A presettable multichannel digital timer.

A digital timer is described which generates a number of pulses whose delays with respect to a periodic reference pulse can be independently preset by means of thumbwheel switches. The timing intervals are crystal-controlled and can be varied over a wide range--typically 0.1 ms to 99.99 s. It is shown how a pulse train of up to 46 pulses may be obtained, the delay of each pulse in the train being individually presettable. Digital integrated circuits are used throughout, except for the output stage of enhanced drive capability.     

Phase response versus positive and negative division delay in animal cells

The time of median cell division in V79 Chinese hamster cells following high serum pulses was determined for two synchronous cell generations following mitotic selection. Differences in cell cycle time for each pair of pulse and control cultures were computed and plotted as a function of time of serum pulse. This phase response curve for hamster cells with an 8.5 h cell cycle shows a characteristic biphasic pattern. Beginning 0.5 h after mitotic selection, pulses with serum produce delays in the midpoint of the subsequent mitotic waves. Delay is maximum at 1.5 h. Delays give way abruptly to advances at 2.5 h and the amount of advance then decreases as pulses are given between 3 and 5 h into the cycle. At 5 h decreasing advances become delays, with increasing delays due to serum pulses occurring between 5 and 6 h. Delays again give way abruptly to advances at 6 h and again the amount of advance decreases through the late portion of the cycle. Pulses very late in the cycle appear to generate phase delays. This biphasic response to serum is interpreted as an expression of an underlying time-keeping oscillator whose period is nominally of 4 h duration.     

A Model for the Propagation of Action Potentials in Non-Uniformly Excitable Media

Electrophysiological properties of cardiac tissue change as a function of position. We define the "excitability" as the propagation velocity of an excitation pulse through the tissue, and study a simple FitzHugh-Nagumo (FHN) model of heart tissue whose excitability changes with position. The propagation velocity is shown to be a good continuous measure of the excitability for both limit cycle and excitable tissue. The influence of the spatial dependence of the excitability is examined for several normal and pathological situations. A novel transient effect is observed for a train of pulses propagating across an excitability step. Copyright 1999 Academic Press.     

Islet hormone pulse intervals are dependent upon sampling frequency.

Pulsatile insulin secretion has been reported from a variety of in vivo and in vitro systems. While it is agreed that insulin pulses exist, there is little agreement concerning the basal frequency or interpulse interval either within the same species in vivo, as both long and short term pulses have been reported, or between in vivo and in vitro preparations. We propose that the frequency of sampling may have profound effects upon the calculated pulse interval. Three systems were used to test this hypothesis: 1) artificial test data were designed to produce regular pulses with an exact 11 min period, 2) perfusate insulin concentration from isolated canine pancreata sampled at 1 min intervals and 3) peripheral blood insulin concentrations from human volunteers sampled every 2 and 5 min. Pulse parameters were determined at 1, 2, 5, 20, 15, 30 and 60 min sampling intervals for each data set by the use of the computer algorithms Pulsar and Cycle Detector. The results indicate that for insulin secretory pulses, sampling frequencies longer than 2 min may result in the production of spurious pulse trains with multiple longer term pulse periods. It is concluded that islet hormone secretory pulse period calculations are dependent upon the sampling frequency.     

A neuronal model for the discharge patterns produced by cyclic inputs

To understand the patterns of nerve impulses produced by sinusoidal stimuli, a simple model is considered which integrates input currents with a finite time constant until a threshold voltage is reached, whereupon an output pulse is produced and the process is restarted. We show here that (a) a general analytic solution exists for this model driven by sinusoidal stimuli, determining the interval between every member of the pulse train, (b) for all values of the parameters of the model a pattern exists which repeats periodically after a finite number of pulses in the absence of noise, (c) the system will approach a stable pattern which, if perturbed, will be recovered once the perturbation is removed, (d) the linear integrator or relaxation oscillator and the curren multiplier are limiting cases of this model.     

