The V̇O2 response for an exhaustive treadmill run at 800-m pace: a breath-by-breath analysis

Recent research in which data were averaged over 10 or 30 s suggests that the O₂ response of aerobically fit individuals plateaus below O_{2 max} in an exhaustive square-wave run lasting ~2 min. To investigate this phenomenon we examined the breath-by-breath O₂ response of trained runners to an exhaustive treadmill run at 800 m pace. Eight male competitive runners completed two treadmill tests on separate days: a ramp test to exhaustion and an exhaustive square-wave run at 800-m pace. For the ramp test, the breath-by-breath data were smoothed with a 15-s moving average and the highest of the smoothed values was taken as O_{2 peak} [mean (SD): 68.9 (5.6) ml kg^–1 min^–1]. For the square-wave, the breath-by-breath data were interpolated to give one value per second and modelled using a monoexponential function. Following a delay of 11.2 (1.5) s, O₂ increased quickly [phase-2 time constant of 10.7 (2.7) s] towards an asymptote that represented just 85 (6)% of O_{2 peak} from the ramp test. Expressed in ml kg^–1 min^–1, this asymptote was independent of O_{2 peak} (r=0.04, P=0.94). However, as a percentage of O_{2 peak} it was negatively correlated with O_{2 peak} itself (r=–0.96, P<0.001). It is concluded that in an exhaustive square-wave treadmill run lasting ~2 min the O₂ of aerobically fit runners increases quickly to plateau at a level that is lower than, but independent of, O_2max     

Absence of long-term modulation of ventilation by dead-space loading during moderate exercise in humans

The stability of arterial PCO₂ (P_aCO₂) during moderate exercise in humans suggests a CO₂-linked control that matches ventilation (_E) to pulmonary CO₂ clearance (CO₂). An alternative view is that _E is subject to long-term modulation (LTM) induced by hyperpnoeic history. LTM has been reported with associative conditioning via dead-space (V_D) loading in exercising goats (Martin and Mitchell 1993). Whether this prevails in humans is less clear, which may reflect differences in study design (e.g. subject familiarisation; V_D load; whether or not _E is expressed relative to CO₂; choice of P_aCO₂ estimator). After familiarisation, nine healthy males performed moderate constant-load cycle-ergometry (20 W-80 W-20 W; <lactate threshold, _L): day 1, pre-conditioning, n=3; day 2, conditioning (V_D=1.59 l, doubling _E at 20 W and 80 W), n=8 with 10 min rest between tests; and, after 1 h rest, post-conditioning, n=3. Gas exchange was determined breath-by-breath. Post-conditioning, neither the transient [phase 1, phase 2 (1, 2)] nor steady-state _E exercise responses, nor their proportionality to CO₂, differed from pre-conditioning. For post-conditioning trial 1, steady-state _E was 28.1 (4.7) l min^–1 versus 29.1 (3.8) l min^–1 pre-conditioning, and mean-alveolar PCO₂ (a validated P_aCO₂ estimator) was 5.53 (0.48) kPa [41.5 (3.6) mmHg] versus 5.59 (0.49) kPa [41.9 (3.7) mmHg]; the 1 _E increment was 4.2 (2.9) l min^–1 versus 5.2 (1.9) l min^–1; the 2 _E time-constant () was 64.4 (24.1) s versus 64.1 (25.3) s; _E/CO₂ was 1.12 (0.04) versus 1.10 (0.04); and the _E-CO₂ slope was 21.7 (3.4) versus 21.2 (3.2). In conclusion, we could find no evidence to support ventilatory control during moderate exercise being influenced by hyperpnoeic history associated with dead-space loading in humans.     

Diffusionsfehler und Eigenverbrauch der Pt-elektrode beipO2-Messungen im steady state

Zusammenfassung Im steady state beeinflussen Diffusionsfehler und Eigenverbrauch der Pt-Elektrode als systematische Fehler O₂-Partialdruckmessungen. Sie sind abhängig von den geometrischen Eigenschaften der Elektrode, den Diffusionseigenschaften der Membran sowie den Diffusions- und Konvektionseigenschaften des Meßmediums. Das Diffusionsfeld vor der Pt-Oberfläche und das dadurch bestimmte stationäre Meßsignal werden für gasförmige und nicht gasförmige Medien mit und ohne Konvektion berechnet. Daraus resultieren quantitative Aussagen über die systematischen Fehler. Speziell für Messungen in durchbluteten Geweben (z. B. Hirnrinde und Myokard) wird der Einfluß des Eigenverbrauchs von Pt-Elektroden auf den intracapillärenpO₂-Abfall in Durchblutungsrichtung und das intercapillärepO₂-Feld am Meßort der Elektrode ermittelt. Diese Berechnungen erfolgten mit Hilfe eines Digitalmodells.

