Quantitative analysis of transpleural flux in the isolated lung

Li, M. H., J. Hildebrandt, and M. P. Hlastala.Quantitative analysis of transpleural flux in the isolated lung.J. Appl. Physiol. 82(2): 545-551, 1997.In this study, the loss of inert gas through the pleura of anisolated ventilated and perfused rabbit lung was assessed theoreticallyand experimentally. A mathematical model was used to represent an idealhomogeneous lung placed within a box with gas flow(box) surrounding the lung. Thealveoli are assumed to be ventilated with room air(A) andperfused at constant flow () containinginert gases (x) with various perfusate-air partition coefficients(_p,x).The ratio of transpleural flux of gas(pl_x)to its total delivery to the lung via pulmonary artery( ),representing fractional losses across the pleura, can be shown todepend on four dimensionless ratios:1)_p,x,2) the ratio of alveolar ventilation to perfusion(A/), 3) the ratioof the pleural diffusing capacity(Dpl_x) to the conductance ofthe alveolar ventilation (Dpl_x /A_g,where _g is the capacitancecoefficient of gas), and 4) theratio of extrapleural (box) ventilation to alveolar ventilation(box/A).Experiments were performed in isolated perfused and ventilated rabbitlungs. The perfusate was a buffer solution containing six dissolvedinert gases covering the entire 10⁵-fold range of_p,x usedin the multiple inert gas elimination technique. Steady-state inert gasconcentrations were measured in the pulmonary arterial perfusate,pulmonary venous effluent, exhaled gas, and box effluent gas. Theexperimental data could be described satisfactorily by thesingle-compartment model. It is concluded that a simple theoreticalmodel is a useful tool for predicting transpleural flux from isolatedlung preparations, with known ventilation and perfusion, for inertgases within a wide range of .

     

Role for anions in pulmonary endothelial permeability

Griffin, M. Pamela. Role for anions in pulmonaryendothelial permeability. J. Appl.Physiol. 83(2): 615-622, 1997.-Adrenergic stimulation reduces albumin permeation across pulmonary artery endothelial monolayers and induces changes in cell morphology that aremediated by Cl flux. Wetested the hypothesis that anion-mediated changes in endothelial cellsresult in changes in endothelial permeability. We measured permeationof radiolabeled albumin across bovine pulmonary arterial endothelialmonolayers when the extracellular anion was Cl,Br,I,F, acetate(Ac), gluconate(G), and propionate(Pr). Permeability toalbumin (P_albumin)was calculated before and after addition of 0.2 mM of thephosphodiesterase inhibitor 3-isobutyl-1-methylxanthine (IBMX), whichreduces permeability. InCl, theP_albumin was 3.05 ± 0.86 × 10⁶ cm/s andfell by 70% with the addition of IBMX. The initialP_albumin was lowest forPr andAc. InitialP_albumin was higher inBr,I,G, andF than inCl. A permeability ratiowas calculated to examine the IBMX effect. The greatest IBMX effect wasseen when Cl was theextracellular anion, and the order among halide anions wasCl > Br > I > F. Although the level ofextracellular Ca²⁺ concentration([Ca²⁺]_o)varied over a wide range in the anion solutions,[Ca²⁺]_odid not systematically affect endothelial permeability in this system.When Cl was theextracellular anion, varying[Ca²⁺]_ofrom 0.2 to 2.8 mM caused a change in initialP_albumin but no changein the IBMX effect. The anion channel blockers4-acetamido-4-isothiocyanotostilbene-2,2-disulfonic acid(0.25 mM) and anthracene-9-carboxylic acid (0.5 mM) significantly altered initialP_albumin and the IBMXeffect. The anion transport blockers bumetanide (0.2 mM) and furosemide(1 mM) had no such effects. We conclude that extracellular anionsinfluence bovine pulmonary arterial endothelial permeability and thatthe pharmacological profile fits better with the activity of anionchannels than with other anion transport processes.

     

Influence of muscle fiber type and pedal frequency on oxygen uptake kinetics of heavy exercise