Running activity mediates the phase-advancing effects of dark pulses on hamster circadian rhythms

Summary Pulses of darkness can phase-shift the circadian activity rhythms of hamsters,Mesocricetus auratus, kept in constant light. Dark pulses under these conditions alter photic input to the circadian system, but they also commonly trigger wheel-running activity. This paper investigates the contribution of running activity to the phase-shifting effects of dark pulses. A first experiment showed that running activity by itself can phaseshift rhythms in constant light. Hamsters were induced to run by being confined to a novel wheel for 3–5 h. When this was done at circadian times (CT) 0, 6, and 9, the mean steady-state phase-shifts were 0.6 h, 3.5 h, and 2.3 h, respectively. The latter two values are at least as large as those previously obtained with dark pulses of similar durations and circadian phases. A second experiment showed that restricting the activity of hamsters during 3-h dark pulses at CT 9 reduces the amplitude of the phase-shifts. Unrestrained animals phase-advanced by 1.1 h, but this shift was halved in animals whose wheel was locked, and completely abolished in animals confined to nest boxes during the dark pulse. Activity restriction in itself (without dark pulses) had only minimal phase-delaying effects on free-running rhythms when given between ca. CT 10 and CT 13. These results support the idea that, in hamsters at least, dark pulses affect the circadian system mostly by altering behavioural states rather than by altering photic input to the internal clock.Abbreviations CT circadian time - DD constant darkness - LD light-dark - LL constant light - PRC phase response curve - period of rhythm     

Pulsatile urea excretion in the gulf toadfish: mechanisms and controls

Opsanus beta expresses a full complement of ornithine–urea cycle (OUC) enzymes and is facultatively ureotelic, reducing ammonia-N excretion and maintaining urea-N excretion under conditions of crowding/confinement. The switch to ureotelism is keyed by a modest rise in cortisol associated with a substantial increase in cytosolic glutamine synthetase for trapping of ammonia-N and an upregulation of the capacity of the mitochondrial OUC to use glutamine-N. The entire day's urea-N production is excreted in 1 or 2 short-lasting pulses, which occur exclusively through the gills. The pulse event is not triggered by an internal urea-N threshold, is not due to pulsatile urea-N production, but reflects pulsatile activation of a specific branchial excretion mechanism that rapidly clears urea-N from the body fluids. A bidirectional facilitated diffusion transporter, with pharmacological similarity to the UT-A type transporters of the mammalian kidney, is activated in the gills, associated with an increased trafficking of dense-cored vesicles in the pavement cells. An 1814 kB cDNA (‘tUT’) coding for a 475–amino acid protein with approximately 62% homology to mammalian UT-A's has been cloned and facilitates phloretin-sensitive urea transport when expressed in Xenopus oocytes. tUT occurs only in gill tissue, but tUT mRNA levels do not change over the pulse cycle, suggesting that tUT regulation occurs at a level beyond mRNA. Circulating cortisol levels consistently decline prior to a pulse event and rise thereafter. When cortisol is experimentally clamped at high levels, natural pulse events are suppressed in size but not in frequency, an effect mediated through glucocorticoid receptors. The cortisol decline appears to be permissive, rather than the actual trigger of the pulse event. Fluctuations in circulating AVT levels do not correlate with pulses; and injections of AVT (at supraphysiological levels) elicit only minute urea-N pulses. However, circulating 5-hydroxytryptamine (5-HT) levels fluctuate considerably and physiological doses of 5-HT cause large urea-N pulse events. When the efferent cranial nerves to the gills are sectioned, natural urea pulse events persist, suggesting that direct motor output from the CNS to the gill is not the proximate control.     

Circadian rhythms in Neurospora: a new measurement, the reset zone

The authors define a new feature of a circadian rhythm, the reset zone, and point out its usefulness for predictions concerning oscillator behavior. The reset zone measures the responses of a circadian system to resetting pulses. It can be easily determined from a phase transition curve (PTC), which is simply a phase response curve (PRC) replotted as new phase versus old phase (Winfree's format). The reset zone is the range of new phases seen in such a plot and has two potentially useful characteristics: its size and its midpoint. A series of experiments with Neurospora involving temperature pulses indicated that the size of the reset zone changed in a nonlinear way in response to both the duration of 40 degrees C pulses and to the magnitude of temperature change for 3-h pulses. Other existing data are replotted to show how the reset zone size varies with growth temperature and with the period of different clock mutants. Employing exclusively reset zone data within the framework of a limit cycle displacement model, an equation is formulated that predicts the relative changes in the values of state variables of the oscillator for changes in any given environmental condition, such as temperature. Examples are also drawn from other organisms, such as hamsters, Gonyalaux, Kalanchoe, and Drosophila, illustrating the usefulness of the reset zone measurement. It can be used as a numerical scale for assessing the strength of a pulse, for comparing the relative effects of a given pulse applied to different organisms or mutants, for determining the directionality of the changes in state variables produced by various types of pulses, and possibly for measuring clock amplitude.     

