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1 Deparmement of Medicine University of California, San Diego, La Jolla, California 92093; 2 Department of Radiology University of Pennsylvania, Philadelphia, Pennsylvania 19104; and 3 Copenhagen Muscle Research Centre, Rigshopitalet, Copenhagen, Denmark
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ABSTRACT |
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We studied muscle blood flow,
muscle oxygen uptake (
O2), net muscle CO
uptake, Mb saturation, and intracellular bioenergetics during
incremental single leg knee-extensor exercise in five healthy young
subjects in conditions of normoxia, hypoxia (H; 11% O2), normoxia + CO (COnorm), and 100% O2 + CO (COhyper). Maximum work rates and maximal oxygen
uptake (
O2 max) were equally reduced by
14% in H, COnorm, and COhyper.
The reduction in arterial oxygen content (CaO2)
(
20%) resulted in an elevated blood flow (Q) in the CO and H
trials. Net muscle CO uptake was attenuated in the CO trials.
Suprasystolic cuff measurements of the deoxy-Mb signal were not
different in terms of the rate of signal rise or maximum signal
attained with and without CO. At maximal exercise, calculated mean
capillary PO2 was most reduced in H and
resulted in the lowest Mb-associated PO2.
Reductions in ATP, PCr, and pH during H, COnorm, and
COhyper occurred earlier during progressive exercise than
in normoxia. Thus the effects of reduced CaO2 due to
mild CO poisoning are similar to H.
exercise; metabolism; CO toxicity; magnetic resonance spectroscopy; 31P; maximal O2 consumption; intracellular partial pressure of O2
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INTRODUCTION |
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THE STRONG AFFINITY of carbon monoxide (CO) for Hb has afforded researchers the opportunity to measure Hb mass and blood volume (5), examine O2 transport (12, 18), and most recently to manipulate blood Hb levels while independently manipulating arterial PO2 to study the control of skeletal muscle blood flow (9). Additionally, mild CO poisoning is an unavoidable consequence of cigarette smoking (36). The usefulness of CO as a tool is enhanced by the fact that unlike hypoxia (H), mild CO exposure does not stimulate the carotid body and does not result in an increase in cardiac output or ventilation (33). However, the validity of using CO in vascular research and the clinical consequences of mild CO poisoning are highly dependent on the magnitude of the diffusive movement of CO from the vascular to intracellular space and the subsequent intracellular consequences of any such movement.
In favor of limited CO movement and consistent with the normal physiological function of CO disposal (as a catalytic byproduct of heme), the ligand affinities for CO are the reverse of those for O2. Hence, Mb has a higher CO affinity than cytochrome oxidase and Hb has a higher affinity than myoglobin (Mb). Additionally, on the basis of the high affinity Hb has for CO, the major driving force for CO movement (CO partial pressure in the blood) should theoretically remain low with a mild level of Hb-CO. Despite this concept, both researchers and clinicians concern's regarding the exposure of muscle to CO have revolved around the effect of CO on O2 transport by interfering with Mb-facilitated O2 diffusion and the metabolic effects of CO binding with cytochrome oxidase (7, 12, 18). In fact, there are data that do indeed suggest that some CO, even at low levels (2-2.5% Hb-CO), moves from Hb to Mb during exercise (6). However, currently there is limited understanding of the extent to which CO moves into skeletal muscle and the intracellular effects of this potential CO movement.
Consequently, the purpose of this study was to combine invasive
vascular measures of arterial and venous blood and muscle blood flow
(Q) with noninvasive magnetic resonance spectroscopy (MRS) of both
deoxy-Mb and high-energy phosphates to determine both the intravascular
and intracellular effects of mild CO poisoning (
20% Hb-CO) in
humans during muscular work. Specifically, beyond the expected increase
in Q with decreased Hb-O2, we tested the following
hypotheses. 1) A 20% Hb-CO level will not reduce the intramuscular concentration of Mb ([Mb]) available for O2
binding. 2) Submaximally, muscle oxygen consumption
(
O2) will be unaffected by CO, whereas
maximal oxygen consumption (
O2 max)
will be attenuated by the effect CO has on O2 availability.
3) Reduced O2 availability will reduce
intracellular PO2 in the presence of CO.
