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

Five 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 a discontinuous inspiratory elastic load (IEL) of approximately 10 cmH2O/l. 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 IEL. Compared with NL, the VE-VCO2 slope was depressed by IEL, more so in hypercapnic [-28.7 +/- 7.2 (SE) %] than in eucapnic exercise (-16.0 +/- 2.8%). The steady-state hypercapnic ventilatory response at rest was also markedly depressed (-32.1 +/- 11.2%). Occlusion pressure response was augmented in response to IEL during eucapnic exercise (88.7 +/- 13.3%) but not during CO2 inhalation at rest or during exercise. Breathing pattern characteristics were similar regardless of the type of stimulus input and the level of inspiratory load. Results are consistent with the notion that the control of VE and breathing pattern may both be influenced by a balance between the prevailing chemical drive and a propensity of the controller to reduce respiratory effort.     

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.     

Steady-state response of quadriplegic subjects to inspiratory resistive load

Normal subjects preserve tidal volume (VT) in the face of added inspiratory resistance by increasing maximal amplitude and duration of the rising phase of respiratory driving pressure (DP) and by changing the shape of this phase to one that is more concave to the time axis. To explore the possible role of chest wall afferents in mediating these responses, we determined averaged DP in eight quadriplegic subjects during steady-state unloaded breathing and while breathing through an inspiratory resistance (8.5 cmH2O X 1(-1) X s). As with normal subjects, quadriplegics preserved VT (loaded VT = 106% control) by utilizing all three mechanisms. However, prolongation of the inspiratory duration derived from the DP waveform (+22% vs. +42%) and shape response were significantly less in the quadriplegic subjects. Shape response was completely absent in subjects with C4 lesions. The results provide strong evidence that respiratory muscle spindles are responsible for shape response and that changes in afferent feedback from the chest wall play an important role in mediating inspiratory prolongation.     

Steady-state response of normal subjects to inspiratory resistive load

Tidal volume (VT) is usually preserved when conscious humans are made to breathe against an inspiratory resistance. To identify the neural changes responsible for VT compensation we calculated the respiratory driving pressure waveform during steady-state unloaded and loaded breathing (delta R = 8.5 cmH2O X 1(-1) X s) in eight conscious normal subjects. Driving pressure (DP) was calculated according to the method of Younes et al. (J. Appl. Physiol. 51: 963-989, 1981), which provides the equivalent of occlusion pressure at functional residual capacity throughout the breath. VT during resistance breathing was 108% of unloaded VT, as opposed to a predicted value of 82% of control in the absence of neural compensation. Compensation was accomplished through three changes in the DP waveform: 1) peak amplitude increased (+/- 23%), 2) the duration of the rising phase increased (+42%); and 3) the rising phase became more concave to the time axis. There were no changes in the relative decay rate of inspiratory pressure during expiration, in the shape of the declining phase of DP, or in end-expiratory lung volume.     

Model analysis of respiratory responses to inspiratory resistive loads

Based on experimental inspiratory driving pressure waveforms and active respiratory impedance data of anesthetized cats, we made model predictions of the factors that determine the immediate (first loaded breath) intrinsic (i.e., nonneural) tidal volume compensation to added inspiratory resistive loads. The time course of driving pressure (P) was given by P = atb, where a is the pressure at 1 s from onset of inspiration and represents the intensity of neuromuscular drive, t is time, and b is a dimensionless index of the shape of the driving pressure wave. For a given value of active respiratory impedance, tidal volume compensation to added resistive loads increases with increasing inspiratory duration and decreasing value of b but is independent of a. Model predictions of load compensation are compared to experimental results.     

