Conduction velocity and excitability of A and C fibers of cat mesenteric nerves

The conduction velocity and excitability of fibers running from the mesenteric into the splanchnic nerves were studied in experiments on cats. Among the A fibers of these nerves there were shown to be: 1) fibers with an excitation threshold of 0.06–0.10 V (stimulus duration 0.1 msec) and a maximal conduction velocity of 48–85 m/sec; 2) fibers with an excitation threshold of 0.3–0.7 V, impulses of which form up to five waves in the composition of the action potential, with maximal conduction velocities of between 8–10 and 33–39 m/sec; 3) fibers with an excitation threshold of over 1 V and a conduction velocity of between 1.8 and 7 m/sec. The excitation threshold of the group C fibers was 6–8 V. Impulses of these fibers form a low-amplitude wave in the composition of the action potential of the mesenteric and splanchnic nerves with a conduction velocity of 1.0–1.8 m/sec, several waves of higher amplitude with a conduction velocity of 0.5–1.2 m/sec, and several low-amplitude waves with a conduction velocity of 0.35–0.55 m/sec. The results of experiments with different combinations of arrangement of the stimulating and recording electrodes on the mesenteric and splanchnic nerves indicate that sympathetic postganglionic C fibers of the mesenteric nerves occur only in the second group, whereas afferent C fibers occur in all three of the groups distinguished.Institute of Normal and Pathological Physiology, Academy of Medical Sciences of the USSR, Moscow. Translated from Neirofiziologiya, Vol. 7, No. 3, pp. 272–278, May–June, 1975.     

Response of Renshaw cells to sinusoidal stretch of hindlimb extensor muscles.

1. Renshaw cells responding disynaptically to electrically induced group I volleys in the intact gastrocnemius-soleus (GS) nerve, were submitted to small-amplitude, high-frequency vibration applied longitudinally to the deefferented GS muscle in precollicular decerebrate cats. 2. Vibration of the GS muscle at 200/sec, 180 mu peak-to-peak amplitude for 80-100 msec produced a sudden increase in the discharge rate of Renshaw cells, which gradually decreased within 25-50 msec to reach a steady level higher than that recorded in the absence of vibration. 3. Excitation of Renshaw cells appeared at a threshold amplitude of vibration (at 200-250/sec) of 5-20 mu and increased to a maximum value for amplitudes of about 70-80 mu, i.e., when all the primary endings of the spindles from the GS muscle had been driven by the stimulus. Recruitment of the secondary endings of the muscle spindles, due to large amplitude muscle vibration, did not modify the response of the Renshaw cells to the mechanically induced group Ia volleys. 4. These findings were obtained with the GS muscle pulled at 8 mm of initial extension. A threshold response of Renshaw cells to vibration appeared at 4 mm of static stretch, while maximal responses occurred at 8 mm. No further increase and actually a slight decrease in the response appeared for initial extensions of the muscle of 10-12 mm. 5. For a given vibration amplitude, the response of the Renshaw cells increased with increasing frequencies of vibration to reach the maximum at frequencies of 150-250/sec. Bursts of Renshaw cell discharges synchronous to each stroke of vibrator occurred only for low frequencies of stimulation (less than 25/sec). 6. It is concluded that vibration of the GS muscle represents a very effective method in exciting the Renshaw cells and that this response depends upon selective stimulation of homonymous motoneurons monosynaptically excited by the orthodromic volleys originating from the primary endings of the corresponding muscle spindles.     

Cortical and subcortical spreading depression in rats produced by focused ultrasound

Steady potential shifts produced by focused ultrasond were recorded in the cerebral cortex, hippocampus, thalamus, and caudate nucleus. Impulses of 50–100 msec duration were presented at a frequency of 5 and 10 Hz. Negative steady potential shifts were produced in each of the structures investigated, which gradually increased during rhythmic electrical reaction to reach –3 to –7 mV within 10–30 sec, often succeeded by a wave of spreading depression (SD). In each structure analyzed amplitude of SD waves measured 20–30 mV, lasting 30–40 sec in the cortex, the caudate nucleus and the thalamus, and 80–120 sec in the hippocampus. In unanesthetized and lightly anesthetized animals SD waves were on occasions the precursors of convulsive discharges forming under the action of focused ultrasound. Ultrasound at threshold doses proved ineffective for 5–7 min after the occurrence of an SD wave, but again evoked repeated SD waves once the refractory period had ended. Accordingly, local effects produced by focused ultrasound can result in functional blockage of the brain structures due to cortical and subcortical spreading depression.Institute of Higher Nervous Activity and Neurophysiology, Academy of Sciences of the USSR, Moscow. Institute of Brain Research, All-Union Research Center of Mental Health, Academy of Medical Sciences of the USSR, Moscow. N. N. Andreev Acoustic Institute, Academy of Sciences of the USSR, Moscow. Translated from Neirofiziologiya, Vol. 18, No. 1, pp. 55–61, January–February, 1986.     