4) The reduction in O2 availability with CO will
cause an early perturbation of muscle bioenergetics, as measured by intramuscular levels of phosphocreatine (PCr), ATP, and pH.
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METHODS |
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Subjects. Seven recreationally active males (age mean ± SD): 26 ± 1 yr; weight: 77 ± 4 kg; and height: 178.2 ± 4 cm, volunteered to participate in this study. All but one of the subjects were nonsmokers. The single smoker was a "recreational" smoker only (0-4 cigarettes/day). Informed written consent was obtained according to the Code of Ethics of the World Medical Association (Declaration of Helsinki), the Ethics Committee of Copenhagen and Frederiksberg communities, and the University of Pennsylvania Human Subjects Committee requirements. All subjects were successfully studied during the catheter-based investigations and five of these subjects completed the MRS portion of the work.
Exercise modality and protocol. Single leg knee-extensor exercise, designed to limit work to the quadriceps muscles of the left leg (24), was employed. Before the exercise protocol, all subjects were familiarized with the testing environment and ergometer. Briefly, subjects were semirecumbent in a chair placed in the laboratory for the catheter-based studies or within a 2.0-Tesla Oxford imaging magnet for the MRS studies. A special ankle boot placed on their left leg connected them by a bar to the ergometer (24). Contractions of the quadriceps muscles caused the lower part of the leg to extend from an angle of 90° to 170°. Therefore, the lower leg traveled with an arc-shaped trajectory of ~80°. The momentum of the ergometer passively returned the relaxed leg to the start position and, as a result, the quadriceps muscle was functionally isolated (23). The graded exercise tests required subjects to maintain each work rate for 180 s, after which the work rate was incremented. The subjects continued until they were unable to maintain a cadence of 60 rpm for the entire 3 min. During the catheter-based studies, heart rate and arterial blood pressure were recorded continuously and muscle Q was measured (thermodilution) at minutes 2 and 3 of exercise at each work level. Arterial and venous blood samples were withdrawn after Q measurements. During magnet-based studies, data were collected continuously, with the 31P and 1H data being interleaved every 4 s. The exercise bouts involving CO were always performed last, due to the relatively long elimination period required to return to low Hb-CO levels; within this logistical restraint, the H and normoxia and normoxia + CO (COnorm) and hyperoxia + CO (COhyper) treatments were performed in a balanced order across subjects. One hour before the exercise tests in the magnet, total ischemia in the left leg was induced by a suprasystolic cuff to allow the assessment and calibration of the Mb signal. The assessment of the cuffed Mb signal in the presence of CO was performed with the subject on the rebreathing system 1 h before the COnorm exercise bout.
H and CO treatments.
Before and during exercise in both the H and CO trials, subjects
breathed in a closed-circuit system (previously illustrated in Ref.
9). This rebreathing system consisted of a 4-liter custom-made chamber containing CO2 absorber (Sofnolime,
Molecular Products, Essex, UK), a 10-liter reservoir, a two-way
breathing valve (Hans-Rudolph, Kansas City, MO), and two hoses
connecting the chamber and the breathing valve. The inspired gas in the
reservoir was manually adjusted using gas regulators connected to two
tanks containing 11% O2 in N2 and 100%
O2, respectively, while O2 and CO2
were monitored online (Beckman OM11 and LB2, Fullerton, CA). During the
rest period after the hypoxic trial, CO (95% purity) was administered
through an extension line connected to the two-way valve, using plastic
syringes. A series of CO boluses estimated to increase Hb-CO by
10-15% was initially administered and venous Hb-CO was
measured spectrophotometrically (OSM-3 Hemoximeter, Radiometer,
Copenhagen, Denmark) after 20 min via a venous blood sample. A second
CO dose aimed to increase Hb-CO to
20% was then administered (total
CO administered 312 ± 25 ml).
MRS: [Mb], intracellular PO2, and
31P.
Spectra were collected from the muscle region below the 7-cm diameter
surface coil double-tuned to proton (85.45 MHz) and phosphorus (34.59 MHz) placed over the rectus femoris portion of the quadriceps group
(35) ~20-25 cm proximal to the knee. For these
studies, this "sensitive region" was <100 cm3 of
muscle, which isolated signal detection predominantly to the rectus
femoris (1). Details of the theory behind oxygen-sensitive Mb signals have been published previously (3, 24).
