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J Appl Physiol 94: 353-357, 2003. First published October 11, 2002; doi:10.1152/japplphysiol.00559.2002
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Vol. 94, Issue 1, 353-357, January 2003

INNOVATIVE TECHNIQUES
Assessment of O2 uptake dynamics in isolated single skeletal myocytes

Casey A. Kindig, Kevin M. Kelley, Richard A. Howlett, Creed M. Stary, and Michael C. Hogan

Division of Physiology, Department of Medicine, University of California, San Diego, La Jolla, California 92093-0623


    ABSTRACT
TOP
ABSTRACT
INTRODUCTION
METHODS
RESULTS
DISCUSSION
REFERENCES

The purpose of this research was to develop a technique for rapid measurement of O2 uptake (VO2) kinetics in single isolated skeletal muscle cells. Previous attempts to measure single cell VO2 have utilized polarographic-style electrodes, thereby mandating large fluid volumes and relatively poor sensitivity. Thus our laboratory has developed an ~100-µl, well-stirred chamber for the measurement of VO2 in isolated Xenopus laevis myocytes using a phosphorescence quenching technique [Ringer solution with 0.05 mM Pd-meso-tetra(4-carboxyphenyl)porphine] to monitor the fall in extracellular PO2 (which is proportional to cellular VO2 within the sealed chamber). VO2 in single living myocytes dissected from Xenopus lumbrical muscles was measured from rest across a bout of repetitive tetanic contractions (0.33 Hz) and in response to a ramp protocol utilizing an increasing contraction frequency. In response to the square-wave contraction bout, the increase in VO2 to steady state (SS) was 16.7 ± 1.3 ml · 100 g-1 · min-1 (range 13.0-21.9 ml · 100 g-1 · min-1; n = 6). The rise in VO2 at contractions onset (n = 6) was fit with a time delay (2.1 ± 1.2 s, range 0.0-7.7 s) plus monoexponential rise to SS (time constant = 9.4 ± 1.5 s, range 5.2-14.9 s). Furthermore, in two additional myocytes, VO2 increased progressively as contraction frequency increased (ramp protocol). This technique for measuring VO2 in isolated, single skeletal myocytes represents a novel and powerful investigative tool for gaining mechanistic insight into mitochondrial function and VO2 dynamics without potential complications of the circulation and other myocytes.

phosphorescence quenching; Xenopus laevis; skeletal muscle; oxygen uptake kinetics


    INTRODUCTION
TOP
ABSTRACT
INTRODUCTION
METHODS
RESULTS
DISCUSSION
REFERENCES

THE STUDY OF O2 uptake (VO2) at the transition to a higher metabolic rate offers valuable insight into mechanisms regulating metabolic control during muscle contractions. In this regard, VO2 kinetics measured at the mouth (pulmonary) have very similar characteristics to that seen across skeletal muscle (1, 10). However, Whipp et al. (28) speculate that metabolic heterogeneities associated with skeletal muscle fiber type and fiber-type recruitment make metabolic control inferences based on pulmonary VO2 kinetic profiles difficult. In addition to fiber-type issues, concerns within intact, exercising muscle, including convective O2 delivery, O2 delivery-to-VO2 matching, and O2 diffusion, further compound this issue (7). At the other end of the spectrum, although metabolic control has been studied extensively in isolated mitochondria, these preparations reveal that mitochondria do not necessarily perform the same in culture as in vivo (e.g., Refs. 24, 29). Thus the ability to study VO2 dynamics in single, intact myocytes would represent a powerful tool that would either eliminate or allow control of the aforementioned potentially confounding variables.

With the use of polarographic-style O2 electrodes, VO2 has been measured previously in both isolated muscles (e.g., Refs. 6, 14) and myocytes (e.g., Refs. 5, 25). However, these investigations were hindered by inherent complications associated with the O2 electrode, including 1) the necessity for relatively large chamber fluid volumes, resulting in a low signal-to-noise ratio; 2) intrinsic O2 consumption; and 3) inertia (slow response times). An optical method for extremely rapid assessment of PO2 using O2-dependent quenching of phosphorescence has been pioneered by Wilson (for review, Ref. 30). This technique has been adapted for measurement of both in vitro and in vivo PO2 within biological systems (3, 4, 11, 23, 31). This present investigation was undertaken to develop a method using phosphorescence quenching techniques (to avoid complications associated with polarographic style O2 electrodes) for rapid assessment of VO2 in isolated single living skeletal myocytes with high signal-to-noise resolution across the rest-to-contractions transition.


