Journal of Applied Physiology AJP: Cell Physiology
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J Appl Physiol 89: 2422-2429, 2000;
8750-7587/00 $5.00
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Vol. 89, Issue 6, 2422-2429, December 2000

Metabolic component of intestinal PCO2 during dysoxia

Ovais Raza and Robert Schlichtig

Department Research and Development, Veterans Affairs Medical Center, Pittsburgh, Pennsylvania 15240


    ABSTRACT
TOP
ABSTRACT
INTRODUCTION
METHODS
RESULTS
DISCUSSION
REFERENCES

The adequacy of intestinal perfusion during shock and resuscitation might be estimated from intestinal tissue acid-base balance. We examined this idea from the perspective of conventional blood acid-base physicochemistry. As the O2 supply diminishes with failing blood flow, tissue acid-base changes are first "respiratory," with CO2 coming from combustion of fuel and stagnating in the decreasing blood flow. When the O2 supply decreases to critical, the changes become "metabolic" due to lactic acid. In blood, the respiratory vs. metabolic distinction is conventionally made using the buffer base principle, in which buffer base is the sum of HCO3- and noncarbonate buffer anion (A-). During purely respiratory acidosis, buffer base stays constant because HCO3- cannot buffer its own progenitor, carbonic acid, so that the rise of HCO3- equals the fall of A-. During anaerobic "metabolism," however, lactate's H+ is buffered by both A- and HCO3-, causing buffer base to decrease. We quantified the partitioning of lactate's H+ between HCO3- and A- buffer in anoxic intestine by compressing intestinal segments of anesthetized swine into a steel pipe and measuring PCO2 and lactate at 5- to 10-min intervals. Their rises followed first-order kinetics, yielding k = 0.031 min-1 and half time = ~22 min. PCO2 vs. lactate relations were linear. Over 3 h, lactate increased by 31 ± 3 mmol/l tissue fluid (mM) and PCO2 by ~17 mM, meaning that one-half of lactate's H+ was buffered by tissue HCO3- and one-half by A-. The data were consistent with a lumped pKa value near 6.1 and total A- concentration of ~30 mmol/kg. We conclude that the respiratory vs. metabolic distinction could be made in tissue by estimating tissue buffer base from measured pH and PCO2.

intestine; lactate; acid-base imbalance; diagnosis; laboratory


    INTRODUCTION
TOP
ABSTRACT
INTRODUCTION
METHODS
RESULTS
DISCUSSION
REFERENCES

INTESTINAL TISSUE ACID-BASE balance has been investigated by many as a detector of inadequate or "dysoxic" intestinal perfusion (8). However, interpretation of tissue acid-base balance remains controversial (31, 39). Early proponents (8) proposed calculation of intestinal tissue pH from measured intestinal PCO2 and arterial plasma HCO3-. Our laboratory (23, 26) proposed interpreting just the intestinal PCO2. The idea was that critical or "maximum respiratory" PCO2 should be that which would occur if all the O2 in a given arterial blood sample were replaced with CO2, thereby simulating maximum O2 extraction and CO2 stagnation in the absence of strong acid. Larger than maximum respiratory PCO2 would indicate tissue HCO3- degradation to CO2 by strong or "metabolic" acid. However, our prediction of critical PCO2 turned out to be an underestimate when later applied prospectively (22). The problem, we suspected, had to do with countercurrent CO2 exchange in vivo, which is difficult to predict (33).

The intent of the current investigation was to consider tissue acid-base balance as a potential detector of dysoxia from the perspective of the respiratory vs. metabolic distinction conventionally employed during the past 50 years in blood (9, 27, 35-38). This understanding is consistent both conceptually and quantitatively. Although several different sets of acid-base nomenclature are used according to preference, all are based on the same fundamental reasoning (24, 27) and all yield practically identical conclusions when properly translated (28, 29).