Barstow, Thomas J., Andrew M. Jones, Paul H. Nguyen, andRichard Casaburi. Influence of muscle fiber type and pedal frequency on oxygen uptake kinetics of heavy exercise.J. Appl. Physiol. 81(4):1642-1650, 1996.We tested the hypothesis that the amplitude ofthe additional slow component ofO₂ uptake(O₂) during heavy exerciseis correlated with the percentage of type II (fast-twitch) fibers inthe contracting muscles. Ten subjects performed transitions to a workrate calculated to require aO₂ equal to 50% betweenthe estimated lactate (Lac) threshold and maximalO₂ (50%).Nine subjects consented to a muscle biopsy of the vastus lateralis. Toenhance the influence of differences in fiber type among subjects,transitions were made while subjects were pedaling at 45, 60, 75, and90 rpm in different trials. Baseline O₂ was designed to besimilar at the different pedal rates by adjusting baseline work ratewhile the absolute increase in work rate above the baseline was thesame. The O₂ response after the onset of exercise was described by a three-exponential model. Therelative magnitude of the slow component at the end of 8-min exercisewas significantly negatively correlated with %type I fibers at everypedal rate (r = 0.64 to 0.83, P < 0.05-0.01). Furthermore,the gain of the fast component forO₂ (asml ^· min^{1 ·} W¹)was positively correlated with the %type I fibers across pedal rates(r = 0.69-0.83). Increase inpedal rate was associated with decreased relative stress of theexercise but did not affect the relationships between%fiber type and O₂parameters. The relative contribution of the slow component was alsosignificantly negatively correlated with maximalO₂(r = 0.65), whereas the gainfor the fast component was positively associated(r = 0.68-0.71 across rpm). Theamplitude of the slow component was significantly correlated with netend-exercise Lac at all four pedal rates(r = 0.64-0.84), but Lac was notcorrelated with %type I (P > 0.05).We conclude that fiber type distribution significantly affects both thefast and slow components ofO₂ during heavy exerciseand that fiber type and fitness may have both codependent andindependent influences on the metabolic and gas-exchange responses toheavy exercise.

     

Susceptibility to periodic breathing with assisted ventilation during sleep in normal subjects

Assisted ventilation with pressure support (PSV)or proportional assist (PAV) ventilation has the potential to produceperiodic breathing (PB) during sleep. We hypothesized that PB willdevelop when PSV level exceeds the product of spontaneous tidal volume (VT) and elastance(VT_sp · E)but that the actual level at which PB will develop[PSV(PB)] will be influenced by thePCO₂ (difference between eupneicPCO₂ andCO₂ apneic threshold) and by RR[response of respiratory rate (RR) to PSV]. We also wishedto determine the PAV level at which PB develops to assess inherentventilatory stability in normal subjects. Twelve normal subjectsunderwent polysomnography while connected to a PSV/PAV ventilatorprototype. Level of assist with either mode was increased in smallsteps (2-5 min each) until PB developed or the subject awakened.End-tidal PCO₂,VT, RR, and airway pressure (Paw) were continuously monitored, and the pressure generated byrespiratory muscle (Pmus) was calculated. The pressure amplification factor (PAF) at the highest PAV level was calculated from[(Paw + Pmus)/Pmus], where Paw is peak Paw  continuous positive airway pressure. PB with central apneas developedin 11 of 12 subjects on PSV. PCO₂ranged from 1.5 to 5.8 Torr. Changes in RR with PSV were small andbidirectional (+1.1 to 3.5min¹). With use ofstepwise regression, PSV(PB) was significantly correlated withVT_sp(P = 0.001), E(P = 0.00009),PCO₂ (P = 0.007), and RR(P = 0.006). The final regressionmodel was as follows: PSV(PB) = 11.1 VT_sp + 0.3E  0.4 PCO₂  0.34 RR  3.4 (r = 0.98). PBdeveloped in five subjects on PAV at amplification factors of1.5-3.4. It failed to occur in seven subjects, despite PAF of upto 7.6. We conclude that 1) aPCO₂ apneic threshold exists duringsleep at 1.5-5.8 Torr below eupneicPCO₂,2) the development of PB during PSVis entirely predictable during sleep, and3) the inherent susceptibility to PBvaries considerably among normal subjects.

     

Association of chest wall motion and tidal volume responses during CO2 rebreathing