Spread of fast thermowaves through the cerebral cortex produced by visual stimulation

Thermowaves spreading through the cerebral cortex were observed and investigated during acute experiments on white rats using a new technique — that of thermoencephaloscopy (TES) through the intact skull. These waves were induced by regular visual stimulation (at intervals of 1.5–3 min) or by initiating one of the flashes and spread through the cortex along trajectories of five basic types; amplitude of thermowaves: 0.005–0.1°C; length: 10–15 mm; duration 1.2–11.4 sec; velocity: 1–33 mm/sec; extent of pathway: 2–56 mm. They appeared with a high degree of probability (of 0.92) during the interval between 15 sec before and 26 sec after the flash. Numbers of moving waves declined by the point of stimulus application and rose by 7–8 sec after the flash. Waves arose in 50% of cases in the contralateral visual cortex (areas 17 and 18a), spreading to the midline and crossing to the ipsilateral hemisphere (areas 17, 18a, and 7). Local waves moving along a circular trajectory were also discovered in the contralateral visual cortex. Several types of wave, differing in trajectory, also arose in the ipsilateral visual cortex. Mechanisms and possible significance of this effect are examined.Institute of Higher Nervous Activity and Neurophysiology, Academy of Sciences of the USSR, Moscow. Translated from Neirofiziologiya, Vol. 21, No. 4, pp. 467–475, July–August, 1989.     

Behavioral and neurophysiological assessment of lateral line sensitivity in the mottled sculpin,Cottus bairdi

1. The unconditioned feeding response of the mottled sculpin, Cottus bairdi, was used to measure threshold sensitivity of the lateral line system to a vibrating sphere as a function of stimulus position (i.e., sphere near head, trunk or tail) and vibration frequency. In addition, extracellular recording techniques were used to measure threshold sensitivity curves for posterior lateral line nerve fibers for the same stimulus positions used for measuring trunk sensitivity in behavioral measurements. 2. For all stimulus positions, behaviorally-measured threshold sensitivity was relatively independent of vibration frequency from 10 to 100 Hz when defined in terms of water acceleration, rather than velocity or displacement. Best thresholds for stimuli placed 15 mm away from the head were around -75 dB re: 1m/s(2), approximately 20 dB less than that for stimuli placed at the same distance near the tail. Trunk sensitivity was intermediate. 3. Physiologically-measured threshold sensitivity, in terms of acceleration, was also relatively independent of of frequency from 10 to 100 Hz in most fibers. A smaller number of fibers showed a decline in acceleration sensitivity after 10-30 Hz, with the rate of decline being equivalent to equal velocity sensitivity. Best sensitivity of all fibers fell between -40 and -70 dB re: 1m/s (2). 4. These results indicate that (a) behavioral thresholds are based on acceleration-sensitive endorgans--most likely lateral line canal (rather than superficial) neuromasts, (b) behavioral performance can be accounted for on the basis of information from a single population of fibers, and (c) sensitivity varies along the fish's body in a manner that corresponds to the size and distribution of neuromasts.     

Axonal transmission in the retina introduces a small dispersion of relative timing in the ganglion cell population response

Background

Visual stimuli elicit action potentials in tens of different retinal ganglion cells. Each ganglion cell type responds with a different latency to a given stimulus, thus transforming the high-dimensional input into a temporal neural code. The timing of the first spikes between different retinal projection neurons cells may further change along axonal transmission. The purpose of this study is to investigate if intraretinal conduction velocity leads to a synchronization or dispersion of the population signal leaving the eye.