In blood, H+ is the acid-base variable regulated by biological processes, but it is a dependent variable physicochemically. H+ homeostasis of an organism is therefore produced by one or more of the three independent physicochemical variables: PCO2 (respiratory), strong ion difference (SID; metabolic), and total noncarbonic weak acid buffer (Atot). CO2 is an acid because it combines with H2O to form H+ and HCO3-. It is a "weak" acid because the net reaction is reversible, with its final equilibrium dependent on prevailing H+ availability. The second independent variable, SID, is the net charge of strong (38) or "fixed" (37) ions that do not bond with any other regardless of pH. SID is typically Na+ + K+ - Cl- - lactate (La-). The third variable, Atot (nonvolatile or noncarbonic weak acid buffer), is also a weak acid. Atot is mainly histidine residues on protein (e.g., hemoglobin, albumin). Like CO2, Atot can donate or accept H+ depending on prevailing H+ availability. Unlike CO2, however, Atot does not change with lung ventilation or perfusion so that it typically does not change quickly enough in physiological systems to produce substantive acid-base changes (24).

In blood, the distinction between respiratory and metabolic disturbances can be made using the buffer base principle (37). Buffer base is the sum of the two buffers that account for virtually all of H+ buffered, HCO3-, and anion (A-). Buffer base is a physicochemical "mirror image" of SID (metabolic). The sum of HCO3- and A- is negative and must equal the net charge of the strong ions (SID), which is positive, to preserve electroneutrality. HCO3- is estimated from pH and PCO2, and A- is estimated from the same pH and an estimate of Atot. Buffer base (like SID) stays constant during respiratory disturbances because the H+ coming from carbonic acid cannot be buffered by its by-product, HCO3-, so that the decrease in A- equals the increase in HCO3-. During metabolic acidosis, however, both HCO3- and A- buffer the H+, and buffer base (like SID) decreases.

During progressively decreasing perfusion in tissue, the acidosis is initially respiratory. The CO2 produced by aerobic metabolism stagnates in the decreased blood flow, causing PCO2 to increase and pH to decrease. Buffer base (or SID) remains constant because no appreciable strong acid is being produced. As flow decreases to critical, however, lactic acid is produced by anaerobic metabolism, causing buffer base (or SID) to decrease.

The goal of the current investigation was to examine how respiratory (aerobic) and metabolic (anaerobic) acid-base disturbances might be distinguished in tissues by applying this common acid-base scheme. We packed freshly harvested intestine of anesthetized swine into steel pipes and sequentially measured PCO2 and lactate concentration. The behavior of the resulting PCO2 vs. lactate relations, analyzed from the perspective of common acid-base chemistry, provided estimates of the concentration and lumped negative logarithm of the equilibrium constant (pKa) value of intestinal tissue Atot. Application of this scheme to distinguish respiratory from metabolic acid-base balance in tissue would require that both tissue pH and PCO2 be measured.


    METHODS
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ABSTRACT
INTRODUCTION
METHODS
RESULTS
DISCUSSION
REFERENCES

Surgical preparation. In a protocol approved by the Institutional Animal Care and Use Committee, seven domestic juvenile swine weighing ~20 kg each were fasted for 24 h, sedated with 10 mg/kg im ketamine, and anesthetized with 30 mg/kg iv pentobarbital sodium injected through an ear vein. Tracheas were cannulated for mechanical lung ventilation, and lungs were ventilated at a tidal volume, rate, and inspired O2 fraction sufficient to maintain arterial PO2 at ~150 Torr and arterial PCO2 at ~40 Torr. The right internal jugular vein was cannulated for continuous infusion of pentobarbital sodium at 2-4 mg · kg-1 · h-1, and a catheter was advanced into the carotid artery to monitor arterial blood pressure and to sample arterial blood gases. All animals were volume loaded with lactated Ringer sufficient to maintain systolic arterial blood pressure >110 mmHg and were given 250 ml of 10% dextrose 30 min before data collection so as to maximize substrate available for anaerobic glycolysis. The intestines were exposed via a midline laparotomy.

