Properties of the vertebrate skeletal muscle tubular system as a sealed compartment

Confocal imaging of impermeant fluorescent dyes trapped in the tubular (t-) system of skeletal muscle fibres of rat and cane toad was used to examine changes in the morphology of the t-system upon mechanical skinning, the time course of dye loss from the sealed t-system in mechanically skinned fibres and the influence of rapid application and removal of glycerol on the morphology of the sealed t-system. In contrast to intact fibres, which have a t-system open to the outside, the sealed t-system of toad mechanically skinned fibres consistently displayed local swellings (vesicles). The occurrence of vesicles in the sealed t-system of rat-skinned fibres was infrequent. Application and removal of 200-400 mM glycerol to the sealed t-system did not produce any obvious changes in its morphology. The dyes fluo-3, fura-2 and Oregon green 488 were lost from the sealed t-system of toad fibres at different rates suggesting that the mechanism of organic anion transport across the tubular wall was not by indiscriminate bulk transport. The rate of fluo-3 and fura-2 loss from the sealed t-system of rat fibres was greater in rat than in toad fibres and could be explained by differences in surface area: volume ratio of the t-system in the two fibre types. Based on the results presented here and on other results from this laboratory, an explanation is given for the formation of numerous vesicles in toad-skinned fibres and lack of vesicle formation in rat-skinned fibres. This explanation can also help with better understanding the mechanism responsible for vacuole formation in intact fibres.     

Comparison of simulated and measured calcium sparks in intact skeletal muscle fibers of the frog

Calcium sparks in frog intact skeletal muscle fibers were modeled as stereotypical events that arise from a constant efflux of Ca(2+) from a point source for a fixed period of time (e.g., 2.5 pA of Ca(2+) current for 4.6 ms; 18 degrees C). The model calculates the local changes in the concentrations of free Ca(2+) and of Ca(2+) bound to the major intrinsic myoplasmic Ca(2+) buffers (troponin, ATP, parvalbumin, and the SR Ca(2+) pump) and to the Ca(2+) indicator (fluo-3). A distinctive feature of the model is the inclusion of a binding reaction between fluo-3 and myoplasmic proteins, a process that strongly affects fluo-3's Ca(2+)-reaction kinetics, its apparent diffusion constant, and hence the morphology of sparks. DeltaF/F (the change in fluo-3's fluorescence divided by its resting fluorescence) was estimated from the calculated changes in fluo-3 convolved with the microscope point-spread function. To facilitate comparisons with measured sparks, noise and other sources of variability were included in a random repetitive fashion to generate a large number of simulated sparks that could be analyzed in the same way as the measured sparks. In the initial simulations, the binding of Ca(2+) to the two regulatory sites on troponin was assumed to follow identical and independent binding reactions. These simulations failed to accurately predict the falling phase of the measured sparks. A second set of simulations, which incorporated the idea of positive cooperativity in the binding of Ca(2+) to troponin, produced reasonable agreement with the measurements. Under the assumption that the single channel Ca(2+) current of a ryanodine receptor (RYR) is 0.5-2 pA, the results suggest that 1-5 active RYRs generate an average Ca(2+) spark in a frog intact muscle fiber.     

Resting myoplasmic free calcium in frog skeletal muscle fibers estimated with fluo-3.