Briefly, the heme iron exhibits oxygen-dependent spin states that in
turn influence nearby protons. The N-
proton on proximal histidine F8, one of the ligands coordinated to the iron, is particularly sensitive to these changes. When oxygen is bound to the active site,
the resonance of this proton is hidden beneath the dominant water
signal. However, when Mb becomes deoxygenated, changes in the iron spin
state shift this peak to a temperature-dependent position that is
clearly distinct from all other resonances. Fractional deoxy-Mb
(fdeoxy-Mb) during exercise was determined by normalizing
the signal areas (integration under the curve) to the average signal
areas obtained between the 10th and 14th min of cuff ischemia
at suprasystolic pressure (270 mmHg). Intramuscular O2
depletes within ~8 min of occlusion (39). Therefore, the
plateaued signals obtained during the last 2 min of cuff occlusion
represent complete deoxygenation of Mb that are used to estimate total
Mb content within the muscle. Conversion to PO2
values were then calculated from the oxygen binding curve for Mb:
PO2 = fMbO2 · Mb
P50/fdeoxy-Mb, where
fMbO2 is the fraction of Mb that is oxygenated
and P50 is the O2 pressure where 50% of the Mb
binding sites are bound with O2. The temperature-dependent
Mb half saturation (P50) of 3.2 mmHg was used
(32).
Catheter-based vascular measurements across the working quadriceps muscle. Two catheters were placed using the Seldinger technique, one in the femoral vein and the other in the femoral artery of the right leg. Both catheters were positioned in close proximity to the inguinal ligament and femoral arterial and femoral venous blood samples were collected from these sites. To facilitate the thermodilution technique for determining Q (2), both venous and infusate temperatures were measured continuously during saline infusion (15-20 s, 110 ml/min; Harvard pump 44, Harvard Apparatus, Millis, MA) via thermistors (Edslab, TD probe 94-030-2.5F) connected to a custom-made electronic box, which was interfaced to a Power Macintosh computer using a MacLab/16 s data-acquisition system (ADInstruments, Sydney, Australia). The venous thermistor was positioned ~10 cm beyond the tip of the 8-cm catheter. Muscle Q was calculated using a heat balance equation.
Hb concentration, Hb saturation, and Hb-CO were determined spectrophotometrically (OSM-3 Hemoximeter, Radiometer, Copenhagen, Denmark). PO2 was determined with the Astrup technique (ABL5, Radiometer). To facilitate the calculation of net CO uptake across the exercising muscle, arterial and venous Hb concentrations (g/dl) were converted to millimoles per liter of Hb and then each multiplied by the femoral arterial and femoral venous fraction of Hb-CO, respectively. Net CO uptake was then calculated as the product of muscle Q and the arterial venous (a-v) Hb-CO difference (mmol/min). Both arterial oxygen content (CaO2) and venous oxygen content (CvO2) were calculated as (1.39 × [Hb] × O2 saturation) + (0.003 × PO2) and CvO2 was subtracted from CaO2 to provide a-v O2 difference. Skeletal muscle
O2 was calculated as the product of
muscle Q and this arterial and venous O2 content difference.
Arterial blood pressure was continuously monitored in the femoral
artery in the inguinal region (40-60 cm below the heart) by a
pressure transducer (Pressure Monitoring Kit, Baxter). Mean arterial
blood pressure was computed by integration of each pressure curve.
Muscle O2 transport conductance and mean capillary
PO2 calculations.
With the use of the measured intracellular PO2
values, Hill n, and P50 values muscle
O2 transport conductance (DO2) and
mean capillary PO2
(PcapO2) were calculated as described
previously (38) at maximum work rate. Briefly, a numerical
integration procedure is used to determine that value of
DO2, assumed constant along the capillary,
which produces the measured femoral venous PO2,
given the measured arterial PO2. As these
calculations used the measured Mb-associated
PO2, they were no longer burdened by the
assumption of a low intracellular PO2 at
maximal work rate (38). An additional, and at this
time unavoidable, assumption of this calculation is that the only
explanation of O2 remaining in the femoral venous blood is
diffusion limitation of O2 efflux from the muscle
microcirculation. Perfusion/
O2
heterogeneity and perfusional or diffusional shunt are considered
negligible. To the extent that these phenomena do not contribute
O2 to femoral venous blood, the parameter
DO2 is a conductance coefficient that expresses
the diffusing capacity that would be required to achieve the
measured
O2 max, assuming only
diffusion limitation. This assumption cannot be avoided currently for
the lack of specific means for detecting
perfusion/
O2 heterogeneity and shunt in this model. Mean capillary PO2 is the numerical
average of all PO2 values computed, equally
spaced in time, along the capillary from the arterial to the venous end.
