Effect of frequency on perceived magnitude of added loads to breathing

Using open-magnitude scaling, six normal subjects estimated the perceived magnitude of a range of added elastic loads (20-76 cmH2O/l), applied for a sequence of five breaths, at frequencies varying from 5 to 26.4 breaths/min. Two experiments were performed. In the first, frequency was increased by a reduction in expiratory duration (TE), and the duty cycle (ratio of inspiratory duration to total breath duration, TI/TT) ranged between 0.10 and 0.52. The perceived magnitude psi increased significantly with the peak airway pressure (Pm) (P less than 0.0001) but did not reach conventional significance with frequency (fb) (P = 0.15): psi = K0Pm1.23fb0.07 (r = 0.911). However, the sensory magnitude increased significantly as the duty cycle increased (P less than 0.01), but when it was included, the magnitude decreased minimally with frequency (P less than 0.01): psi = K0Pm1.3fb-0.97 TI/TT1.14 (r = 0.92). In the second experiment the duty cycle (TI/TT) was kept constant [(0.43 +/- 0.008 (SE)] and frequency (5-26.4 breaths/min) increased at the expense of shortening both TI and TE. The perceived magnitude of the added elastances decreased with the increase in frequency. However, when the perceived magnitude was corrected for the duration of inspiration, which is known to increase the sensory magnitude, psi = K0Pm1.3TI0.56, the sensory magnitude increased significantly with frequency (P less than 0.001): psi/TI0.56 = K0Pm1.21fb0.28 (r = 0.773). The decrease in inspiratory duration had a greater quantitative effect decreasing sensory magnitude than frequency had on increasing the magnitude. The effect of increasing frequency is complex and depends on the simultaneous intensity, duration of inspiratory pressure, and the duty cycle.     

Effects of expiratory resistive loading on the sensation of dyspnea

To determine whether an increase in expiratory motor output accentuates the sensation of dyspnea (difficulty in breathing), the following experiments were undertaken. Ten normal subjects, in a series of 2-min trials, breathed freely (level I) or maintained a target tidal volume equal to (level II) or twice the control (level III) at a breathing frequency of 15/min (similar to the control frequency) with an inspiratory load, an expiratory load, and without loads under hyperoxic normocapnia. In tests at levels II and III, end-expiratory lung volume was maintained at functional residual capacity. A linear resistance of 25 cmH2O.1(-1).s was used for both inspiratory and expiratory loading; peak mouth pressure (Pm) was measured, and the intensity of dyspnea (psi) was assessed with a visual analog scale. The sensation of dyspnea increased significantly with the magnitude of expiratory Pm during expiratory loading (level II: Pm = 9.4 +/- 1.5 (SE) cmH2O, psi = 1.26 +/- 0.35; level III: Pm = 20.3 +/- 2.8 cmH2O, psi = 2.22 +/- 0.48) and with inspiratory Pm during inspiratory loading (level II: Pm = 9.7 +/- 1.2 cmH2O, psi = 1.35 +/- 0.38; level III: Pm = 23.9 +/- 3.0 cmH2O, psi = 2.69 +/- 0.60). However, at each level of breathing, neither the intensity of dyspnea nor the magnitude of peak Pm during loading was different between inspiratory and expiratory loading. The augmentation of dyspnea during expiratory loading was not explained simply by increases in inspiratory activity. The results indicate that heightened expiratory as well as inspiratory motor output causes comparable increases in the sensation of difficulty in breathing.     