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Erklärung der Symbole A O₂-Verbrauch des Gewebes - Bunsenscher Löslichkeitskoeffizient des Mediums - _m Bunsenscher Löslichkeitskoeffizient der Membran - C ₁,C ₁,C ₂,C ₂,C ₃ Konstanten - D Diffusionskoeffizient des Mediums - DF, DF Diffusionsfehler bei einfacher und doppelter Membran - DGl Differentialgleichung - d Capillarabstand - d _h Dicke der hydrodynamischen Grenzschicht - d _m ,d _m Dicke der Membranen - , , , , , dimensionslose Parameter - exp Exponentialfunktion - F Faradaykonstante - grad Gradient - I _o stationäres Meßsignal in Medien ohne Konvektion - I stationäres Meßsignal in Gasen - I _o stationäres Meßsignal in Flüssigkeiten mit Konvektion - J _o nullte Bessel-Funktion - K Diffusionsleitfähigkeit des Mediums - KE, KE Konvektionseffekt bei einfacher und doppelter Membran - K _m ,K _m Diffusionsleitfähigkeit der Membranen - l Capillarlänge - l Capillarabschnitt - Viscosität des Mediums - p, pO₂,p(r), p(r,z) O₂-Partialdruck - p mittlerer Partialdruck - P _a O₂-Partialdruck am arteriellen Capillarende - p _c konstanter Partialdruck - P/r _o +d _m O₂-Partialdruck an der Grenze Membran/Medium - P _v O₂-Partialdruck am venösen Capillarende - P _g relativer O₂-Partialdruckabfall im Gewebe - P _v relativer O₂-Partialdruckabfall am venösen Capillarende - R Radius der ebenen kreisförmigen Elektrode - RB Randbedingung - RDF, RDF restlicher Diffusionsfehler einfacher und doppelter Membranen - r _o Radius der Elektrode mit halbkugelförmiger Pt-Oberfläche - r, z Zylinderkoordinaten - r _K Capillarradius - S Sättigungsabfall im Capillarblut ohne Elektrode - S Sättigungsabfall im Capillarblut mit Elektrode - u O₂-Konzentration - V Diffusionsgesamtfluß - V _K Diffusionsfluß aus einem Capillarabschnitt - v _r ,v _z Komponenten des Stromdichtevektors inr- bzw.z-Richtung (Zylinderkoordinaten) - mittlere Stromdichte - Stromdichtevektor des Flusses der O₂-Moleküle - v _c konstante Geschwindigkeit des bewegten Mediums - x, y, z Kartesische Koordinaten - Integrationsvariable - ² Laplace-Operator - partielle Ableitung nach der Zeit     

Einstellzeit der Pt-Elektrode bei Messungen nicht stationärer O2-Partialdrucke

Zusammenfassung Das Meßsignal bei sprunghaftenpO₂-Änderungen wird anhand des Diffusionsfeldes der Elektrode beschrieben. Es wird das zeitliche Verhalten des Meßsignals von blanken und membranbespannten Elektroden in gasförmigen und nicht gasförmigen Meßmedien betrachtet. Aus dem Verhalten des Meßsignals kann jeweils die Einstellzeit alssystematischer Meßfehler abgeleitet werden. In nicht gasförmigen Medien (z. B. biologisches Gewebe) übersteigt das Meßsignal nach einempO₂-Sprung zu höheren Werten das stationäre Endsignal. Daraus ergibt sich eine besondere Betrachtung der Einstellzeit in solchen Medien.Die Einstellzeit für Pt-Elektroden mit einfacher und doppelter Membran wird explizit angegeben. Schließlich wird für biologische Medien die Einstellzeit mit dem Diffusionsfehler [8] verglichen. Die Forderungen an eine Membran der Pt-Elektrode mit kleiner Einstellzeit und gleichzeitig kleinem Diffusionsfehler sind zusammengestellt.