Fluo-3 is an unusual tetracarboxylate Ca2+ indicator. For recent lots supplied by Molecular Probes Inc. (Eugene, OR), FMAX, the fluorescence intensity of the indicator in its Ca(2+)-bound form, is approximately 200 times that of FMIN, the fluorescence intensity of the indicator in its Ca(2+)-free form. (For earlier lots, impurities may account for the smaller reported values of FMAX/FMIN, 36-40). We have injected fluo-3 from a high-purity lot into intact single fibers from frog muscle and measured the indicator's absorbance and fluorescence signals at rest (A and F, respectively) and changes in absorbance and fluorescence following action potential stimulation (delta A and delta F signals substantially lagged behind that of the myoplasmic free Ca2+ transient. Our analysis of fluo-3's signals from myoplasm therefore focused on information about the level of resting myoplasmic free [Ca2+] ([Ca2+]r). From A, delta A, and in vitro estimates of fluo-3's molar extinction coefficients, the change in the fraction of fluo-3 in the Ca(2+)-bound form during activity (delta f) was estimated. From delta f, delta F, and F, the fraction of the indicator in the Ca(2+)-bound form in the resting fiber (fr) was estimated by fr = (delta f x F/delta F) + (1-FMAX/FMIN)-1. Since FMAX/FMIN is large, the contribution of the second term to the estimate of fr is small. At 16 degrees C, the mean value (mean +/- S.E.) of fr was 0.086 +/- 0.004 (N = 15). From two estimates of the apparent dissociation constant of fluo-3 for Ca2+ in the myoplasm, 1.09 and 2.57 microM, the average value of [Ca2+]r is calculated to be 0.10 and 0.24 microM, respectively. The smaller of these estimates lies near the upper end of the range of values for [Ca2+]r in frog fibers (0.02-0.12 microM) estimated by others with aequorin and Ca(2+)-selective electrodes. The larger of the estimates lies within the range of values (0.2-0.3 microM) previously estimated in this laboratory with fura red. We conclude that [Ca2+]r in frog fibers is at least 0.1 microM and possibly as large as 0.3 microM.     

Numerical analysis of Ca2+ signaling in rat ventricular myocytes with realistic transverse-axial tubular geometry and inhibited sarcoplasmic reticulum

The t-tubules of mammalian ventricular myocytes are invaginations of the cell membrane that occur at each Z-line. These invaginations branch within the cell to form a complex network that allows rapid propagation of the electrical signal, and hence synchronous rise of intracellular calcium (Ca(2+)). To investigate how the t-tubule microanatomy and the distribution of membrane Ca(2+) flux affect cardiac excitation-contraction coupling we developed a 3-D continuum model of Ca(2+) signaling, buffering and diffusion in rat ventricular myocytes. The transverse-axial t-tubule geometry was derived from light microscopy structural data. To solve the nonlinear reaction-diffusion system we extended SMOL software tool (http://mccammon.ucsd.edu/smol/). The analysis suggests that the quantitative understanding of the Ca(2+) signaling requires more accurate knowledge of the t-tubule ultra-structure and Ca(2+) flux distribution along the sarcolemma. The results reveal the important role for mobile and stationary Ca(2+) buffers, including the Ca(2+) indicator dye. In agreement with experiment, in the presence of fluorescence dye and inhibited sarcoplasmic reticulum, the lack of detectible differences in the depolarization-evoked Ca(2+) transients was found when the Ca(2+) flux was heterogeneously distributed along the sarcolemma. In the absence of fluorescence dye, strongly non-uniform Ca(2+) signals are predicted. Even at modest elevation of Ca(2+), reached during Ca(2+) influx, large and steep Ca(2+) gradients are found in the narrow sub-sarcolemmal space. The model predicts that the branched t-tubule structure and changes in the normal Ca(2+) flux density along the cell membrane support initiation and propagation of Ca(2+) waves in rat myocytes.     

Effect of osmolality on the initiation of sperm motility in Xenopus laevis

1. Seminal plasma of the South African clawed toad Xenopus laevis exhibited osmolality around 250 mosmol/kg isotonic to blood plasma. 2. Spermatozoa remained immotile when the semen was diluted in solutions of 100 mM NaCl, 100 mM KCl or 200 mM glucose containing 20 mM Hepes-NaOH buffer which exhibited almost the same osmolalities (approximately 240 mosmol/kg) as seminal plasma. 3. The spermatozoa became motile in these three solutions if the osmolalities were decreased. 4. These suggest that motility of Xenopus sperm is suppressed by seminal osmolality in the reproductive organ and initiated by a decrease of osmolality when they are spawned into hypotonic fresh water.     