Steel pipe. A 3-m-long steel pipe (Fig. 1), internal diameter = 1.3 cm and external diameter = 1.7 cm, which was threaded at one end, was used to store intestinal tissue segments anaerobically during ischemic measurements. A steel cap was screwed securely onto the threaded end of the pipe. A tight-fitting hole was drilled into the steel cap for the PCO2 electrode. When inserted into this hole for measurements, the PCO2 electrode protruded ~2 cm into the lumen of the pipe. Intestines were pulled into this pipe with a 4-m length of umbilical tape that passed through this same hole. To seal the opposite end of the pipe anaerobically and also to advance tissue segments for biopsy, a 0.5-cm-diameter steel "ramrod" with a tight-fitting washer at its tip was used.


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Fig. 1.   Depiction of the experimental apparatus used.

Experimental protocol. After the laparatomy was completed, a 7-cm segment of small intestine was isolated by tying umbilical tape strictures at both ends. Mucosal PCO2 was then measured between these strictures through a small antimesenteric incision. The arterial and venous mesenteric blood vessels supplying the segment were then quickly ligated, and the intestinal segment was removed, cut longitudinally, and frozen in liquid N2. About 45 s elapsed from the time that mucosal PCO2 was measured until the segment was vascularly isolated and placed in liquid N2. The ends of the harvested segments adjacent to the umbilical tape strictures were amputated before freezing to isolate perfused from unperfused tissue. This procedure was performed three to four times for each animal.

After these baseline aerobic measurements were obtained, each animal was given an additional 10 mg/kg pentobarbital sodium and rapidly exsanguinated by venting the carotid arterial cannula to a collection bag. A length of intestine was then dissected from the animal and pulled into the steel pipe with umbilical tape. Intestinal contents were milked from the intestinal lumen before drawing them into the steel pipe. When the tied end of intestine reached the threaded end of the steel pipe, the intestine was cut at the umbilical tape. To minimize air within the steel pipe, the capped and threaded end was repeatedly pounded on a solid surface with the pipe in a vertical position, thereby permitting an additional ~0.5 m of intestine to be threaded into the pipe. The steel cap was then removed. The ramrod was used to force the distal end of the intestine into the pipe until a ~2 cm length of intestine (the end with the umbilical tape) protruded from the threaded end of the pipe. This protruding length of intestine was amputated, the steel cap was replaced, the hole in the steel cap was covered tightly with aluminum foil, and the pipe was incubated at 40°C. The process of sealing the intestine in the pipe required 10-15 min. During this time, a third operator monitored luminal PCO2 of intestine still remaining in the animal and prepared frozen segments for La- measurement.

At 5- to 10-min intervals, intestinal segments ~10 cm in length were forced from the pipe by unscrewing the cap at one end and pushing the ramrod from the other. These segments were amputated with a scissors and immediately frozen in liquid N2. The cap was then replaced, and the PCO2 electrode was reinserted against the remaining intestinal surface and allowed to come to a steady reading, which was recorded before amputation of the next sample.

Measurements and calculations. PCO2 electrodes (Microelectrodes, Londonderry, NH) and PCO2 meters (Orion) were calibrated in 40 mM NaHCO3 baths (40°C) as previously described (22) to establish linearity. Bath fluid (40°C) was injected into our Radiometer ABL 330 analyzer where PCO2 was measured at 37°C. We interpreted PCO2 electrode measurements from this 37°C frame of reference. Because the sensitivity of these electrodes tended to drift over time, two-point calibrations were performed before each tissue PCO2 measurement, and this two-point calibration was used to correct measured PCO2 by interpolation or extrapolation.