Statistical analyses.
Multivariate ANOVA was used to determine differences within and between
treatments across multiple work rates, with Bonferroni adjusted
t-tests used to identify the differences. One-way
repeated-measures ANOVA was performed to determine differences at a
single work intensity (e.g., maximal effort), followed by Bonferroni
adjusted t-tests used to identify the differences. When
appropriate, significant differences were also identified using paired
t-tests. Statistics were performed on commercially available
software (SPSS, Chicago, IL). Variables were considered significantly
different when the P value was
0.05.
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RESULTS |
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H and CO levels. The level of H was maintained at 11-12% throughout the H trials. The mean levels of Hb-CO in the COnorm and COhyper conditions were 20.1 ± 0.4 and 20.0 ± 0.7%, respectively. Immediately before suprasystolic cuff inflation and the subsequent measurement of the maximal deoxy-Mb signal in normoxia, the mean Hb-CO level was 2.0 ± 0.1%. All subjects tolerated these procedures well, neither reporting nor showing signs of discomfort.
Deoxy-Mb signal.
At rest, the intramuscular oxygen stores depleted within 6-8 min,
as measured by the appearance of the deoxy-Mb signal (4). Thus the signals from this point until the blood pressure cuff release
represent a steady-state deoxygenation as illustrated in Fig.
1. The developing deoxy-Mb signal
intensity over time during the cuff occlusion is indicative of oxygen
uptake and was not different with or without the CO load
(P = 0.3; Fig. 1). The maximum deoxy-Mb signal
intensity achieved during the suprasystolic cuff occlusion was also not
different with and without the CO load (P = 0.2)
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Intracellular PO2.
At the lower work intensities (<60% of normoxic work rate), a
quantitative assessment of the group average intracelluar
PO2 was limited to two to four subjects in each
condition. This was a consequence of relatively high intracellular
PO2 values and the average signal-to-noise of
the deoxy-Mb signal achieved in this study (5:1). Hence, relatively
small deoxy-Mb signals (15-20% of cuff) were lost within the
noise of the measurement. Intracellular PO2
fell somewhat variably between subjects with the continued increases in
work rate from 40 to 60% of normoxic maximum (Fig. 2). Beyond 60% of normoxic maximum, all
subjects produced a clear and measurable deoxy-Mb signal, and the fall
in intracellular PO2 ceased in all conditions
and a plateau in intracellular PO2 of varying
lengths, dependent on work rate achieved, was clearly apparent (Fig.
2). During the hypoxic condition, intracellular PO2 fell to a significantly lower level
(3.3 ± 0.7 mmHg) (P = 0.03) at its nadir than the
three other exercise trials (normoxia = 4.9 ± 0.9 mmHg;
COnorm = 5.6 ± 0.9 mmHg;
COhyper = 5.0 ± 0.7 mmHg).
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Bioenergetics.
In normoxia, PCr depleted from initial resting levels linearly with
increasing work rate. In H, COnorm, and COhyper
conditions PCr fell with a similar slope to normoxia until
40% of
the maximum normoxic work rate; beyond this point the fall in PCr
significantly increased such that the same level of PCr as normoxia was
achieved at only 86-87% of the normoxic work rate (Fig.
3A). A similar pattern was
apparent in terms of intracellular pH, with a greater rate of pH fall
evident in H, COnorm, and COhyper than during the normoxic exercise culminating in a similar minimum pH for normoxia,
COnorm, and COhyper. In contrast, during
hypoxic exercise, the ultimate pH achieved was significantly lower than
all other conditions (Fig. 3B) (P = 0.02).