Diaphragmatic perfusion heterogeneity during exercise with inspiratory resistive breathing

Regional distribution of diaphragmatic blood flow (Q; 15-microns-diam radionuclide-labeled microspheres) was studied in normal (n = 7) and laryngeal hemiplegic (LH; n = 7) ponies to determine whether the added stress of inspiratory resistive breathing during maximal exercise may cause 1) redistribution of diaphragmatic Q and 2) crural diaphragmatic Q to exceed that in maximally exercising normal ponies. LH-induced augmentation of already high exertional work of breathing resulted in diminished locomotor exercise capacity so that maximal exercise in LH ponies occurred at 25 km/h compared with 32 km/h for normal ponies. The costal and crural regions received similar Q in both groups at rest. However, exercise-induced increments in perfusion were significantly greater in the costal region of the diaphragm. At 25 km/h, costal diaphragmatic perfusion was 154 and 143% of the crural diaphragmatic Q in normal and LH ponies. At 32 km/h, Q in costal diaphragm of normal ponies was 136% of that in the crural region. Costal and crural diaphragmatic Q in LH ponies exercised at 25 km/h exceeded that for normal ponies but was similar to the latter during exercise at 32 km/h. Perfusion pressure for the three conditions was also similar. It is concluded that diaphragmatic perfusion heterogeneity in exercising ponies was preserved during the added stress of inspiratory resistive breathing. It was also demonstrated that vascular resistance in the crural and costal regions of the diaphragm in maximally exercised LH ponies remained similar to that in maximally exercising normal ponies.     

Effects of N2O narcosis on breathing and effort sensations during exercise and inspiratory resistive loading

Fothergill, D. M., and N. A. Carlson. Effects ofN₂O narcosis on breathing andeffort sensations during exercise and inspiratory resistive loading.J. Appl. Physiol. 81(4):1562-1571, 1996.The influence of nitrous oxide(N₂O) narcosis on the responses toexercise and inspiratory resistive loading was studied in thirteen maleUS Navy divers. Each diver performed an incremental bicycle exercisetest at 1 ATA to volitional exhaustion while breathing a 23%N₂O gas mixture and a nonnarcoticgas of the same PO₂, density, andviscosity. The same gas mixtures were used during four subsequent30-min steady-state submaximal exercise trials in which the subjectsbreathed the mixtures both with and without an inspiratory resistance(5.5 vs. 1.1 cmH₂O ^· s ^· l¹at 1 l/s). Throughout each test, subjective ratings of respiratory effort (RE), leg exertion, and narcosis were obtained with acategory-ratio scale. The level of narcosis was rated between slightand moderate for the N₂O mixturebut showed great individual variation. Perceived leg exertion and thetime to exhaustion were not significantly different with the twobreathing mixtures. Heart rate was unaffected by the gas mixture andinspiratory resistance at rest and during steady-state exercise but wassignificantly lower with the N₂O mixture during incremental exercise (P < 0.05). Despite significant increases in inspiratory occlusionpressure (13%; P < 0.05),esophageal pressure (12%; P < 0.001), expired minute ventilation (4%;P < 0.01), and the work rate ofbreathing (15%; P < 0.001) when the subjects breathed the N₂O mixture,RE during both steady-state and incremental exercise was 25% lowerwith the narcotic gas than with the nonnarcotic mixture(P < 0.05). We conclude that the narcotic-mediated changes in ventilation, heart rate, and RE induced by23% N₂O are not of sufficientmagnitude to influence exercise tolerance at surface pressure.Furthermore, the load-compensating respiratory reflexes responsible formaintaining ventilation during resistive breathing are not depressed byN₂O narcosis.

     

Effects of hypercapnia on Breuer-Hering threshold for inspiratory termination

The effects of CO2 concentration on the timing of inspiratory duration (TI) and expiratory duration (TE) and the responses to lung inflation were studied in decerebrate paralyzed cats. With lung volume held at functional residual capacity during the breath cycle, hypercapnia (fractional concentration of inspired CO2 = 0.04) caused variable changes in TI and significant increases in TE. To obtain the Breuer-Hering threshold relationship [tidal volume (VT) vs. TI] and the timing relationship between TE and the preceding TI (TE vs. TI), ramp inflations of various sizes were used to terminate inspiration at different times in the breath cycle. Hypercapnia caused the VT vs. TI curves to shift in an upward direction so that at higher lung volumes TI was lengthened. Also, the slope of the TE vs. TI relationship was increased. The results suggest that hypercapnia diminished the sensitivity of the Breuer-Hering reflex to the lung volume, thus allowing volume to increase with little effect on TI. In addition, TE appears to become more sensitive to changes in the preceding TI. A model is presented which provides a possible neural mechanism for these responses.     

