Sound emission and the acoustic far field of a singing acridid grasshopper (Omocestus viridulus L.)

1999 ◽  
Vol 202 (12) ◽  
pp. 1571-1577
Author(s):  
A. Michelsen ◽  
N. Elsner
Keyword(s):  
Sound Production ◽  
Sound Intensity ◽  
Movement Pattern ◽  
Forward Direction ◽  
Octave Band ◽  
Sound Emission ◽  
Mean Values ◽  
The Mean ◽  
The One ◽  
Sound Intensities

An array of eight microphones, all at a distance of 15 cm, was used to make simultaneous recordings of the sounds emitted by courting male acridid grasshoppers of the species Omocestus viridulus. In this species, the movement pattern for sound production differs in the two hindlegs, and in most cases the leg facing the female moves with the larger amplitude. The sonic sound intensity (the total sound in the one-third octave bands with centre frequencies from 5 to 20 kHz) is maximal ipsilateral to the leg stridulating with the larger amplitude (the dominant leg). A spontaneous switch of dominance to the other leg may cause a significant change in the emitted sound power. The sound intensities contralateral to the dominant leg and frontal to the animal are, on average, approximately half (−3 dB) of the ipsilateral value, whereas the mean sound intensities behind and above the singer are approximately one-fifth (−7 dB) of the ipsilateral value. In most singers, the patterns of sound radiation are close to these mean values, but in some singers the radiation patterns are radically different. The sound radiated in various directions differs not only in terms of sound intensity but also with respect to the frequency spectrum, which was studied up to the one-third octave band with a centre frequency of 31.5 kHz. In particular, the ratio between the ultrasonic and sonic components is much smaller in the forward direction than in other directions. This may allow the courted female to hear whether the courting male is oriented directly towards her.

scholarly journals Retinomotor movements in the Antarctic fish Trematomus newnesi Boulenger submitted to different environmental light conditions

2007 ◽  
Vol 24 (2) ◽  
pp. 457-462 ◽  
Author(s):  
Lucélia Donatti ◽  
Edith Fanta
Keyword(s):  
Pigment Epithelium ◽  
Antarctic Fish ◽  
Constant Darkness ◽  
Time Intervals ◽  
Mean Values ◽  
Environmental Light ◽  
The Mean ◽  
The Difference ◽  
The One ◽  
The Antarctic

The Antarctic fish Trematomus newnesi (Boulenger, 1902) occurs from benthic to pelagic habitats, in seasonally and daily varied photic conditions that induce retinomotor movements. Fish were experimentally kept under constant darkness or light, and 12Light/12Dark for seven days. The retinomotor movement of the pigment epithelium was established through the pigment index, while that of the cones was calculated as the length of the myoid. The retinomotor movement of the pigment epithelium in T.newnesi,revealed that the adaptation to constant light occurred in the one hour of exposure, remaining constant for the next seven days. However, the adaptation to constant darkness, was slower. The difference between the mean values of the pigment indices in the time intervals of sampling was significant in the first hours of the experiment, and only after six hours they were not significant any more. The myoid of cones became elongated in darkness and contracted in light. In the experiments where T.newnesiwas exposed initially to 12 hours light followed by 12 hours darkness 12 was evidenced that the speed and intensity of the retinomotor movements was higher when darkness changed into light, than when light changed into darkness.

Physiological and biophysical limits to work in the heat for clothed men and women

1978 ◽  
Vol 44 (6) ◽  
pp. 918-925 ◽  
Author(s):  
E. Kamon ◽  
B. Avellini ◽  
J. Krajewski
Keyword(s):  
Steady State ◽  
Vapor Pressure ◽  
Physiological Responses ◽  
Men And Women ◽  
Mean Values ◽  
Air Temperatures ◽  
Significant Difference ◽  
The Mean ◽  
Evaporative Heat Transfer ◽  
The One