Efflux of potassium (86Rb+) attenuates the volume-restorative effect of sodium-amino acid cotransport in rat renal inner medullary cells shrunken by exposure to hyperosmotic media.

When the osmolality of the bathing medium was increased from 710 to 2000 mosmol/kg H2O, cells in incubated slices of rat renal inner medulla lost water and K+, and the rate of efflux of preloaded 86Rb+ (a tracer for K+) was significantly depressed. Addition of 2-aminoisobutyric acid (AIB, 10 mmol/l) partly restored cell water content but without re-accumulation of K+; the rate of 86Rb+ efflux was greatly increased. The presence of Ba2+ (1 mmol/l) or trifluoperazine (50 mumol/l) led to complete recovery of cell volume and K+ contents, with markedly reduced efflux of 86Rb+. Neither additive had any significant effect upon these variables in the absence of AIB or in media of 710 mosmol/kg. Efflux of 86Rb+ was pH-sensitive within the physiological range, and was depressed when external AIB was reduced below approx. 5 mmol/l. When external Na+ was increased from 145 to 500 mmol/l (total osmolality 350 to 2500 mosmol/kg) efflux was retarded only slightly if AIB was present, but markedly if AIB was omitted. Inner medullary cells may contain a class of Ba(2+)-inhibitable, calmodulin-dependent K+ conductive pathway which is activated in strongly hyperosmotic media by the operation of an inwardly-directed Na(+)-amino acid symport (cf. Law, R.O. (1988) Pflügers Arch. 413, 43-50) and which serves to moderate the volume-restorative effect of this membrane mechanism.     

Different patterns of cell volume regulation in hyposmotic media between attached and suspended HeLa cells.

Both attached and suspended HeLa cells swelled in a medium of a hypotonic osmolality of 235 mosmol/kg H2O. When the osmolality was further decreased to 166 mosmol/kg H2O, attached cells instantly swelled and then rapidly lost water and K+, followed by slow gains of them. Suspended cells instantly swelled and then K+ loss and regulatory volume decrease (RVD) occurred. Neither 0.1 mM ouabain nor 10 mM TEA changed the water loss of attached cells, whereas ouabain inhibited RVD of suspended cells. Quinine (1 mM) inhibited water losses from both cells and comparison of the losses implies stronger activation of K+ channel in attached cells than in suspended cells. Omission of medium Ca2+ or addition of 10 mM BaCl2 inhibited RVD in part. These results suggest that hyposmotic stress induces net water loss from attached cells, associated with K+ release through the Ca(2+)-dependent K+ channel. Suspended cells osmotically swell, followed by RVD with K+ and Na+ releases through the K+ channel and Na(+)-pump, respectively. The different patterns of volume changes may relate to the difference of activity or time of activation of the K+ channel between both cells.     

Calcium release domains in mammalian skeletal muscle studied with two-photon imaging and spot detection techniques