Methodology/Principal Findings

We ‘imaged’ the initiation and transmission of light-evoked action potentials along individual axons in the rabbit retina at micron-scale resolution using a high-density multi-transistor array. We measured unimodal conduction velocity distributions (1.3±0.3 m/sec, mean ± SD) for axonal populations at all retinal eccentricities with the exception of the central part that contains myelinated axons. The velocity variance within each piece of retina is caused by ganglion cell types that show narrower and slightly different average velocity tuning. Ganglion cells of the same type respond with similar latency to spatially homogenous stimuli and conduct with similar velocity. For ganglion cells of different type intraretinal conduction velocity and response latency to flashed stimuli are negatively correlated, indicating that differences in first spike timing increase (up to 10 msec). Similarly, the analysis of pair-wise correlated activity in response to white-noise stimuli reveals that conduction velocity and response latency are negatively correlated.

Conclusion/Significance

Intraretinal conduction does not change the relative spike timing between ganglion cells of the same type but increases spike timing differences among ganglion cells of different type. The fastest retinal ganglion cells therefore act as indicators of new stimuli for postsynaptic neurons. The intraretinal dispersion of the population activity will not be compensated by variability in extraretinal conduction times, estimated from data in the literature.     

Ca2+ -free medium enhances the magnitude of slow peak in compound action potential of frog sciatic nerve in vitro

The present investigation was carried out to know the effect of Ca2+ on different peaks of compound action potential (CAP) representing the fibers having different conduction velocity. CAP was recorded from a thin bundle of nerve fibers obtained from desheathed frog sciatic nerve. Suction electrodes were used for stimulating and recording purposes. In Ca2+ -free amphibian Ringer, two distinct peaks (Peak-I and Peak-II) were observed. The threshold, conduction velocity (CV), amplitude and duration of Peak-I were 0.32 +/- 0.02 V, 56 +/- 3.0 m/sec, 2.1 +/- 0.2 mV and 0.75 +/- 0.1 ms, respectively. The Peak-II exhibited ten times greater threshold, eight times slower CV, three times lower amplitude and four times greater duration as compared to Peak-I. Addition of 2 mM Ca2+ in the bathing medium did not alter CAP parameters of Peak-I excepting 25% reduction in CV. But, in Peak-II there was 70-75% reduction in area and amplitude. The concentration-attenuation relation of Peak-II to various concentrations of Ca2+ was nonlinear and 50% depression occurred at 0.35 mM of Ca2+. Washing with Ca2+ -free solution with or without Mg2+ (2 mM)/verapamil (10 microM) could not reverse the Ca2+ -induced changes in Peak-II. Washing with Ca2+ -free solution containing EDTA restored 70% of the response. The results indicate that Ca2+ differentially influence fast and slow conducting fibers as the activity of slow conducting fibers is greatly suppressed by external calcium.     

Stimulation of the hippocampus and its effect on electrographic manifestations of the brain in unrestrained rats.

The dorsal hippocampus was electrically stimulated in unanaesthetized, unrestrained rats with a cobalt-gelatin rod in their cortex. The significance of the hippocampus in the elicitation of both physiological spontaneous rhythmic activity (episodic activity of 8--9/sec frequency bound, in rats, to a state of quiet wakefulness, and "sleep spindles") and pathological rhythmic activity of the self-sustained after-discharge (SSAD) type was determined from the aspect of the EEG and behavioural characteristics. 1. Single electrical pulses (0.1 msec, 1--10 V, 0.3/sec) elicited an evoked potential bilaterally in the somatosensory cortex. Elicitation of rhythmic after-activity (of the type of episodes or sleep spindles) was observed only in some cases in which an adequately strong stimulus was used. 2. Repeated series of rhythmic electrical stimuli following each other at short intervals (2--3 min) led to the formation of SSAD in about one third of the cases and at all stimulation frequencies (3-15/sec), although low frequencies (3--4/sec) were the least effective. The character of the SSAD and simultaneous behavioural phenomena differed fundamentally from those evoked by electrical stimulation of the thalamus (Chocholová et al. 1977). The development of paroxysmal after-activity was signalled by responses of a more or less distinct "recruiting" character during stimulation. On the basis of a comparison of electrographic and behavioural manifestations after electrical stimulation of the thalamus and hippocampus, the possibility of both thalamic and extrathalamic projection from the hippocampus to the cortical region is considered.     