Heat-acclimated, lightly clothed men and women (four of each) walked on a treadmill at 25% and 43% VO2 max, respectively, (M =194 W.m-2), under seven air temperatures (Ta) ranging from 36 to 52 degrees C. Each experiment involved 1 h of fixed and a 2nd h of progressively increasing ambient vapor pressure (Pa). The relative steady state of rectal temperature (Tre), mean skin temperature (Tsk), and heart rate (HR) reached in the 1st h were forced upward during the 2nd h by the rising Pa. The critical air vapor pressure (Pcrit) was identified by the Tre point of inflection for each Ta. One man did not fully reach steady state, but inflection could be determined for his physiological responses. The mean values of all points of inflection were calculated for Tre, Tsk, and HR. Significant sex difference in HR was found only by excluding the results of the one man. Tre and Tsk showed no significant difference between men and women. The coefficient for evaporative heat transfer (he), which could be derived using the Pcrit for the low Ta range, was 14.5 +/- 2.2 W.m-1 Torr-1.

the ‘Area Under the Curve’ or AUC. The AUC is taken as a measure of exposure of the drug to the subject. The peak or maximum concen-tration is referred to as Cmax and is an important safety measure. For regulatory approval of bioequivalence it is necessary to show from the trial results that the mean values of AUC and Cmax for T and R are not significantly different. The AUC is calculated by adding up the ar-eas of the regions identified by the vertical lines under the plot in Figure 7.1 using an arithmetic technique such as the trapezoidal rule (see, for example, Welling, 1986, 145–149, Rowland and Tozer, 1995, 469–471). Experience (e.g., FDA Guidance, 1992, 1997, 1999b, 2001) has dictated that AUC and Cmax need to be transformed to the natural logarithmic scale prior to analysis if the usual assumptions of normally distributed errors are to be made. Each of AUC and Cmax is analyzed separately and there is no adjustment to significance levels to allow for multiple testing (Hauck et al., 1995). We will refer to the derived variates as log(AUC) and log(Cmax), respectively. In bioequivalence trials there should be a wash-out period of at least five half-lives of the drugs between the active treatment periods. If this is the case, and there are no detectable pre-dose drug concentrations, there is no need to assume that carry-over effects are present and so it is not necessary to test for a differential carry-over effect (FDA Guidance, 2001). The model that is fitted to the data will be the one used in Section 5.3 of Chapter 5, which contains terms for subjects, periods and treatments. Following common practice we will also fit a sequence or group effect and consider subjects as a random effect nested within sequence. An example of fitting this model will be given in the next section. In the following sections we will consider three forms of bioequivalence: average (ABE), population (PBE) and individual (IBE). To simplify the following discussion we will refer only to log(AUC); the discussion for log(Cmax) is identical. To show that T and R are average bioequivalent it is only necessary to show that the mean log(AUC) for T is not significantly different from the mean log(AUC) for R. In other words we need to show that, ‘on average’, in the population of intended patients, the two drugs are bioequivalent. This measure does not take into account the variability of T and R. It is possible for one drug to be much more variable than the other, yet be similar in terms of mean log(AUC). It was for this reason that PBE was introduced. As we will see in Section 7.5, the measure of PBE that has been recommended by the regulators is a mixture of the mean and variance of the log(AUC) values (FDA Guidance, 1997, 1999a,b, 2000, 2001). Of course, two drugs could be similar in mean and variance over the

2003 ◽  
pp. 350-350
Keyword(s):  
Multiple Testing ◽  
Random Effect ◽  
Area Under The Curve ◽  
Mean Values ◽  
Fda Guidance ◽  
Significance Levels ◽  
Mean And Variance ◽  
The Mean ◽  
Carry Over ◽  
The One

scholarly journals Effects of seasonal variations and collection methods on the mineral composition of propolis from Apis mellifera Linnaeus Beehives

2016 ◽  
Vol 76 (2) ◽  
pp. 396-401 ◽  
Author(s):  
E. A. Souza ◽  
R. Zaluski ◽  
N. Veiga ◽  
R. O. Orsi
Keyword(s):  
Apis Mellifera ◽  
Mineral Composition ◽  
Seasonal Variations ◽  
Atomic Absorption Spectrophotometry ◽  
Mean Values ◽  
Africanized Honey Bees ◽  
Harvesting Method ◽  
The Mean ◽  
One Year ◽  
The One