The spatiotemporal characteristics of the Ca(2+) release process in mouse skeletal muscle were investigated in enzymatically dissociated fibers from flexor digitorum brevis (FDB) muscles, using a custom-made two-photon microscope with laser scanning imaging (TPLSM) and spot detection capabilities. A two-microelectrode configuration was used to electrically stimulate the muscle fibers, to record action potentials (APs), and to control their myoplasmic composition. We used 125 muM of the low-affinity Ca(2+) indicator Oregon green 488 BAPTA-5N (OGB-5N), and 5 or 10 mM of the Ca(2+) chelator EGTA (pCa 7) in order to arrest fiber contraction and to constrain changes in the [Ca(2+)] close to the release sites. Image and spot data showed that the resting distribution of OGB-5N fluorescence was homogeneous along the fiber, except for narrow peaks ( approximately 23% above the bulk fluorescence) centered at the Z-lines, as evidenced by their nonoverlapping localization with respect to di-8-ANEPPS staining of the transverse tubules (T-tubules). Using spot detection, localized Ca(2+) transients evoked by AP stimulation were recorded from adjacent longitudinal positions 100 nm apart. The largest and fastest DeltaF/F transients were detected at sites flanking the Z-lines and colocalized with T-tubules; the smallest and slowest were detected at the M-line, whereas transients at the Z-line showed intermediate features. Three-dimensional reconstructions demonstrate the creation of two AP-evoked Ca(2+) release domains per sarcomere, which flank the Z-line and colocalize with T-tubules. In the presence of 10 mM intracellular EGTA, these domains are formed in approximately 1.4 ms and dissipate within approximately 4 ms, after the peak of the AP. Their full-width at half-maximum (FWHM), measured at the time that Ca(2+) transients peaked at T-tubule locations, was 0.62 mum, similar to the 0.61 mum measured for di-8-ANEPPS profiles. Both these values exceed the limit of resolution of the optical system, but their similarity suggests that at high [EGTA] the Ca(2+) domains in adult mammalian muscle fibers are confined to Ca(2+) release sites located at the junctional sarcoplasmic reticulum (SR).     

Effect of medium osmolality on the growth of murine continuous marrow cultures

The effect of medium osmolality was examined in primary, continuous bone-marrow cultures established from TO strain mice. The non-adherent cell population increased exponentially between weeks 2 and 5 and thereafter declined steadily. The number of CFU-GM followed a similar pattern but showed greater variability. The optimum osmolality in 4 week old cultures was found to be about 345 mosmol/kg which was higher than the plasma osmolality (n = 20; mean = 323.3 mosmol/kg; range = 313-331). Maximum non-adherent cell numbers were found at about 345 mosmol/kg (better than half-maximum between 320 and 370 mosmol/kg). CFU-GM numbers in the culture supernatant were maximal at about 355 mosmol/kg (better than half-maximum between 320 and 400 mosmol/kg). An adherent layer developed over a wider range of osmolality than supported granulopoiesis (better than half-maximum between 258 and 402 mosmol/kg). It was necessary to increase the osmolality of Fischer's medium in order to obtain maximum growth.     

Effects of high myoplasmic L-lactate concentration on E-C coupling in mammalian skeletal muscle.

The effects of high myoplasmic L-lactate concentrations (20-40 mM) at constant pH (7.1) were investigated on contractile protein function, voltage-dependent Ca(2+) release, and passive Ca(2+) leak from the sarcoplasmic reticulum (SR) in mechanically skinned fast-twitch (extensor digitorum longus; EDL) and slow-twitch (soleus) fibers of the rat. L-Lactate (20 mM) significantly reduced maximum Ca(2+)-activated force by 4 +/- 0.5% (n = 5, P < 0.05) and 5 +/- 0.4% (n = 6, P < 0.05) for EDL and soleus, respectively. The Ca(2+) sensitivity was also significantly decreased by 0.06 +/- 0. 002 (n = 5, P < 0.05) and 0.13 +/- 0.01 (n = 6, P < 0.001) pCa units, respectively. Exposure to L-lactate (20 mM) for 30 s reduced depolarization-induced force responses by ChCl substitution by 7 +/- 3% (n = 17, P < 0.05). This inhibition was not obviously affected by the presence of the lactate transport blocker quercetin (10 microM), or the chloride channel blocker anthracene-9-carboxylic acid (100 microM). L-Lactate (20 mM) increased passive Ca(2+) leak from the SR in EDL fibers (the integral of the response to caffeine was reduced by 16 +/- 5%, n = 9, P < 0.05) with no apparent effect in soleus fibers (100 +/- 2%, n = 3). These results indicate that the L-lactate ion per se has negligible effects on either voltage-dependent Ca(2+) release or SR Ca(2+) handling and exerts only a modest inhibitory effect on muscle contractility at the level of the contractile proteins.     