Yan, Sheng, Pawel Sliwinski, and Peter T. Macklem.Association of chest wall motion and tidal volume responses during CO₂ rebreathing.J. Appl. Physiol. 81(4):1528-1534, 1996.The purpose of this study is to investigate theeffect of chest wall configuration at end expiration on tidal volume(VT) response duringCO₂ rebreathing. In a group of 11 healthy male subjects, the changes in end-expiratory andend-inspiratory volume of the rib cage (Vrc,E andVrc,I, respectively) and abdomen (Vab,E and Vab,I, respectively) measured by linearizedmagnetometers were expressed as a function of end-tidalPCO₂(PET_CO2). The changes inend-expiratory and end-inspiratory volumes of the chest wall(Vcw,E and Vcw,I,respectively) were calculated as the sum of the respectiverib cage and abdominal volumes. The magnetometer coils were placed atthe level of the nipples and 1-2 cm above the umbilicus andcalibrated during quiet breathing against theVT measured from apneumotachograph. TheVrc,E/PET_CO2 slope was quite variable among subjects. It was significantly positive (P < 0.05) in fivesubjects, significantly negative in four subjects(P < 0.05), and not different fromzero in the remaining two subjects. TheVab,E/PET_CO2slope was significantly negative in all subjects(P < 0.05) with a much smallerintersubject variation, probably suggesting a relatively more uniformrecruitment of abdominal expiratory muscles and a variable recruitmentof rib cage muscles during CO₂rebreathing in different subjects. As a group, the meanVrc,E/PET_CO2,Vab,E/PET_CO2, andVcw,E/PET_CO2slopes were 0.010 ± 0.034, 0.030 ± 0.007, and0.020 ± 0.032 l / Torr, respectively;only theVab,E/PET_CO2 slope was significantly different from zero. More interestingly, theindividualVT/PET_CO2slope was negatively associated with theVrc,E/PET_CO2(r = 0.68,P = 0.021) and Vcw,E/PET_CO2slopes (r = 0.63,P = 0.037) but was not associated withtheVab,E/PET_CO2slope (r = 0.40, P = 0.223). There was no correlation oftheVrc,E/PET_CO2 andVcw,E/PET_CO2slopes with age, body size, forced expiratory volume in 1 s, orexpiratory time. The groupVab,I/PET_CO2 slope (0.004 ± 0.014 l / Torr) was not significantlydifferent from zero despite theVT nearly being tripled at theend of CO₂ rebreathing. Inconclusion, the individual VTresponse to CO₂, althoughindependent of Vab,E, is a function ofVrc,E to the extent that as theVrc,E/PET_CO2slope increases (more positive) among subjects, theVT response toCO₂ decreases. These results maybe explained on the basis of the respiratory muscle actions andinteractions on the rib cage.

     

Tumor necrosis factor-alpha in ischemia and reperfusion injury in rat lungs

The effects ofboth recombinant rat tumor necrosis factor- (TNF-) and ananti-TNF- antibody were studied in isolated buffer-perfused ratlungs subjected to either 45 min of nonventilated[ischemia-reperfusion (I/R)] or air-ventilated(/R) ischemia followed by 90 min of reperfusion and ventilation. In the I/R group, the vascularpermeability, as measured by the filtration coefficient(K_fc),increased three- and fivefold above baseline after 30 and 90 min ofreperfusion, respectively (P < 0.001). Over the same time intervals, theK_fc for the/R group increased five- and tenfold above baseline values, respectively (P < 0.001).TNF- measured in the perfusates of both ischemic modelssignificantly increased after 30 min of reperfusion. Recombinant ratTNF- (50,000 U), placed into perfusate after baseline measurements,produced no measurable change in microvascular permeability in controllungs perfused over the same time period (135 min), but I/R injury wassignificantly enhanced in the presence of TNF-. An anti-TNF-antibody (10 mg/rat) injected intraperitoneally into rats 2 h beforethe lung was isolated prevented the microvascular damage in lungsexposed to both I/R and /R (P < 0.001). These results indicatethat TNF- is an essential component at the cascade of events thatcause lung endothelial injury in short-term I/R and/R models of lung ischemia.

     

Effects of respiratory muscle work on cardiac output and its distribution during maximal exercise

We have recently demonstrated that changes inthe work of breathing during maximal exercise affect leg blood flow andleg vascular conductance (C. A. Harms, M. A. Babcock, S. R. McClaran, D. F. Pegelow, G. A. Nickele, W. B. Nelson, and J. A. Dempsey. J. Appl. Physiol. 82: 1573-1583,1997). Our present study examined the effects of changesin the work of breathing on cardiac output (CO) during maximalexercise. Eight male cyclists [maximalO₂ consumption(O_{2 max}):62 ± 5 ml · kg¹ · min¹]performed repeated 2.5-min bouts of cycle exercise atO_{2 max}. Inspiratorymuscle work was either 1) at controllevels [inspiratory esophageal pressure (Pes): 27.8 ± 0.6 cmH₂O],2) reduced via a proportional-assistventilator (Pes: 16.3 ± 0.5 cmH₂O), or 3) increased via resistive loads(Pes: 35.6 ± 0.8 cmH₂O).O₂ contents measured in arterialand mixed venous blood were used to calculate CO via the direct Fickmethod. Stroke volume, CO, and pulmonaryO₂ consumption(O₂) were not different(P > 0.05) between control andloaded trials atO_{2 max} but were lower(8, 9, and 7%, respectively) than control withinspiratory muscle unloading atO_{2 max}. Thearterial-mixed venous O₂difference was unchanged with unloading or loading. We combined thesefindings with our recent study to show that the respiratory muscle work normally expended during maximal exercise has two significant effectson the cardiovascular system: 1) upto 14-16% of the CO is directed to the respiratory muscles; and2) local reflex vasoconstriction significantly compromises blood flow to leg locomotor muscles.