    METHODS
TOP
ABSTRACT
INTRODUCTION
METHODS
RESULTS
DISCUSSION
REFERENCES

Adult female African clawed frogs (Xenopus laevis) were doubly pithed and decapitated. Isolated single skeletal myocytes with tendon intact were microdissected from the lumbrical muscles (II-IV). Myocyte fiber type was assessed during dissection according to twitch characteristics (i.e., both the speed of contraction/relaxation rate as well as fatigue rate in response to ramp protocol) and appearance under dark-field illumination (both size and opacity of individual fibers) (26). All procedures were approved by the University of California-San Diego Animal Care and Use Committee and conform to National Institutes of Health guidelines.

Principle of O2-dependent phosphorescence quenching. The O2-dependent quenching of phosphorescence is an optical method for measuring PO2 (31) that can be described quantitatively by the Stern-Volmer equation where
&tgr;<SUB>o</SUB>/&tgr;=1+k<SUB>q</SUB><IT> · &tgr;</IT><SUB>o</SUB><IT> · </IT>P<SC>o</SC><SUB>2</SUB> (1)
thus
P<SC>o</SC><SUB>2</SUB><IT>=</IT>(<IT>&tgr;<SUB>o</SUB>/&tgr;−</IT>1)<IT>/</IT>(<IT>k</IT><SUB>q</SUB><IT> · &tgr;</IT><SUB>o</SUB>) (2)
where tau o and tau  are the phosphorescence lifetimes at anoxia and a given PO2 and kq, the quenching constant (in Torr), is a second-order rate constant that is related to the frequency of collisions between O2 and the excited triplet state of the porphyrin and the probability of energy transfer when collisions occur. The constants for the compound used, Pd-meso-tetra(4-carboxyphenyl)porphine bound to albumin in solution have been well characterized (17). Pd-based O2 probes have very little pH or temperature dependence within the physiological range (30).

The chamber was calibrated with PO2 values ranging from 0 Torr (Ringer solution bubbled with 100% N2) to 159 Torr (room air) at 20°C. The measured phosphorescence lifetime decay in the anoxic environment and the relationship between measured PO2 and the corresponding phosphorescence lifetime as PO2 increased were used to calculate the phosphorescence quenching parameters. From this calibration, kq was set at 180 Torr/s and tau o at 601 µs.

The phosphorescence quenching of the porphyrin probe was measured through a system consisting of a flash lamp (Oxygen Enterprises, Philadelphia, PA), a 425-nm band-pass excitation filter, a 630-nm cut-on emission filter, and a photomultiplier tube for collection of the phosphorescence. To calculate phosphorescence lifetimes from the porphyrin probe, the phosphorescence-decay curves from a series of five flashes (15 Hz) were averaged, and a monoexponential function was fit to the subsequent best-fit decay curve (Medical Systems Analysis software, Greenvale, NY). Measurements were taken every 2 s.

Measurement of VO2. Myocyte VO2 was measured from the change in PO2 in the Ringer solution (with 0.05 mM Pd-porphyrin probe bound to bovine serum albumin) within a sealed chamber (described below) on the basis of the supposition that the fall in Ringer solution PO2 is due solely to O2 uptake from the myocyte. Thus VO2 can be calculated from the fall in PO2 where O2 solubility in physiological Ringer solution is 0.03015 ml O2 /ml at 20°C and 760 Torr (2). The chamber (100 µl volume) was constructed of 0.5-cm Lucite on four sides, whereas the top and bottom are composed of glass. The top is removable and sealed with silicon gel. The chamber has dual infusion-withdrawal ports with a platinum post on one end. The platinum post serves as the site for a stainless steel stirrer (dielectrically coated and driven by a rotating magnet located outside the chamber) and connection site for the platinum clip fastened to the myocyte tendon. The other end of the chamber has a 0.5-mm (ID) port (sealed from the atmosphere with silicon gel) through which a thread attached to the contralateral tendon passes. The thread is fastened to an external, adjustable force transducer (model 400A, Aurora Scientific, Aurora, Ontario, Canada), which is coupled to a data acquisition system (AcqKnowledge, Biopac Systems, Santa Barbara, CA) for subsequent analysis.