Power spectra of inspiratory nerve activity with lung inflations in cats

To investigate the effect of lung inflations on the high-frequency synchrony (70-122 Hz) observed in the inspiratory activity of respiratory motor nerves of decerebrate cats, I applied a step increase in lung inflation pressure at fixed delays into the inspiratory phase and computed power spectra of phrenic neurograms before and during inflation. In 25 decerebrate paralyzed cats the frequency of the high spectral peak was 92.3 +/- 11.1 Hz before and 105.3 +/- 12.1 Hz during the step in inflation pressure, shifting upward by 13.0 +/- 6.0 Hz. For 8 of the 25 cats, the recurrent laryngeal and phrenic neurograms were recorded simultaneously. The high spectral peak was present during inspiration in the recurrent laryngeal power spectra and coherent with the high peak in the phrenic power spectra. In response to lung inflation, the high peak disappeared from the power spectra of the recurrent laryngeal nerve as the inspiratory activity was inhibited; a shift upward in frequency was not detectable. Comparing inspiratory times (TI, based on the phrenic neurograms) for breaths with no lung inflations to those for breaths with lung inflations, I found that lung inflations early in inspiration caused a decrease in TI, lung inflations at intermediates times had no effect on TI, and lung inflations late in inspiration caused an increase in TI. Despite lung inflation decreasing, not affecting, or increasing inspiratory duration and amplitude of the phrenic neurogram, lung inflation always caused a shift upward in the high-frequency peak of the phrenic power density. The fact that lung inflation, a powerful respiratory stimulus, affected the frequency of the high peak in a consistent manner suggests that the high-frequency synchrony is an important and robust feature of the central respiratory pattern generator.     

Inspiratory muscle forces and endurance in maximum resistive loading

The ability of the respiratory muscles to sustain ventilation against increasing inspiratory resistive loads was measured in 10 normal subjects. All subjects reached a maximum rating of perceived respiratory effort and at maximum resistance showed signs of respiratory failure (CO2 retention, O2 desaturation, and rib cage and abdominal paradox). The maximum resistance achieved varied widely (range 73-660 cmH2O X l-1 X s). The increase in O2 uptake (delta Vo2) associated with loading was linearly related to the integrated mouth pressure (IMP): delta Vo2 = 0.028 X IMP + 19 ml/min (r = 0.88, P less than 0.001). Maximum delta Vo2 was 142 ml/min +/- SD 68 ml/min. There were significant (P less than 0.05) relationships between the maximum voluntary inspiratory pressure against an occluded airway (MIP) and both maximum IMP (r = 0.80) and maximum delta Vo2 (r = 0.76). In five subjects, three imposed breathing patterns were used to examine the effect of different patterns of respiratory muscle force deployment. Increasing inspiratory duration (TI) from 1.5 to 3.0 and 6.0 s, at the same frequency of breathing (5.5 breaths/min) reduced peak inspiratory pressure and increased the maximum resistance tolerated (190, 269, and 366 cmH2O X l-1 X s, respectively) and maximum IMP (2043, 2473, and 2913 cmH2O X s X min-1, but the effect on maximum delta Vo2 was less consistent (166, 237, and 180 ml/min). The ventilatory endurance capacity and the maximum O2 uptake of the respiratory muscles are related to the strength of the inspiratory muscles, but are also modified through the pattern of force deployment.     

Effects of almitrine on respiration in unanesthetized newborn rabbits

We previously demonstrated that almitrine, a peripheral chemoreceptor stimulant, increased tidal volume (VT), expired minute ventilation (VE), and respiratory frequency (f) and decreased inspiratory (TI) and expiratory time (TE) in sleeping adult cats. We now hypothesized that almitrine would induce an increase in ventilation in a young animal model. Respiration was studied by the barometric method in 11 unanesthetized New Zealand White rabbit pups between 3 and 6 days of age. Recordings were made in 0.21 FIO2 at base line and after cumulative intraperitoneal infusions of almitrine (2.5, 5.0, and 7.5 mg/kg). The chamber pressure deflection (proportional to VT after appropriate calculation) was computer sampled at 200 Hz. At least 100 breaths for each dose in each animal were analyzed. We found that a 7.5-mg/kg intraperitoneal dose of almitrine increased f to 135 +/- 9% (SE) of base line and decreased TE and TI to 72 +/- 8% and 79 +/- 8% of base line, respectively. Changes in VE, VT/TI, and VT were not significant. Recognizing that apnea is associated with inadequate ventilation and a prolonged TE (failure of the "inspiratory on-switch"), these results, particularly the increase in f and decrease in TE, suggest that almitrine might be useful in treating apnea in preterm infants.     