Frozen intestine was ground into a fine powder in liquid N2 with a mortar and pestle. Thick saran covered the intestine during grinding to minimize condensation of atmospheric H2O. About 5 g of this powder were poured into a plastic test tube, which was mounted on a scale, and an exactly equal weight of 0.2 mM iodoacetic acid was added to prevent further glycolysis during rewarming. This mixture was then thoroughly homogenized with a motorized tissue homogenizer, and the supernatant was analyzed for La- and glucose with a glucose-lactate analyzer (Yellow Springs Instruments). This analyzer measures La- as accurately as the Boehringer Mannheim photoenzymatic method (5). We assumed that the freezing-thawing process, as well as the homogenization process, thoroughly lysed all cells and that La- of the supernatant approximated La- of the liquid phase of the mixture. Initial measurements were performed using this 1:2 dilution. When La- approached the accuracy limits of the glucose-lactate analyzer (~10 mM), supernatants were further diluted with 0.2 M iodoacetic acid. Increases in tissue PCO2 were converted to corresponding decrements in tissue HCO3- by multiplying the change in PCO2 by the solubility coefficient of CO2, 0.0306 mM/Torr (32).

Data analysis. We assumed that changes in SID were equal to changes in La- because La- is a strong anion and because concentrations of other strong ions must have remained constant. Hence, increases in La- were taken as decreases in SID, the independent (metabolic) acid-base variable.

We did not measure total CO2 (CO2tot). Hence, we could quantify only changes in HCO3- using our methods. Changes in HCO3- were quantified as changes in PCO2 multiplied by its solubility coefficient, 0.0306 mM HCO3- per Torr PCO2. To estimate Atot and its dissociation constant of noncarbonic acid (Ka), we used the equation
Buffer base<IT>=</IT>CO<SUB>2tot</SUB><IT>/</IT>(<IT>0.0306×</IT>H<SUP>+</SUP><IT>/K</IT><SUB>c</SUB><IT>+1</IT>) (1)

<IT>+</IT>(<IT>K</IT><SUB>a</SUB><IT>×</IT>A<SUB>tot</SUB>)<IT>/</IT>(H<SUP>+</SUP><IT>+K</IT><SUB>a</SUB>)
where Kc is the dissociation constant of carbonic acid. We reasoned that, in the closed system that we were studying, CO2tot was constant, permitting substitution of (CO2tot - HCO3-)/0.0306 for PCO2 in the Henderson equation and giving HCO3- = CO2tot/(0.0306 × H+/Kc + 1). We further assumed a lumped Atot equilibrium, H+ × A- = Ka × HA, and substituted Atot - A- for HA, giving A- = (Ka × Atot)/(H+ + Ka). Because buffer base = HCO3- + A-, these latter two expressions could be combined to give Eq. 1.

Equation 1 predicts that a value for Ka that is the same as that for carbonic acid yields a linear PCO2 vs. SID relation (or a linear HCO3- vs. SID relation) (Fig. 2). The relation is linear because the values for Ka and Kc are equal, meaning that, as pH changes, the percent change in HCO3- equals the percent change in A-. Hence, new H+ donated by strong acid is divided between HCO3- and A- in direct proportion to their concentrations, resulting in a linear PCO2 or HCO3- vs. SID relation. However, a Ka value higher or lower than that of carbonic acid yields a PCO2 vs. SID relation that is convex upward or downward (Fig. 2). On the basis of this understanding, we reasoned that an experimentally observed PCO2 vs. SID relation that was linear would indicate a pKa value near that of carbonic acid, whereas a curvilinear relation would indicate a pKa value greater than or lower than that of carbonic acid.


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Fig. 2.   Fundamental acid-base physicochemistry in blood. Top: fraction of negatively charged buffer as a function of pH for 3 different buffers with pKa values of 5.1, 6.1, and 7.1. pKa is the pH value at which one-half of the buffer is ionized. Middle and bottom: PCO2 vs. strong ion difference (SID) relations for 3 different closed systems containing 1 of the noncarbonate buffers shown at top in addition to HCO3-. If the pKa of noncarbonate buffer equals 6.1, i.e., the same pKa as carbonic acid, the resulting PCO2 vs. SID relation is linear. If the pKa of the noncarbonate buffer is greater than or less than 6.1, the resulting relations are convex downward or upward, respectively. Middle: PCO2 vs. SID relations for a fluid with a total noncarbonate buffer (Atot) concentration of 20 mM and total CO2 (CO2tot) concentration of 25 mM, typical values for plasma. In bottom, Atot = 105 mM and CO2tot = 13 mM, the values for erythrocyte fluid (29, 35). BB, buffer base.