Effect of Medium Osmolality On the Growth of Murine Continuous Marrow Cultures

The effect of medium osmolality was examined in primary, continuous bone-marrow cultures established from to strain mice. the non-adherent cell population increased exponentially between weeks 2 and 5 and thereafter declined steadily. the number of CFU-GM followed a similar pattern but showed greater variability. the optimum osmolality in 4 week old cultures was found to be about 345 mosmol/kg which was higher than the plasma osmolality (n= 20; mean = 323.3 mosmol/kg; range = 313–331). Maximum non-adherent cell numbers were found at about 345 mosmol/kg (better than half-maximum between 320 and 370 mosmol/kg). CFU-GM numbers in the culture supernatant were maximal at about 355 mosmol/kg (better than half-maximum between 320 and 400 mosmol/kg). an adherent layer developed over a wider range of osmolality than supported granulopoiesis (better than half-maximum between 258 and 402 mosmol/kg). It was necessary to increase the osmolality of Fischer's medium in order to obtain maximum growth.     

A comparative assessment of fluo Ca2+ indicators in rat ventricular myocytes

The fluo family of indicators is frequently used in studying Ca(2+) physiology; however, choosing which fluo indicator to use is not obvious. Indicator properties are typically determined in well-defined aqueous solutions. Inside cells, however, the properties can change markedly. We have characterized each of three fluo variants (fluo-2MA, fluo-3 and fluo-4) in two forms-the acetoxymethyl (AM) ester and the K(+) salt. We loaded indicators into rat ventricular myocytes and used confocal microscopy to monitor depolarization-induced fluorescence changes and fractional shortening. Myocytes loaded with the indicator AM esters showed significantly different Ca(2+) transients and fractional shortening kinetics. Loading the K(+) salts via whole-cell patch-pipette eliminated differences between fluo-3 and fluo-4, but not fluo-2MA. Cells loaded with different indicator AM esters showed different staining patterns-suggesting differential loading into organelles. Ca(2+) dissociation constants (K(d,Ca)), measured in protein-rich buffers mimicking the cytosol were significantly higher than values determined in simple buffers. This increase in K(d,Ca) (decrease in Ca(2+) affinity) was greatest for fluo-3 and fluo-4, and least for fluo-2MA. We conclude that the structurally-similar fluo variants differ with respect to cellular loading, subcellular compartmentalization, and intracellular Ca(2+) affinity. Therefore, judicious choice of fluo indicator and loading procedure is advisable when designing experiments.     

Simulation of calcium sparks in cut skeletal muscle fibers of the frog

Spark mass, the volume integral of Delta F/F, was investigated theoretically and with simulations. These studies show that the amount of Ca2+ bound to fluo-3 is proportional to mass times the total concentration of fluo-3 ([fluo-3T]); the proportionality constant depends on resting Ca2+ concentration ([Ca2+]R). In the simulation of a Ca2+ spark in an intact frog fiber with [fluo-3T] = 100 microM, fluo-3 captures approximately one-fourth of the Ca2+ released from the sarcoplasmic reticulum (SR). Since mass in cut fibers is several times that in intact fibers, both with similar values of [fluo-3T] and [Ca2+]R, it seems likely that SR Ca2+ release is larger in cut fiber sparks or that fluo-3 is able to capture a larger fraction of the released Ca2+ in cut fibers, perhaps because of reduced intrinsic Ca2+ buffering. Computer simulations were used to identify these and other factors that may underlie the differences in mass and other properties of sparks in intact and cut fibers. Our spark model, which successfully simulates calcium sparks in intact fibers, was modified to reflect the conditions of cut fiber measurements. The results show that, if the protein Ca2+-buffering power of myoplasm is the same as that in intact fibers, the Ca2+ source flux underlying a spark in cut fibers is 5-10 times that in intact fibers. Smaller source fluxes are required for less buffer. In the extreme case in which Ca2+ binding to troponin is zero, the source flux needs to be 3-5 times that in intact fibers. An increased Ca2+ source flux could arise from an increase in Ca2+ flux through one ryanodine receptor (RYR) or an increase in the number of active RYRs per spark, or both. These results indicate that the gating of RYRs, or their apparent single channel Ca2+ flux, is different in frog cut fibers--and, perhaps, in other disrupted preparations--than in intact fibers.     