ATP remained relatively constant in all conditions until
40% of the
maximum normoxic work rate, at which point ATP levels fell more rapidly
in the H, COnorm, and COhyper conditions
compared with the normoxic ATP fall (Fig. 3C). The normoxic
ATP fall at maximum exercise was equaled at 86-87% of this
maximum in the H, COnorm, and COhyper
conditions. It is interesting to note that in one subject, the classic
concept of a relatively constant ATP level, even during high-intensity exercise, was supported by moderate ATP fall (6%) even at maximal exercise. However, in the majority of cases ATP levels fell
significantly to average
70% of the resting values, indicating the
high metabolic demand attainable with this single leg knee-extensor
exercise model. The water resonance did not move by >0.1 ppm or
increase in width >2 Hz for any of the subjects, indicating that
motion was limited by the leg yoke designed for the ergometer and did not degrade the signal during the study.
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Q, a-v O2 difference, and
O2 across the exercising muscle.
During submaximal work rates, the a-v O2 difference was
reduced from the normoxic value (13.4 ± 0.2 ml/dl) to 11.3 ± 0.3, 10.7 ± 0.3, and 10 ± 0.2 ml/dl in H,
COhyper, and COnorm, respectively (P = 0.01). At maximal exercise a-v O2
difference was reduced to an even greater extent from the normoxic
value (16.2 ± 0.5 ml/dl) to 13.0 ± 0.4, 12.2 ± 0.5, and 11.4 ± 0.3 ml/dl in H, COhyper, and
COnorm, respectively (P = 0.005). Muscle Q
was significantly elevated for a given work rate in H,
COhyper, and COnorm (Fig. 4B) such that the relationship
between
O2 and work rate was unaltered
in the four trials, but was truncated in all but the normoxic exercise
(Fig. 4B). At maximal effort, muscle Q was significantly elevated above the other trials in the COnorm condition
(Fig. 4B) (P = 0.01). Mean arterial pressure
increased, as expected, across work rates, but was unaltered across the
four trials; thus leg vascular conductance was elevated in the H,
COhyper, and COnorm trials. Heart rate also
increased across work rates and was significantly elevated above the
normoxic values more in H (
10-15 beats/min) than in the CO
trials (
5-10 beats/min) (P = 0.03). At maximal exercise, this difference across trials was no longer significant.
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Maximal work rate. As illustrated in Figs. 2-4, maximal work rate was significantly and equally compromised in all studies during the H, COhyper, and COnorm trials compared with the normoxic exercise. Specifically, in the intravascular studies (which provided absolute work rates), the maximum work rate fell from 73 ± 6 W (100%) in the normoxia to 63 ± 5 W (87%) in H, 63 ± 5 W (86%) in COnorm, and 63 ± 5 W (86%) in COhyper (P = 0.008; Fig. 4).
Net CO uptake from the vascular space. The measurement of arterial and venous Hb-CO across the leg revealed a significant CO uptake in the normoxic and hypoxic conditions that increased with increasing work intensity of the quadriceps muscles (Fig. 4C). This was in contrast to the almost zero net CO uptake in the COnorm and COhyper conditions (Fig. 4C).
Muscle O2 transport conductance and
PcapO2.
The normoxic and COhyper had similar
PcapO2 values, both of which were higher than
the other two conditions. The PcapO2 for COnorm was lower than normoxia and COhyper but
was greater than the PcapO2 in H (Fig.
5, top). As the Mb-associated
PO2 was invariant across the normoxic,
COhyper, and COnorm conditions, the gradient from blood to cell was smallest in the COnorm condition due
to its having the lowest PcapO2. Interestingly,
although the H condition had an even lower
PcapO2 than COnorm, the driving
PO2 gradient from blood to cell was maintained
by the reduced intracellular PO2 recorded
in H (Fig. 5, top). The analysis of
PcapO2 in relation to changes in
O2 max results in the assessment of
muscle DO2 as illustrated in Fig. 5,
bottom. All conditions, except COhyper, produced
similar maximal DO2 values and therefore fell
on a line passing through the origin.