Equation 1 also predicts that the slope of HCO3- or PCO2 vs. SID is directly proportional to the CO2tot fraction of total buffer, i.e., CO2tot/(CO2tot + Atot), provided that noncarbonate buffer pKa is near 6.1. The reason is that CO2 and Atot exhibit identical buffering characteristics at any given pH, so that HCO3- is depleted at fractionally the same rate as that for A-. The slope of the line, i.e., Delta PCO2/Delta SID, equals 32.7 times the CO2 fraction of total buffer, where total buffer is Atot + CO2tot (Fig. 3).


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Fig. 3.   Slope of PCO2 vs. SID relations as a function of the CO2tot fraction of total buffer for any closed system in which the pKa of the noncarbonate buffer equals that of carbonic acid, i.e., 6.1 pH units.

Statistical considerations. The increase in PCO2 and the increase in tissue La- with time were compared using Pearson's correlation, and significance was taken as P < 0.05. The relations between PCO2 and intestinal tissue La- were analyzed by linear regression.


    RESULTS
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ABSTRACT
INTRODUCTION
METHODS
RESULTS
DISCUSSION
REFERENCES

Initial and final values of PCO2, La-, and glucose are displayed in Table 1. La- increased by ~30 mM, whereas PCO2 increased by ~550 Torr, meaning that HCO3- decreased by ~0.0306 × 550 or 17 mM. Figure 4, top, shows the increases in PCO2 and La- with time for the group. Dissolved CO2 (in mM) increased at about one-half the rate that La- increased, indicating that about one-half of lactate's H+ was taken up by HCO3- and one-half by A-. Our data fit the equation PCO2 = 597 - 514-t/32.4. Figure 4, bottom, expresses the same data in terms anaerobic CO2 production rate (VCO2) (right axis) and in terms of HCO3- decay rate (left axis). The initial rate of anaerobic VCO2 was ~0.5 mmol · kg-1 · min-1. This compares with a normal aerobic intestinal VCO2 of ~0.8 mmol/min, calculated from intestinal O2 consumption of 20 ml · kg-1 · min-1 (19, 20) and respiratory quotient of 0.85 (42). HCO3- decay was consistent with first-order kinetics with a half time of 22.4 min and rate constant of 0.031 min-1.

                              
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Table 1.   Initial values, final values, and total change in values for PCO2, La-, and glucose



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Fig. 4.   Top: increase in dissolved CO2 () and in tissue La- () over time for a group of 6 animals. Values represent means ± SE. Brackets indicate concentration. Bottom expresses the same data in terms anaerobic CO2 production rate (VCO2; right) and in terms of HCO3- decay rate (left).

Figure 5A shows the relation between PCO2 and tissue La-. Each of these relations was approximately linear, with the exception of subject 3, for which PCO2 decreased progressively during the final five data collections. We believe these data represented loss of CO2 gas from the steel pipe and thus did not include them in the analysis. Average r2 was 0.94 ± 0. Because the PCO2 vs. La- relations were linear, the pKa value for noncarbonate buffer (Atot) should have been near 6.1, as per our methods displayed in Fig. 2, middle and bottom. Average slope of our relations was 16.7 ± 1.6 Torr/mM change in tissue La-, suggesting a CO2tot-to-total buffer ratio of ~50%, as per our methods displayed in Fig. 3. Hence, CO2tot concentration approximated Atot concentration. We did not measure CO2tot but would estimate it roughly at 30 mM, the quantity of HCO3- degraded in the subject with the largest change in La- concentration (subject 2).


