Isolation and some characteristics of cell nuclei from brain cortex of adult cat

A rapid detergent method for the isolation of nuclei from cat brain cortex is described. It involves the homogenization of the tissue in buffered 0.34 M sucrose with the addition of the non-ionic detergent Cemulsol NPT 12 and the subsequent low speed centrifugal sieving of the nuclei through two layers of sucrose (0.68 M and 1.0 M). The final purification is achieved by high speed centrifugation (40,000 g) of the nuclear suspension layered over 1.8 M sucrose. Observations by light microscopy indicate that highly purified and well preserved nuclei are obtained from neurons and glial cells. Electron microscopy reveals some microsomal contaminants adhering to the nuclear membrane. According to an analysis of the nuclear size distribution, a considerable loss of smaller nuclei (10 to 20µ²), mainly from glial cells, occurs during the purification procedure. The action of different detergents is compared, the best results being obtained with Cemulsol NPT 12 or Triton X-100. Chemical analyses of the purified nuclear fraction give the following content expressed in picograms per nucleus: DNA, 6.54; RNA, 2.94; cholesterol, 1.50; and protein, 97.5. The sucrose density gradient centrifugation of nuclei isolated from cat brain cortex shows that their density is equal to or higher than that of 2.2 M sucrose and is thus similar to the density of nuclei from other tissues. The observation of a varying influence of different suspending media on the density of brain cell nuclei resolves the conflicting data in the literature on the density of these nuclei.     

Thymidine transport by cultured Novikoff hepatoma cells and uptake by simple diffusion and relationship to incorporation into deoxyribonucleic acid

The initial rate of thymidine-³H incorporation into the acid-soluble pool by cultured Novikoff rat hepatoma cells was investigated as a function of the thymidine concentration in the medium. Below, but not above 2 µM, thymidine incorporation followed normal Michaelis-Menten kinetics at 22°, 27°, 32°, and 37°C with an apparent K_m of 0.5 µM, and the V_max values increased with an average Q₁₀ of 1.8 with an increase in temperature. The intracellular acid-soluble ³H was associated solely with thymine nucleotides (mainly deoxythymidine triphosphate [dTTP]). Between 2 and 200 µM, on the other hand, the initial rate of thymidine incorporation increased linearly with an increase in thymidine concentration in the medium and was about the same at all four temperatures. Pretreatment of the cells with 40 or 100 µM p-chloromercuribenzoate for 15 min or heat-shock (49.5°C, 5 min) markedly reduced the saturable component of uptake without affecting the unsaturable component or the phosphorylation of thymidine. The effect of p-chloromercuribenzoate was readily reversed by incubating the cells in the presence of dithiothreitol. Persantin and uridine competitively inhibited thymidine incorporation into the acid-soluble pool without inhibiting thymidine phosphorylation. At concentrations below 2 µM, thymidine incorporation into DNA also followed normal Michaelis-Menten kinetics and was inhibited in an apparently competitive manner by Persantin and uridine. The apparent K_m and K_i values were about the same as those for thymidine incorporation into the nucleotide pool. The over-all results indicate that uptake is the rate-limiting step in the incorporation of thymidine into the nucleotide pool as well as into DNA. The cells possess an excess of thymidine kinase, and thymidine is phosphorylated as rapidly as it enters the cells and is thereby trapped. At low concentrations, thymidine is taken up mainly by a transport reaction, whereas at concentrations above 2 µM simple diffusion becomes the principal mode of uptake. Evidence is presented that indicates that uridine and thymidine are transported by different systems. Upon inhibition of DNA synthesis, net thymidine incorporation into the acid-soluble pool ceased rapidly. Results from pulse-chase experiments indicate that a rapid turnover of dTTP to thymidine may be involved in limiting the level of thymine nucleotides in the cell.     