Effect of expiratory loading on glottic dimensions in humans

We examined the effects of external mechanical loading on glottic dimensions in 13 normal subjects. When flow-resistive loads of 7, 27, and 48 cmH2O X l-1 X s, measured at 0.2 l/s, were applied during expiration, glottic width at the mid-tidal volume point in expiration (dge) was 2.3 +/- 12, 37.9 +/- 7.5, and 38.3 +/- 8.9% (means +/- SE) less than the control dge, respectively. Simultaneously, mouth pressure (Pm) increased by 2.5 +/- 4, 3.0 +/- 0.4, and 4.6 +/- 0.6 cmH2O, respectively. When subjects were switched from a resistance to a positive end-expiratory pressure at comparable values of Pm, both dge and expiratory flow returned to control values, whereas the level of hyperinflation remained constant. Glottic width during inspiration (unloaded) did not change on any of the resistive loads. There was a slight inverse relationship between the ratio of expiratory to inspiratory glottic width and the ratio of expiratory to inspiratory duration. Our results show noncompensatory glottic narrowing when subjects breathe against an expiratory resistance and suggest that the glottic dimensions are influenced by the time course of lung emptying during expiration. We speculate that the glottic constriction is related to the increased activity of expiratory medullary neurons during loaded expiration and, by increasing the internal impedance of the respiratory system, may have a stabilizing function.     

Effects of inspiratory resistive load on respiratory control in hypercapnia and exercise

Eight healthy young men underwent two separate steady-state incremental exercise runs within the aerobic range on a treadmill with alternating periods of breathing with no load (NL) and with an inspiratory resistive load (IRL) of approximately 12 cmH2O.1-1.s. End-tidal PCO2 was maintained constant throughout each run at the eucapnic or a constant hypercapnic level by adding 0-5% CO2 to the inspired O2. Hypercapnia caused a steepening, as well as upward shift, relative to the corresponding eucapnic ventilation-CO2 output (VE - VCO2) relationship in NL and IRL. Compared with NL, the VE - VCO2 slope was depressed by IRL, more so in hypercapnic [-19.0 +/- 3.4 (SE) %] than in eucapnic exercise (-6.0 +/- 2.0%), despite a similar increase in the slope of the occlusion pressure at 100 ms - VCO2 (P100 - VCO2) relationship under both conditions. The steady-state hypercapnic ventilatory response at rest was markedly depressed by IRL (-22.6 +/- 7.5%), with little increase in P100 response. For a given inspiratory load, breathing pattern responses to separate or combined hypercapnia and exercise were similar. During IRL, VE was achieved by a greater tidal volume (VT) and inspiratory duty cycle (TI/TT) along with a lower mean inspiratory flow (VT/TI). The increase in TI/TT was solely because of a prolongation of inspiratory time (TI) with little change in expiratory duration for any given VT. The ventilatory and breathing pattern responses to IRL during CO2 inhalation and exercise are in favor of conservation of respiratory work.(ABSTRACT TRUNCATED AT 250 WORDS)     

Respiratory load compensation in neuromuscular disorders

First-breath ventilatory responses to graded elastic (delta E) and resistive (delta R) loads from 10 people with spinal muscular atrophy (SMA), 15 people with Duchenne muscular dystrophy (DMD), and 80 able-bodied people were compared. The SMA and DMD groups produced equal tidal volume, respiratory frequency, inspiratory duration (TI), expiratory duration, mean inspiratory airflow, and duty cycle responses to both delta E and delta R. Thus SMA (primarily a motoneuron disorder) and DMD (primarily a muscle disorder) have the same net effect on loaded breathing responses. The SMA and DMD groups failed to duplicate the normal group's short expirations during delta E, long inspirations during delta R, and thus, extended duty cycles during both delta E and delta R. The deficit in load compensation therefore was due to impaired regulation of respiratory timing (reflecting neural mechanisms) but not airflow defense (reflecting mechanical and neural mechanisms). One-fifth of the normal but none of the SMA or DMD subjects actively generated an "optimal" TI response (defined theoretically as TI greater than 160% control during large delta R and TI less than 75% control during large delta E). This lack of optimal responses, which is the same abnormality exhibited by quadriplegic people, suggests that SMA and DMD also impair human ability to discriminate between large delta R and delta E. These findings support the hypothesis that neuromuscular disorders can lead to disturbances in respiratory perception.     