Effect of stretching on the action potentials of the human and rabbit ventricular myocardium

The effect of stretching from L0 to Lmax on the electrical activity was studied on human myocardial preparations from patients with heart disease and on strips of rabbit ventricular myocardium. Muscular deformation was shown to decrease the amplitude and velocity of depolarization in slow action potentials. The action potentials (AP) possessing a fast depolarization phase were not sensitive to physiological stretching. Antiarrhythmic drugs--ethmozin (2 X 10(-5) M) and ethacizin (2 X 10(-6) M)--caused a decrease in the rate of AP depolarization, thus increasing AP sensitivity to deformation. It is suggested that stretching under the action of ethmozin and ethacizin reduced cardiomyocyte excitability due to suppression of slow Ca-current.     

Spread of directly evoked responses in the cat''s cerebral cortex

A study has been made of the electrical responses to direct stimulation of the exposed cerebral cortex of cats that had been immobilized with neuromuscular blocking drugs, and whose muscle and skin wounds had been locally anesthetized. The characteristics and spread of the first and second surface-negative responses are described. It was found that the first surface-negative response to weak stimuli decays linearly to zero at 3 to 6 mm. from the point of stimulation. Intermediate stimuli cause farther and non-linear spread: responses are re-initiated, or reinforced, at 6 to 10 mm.; and supramaximal stimulation produces reinforcement both at 5 and at 10 mm. The conduction velocity of these responses is uniform for linear spread (0.7 to 2.0 m./sec.), but reinforced responses occur 1 to 3 msec. earlier than would be expected for simple conduction. The phenomenon of re-initiation, or reinforcement, depends upon the excitatory state of the brain; circulation and previous stimulation are important factors. Connections outside the gyrus matter only in so far as they provide other sources of general excitation. It is concluded that two types of transmission: slow and fast, can lead to generation of similar surface-negative responses. The suggestion is made that the slowly conducted surface-negative potentials are due to direct or to synaptic excitation of pyramidal cells; while the responses with shortened latency are initiated synaptically on other pyramidal cells after fast conduction at about 10 m./sec. in tangential fibres.     

Cross-sectional growth study in patients with Turner's syndrome

The body height, weight and growth velocity were investigated in 416 patients with Turner's syndrome whose age ranged from 3 to 17 years. They were all prepubertal at the time of the present study. The chromosomal analysis revealed 45, X monosomy in 148 cases, mosaicism in 208 cases, and nonmosaic structural abnormalities of X chromosome in 60 cases. There were no significant differences in height, growth velocity and weight between the patients with the 45, X karyotype and those with other chromosomal variants at any age. Combined mean heights at 3, 10 and 17 years of age were 86.0 +/- 3.5 (m +/- SD), 116.7 +/- 5.8 and 136.8 +/- 4.8 cm, respectively. These values were below -2.0 SD of normal Japanese girls. The growth velocity was 6.0 +/- 0.5 cm/year at 4 years of age, but decreased gradually and was 1.6 +/- 0.7 cm/year at 17 years of age. The degree of overweight was within +/- 10% of ideal body weight for height between the ages of 3 and 8, 10-20% between the ages of 9 and 10, and 20-30% above the age of 11 years.     

Cortical spreading depression synaptically induced by brief high-frequency electrical stimulation of the rat brain

Electrical stimulation (ES) at the surface of the rat brain (10–200 Hz; brief trains of 10 pulses) was found to be most effective for evoking waves of spreading depression (SD) in the cortex. Repeated stimuli spaced at 10–15 min intervals did not produce convulsive activity and nor did mechanisms of SD inhibition set in under these conditions. A 5–6-fold reduction in SD threshold occurred when the intra-burst rate was increased from 10 to 200 Hz. Temporal summation of residual processes occurring with suprathreshold ES applied at the rate of 50 and 200 Hz resulted in significant broadening of the SD focus in the ES area and regular occurrence of additional SD foci on the side ipsilateral to stimulation and in the contralateral cortex. The protracted changes in cortical excitation lingering after ES by high-frequency currents brought about a decline in SD threshold and pointed to the active part played by synaptic processes in triggering this reaction.Institute of Higher Nervous Activity and Neurophysiology, Academy of Sciences of the USSR, Moscow. Translated from Neirofiziologiya, Vol. 21, No. 6, pp. 789–796, November–December, 1989.     