Experimental protocol. After microdissection, the isolated myocyte was placed in the chamber. All air bubbles were removed, the chamber was sealed as described above, and optimum muscle length was set on the basis of maximal tetanic force output. Fibers were stimulated electrically to induce direct tetanic muscle contractions (50 impulses/s of 2-ms duration, 200-ms train duration, 8-10 V). Isolated myocytes were then subjected to a contraction protocol consisting of either 1) 3 min at 0.33 Hz (n = 6) or 2) incremental ramp protocol (2-min intervals) from 0.1, 0.2, 0.25, 0.33, 0.5, and 1.0 Hz or until developed force dropped to ~60% of peak values (n = 2). This latter protocol resulted in an estimated peak VO2. After the contraction protocol, the fibers were mounted at a constant muscle length, and fiber width (widest and narrowest at 2 locations) and length measurements were taken in duplicate. Volume (V) was calculated assuming an ellipse as V = pi  · r(1) · r(2) · length, where r is the cell radius and 1 and 2 are narrowest and widest, respectively (5), and was converted to a mass (1.10 g/cm3).

Kinetic modeling. For kinetic analysis of VO2 dynamics from rest to steady-state contractions, Kaliedagraph data-analysis software (Synergy Software, Reading, PA) was used. A monoexponential model was used as follows
<A><AC>V</AC><AC>˙</AC></A><SC>o</SC><SUB>2</SUB>(<IT>t</IT>)<IT>=</IT><A><AC>V</AC><AC>˙</AC></A><SC>o</SC><SUB>2</SUB>(b)+<IT>A</IT> · [1 − <IT>e</IT><SUP>−(t−TD)/&tgr;</SUP>] (3)
where t is elapsed time after contractions onset, b is baseline, A is asymptotic amplitude for the exponential curve, TD is time delay, and tau  is the time constant.


    RESULTS
TOP
ABSTRACT
INTRODUCTION
METHODS
RESULTS
DISCUSSION
REFERENCES

Metabolic and force output responses to a typical "square-wave" contraction trial in one representative fiber are shown in Fig. 1. For single myocytes (n = 6) subjected to 3 min of tetanic contractions at 0.33-Hz frequency, the VO2 A was 16.7 ± 1.3 ml · 100 g-1 · min-1 (range 13.0-21.9 ml · 100 g-1 · min-1), whereas the TD was 2.1 ± 1.2 (range 0.0-7.7 s) and tau  was 9.4 ± 1.5 s (range 5.2-14.9 s) as determined by Eq. 3. For all cells, force production did not drop below 75% of peak (initial) tension.


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Fig. 1.   Metabolic and force output responses to a typical "square-wave" tetanic contraction trial in 1 representative single myocyte. A: force response and demonstration that this protocol (0.33 Hz for 3 min) did not induce fatigue. B: chamber PO2 before, during, and after contractions (measured every 2 s smoothed with a 6-s rolling average). C: myocyte O2 uptake as calculated from the fall in extracellular PO2 from the chamber.

Figure 2 demonstrates the responses of a fast-twitch (more glycolytic) and slow-twitch (more oxidative) muscle cell type to a "ramp" protocol of increasing contraction frequency. The fall in extracellular PO2 was significantly greater per a given contraction frequency in the glycolytic myocyte (Fig. 2A) due, in part, to a threefold greater mass (slow-twitch = 34 vs. fast-twitch = 104 µg). The more oxidative myocyte was capable of sustaining force production at a level above 60% of initial values significantly longer than the more glycolytic myocyte. However, absolute force production was greater for the glycolytic fiber, thereby mandating a higher VO2 at a given contractile frequency (at 0.1 and 0.2 Hz) compared with the oxidative fiber (Fig. 2B). In general, and as expected, VO2 increased as contraction frequency increased. Furthermore, peak VO2 was greater in the oxidative (31.9 ml · 100 g-1 · min-1) compared with the more glycolytic (26.7 ml · 100 g-1 · min-1) cell (Fig. 2B).