     

Human ventilatory response to 8h of euoxic hypercapnia

Tansley, John G., Michala E. F. Pedersen, Christine Clar,and Peter A. Robbins. Human ventilatory response to 8 h of euoxic hypercapnia. J. Appl.Physiol. 84(2): 431-434, 1998.Ventilation (E) risesthroughout 40 min of constant elevated end-tidalPCO₂ without reaching steady state(S. Khamnei and P. A. Robbins. Respir. Physiol. 81: 117-134, 1990). The present studyinvestigates 8 h of euoxic hypercapnia to determine whetherE reachessteady state within this time. Two protocols were employed:1) 8-h euoxic hypercapnia (end-tidalPCO₂ = 6.5 Torr above prestudy value,end-tidal PO₂ = 100 Torr) followed by 8-h poikilocapnic euoxia; and2) control, where the inspired gaswas air. Ewas measured over a 5-min period before the experiment and then hourly over a 16-h period. In the hypercapnia protocol,E had notreached a steady state by the first hour(P < 0.001, analysis of variance), but there were no further significant differences inEover hours 2-8 (analysis ofvariance). Efell promptly on return to eucapnic conditions. We conclude that,whereas there is a component of theE responseto hypercapnia that is slow, there is no progressive rise inE throughoutthe 8-h period.

     

Combined heart rate and activity improve estimates of oxygen consumption and carbon dioxide production rates

Moon, Jon K., and Nancy F. Butte. Combined heart rateand activity improve estimates of oxygen consumption and carbon dioxideproduction rates. J. Appl. Physiol.81(4): 1754-1761, 1996.Oxygen consumption(O₂) andcarbon dioxide production (CO₂) rates were measuredby electronically recording heart rate (HR) and physical activity (PA).Mean daily O₂ andCO₂ measurements by HR andPA were validated in adults (n = 10 women and 10 men) with room calorimeters. Thirteen linear and nonlinear functions of HR alone and HR combined with PA were tested as models of24-h O₂ andCO₂. Mean sleepO₂ andCO₂ were similar to basalmetabolic rates and were accurately estimated from HR alone[respective mean errors were 0.2 ± 0.8 (SD) and0.4 ± 0.6%]. The range of prediction errorsfor 24-h O₂ andCO₂ was smallestfor a model that used PA to assign HR for each minute to separateactive and inactive curves(O₂, 3.3 ± 3.5%; CO₂, 4.6 ± 3%). There were no significant correlations betweenO₂ orCO₂ errors and subject age,weight, fat mass, ratio of daily to basal energy expenditure rate, orfitness. O₂,CO₂, and energy expenditurerecorded for 3 free-living days were 5.6 ± 0.9 ml ^· min^{1 ·} kg¹,4.7 ± 0.8 ml ^· min^{1 ·} kg¹,and 7.8 ± 1.6 kJ/min, respectively. Combined HR and PA measured 24-h O₂ andCO₂ with a precisionsimilar to alternative methods.

     

The VO2 slow component for severe exercise depends on type of exercise and is not correlated with time to fatigue

The purpose ofthis study was to examine the influence of the type of exercise(running vs. cycling) on the O₂uptake (O₂) slow component.Ten triathletes performed exhaustive exercise on a treadmill and on acycloergometer at a work rate corresponding to 90% of maximalO₂ (90% work rate maximalO₂). The duration of thetests before exhaustion was superimposable for both type of exercises(10 min 37 s ± 4 min 11 s vs. 10 min 54 s ± 4 min 47 s forrunning and cycling, respectively). TheO₂ slow component (difference between O₂ atthe last minute and minute 3 ofexercise) was significantly lower during running compared with cycling(20.9 ± 2 vs. 268.8 ± 24 ml/min). Consequently, there was norelationship between the magnitude of theO₂ slow component and thetime to fatigue. Finally, because blood lactate levels at the end of the tests were similar for both running (7.2 ± 1.9 mmol/l) and cycling (7.3 ± 2.4 mmol/l), there was a clear dissociation between blood lactate and the O₂slow component during running. These data demonstrate that1) theO₂ slow component dependson the type of exercise in a group of triathletes and2) the time to fatigue isindependent of the magnitude of theO₂ slow component and bloodlactate concentration. It is speculated that the difference in muscularcontraction regimen between running and cycling could account for thedifference in theO₂ slow component.