Cholinesterase activity per unit surface area of conducting membranes

According to theory, the action of acetylcholine (ACh) and ACh-esterase is essential for the permeability changes of excitable membranes during activity. It is, therefore, pertinent to know the activity of ACh-esterase per unit axonal surface area instead of per gram nerve, as it has been measured in the past. Such information has now been obtained with the newly developed microgasometric technique using a magnetic diver. (1) The cholinesterase (Ch-esterase) activity per mm² surface of sensory axons of the walking leg of lobster is 1.2 x 10^-3 µM/hr. (σ = ± 0.3 x 10^-3; SE = 0.17 x 10^-3); the corresponding value for the motor axons isslightly higher: 1.93 x 10^-3 µM/hr. (σ = ± 0.41 x 10^-3; SE = ± 0.14 x 10^-3). Referred to gram nerve, the Ch-esterase activity of the sensory axons is much higher than that of the motor axons: 741 µM/hr. (σ = ± 73.5; SE = ± 32.6) versus 111.6 µM/hr. (σ = ± 28.3; SE = ± 10). (2) The enzyme activity in the small fibers of the stellar nerve of squid is 3.2 x 10^-4 µM/mm²/hr. (σ = ± 0.96 x 10^-4; SE = ± 0.4 x 10^-4). (3) The Ch-esterase activity per mm² surface of squid giant axon is 9.5 x 10^-5 µM/hr. (σ = ± 1.55 x 10^-5; SE = ± 0.38 x 10^-5). The value was obtained with small pieces of carefully cleaned axons after removal of the axoplasm and exposure to sonic disintegration. Without the latter treatment the figurewas 3.85 x 10^-5 µM/mm²/hr. (σ = ± 3.24 x 10^-5; SE = ± 0.93 x 10^-5). The experiments indicate the existence of permeability barriers in the cell wall surrounding part of the enzyme, since the substrate cannot reach all the enzyme even when small fragments of the cell wall are used without disintegration. (4) On the basis of the data obtained, some tentative approximations are made of the ratio of ACh released to Na ions entering the squid giant axon per cm² per impulse.     

Potassium fluxes in dialyzed squid axons

Measurements have been made of K influx in squid giant axons under internal solute control by dialysis. With [ATP]_i = 1 µM, [Na]_i = 0, K influx was 6 ± 0.6 pmole/cm² sec; an increase to [ATP]_i = 4 mM gave an influx of 8 ± 0.5 pmole/cm² sec, while [ATP]_i 4, [Na]_i 80 gave a K influx of 19 ± 0.7 pmole/cm² sec (all measurements at ∼16°C). Strophanthidin (10 µM) in seawater quantitatively abolished the ATP-dependent increase in K influx. The concentration dependence of ATP-dependent K influx on [ATP]_i, [Na]_i, and [K]_o was measured; an [ATP]_i of 30 µM gave a K influx about half that at physiological concentrations (2–3 mM). About 7 mM [Na]_i yielded half the K influx found at 80 mM [Na]_i. The ATP-dependent K influx responded linearly to [K]_o from 1–20 mM and was independent of whether Na, Li, or choline was the principal cation of seawater. Substances tested as possible energy sources for the K pump were acetyl phosphate, phosphoarginine, PEP, and d-ATP. None was effective except d-ATP and this substance gave 70% of the maximal flux only when phosphoarginine or PEP was also present.     

Concentrative accumulation of choline by human erythrocytes

Influx and efflux of choline in human erythrocytes were studied using ¹⁴C-choline. When incubated at 37°C with physiological concentrations of choline erythrocytes concentrate choline; the steady-state ratio is 2.08 ± 0.23 when the external choline is 2.5 µM and falls to 0.94 ± 0.13 as the external concentration is raised to 50 µM. During the steady state the influx of choline is consistent with a carrier system with an apparent Michaelis constant of 30 x 10^-6 and a maximum flux of 1.1 µmoles per liter cells per min. For the influx into cells preequilibrated with a choline-free buffer the apparent Michaelis constant is about 6.5 x 10^-6 M and the maximum flux is 0.22 µmole per liter cells per min. At intracellular concentrations below 50 µmole per liter cells the efflux in the steady state approximates first order kinetics; however, it is not flux through a leak because it is inhibited by hemicholinium. Influx and efflux show a pronounced exchange flux phenomenon. The ability to concentrate choline is lost when external sodium is replaced by lithium or potassium. However, the uphill movement of choline is probably not coupled directly to the Na⁺ electrochemical gradient.     