Abstract The effects of seasonal variations and the methods of collection of propolis produced by Africanized honey bees Apis mellifera Linnaeus, 1758, on the composition of constituent minerals such as magnesium (Mg), zinc (Zn), iron (Fe), sodium (Na), calcium (Ca), copper (Cu), and potassium (K) were evaluated. Propolis was harvested from 25 beehives by scraping or by means of propolis collectors (screen, “intelligent” collector propolis [ICP], lateral opening of the super [LOS], and underlay method). During the one-year study, the propolis produced was harvested each month, ground, homogenized, and stored in a freezer at -10 ºC. Seasonal analyses of the mineral composition were carried out by atomic absorption spectrophotometry and the results were evaluated by analysis of variance (ANOVA), followed by Tukey-Kramer’s test to compare the mean values (p<0.05). The results showed that seasonal variations influence the contents of 5 minerals (Mg, Fe, Na, Ca, and Cu), and the propolis harvesting method affects the contents of 4 minerals (Mg, Zn, Fe, and Ca).

PHARMACOKINETICS OF EN0XAPARIN AFTER SINGLE SUBCUTANEOUS ADMINISTRATION OF INCREASING DOSES (20 UP TO 80 MG) TO HEALTHY VOLUNTEERS

1987 ◽  
Author(s):  
L Bara ◽  
Y Le Roux ◽  
M Woler ◽  
F Chauliac ◽  
A Frydman ◽  
...  
Keyword(s):  
Subcutaneous Administration ◽  
Apparent Volume ◽  
Volume Of Distribution ◽  
Thrombin Time ◽  
Mean Values ◽  
Elimination Half ◽  
Heparin Plasma ◽  
The Mean ◽  
The One ◽  
Apparent Volume Of Distribution

The pharmacokinetics of enoxaparin (E) was randomly studied in 12 healthy male volunteers. Each dose (20-40-60 and 80 mg) was injected via subcutaneous (sc) route with a one-week wash out period. Anti-Xa and anti-IIa activities (ACT), calcium thrombin time (CTT) and Heptest were measured over a 36 hour period. E and the IV th International Heparin Standard were both used as internal standards.The anti IIa and CTT effects were only measurable when the injected dose was higher than 40 mg. The maximum anti-Xa and anti-IIa ACT were obtained 3 to 4 hours after the dose. As anti-IIa ACT is lower than anti-Xa ACT (anti-Xa/anti-IIa ACT ration I .6 to 2), the complete pharmacokinetic description of E was only based on anti-Xa data. Thus, the mean values of the maximal anti-Xa ACT (A max) were respectively: 1.58 ± 0.35 pg/ml; 3.83 ± 0.98 jig/ml, 5.38 ± 0.75 ug/ml and 7.44 ± 1.4 pg/ml for the four doses (20-40-60 and 80 mg). The resorption of E after sc injection was strictly linear whereas the relationships between A max or AUC in the one hand and dose in the other hand were A (anti Xa) Max = 0.0954 (dose) - 0,2083 r = 0.9146/p < 0.001; n = 48) and AUC (0 - 36 h) = 0.9117 (dose) - 7.59 (r = 0.9133/p < 0.001; n = 48). The mean residence time of E was close to 6 h (5.83 ± 0.86 h for D = 40 mg; 6.19 ± 0.74 h for D = 60 mg and 6.44 ± 0.76 h for 80 mg) indicating that around 50% of the total anti Xa ACT is induced in a 6 hour interval. The apparent volume of distribution V is close to 61 (6.59 1 ±1.33 1 for D = 60 mg) and the total Dody clearance is equal to 1.25 1/h, indicating the rate of depolymerisation of enoxaparin is lower than that of heparin. Plasma elimination half-life of anti-Xa ACT is equal to 4.36 ± 1.07 h (D = 40 mg) whereas that of anti-IIa ACT is shorter, fi) = 2.1 h). These results indicate that enoxaparin exhibits i) a differential anti-Xa/anti-IIa ACT profile, ii) a linear relationship between dose and anti-Xa/anti-IIa ACT and iii) a kinetic profile which is significantly different from that of standard heparin.

scholarly journals Study of Factors Influencing the Risk and their Relation to Credibility Theory

1977 ◽  
Vol 9 (1-2) ◽  
pp. 84-104 ◽  
Author(s):  
Maria Amélia Cabral ◽  
Jorge Afonso Garcia
Keyword(s):  
Least Squares Method ◽  
A Priori ◽  
Mean Value ◽  
The Other ◽  
Credibility Theory ◽  
Mean Values ◽  
Factors Influencing ◽  
The Mean ◽  
The One ◽  
Different Characteristics