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DISCUSSION |
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Directly testing the four original hypotheses, this study
determined the following. 1) Hb-CO levels of 20% do not
influence Mb-O2 binding as indicated by the unaltered
deoxy-Mb signal during total cuff occlusion. 2) Resting
skeletal muscle metabolic rate, as measured by the rate of appearance
of the deoxy-Mb signal during cuffing, and muscle
O2 during submaximal exercise was
unaffected by the presence of 20% Hb-CO. However,
O2 max was significantly attenuated in
the presence of CO, as seen in H. 3) Unlike H, which resulted in a similar fall in CaO2, the CO load
did not result in a significant decrement in intracellular
PO2 when compared with normoxia. 4)
The 20% Hb-CO altered exercising muscle bioenergetics, as measured by
pH, PCr, and ATP levels, in a very similar fashion to H, but with a
better defense of intracellular pH at maximal exercise. In addition to
the original hypotheses, this study documented that there was less net
uptake of CO from the blood to tissue during the 20% Hb-CO trials than
during those with 1-2% Hb-CO levels in normoxia and H. Thus it
can be concluded that a mild CO load does reduce maximal work rate and
muscle
O2 max; however, on the basis of
the current measurements, this level of CO appears to have benign
intracellular effects. These effects are most likely secondary to
limited maximal O2 availability, similar to those
associated with H, and not due to direct metabolic CO poisoning per se.
Therefore, the mild CO loads associated with smoking appear to have no
direct cellular effects, and CO as a vascular research tool is well
suited for use in human biomedical studies.
Deoxy-Mb signal and CO. When CO binds to Mb, the deoxy-Mb signal is attenuated and the reciprocal signal for Mb-CO increases (8). Hence, although the Mb-CO signal was not measured in the present study, an increased Mb-CO would have been reflected by a reduced deoxy-Mb signal. This did not occur despite the scenario of total occlusion for 12 min in which the intracellular PO2 had fallen to an extremely low level, perhaps even zero (26, 39). This would be considered a perfect scenario in which to invoke CO movement into the cell, if it were going to occur, as CO moves much more readily toward hemoproteins in a reduced state. During exercise, where Mb typically desaturates to only 50% of the level attained during the cuff procedure (25, 26, 28), there is even less likelihood of CO binding Mb. This is also supported by the similarity of the deoxy-Mb signal attained during exercise in the normoxic, COnorm, and the COhyper conditions (converted to PO2 in Fig. 2).
Additionally, here it is important to recognize that within a given volume of muscle there are differences in both [Hb] and [Mb] and binding capacities: with the measured value of 15 g/dl of Hb and assuming an average circulating blood volume of 6,000 ml, 20% of which perfuses 25 kg of resting muscle (34), and a Mb concentration of 5 mg/ml (21), we can estimate that during the suprasystolic cuff procedure the volume of tissue under the MRS coil (100 ml) would contain ~0.75 g of Hb (5 ml of blood) and 0.5 g of Mb. Hb has approximately half the molecular weight of Mb, but has four times the O2/CO binding sites. Therefore, the Hb has ~200% more O2/CO binding capacity than Mb in the same tissue volume. Thus, if the 20% Hb-CO were to unload to Mb, this would decrease the deoxy-Mb signal by ~60% (i.e., a 3% fall in deoxy-Mb signal per 1% fall in Hb-CO). With such a large effect size, the statistical power of this test is high (power = 0.80), despite some variance in the deoxy-Mb measurement and the limited number of subjects (n = 5).CO and O2 transport into the muscle cell.
The CO load resulted in a clear reduction O2 extraction
(CaO2
CvO2)
(Fig. 5, middle); this is in agreement with previous studies
using CO that have proposed that the mechanism may involve Mb blockade
when CO is present (12, 18). The present study affords the
assessment of intravascular and intracellular processes and clearly
refutes this mechanism by the observed reduction in O2
extraction with CO present, but has no effect on functional [Mb].
O2 remains constant (Fig.
4A).