Kinetic analyses of calcium movements in cell cultures. 3. Effects of calcium and parathyroid hormone in kidney cells

Calcium compartments and fluxes were measured by kinetic analyses in kidney cell suspensions in a three-compartment closed system. The fast phase influx and compartment size increase linearly with the medium calcium and the half-time of exchange is only 1.3 min which suggests that the fast component is extracellular. The slow phase compartment rises linearly from 0.1 to 0.5 mmole calcium/kg cell water when the medium calcium is raised from 0.02 to 2.5 mM. The slow phase calcium influx exhibits the pattern of saturation kinetics with a V _max of 0.065 µµmole cm^-2 sec^-1 and a K_m of 0.3 mM indicating that it is a carrier-mediated transport process. PTH has no effect on the fast phase of calcium influx, but increases both calcium influx and the calcium pool size of the slow component. The maximum effect is obtained at medium calcium concentration of 1.3 mM. Below 0.3 mM extracellular calcium, the effects of the hormone cannot be demonstrated. PTH increases the V _max of calcium influx from 0.065 to 0.128 µµmole cm^-2 sec^-1 while the K_m rises from 0.3 to 1.15 mM. These findings suggest that PTH increases the translocation of the calcium-carrier complex across the membrane and not the carrier concentration or its binding affinity for calcium.     

High-resolution radioautography of phlorizin-3H in rings of hamster intestine

Quantitative light microscope radioautographs of galactose-³H and phlorizin-³H were prepared from freeze-dried plastic-embedded hamster small intestine incubated in vitro. The usual uphill epithelial cell accumulation of galactose accompanied by a somewhat smaller lamina propria accumulation was observed in control tissue incubated 3 min in 1 mM galactose-³H. The addition of 5 x 10^-4 M phlorizin to the medium blocked uphill accumulation, but did not prevent galactose equilibration with the epithelial cells. The galactose content of the lamina propria was considerably less than the galactose content of the epithelial cell. Varying the phlorizin-³H content of the medium from 0.6 to 60 µM revealed a brush border binding of phlorizin which followed a Langmuir adsorption isotherm with a half-saturation constant of 13 µM and a maximum binding of 84 µmoles of phlorizin/liter of microvilli or 2.6 x 10⁶ sites/epithelial cell. The phlorizin content of the epithelial cell compartment, excluding microvilli, never exceeded 10% that of the medium after 20 min of incubation. These findings directly support the view that phlorizin is a nontransported inhibitor which binds glucose-galactose carriers at the surface of epithelial cell microvilli.     

Sodium fluxes in internally dialyzed squid axons

The effects which alterations in the concentrations of internal sodium and high energy phosphate compounds had on the sodium influx and efflux of internally dialyzed squid axons were examined. Nine naturally occurring high energy phosphate compounds were ineffective in supporting significant sodium extrusion. These compounds were: AcP, PEP, G-3-P, ADP, AMP, GTP, CTP, PA, and UTP.¹ the compound d-ATP supported 25–50% of the normal sodium extrusion, while ATP supported 80–100%. The relation between internal ATP and sodium efflux was nonlinear, rising most steeply in the range 1 to 10 µM and more gradually in the range 10 to 10,000 µM. There was no evidence of saturation of efflux even at internal ATP concentrations of 10,000 µM. The relation between internal sodium and sodium efflux was linear in the range 2 to 240 mM. The presence of external strophanthidin (10 µM) changed the sodium efflux to about 8–12 pmoles/cm² sec regardless of the initial level of efflux; this changed level was not altered by subsequent dialysis with large concentrations of ATP. Sodium influx was reduced about 50 % by removal of either ATP or Na and about 70 % by removing both ATP and Na from inside the axon.     