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Erklärung der Symbole a Verhältnis der Diffusionskoeffizienten zweier Membranen - Bunsenscher Löslichkeitskoeffizient des Mediums - _m Bunsenscher Löslichkeitskoeffizient der Membran - b Verhältnis der Diffusionsleitfähigkeiten von Membran und Medium - C ₁,C ₂ Proportionalitätskonstanten zwischen Meßsignal und O₂-Partialdruck - D Diffusionskoeffizient des Mediums - D _m,D _m Diffusionskoeffizienten der Membranen - Diffusionskoeffizient der effektiven Membran - DF Diffusionsfehler - DGl Differentialgleichung - d _m,d _m Dicke der Membranen - Dicke der effektiven Membran - dimensionsloser Parameter des Diffusionsfehlers - erf Fehlerfunktion - exp Exponentialfunktion - F Faradaykonstante - grad Gradient - I stationäres Meßsignal vor dempO₂-Sprung - I stationäres Meßsignal nach dempO₂-Sprung - I(t), I(),I() instationäres Meßsignal als Funktion der Zeit bzw. zeitabhängiger dimensionsloser Parameter - K Diffusionsleitfähigkeit des Mediums - K _m Diffusionsleitfähigkeit der Membran - Diffusionsleitfähigkeit der effektiven Membran - dimensionsloser Parameter - n Summationsindex - pO₂ O₂-Partialdruck - pO₂ als Funktion von Ort und Zeit bzw. zeitabhängiger dimensionsloser Parameter; Diffusionsfeld der Elektrode - p _c konstanterpO₂ vor dempO₂-Sprung - p _c konstanterpO₂ nach dempO₂-Sprung - p(r ₀+d _m , ) pO₂ an der Grenze Membran/Medium in Abhängigkeit des Zeitparameters - p(r,o) Diffusionsfeld zum Zeitpunkt (t=0) despO₂-Sprunges - p(r₀+d_m, o) pO₂ an der Grenze Membran/Medium zum Zeitpunkt despO₂-Sprunges - R Radius der ebenen, kreisförmigen Elektrode - r ₀ Radius der Elektrode mit halbkugelförmiger Pt-Oberfläche - r Kugelkoordinate - ₁,₂ dimensionslose ortsabhängige Parameter - T ₉₀,T ₉₅ Zeit, bis 90% bzw. 95% des Signalunterschiedes nach dempO₂-Sprung ausgeglichen sind (Einstellzeit) - T ₉₀,T ₉₅ Einstellzeit der Elektrode mit Doppelmembran - T _90*,T _95* Zeit, bis sich das Signal nach Übersteigen des stationären Endwertes diesem auf 10% bzw. 5% angenähert hat - dimensionslose Parameter zu den vorangegangenen Einstellzeiten - t Zeitkoordinate - , dimensionslose zeitabhängige Parameter - t _max, _max Zeit maximaler Signalhöhe nachpO₂-Sprung und zugehöriger dimensionsloser Parameter - V(t) Diffusionsgesamtfluß zur Pt-Oberfläche - Stromdichtevektor der diffundierenden O₂-Moleküle - x, y, z Kartesische Koordinaten - Integrationsvariable - ² Laplace-Operator - partielle Ableitung nach der Zeit - Integral über eine Fläche - gerichtetes Flächenelement     

Energetics of locomotion in African pygmies

Summary The energy cost of walking (C _w). and running (C _r), and the maximal O₂ consumption (VO_2max) were determined in a field study on 17 Pygmies (age 24 years, SD 6; height 160 cm, SD 5; body mass 57.2 kg, SD 4.8) living in the region of Bipindi, Cameroon. TheC _w varied from 112 ml·kg^–1·km^–1, SD 25 [velocity (), 4 km·h^–1] to 143 ml·kg^–1·km^–1, SD 16 (, 7 km·h^–1). Optimal walking was 5 km·h^–1. TheC _r was 156 ml·kg^–1·km^–1, SD 14 (, 10 km·h^–1) and was constant in the 8–11 km·h^–1 speed range. TheVO_2max was 33.7 ml·kg^–1· min^–1, i.e. lower than in other African populations of the same age. TheC _r andC _w were lower than in taller Caucasian endurance runners. These findings, which challenge the theory of physical similarity as applied to animal locomotion, may depend either on the mechanics of locomotion which in Pygmies may be different from that observed in Caucasians, or on a greater mechanical efficiency in Pygmies than in Caucasians. The lowC _r values observed enable Pygmies to reach higher running speeds than would be expected on the basis of theirVO_2max.     