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Fig. 2.   A: chamber PO2 at rest and during progressive (increased contraction frequency every 2 min) ramp protocol in a glycolytic and oxidative myocyte. B: calculated steady-state VO2 at each contraction frequency for each fiber. For each fiber, contractions were induced electrically to elicit tetanic contractions. In A, horizontal lines demarcate alterations in stimulation frequency, whereas vertical lines distinguish the net fall in chamber PO2 at each stimulation frequency.


    DISCUSSION
TOP
ABSTRACT
INTRODUCTION
METHODS
RESULTS
DISCUSSION
REFERENCES

Phosphorescence-quenching techniques were utilized in the present study to develop a novel procedure for measuring steady-state VO2 during contractions and VO2 dynamics across the rest-to-contractions transition in single isolated X. laevis myocytes. To our knowledge, this is the first investigation to quantify VO2 on-kinetics in a single muscle cell.

Agreement with previous findings. Muscle VO2 has been measured in a number of species, including humans, dogs, rats, and frogs. Maximal values obtained either volitionally [e.g., humans, ~60 ml · 100 g-1 · min-1 (22)] or induced electrically [e.g., rat, ~9 ml · 100 g-1 · min-1 (20); dog, ~27 ml · 100 g-1 · min-1 (13)] vary on the basis of species. Furthermore, with the use of a polarographic O2 electrode, values for isolated X. laevis iliofibularis myoyctes reached ~19.5 ml · 100 g-1 · min-1 (25). With use of the technique described herein, maximal VO2 values for the two myocytes in which this was measured ranged from ~25 to 32 ml · 100 g-1 · min-1 (Fig. 2), which fall within the range for that reported previously.

Technical limitations (as discussed below) have precluded the quantification of VO2 kinetics in single myocytes. However, muscle VO2 on-kinetics have been reported in intact muscle groups such as human quadriceps [e.g., half-time of the response (t1/2) = 28 s (10); t1/2 = 25 s (1)] and canine gastrocnemius-plantaris muscle [t1/2 = 16.5 s (21); t1/2 = ~20 s (9)]. One question, which has remained elusive, is whether an actual TD in oxidative phosphorylation exists at the rest-to-work transition. When Bangsbo et al. (1) corrected for blood transit time from femoral vein to sampling port, the TD before an increase in VO2 occurred between 2 and 6 s from exercise onset. Data presented in this study suggest that the readjustment of oxidative metabolism to a higher metabolic demand can begin quite rapidly and, in some cases, almost immediately.

After the TD, the increase in muscle VO2 has been well characterized by a monoexponential rise to steady-state levels (e.g., Refs. 9, 21). The value of tau  for the myocytes studied in the investigation was ~9 s. This value is comparatively fast to that shown for human and dog muscle, yet it is similar to the pulmonary VO2 primary component time constant at the transition to a higher running speed in the horse (16). It seems plausible that much of the variability seen both within and across species regarding VO2 kinetics and amplitude can be explained by fiber type (14) and/or oxidative capacity (25). However, to date, that issue has yet to be resolved. As discussed below, this single myocyte preparation, coupled with the facility to discriminate fiber type and assess oxidative capacity, offers a strong tool to elucidate the contribution of fiber type per se (vs. oxidative capacity) in determining not only the maximal aerobic capacity of muscle but also the rate at which aerobic metabolism adjusts to step increases in metabolic demand.