A nicardipine-sensitive Ca2+ entry contributes to the hypotonicity-induced increase in [Ca2+]i of principal cells in rat cortical collecting duct

We examined the mechanisms involved in the [Ca(2+)](i) response to the extracellular hypotonicity in the principal cells of freshly isolated rat cortical collecting duct (CCD), using Fura-2/AM fluorescence imaging. Reduction of extracellular osmolality from 305 (control) to 195 mosmol/kgH(2)O (hypotonic) evoked transient increase in [Ca(2+)](i) of principal cells of rat CCDs. The [Ca(2+)](i) increase was markedly attenuated by the removal of extracellular Ca(2+)(.) The application of a P(2) purinoceptor antagonist, suramin failed to inhibit the hypotonicity-induced [Ca(2+)](i) increase. The [Ca(2+)](i) increase in response to extracellular hypotonicity was not influenced by application of Gd(3+) and ruthenium red. On the other hand, a voltage-gated Ca(2+) channel inhibitor, nicardipine, significantly reduced the peak amplitude of [Ca(2+)](i) increase in the principal cells. In order to assess Ca(2+) entry during the hypotonic stimulation, we measured the quenching of Fura-2 fluorescence intensity by Mn(2+). The hypotonic stimulation enhanced quenching of Fura-2 fluorescence by Mn(2+), indicating that a Ca(2+)-permeable pathway was activated by the hypotonicity. The hypotonicity-mediated enhancement of Mn(2+) quenching was significantly inhibited by nicardipine. These results strongly suggested that a nicardipine-sensitive Ca(2+) entry pathway would contribute to the mechanisms underlying the hypotonicity-induced [Ca(2+)](i) elevation of principal cells in rat CCD.     

An analysis of the relationships between subthreshold electrical properties and excitability in skeletal muscle

Skeletal muscle activation requires action potential (AP) initiation followed by its sarcolemmal propagation and tubular excitation to trigger Ca(2+) release and contraction. Recent studies demonstrate that ion channels underlying the resting membrane conductance (G(M)) of fast-twitch mammalian muscle fibers are highly regulated during muscle activity. Thus, onset of activity reduces G(M), whereas prolonged activity can markedly elevate G(M). Although these observations implicate G(M) regulation in control of muscle excitability, classical theoretical studies in un-myelinated axons predict little influence of G(M) on membrane excitability. However, surface membrane morphologies differ markedly between un-myelinated axons and muscle fibers, predominantly because of the tubular (t)-system of muscle fibers. This study develops a linear circuit model of mammalian muscle fiber and uses this to assess the role of subthreshold electrical properties, including G(M) changes during muscle activity, for AP initiation, AP propagation, and t-system excitation. Experimental observations of frequency-dependent length constant and membrane-phase properties in fast-twitch rat fibers could only be replicated by models that included t-system luminal resistances. Having quantified these resistances, the resulting models showed enhanced conduction velocity of passive current flow also implicating elevated AP propagation velocity. Furthermore, the resistances filter passive currents such that higher frequency current components would determine sarcolemma AP conduction velocity, whereas lower frequency components excite t-system APs. Because G(M) modulation affects only the low-frequency membrane impedance, the G(M) changes in active muscle would predominantly affect neuromuscular transmission and low-frequency t-system excitation while exerting little influence on the high-frequency process of sarcolemmal AP propagation. This physiological role of G(M) regulation was increased by high Cl(-) permeability, as in muscle endplate regions, and by increased extracellular [K(+)], as observed in working muscle. Thus, reduced G(M) at the onset of exercise would enhance t-system excitation and neuromuscular transmission, whereas elevated G(M) after sustained activity would inhibit these processes and thereby accentuate muscle fatigue.     