Overshoot in <Emphasis Type="Italic">V̇</Emphasis>O<Subscript>2</Subscript> following the onset of moderate-intensity cycle exercise in trained cyclists

We have previously observed that following the onset of moderate intensity cycle ergometry, the pulmonary O₂ uptake (O₂) in trained cyclists often does not increase towards its steady-state value with the typical mono-exponential characteristics; rather, there is a transient overshoot. The purpose of this study was to systematically examine this phenomenon by comparing the O₂responses to two moderate-intensity work rates and one high-intensity work rate in trained and untrained subjects. Following a ramp exercise test to the limit of tolerance for the determination of the gas exchange threshold (GET) and O_2peak, seven trained cyclists [mean (SD); O_2peak 66.6 (2.5) ml·kg^–1·min^–1] and eight sedentary subjects [O_2peak 42.9 (5.1) ml·kg^–1·min^–1] completed six step transitions from baseline cycling to work rates requiring 60% and 80% GET and three step transitions from baseline cycling to a work rate requiring 50% of the difference between GET and O_2peak (50%). O₂ was measured breath-by-breath and modelled using standard techniques. The sedentary subjects did not overshoot the steady-state O₂ at any intensity. At 60% GET, six of the seven cyclists overshot the steady-state O₂ [by an integral volume of 164 (44) ml between ~45 and 125 s]. At 80% GET, four of the seven cyclists overshot the steady-state O₂ [by an integral volume of 185 (92) ml between ~55 and 140 s]. None of the cyclists showed an overshoot at 50%. These results indicate that trained cyclists evidence an overshoot in O₂ before steady-state is reached in the transition to moderate-intensity exercise. The mechanism(s) responsible for this effect remains to be elucidated, as does whether the overshoot confers any functional or performance benefit to the trained cyclist.     

Influence of muscle fibre type and pedal rate on the V̇O2-work rate slope during ramp exercise

We hypothesised that the ratio between the increase in oxygen uptake and the increase in work rate (O₂/WR) during ramp cycle exercise would be significantly related to the percentage type II muscle fibres at work rates above the gas exchange threshold (GET) where type II fibres are presumed to be active. We further hypothesised that ramp exercise at higher pedal rates, which would be expected to increase the proportional contribution of type II fibres to the total power delivered, would increase the O₂/WR slope at work rates above the GET. Fourteen healthy subjects [four female; mean (SD): age 25 (3) years, body mass 74.3 (15.1) kg] performed a ramp exercise test to exhaustion (25 W min^–1) at a pedal rate of 75 rev min^–1, and consented to a muscle biopsy of the vastus lateralis. Eleven of the subjects also performed two further ramp tests at pedal rates of 35 and 115 rev min^–1. The O₂/WR slope for exercise <GET (S ₁) was significantly correlated with O₂ peak in ml kg^–1 min^–1 (r=0.60; P<0.05), whereas the O₂/WR slope for exercise >GET (S ₂) was significantly correlated to percentage type II fibres (r=0.54; P=0.05). The ratio between the O₂/WR slopes for exercise above and below the GET (S ₂/S ₁) was significantly greater at the pedal rate of 115 rev min^–1 [1.22 (0.09)] compared to pedal rates of 35 rev min^–1 [0.96 (0.02)] and 75 rev min^–1 [1.09 (0.05), (P<0.05)]. The greater increase in S ₂ relative to S ₁ in subjects (1) with a high percentage type II fibres, and (2) at a high pedal rate, suggests that a greater recruitment of type II fibres contributes in some manner to the xs O₂ observed during ramp exercise.     

Characterisation, asymmetry and reproducibility of on- and off-transient pulmonary oxygen uptake kinetics in endurance-trained runners