The study and analysis of the various factors influencing insurance risks constitutes an intricate and usually quite extensive problem. We have to consider on the one hand the nature and heterogeneity of the elements we have been able to measure, and on the other the problem of deciding—without knowing exactly what results to expect—on the types of analysis to carry out and the form in which to present the results.These difficulties, essentially stemming from the fact that we cannot easily define “a priori” a measure of influence, can be overcome only by using highly sophisticated mathematical models. The researcher must define his objectives clearly if he is to avoid spending too much of his time in exploring such models.Either for these reasons or for lack of our experience in this field we were led to the study of three models, presenting entirely different characteristics though based on the analysis and behaviour of mean value fluctuations, measured by their variances or by the least-squares method.Our first model, described in II. 1, associates the notion of influence with the notion of variance. It analyses in detail the alteration of the mean values variance, when what we refer to as a “margination” is executed in the parameter space, taking each of the parameters in turn. We start off by having n distinct parameters, reducing them by one with each step.

scholarly journals Q beta and Q gamma components of intramembranous charge movement in frog cut twitch fibers.

1991 ◽  
Vol 98 (3) ◽  
pp. 429-464 ◽  
Author(s):  
C S Hui ◽  
W K Chandler
Keyword(s):  
Boltzmann Distribution ◽  
Active State ◽  
Charge Movement ◽  
Mean Values ◽  
Pulse Charge ◽  
Boltzmann Function ◽  
Voltage Dependent ◽  
The Mean ◽  
The Difference ◽  
The One

Intramembranous charge movement was measured in frog cut twitch fibers mounted in a double Vaseline-gap chamber with a TEA.Cl solution at 13-14 degrees C in the central pool. When a fiber was depolarized from a holding potential of -90 mV to a potential near -60 mV, the current from intramembranous charge movement was outward in direction and had an early, rapid component and a late, more slowly developing component, referred to as I beta and I gamma, respectively (1979. J. Physiol. [Lond.]. 289:83-97). When the pulse to -60 mV was preceded by a 100-600-ms pulse to -40 mV, early I beta and late I gamma components were also observed, but in the inward direction. The shape of the Q gamma vs. voltage curve can be estimated with this two-pulse protocol. The first pulse to voltage V allows the amounts of Q beta and Q gamma charge in the active state to change from their respective resting levels, Q beta (-90) and Q gamma (-90), to new steady levels, Q beta (V) and Q gamma (V). A second 100-120-ms pulse, usually to -60 mV, allows the amount of Q beta charge in the active state to change from Q beta (V) to Q beta (-60) but is not sufficiently long for the amount of Q gamma charge to change completely from Q gamma (V) to Q gamma (-60). The difference between the amount of Q gamma charge at the end of the second pulse and Q gamma (-60) is estimated from the OFF charge that is observed on repolarization to -90 mV. The OFF charge vs. voltage data were fitted, with gap corrections, with a Boltzmann distribution function plus a constant. The mean values of V (the potential at which, in the steady state, charge is distributed equally between the resting and active states) and k (the voltage dependence factor) were -59.2 mV (SEM, 1.1 mV) and 1.2 mV (SEM, 0.6 mV), respectively. The one-pulse charge vs. voltage data from the same fibers were fitted with a sum of two Boltzmann functions (1990. J. Gen. Physiol. 96:257-297). The mean values of V and k for the steeply voltage-dependent Boltzmann function, which is likely to be associated with the Q gamma component of charge, were -55.3 mV (SEM, 1.3 mV) and 3.3 mV (SEM, 0.6 mV), respectively, similar to the corresponding values obtained with the two-pulse protocol.(ABSTRACT TRUNCATED AT 400 WORDS)

scholarly journals Airpolishing effect on bovine enamel and the posterior remineralizing effect of saliva: estudo in vitro

2006 ◽  
Vol 14 (3) ◽  
pp. 193-197
Author(s):  
Helena Zaramella Vono Ribeiro ◽  
José Eduardo de Oliveira Lima ◽  
Bernardo Gonzalez Vono ◽  
Maria Aparcida de Andrade Moreira Machado ◽  
Salete Moura Bonifácio da Silva
Keyword(s):  
Sodium Bicarbonate ◽  
Artificial Saliva ◽  
Mean Value ◽  
Surface Microhardness ◽  
Mean Values ◽  
The Mean ◽  
Repairing Effect ◽  
The One ◽  
Bovine Enamel