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Fig. 5.   Relation between intestinal tissue PCO2 and La- (A) and between intestinal tissue La- and glucose (B). The  values were included in statistical analysis; + values were excluded from statistical analysis.

Figure 5B shows the relation between tissue La- and tissue glucose. These relations were also linear (average r2 = 0.91 ± 0, average slope = -2.75 ± 0.2 mmol tissue La-/mmol tissue glucose). This finding of more La- produced than glucose catabolized suggests perhaps some pyruvate production by alanine transaminase, i.e., alpha -keto acid + alanine left-right-arrow alpha -amino acid + pyruvate. Average y- and x-intercepts were 44 ± 4 and 16.2 ± 2 mM.


    DISCUSSION
TOP
ABSTRACT
INTRODUCTION
METHODS
RESULTS
DISCUSSION
REFERENCES

Care of critically ill patients might advance if dysoxia, i.e., insufficient O2 to support O2 demand, could be detected in organs other than the beating heart or conscious brain. It would then be possible to reevaluate resuscitation and life support therapies currently in use. Here, we address the question of how tissue acid-base balance might be used to detect dysoxia, suggesting application of an old conceptual framework. Respiratory imbalance means abnormal CO2 efflux from the system and is quantified as the difference between normal and measured PCO2. Metabolic imbalance means abnormal accumulation of strong acid or base. Metabolic imbalance can be quantified by measuring pH and PCO2 if Atot and Ka are known (9, 27, 29, 35-38). Our findings suggest an intestinal tissue pKa near 6.1 and Atot of roughly 30 mmol/l.

What is the intestinal tissue value for Ka? Our method for estimating intestinal tissue Ka from PCO2 vs. La- relations (Eq. 1 and Fig. 3) is new. It is a simplification of an approach earlier used by Katsura et al. (15) to draw conclusions about the buffering characteristics of brain tissue. They had observed linear PCO2 vs. La- relations in anoxic brain and proposed several arbitrary pKa values for brain proteins to simulate their data (15). Here, we have assumed that tissue protein behaves as if there were a single Ka value. We based this assumption on the fact that this simplification is entirely satisfactory in blood. For example, Figge et al. (9) estimated the Ka value for each individual histidine residue on the albumin molecule and developed a complex buffer base or "estimated SID" equation that used a different Ka value for each residue. However, their equation proved reducible to a simple linear equation that assumed a common Ka value for albumin, sacrificing no accuracy in this process (24). Their equation further proved to be no improvement over Siggaard-Andersen's original base excess equations, which had assumed a single Ka value for plasma of all individuals, regardless of plasma albumin or phosphate concentration (29). We therefore submit that buffering in any given fluid compartment (e.g., plasma, hemoglobin, intestinal tissue, brain tissue) does not differ sufficiently among individuals to require direct measurement of buffer concentration. Only pH and PCO2 are needed if the typical buffer concentration and its pKa is known.

Equation 1 can be applied to the data of Katsura et al. (15) to give practically the same estimates that they provided. The weighted average of the arbitrary pKa values that they (15) had proposed to simulate their data was 5.9, which is close to the 6.1 value that we would assign based on the simple linearity of their PCO2 vs. La- relations.

What is the intestinal tissue value for Atot? The slopes (Fig. 3) of the PCO2 vs. La- relations (Fig. 5) indicated that Atot was approximately equal to CO2tot. Because we didn't measure CO2tot, our rough estimate of it was based on HCO3- degraded in the subject with the largest La- accumulation (subject 2, Fig. 5), i.e., 30 mmol/kg. Our methods are more easily applied to the data of Katsura et al., who measured CO2tot directly in their preparations (15). CO2tot of their hypocapnic preparations was ~13 mmol/kg, and their slope for brain PCO2 vs. La- was ~ 6.2 Torr/mM, giving a CO2tot fraction of total buffer equal to 19% (Fig. 3) and an Atot concentration of ~55 mmol/l. In their normocapnic preparations, CO2tot was ~18 mmol/l and slope of PCO2 vs. La- was ~7.5 Torr/mM, giving an Atot concentration of 60 mmol/l. These estimates compare with their Atot estimate of 58 mmol/l, which they had based on best fit of five arbitrary protein Ka values and concentrations.