     

Vascular tree structure affects lung blood flow heterogeneity simulated in three dimensions

Parker, James C., Chris B. Cave, Jeffrey L. Ardell, CharlesR. Hamm, and Susan G. Williams. Vascular treestructure affects lung blood flow heterogeneity simulated in threedimensions. J. Appl. Physiol. 83(4):1370-1382, 1997.Pulmonary arterial tree structures related toblood flow heterogeneity were simulated by using a symmetrical,bifurcating model in three-dimensional space. The branch angle (),daughter-parent length ratio(r_L), branchrotation angle (), and branch fraction of parent flow () for asingle bifurcation were defined and repeated sequentially through 11 generations. With  fixed at 90°, tree structures were generatedwith  between 60 and 90°,r_L between 0.65 and 0.85, and an initial segment length of 5.6 cm and sectioned into1-cm³ samples for analysis. Bloodflow relative dispersions (RD%) between 52 and 42% and fractaldimensions (D_s)between 1.20 and 1.15 in 1-cm³samples were observed even with equal branch flows. When  0.5, RD% increased, butD_s eitherdecreased with gravity bias of higher branch flows or increased withrandom assignment of higher flows. Blood flow gradients along gravityand centripetal vectors increased with biased flow assignment of higherflows, and blood flows correlated negatively with distance only when   0.5. Thus a recursive branching vascular tree structuresimulated D_s andRD% values for blood flow heterogeneity similar to those observedexperimentally in the pulmonary circulation due to differences in thenumber of terminal arterioles per1-cm³ sample, but blood flowgradients and a negative correlation of flows with distance requiredunequal partitioning of blood flows at branchpoints.

     

Gas exchange and cardiovascular kinetics with different exercise protocols in heart transplant recipients

Grassi, Bruno, Claudio Marconi, Michael Meyer, Michel Rieu,and Paolo Cerretelli. Gas exchange and cardiovascular kinetics with different exercise protocols in heart transplant recipients. J. Appl. Physiol. 82(6): 1952-1962, 1997.Metabolicand cardiovascular adjustments to various submaximal exercises wereevaluated in 82 heart transplant recipients (HTR) and in 35 controlsubjects (C). HTR were tested 21.5 ± 25.3 (SD) mo (range1.0-137.1 mo) posttransplantation. Three protocols were used:protocol A consisted of 5 min of rectangular 50-W load repeatedtwice, 5 min apart [5 min rest, 5 min 50 W (Ex 1), 5 minrecovery, 5 min 50 W (Ex 2)]; protocol B consistedof 5 min of rectangular load at 25, 50, or 75 W; protocol Cconsisted of 15 min of rectangular load at 25 W. Breath-by-breathpulmonary ventilation (E),O₂ uptake (O₂),and CO₂ output(CO₂) were determined.During protocol A, beat-by-beat cardiacoutput () was estimated by impedance cardiography. The half times (t_1/2) of the on- andoff-kinetics of the variables were calculated. In all protocols,t_1/2 values forO₂ on-,E on-, andCO₂ on-kinetics were higher(i.e., the kinetics were slower) in HTR than in C, independently ofworkload and of the time posttransplantation. Also,t_1/2 on- was higher in HTRthan in C. In protocol A, no significant difference of t_1/2 O₂on- was observed in HTR between Ex 1 (48 ± 9 s) and Ex2 (46 ± 8 s), whereas t_1/2 on- was higher during Ex 1 (55 ± 24 s)than during Ex 2 (47 ± 15 s). In all protocols and for all variables, the t_1/2 off-values were higher in HTRthan in C. In protocol C, no differences of steady-stateE,O₂, andCO₂ were observed in bothgroups between 5, 10, and 15 min of exercise. We conclude that1) in HTR, a "priming" exercise, while effective inspeeding up the adjustment of convective O₂ flow to muscle fibers during a second on-transition, did not affect theO₂ on-kinetics, suggestingthat the slower O₂ on- inHTR was attributable to peripheral (muscular) factors; 2) thedissociation between on- andO₂ on-kinetics in HTRindicates that an inertia of muscle metabolic machinery is the mainfactor dictating theO₂ on-kinetics; and 3) theO₂ off-kinetics was slowerin HTR than in C, indicating a greater alactic O₂ deficitin HTR and, therefore, a sluggish muscleO₂ adjustment.