At maximal exercise, normoxic muscle
O2 max was attenuated in both CO
conditions and H (Figs. 4B and 5, middle and bottom). The level of O2 delivery at maximal
exercise was not reduced in the CO conditions, whereas it was clearly
lower in H (Fig. 5, middle). This was probably due to an
increased vasodilatory response to the reduced O2
availability (via changes in the O2-Hb dissociation curve)
above and beyond the fall in CaO2 that was matched with H. This clearly illustrates the importance of the O2-Hb dissociation as a determinant of
O2 max. In terms of the diffusional
component of O2 supply limiting
O2 max, these data illustrate that
despite the restoration of an equivalent calculated
PcapPO2 in COhyper, muscle
O2 max remained compromised. As
there is no evidence of CO uptake or negative intracellular effects of
CO (which would explain a leveling off in
O2 max), it is likely that both the
left shift of the O2-Hb dissociation curve and the
reduction in the Hill n have combined to attenuate
DO2 in COhyper that limits
O2 max (Fig. 5, bottom).
Intracellular PO2 and CO.
The calculation of intracellular PO2 or, more
specifically, the ultimate plateau in intracellular
PO2 attained during high-intensity exercise
provides an interesting window from which to view the effect of CO on
intracellular O2 levels (Fig. 2). Prior to
60% of
maximal normoxic work rate, the intracellular
PO2 values across conditions were statistically
indiscernible. However, consistent with previous reports (24,
27), beyond
60%, the hypoxic exercise bout resulted in
significantly lower intracellular PO2 values than the normoxic exercise. Somewhat surprisingly, intracellular PO2 in the COnorm condition did not
fall to the level of hypoxic exercise, but was maintained at the
normoxic level. The fall in intracellular PO2
during COnorm was anticipated based on the assumption of a
lowered mean capillary PO2, the expected result
of the left-shifted Hb-O2 dissociation curve in the
presence of CO. It is possible that the increased O2
delivery recorded in both CO trials was enough to offset this potential
fall in intracellular PO2. However, as
illustrated in Fig. 5, top, it can be implied that although CO reduced the PcapO2, the effect was not great
enough in COnorm to reach what may be a critical
intravascular PO2 achieved in H. Consistent
with this concept of a reduced driving force of O2 from
blood to cell in the presence of CO is the matching of PcapO2 in COhyper and normoxia
(Fig. 5, top). As a result, COhyper failed to
elevate intracellular PO2 as previously
reported in simple hyperoxia in similar subjects (25).
Independent intracellular pH measurements, collected simultaneously,
support these intracellular PO2 observations
because of the previously recognized concept that a decreased
intracellular PO2 will be accompanied by a
decreased intracellular pH (28). Maximal exercise during H
was the only condition in which pH was significantly reduced,
suggestive of an increased lactate efflux due, perhaps in part, to an
altered intracellular oxygenation state (28). Similar to
previous work with H, the measurement of muscle bioenergetics during
COnorm, COhyper, and H revealed a more rapid
fall in PCr, ATP, and pH when compared with normoxia (14).
However, pH and the deoxy-Mb signal in the hypoxic exercise bout were
the only MRS variables that did not reach the same ultimate
end-exercise level in all conditions (Figs. 2 and 3).
CO uptake across the muscle.
In addition to the lack of an effect of CO on the deoxy-Mb signal the
vascular data (Fig. 4C) offer more compelling evidence that
CO at the level that binds
20% of the available Hb exhibits no net
movement out of the vascular space. This is in contrast to the normoxic
and hypoxic conditions where Hb-CO levels were
2% due to
environmental CO levels (Fig. 4), where there was measurable net CO
uptake that increased with increasing exercise intensity. These latter
observations are in agreement with the previous results of Clark and
Coburn (6) who, aiming not to compromise
O2 max but wishing to use CO uptake and
its assumed binding to Mb to determine intracellular
PO2, invoked only 2-2.5% levels of Hb-CO in human subjects. Under these conditions, CO moved from the vascular space to a greater extent both with increasing work rate and with the
reduction in the fraction of inspired O2. It is clear from the current lowest Hb-CO conditions (1-2% Hb-CO), Clark and
Coburn's work (6), and the most recent MRS work of Glabe
et al. (8) that, under the appropriate conditions, CO can
move into muscle tissue and potentially bind Mb to some extent.
However, the present study provides no evidence of net CO movement from
blood to skeletal muscle or Mb binding with Hb-CO levels of
20%.