Partial inhibition of skeletal muscle contraction by dantrolene sodium and its modification with perchlorate and Bay K 8644.

The effects of dantrolene sodium (DAN) on the dihydropyridine receptor (DHPR) of the transverse (T) tubule voltage sensor (Ca2+ channel) was studied with single fibers from bullfrog toe muscle. Perchlorate (ClO4-), which acts selectively on the DHPR, overcame DAN-induced inhibition of twitch tension. Bay K 8644, a DHPR agonist, slowed the rate of twitch inhibition by DAN. DAN inhibited twitch tension to a greater extent in Ca(2+)-free solution than in Ringer solution or solution containing Zn2+, whereas twitch inhibition by DAN was less in caffeine-containing solution than in the control. The effects of DAN on Zn(2+)- and caffeine-treated fibers and on fibers in Ca(2+)-free solution suggest that DAN must act near the voltage sensor of the T tubule. However, differences in net twitch inhibition by DAN between control fibers and fibers potentiated by ClO4- or Bay K 8644 suggest that DAN does not bind to the same site as these potentiating agents do. The role of myoplasmic Ca2+ in DAN-induced inhibition of twitch and the effects of DAN on the mechanical threshold and membrane potential in skeletal muscle are discussed.     

Influence of plasma osmolality on baroreflex control of sympathetic activity

The purpose of this study was to determine if plasma osmolality alters baroreflex control of sympathetic activity when controlling for a change in intravascular volume; we hypothesized that baroreflex control of sympathetic activity would be greater during a hyperosmotic stimulus compared with an isoosmotic stimulus when intravascular volume expansion was matched. Seven healthy subjects (25 +/- 2 yr) completed two intravenous infusions: a hypertonic saline infusion (HSI; 3% NaCl) and, on a separate occasion, an isotonic saline infusion (ISO; 0.9% NaCl), both at a rate of 0.15 ml x kg(-1) x min(-1). To isolate the effect of osmolality, comparisons between HSI and ISO conditions were retrospectively matched based on hematocrit; therefore, baroreflex control of sympathetic outflow was determined at 20 min of a HSI and 40 min of an ISO. Muscle sympathetic outflow (MSNA) was directly measured using the technique of peroneal microneurography; osmolality and blood pressure (Finometer) were assessed. The baroreflex control of sympathetic outflow was estimated by calculating the slope of the relationship between MSNA and diastolic blood pressure during controlled breathing. Plasma osmolality was greater during the HSI compared with the ISO (HSI: 292 +/- 0.9 mosmol/kg and ISO: 289 +/- 0.8 mosmol/kg, P < 0.05). Hematocrits were matched (HSI: 39.1 +/- 1% and ISO: 39.1 +/- 1%, P > 0.40); thus, we were successful in isolating osmolality. The baroreflex control of sympathetic outflow was greater during the HSI compared with the ISO (HSI: -8.3 +/- 1.2 arbitrary units x beat(-1) x mmHg(-1) vs. ISO: -4.0 +/- 0.8 arbitrary units x beat(-1) x mmHg(-1), P = 0.01). In conclusion, when controlling for intravascular volume, increased plasma osmolality enhances baroreflex control of sympathetic activity in humans.     

Ca2+ ion transport through channels formed by α-hemolysin analyzed using a microwell array on a Si substrate