     

Respiratory gas-exchange ratios during graded exercise in fed and fasted trained and untrained men

We evaluated the hypotheses that endurance training increasesrelative lipid oxidation over a wide range of relative exercise intensities in fed and fasted states and that carbohydrate nutrition causes carbohydrate-derived fuels to predominate as energy sources during exercise. Pulmonary respiratory gas-exchange ratios [(RER) = CO₂production/O₂ consumption(O₂)] were determinedduring four relative, graded exercise intensities in both fed andfasted states. Seven untrained (UT) men and seven category 2 and 3 US Cycling Federation cyclists (T) exercised in the morning in random order, with target power outputs of 20 and 40% peakO₂(O_{2 peak}) for 2 h,60% O_{2 peak} for 1.5 h, and 80%O_{2 peak} fora minimum of 30 min after either a 12-h overnight fast or 3 h after astandardized breakfast. Actual metabolic responses were 22 ± 0.33, 40 ± 0.31, 59 ± 0.32, and 75 ± 0.39%O_{2 peak}. T subjectsshowed significantly (P < 0.05)decreased RER compared with UT subjects at absolute workloads when fedand fasted. Fasting significantly decreased RER values compared withthe fed state at 22, 40, and 59%O_{2 peak} inT and at 40 and 59%O_{2 peak} in UTsubjects. Training decreased (P < 0.05) mean RER values compared with UT subjects at 22%O_{2 peak} when theyfasted, and at 40%O_{2 peak} when fed orfasted, but not at higher relative exercise intensities in eithernutritional state. Our results support the hypothesis that endurancetraining enhances lipid oxidation in men after a 12-h overnight fast at low relative exercise intensities (22 and 40%O_{2 peak}). However, atraining effect on RER was not apparent at high relative exercise intensities (59 and 75%O_{2 peak}). Becausemost athletes train and compete at exercise intensities >40% maximalO₂, they will not oxidize agreater proportion of lipids compared with untrained subjects,regardless of nutritional state.     

Nitric oxide response in exhaled air during an incremental exhaustive exercise

Chirpaz-Oddou, M. F., A. Favre-Juvin, P. Flore, J. Eterradossi, M. Delaire, F. Grimbert, and A. Therminarias. Nitric oxide response in exhaled air during an incremental exhaustive exercise. J. Appl. Physiol. 82(4):1311-1318, 1997.This study examines the response of the exhalednitric oxide (NO) concentration (CNO) and the exhaled NOoutput(NO)during incremental exercise and during recovery in six sedentary women,seven sedentary men, and eight trained men. The protocolconsisted of increasing the exercise intensity by 30 W every 3 minuntil exhaustion, followed by 5 min of recovery. Minute ventilation(E), oxygen consumption (O₂), carbon dioxideproduction, heart rate, CNO, andNOwere measured continuously. TheCNO in exhaled air decreasedsignificantly provided that the exercise intensity exceeded 65% of thepeak O₂. It reached similarvalues, at exhaustion, in all three groups. TheNO increasedproportionally with exercise intensity up to exhaustion and decreasedrapidly during recovery. At exhaustion, the mean values weresignificantly higher for trained men than for sedentary men andsedentary women. During exercise,NOcorrelates well with O₂,carbon dioxide production, E, and heartrate. For the same submaximal intensity, and thus a givenO₂ and probably a similarcardiac output,NO appearedto be similar in all three groups, even if theE was different. These results suggestthat, during exercise,NO is mainlyrelated to the magnitude of aerobic metabolism and that thisrelationship is not affected by gender differences or by noticeabledifferences in the level of physical training.

     

Mechanical and metabolic determination of VO2 and fatigue during repetitive isometric contractions in situ

Repetitiveisometric tetanic contractions (1/s) of the caninegastrocnemius-plantaris muscle were studied either at optimal length(L_o) or shortlength (L_s;~0.9 · L_o),to determine the effects of initial length on mechanical and metabolicperformance in situ. Respective averages of mechanical and metabolicvariables were(L_o vs.L_s, allP < 0.05) passive tension (preload) = 55 vs. 6 g/g, maximal active tetanic tension(P_o) = 544 vs. 174 (0.38 · P_o)g/g, maximal blood flow () = 2.0 vs. 1.4 ml · min¹ · g¹,and maximal oxygen uptake(O₂) = 12 vs. 9 µmol · min¹ · g¹.Tension at L_odecreased to0.64 · P_o over20 min of repetitive contractions, demonstrating fatigue; there were nosignificant changes in tension atL_s. In separatemuscles contracting atL_o, was set to that measured atL_s (1.1 ml · min¹ · g¹),resulting in decreased O₂(7 µmol · min¹ · g¹),and rapid fatigue, to0.44 · P_o. Thesedata demonstrate that 1)muscles at L_ohave higher andO₂ values than those at L_s;2) fatigue occurs atL_o with highO₂, adjusting metabolic demand (tension output) to match supply; and3) the lack of fatigue atL_s with lowertension, , andO₂ suggestsadequate matching of metabolic demand, set low by shortmuscle length, with supply optimized by low preload. Thesedifferences in tension andO₂ betweenL_o andL_s groupsindicate that muscles contracting isometrically at initial lengthsshorter than L_oare working under submaximal conditions.