The purpose of this study was three-fold: (1) to characterise both the on- and off-transient oxygen uptake (O₂) kinetics in endurance runners during moderate-intensity treadmill running; (2) to determine the degree of symmetry between on- and off-transients; and (3) to determine the reproducibility of O₂ kinetic parameters in endurance runners. Twelve endurance-trained runners [mean (SD) age 25.2 (4.7) years, body mass 70.1 (9.7) kg, height 179.5 (7.5) cm, ventilatory threshold (V_T), 3,429 (389) ml.min^–1, maximal O₂ (O_2max) 4,138 (625) ml.min^–1] performed two multiple square-wave transition protocols on separate days. The protocol consisted of six (three transitions, 15 min rest, three transitions) square-wave transitions from walking at 4 km.h^–1 to running at a speed equivalent to 80% of the O₂ at the V_T (80%V_T). To determine the reproducibility, the protocol was repeated on a separate day (i.e. a test-retest design). Pulmonary gas-exchange was measured breath-by-breath. The O₂ data were modelled [from 20 s post-onset (or offset) of exercise] using non-linear least squares regression by a mono-exponential model, incorporating a time delay. The on- and off-transient time constants (_on and _off), mean response times (MRT_on and MRT_off) and amplitudes (A_on and A_off) were obtained from the model fit. On- and off transient kinetics were compared using paired t-tests. The reproducibility of each kinetic parameter was explored using statistical (paired t-tests) and non-statistical techniques [95% limits of agreement (LOA, including measurement error and systematic bias) and coefficient of variation (CV)]. It was found that the _on [12.4 (1.9)] was significantly (P<0.001) shorter than _off [24.5 (2.3) s]. Similarly, MRT_on [27.1 (1.9) s] was shorter than MRT_off [33.4 (2.2) s]. With respect to the reproducibility of the parameters, paired t-tests did not reveal significant differences between test 1 and test 2 for any on- or off-transient O₂ kinetic parameter (P>0.05). The LOA for _on (1.9 s), _off (2.3 s), MRT_on (1.2 s), MRT_off (3.2 s), A_on (204 ml.min^–1) and A_off (198 ml.min^–1) were narrow and acceptable. Furthermore, the measurement error (range, 4.3 to 15.1%) and CV (1.3 to 4.8%) all indicated good reproducibility. There was a tendency for _off to be more reproducible than _on. However, MRT_on was the most reproducible kinetic parameter. Overall, the results suggest that: (1) a multiple square-wave transition protocol can be used to characterise, reproducibly, both on- and off-transient O₂ kinetic parameters during treadmill running in runners; (2) the phase II time constant is independent of O_{2 max}, and (3) asymmetry exists between on- and off transient O₂ kinetic parameters.     

Effect of alteration of peripheral blood flow on the central circulation in man during supine cycling in different ambient temperatures

Summary Whether the alteration of peripheral circulation caused by changing ambient temperature (T_a) affects central circulatory changes in man during supine cycling was investigated in four well-trained men, who exercised at two levels (117.7 or 176.6 W). Exercise metabolic rate (VO₂) in cold (0 C or 10 C) was the same as it was at 20 C, whereas the cardiac output (CO; CO₂ rebreathing technique) and heart rate were significantly lower (e.g., 176.6 W at 0 C, both p<0.01). In heat (30 C or 40 C), the VO₂ reduced with falling CO and mean arterial blood pressure from those at 20 C (e.g., 176.6 W at 40 C, all cases p<0.01), whereas the peak post-exercise calf blood flow (CBF_p) increased (p<0.01). The VO₂ and stroke volume (SV) were inversely proportional to the ratio of CBF_p to CO/kg body weight (CBF_p/CO) (r>–0.78, p<0.001). Total peripheral resistance (TPR) was related to arteriovenous oxygen difference (A-VO₂ difference) (r>0.78, p<0.001). The TPR and A-VO₂ difference decreased as T_a rose, while CBF_p/CO was almost the same. As CBF_p/CO had exceeded 50 and further progressed, however, the two parameters elevated until the same level as that at 0 C. The present results suggest that during moderately prolonged (16–60 min) supine cycling in different T_a's the central circulatory changes are mainly affected by the altered peripheral blood flow in competing between skin and muscle for blood flow.     

The effectiveness of the control of pH in the extracellular fluid of the brain by the respiratory control system

Summary The effectiveness of the respiratory control system as a regulator of the pH in the extracellular fluid of the brain is defined by pH_{ECF op}/pH_{ECF cl} where pH_{ECF op} means the primary or open loop shift and pH_{ECF cl} the final or closed loop shift of brain extracellular fluid pH. The analysis of a steady state model described in a preceding paper (Loeschcke, 1973) allows, in the limits of the suppositions and simplifications, to calculate the effectiveness of the feedback regulator in the cases of increased metabolism, metabolic acidosis-alkalosis and inhalation of CO₂. The effectiveness is diminished if CO₂ production is increased, it drops in metabolic acidosis and rises in metabolic alkalosis and it drops steeply if CO₂ is inhaled. The effectiveness of this control system depends on the controlling action of the controlling element (the ventilation) rather than on varying sensitivity of the sensing element. The controlling effect is defined asC=–d P _CO2/d V _A orC=d pH_ECF/d V _A.Im Rahmen des Programms des Sonderforschungsbereiches 114 (Bionach) der Deutschen Forschungsgemeinschaft.     