Effect of inspiratory resistive loading on control of ventilation during progressive exercise

Eight healthy volunteers performed gradational tests to exhaustion on a mechanically braked cycle ergometer, with and without the addition of an inspiratory resistive load. Mean slopes for linear ventilatory responses during loaded and unloaded exercise [change in minute ventilation per change in CO2 output (delta VE/delta VCO2)] measured below the anaerobic threshold were 24.1 +/- 1.3 (SE) = l/l of CO2 and 26.2 +/- 1.0 l/l of CO2, respectively (P greater than 0.10). During loaded exercise, decrements in VE, tidal volume, respiratory frequency, arterial O2 saturation, and increases in end-tidal CO2 tension were observed only when work loads exceeded 65% of the unloaded maximum. There was a significant correlation between the resting ventilatory response to hypercapnia delta VE/delta PCO2 and the ventilatory response to VCO2 during exercise (delta VE/delta VCO2; r = 0.88; P less than 0.05). The maximal inspiratory pressure generated during loading correlated with CO2 sensitivity at rest (r = 0.91; P less than 0.05) and with exercise ventilation (delta VE/delta VCO2; r = 0.83; P less than 0.05). Although resistive loading did not alter O2 uptake (VO2) or heart rate (HR) as a function of work load, maximal VO2, HR, and exercise tolerance were decreased to 90% of control values. We conclude that a modest inspiratory resistive load reduces maximum exercise capacity and that CO2 responsiveness may play a role in the control of breathing during exercise when airway resistance is artificially increased.     

Effects of changes in inspiratory muscle strength on the sensation of respiratory force

The sensation of respiratory muscle force was compared in seven normal subjects before and after inspiratory muscle strength training. Subjects performed 20 sustained maximal inspiratory maneuvers daily for 6-18 wk. Maximal inspiratory pressures (MIP) increased from 124 +/- 10 to 187 +/- 9 (SE) cmH2O (P less than 0.005). Exponents of the power function relationships between mouth pressure (Pm) and the intensity of the sensation of force, corrected for inspiratory duration, during magnitude scaling of resistive and elastic ventilatory loads were the same before and after training (P greater than 0.05). However, absolute sensation intensity (S) during resistive and elastic loading was reduced significantly after strength training but returned toward baseline levels greater than or equal to 8 wk after the cessation of training when the MIP had fallen to 150 +/- 5 cmH2O. The absolute S at a given Pm during ventilatory loading changed inversely with changes in MIP (P less than 0.001). Furthermore the relationship between absolute S and Pm expressed as a proportion of the MIP (Pm/MIP) was constant over testing periods. These results suggest that the sensation of respiratory muscle force reflects the proportion of the maximum force utilized in breathing and may be based on the level of respiratory motor command signals.     

Steady-state response of normal subjects to an inspiratory sinusoidal pressure load

Inspiratory duration (TI) increases during inspiratory resistive loading in conscious humans. To ascertain whether this response is related to the temporal pattern of pressure perturbation (reaching a peak in early or midinspiration and declining subsequently) we compared the response of nine normal subjects to a usual resistor (narrow tube, RES) with their response when mouth pressure was reduced in a sinusoidal fashion during inspiration (SIN). Whereas the negative pressure pattern was similar with both loads (peak negative pressure near midinspiration), there was no relation between pressure and flow in the case of sinusoidal loading. Each experiment consisted of two loading periods, 4 min each, and three unloaded periods, also 4 min each, bracketing the periods of loading. The order of RES and SIN was randomized. TI during loading was compared with the average TI of the preceding and following unloaded periods. TI increased 0.74 +/- 0.12 and 0.27 +/- 0.05 (SE) s during RES and SIN, respectively (P less than 0.01). We conclude that the temporal pattern of pressure change during resistance breathing plays a small role in mediating the TI prolongation. Coupling between flow and the pressure perturbation appears to be an important determinant of TI prolongation.     

Relationship between inspiratory effort and breathlessness in pregnancy.