As discussed above, the time between metabolic stimulus and a discernable increase in oxidative metabolism (i.e., TD) is <6 s in human quadriceps (1) and was less in most of the myocytes studied in this investigation. Hogan (12) demonstrated that, at contraction onset, the time before a fall in single frog myocyte intracellular PO2 was ~13 s during the first contraction bout and speeded significantly to ~5 s with the second stimulation. The measurements of VO2 in the present study show somewhat faster kinetics, as calculated in Eq. 3, than that seen in the fall in intracellular PO2 (11, 12). Although it is uncertain at present as to why this discrepancy exists, it may be that if the O2 diffusing capacity of the myocyte exceeds the metabolic rate of the cell, an O2 gradient will only exist temporally; i.e., there may be measurable flux of O2 without a large PO2 gradient. Consequently, the TD before the fall in intracellular PO2 (12) does not necessarily equate with the onset of aerobic metabolism but rather the point at which the rate of aerobic metabolism becomes greater than the O2 diffusive capacity of the cell. Moreover, if the mitochondria are located primarily in the periphery of the cell, then a loss of O2 may occur from the extracellular fluid before mean intracellular PO2 is altered significantly.

Methodological limitations. A major concern in the present preparation was adequate mixing within the chamber. However, in the present study, acute manipulations in PO2 within the chamber, either by exposing the chamber to the atmosphere or infusing Ringer solution at a different PO2, were detected within 1 s. Furthermore, the minimal TD in the VO2 increase at contraction onset further suggests that the unstirred layer surrounding the myocyte is likely too thin to contribute significantly to the O2 diffusion barrier present under these experimental conditions. A second concern is that O2 conductance is inherently different in this preparation than from seen in an intact muscle preparation where O2 flux takes place primarily between the discrete capillary-to-myocyte interface (19). However, as it has traditionally remained technically formidable to not only quantify the myocyte-to-capillary surface area ratio in whole muscle but also to determine the PO2 within the capillary network, the ability to carefully set and control a homogeneous O2 environment surrounding the single myocyte in the present preparation eliminates the need for these determinations. A third concern is that PO2 within the chamber falls (i.e., becoming more hypoxic), due toVO2, over the duration of the contraction protocol given the finite O2 volume within the sealed chamber. However, over the arguably most critical time period (first 30-60 s) of contraction onset, chamber PO2 drops 1-5 Torr, which would not be expected to alter significantly the initial metabolic response.

Advantages and applications of this technique. Previous attempts to measure VO2 within single muscle cells (e.g., Refs. 5, 25) or isolated muscle fiber bundles (e.g., Refs. 6, 15) have invariably used a polarographic style O2 electrode, which necessitates larger fluid volumes and introduces noise in the electrode signal as a result of the voltage pulse necessary to stimulate the fiber (18). Given the stability of the Pd-porphyrin O2 probe, its innocuous nature when in contact with biological tissue and the rapidity with which it can be sampled (for review, see Ref. 30), the phosphorescence-quenching technique offers a viable solution for measuring PO2 in small volumes. Indeed, phosphorescence quenching is currently used to measure frog single myocyte intracellular PO2 (11) as well as rat microvascular PO2 (3).

Resolution of the contributing factors that may be responsible for setting the VO2 on-kinetic response is hindered by heterogeneity associated with fiber-type composition as well as convective and conductive O2 delivery (27). The technique described herein is particularly advantageous in that VO2 dynamics can be studied independent of fiber type, muscle recruitment, blood flow patterns, and/or humoral variables. Furthermore, the mechanistic basis for the VO2 slow component that occurs at work performed above the lactate threshold is likely confounded by or associated with muscle recruitment (8). Thus this single-myocyte preparation offers an excellent tool to assess whether the additional O2 cost arises within the individual myocytes or is associated with some alteration in fiber recruitment. Furthermore, this technique can be developed for measurement of economy and efficiency of different fiber types at different time points during contractions, including during fatiguing and hypoxic conditions. One final and particularly powerful application of this methodology is that intracellular biochemical responses assessed via fluorescence microscopy and VO2 can be measured simultaneously.