For the functional analysis of ion channel activity, an artificial lipid bilayer suspended over microwells was formed that ruptured giant unilamellar vesicles on a Si substrate. Ca(2+) ion indicators (fluo-4) were confined in the microwells by sealing the microwells with a lipid bilayer. An overhang formed at the microwells prevented the lipid membrane from falling into them and allowed the stable confinement of the fluorescent probes. The transport of Ca(2+) ions through the channels formed by α-hemolysin inserted in a lipid membrane was analyzed by employing the fluorescence intensity change of fluo-4 in the microwells. The microwell volume was very small (1-100 fl), so a highly sensitive monitor could be realized. The detection limit is several tens of ions/s/μm(2), and this is much smaller than the ion current in a standard electrophysiological measurement. Smaller microwells will make it possible to mimic a local ion concentration change in the cells, although the signal to noise ratio must be further improved for the functional analysis of a single channel. We demonstrated that a microwell array with confined fluorescent probes sealed by a lipid bilayer could constitute a basic component of a highly sensitive biosensor array that works with functional membrane proteins. This array will allow us to realize high throughput and parallel testing devices.     

Differential impact of mitochondrial positioning on mitochondrial Ca(2+) uptake and Ca(2+) spark suppression in skeletal muscle

Muscle contraction requires ATP and Ca(2+) and, thus, is under direct control of mitochondria and the sarcoplasmic reticulum. During postnatal skeletal muscle maturation, the mitochondrial network exhibits a shift from a longitudinal ("longitudinal mitochondria") to a mostly transversal orientation as a result of a progressive increase in mitochondrial association with Ca(2+) release units (CRUs) or triads ("triadic mitochondria"). To determine the physiological implications of this shift in mitochondrial disposition, we used confocal microscopy to monitor activity-dependent changes in myoplasmic (fluo 4) and mitochondrial (rhod 2) Ca(2+) in single flexor digitorum brevis (FDB) fibers from 1- to 4-mo-old mice. A robust and sustained Ca(2+) accumulation in triadic mitochondria was triggered by repetitive tetanic stimulation (500 ms, 100 Hz, every 2.5 s) in FDB fibers from 4-mo-old mice. Specifically, mitochondrial rhod 2 fluorescence increased 272 ± 39% after a single tetanus and 412 ± 45% after five tetani and decayed slowly over 10 min following the final tetanus. Similar results were observed in fibers expressing mitochondrial pericam, a mitochondrial-targeted ratiometric Ca(2+) indicator. Interestingly, sustained mitochondrial Ca(2+) uptake following repetitive tetanic stimulation was similar for triadic and longitudinal mitochondria in FDB fibers from 1-mo-old mice, and both mitochondrial populations were found by electron microscopy to be continuous and structurally tethered to the sarcoplasmic reticulum. Conversely, the frequency of osmotic shock-induced Ca(2+) sparks per CRU density decreased threefold (from 3.6 ± 0.2 to 1.2 ± 0.1 events·CRU(-1)·min(-1)·100 μm(-2)) during postnatal development in direct linear correspondence (r(2) = 0.95) to an increase in mitochondrion-CRU pairing. Together, these results indicate that mitochondrion-CRU association promotes Ca(2+) spark suppression but does not significantly impact mitochondrial Ca(2+) uptake.     

The value of urine osmolality as an index of stress in the ovine fetus

In ovine fetuses, during 100-130 days of gestation, urine osmolalities less than 175 mosmol/kg water were associated with plasma immunoreactive adrenocorticotrophin (ACTH) concentrations below 40 pg/ml in 40/41 samples. In 18/29 fetuses with urine osmolalities greater than 175 mosmol/kg water plasma ACTH was significantly elevated. In 38 samples of fetal blood there was a significant correlation between plasma ADH and ACTH concentrations. By least squares regression the equation to the line was [ACTH] = 5.06 + 3.70 [ADH] (r = 0.62, P less than 0.001). In 50 samples from fetuses of gestational ages 100-140 days, with urine osmolalities of 302 +/- 86 mosmol/kg (mean +/- SD) the blood pH, pO2 and pCO2 values were not significantly different from those in 50 samples from fetuses with urine osmolalities of 125 +/- 22 mosmol/kg. It is proposed that the measurement of fetal urine osmolality provides a good index of fetal stress. A fetus with a urine osmolality less than 175 mosmol/kg is almost invariably in the optimum, unstressed condition.