The Site of Calcium Binding in Relation to the Activation of Myofibrillar Contraction

Skeletal muscle myofibrils, in the presence of 2 mM MgCl₂ at pH 7.0, were found to have two classes of calcium-binding sites with apparent affinity constants of 2.1 x 10⁶ M ^-1 (class 1) and ∼3 x 10⁴ M ^-1 (class 2), respectively. At free calcium concentrations essential for the activation of myofibrillar contraction (∼10^-6 M) there would be significant calcium binding only to the class 1 sites. These sites could bind about 1.3 µmoles of calcium per g protein. Extraction of myosin from the myofibrils did not alter their calcium-binding parameters. Myosin A, under identical experimental conditions, had little affinity for calcium. The class 1 sites are, therefore, presumed to be located in the I filaments. The class 1 sites could only be detected in F actin and myosin B preparations which were contaminated with the tropomyosin-troponin complex. Tropomyosin bound very little calcium. Troponin, which in conjunction with tropomyosin confers calcium sensitivity on actomyosin systems, could bind 22 µmoles of calcium per g protein with an apparent affinity constant of 2.4 x 10⁶ M ^-1. In view of the identical affinity constants of the myofibrils and troponin and the much greater number of calcium-binding sites on troponin it is suggested that calcium activates myofibrillar contraction by binding to the troponin molecule.     

Effects of acriflavine on the mitochondria and kinetoplast of Crithidia fasciculata. Correlation of fine structure changes with decreased mitochondrial enzyme activity

The effects of acriflavine on the fine structure and function of the mitochondria and the kinetoplast in Crithidia fasciculata have been investigated. A mitochondrial fraction was prepared by differential centrifugation of cells broken by grinding with neutral alumina. Isolated mitochondria or intact cells revealed by spectrophotometric measurements the presence of cytochromes a + a ₃, b, c ₅₅₅ and o. After cells were grown in acriflavine for 3–4 days, the fine structure of the mitochondria and their cytochrome content were affected. Cells grown in 5.0 µM acriflavine had a threefold decrease in cytochrome a + a ₃ and decreased respiratory activity. The mitochondrial preparation from these cells had a fivefold decrease in cytochrome a + a ₃ and a less but significant decrease of other cytochromes present. There was also a decrease in the mitochondrial enzyme activities of NADH, succinic and L-α-glycerophosphate oxidases, and succinic and L-α-glycerophosphate dehydrogenases. Dyskinetoplastic cells could be demonstrated after growth in 1.0 µM acriflavine. At 5 µM, 80–90% of the cells were dyskinetoplastic. The kinetoplastic DNA was condensed, nonfibrillar, and did not incorporate thymidine-³H. The mitochondria in these cells had few cristae and were shorter and more swollen than the controls. Acriflavine may induce the fine structure effects we have observed and may affect the formation of the mitochondria in C. fasciculata.     

Ca 2+ -specific removal of Z lines from rabbit skeletal muscle

Removal of rabbit psoas strips immediately after death and incubation in a saline solution containing 1 mM Ca²⁺ and 5 nM Mg²⁺ for 9 hr at 37°C and pH 7.1 causes complete Z-line removal but has no ultrastructurally detectable effect on other parts of the myofibril. Z lines remain ultrastructurally intact if 1 mM 1,2-bis-(2-dicarboxymethylaminoethoxy)-ethane (EGTA) is substituted for 1 mM Ca²⁺ and the other conditions remain unchanged. Z lines are broadened and amorphous but are still present after incubation for 9 hr at 37°C if 1 mM ethylenediaminetetraacetate (EDTA) is substituted for 1 mM Ca²⁺ and 5 mM Mg²⁺ in the saline solution. A protein fraction that causes Z-line removal from myofibrils in the presence of Ca²⁺ at pH 7.0 can be isolated by extraction of ground muscle with 4 mM EDTA at pH 7.0–7.6 followed by isoelectric precipitation and fractionation between 0 and 40% ammonium sulfate saturation. Z-line removal by this protein fraction requires Ca²⁺ levels higher than 0.1 mM, but Z lines are removed without causing any other ultrastructurally detectable degradation of the myofibril. This is the first report of a protein endogenous to muscle that is able to catalyze degradation of the myofibril. The very low level of unbound Ca²⁺ in muscle cells in vivo may regulate activity of this protein fraction, or alternatively, this protein fraction may be localized in lysosomes.     