Using open-magnitude scaling, we compared the relationships between breathlessness, inspiratory esophageal pressure swing (delta Pes), and ventilation in pregnancy and postpartum. Thirteen healthy women performed progressive cycle exercise tests at 33 +/- 2 wk gestation and 12 +/- 3 wk postpartum. Pulmonary function and maximal transdiaphragmatic pressure did not change. Minute ventilation (VE) was greater in the third trimester. This increase was entirely due to the increase in tidal volume (VT; 0.74 +/- 0.18 vs. 0.54 +/- 0.18 liters at rest, P less than 0.01; 1.56 +/- 0.3 vs. 1.24 +/- 0.24 liters at 48 W, P less than 0.001). delta Pes (15.3 +/- 3.0 vs. 11.9 +/- 3.5 cmH2O at 48 W, P less than 0.01) and breathlessness (1.8 +/- 1.4 vs. 1.0 +/- 0.9 at 48 W, P less than 0.05) were greater in the third trimester. However, the relationships between VT and delta Pes and between delta Pes and breathlessness were identical in the two conditions. The VT-tidal abdominal volume (Vab) and Vab-tidal gastric pressure swing (delta Pga) relationships were similar in the two conditions. In conclusion, the relationship between delta Pes and breathlessness is the same in the third trimester and postpartum. The increased VE is responsible for the breathlessness in the third trimester. Despite progressive abdominal distension by the gravid uterus, the VT-Vab and Vab-delta Pga relationships were the same in the two conditions.     

Effect of inspiratory muscle fatigue on perception of effort during loaded breathing

The present study examined the relationship between the intensity of the sense of effort during inspiratory threshold loading and the severity of inspiratory muscle fatigue. Studies were performed on normal subjects in whom the magnitude of airway pressure developed (Pm) and the duty cycle of breathing (TI/TT) were constrained to achieve a pressure-time integral (i.e., Pm/Pmax X TI/TT) 24% of maximum. In separate trials, the same pressure-time index (24%) was achieved using two widely different patterns of pressure magnitude and duty cycle to allow the effects of changes in the pattern of inspiratory muscle contraction on sensation and fatigue to be assessed. The intensity of the sense of effort was assessed using a category (Borg) scale. The severity of inspiratory muscle fatigue was assessed both from changes in the centroid frequency of the diaphragm electromyogram and from changes in the maximum static inspiratory pressure. Loaded breathing produced inspiratory muscle fatigue and a progressive increase in the sense of effort over time in all subjects. The rate at which the inspiratory muscles fatigued was the same with the two patterns of loading. In contrast, the rate of growth in the intensity of the sense of effort varied significantly as a function of the pattern of loaded breathing. The sense of effort increased at a faster rate with the high pressure-short duty cycle pattern of contraction as compared with the low pressure-long duty cycle pattern. As a result, the intensity of the sense of effort was not uniquely related to the severity of inspiratory muscle fatigue.(ABSTRACT TRUNCATED AT 250 WORDS)     

Sleep and maturation of eucapnic ventilation and CO2 sensitivity in the premature primate

The effects of sleep state and postnatal maturation on steady-state CO2 sensitivity, "inspiratory drive" (VT/TI), and the inspiratory "duty cycle" (TI/Ttot) were examined in nine unanesthetized premature Macaca nemestrina in the first 3 wk of life. Minute volume (VE) in room air was less in NREM sleep than in the awake state but there were no differences in VE, VT/TI, or TI/Ttot between REM and NREM sleep. VE and VT/TI corrected for body weight increased in REM and NREM sleep with postnatal maturation whereas TI/Ttot did not vary. Concomitant with this increase in room air VE and VT/TI, an increase in CO2 sensitivity (delta V/delta Paco2) with postnatal maturation was documented in NREM sleep. CO2 sensitivity was similar between REM and NREM states at each postnatal age. The increase in VE following inhalation of 2-5% CO2 was mediated by an increase in VT/TI, whereas TI/Ttot remained constant. The differences in the effect of sleep on CO2 sensitivity between neonates and adults are discussed and possible mechanisms for the observed developmental increase in CO2 sensitivity are proposed.     

Electrically evoked isometric and isokinetic properties of the triceps surae in young male subjects

The relationship between electrically evoked isometric and isokinetic properties of the triceps surae have been studied in 11 healthy male subjects. The results showed that the time to peak tension (TPT) and half relaxation time (1/2 RT) of the maximal twitch were 110 +/- 11 ms and 82 +/- 11 ms respectively, and the peak rates of rise of contraction (delta P50, delta P200) and relaxation (delta PR50, delta PR200) at 50 and 200 Hz were 0.36 +/- 0.07, 0.48 +/- 0.08 and 1.27 +/- 0.33, 1.25 +/- 0.27% Po ms-1 respectively. The decline in force during a fatigue test was significantly (P less than 0.02) associated with the decrease in maximal relaxation rate (r = 0.79). The TPT was significantly (P less than 0.05) and inversely related to delta P50 and delta P200. The mean angle specific torque-velocity relationship for the 11 subjects was adequately described by the empirical exponential equation of the form: V = 16.5 (e-P/30.8-e-84.3/30.8) where V = velocity (rads s-1) and P = torque (Nm). The only significant association found between the isometric and isokinetic properties of the muscle was between delta PR200 and the torque expressed at a given velocity of 4 rads s-1. This lack of association between the two variables is difficult to explain with certainty but it is suggested that it may be due to the differential effects of Ca2+ release and uptake and cross-bridge turnover rate in the two situations.     