PURPOSE: The aim of the present study was to evaluate the alterations of surface microhardness and wear caused by the sodium bicarbonate jet on bovine enamel and the further remineralizing effect of artificial saliva. METHODS: Fifteen enamel samples (4,0mm x 4,0mm) were used, which constituted the groups: no treatment (MI); treatment with sodium bicarbonate jet (MII and DI); treatment with sodium bicarbonate jet and immersion in saliva for one hour (MIII and DII), 24 hours (MIV and DIII) and 7 days (MV and DIV). Microhardness tests were carried out using a microdurometer in groups M and wear tests by a rugosimeter in groups D. The data were assessed by the one criterion variance analysis and Tukey test. RESULTS: The mean value of microhardness, in KHN, in groups MI, MII, MIII, MIV and MV were 359,80; 335,46; 369,20; 377,73 and 341,86, respectively, whereas the mean values in µm, of wear for group DI, DII, DIII and DIV were 0,564; 0,519; 0,441 and 0,428, respectively. CONCLUSIONS: The sodium bicarbonate jet caused a wear and a reduction in microhardness on the enamel surface; saliva promoted the recovery of initial condition surface microhardness and reduced the wear; the repairing effect of saliva on the surface microhardness alterations occurred within one hour of treatment, having no significant statistical difference from the effect obtained in 24 hours; the best saliva repairing effect on the wear occurred with treatment of 24 hours.

Redistribution of soil water after infiltration

Soil Research ◽  
1971 ◽  
Vol 9 (2) ◽  
pp. 59 ◽  
Author(s):  
AJ Peck
Keyword(s):  
Moisture Content ◽  
Surface Zone ◽  
Order Ordinary Differential Equation ◽  
Mean Values ◽  
Wide Range ◽  
Two Factors ◽  
Homogeneous Soil ◽  
The Mean ◽  
The One ◽  
Different Soils

The one-dimensional vertical redistribution of water is studied following infiltration into deep homogeneous soil with an initially uniform moisture content. There is assumed to be no loss of water by evaporation or transpiration during the redistribution. Assuming two factors to be constants, a first-order ordinary differential equation is derived which can be integrated numerically to compute the mean moisture content in the surface zone of draining soil as a function of the redistribution time. The depth of the draining zone increases with time, and this can be calculated too. That these factors are relatively constant is indicated by analysis of data for several soils and wetting depths over a wide range of redistribution times. Using mean values of the factors for several soils, and only wetting values of the diffusivity and conductivity functions, predicted redistribution behaviour agrees well with experimental data in four of six soils. In the remaining cases calculation of the factors for the particular soils, using an approximate method which includes hysteresis data, gives better results. The model is applied to predict the redistribution behaviour of different soils under identical treatments, and of a single soil for various infiltration quantities and initial moisture contents.

The fine structure of atmospheric turbulence in relation to the propagation of sound over the ground

1950 ◽  
Vol 203 (1073) ◽  
pp. 149-164 ◽  
Keyword(s):  
Background Noise ◽  
Sound Intensity ◽  
The Other ◽  
Hot Wire ◽  
Velocity Fluctuations ◽  
Simultaneous Measurements ◽  
The Mean ◽  
The One ◽  
Made In ◽  
Phase Relationships

With the aid of hot-wire instruments, measurements have been made of the fluctuations of the wind in the lowest 50 ft. of the atmosphere and, in particular, of the mean eddy diameter and of the ratio of vertical and cross-wind components in such fluctuations. It appears that the turbulent elements near the ground are smaller in size and more nearly isotropic in character than those higher up. Some correlation between the temperature and velocity fluctuations near the ground has been observed. Simultaneous measurements of the fluctuations in sound intensity at a distance from a steady source and of the intervening gustiness have been made in order to discuss the relation between sound scattering and background noise, on the one hand, and the intensity and scale of the prevailing turbulence on the other. The effect of the latter on the phase relationships between the signals picked up at two points is also demonstrated.

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