The penetration of sodium into the epithelium of the frog skin

The aim of this paper is twofold. First, to describe a method for the measurement of the unidirectional flux of Na from the outer bathing solution into epithelium (J_OT), and second, to describe the use of this method under a variety of experimental conditions in order to obtain some insight into the nature of this flux. The method developed is based on the exposure of a frog skin to a Ringer solution containing ²²Na. The exposure is made so that neighboring points along the surface remain in contact with the ²²Na solution for gradually longer periods, ranging from 0 to 46 sec. Some 8 to 10 samples of the exposed part are used to obtain the time course of the uptake of ²²Na and this time course is used, in turn, to evaluate J_OT. This flux is then studied in skins mounted between two identical Ringer solutions with 115 mM Na (11.25 ± 0.10 [18] µmole·hr^-2 cm^-2), and in skins mounted with Ringer with 1 mM Na on the outside and 115 mM Na on the inside (0.43 ± 0.05 [18] µmole·hr^-1·cm^-2. From the observations that the flux is much larger than the net Na flux across the whole skin, that it is inhibited by K⁺, and is unaffected by ouabain, it is concluded that the penetration of Na⁺ into the epithelium does not occur by simple diffusion and is not directly dependent on an ouabain-sensitive mechanism. In the course of these experiments it was observed that when the skin was crushed between two chambers the uptake of Na in the neighboring exposed areas was decreased.     

Choline permeability in cardiac muscle cells of the cat

Permeability of the cardiac cell membrane to choline ions was estimated by measuring radioactive choline influx and efflux in cat ventricular muscle. Maximum values for choline influx in 3.5 and 137 mM choline were respectively 0.56 and 9 pmoles/cm²·sec. In 3.5 mM choline the intracellular choline concentration was raised more than five times above the extracellular concentration after 2 hr of incubation. In 137 mM choline, choline influx corresponded to the combined loss of intracellular Na and K ions. Paper chromatography of muscle extracts indicated that choline was not metabolized to any important degree. The accumulation of intracellular choline rules out the existence of an efficient active pumping mechanism. By measuring simultaneously choline and sucrose exchange, choline efflux was analyzed in an extracellular phase, followed by two intracellular phases: a rapid and a slow one. Efflux corresponding to the rapid phase was estimated at 16–45 pmoles/cm²·sec in 137 mM choline and at 1.3–3.5 pmoles/cm²·sec in 3.5 mM choline; efflux in 3.5 mM choline was proportional to the intracellular choline concentration. The absolute figures for unidirectional efflux were much larger than the net influx values. The data are compared to Na and Li exchange in heart cells. Possible mechanisms for explaining the choline behavior in heart muscle are discussed.     

Kinetic analyses of calcium movements in HeLa cell cultures. I. Calcium influx

Calcium influx was studied in monolayers of HeLa cells to determine the number of exchangeable and nonexchangeable pools and the rate constant of the different fluxes. Of the two exchangeable pools, one has a very fast rate of exchange with a half-time of 1.54 min, a compartment size of 1.06 mµmoles/mg cell protein, and an exchange rate of 474 µµmoles/(mg protein\·min). This compartment is likely to be extracellular and could represent calcium exchange between the extracellular fluids and surface binding sites of the cell membrane. The second exchangeable pool has a half-time of exchange of 31 min, a compartment size of 2.69 mµmoles/mg cell protein (0.224 millimole calcium/kg cell water), and a flux rate of 0.0546 µµmole cm^-2 sec^-1. This compartment can be considered to be the intracellular pool of exchangeable calcium. An unexchangeable intracellular pool of calcium of 3.05 mµmoles/mg cell protein was detected implying that only 45% of the intracellular calcium is exchangeable. In addition, a large extracellular pool of calcium has been found to be unexchangeable, probably a part of the cell glycocalix. Finally, dinitrophenol 10^-3 M does not affect the slow component of the calcium uptake curve which brings new evidence that calcium entry into the cell is not a metabolically dependent process.     