These results demonstrate that VO2 can be quantified in isolated single skeletal myocytes with the use of a phosphorescence-quenching-based technique. VO2 values in the Xenopus lumbrical myocytes, both amplitudes and kinetics, are consistent with that seen in skeletal muscle of other species as well as in other muscles of the frog. This technique can be utilized to study single myocyte VO2 independent of confounding variables associated with whole muscle preparations and thus represents a powerful tool in understanding the readjustment of oxidative phosphorylation to an increased metabolic demand.


    ACKNOWLEDGEMENTS

This work was supported, in part, by National Institute of Arthritis and Muscloskeletal and Skin Diseases (NIAMSD) Grant AR-40155 (to M. C. Hogan), NIAMSD Grant 1 F32 AR-48461 (to C. A. Kindig), and National Institute on Aging Grant 1 F32 AG-20014 (to K. M. Kelley). R. A. Howlett is a Parker B. Francis fellow.


    FOOTNOTES

Address for reprint requests and other correspondence: C. A. Kindig, Div. of Physiology, Dept. of Medicine, Univ. of California, San Diego, 9500 Gilman Dr., MC0623A, La Jolla, CA 92093-0623 (E-mail: ckindig{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.

October 11, 2002;10.1152/japplphysiol.00559.2002

Received 26 June 2002; accepted in final form 28 September 2002.


    REFERENCES
TOP
ABSTRACT
INTRODUCTION
METHODS
RESULTS
DISCUSSION
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P. McDonough, B. J Behnke, D. J Padilla, T. I Musch, and D. C Poole
Control of microvascular oxygen pressures in rat muscles comprised of different fibre types
J. Physiol., March 15, 2005; 563(3): 903 - 913.
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Am. J. Physiol. Cell Physiol.Home page
Y. Chung, P. A. Mole, N. Sailasuta, T. K. Tran, R. Hurd, and T. Jue
Control of respiration and bioenergetics during muscle contraction
Am J Physiol Cell Physiol, March 1, 2005; 288(3): C730 - C738.
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J. Physiol.Home page
C. A. Kindig, C. M. Stary, and M. C. Hogan
Effect of dissociating cytosolic calcium and metabolic rate on intracellular PO2 kinetics in single frog myocytes
J. Physiol., January 15, 2005; 562(2): 527 - 534.
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Am. J. Physiol. Regul. Integr. Comp. Physiol.Home page
S. Koga, D. C. Poole, T. Shiojiri, N. Kondo, Y. Fukuba, A. Miura, and T. J. Barstow
Comparison of oxygen uptake kinetics during knee extension and cycle exercise
Am J Physiol Regulatory Integrative Comp Physiol, January 1, 2005; 288(1): R212 - R220.
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J. Physiol.Home page
D. P Wilkerson, I. T Campbell, and A. M Jones
Influence of nitric oxide synthase inhibition on pulmonary O2 uptake kinetics during supra-maximal exercise in humans
J. Physiol., December 1, 2004; 561(2): 623 - 635.
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J. Appl. Physiol.Home page
E. G. Mik, T. G. van Leeuwen, N. J. Raat, and C. Ince
Quantitative determination of localized tissue oxygen concentration in vivo by two-photon excitation phosphorescence lifetime measurements
J Appl Physiol, November 1, 2004; 97(5): 1962 - 1969.
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Am. J. Physiol. Heart Circ. Physiol.Home page
A. Lo, A. J. Fuglevand, and T. W. Secomb
Theoretical simulation of K+-based mechanisms for regulation of capillary perfusion in skeletal muscle
Am J Physiol Heart Circ Physiol, August 1, 2004; 287(2): H833 - H840.
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Am. J. Physiol. Heart Circ. Physiol.Home page
A. Lo, A. J. Fuglevand, and T. W. Secomb
Oxygen delivery to skeletal muscle fibers: effects of microvascular unit structure and control mechanisms
Am J Physiol Heart Circ Physiol, August 7, 2003; 285(3): H955 - H963.
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J. Appl. Physiol.Home page
C. A. Kindig, R. A. Howlett, and M. C. Hogan
Effect of extracellular PO2 on the fall in intracellular PO2 in contracting single myocytes
J Appl Physiol, May 1, 2003; 94(5): 1964 - 1970.
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