What is the underlying acid-base disturbance of dysoxia? Here we have assumed that the primary acid-base disturbance of dysoxia is a lactic acidosis. This assumption is at odds with the current belief (10, 11, 14) that lactate does not acidify because it is generated without a proton. This belief is based on chemical balance equations predicting that anaerobic glycolysis should produce no protons per glucose catabolized. The idea is that H+ is added to the system during anaerobiosis only if ATP is hydrolyzed irreversibly. Our data do not address this controversy directly. However, intestinal ATP is only ~2 mM in muscularis (3, 13) and ~2 mM in homogenized whole intestine (16, 18). In our investigation, 17 mM of tissue HCO3- decayed to CO2, requiring at least 17 mM of H+. This 17 mM of H+ could not have come from 2 mM of ATP. In fact, even more than 17 mM of H+ must have been produced to account for the HCO3- decomposed because tissue, like blood, must contain substantial quantities of protein with histidine residues, which also buffer H+. We thus submit that lactic acid is the chief anaerobic product.

Phosphocreatine (PCr2-) is thought to be a strong anion, with a pKa of 4.5 (17). Hence, the influence of increasing lactate concentration on the SID could be counterbalanced by decreases in PCr2- as dysoxia progresses in organs such as skeletal muscle. However, PCr2- concentration in intestinal muscularis is only 2-3 mmol/l, and it is not present in mucosa at all (3, 13). We are not aware of any other tissue strong ions that change appreciably during dysoxia. In dysoxic intestine that is still perfused, K+ is excreted in equal proportion with La- (22) so that net tissue SID should not change appreciably.

Why were the PCO2 values so large? In our gas-tight chamber, intestinal PCO2 approached atmospheric pressure within ~2 h (Fig. 5). These PCO2 values may seem quite large but are similar to those originally reported by Bass et al. (2) who measured PCO2 with a mass spectrometer. In most subsequent investigations, intestinal tissue PCO2 has been measured with silastic balloon tonometers (8, 26, 40), which have given lower estimates. For example, when our laboratory (26) and Walley et al. (40) used balloon tonometers in small intestine during progressive flow reduction, critical and maximum intestinal PCO2 values were only ~60 and ~150 Torr, respectively. However, use of PCO2 electrodes (22) in similar preparations yielded much larger critical and maximum PCO2 values of ~100 and ~380 Torr, respectively. Tonometers occupy most of the unstressed volume of the small intestinal lumen in medium-sized animals, doubling the space into which CO2 gas can diffuse and thus diluting CO2 gas arising from anaerobic metabolism.

It is conceivable that new CO2 was being generated by decarboxylation of tissue fuel as dysoxia progressed. If so, tissue CO2tot may have been increasing, contrary to what we assumed. However, the main source of tissue CO2tot is mitochondria and O2 is required for its formation.

Although we tried to minimize air space within the pipe, by holding it vertically while pounding it repeatedly on a solid surface, some of the CO2 generated by anaerobic metabolism must have diffused into this air. Because gas space takes up twice as much CO2 as does equivalent tissue space, owing to CO2 solubility, our tissue PCO2 measurements were underestimated to some extent, depending on how much air was in the pipe and on the rate that CO2 diffused from tissue to air within the pipe.

What was the range of tissue pH in our preparations? Without having measured pH, we can provide only a rough approximation, using the Henderson-Hasselbalch equation, of our measured PCO2 values (Table 1) and a guess of initial intestinal HCO3- in our preparations. If we assume that initial HCO3- concentration was approximately equal to HCO3- degraded in the subject with the largest La- accumulation (subject 2, Fig. 5), i.e., 30 mmol/l, then initial pH would be 6.1 + log 30/(0.0306 × 84) or 7.17 pH units. Final HCO3- would be 30 mmol/l minus the average change in HCO3-, 17 mmol/kg, and final pH would be 6.1 + log 14/(0.0306 × 640) or 5.95 pH units. Because we studied tissue, which contains only a small proportion of blood and interstitial fluid, these results would represent average intracellular pH estimates.