Hyperoxia and moderate hypoxia fail to affect inspiratory muscle fatigue in humans

Normal human subjects (n = 7) breathing 21% O2 (normoxia), 13% O2 (hypoxia), or 100% O2 (hyperoxia) performed repeated maximal inspiratory maneuvers (inspiratory duration = 1.5 s, total breath duration = 3.5 s) on an "isoflow" system, which delivered a constant mouth flow (1.25 or 1 l/s) while maintaining normocapnia (5.5% end-tidal CO2). Respective mean arterial O2 saturation values (ear lobe oximetry) were 98 +/- 1, 91 +/- 4 (P less than or equal to 0.01), and 99 +/- 1% (NS). Maximal mouth pressure (Pm) was measured during inspirations at rest and during a 10-min fatigue trial, and the Pm measurements obtained during the fatigue trials were fit to an exponential equation. The parameters of the equation included the time constant (tau), which describes the rate of decay of Pm from the initial pressure (Pi) to the asymptote, or "sustainable" pressure (Ps). The mean fraction of Pm remaining at the end of the fatigue trials (Ps/Pi) was 63 +/- 5%. No significant differences in Pi, Ps, or tau were observed between O2 treatments. This suggests that fatigue of the inspiratory muscles in normal humans occurs by a mechanism that is insensitive to changes in blood O2 content that occur during inspiration of O2 in the range of 13-100%.     

Stress adaptation and low-frequency impedance of rat lungs

At transpulmonary pressures (Ptp) of 7-12 cmH2O, pressure-volume hysteresis of isolated cat lungs has been found to be 20-50% larger than predicted from their amount of stress adaptation (J. Hildebrandt, J. Appl. Physiol. 28: 365-372, 1970). This behavior is inconsistent with linear viscoelasticity and has been interpreted in terms of plastoelasticity. We have reinvestigated this phenomenon in isolated lungs from 12 Wistar rats by measuring 1) the changes in Ptp after 0.5-ml step volume changes (initial Ptp of 5 cmH2O) and 2) their response to sinusoidal pressure forcing from 0.01 to 0.67 Hz (2 cmH2O peak to peak, mean Ptp of 6 cmH2O). Stress adaptation curves were found to fit approximately Hildebrandt's logarithmic model [delta Ptp/delta V = A - B.log(t)] from 0.2 to 100 s, where delta V is the step volume change, A and B are coefficients, and t is time. A and B averaged 1.06 +/- 0.11 and 0.173 +/- 0.019 cmH2O/ml, respectively, with minor differences between stress relaxation and stress recovery curves. The response to sinusoidal forcing was characterized by the effective resistance (Re) and elastance (EL). Re decreased from 2.48 +/- 0.41 cmH2O.ml-1.s at 0.01 Hz to 0.18 +/- 0.03 cmH2O.ml-1.s at 0.5 Hz, and EL increased from 0.99 +/- 0.10 to 1.26 +/- 0.20 cmH2O/ml on the same frequency range. These data were analyzed with the frequency-domain version of the same model, complemented by a Newtonian resistance (R) to account for airway resistance: Re = R + B/ (9.2f) and EL = A + 0.25B + B . log 2 pi f, where f is the frequency.(ABSTRACT TRUNCATED AT 250 WORDS)     

Dynamics of microvascular oxygen pressure in the rat diaphragm.