Cardiac output and oxygen release during very high-intensity exercise performed until exhaustion

Our objectives were firstly, to study the patterns of the cardiac output () and the arteriovenous oxygen difference [(a–)O₂] responses to oxygen uptake (O₂) during constant workload exercise (CWE) performed above the respiratory compensation point (RCP), and secondly, to establish the relationships between their kinetics and the time to exhaustion. Nine subjects performed two tests: a maximal incremental exercise test (IET) to determine the maximal O₂ ( V ̇O₂peak), and a CWE test to exhaustion, performed at p 50 (intermediate power between RCP and O₂peak). During CWE, V ̇O₂ was measured breath-by-breath, Q ̇ was measured beat-by-beat with an impedance device, and blood lactate (LA) was sampled each minute. To calculate ( a–v ̄)O₂, the values of V ̇O₂ and Q ̇ were synchronised over 10 s intervals. A fitting method was used to describe the V ̇O₂, Q ̇ and ( a–v ̄)O₂ kinetics. The ( a–v ̄)O₂ difference followed a rapid monoexponential function, whereas both V ̇O₂ and Q ̇ were best fitted by a single exponential plus linear increase: the time constant () V ̇O₂ [57 (20 s)] was similar to ( a–v ̄)O₂, whereas for Q ̇ was significantly higher [89 (34) s, P <0.05] (values expressed as the mean and standard error). LA started to increase after 2 min CWE then increased rapidly, reaching a similar maximal value as that seen during the IET. During CWE, the rapid component of O₂ uptake was determined by a rapid and maximal ( a–)O₂ extraction coupled with a two-fold longer Q ̇ increase. It is likely that lactic acidosis markedly increased oxygen availability, which when associated with the slow linear increase of Q ̇, may account for the V ̇O₂ slow component. Time to exhaustion was larger in individuals with shorter time delay for ( a–v ̄)O₂ and a greater for .     

Influence of ageing on aerobic parameters determined from a ramp test

Summary The purpose of this study was to examine the four parameters of aerobic function, the maximum oxygen uptake ( O_2max), ventilation threshold (Th _VE), efficiency, and the effective time constant for oxygen consumption ( 0₂), across age. In particular, the study was designed to observe whether there may be accelerated declines in aerobic function beyond 60 years of age. Seventy-nine sedentary men aged 30–84 years were studied. Each subject performed two maximal cycle ramp function tests, and data were collected on a breath-by-breath basis. The O_2max, from a plateau in 0₂, was achieved in 87% of the subjects using the ramp test. The O_2max showed a significant decrease with increasing age (from linear regression,r = –0.81) at a rate averaging 0.037 l·min^–1·year^–1. The Th _VE also declined with increasing age, but at a slower rate (0.013 l·min^–1·year^–1). The O₂ was significantly increased across the age groups from 69 s for those aged 30–40 years to 98s for those aged 60 years or more. There was no evidence of accelerated decline in these aerobic parameters beyond age 60 years, and there were no differences in efficiency (27.5–29.9%) across age. Although other forcing functions should be used to confirm this characterization of the oxygen kinetics, this slowed response with age would result in greater oxygen deficit and possibly earlier fatigue in response to even light exercise in older individuals.     

Effects of training on plasma FFA during exercise in women

Summary The purpose of this study was to investigate the effects of training on plasma FFA concentrations in women during 60 min of work. All subjects (n=10) exercised at 55% of their initial VO_{2 max} for 60 min on a bicycle ergometer. Five subjects then participated in a training program, consisting of bicycling five days per week for four weeks while five control subjects remained inactive. Following the training or control period, all 10 subjects repeated the initial 1-h test at the same absolute work load. The training program resulted in a 14% increase in VO_{2 max} and a decreased resting HR (p<0.05). The submaximal exercise HR and R were also lower following training (p<0.05). Plasma FFA were significantly lower (p<0.05) during exercise in the experimental group following training. The average increase in plasma FFA during the 60 min bicycle test was 0.22 mol/l, from 0.48 mol/l at rest to 0.70 mol/l after 60 min of exercise prior to training. After training the same absolute work load resulted in an increased plasma FFA of only 0.10 mol/l from 0.29 to 0.39 mol/l. No significant changes due to training were observed for glycerol or lactate. The results suggest that the metabolic response of women is similar to men during exercise before and after training. Possible mechanisms for the decreased plasma FFA response after training are discussed.     