How do our findings elucidate intestinal tissue acid-base balance as a potential detector of dysoxia? Our measurements indicated that CO2 generation and lactate accumulation proceeded at the same rate, consistent with first-order kinetics (Fig. 4). The half time of both their accumulations was ~22 min. The initial rate of anaerobic CO2 accumulation was substantively less than normal aerobic VCO2, but PCO2 was much larger than normal because no blood was flowing to carry the CO2 away. One implication of these findings is that the fundamental acid-base change of intestinal dysoxia is lactate accumulation. Another implication is that flow must be extremely low, probably near zero, for PCO2 to increase to the large values that we (22) and others (2) have observed in vivo. If dysoxic tissue were to become reperfused, even transiently, the CO2 ought to be flushed from the tissue quickly. Hence, a large tissue PCO2 value, e.g., >130 Torr (22), ought to be highly specific for dysoxia but possibly insensitive.

What we have primarily suggested in the present paper is application of a common physicochemical scheme for discriminating critical from noncritical reductions in blood flow. If current methods for interpreting intestinal tissue acid-base balance are unreliable, then perhaps this more thoroughly investigated acid-base scheme, used in one form or another for the past half century, might be applied. Noninvasive tissue pH measurements are being explored (21), and it might further be possible to measure PCO2 in a similar manner. If both pH and PCO2 could be measured reliably in tissue, buffer base excess (called base excess) (35, 36) could be computed. Base excess is HCO3- + A-, relative to normal, instead of absolute HCO3- + A-. It would be essential to determine whether the pH measurements were coming from interstitial fluid or from cells (25).

Because La- increases during seemingly nondysoxic conditions such as sepsis (6) and exercise (12), detection of a negative "tissue base excess" by itself might not signify dysoxia. Other systemic acid-base disturbances, such as ketoacidosis and poisoning, produce parallel acid-base changes in tissue in the absence of dysoxia (1). In these conditions, the absence of dysoxia might be inferred from the low tissue PCO2 caused by blood flow adequate to flush CO2 from the tissue or perhaps from the difference between blood and tissue base excess.

Some (41) argue that La- accumulation during hypoxia reflects a buildup of mitochondrial NADH, which drives ATP synthesis toward completion by mass action when O2 is scarce. If so, negative tissue base excess could signify successful adaptation for hypoxia, as opposed to dysoxia. We agree that this argument is valid in isolated cells with uniform PO2. We do not agree that this argument should be applied to intact tissue, where PO2 is different in each cell. In intact tissue, cells with a PO2 that permits increasing redox state to forestall dysoxia are a minor proportion of total cells (4, 30, 34). Consequently, the argument that redox assessment is an insensitive detector of dysoxia does not apply to intact tissue. Cytoplasmic redox state (estimated as lactate/pyruvate) and mitochondrial redox state (estimated as beta -hydroxybutyrate/acetoacetate) remain constant until dysoxia commences in tissue, unlike isolated cells (4, 34).


    ACKNOWLEDGEMENTS

We thank Tracy Ann Gavidia for technical assistance and Prof. John W. Severinghaus for helpful comments during the preparation of this manuscript.


    FOOTNOTES

This work was supported by a grant from the Laerdal Foundation for Acute Medicine.

Address for reprint requests and other correspondence: R. Schlichtig, Noble Hospital, 115 West Silver, Westfield, MA 01086 (E-mail: 104227.2214{at}compuserve.com).

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.

Received 17 December 1998; accepted in final form 7 July 2000.


    REFERENCES
TOP
ABSTRACT
INTRODUCTION
METHODS
RESULTS
DISCUSSION
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J APPL PHYSIOL 89(6):2422-2429
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