl phosphate. The compounds 2' deoxy-ATP and the hydrolyzable analog alpha,beta-methylene ATP were able to activate the Ca efflux. The nonhydrolyzable analog beta,gamma-methylene ATP competes with ATP for the activating site, but is unable to activate the Ca efflux. The results are discussed in terms of the specificity of the nucleotide site responsible for the ATP-dependent Ca efflux.

The diffusion of two series of alcohols and amides through complex cellulose acetate membranes was studied. The thin dense part of these membranes behaves as a nonporous layer of low water content. In this layer, called the skin, the solute diffusion coefficients, ω, depend upon size, steric configuration, and the partition coefficient, K8, between membrane and bathing solution. From the experimental values of ω and K8, the over-all friction, f, experienced by the solutes in the membrane was computed. It was found that f depends upon the chemical nature of the solute and is related to hydrogen-bonding ability. In the coarse, porous layer of the cellulose acetate membrane, diffusion occurs mainly through aqueous channels. In this instance also the hydrogen-bonding ability of the solute seems to exercise a smaller but significant influence.

The transport parameters of a cellulose acetate membrane prepared from a mixture of cellulose acetate, formamide, and acetone, 25:25:50 by weight, were studied. The membrane consists of a thin, porous layer, the skin, in series with a thick, highly porous layer, the coarse support. In the skin the diffusional permeability coefficient, ω, of a number of small amides and alcohols depends critically upon the partition coefficient, Ks, the size of the molecule, and the apparent hydrogen-bonding ability, Ns, of the solute. These observations are in general agreement with our earlier conclusions on the properties of nonporous membranes. On the other hand, the corrected reflection coefficient, σ', is not a very sensitive function of either Ns or Ks taken separately. The correlation between σ' and molecular diameter is reasonably good; however, it is much improved when both Ns and Ks are taken into consideration. Isotope interaction was also studied in the present preparation and was found to provide only a small (5–8%) contribution to the diffusional permeability coefficient of ethylene glycol. The contribution of solute-water friction was found to be less than 24% of the total solute friction.

Chloride outflux and influx has been studied in single isolated muscle fibers from the giant barnacle under constant internal composition by means of a dialysis perfusion technique. Membrane potential was continually recorded. The chloride outfluxes and influxes were 143 and 144 pmoles/cm2-sec (mean resting potential: 58 mv, temperature: 22°–24°C) with internal and external chloride concentrations of 30 and 541 mM, respectively. The chloride conductance calculated from tracer measurements using constant field assumptions is about fourfold greater than that calculated from published electrical data. Replacing 97% of the external chloride ions by propionate reduces the chloride efflux by 51%. Nitrate ions applied either to the internal or external surface of the membrane slows the chloride efflux. The external pH dependence of the chloride efflux follows the external pH dependence of the membrane conductance, in the range pH 3.9–4.7, increasing with decreasing pH. In the range pH 5–9, the chloride efflux increased with increasing pH, in a manner similar to that observed in frog muscle fibers. The titration curve for internal pH changes in the range 4.0–7.0 was quantitatively much different from that for external pH change, indicating significant asymmetry in the internal and external pH dependence of the chloride efflux.