Noninvasive cardiac output estimation: a preliminary study

 The availability of a simple-to-use, automatic measurement system for noninvasive flow estimation is imperative, given the clinical demand for an acceptable noninvasive procedure rather than the standard invasive procedure of thermodilution. A method for calculating cardiac output from noninvasively derived pressure pulses has been developed, and the results of a preliminary evaluation study on post-cardiac surgery patients for whom invasive flow measures were readily available for comparison are provided in this report. The proposed method relies on fast Fourier transform (FFT) analysis of pulses measured externally at the carotid and femoral pressure points. A transfer function of the aorta is computed from digitally filtered pulse measurements, and a tapered model of the aorta is parametrically adapted using a simplex optimization algorithm so that its transfer function matches that derived experimentally. An aortic input impedance term is obtained from the optimized model and utilized along with the carotid pulse (analogous to input voltage) to compute aortic flow. In addition to its automation, attractive features of this method include the requirement for relatively few pulses for analysis as well as considerable resistance to noise artifact. For 59 data records collected from 54 post-cardiac surgery patients, the average flow measurements computed over several pulses compare well with the standard, invasive method of thermodilution. Preliminary results also indicate a strong potential for tracking changes in cardiac output over time, and invite further use of the method in monitoring hemodynamically unstable patients. Received: 18 February 1997 / Accepted in revised form: 12 May 1997     

Pharmacokinetics and pharmacodynamics of fenoldopam mesylate for blood pressure control in pediatric patients

Background

Intermittent measurement of cardiac output may be performed using a lithium dilution technique (LiDCO). This can then be used to calibrate a pulse power algorithm of the arterial waveform which provides a continuous estimate of this variable. The purpose of this study was to examine the duration of accuracy of the pulse power algorithm in critically ill patients with respect to time when compared to measurements of cardiac output by an independent technique.

Methods

Pulse power analysis was performed on critically ill patients using a proprietary commercial monitor (PulseCO). All measurements were made using an in-dwelling radial artery line and according to manufacturers instructions. Intermittent measurements of cardiac output were made with LiDCO in order to validate the pulse power measurements. These were made at baseline and then following 1, 2, 4 and 8 hours. The LiDCO measurement was considered the reference for comparison in this study. The two methods of measuring cardiac output were then compared by linear regression and a Bland Altman analysis. An error rate for the limits of agreement (LOA) between the two techniques of less than 30% was defined as being acceptable for this study.

Results

14 critically ill medical and surgical patients were enrolled over a three month period. At baseline patients showed a wide range of cardiac output (median 7.5 L/min, IQR 5.1 -9.0 L/min). The bias and limits of agreement between the two techniques was deemed acceptable for the first four hours of the study with percentage errors being 29%, 22%, and 285 respectively. The percentage error at eight hours following calibration increased to 36%. The ability of the PulseCo to detect changes in cardiac output was assessed with a similar analysis. The PulseCO tracked the changes in cardiac output with adequate accuracy for the first four hours with percentage errors being 20%, 24% and 25%. However at eight hours the error had increased to 43%.

Conclusion

The agreement between lithium dilution cardiac output and the pulse power algorithm in the PulseCO monitor remains acceptable for up to four hours in critically ill patients.     

Repetitively rated plasma relativistic microwave oscillator with a controllable frequency in every pulse

A repetitively rated microwave oscillator whose frequency can be varied electronically from pulse to pulse in a predetermined manner is created for the first time. The microwave oscillator has a power on the order of 10⁸ W and is based on the Cherenkov interaction of a high-current relativistic electron beam with a plasma preformed before each pulse. Electronic control over the plasma properties allows one to arbitrarily vary the microwave frequency from pulse to pulse at a pulse repetition rate of up to 50 Hz.     

Mechanoelectrical excitation by fluid jets in monolayers of cultured cardiac myocytes.

Although the prevailing view of mechanoelectric feedback (MEF) in the heart is in terms of longitudinal cell stretch, other mechanical forces are considerable during the cardiac cycle, including intramyocardial pressure and shear stress. Their contribution to MEF is largely unknown. In this study, mechanical stimuli in the form of localized fluid jet pulses were applied to neonatal rat ventricular cells cultured as confluent monolayers. Such pulses result in pressure and shear stresses (but not longitudinal stretch) in the monolayer at the point of impingement. The goal was to determine whether these mechanical stimuli can trigger excitation, initiate a propagated wave, and induce reentry. Cells were stained with the voltage-sensitive dye RH237, and multi-site optical mapping was used to record the spread of electrical activity in isotropic and anisotropic monolayers. Pulses (10 ms) with velocities ranging from 0.3 to 1.8 m/s were applied from a 0.4-mm diameter nozzle located 1 mm above the cell monolayer. Fluid jet pulses resulted in circular wavefronts that propagated radially from the stimulus site. The likelihood for mechanical stimulation was quantified as an average stimulus success rate (ASSR). ASSR increased with jet amplitude and time waited between stimuli and decreased with the application of gadolinium and streptomycin, blockers of stretch-activated channels, but not with nifedipine, a blocker of the L-type Ca channel. Absence of cellular injury was confirmed by smooth propagation maps and propidium iodide stains. In rare instances, the mechanical pulse resulted in the induction of reentrant activity. We conclude that mechanical stimuli other than stretch can evoke action potentials, propagated activity, and reentrant arrhythmia in two-dimensional sheets of cardiac cells.     