Transport of glucose and galactose in kidney-cortex cells

1. The aerobic transport of d-glucose and d-galactose in rabbit kidney tissue at 25° was studied. 2. In slices forming glucose from added substrates an accumulation of glucose against its concentration gradient was found. The apparent ratio of intracellular ([S]_i) and extracellular ([S]_o) glucose concentrations was increased by 0·4mm-phlorrhizin and 0·3mm-ouabain. 3. Slices and isolated renal tubules actively accumulated glucose from the saline; the apparent [S]_i/[S]_o fell below 1·0 only at [S]_o higher than 0·5mm. 4. The rate of glucose oxidation by slices was characterized by the following parameters: K_m 1·16mm; V_max. 4·5μmoles/g. wet wt./hr. 5. The active accumulation of glucose from the saline was decreased by 0·1mm-2,4-dinitrophenol, 0·4mm-phlorrhizin and by the absence of external Na⁺. 6. The kinetic parameters of galactose entry into the cells were: K_m 1·5mm; V_max 10μmoles/g. wet wt./hr. 7. The efflux kinetics from slices indicated two intracellular compartments for d-galactose. The galactose efflux was greatly diminished at 0°, was inhibited by 0·4mm-phlorrhizin, but was insensitive to ouabain. 8. The following mechanism of glucose and galactose transport in renal tubular cells is suggested: (a) at the tubular membrane, these sugars are actively transported into the cells by a metabolically- and Na⁺-dependent phlorrhizin-sensitive mechanism; (b) at the basal cell membrane, these sugars are transported in accordance with their concentration gradient by a phlorrhizin-sensitive Na⁺-independent facilitated diffusion. The steady-state intracellular sugar concentration is determined by the kinetic parameters of active entry, passive outflow and intracellular utilization.     

Cation regulation in the smooth muscle of frog stomach

Cation composition of frog smooth muscle cells was investigated. Fresh stomach muscle rings resembled skeletal muscle, but marked Na gain and K loss followed immersion. Mean Na (49.8–79.7 mM/kg tissue) and K (61.8–80.1 mM/kg tissue) varied between batches, but were stable for long periods in vitro. Exchange of 6–30 mM Na/kg tissue with ²²Na was extremely slow and distinct. Extracellular water was estimated from sucrose-¹⁴C uptake. Calculated exchangeable intracellular Na was 9 mM/kg cell water, and varied little. Thus steady-state transmembrane cation gradients appeared to be steep. K-free solution had only slight effects. Ouabain (10^-4 M) caused marked Na gain and reciprocal K loss; at 30°C, Na and K varied linearly with time over a wide range of contents, indicating constant net fluxes. Net fluxes decreased with temperature decrease. ²²Na exchange in ouabain-treated tissue at 20–30°C was rapid and difficult to analyze. The best minimum estimates of unidirectional Na fluxes at 30°C were 10–12 times the constant net flux; constant pump efflux may explain these findings. The rapidity of Na exchange may not reflect very high permeability, but it does require a high rate of transport work.     

Caffeine and excitation-contraction coupling in the guinea pig taenia coli

The effects of caffeine (0.2–10 mM) on the electrical and mechanical activities of guinea pig taenia coli were investigated with the double sucrose-gap method. Caffeine evoked a small tension with a latency of 20–30 sec, then phasic contraction developed and finally relaxation. The initial tension development also appeared in the Na-free solution without any marked changes in the membrane potential and membrane resistance. The phasic contraction disappeared in the Na-free solution. The relaxation in the presence of caffeine was accompanied by depolarization block of the spike generation. The minimum concentration of Ca ion needed to evoke the tension development by the caffeine was 10^-7 M. Caffeine also potentiated the twitch tension below a concentration of 5 mM either in the Na-free solution or at low temperature (5°C). NO₃ ^- and Br^- showed a similar response to caffeine on the potentiation of the twitch tension at low temperature.     