Serum carbonic anhydrase III,an enzyme of type I muscle fibres,and the intensity of physical exercise

The effects of 30 min running with stepwise increasing intensity (exhaustive, energy demand approx. 50 100% ofVO_2max), 60 s supramaximal running (anaerobic, 125% ofVO_2max) and 40–60 min low-intensity running (acrobic, 40–60% ofVO_2max) on serum concentration of muscle-derived proteins were studied in 5 male and 5 female elite orienteerers. S-Carbonic anhydrase III (S-CA III) was used as a marker of protein leakage from type I (slow oxidative) muscle fibres and S-myoglobin (S-Mb) as a non-selective (type I+II) muscular marker. The fractional increase in S-CA III (S-Ca III) was 0.37±0.09 (mean±SEM,p<0.001), 0.10±0.05 (N. S.) and 0.46±0.09 (p<0.001) 1 h after exhaustive, anaerobic and aerobic exercise, respectively. The corresponding values for S-Mb were 1.45±0.36 (p<0.001), 0.39±0.13 (p<0.01) and 0.67±0.18 (p<0.001). The value for the S-CA III/S-Mb ratio was 0.68±0.03 after the acrobic exercise, but only 0.25–0.26 (p vs. aerobic exercise <0.001) after the two high-intensity forms of exercise. Since type I fibres of skeletal muscle are known to be responsible for power production during low-intensity exercise, whereas fibres of both type I and type II are active at higher intensities, the S-CA III/S-Mb ratio may depend on the recruitment profile of type I vs. type I+II fibres.     

Breath-by-breath alveolar oxygen transfer at the onset of step exercise in humans: methodological implications

The effects of using different algorithms to estimate the time constant of changes in oxygen uptake at the onset of square-wave 120 W cycloergometric exercise were evaluated in seven subjects. The volume of oxygen taken up at the alveoli (VO_2Ai) was determined breath-by-breath (BB) from the volume of O₂ transferred at the mouth (VO_2mi) minus the corresponding volume changes in O₂ stores in the alveoli: VO_2Ai=VO_2mi–[V _Ai–1(FO_2Ai–FO_2Ai–1)+FO_2Ai·ΔV _Ai], where V _Ai–1 is the alveolar volume at the end of the previous breath, FO_2Ai and FO_2Ai–1 are estimated from the fractions of end-tidal O₂ in the current and previous breaths, respectively, and ΔV _Ai is the change in volume during breath i. These quantities can be measured BB, with the exception of V _Ai–1 which must be assumed. The respiratory cycle has been defined as the time elapsing between identical fractions of expiratory gas in two successive breaths. Using this approach, since FO_2Ai=FO_2Ai–1, any assumption regarding V _Ai–1 becomes unnecessary. In the present study, VO_2Ai was calculated firstly, by using this approach, and secondly by setting different V _Ai–1 values (from 0 to FRC+0.5 l, where FRC is the functional residual capacity). Values for alveolar O₂ flow (V˙O_2Ai), as calculated from the quotient of VO_2Ai divided by breath duration, were then fitted bi-exponentially. The time constant of the phase II kinetics of V˙O_2Ai (τ₂) was linearly related to V _Ai–1, increasing from 36.6 s (V _Ai–1=0) to 46.8 s (V _Ai–1=FRC+0.5 l) while τ₂ estimated using the first approach amounted to 34.3 s. We concluded that, firstly, the first approach allowed us to calculate V˙O_2A during transitions in step exercise; and secondly, when using methods wherein V _Ai–1 must be assumed, τ₂ depended on V _Ai–1. Electronic Publication     

Dichloroacetate does not speed phase-II pulmonary V̇O2 kinetics following the onset of heavy intensity cycle exercise

We hypothesised that pharmacological activation of the pyruvate dehydrogenase enzyme complex (PDC) by dichloroacetate (DCA) would speed phase-II pulmonary O₂ uptake (O₂) kinetics following the onset of high-intensity, sub-maximal exercise. Eight healthy males (aged 19–33 years) completed two square-wave transitions of 6 min duration from unloaded cycling to a work-rate equivalent to ~80% of peak O₂ either with or without prior i.v. infusion of DCA (50 mg kg^–1 body mass in 50 ml saline). Pulmonary O₂ was measured breath-by-breath throughout all tests, and O₂ kinetics were determined using non-linear regression techniques from the averaged individual response to each of the conditions. Infusion of DCA resulted in significantly lower blood [lactate] during the baseline cycling period (means±SEM: control 0.9±0.1, DCA 0.5±0.1 mM; P<0.01) consistent with successful activation of PDC. However, DCA had no discernible effect on the rate at which O₂ increased towards the initially anticipated steady state following the onset of exercise as reflected in the time constant of the fundamental O₂ response (control 26.7±4.1, DCA 27.7±2.8 s). These results indicate that the principal limitation to oxidative metabolism following the onset of high-intensity, sub-maximal cycle exercise lies downstream from PDC and/or that muscle O₂ consumption is primarily under feedback control via the concentration of one or more of the reactants associated with ATP hydrolysis.     