The relative amplitudes and rates of increase of muscle blood flow (and O(2) delivery) and O(2) uptake responses determine the O(2) pressure within the muscle microvasculature (Pm(O(2))) across the rest-to-contraction transition. Skeletal muscle function is a primary determinant of pulmonary O(2) uptake kinetics; however, it has never been determined whether the dynamics of muscle Pm(O(2)) are faster in a highly oxidative muscle [e.g., diaphragm (Dia), citrate synthase activity of 39 micromol. min(-1). g(-1)] compared with less oxidative muscles [e.g., spinotrapezius (Spino), citrate synthase activity of 14 micromol. min(-1). g(-1), male Sprague-Dawley rats; Delp MD and Duan C, J Appl Physiol 80: 261-270, 1996]. Phosphorescence quenching techniques (porphyrin dendrimer, R2) were used to determine Pm(O(2)) across the transition to electrically stimulated contractions (1 Hz) within the rat Dia. After a delay of 10.4 +/- 1.3 (SE) s at the beginning of Dia contractions, Pm(O(2)) decreased close to monoexponentially from 42 +/- 2 to 27 +/- 3 Torr (P < 0.05) with an extremely fast time constant of 7.1 +/- 1.1 s. Thus Dia Pm(O(2)) decreased with significantly (P < 0.05) faster kinetics than reported previously for the Spino muscle (delay, 19.2 +/- 2.8 s; time constant Pm(O(2)), 21.7 +/- 2.1 s; Behnke BJ, Kindig CA, Musch TI, Koga S, and Poole DC, Respir Physiol 126: 53-63, 2001). With the use of two specialized muscles with similar fiber-type composition but widely disparate oxidative capacities (Delp MD and Duan C, J Appl Physiol 80: 261-270, 1996), these data demonstrate that Pm(O(2)) kinetics are significantly faster in the highly oxidative Dia compared with the low-oxidative Spino muscle and that this effect is not dependent on muscle fiber-type composition.     

Ventilatory response to high-frequency airway oscillation in humans

To investigate respiratory control during high-frequency oscillation (HFO), ventilation was monitored in conscious humans by respiratory inductive plethysmography during application at the mouth of high-frequency pressure oscillations. Studies were conducted before and after airway and pharyngeal anesthesia. During HFO, breathing became slow and deep with an increase in tidal volume (VT) of 37% (P less than 0.01) and inspiratory duration (TI) of 34% (P less than 0.01). Timing ratio (TI/TT) increased 14% (P less than 0.05) and respiratory frequency (f) decreased 12% (P less than 0.01). Mean inspiratory flow (VT/TI) did not change during HFO. Following airway anesthesia, VT increased only 26% during HFO (P less than 0.01), whereas significant changes in TI, TI/TT, and f were not observed. Pharyngeal anesthesia failed to diminish the effect of HFO on TI, TT, or f, although the increase in VT was reduced. These results indicate that 1) HFO presented in this manner alters inspiratory timing without affecting the level of inspiratory activity, and 2) receptors in the larynx and/or lower airways may in part mediate the response.     

Effect of increased arterial CO2 on fetal breathing and behavior in sheep

We studied breathing and behavioral response to increased arterial CO2 (PaCO2) in 12 fetal sheep between 130 and 145 days of gestation. Of these 12 fetuses, 10 had an increase in PaCO2 through maternal rebreathing of CO2; in the other 2 fetuses CO2 was increased via an endotracheal tube and application of continuous distending airway pressure. We used our window technique to observe and videotape fetal behavior. The experiments consisted of recording breathing activity and behavior during resting conditions (1 low- and high-voltage ECoG cycle) and during administration of CO2. We measured electrocortical activity (ECoG), eye movements (EOG), electromyography of the diaphragm (EMGdi) and neck muscles, tracheal (Ptr), amniotic, and carotid arterial pressures. Administration of CO2 by the rebreathing technique produced an increase in the amplitude of breathing activity as reflected by an increase in Ptr from 5.0 +/- 0.6 to 12 +/- 1.9 mmHg (P less than 0.01) and an increase in SEMGdi from 32 +/- 4 to 77 +/- 8% max (P less than 0.001). Frequency increased due to a decrease in inspiratory (TI) and expiratory duration. Ptr/TI increased from 11.0 +/- 2.0 to 37.4 +/- 9.0 mmHg/s (P less than 0.05) and SEMGdi/TI increased from 67 +/- 7 to 221 +/- 28% max/s (P less than 0.001). Although the response was at times prolonged into the transitional high-voltage zone, it did not persist during established high-voltage ECoG.(ABSTRACT TRUNCATED AT 250 WORDS)