Calcium efflux from frog twich muscle fibers

An apparatus is described which collects the effluent from the center 0.7 cm of a single muscle fiber or bundle of muscle fibers. It was used to study the efflux of ⁴⁵Ca from twitch muscle fibers. The efflux can be described by three time constants 18 ± 2 min, 300 ± 40 min, and 882 ± 172 min. These kinetics have been interpreted as those of a three-compartment system. The fastest is thought to be on the surface membrane of the muscle and of the T system. It contains 0.07 ± 0.03 mM Ca/liter of fiber and the Ca efflux is 0.11 ± 0.04 pM Ca/cm². sec. The intermediate rate compartment is thought to represent the Ca in the longitudinal reticulum. It contains approximately 0.77 mM Ca/liter. Only the efflux from this compartment increases during stimulation. The most slowly exchanging compartment is poorly defined. Neither Ca-free nor Ni-Ringer solutions alter the rate of loss from the fastest exchanging compartment. Ni apparently alters the rate of loss from the slowest compartment.     

Specific uncoupling of excitation and contraction in mammalian cardiac tissue by lanthanum

Arterially cannulated rabbit interventricular septal tissue was exposed to 5–40 µM La in 2.5 mM Ca perfusate. Immediately following perfusion with La two concurrent events were consistently observed: (a) a rapid decline of active tension to a lesser steady-state value, and (b) an abrupt, release of short duration of tissue-bound Ca. The magnitude of both events was directly related to the [La]_o. If the duration of exposure to La was brief, contractility returned toward normal upon return to the La-free perfusate. Elevation of [Ca]_o during exposure to La counteracted its effect and induced a concurrent displacement of tissue-bound La. Cellular action potentials recorded during brief perfusion with La demonstrated that essentially normal regenerative depolarization was maintained. Analysis of the quantities of ⁴⁵Ca released following exposure to 10 µM La indicated that this La-susceptible Ca was being displaced from a homogeneous pool—the one previously shown by Langer to represent contractile dependent Ca. These data led to the following conclusions: During perfusion with 2.5 mM Ca contractile dependent Ca was derived primarily from "superficially" located sites. La effected the release of contractile dependent Ca by modifying the normal permselectivity of this "superficial" membrane for activator Ca. These and other data infer that contractile dependent Ca is derived primarily from superficially located sites.     

Sodium flux in the smooth muscle of frog stomach

Sodium efflux from rings of frog stomach muscle was measured at 5° and 15°C in three different steady states. After incubation in normal, K-free, or ouabain (10^-4 M) solutions, intracellular cations stabilized at markedly differing levels. At 5°C, inhibition of Na extrusion was shown in the rate coefficients for ²²Na efflux, which were slightly smaller in K-free than in normal solutions, and much smaller in ouabain. Due to the intracellular Na concentration differences, total Na efflux was similar in K-free and ouabain solutions, and only ⅕ as large in normal solution. At 15°C, normal total Na flux was only 1/7;–1/10 inhibitors, and may be underestimated. The total flux differences may involve dependence of the Na pump and Na permeation on internal Na concentration. The Q ₁₀ of the steady-state fluxes was 3.7 in ouabain, 2.8 in K-free solution, and 1.9 in normal solution. The high temperature dependence of influx as well as efflux suggests transport mechanisms other than simple diffusion. Sodium turnover in the cell water was 46–66 mM/hr in inhibitors at 15°C, and a high rate of Na extrusion in normal muscle is suggested. However, cell volume:surface ratio is only 1.6 µ and all estimates of Na flux were under 3 pmoles/cm² per sec, indicating low Na permeability.