     

Muscle capillarization, O2 diffusion distance, and VO2 kinetics in old and young individuals

Chilibeck, P. D., D. H. Paterson, D. A. Cunningham, A. W. Taylor, and E. G. Noble. Muscle capillarization,O₂ diffusion distance, andO₂ kinetics in old andyoung individuals. J. Appl. Physiol.82(1): 63-69, 1997.The relationships between muscle capillarization, estimated O₂diffusion distance from capillary to mitochondria, andO₂ uptake(O₂) kineticswere studied in 11 young (mean age, 25.9 yr) and 9 old (mean age, 66.0 yr) adults. O₂kinetics were determined by calculating the time constants () forthe phase 2 O₂ adjustment to andrecovery from the average of 12 repeats of a 6-min, moderate-intensityplantar flexion exercise. Muscle capillarization was determined fromcross sections of biopsy material taken from lateral gastrocnemius.Young and old groups had similarO₂ kinetics(O₂-on = 44 vs. 48 s;O₂-off = 33 vs. 44 s, for young and old, respectively), muscle capillarization, andestimated O₂ diffusion distances.Muscle capillarization, expressed as capillary density or averagenumber of capillary contacts per fiber/average fiber area, and theestimates of diffusion distance were significantly correlated toO₂-off kinetics in theyoung (r = 0.68 to 0.83;P < 0.05). We conclude that1) capillarization andO₂ kinetics during exerciseof a muscle group accustomed to everyday activity (e.g., walking) arewell maintained in old individuals, and2) in the young, recovery of O₂ after exercise isfaster, with a greater capillary supply over a given muscle fiber areaor shorter O₂ diffusion distances.

     

Respiratory muscle work compromises leg blood flow during maximal exercise

Harms, Craig A., Mark A. Babcock, Steven R. McClaran, DavidF. Pegelow, Glenn A. Nickele, William B. Nelson, and Jerome A. Dempsey.Respiratory muscle work compromises leg blood flow during maximalexercise. J. Appl. Physiol.82(5): 1573-1583, 1997.We hypothesized that duringexercise at maximal O₂ consumption (O_{2 max}),high demand for respiratory muscle blood flow() would elicit locomotor muscle vasoconstrictionand compromise limb . Seven male cyclists(O_{2 max} 64 ± 6 ml · kg¹ · min¹)each completed 14 exercise bouts of 2.5-min duration atO_{2 max} on a cycleergometer during two testing sessions. Inspiratory muscle work waseither 1) reduced via aproportional-assist ventilator, 2)increased via graded resistive loads, or3) was not manipulated (control).Arterial (brachial) and venous (femoral) blood samples, arterial bloodpressure, leg (legs;thermodilution), esophageal pressure, andO₂ consumption(O₂) weremeasured. Within each subject and across all subjects, at constantmaximal work rate, significant correlations existed(r = 0.74-0.90;P < 0.05) between work of breathing(Wb) and legs (inverse), leg vascular resistance (LVR), and leg O₂(O_{2 legs};inverse), and between LVR and norepinephrine spillover. Mean arterialpressure did not change with changes in Wb nor did tidal volume orminute ventilation. For a ±50% change from control in Wb,legs changed 2 l/min or 11% of control, LVRchanged 13% of control, and O₂extraction did not change; thusO_{2 legs}changed 0.4 l/min or 10% of control. TotalO_{2 max} was unchangedwith loading but fell 9.3% with unloading; thusO_{2 legs}as a percentage of totalO_{2 max} was 81% incontrol, increased to 89% with respiratory muscle unloading, anddecreased to 71% with respiratory muscle loading. We conclude that Wbnormally incurred during maximal exercise causes vasoconstriction inlocomotor muscles and compromises locomotor muscle perfusion andO₂.