Effects of hypercapnia on inspiratory and expiratory muscle activity during expiration

Persistence of inspiratory muscle activity during the early phase of expiratory airflow slows the rate of lung deflation, whereas heightened expiratory muscle activity produces the opposite effect. To examine the influence of increased chemoreceptor drive and the role of vagal afferent activity on these processes, the effects of progressive hypercapnia were evaluated in 12 anesthetized tracheotomized dogs before and after vagotomy. Postinspiratory activity of inspiratory muscles (PIIA) and the activity of expiratory muscles were studied. During resting breathing, the duration of PIIA correlated with the duration of inspiration but not with expiration. Parasternal intercostal PIIA was directly related to that of the diaphragm. Based on their PIIA, dogs could be divided into two groups: one with prolonged PIIA (mean 0.57 s) and the other with brief PIIA (mean 0.16 s). Hypercapnia caused progressive shortening of the PIIA in the dogs with prolonged PIIA during resting breathing. The electrical activity of the external oblique and internal intercostal muscles increased gradually during CO2 rebreathing in all dogs both pre- and postvagotomy. After vagotomy, abdominal activity continued to increase with hypercapnia but was less at all levels of PCO2. The internal intercostal response to hypercapnia was not affected by vagotomy. The combination of shorter PIIA and augmented expiratory activity with hypercapnia might, in addition to changes in lung recoil pressure and airway resistance, hasten exhalation.     

Effects of mechanical loading and hypercapnia on inspiratory muscle EMG.

The electromyograms of the diaphragm and an external intercostal muscle were analyzed to see if the effects of hypercapnia on inspiratory muscle electrical activity could be distinguished from those of mechanical loading and to determine whether changes in inspiratory muscle electrical activity were a sueful measure of CO2 response during mechanical loading. Anesthetized dogs were studied: 1) during progressive hypercapnia without mechanical loading, 2) during flow-resistive and elastic loading at constant PCO2, and 3) during progressive hypercapnia and mechanical loading. Both mechanical loading and hypercapnia increased total inspiratory diaphragmatic and intercostal muscle electrical activity. However, inspiratory duration was increased by mechanical loads but reduced by hypercapnia. Because of these changes in inspiratory duration, the average rate of diaphragmatic electrical activity remained unaffected by mechanical loading before and after vagotomy but was increased by hypercapnia. In contrast, both hypercapnia and mechanical loading increased the average rate of intercostal muscle electrical activity. There was a greater increase in both total and average rate of intercostal muscle electrical activity during hypercapnia in the presence of mechanical loading than during unloaded breathing. However, the change in total and average rate of diaphragmatic electrical activity with PCO2 was unaffected by added mechanical loads. These results suggest that diaphragmatic but not intercostal muscle electrical activity can be used as an index of CO2 response even during mechanical loading.     

Ventilatory control in hypercapnia and exercise: optimization hypothesis

A model of the respiratory control system incorporating both chemical and respiratory neuromechanical feedbacks is proposed to describe the steady-state ventilatory responses to CO2 inhalation and exercise. It is postulated that ventilatory output (VE) is set by the respiratory center to minimize a net operating cost representing the conflicting challenges of arterial chemical imbalance and respiratory-mechanical discomfort (intolerance of effort), given, respectively, by a quadratic function of arterial PCO2 and a logarithmic function of VE. In addition, the system is assumed to be mechanically limited at maximum VE (Vmax). The predicted responses in VE during moderate hypercapnia, exercise, and ventilatory loading closely mimic those normally observed, even though no separate signal unique to exercise is assumed. As a quantitative validation, the model yielded good fits to ventilatory response data obtained in eight healthy subjects during eucapnic and hypercapnic exercise; the predicted Vmax averaged approximately 77% of the maximum voluntary ventilation in all subjects. The results demonstrate the plausibility of the proposed optimization mechanism and suggest an important role for respiratory-mechanical factors in the control of VE.