Assessment of Model Based (Input) Impedance,Pulse Wave Velocity,and Wave Reflection in the Asklepios Cohort

Objectives

Arterial stiffness and wave reflection parameters assessed from both invasive and non-invasive pressure and flow readings are used as surrogates for ventricular and vascular load. They have been reported to predict adverse cardiovascular events, but clinical assessment is laborious and may limit widespread use. This study aims to investigate measures of arterial stiffness and central hemodynamics provided by arterial tonometry alone and in combination with aortic root flows derived by echocardiography against surrogates derived by a mathematical pressure and flow model in a healthy middle-aged cohort.

Methods

Measurements of carotid artery tonometry and echocardiography were performed on 2226 ASKLEPIOS study participants and parameters of systemic hemodynamics, arterial stiffness and wave reflection based on pressure and flow were measured. In a second step, the analysis was repeated but echocardiography derived flows were substituted by flows provided by a novel mathematical model. This was followed by a quantitative method comparison.

Results

All investigated parameters showed a significant association between the methods. Overall agreement was acceptable for all parameters (mean differences: -0.0102 (0.033 SD) mmHg*s/ml for characteristic impedance, 0.36 (4.21 SD) mmHg for forward pressure amplitude, 2.26 (3.51 SD) mmHg for backward pressure amplitude and 0.717 (1.25 SD) m/s for pulse wave velocity).

Conclusion

The results indicate that the use of model-based surrogates in a healthy middle aged cohort is feasible and deserves further attention.     

Schwimmverhalten und Schwimmgeschwindigkeit bei den Larven des HeringsClupea harengus

The present study is based on two year experiments; it analyses swimming behaviour and swimming speed at different developmental stages of the herring. Yolk sac larvae tend to sink rather rapidly during resting phases. At the end of the yolk sac stage the sinking rate is at its minimum; it increases again with increasing larva size. During the phase of yolk sac resorption, vertical movements become gradually transformed into horizontal ones. Generally, three types of swimming can be distinguished: (1) “Abrupt swimming” consisting of very short periods of fast swimming; normally each dart is connected with a change in swimming direction. (2) “Normal swimming” characterized by steady movements for several seconds; it results in a winding path. (3) “Slow meandering” representing search swimming, a slowly winding locomotion with a large amplitude of each winding but with very little net progression of the larva. Swimming speed varies considerably in all size groups. The 8 to 11 mm (total length) larvae reach a mean swimming velocity (undulation) of 1.0 to 1.2 cm per second. Swimming speed, measured as the straight line distance between start and end points of a single swimming phase, attains mean values of 7 to 8 mm/sec in 8 to 11 mm larvae, 10 to 11 mm/sec in 11 to 15 mm larvae, 21 to 25 mm/sec in 19 to 24 mm larvae, and 40 to 50 mm/sec in 32 to 40 mm larvae. Swimming activity changes during larval development and seems to be influenced by food supply. The total distance travelled in 5 minutes by the head of a yolk sac larva is 1 to 3 m. About 8 days after hatching, sinking rate is low and “search swimming” (slow meandering movements) prevails. The path covered by the head within 5 minutes is 0.8 to 1.5 m.     

Critical determinants of endurance performance in middle-aged and elderly endurance runners with heterogeneous training habits

The current investigation was designed to determine which factor or what combination of factors would best account for distance running performance in middle-aged and elderly runners (mean age 57.5 years SD +/- 9.7) with heterogeneous training habits. Among 35 independent variables which were arbitrarily selected as possible prerequisites in the distance running performance of these runners, oxygen uptake (VO2) at lactate threshold (LT) (r = 0.781-0.889), maximal oxygen uptake (VO2 max) (r = 0.751 approximately 0.886), and chronological age (r = -0.736-(-)0.886) were found to be the 3 predictor variables showing the highest correlations with the mean running velocity at 5 km (V5km), 10 km (V10km), and marathon (VM). When all independent variables were used in a multiple regression analysis, any 3 or 4 variables selected from among VO2 at LT, chronological age, systolic blood pressure (SBP), atherogenic index (AI), and Katsura index (KI) were found to give the best explanation of V5km, V10km, or VM in a combined linear model. Linear multiple regression equations constructed for predicting the running performances were: V5km = 0.046X1-0.026X2-0.0056X3+5.17, V10km = 0.028X1-0.028X2-0.190X4-1.34X5+6.45, and VM = -0.0400X2-0.324X4-1.16X5+7.36, where X1 = VO2 at LT (ml.min-1.kg-1), X2 = chronological age, X3 = SBP, X4 = AI, and X5 = KI.(ABSTRACT TRUNCATED AT 250 WORDS)     