     

Changes in maximum oxygen uptake during prolonged training, overtraining, and detraining in horses

Tyler, Catherine M., Lorraine C. Golland, David L. Evans,David R. Hodgson, and Reuben J. Rose. Changes in maximum oxygenuptake during prolonged training, overtraining, and detraining inhorses. J. Appl. Physiol. 81(5):2244-2249, 1996.Thirteen standardbred horses were trained asfollows: phase 1 (endurance training, 7 wk),phase 2 (high-intensity training, 9 wk),phase 3 (overload training, 18 wk), andphase 4 (detraining, 12 wk). Inphase 3, the horses were divided intotwo groups: overload training (OLT) and control (C). The OLT groupexercised at greater intensities, frequencies, and durations than groupC. Overtraining occurred after 31 wk of training and was defined as asignificant decrease in treadmill run time in response to astandardized exercise test. In the OLT group, there was a significantdecrease in body weight (P < 0.05).From pretraining values of 117 ± 2 (SE)ml ^· kg^{1 ·} min¹,maximal O₂ uptake(O_{2 max}) increased by15% at the end of phase 1, and when signs of overtraining werefirst seen in the OLT group,O_{2 max} was 29%higher (151 ± 2 ml ^· kg^{1 ·} min¹in both C and OLT groups) than pretraining values. There was nosignificant reduction inO_{2 max} until after 6 wk detraining whenO_{2 max} was 137 ± 2 ml ^· kg^{1 ·} min¹.By 12 wk detraining, meanO_{2 max} was134 ± 2 ml ^· kg^{1 ·} min¹,still 15% above pretraining values. When overtraining developed, O_{2 max} was notdifferent between C and OLT groups, but maximal values forCO₂ production (147 vs. 159 ml ^· kg^{1 ·} min¹)and respiratory exchange ratio (1.04 vs. 1.11) were lower in the OLTgroup. Overtraining was not associated with a decrease inO_{2 max} and, afterprolonged training, decreases inO_{2 max} occurredslowly during detraining.

     

Mitochondrial redox state as a potential detector of liver dysoxia in vivo

Dysoxia canbe defined as ATP flux decreasing in proportion toO₂ availability with preserved ATPdemand. Hepatic venous -hydroxybutyrate-to-acetoacetate ratio(-OHB/AcAc) estimates liver mitochondrial NADH/NAD and may detectthe onset of dysoxia. During partial dysoxia (as opposed to anoxia),however, flow may be adequate in some liver regions, diluting effluentfrom dysoxic regions, thereby rendering venous -OHB/AcAc unreliable.To address this concern, we estimated tissue ATP whilegradually reducing liver blood flow of swine to zero in a nuclearmagnetic resonance spectrometer. ATP flux decreasing withO₂ availability was taken asO₂ uptake(O₂) decreasing inproportion to O₂ delivery(O₂);and preserved ATP demand was taken as increasingP_i/ATP.O₂, tissueP_i/ATP, and venous -OHB/AcAcwere plotted againstO₂to identify critical inflection points. Tissue dysoxia required meanO₂for the group to be critical for bothO₂ and forP_i/ATP. CriticalO₂values for O₂ andP_i/ATP of 4.07 ± 1.07 and 2.39 ± 1.18 (SE) ml · 100 g¹ · min¹,respectively, were not statistically significantly different but notclearly the same, suggesting the possibility that dysoxia might havecommenced after O₂ begandecreasing, i.e., that there could have been"O₂ conformity." CriticalO₂for venous -OHB/AcAc was 2.44 ± 0.46 ml · 100 g¹ · min¹(P = NS), nearly the same as that forP_i/ATP, supporting venous -OHB/AcAc as a detector of dysoxia. All issues considered, tissue mitochondrial redox state seems to be an appropriate detector ofdysoxia in liver.

     

Oxygen transport in conscious newborn dogs during hypoxic hypometabolism

We questioned whether the decrease inO₂ consumption(O₂) during hypoxia innewborns is a regulated response or reflects a limitation inO₂ availability. Experiments wereconducted on previously instrumented conscious newborn dogs.O₂ was measured at a warmambient temperature (30°C, n = 7)or in the cold (20°C, n = 6),while the animals breathed air or were sequentially exposed to 15 minof fractional inspired O₂(FI_O2): 21, 18, 15, 12, 10, 8, and 6%. In normoxia,O₂ averaged 15 ± 1 (SE)and 25 ± 1 ml · kg¹ · min¹in warm and cold conditions, respectively. In the warmcondition, hypometabolism (i.e., hypoxicO₂ < normoxicO₂) occurred at FI_O2 10%, whereas in thecold condition, hypometabolism occurred atFI_O2 12%. The sameresults were obtained in a separate group(n = 14) of noninstrumented puppies.For all levels of FI_O2 withhypometabolism, the relationships between measures ofO₂ availability (arterialO₂ saturation or content, venousPO₂ or saturation,x-axis) vs.O₂(y-axis) had lower slopes in warm than in coldconditions. Hence, O₂ during hypometabolism in the warm condition was not the maximal attainable for the level of oxygenation. The results do not support thepossibility that the hypoxic drop inO₂ in the newborn reflects a limitation in O₂availability. The results are compatible with the ideathat the phenomenon is one of "regulated conformism" tohypoxia.