The neuroendocrinology of human puberty revisited

The fundamental aspects of the hypothalamic luteinizing hormone-releasing hormone (LHRH)(1) [1]pulse generator-pituitary gonadotrophin-gonadal apparatus in mammals have striking commonalities. There are, however, critical, substantive differences in the neuroendocrinology of puberty among species. The onset of puberty in the human is marked by an increase in the amplitude of LH pulses, an indirect indicator of the increase in amplitude of LHRH pulses. The hypothalamic LHRH-pituitary gonadotrophin complex is functional by at least 0.3 gestation in the human foetus; the sex difference in the fetal and neonatal pattern of LH and FSH secretion is an apparent consequence of imprinting of the fetal hypothalamus-pituitary-gonadotropin apparatus by fetal testosterone. Until about 6 months of age in boys and 12-24 months in girls, the testes and ovaries respond to the increased LH in boys and follicle-stimulating hormone (FSH) in girls by secreting testosterone and oestradiol, respectively, reaching levels that are not again achieved before the onset of puberty. Striking features of the ontogeny of the human hypothalamic pulse generator are: (1) its development and function in the foetus; (2) the continued function of the hypothalamic LHRH pulse generator-pituitary gonadotrophin-gonadal axis in infancy; (3) the gradual damping of hypothalamic LHRH oscillator activity during late infancy; (4) its quiescence during childhood - the so-called juvenile pause; (5) during late childhood the gradual disinhibition and reactivation of the LHRH pulse generator, mainly at night; (6) the increasing amplitude of the LHRH pulses, which are reflected in the progressively increased and changing pattern of circulating LH pulses, with the approach of and during puberty. The intrinsic central nervous system (CNS) mechanisms responsible for the inhibition of the LHRH pulse generator during childhood (the juvenile phase) involve the major role of an inhibitory neuronal system - the CNS inhibitory neurotransmitter gamma-aminobutyric acid (GABA) and GABAergic neurons, as revealed by studies in the rhesus monkey by Terasawa and her associates. With the onset of puberty, the disinhibition and reactivation of the LHRH pulse generator is associated with a fall in GABAergic neurotransmission and a concomitant increase in the input of excitatory amino acid neurotransmitters (including glutamate) and possibly astroglial-derived growth factors. Despite remarkable progress over the past three decades, large gaps remain in our understanding of the neurobiological, genetic and environmental mechanisms involved in the control of the onset of puberty. The role of leptin in the control of the onset of puberty is reviewed. Severe leptin deficiency is associated with hypogonadotrophic hypogonadism; it appears that a critical level of leptin and a leptin signal is required to achieve puberty. The weight of evidence supports the hypothesis that leptin acts as one of several permissive factors and not a trigger in the onset of human puberty. The application of these advances provides a framework for the described classification of sexual precocity and delayed puberty.1 GnRH is synonymous with LHRH.     

Stochastic radial basis functions

Stochastic signal processing can implement gaussian activation functions for radial basis function networks, using stochastic counters. The statistics of neural inputs which control the increment and decrement operations of the counter are governed by Bernoulli distributions. The transfer functions relating the input and output pulse probabilities can closely approximate gaussian activation functions which improve with the number of states in the counter. The means and variances of these gaussian approximations can be controlled by varying the output combinational logic function of the binary counter variables.     

Seasonal pattern of luteinizing hormone and testosterone pulsatile secretion in young adult red deer stags (Cervus elaphus) and its association with the antler cycle.