A finite element study of mechanical stimuli in scaffolds for bone tissue engineering

Mechanical stimuli are one of the factors that affect cell proliferation and differentiation in the process of bone tissue regeneration. Knowledge on the specific deformation sensed by cells at a microscopic level when mechanical loads are applied is still missing in the development of biomaterials for bone tissue engineering. The objective of this study was to analyze the behavior of the mechanical stimuli within some calcium phosphate-based scaffolds in terms of stress and strain distributions in the solid material phase and fluid velocity, fluid pressure and fluid shear stress distributions in the pores filled of fluid, by means of micro computed tomographed (CT)-based finite element (FE) models. Two samples of porous materials, one of calcium phosphate-based cement and another of biodegradable glass, were used. Compressive loads equivalent to 0.5% of compression applied to the solid material phase and interstitial fluid flows with inlet velocities of 1, 10 and 100 microm/s applied to the interconnected pores were simulated, changing also the inlet side and the viscosity of the medium. Similar strain distributions for both materials were found, with compressive and tensile strain maximal values of 1.6% and 0.6%, respectively. Mean values were consistent with the applied deformation. When 10 microm/s of inlet fluid velocity and 1.45 Pas viscosity, maximal values of fluid velocity were 12.76 mm/s for CaP cement and 14.87 mm/s for glass. Mean values were consistent with the inlet ones applied, and mean values of shear stress were around 5 x 10(-5)Pa. Variations on inlet fluid velocity and fluid viscosity produce proportional and independent changes in fluid velocity, fluid shear stress and fluid pressure. This study has shown how mechanical loads and fluid flow applied on the scaffolds cause different levels of mechanical stimuli within the samples according to the morphology of the materials.     

Norepinephrine induced contractions of the feline mesenterial vein under oxygenized and hypoxic conditions in vitro

Cylindrical segments from mesenteric veins of 8 cats were prepared and mounted in a Krebs-Ringer tissue bath. The oxygenized solution was bubbled with 95% O2 and 5% CO2. For lowered oxygen tension 95% N2 and 5% CO2 was used. Intraluminal pressure was changed between 0-20-0 mm Hg in consecutive cycles at a rate of 0.93-1.33 mm Hg/sec. Outer radii on the upward routes were recorded. Norepinephrine was added in doses of 6 X 10(-8) -6 X 10(-5) M, first in the oxygenized medium then under hypoxic conditions, and then in oxygenized medium again. Maximally relaxed curves were taken with 1.5 X 10(-4) M papaverine at the end of the experiment. Outer radius of relaxed segments at 20 mm Hg intraluminal pressure was 2.03 +/- 0.12 mm which slowly dilated to 2.09-0.12 mm toward the end of the experiment, and reached 2.11 +/- 0.11 mm with papaverine. Maximum active contractions of the outer radii were found at 6 mm Hg intraluminal pressure and with 6 X 10(-5) M norepinephrine in the bath: 23.1 +/- 3.2% in oxygenized, 20.3 +/- 3.4% in hypoxic and 19.0 +/- 3.4% again in oxygenized media. The observations showed that acute hypoxia had no or had only a limited effect on the contraction of the feline mesenteric vein.     