The explanation for this is likely related to the interplay between
several key factors: the PCO2 in the blood, the
degree to which the Hb-O2 dissociation curve is shifted to
the left, and the level to which Mb is deoxygenated. In the CO
conditions, intracellular PO2 during high-intensity work was not reduced compared with normoxic levels; the
PCO2 in the blood would be very low due to the
Hb sink and the leftward shift in the O2 dissociation curve
not only increases the affinity of Hb for O2 but also
increases the affinity of Hb for CO (diminishing off-loading at the
tissue). Hence, it is suggested that the combination of these variables
acted to protect against CO movement from blood to tissue (at the 20%
Hb-CO level), while elevated Q facilitated an unaltered oxygen flux and
consumption for a given work rate (Fig. 4A).
CO and blood volume calculations. The use of CO to assess Hb mass and blood volume is not universally accepted because of potential CO loss from blood to cell. The currently employed practice of elevating Hb-CO levels by 5-15% appears appropriate; however, the present data positively support the use of the higher Hb-CO levels, as this appears to minimize CO loss into the tissue. Consequently, with the proviso that moderate levels of CO are used, the current data indicate and support prior predictions that it is not necessary to correct Hb and blood volume measurements for loss of CO to Mb (5).
ATP fall at maximal exercise. As many studies have failed to clearly perturb the level of ATP during exercise (20), it may concern some to see a significant reduction in ATP in the current data. In fact, there are a considerable number of studies that have documented a significant fall in ATP in the range of 25% as a consequence of high-intensity muscular exercise (11, 15, 16). However, even more recently, a similar ATP fall in type I muscle fibers was reported in an elegant study by Karatzaferi et al. (17), but this study also documented an ATP fall of 80% for the type II muscle fiber population. This has significant implications for the current study, in which we report an average fall in ATP as great as 38% in the COnorm condition because there is no doubt that the muscles being studied are made up of a roughly equal number of slow- and fast-twitch fibers (31). It is important to recognize that, as in other studies, the attainment of ATP fall at maximal exercise was quite varied: subject A, ATP 98% of rest, PCr 11.3% of rest, and pH 6.68; subject B, ATP 48% of rest, PCr 1.3% of rest, and pH 6.50. Not only do these data illustrate the heterogeneity of the data, but they also refute the issue of a large signal loss (that would be evident across the complete spectrum) due to potential movement during high-intensity exercise. In subject A, it is clear that PCr demonstrated a significant fall that was not accompanied by the fall in ATP that would occur were this fall due simply to signal loss. It should also be recognized that in the current study using knee-extensor exercise, the intracellular pH falls to very low levels, which is not the case in previous studies that have revealed invariant ATP levels, even at maximal exercise (20).
Experimental limitations. Experimental limitations associated with this study include a small sample size (n = 5) that was the result of the complex, dual-site investigation, and invasiveness of the catheter-based assessments. However, it should be noted that previously both interesting and statistically significant results have been reported with a similar combination of exercise, MRS, and vascular methodologies and small sample sizes (n = 5) (25) and exercise and MRS alone (n = 4) (20).
In summary, the use of CO at mild levels has many biomedical uses that depend on limited transport into tissue and therefore zero or minor intracellular effects. With the use of a combination of 1H- and 31P-MRS in conjunction with vascular measures of
O2 and net CO uptake, it has
been demonstrated that there is immeasurable CO movement from blood to
muscle. Consequently, the physiological consequences of inducing Hb-CO
levels of
20% are similar in many ways to the benign effects of
hypoxic exercise.
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ACKNOWLEDGEMENTS |
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We thank the dedicated subjects who took part in this complex multisite investigation.
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FOOTNOTES |
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This research was supported by the National Heart, Lung, and Blood Institute (HL-17731) and the Danish National Research Foundation (504-14).
Address for reprint requests and other correspondence: R.S. Richardson, Dept. of Medicine, 0623, UC, San Diego, 9500 Gilman Drive, La Jolla, CA 92093 (E-mail: rrichardson{at}ucsd.edu).
The costs of publication of this article were defrayed in part by the payment of page charges. The article must therefore be hereby marked "advertisement" in accordance with 18 U.S.C. Section 1734 solely to indicate this fact.
July 11, 2002;10.1152/ajpregu.00226.2002
Received 22 April 2002; accepted in final form 11 July 2002.
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