Blood from stages aged 15 months (n = 6) was sampled at monthly intervals every 30 min for 24 h for 12 months, at 45 degrees S in New Zealand. Three extra samplings each for 24 h were carried out at about the anticipated time of antler casting. All samples were analysed for luteinizing hormone (LH) and testosterone and the resulting data further analysed by the Pulsar pulse detection routine. The animals were kept indoors under natural daylength and were fed ad libitum. All animals were weighed, antler status and size recorded and testes diameter was measured on each sampling day. Mean LH and testosterone pulsatily and plasma concentration varied seasonally. LH pulse frequency was low during autumn (2.5 pulses in 24 h), winter (1.0-1.5 pulses in 24 h) and early spring (1 pulse in 24 h) and lowest in late spring (0.2 pulse in 24 h) before rising in summer (1.0-4.0 pulses in 24 h). LH pulse amplitude and mean plasma concentration were low (< 1 ng ml-1) from March to November (autumn-spring); both rose to a peak in January (summer) of 3.4 and 1.6 ng ml-1, respectively. Testosterone pulse frequency was generally similar to LH except that slightly more pulses of testosterone than of LH were detected from March to November and more pulses of LH from November to February (summer). Testosterone pulse amplitude fell from March to November (5.3 ng ml-1 to undetectable) although there was a conspicuous peak in July (midwinter) of almost 5 ng ml-1.(ABSTRACT TRUNCATED AT 250 WORDS)     

Na-Ca exchange and the trigger for sarcoplasmic reticulum Ca release: studies in adult rabbit ventricular myocytes.

The importance of Na-Ca exchange as a trigger for sarcoplasmic reticulum (SR) Ca release remains controversial. Therefore, we measured whole-cell Ca currents (ICa), Na-Ca exchange currents (INaCa), cellular contractions, and intracellular Ca transients in adult rabbit cardiac myocytes. We found that changing pipette Na concentration markedly affected the relationship between cell shortening (or Ca transients) and voltage, but did not affect the Ca current-voltage relationship. We then inhibited Na-Ca exchange and varied SR content (by changing the number of conditioning pulses before each test pulse). Regardless of SR Ca content, the relationship between contraction and voltage was bell-shaped in the absence of Na-Ca exchange. Next, we rapidly and completely blocked ICa by applying nifedipine to cells. Cellular shortening was variably reduced in the presence of nifedipine. The component of shortening blocked by nifedipine had a bell-shaped relationship with voltage, whereas the "nifedipine-insensitive" component of contraction increased with voltage. With the SR disabled (ryanodine and thapsigargin pretreatment), ICa could initiate late-peaking contractions that were approximately 70% of control amplitude. In contrast, nifedipine-insensitive contractions could not be elicited in the presence of ryanodine and thapsigargin. Finally, we recorded reverse Na-Ca exchange currents that were activated by membrane depolarization. The estimated sarcolemmal Ca flux occurring by Na-Ca exchange (during voltage clamp steps to +30 mV) was approximately 10-fold less than that occurring by ICa. Therefore, Na-Ca exchange alone is unlikely to raise cytosolic Ca concentration enough to directly activate the myofilaments. We conclude that reverse Na-Ca exchange can trigger SR Ca release. Because of the sigmoidal relationship between the open probability of the SR Ca release channel and pCa, the effects of ICa and INaCa may not sum in a linear fashion. Rather, the two triggers may act synergistically in the modulation of SR release.     

Stridulation and hearing in the noctuid mothThecophora fovea (Tr.)

Summary MaleThecophora fovea (Tr.) (Noctuidae) sing continuously for several minutes by rubbing the 1. tarsal segment of the metathoracic leg against a stridulatory swelling on the hindwing. In Northern Yugoslavia (Slovenia) the males emerge in late October and start stridulating about a week later when the females emerge.The sounds are pulse trains consisting of 10–12 ms long sound pulses with main energy around 32 kHz and a PRR of 20 pulses/s. The mechanics of the sound producing apparatus was studied by activating the stridulatory swelling with short sound impulses. The impulse response of the swelling was recorded by laser vibrometry and amplitude spectra of the vibrations showed maximum velocities between 25 and 35 kHz. Hence, it seems likely that the stridulatory swelling is driven as a mechanical oscillator with a resonance frequency which determines the carrier frequency of the sounds.Audiograms of both males and females showed peak sensitivities at 25–30 kHz. The median threshold at the BF was 36 dB SPL. The peak intensity of the sound pulses was 83 dB SPL at 1 m, which should enable the moths to hear each other at distances of around 30 m. Therefore sound production inT. fovea might function in long distance calling. It is argued thatT. fovea can survive making such a noise in spite of being palatable to bats because it flies so late in the year that it is temporally isolated from bats.Abbreviations PRR pulse repetition rate - SPL sound pressure level - BF best frequency