Properties of calcium and potassium currents of clonal adrenocortical cells

The ionic currents of clonal Y-1 adrenocortical cells were studied using the whole-cell variant of the patch-clamp technique. These cells had two major current components: a large outward current carried by K ions, and a small inward Ca current. The Ca current depended on the activity of two populations of Ca channels, slow (SD) and fast (FD) deactivating, that could be separated by their different closing time constants (at -80 mV, SD, 3.8 ms, and FD, 0.13 ms). These two kinds of channels also differed in (a) activation threshold (SD, approximately -50 mV; FD, approximately -20 mV), (b) half-maximal activation (SD, between -15 and -10 mV; FD between +10 and +15 mV), and (c) inactivation time course (SD, fast; FD, slow). The total amplitude of the Ca current and the proportion of SD and FD channels varied from cell to cell. The amplitude of the K current was strongly dependent on the internal [Ca2+] and was almost abolished when internal [Ca2+] was less than 0.001 microM. The K current appeared to be independent, or only slightly dependent, of Ca influx. With an internal [Ca2+] of 0.1 microM, the activation threshold was -20 mV, and at +40 mV the half-time of activation was 9 ms. With 73 mM external K the closing time constant at -70 mV was approximately 3 ms. The outward current was also modulated by internal pH and Mg. At a constant pCa gamma a decrease of pH reduced the current amplitude, whereas the activation kinetics were not much altered. Removal of internal Mg produced a drastic decrease in the amplitude of the Ca-activated K current. It was also found that with internal [Ca2+] over 0.1 microM the K current underwent a time-dependent transformation characterized by a large increase in amplitude and in activation kinetics.     

The chemo-mechanical coupling relation in the oscillatory contraction-relaxation cycles of insect fibrillar muscle.

The mechanical properties and the activity of the myofibrillar ATPase have been investigated at 21 degrees C on glycerinated back muscle from the water-bug Lethocerus colossicus. When the fibres were held under isometric conditions after stretching them by 0.5--4%, the ATPase required to maintain a given tension increases from 19 to 39 p-moles ATP split for each mg of tension developed as the Ca2+ level is increased from 10(-7) to up to 10(-5) M. The mechanical properties and the ATPase activity have been determined for Ca2+-activated fibres using sinusoidal frequencies of 1--30 HZ and oscillatory amplitudes of 0.5--6% peak-to-peak. In this way the R.M.S. velocity of sinusoidal movement was varied between 0.1-10 mm/sec. The rate of ATP splitting associated with oscillatory tension development, the dynamic tension cost, increases both with Ca2+ and with frequency of oscillation (at 1% peak-to-peak amplitude), becoming as high as four times the isometric value. The oscillatory power output which can be obtained is increased when the Ca2+ level is raised from 10(-7) to 10(-5) M or towards higher amplitudes of oscillation. The chemo-mechanical coupling efficiency increases proportionally with the R.M.S. velocity of muscle movement. In presence of 10(-5) M Ca2+ optimal efficiencies of 5.5--6.2 kcal work per mole ATP split are obtained at R.M.S. velocities of 1.3--2 muscle lengths/sec. The ability of the muscle fibres to perform osciillatory work at the higher frequencies was much reduced at lower Ca2+ levels of 10(-6) or 10(-7) M and the maximal efficiencies never exceeded 2.2 kcal/mole.     

Subtle Paranodal Injury Slows Impulse Conduction in a Mathematical Model of Myelinated Axons

This study explores in detail the functional consequences of subtle retraction and detachment of myelin around the nodes of Ranvier following mild-to-moderate crush or stretch mediated injury. An equivalent electrical circuit model for a series of equally spaced nodes of Ranvier was created incorporating extracellular and axonal resistances, paranodal resistances, nodal capacitances, time varying sodium and potassium currents, and realistic resting and threshold membrane potentials in a myelinated axon segment of 21 successive nodes. Differential equations describing membrane potentials at each nodal region were solved numerically. Subtle injury was simulated by increasing the width of exposed nodal membrane in nodes 8 through 20 of the model. Such injury diminishes action potential amplitude and slows conduction velocity from 19.1 m/sec in the normal region to 7.8 m/sec in the crushed region. Detachment of paranodal myelin, exposing juxtaparanodal potassium channels, decreases conduction velocity further to 6.6 m/sec, an effect that is partially reversible with potassium ion channel blockade. Conduction velocity decreases as node width increases or as paranodal resistance falls. The calculated changes in conduction velocity with subtle paranodal injury agree with experimental observations. Nodes of Ranvier are highly effective but somewhat fragile devices for increasing nerve conduction velocity and decreasing reaction time in vertebrate animals. Their fundamental design limitation is that even small mechanical retractions of myelin from very narrow nodes or slight loosening of paranodal myelin, which are difficult to notice at the light microscopic level of observation, can cause large changes in myelinated nerve conduction velocity.