Antidiuretic hormone—V2-receptor—aquaporin-2 system in rat kidneys during acute inflammation

Expression of antidiuretic hormone V₂-receptor, water channel protein aquaporin-2, and cytokines interleukin-1 and interleukin-6 was studied in the kidneys of rats with acute inflammation produced by intraperitoneal injection of lipopolysaccharide in a dose of 250 µg/100 g. Reduced expression of aquaporin-2 and V₂-receptor led to impairment of concentration capacity in the kidneys and decrease in urine osmolarity.Translated from Byulleten Eksperimentalnoi Biologii i Meditsiny, Vol. 138, No. 11, pp. 511–516, November, 2004     

Cardiac Purkinje fibres

Summary The influence of intracellular calcium concentration [Ca²⁺] _i on the steady state membrane currentsi was studied in a range of clamp potentials between –20 and –100 mV. Injection of CaCl₂ or Ca-EGTA (pCa 6) increasedi whereas injection of K-EGTA diminished it. The changes i were attributed to a change in steady state potassium conductance, g_K, by four arguments: i was restricted to potentials negative to –20 mV and depended on clamp potential in an inward rectifying manner. i displayed a reversal potential, E_rev, which followed log [K⁺]₀ with 60 mV for a tenfold change. Since E_rev obtained during Ca injection agreed with E_rev observed during EGTA injection the potassium driving force had to be constant. Wheng _K was blocked by superfusion with 20 mM Cesium neither CaCl₂ nor K-EGTA injection modifiedi .Supported by SFB 38, Membranforschung, project G2     

An electrophysiological study of angiotensin II regulation of Na-HCO3 cotransport and K conductance in renal proximal tubules

The effect of picomolar concentrations of angiotensin II (AII) was investigated in isolated perfused rabbit renal proximal tubules using conventional or pH-sensitive intracellular microelectrodes. Under control conditions cell membrane potential (V _b) and cell pH (pH_i) averaged –53.8±1.9 mV (mean±SEM,n=49) and 7.24±0.01 (n=10), respectively. AII (at 10^–11 mol/l), when applied from the bath (but not when applied from the lumen perfusate), produced the following effects: approximately 85% of the viable tubules responded with a small depolarization (+ 5.5±0.4 mV,n=43) which was accompanied in half of the pH_i measurements by a slow acidification (pH_i=–0.03±0.01,n=5). The remaining 15% responded with a small hyperpolarization (V_b=–3.1±0.4 mV,n=6). All changes were fully reversible and repeatable. Experiments with fast changes in bath HCO₃ or K concentrations, as well as measurements of the basolateral voltage divider fraction in response to transepithelial current flow, explain these observations as stimulation of a basolateral Na-HCO₃ cotransporter and of a basolateral K conductance. Both counteract in their effect onV _b, but can be individuated by blocker experiments with 4,4-diisothiocyanatostilbene-2,2-disulphonic acid (DIDS) and barium. Both the stimulation of Na-HCO₃ cotransport and the stimulation of the K conductance may result from down-regulation of the level of cyclic adenosine monophosphate in the cell.     

Effects of priming exercise intensity on the dynamic linearity of the pulmonary V̇O2 response during heavy exercise

Prior heavy-intensity exercise facilitates the pulmonary oxygen uptake (O₂) response during subsequent exercise, such that its kinetics returns towards first-order. To better understand this priming phenomenon, we investigated the effect of priming exercise, over a range of intensities, on the O₂ response to heavy-intensity cycle ergometry at a work rate of 50% [halfway between lactate threshold (LT) and O_2max]. Eight subjects performed two consecutive 6-min bouts separated by 6 min at 20 W. The first bout was each of: no warm-up control (CON), sub-lactate threshold (LT) at 80% of LT, and three supra-LT conditions (20%, 40%, and 60%). The O₂ response during the subsequent bout was evaluated using the effective time constant (), and the O₂ difference between minutes 3 and 6 (O_2(6–3)). The goodness-of-fit, indicative of first-order kinetics, was determined by the residual profile, and the mean square of errors (MSEr). The heart rate and blood lactate concentration ([La]r) just prior to the second bout were also measured. Compared with CON, and O_2(6–3) were significantly reduced following all supra-LT priming bouts, while the goodness-of-fit was significantly improved following 40% exercise. O_2(6–3) and [La]r were negatively correlated (P<0.05), unlike HR. In conclusion, prior exercise just above, but not below, LT facilitated the O₂ response in a threshold-like manner. Supra-LT priming exercise influenced the O₂ response allowing it to return to within as little as 12% from first-order (compared to ~50% in CON). The associated increases in circulating lactate and/or related factors seem to be centrally involved in this phenomenon.